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| 118 | </head> |
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| 119 | |
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| 120 | <body lang=EN-US vlink=purple> |
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| 121 | |
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| 122 | <div class=Section1> |
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| 123 | |
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| 124 | <p class=MsoNormal><b><span style='font-size:16.0pt'>Model Functions</span></b></p> |
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| 125 | |
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| 126 | <p class=MsoNormal> </p> |
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| 127 | |
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| 128 | <ul> |
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| 129 | <li><a href="#Introduction"><b>Introduction</b></a></li> |
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| 130 | <li><a href="#Shapes"><b>Shapes</b></a>: |
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| 131 | <a href="#SphereModel">SphereModel</a>, |
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| 132 | <a href="#CylinderModel">CylinderModel</a>, |
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| 133 | <a href="#EllipsoidModel">EllipsoidModel</a>, |
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| 134 | <a href="#CoreShellModel">CoreShellModel</a>, |
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| 135 | <a href="#CoreShellCylinderModel">CoreShellCylinderModel</a>, |
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| 136 | <a href="#EllipticalCylinderModel">EllipticalCylinderModel</a>. |
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| 137 | </li> |
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| 138 | <li><a href="#Shape-Independent"><b>Shape-Independent</b></a>: |
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| 139 | <a href="#Debye">Debye</a>, |
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| 140 | <a href="#Lorentz">Lorentz</a>, |
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| 141 | <a href="#DAB_Model">DAB_Model</a>, |
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| 142 | <a href="#Power_Law">Power_Law</a>, |
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| 143 | <a href="#Teubner Strey">Teubner Strey</a>, |
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| 144 | <a href="#BEPolyelectrolyte">BEPolyelectrolyte</a>, |
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| 145 | <a href="#Number Density Fractal">Number Density Fractal</a>, |
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| 146 | <a href="#Guinier">Guinier</a>, |
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| 147 | <a href="#PorodModel">PorodModel</a>. </li> |
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| 148 | <li><a href="#Customized Models"><b>Customized Models</b></a>: |
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| 149 | <a href="#A+Bcos(2x)+Csin(2x)">A+Bcos(2x)+Csin(2x)</a>. </li> |
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| 150 | <li><a href="#Structure Factors"><b>Structure Factors</b></a>: |
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| 151 | <a href="#HardSphereStructure">HardSphereStructure</a>, |
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| 152 | <a href="#SquareWellStructure">SquareWellStructure</a>, |
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| 153 | <a href="#HayterMSAStructure">HayterMSAStructure</a>, |
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| 154 | <a href="#StickyHSStructure">StickyHSStructure</a>.</li> |
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| 155 | <li><a href="#References"><b>References</b></a></li> |
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| 156 | </ul> |
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| 157 | |
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| 158 | <p class=MsoNormal style='margin-left:.25in;text-indent:-.25in'><b><span |
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| 159 | style='font-size:14.0pt'>1.<span style='font:7.0pt "Times New Roman"'> |
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| 160 | </span></span></b><b><span style='font-size:14.0pt'><a name="Introduction">Introduction</a></span></b></p> |
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| 161 | |
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| 162 | <p class=MsoNormal>The present text documents the modules made available by the |
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| 163 | DANSE software for SANS. </p> |
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| 164 | |
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| 165 | <p class=MsoNormal> </p> |
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| 166 | |
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| 167 | <p class=MsoNormal>Readers are also referred to the SANS/DANSE wiki page:</p> |
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| 168 | |
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| 169 | <p class=MsoNormal> </p> |
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| 170 | |
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| 171 | <p class=MsoNormal style='text-indent:.25in'><i>http://danse.us/trac/sans</i></p> |
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| 172 | |
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| 173 | <p class=MsoNormal> </p> |
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| 174 | |
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| 175 | <p class=MsoNormal>Users can report a bug at the following URL:</p> |
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| 176 | |
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| 177 | <p class=MsoNormal> </p> |
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| 178 | |
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| 179 | <p class=MsoNormal style='text-indent:.25in'><i>http://danse.us/trac/sans/newticket</i></p> |
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| 180 | |
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| 181 | <p class=MsoNormal><b> </b></p> |
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| 182 | |
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| 183 | |
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| 184 | <p class=MsoNormal style='margin-left:.25in;text-indent:-.25in'><b><span |
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| 185 | style='font-size:14.0pt'>2.<span style='font:7.0pt "Times New Roman"'> |
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| 186 | </span></span></b><b><span style='font-size:14.0pt'><a name="Shapes">Shapes (Scattering intensity models)</a></span></b></p> |
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| 187 | |
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| 188 | <p class=MsoNormal> </p> |
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| 189 | |
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| 190 | <p class=MsoNormal>This software provides form factors for various particle |
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| 191 | shapes. After giving a mathematical definition of each model, we draw the list |
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| 192 | of parameters available to the user. Validation plots for each model are also |
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| 193 | presented. Instructions on how to use the software is available with the source |
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| 194 | code, available from SVN:</p> |
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| 195 | |
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| 196 | <p class=MsoNormal> </p> |
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| 197 | |
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| 198 | <p class=MsoNormal style='text-indent:.25in'><i>svn co svn://danse.us/sans/releases/sansmodels-x.x</i></p> |
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| 199 | |
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| 200 | <p class=MsoNormal> </p> |
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| 201 | |
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| 202 | <p class=MsoNormal>To easily compare to the scattering intensity measured in |
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| 203 | experiments, we normalize the form factors by the volume of the particle:</p> |
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| 204 | |
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| 205 | <p class=MsoNormal align=center style='text-align:center'><sub><img width=192 |
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| 206 | height=43 src="../images/html/image001.gif"></sub> (1)</p> |
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| 207 | |
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| 208 | <p class=MsoNormal>with</p> |
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| 209 | |
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| 210 | <p class=MsoNormal align=center style='text-align:center'><sub><img width=159 |
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| 211 | height=29 src="../images/html/image002.gif"></sub> (2)</p> |
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| 212 | |
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| 213 | <p class=MsoNormal>where <i>P</i><sub>0</sub><i>(<b>q</b>)</i> is the |
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| 214 | un-normalized form factor, <i>ρ(<b>r</b>)</i> is the scattering length |
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| 215 | density at a given point in space and the integration is done over the volume <i>V</i> |
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| 216 | of the scatterer. </p> |
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| 217 | |
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| 218 | <p class=MsoNormal> </p> |
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| 219 | |
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| 220 | <p class=MsoNormal>For systems without inter-particle interference, the form |
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| 221 | factors we provide can be related to the scattering intensity by the particle |
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| 222 | volume fraction:<sub><img width=92 height=21 |
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| 223 | src="../images/html/image003.gif"></sub>.</p> |
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| 224 | |
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| 225 | <p class=MsoNormal> </p> |
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| 226 | |
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| 227 | <p class=MsoNormal>Our so-called 1D scattering intensity functions provide <i>P(q) |
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| 228 | </i>for the case where the scatterer is randomly oriented. In that case, the |
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| 229 | scattering intensity only depends on the length of q. The intensity measured on |
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| 230 | the plane of the SANS detector will have an azimuthal symmetry around <i>q</i>=0.</p> |
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| 231 | |
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| 232 | <p class=MsoNormal> </p> |
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| 233 | |
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| 234 | <p class=MsoNormal>Our so-called 2D scattering intensity functions provide <i>P(q, |
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| 235 | </i><i><span style='font-family:"Arial","sans-serif"'>φ</span>)</i> for an |
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| 236 | oriented system as a function of a q-vector in the plane of the detector. We |
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| 237 | define the angle <span style='font-family:"Arial","sans-serif"'>φ</span> |
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| 238 | as the angle between the q vector and the horizontal (x) axis of the plane of |
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| 239 | the detector.</p> |
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| 240 | |
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| 241 | <p class=MsoNormal> </p> |
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| 242 | |
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| 243 | |
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| 244 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
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| 245 | style='font-size:14.0pt'>2.1.<span style='font:7.0pt "Times New Roman"'> |
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| 246 | </span></span></b><b><span style='font-size:14.0pt'><a name="SphereModel">SphereModel</a></span></b></p> |
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| 247 | |
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| 248 | <p class=MsoNormal> </p> |
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| 249 | |
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| 250 | <p class=MsoNormal>This model provides the form factor, P(q), for a |
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| 251 | monodisperse spherical particle with uniform scattering length density. The |
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| 252 | form factor is normalized by the particle volume as described below.</p> |
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| 253 | |
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| 254 | <p class=MsoNormal> </p> |
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| 255 | |
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| 256 | <p class=MsoNormal style='margin-left:.85in;text-indent:-.35in'><b>2.1.1.<span |
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| 257 | style='font:7.0pt "Times New Roman"'> </span></b><b>Definition</b></p> |
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| 258 | |
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| 259 | <p class=MsoNormal> </p> |
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| 260 | |
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| 261 | <p class=MsoNormal>The 1D scattering intensity is calculated in the following way |
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| 262 | (Guinier, 1955):</p> |
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| 263 | |
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| 264 | <p class=MsoNormal align=center style='text-align:center'><sub><img width=337 |
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| 265 | height=53 src="../images/html/image004.gif"></sub> (3)</p> |
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| 266 | |
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| 267 | <p class=MsoNormal>where <i>scale</i> is a scale factor, V is the volume of the |
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| 268 | scatterer, <i>r</i> is the radius of the sphere, <i>bkg</i> is the background |
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| 269 | level and <i><span style='font-family:"Arial","sans-serif"'>Δ</span>ρ</i> |
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| 270 | (contrast) is the scattering length density difference between the scatterer |
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| 271 | and the solvent it is in.</p> |
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| 272 | |
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| 273 | <p class=MsoNormal> </p> |
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| 274 | |
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| 275 | <p class=MsoNormal>The 2D scattering intensity is the same as P(q) above, |
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| 276 | regardless of the orientation of the q vector.</p> |
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| 277 | |
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| 278 | <p class=MsoNormal> </p> |
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| 279 | |
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| 280 | <p class=MsoNormal>The returned value is scaled to units of [cm<sup>-1</sup>] |
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| 281 | and the parameters of the sphere model are the following:</p> |
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| 282 | |
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| 283 | <div align=center> |
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| 284 | |
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| 285 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
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| 286 | style='border-collapse:collapse;border:none'> |
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| 287 | <tr style='height:13.5pt'> |
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| 288 | <td width=135 valign=top style='width:101.0pt;border:solid windowtext 1.0pt; |
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| 289 | padding:0in 5.4pt 0in 5.4pt;height:13.5pt'> |
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| 290 | <p class=MsoBodyText>Parameter name</p> |
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| 291 | </td> |
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| 292 | <td width=135 valign=top style='width:101.0pt;border:solid windowtext 1.0pt; |
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| 293 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:13.5pt'> |
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| 294 | <p class=MsoBodyText>Units</p> |
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| 295 | </td> |
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| 296 | <td width=135 valign=top style='width:101.0pt;border:solid windowtext 1.0pt; |
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| 297 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:13.5pt'> |
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| 298 | <p class=MsoBodyText>Default value</p> |
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| 299 | </td> |
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| 300 | </tr> |
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| 301 | <tr style='height:12.8pt'> |
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| 302 | <td width=135 valign=top style='width:101.0pt;border:solid windowtext 1.0pt; |
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| 303 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:12.8pt'> |
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| 304 | <p class=MsoBodyText>Scale</p> |
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| 305 | </td> |
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| 306 | <td width=135 valign=top style='width:101.0pt;border-top:none;border-left: |
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| 307 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
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| 308 | padding:0in 5.4pt 0in 5.4pt;height:12.8pt'> |
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| 309 | <p class=MsoBodyText>None</p> |
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| 310 | </td> |
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| 311 | <td width=135 valign=top style='width:101.0pt;border-top:none;border-left: |
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| 312 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
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| 313 | padding:0in 5.4pt 0in 5.4pt;height:12.8pt'> |
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| 314 | <p class=MsoBodyText>1.0e-6</p> |
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| 315 | </td> |
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| 316 | </tr> |
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| 317 | <tr style='height:12.8pt'> |
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| 318 | <td width=135 valign=top style='width:101.0pt;border:solid windowtext 1.0pt; |
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| 319 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:12.8pt'> |
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| 320 | <p class=MsoBodyText>Radius</p> |
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| 321 | </td> |
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| 322 | <td width=135 valign=top style='width:101.0pt;border-top:none;border-left: |
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| 323 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
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| 324 | padding:0in 5.4pt 0in 5.4pt;height:12.8pt'> |
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| 325 | <p class=MsoBodyText>Å</p> |
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| 326 | </td> |
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| 327 | <td width=135 valign=top style='width:101.0pt;border-top:none;border-left: |
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| 328 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
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| 329 | padding:0in 5.4pt 0in 5.4pt;height:12.8pt'> |
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| 330 | <p class=MsoBodyText>60</p> |
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| 331 | </td> |
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| 332 | </tr> |
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| 333 | <tr style='height:12.8pt'> |
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| 334 | <td width=135 valign=top style='width:101.0pt;border:solid windowtext 1.0pt; |
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| 335 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:12.8pt'> |
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| 336 | <p class=MsoBodyText>Contrast</p> |
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| 337 | </td> |
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| 338 | <td width=135 valign=top style='width:101.0pt;border-top:none;border-left: |
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| 339 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
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| 340 | padding:0in 5.4pt 0in 5.4pt;height:12.8pt'> |
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| 341 | <p class=MsoBodyText>Å<sup> -2</sup></p> |
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| 342 | </td> |
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| 343 | <td width=135 valign=top style='width:101.0pt;border-top:none;border-left: |
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| 344 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
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| 345 | padding:0in 5.4pt 0in 5.4pt;height:12.8pt'> |
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| 346 | <p class=MsoBodyText>1</p> |
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| 347 | </td> |
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| 348 | </tr> |
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| 349 | <tr style='height:12.8pt'> |
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| 350 | <td width=135 valign=top style='width:101.0pt;border:solid windowtext 1.0pt; |
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| 351 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:12.8pt'> |
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| 352 | <p class=MsoBodyText>Background</p> |
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| 353 | </td> |
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| 354 | <td width=135 valign=top style='width:101.0pt;border-top:none;border-left: |
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| 355 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
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| 356 | padding:0in 5.4pt 0in 5.4pt;height:12.8pt'> |
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| 357 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
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| 358 | </td> |
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| 359 | <td width=135 valign=top style='width:101.0pt;border-top:none;border-left: |
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| 360 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
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| 361 | padding:0in 5.4pt 0in 5.4pt;height:12.8pt'> |
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| 362 | <p class=MsoBodyText>0</p> |
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| 363 | </td> |
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| 364 | </tr> |
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| 365 | </table> |
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| 366 | |
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| 367 | </div> |
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| 368 | |
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| 369 | <p class=MsoNormal> </p> |
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| 370 | |
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| 371 | <p class=MsoNormal>Our model uses the form factor calculations implemented in a |
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| 372 | c-library provided by the NIST Center for Neutron Research (Kline, 2006).</p> |
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| 373 | |
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| 374 | <p class=MsoNormal> </p> |
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| 375 | |
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| 376 | |
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| 377 | <p class=MsoNormal style='margin-left:.85in;text-indent:-.35in'><b>2.1.2.<span |
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| 378 | style='font:7.0pt "Times New Roman"'> </span></b><b>Validation |
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| 379 | of the sphere model</b></p> |
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| 380 | |
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| 381 | <p class=MsoNormal> </p> |
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| 382 | |
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| 383 | <p class=MsoNormal>Validation of our code was done by comparing the output of |
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| 384 | the 1D model to the output of the software provided by the NIST (Kline, 2006). |
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| 385 | Figure 1 shows a comparison of the output of our model and the output of the |
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| 386 | NIST software.</p> |
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| 387 | |
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| 388 | <p class=MsoNormal> </p> |
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| 389 | |
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| 390 | <p class=MsoBodyText align=center style='text-align:center;page-break-after: |
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| 391 | avoid'><img width=573 height=315 id="Picture 5" |
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| 392 | src="../images/html/image005.jpg" alt="sphere_1D_validation"></p> |
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| 393 | |
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| 394 | <p class=MsoCaption>Figure 1: Comparison of the DANSE scattering intensity for |
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| 395 | a sphere with the output of the NIST SANS analysis software. The parameters |
---|
| 396 | were set to: Scale=1.0, Radius=60 Å, Contrast=1e-6 Å<sup> -2</sup>, and |
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| 397 | Background=0.01 cm<sup> -1</sup>.</p> |
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| 398 | |
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| 399 | <p class=MsoNormal> </p> |
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| 400 | |
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| 401 | |
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| 402 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
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| 403 | style='font-size:14.0pt'>2.2.<span style='font:7.0pt "Times New Roman"'> |
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| 404 | </span></span></b><b><span style='font-size:14.0pt'><a name="CylinderModel">CylinderModel</a></span></b></p> |
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| 405 | |
---|
| 406 | <p class=MsoNormal> </p> |
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| 407 | |
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| 408 | <p class=MsoNormal>This model provides the form factor for a monodisperse right |
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| 409 | circular cylinder with uniform scattering length density. The form factor is |
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| 410 | normalized by the particle volume.</p> |
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| 411 | |
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| 412 | <p class=MsoNormal> </p> |
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| 413 | |
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| 414 | <p class=MsoNormal style='margin-left:.85in;text-indent:-.35in'><b>2.2.1.<span |
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| 415 | style='font:7.0pt "Times New Roman"'> </span></b><b>Definition</b></p> |
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| 416 | |
---|
| 417 | <p class=MsoNormal> </p> |
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| 418 | |
---|
| 419 | <p class=MsoNormal>The output of the 2D scattering intensity function for |
---|
| 420 | oriented cylinders is given by (Guinier, 1955):</p> |
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| 421 | |
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| 422 | <p class=MsoNormal align=center style='text-align:center'><sub><img width=184 |
---|
| 423 | height=41 src="../images/html/image006.gif"></sub> (4)</p> |
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| 424 | |
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| 425 | <p class=MsoNormal align=center style='text-align:center'><sub><img width=373 |
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| 426 | height=45 src="../images/html/image007.gif"></sub> (5)</p> |
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| 427 | |
---|
| 428 | <p class=MsoNormal>where <span style='font-family:"Arial","sans-serif"'>α</span> |
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| 429 | is the angle between the axis of the cylinder and the q-vector, V is the volume |
---|
| 430 | of the cylinder, L is the length of the cylinder, r is the radius of the |
---|
| 431 | cylinder, and <i><span style='font-family:"Arial","sans-serif"'>Δ</span>ρ</i> |
---|
| 432 | (contrast) is the scattering length density difference between the scatterer |
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| 433 | and the solvent. J<sub>1</sub> is the first order Bessel function.</p> |
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| 434 | |
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| 435 | <p class=MsoNormal> </p> |
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| 436 | |
---|
| 437 | <p class=MsoNormal>To provide easy access to the orientation of the cylinder, we |
---|
| 438 | define the axis of the cylinder using two angles θ and <span |
---|
| 439 | style='font-family:"Arial","sans-serif"'>φ</span>. Those angles are |
---|
| 440 | defined on Figure 2.</p> |
---|
| 441 | |
---|
| 442 | <p class=MsoNormal align=center style='text-align:center;page-break-after:avoid'><img |
---|
| 443 | width=300 height=281 id="Picture 8" src="../images/html/image008.jpg" |
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| 444 | alt=angles></p> |
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| 445 | |
---|
| 446 | <p class=MsoCaption align=center style='text-align:center'><a |
---|
| 447 | name="_Ref173306040"></a><a name="_Ref173213915">Figure </a>2: Definition of the angles for oriented cylinders.</p> |
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| 448 | |
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| 449 | <p class=MsoNormal> </p> |
---|
| 450 | |
---|
| 451 | |
---|
| 452 | <p class=MsoNormal>The returned value is scaled to units of [cm<sup>-1</sup>] |
---|
| 453 | and the parameters of the cylinder model are the following:</p> |
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| 454 | |
---|
| 455 | <p class=MsoNormal> </p> |
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| 456 | |
---|
| 457 | <div align=center> |
---|
| 458 | |
---|
| 459 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
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| 460 | style='border-collapse:collapse;border:none'> |
---|
| 461 | <tr style='height:19.85pt'> |
---|
| 462 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 463 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 464 | <p class=MsoBodyText>Parameter name</p> |
---|
| 465 | </td> |
---|
| 466 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
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| 467 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 468 | <p class=MsoBodyText>Units</p> |
---|
| 469 | </td> |
---|
| 470 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
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| 471 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 472 | <p class=MsoBodyText>Default value</p> |
---|
| 473 | </td> |
---|
| 474 | </tr> |
---|
| 475 | <tr style='height:19.85pt'> |
---|
| 476 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 477 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 478 | <p class=MsoBodyText>Scale</p> |
---|
| 479 | </td> |
---|
| 480 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 481 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 482 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 483 | <p class=MsoBodyText>None</p> |
---|
| 484 | </td> |
---|
| 485 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 486 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 487 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 488 | <p class=MsoBodyText>1.0</p> |
---|
| 489 | </td> |
---|
| 490 | </tr> |
---|
| 491 | <tr style='height:19.85pt'> |
---|
| 492 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 493 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 494 | <p class=MsoBodyText>Radius</p> |
---|
| 495 | </td> |
---|
| 496 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 497 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 498 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 499 | <p class=MsoBodyText>Å</p> |
---|
| 500 | </td> |
---|
| 501 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 502 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 503 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 504 | <p class=MsoBodyText>20.0</p> |
---|
| 505 | </td> |
---|
| 506 | </tr> |
---|
| 507 | <tr style='height:19.85pt'> |
---|
| 508 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 509 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 510 | <p class=MsoBodyText>Length</p> |
---|
| 511 | </td> |
---|
| 512 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 513 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 514 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 515 | <p class=MsoBodyText>Å</p> |
---|
| 516 | </td> |
---|
| 517 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 518 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 519 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 520 | <p class=MsoBodyText>400.0</p> |
---|
| 521 | </td> |
---|
| 522 | </tr> |
---|
| 523 | <tr style='height:19.85pt'> |
---|
| 524 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 525 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 526 | <p class=MsoBodyText>Contrast</p> |
---|
| 527 | </td> |
---|
| 528 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 529 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 530 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 531 | <p class=MsoBodyText>Å<sup> -2</sup></p> |
---|
| 532 | </td> |
---|
| 533 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 534 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 535 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 536 | <p class=MsoBodyText>3.0e-6</p> |
---|
| 537 | </td> |
---|
| 538 | </tr> |
---|
| 539 | <tr style='height:19.85pt'> |
---|
| 540 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 541 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 542 | <p class=MsoBodyText>Background</p> |
---|
| 543 | </td> |
---|
| 544 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 545 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 546 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 547 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 548 | </td> |
---|
| 549 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 550 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 551 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 552 | <p class=MsoBodyText>0.0</p> |
---|
| 553 | </td> |
---|
| 554 | </tr> |
---|
| 555 | <tr style='height:19.85pt'> |
---|
| 556 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 557 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 558 | <p class=MsoBodyText>Cyl_theta</p> |
---|
| 559 | </td> |
---|
| 560 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 561 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 562 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 563 | <p class=MsoBodyText>Radian</p> |
---|
| 564 | </td> |
---|
| 565 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 566 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 567 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 568 | <p class=MsoBodyText>1.0</p> |
---|
| 569 | </td> |
---|
| 570 | </tr> |
---|
| 571 | <tr style='height:20.6pt'> |
---|
| 572 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 573 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:20.6pt'> |
---|
| 574 | <p class=MsoBodyText>Cyl_phi</p> |
---|
| 575 | </td> |
---|
| 576 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 577 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 578 | padding:0in 5.4pt 0in 5.4pt;height:20.6pt'> |
---|
| 579 | <p class=MsoBodyText>Radian</p> |
---|
| 580 | </td> |
---|
| 581 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 582 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 583 | padding:0in 5.4pt 0in 5.4pt;height:20.6pt'> |
---|
| 584 | <p class=MsoBodyText>1.0</p> |
---|
| 585 | </td> |
---|
| 586 | </tr> |
---|
| 587 | </table> |
---|
| 588 | |
---|
| 589 | </div> |
---|
| 590 | |
---|
| 591 | <p class=MsoNormal> </p> |
---|
| 592 | |
---|
| 593 | <p class=MsoNormal>The output of the 1D scattering intensity function for |
---|
| 594 | randomly oriented cylinders is then given by:</p> |
---|
| 595 | |
---|
| 596 | <p class=MsoNormal align=center style='text-align:center'><a |
---|
| 597 | name="_Ref173306479"></a><a name="_Ref173306528"><sub><img width=253 height=56 |
---|
| 598 | src="../images/html/image009.gif"></sub> (</a>6)</p> |
---|
| 599 | |
---|
| 600 | <p class=MsoNormal> </p> |
---|
| 601 | |
---|
| 602 | <p class=MsoNormal>The <i>cyl_theta</i> and <i>cyl_phi</i> parameter are not |
---|
| 603 | used for the 1D output. Our implementation of the scattering kernel and the 1D |
---|
| 604 | scattering intensity use the c-library from NIST.</p> |
---|
| 605 | |
---|
| 606 | <p class=MsoNormal> </p> |
---|
| 607 | |
---|
| 608 | |
---|
| 609 | <p class=MsoNormal> </p> |
---|
| 610 | |
---|
| 611 | <p class=MsoNormal style='margin-left:.85in;text-indent:-.35in'><b>2.2.2.<span |
---|
| 612 | style='font:7.0pt "Times New Roman"'> </span></b><b>Validation |
---|
| 613 | of the cylinder model</b></p> |
---|
| 614 | |
---|
| 615 | <p class=MsoNormal> </p> |
---|
| 616 | |
---|
| 617 | <p class=MsoNormal>Validation of our code was done by comparing the output of |
---|
| 618 | the 1D model to the output of the software provided by the NIST (Kline, 2006). Figure |
---|
| 619 | 3 shows a comparison of the 1D output of our model and the output of the NIST |
---|
| 620 | software.</p> |
---|
| 621 | |
---|
| 622 | <p class=MsoNormal> </p> |
---|
| 623 | |
---|
| 624 | <p class=MsoNormal>In general, averaging over a distribution of orientations is |
---|
| 625 | done by evaluating the following:</p> |
---|
| 626 | |
---|
| 627 | <p class=MsoNormal align=center style='text-align:center'><sub><img width=244 |
---|
| 628 | height=51 src="../images/html/image010.gif"></sub> (7)</p> |
---|
| 629 | |
---|
| 630 | <p class=MsoNormal>where <i>p(θ,</i><i><span style='font-family:"Arial","sans-serif"'>φ</span>)</i> |
---|
| 631 | is the probability distribution for the orientation and <i>P<sub>0</sub>(q,</i><i><span |
---|
| 632 | style='font-family:"Arial","sans-serif"'>α</span>)</i> is the scattering |
---|
| 633 | intensity for the fully oriented system. Since we have no other software to |
---|
| 634 | compare the implementation of the intensity for fully oriented cylinders, we |
---|
| 635 | can compare the result of averaging our 2D output using a uniform distribution <i>p(θ,</i><i><span |
---|
| 636 | style='font-family:"Arial","sans-serif"'>φ</span>)</i> = 1.0. Figure 4 |
---|
| 637 | shows the result of such a cross-check.</p> |
---|
| 638 | |
---|
| 639 | <p class=MsoNormal> </p> |
---|
| 640 | |
---|
| 641 | <p class=MsoNormal style='page-break-after:avoid'><img width=573 height=315 |
---|
| 642 | id="Picture 11" src="../images/html/image011.jpg" |
---|
| 643 | alt="cylinder_1D_validation"></p> |
---|
| 644 | |
---|
| 645 | <p class=MsoCaption><a name="_Ref173211049"></a><a name="_Ref173211066">Figure </a>3: Comparison of the DANSE scattering intensity for a cylinder with the output of the |
---|
| 646 | NIST SANS analysis software. The parameters were set to: Scale=1.0, Radius=20 Å, |
---|
| 647 | Length=400 Å, Contrast=3e-6 Å<sup> -2</sup>, and Background=0.01 cm<sup> -1</sup>.</p> |
---|
| 648 | |
---|
| 649 | <p class=MsoCaption> </p> |
---|
| 650 | |
---|
| 651 | <p class=MsoNormal style='page-break-after:avoid'><img width=573 height=315 |
---|
| 652 | id="Picture 12" src="../images/html/image012.jpg" |
---|
| 653 | alt="cylinder_2D_average"></p> |
---|
| 654 | |
---|
| 655 | <p class=MsoCaption><a name="_Ref173213305">Figure </a>4: Comparison of the |
---|
| 656 | intensity for uniformly distributed cylinders calculated from our 2D model and |
---|
| 657 | the intensity from the NIST SANS analysis software. The parameters used were: |
---|
| 658 | Scale=1.0, Radius=20 Å, Length=400 Å, Contrast=3e-6 Å<sup> -2</sup>, and |
---|
| 659 | Background=0.0 cm<sup> -1</sup>.</p> |
---|
| 660 | |
---|
| 661 | <p class=MsoCaption> </p> |
---|
| 662 | |
---|
| 663 | <p class=MsoNormal> </p> |
---|
| 664 | |
---|
| 665 | |
---|
| 666 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 667 | style='font-size:14.0pt'>2.3.<span style='font:7.0pt "Times New Roman"'> |
---|
| 668 | </span></span></b><b><span style='font-size:14.0pt'><a name="EllipsoidModel">EllipsoidModel</a></span></b></p> |
---|
| 669 | |
---|
| 670 | <p class=MsoNormal> </p> |
---|
| 671 | |
---|
| 672 | <p class=MsoNormal>This model provides the form factor for a monodisperse |
---|
| 673 | ellipsoid (ellipsoid of revolution) with uniform scattering length density. The |
---|
| 674 | form factor is normalized by the particle volume.</p> |
---|
| 675 | |
---|
| 676 | <p class=MsoNormal> </p> |
---|
| 677 | |
---|
| 678 | <p class=MsoNormal style='margin-left:.85in;text-indent:-.35in'><b>2.3.1.<span |
---|
| 679 | style='font:7.0pt "Times New Roman"'> </span></b><b>Definition</b></p> |
---|
| 680 | |
---|
| 681 | <p class=MsoNormal> </p> |
---|
| 682 | |
---|
| 683 | <p class=MsoNormal>The output of the 2D scattering intensity function for |
---|
| 684 | oriented ellipsoids is given by (Feigin, 1987):</p> |
---|
| 685 | |
---|
| 686 | <p class=MsoCaption align=center style='text-align:center'><sub><img width=184 |
---|
| 687 | height=41 src="../images/html/image006.gif"></sub> <span |
---|
| 688 | style='font-size:12.0pt;font-weight:normal'>(8)</span></p> |
---|
| 689 | |
---|
| 690 | <p class=MsoCaption align=center style='text-align:center'><sub><img width=371 |
---|
| 691 | height=47 src="../images/html/image013.gif"></sub> <span |
---|
| 692 | style='font-size:12.0pt;font-weight:normal'>(9)</span></p> |
---|
| 693 | |
---|
| 694 | <p class=MsoCaption align=center style='text-align:center'><sub><img width=272 |
---|
| 695 | height=29 src="../images/html/image014.gif"></sub> <span |
---|
| 696 | style='font-size:12.0pt;font-weight:normal'>(10)</span></p> |
---|
| 697 | |
---|
| 698 | <p class=MsoNormal>where <span style='font-family:"Arial","sans-serif"'>α</span> |
---|
| 699 | is the angle between the axis of the ellipsoid and the q-vector, V is the |
---|
| 700 | volume of the ellipsoid, R<sub>a</sub> is the radius along the rotation axis of |
---|
| 701 | the ellipsoid, R<sub>b</sub> is the radius perpendicular to the rotation axis of |
---|
| 702 | the ellipsoid and <i><span style='font-family:"Arial","sans-serif"'>Δ</span>ρ</i> |
---|
| 703 | (contrast) is the scattering length density difference between the scatterer |
---|
| 704 | and the solvent. </p> |
---|
| 705 | |
---|
| 706 | <p class=MsoNormal> </p> |
---|
| 707 | |
---|
| 708 | <p class=MsoNormal>To provide easy access to the orientation of the ellipsoid, |
---|
| 709 | we define the rotation axis of the ellipsoid using two angles θ and <span |
---|
| 710 | style='font-family:"Arial","sans-serif"'>φ</span>. Similarly to the case |
---|
| 711 | of the cylinder, those angles are defined on Figure 2. For the ellipsoid, |
---|
| 712 | θ is the angle between the rotation axis and the z-axis. </p> |
---|
| 713 | |
---|
| 714 | <p class=MsoNormal> </p> |
---|
| 715 | |
---|
| 716 | <p class=MsoNormal>The returned value is scaled to units of [cm<sup>-1</sup>] |
---|
| 717 | and the parameters of the ellipsoid model are the following:</p> |
---|
| 718 | |
---|
| 719 | <p class=MsoNormal> </p> |
---|
| 720 | |
---|
| 721 | <div align=center> |
---|
| 722 | |
---|
| 723 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 724 | style='border-collapse:collapse;border:none'> |
---|
| 725 | <tr style='height:19.85pt'> |
---|
| 726 | <td width=180 valign=top style='width:135.1pt;border:solid windowtext 1.0pt; |
---|
| 727 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 728 | <p class=MsoBodyText>Parameter name</p> |
---|
| 729 | </td> |
---|
| 730 | <td width=105 valign=top style='width:78.9pt;border:solid windowtext 1.0pt; |
---|
| 731 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 732 | <p class=MsoBodyText>Units</p> |
---|
| 733 | </td> |
---|
| 734 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 735 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 736 | <p class=MsoBodyText>Default value</p> |
---|
| 737 | </td> |
---|
| 738 | </tr> |
---|
| 739 | <tr style='height:19.85pt'> |
---|
| 740 | <td width=180 valign=top style='width:135.1pt;border:solid windowtext 1.0pt; |
---|
| 741 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 742 | <p class=MsoBodyText>Scale</p> |
---|
| 743 | </td> |
---|
| 744 | <td width=105 valign=top style='width:78.9pt;border-top:none;border-left: |
---|
| 745 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 746 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 747 | <p class=MsoBodyText>None</p> |
---|
| 748 | </td> |
---|
| 749 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 750 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 751 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 752 | <p class=MsoBodyText>1.0</p> |
---|
| 753 | </td> |
---|
| 754 | </tr> |
---|
| 755 | <tr style='height:19.85pt'> |
---|
| 756 | <td width=180 valign=top style='width:135.1pt;border:solid windowtext 1.0pt; |
---|
| 757 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 758 | <p class=MsoBodyText>Radius_a (parallel)</p> |
---|
| 759 | </td> |
---|
| 760 | <td width=105 valign=top style='width:78.9pt;border-top:none;border-left: |
---|
| 761 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 762 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 763 | <p class=MsoBodyText>Å</p> |
---|
| 764 | </td> |
---|
| 765 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 766 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 767 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 768 | <p class=MsoBodyText>20.0</p> |
---|
| 769 | </td> |
---|
| 770 | </tr> |
---|
| 771 | <tr style='height:19.85pt'> |
---|
| 772 | <td width=180 valign=top style='width:135.1pt;border:solid windowtext 1.0pt; |
---|
| 773 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 774 | <p class=MsoBodyText>Radius_b (perpendicular)</p> |
---|
| 775 | </td> |
---|
| 776 | <td width=105 valign=top style='width:78.9pt;border-top:none;border-left: |
---|
| 777 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 778 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 779 | <p class=MsoBodyText>Å</p> |
---|
| 780 | </td> |
---|
| 781 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 782 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 783 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 784 | <p class=MsoBodyText>400.0</p> |
---|
| 785 | </td> |
---|
| 786 | </tr> |
---|
| 787 | <tr style='height:19.85pt'> |
---|
| 788 | <td width=180 valign=top style='width:135.1pt;border:solid windowtext 1.0pt; |
---|
| 789 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 790 | <p class=MsoBodyText>Contrast</p> |
---|
| 791 | </td> |
---|
| 792 | <td width=105 valign=top style='width:78.9pt;border-top:none;border-left: |
---|
| 793 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 794 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 795 | <p class=MsoBodyText>Å<sup> -2</sup></p> |
---|
| 796 | </td> |
---|
| 797 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 798 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 799 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 800 | <p class=MsoBodyText>3.0e-6</p> |
---|
| 801 | </td> |
---|
| 802 | </tr> |
---|
| 803 | <tr style='height:19.85pt'> |
---|
| 804 | <td width=180 valign=top style='width:135.1pt;border:solid windowtext 1.0pt; |
---|
| 805 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 806 | <p class=MsoBodyText>Background</p> |
---|
| 807 | </td> |
---|
| 808 | <td width=105 valign=top style='width:78.9pt;border-top:none;border-left: |
---|
| 809 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 810 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 811 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 812 | </td> |
---|
| 813 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 814 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 815 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 816 | <p class=MsoBodyText>0.0</p> |
---|
| 817 | </td> |
---|
| 818 | </tr> |
---|
| 819 | <tr style='height:19.85pt'> |
---|
| 820 | <td width=180 valign=top style='width:135.1pt;border:solid windowtext 1.0pt; |
---|
| 821 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 822 | <p class=MsoBodyText>Axis_theta</p> |
---|
| 823 | </td> |
---|
| 824 | <td width=105 valign=top style='width:78.9pt;border-top:none;border-left: |
---|
| 825 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 826 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 827 | <p class=MsoBodyText>Radian</p> |
---|
| 828 | </td> |
---|
| 829 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 830 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 831 | padding:0in 5.4pt 0in 5.4pt;height:19.85pt'> |
---|
| 832 | <p class=MsoBodyText>1.57</p> |
---|
| 833 | </td> |
---|
| 834 | </tr> |
---|
| 835 | <tr style='height:20.6pt'> |
---|
| 836 | <td width=180 valign=top style='width:135.1pt;border:solid windowtext 1.0pt; |
---|
| 837 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:20.6pt'> |
---|
| 838 | <p class=MsoBodyText>Axis_phi</p> |
---|
| 839 | </td> |
---|
| 840 | <td width=105 valign=top style='width:78.9pt;border-top:none;border-left: |
---|
| 841 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 842 | padding:0in 5.4pt 0in 5.4pt;height:20.6pt'> |
---|
| 843 | <p class=MsoBodyText>Radian</p> |
---|
| 844 | </td> |
---|
| 845 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 846 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 847 | padding:0in 5.4pt 0in 5.4pt;height:20.6pt'> |
---|
| 848 | <p class=MsoBodyText>0.0</p> |
---|
| 849 | </td> |
---|
| 850 | </tr> |
---|
| 851 | </table> |
---|
| 852 | |
---|
| 853 | </div> |
---|
| 854 | |
---|
| 855 | <p class=MsoNormal> </p> |
---|
| 856 | |
---|
| 857 | <p class=MsoNormal>The output of the 1D scattering intensity function for |
---|
| 858 | randomly oriented ellipsoids is then given by equation 6.</p> |
---|
| 859 | |
---|
| 860 | <p class=MsoNormal> </p> |
---|
| 861 | |
---|
| 862 | <p class=MsoNormal>The <i>axis_theta</i> and axis<i>_phi</i> parameters are not |
---|
| 863 | used for the 1D output. Our implementation of the scattering kernel and the 1D |
---|
| 864 | scattering intensity use the c-library from NIST.</p> |
---|
| 865 | |
---|
| 866 | <p class=MsoNormal> </p> |
---|
| 867 | |
---|
| 868 | |
---|
| 869 | <p class=MsoNormal style='margin-left:.85in;text-indent:-.35in'><b>2.3.2.<span |
---|
| 870 | style='font:7.0pt "Times New Roman"'> </span></b><b>Validation |
---|
| 871 | of the ellipsoid model</b></p> |
---|
| 872 | |
---|
| 873 | <p class=MsoNormal> </p> |
---|
| 874 | |
---|
| 875 | <p class=MsoNormal>Validation of our code was done by comparing the output of |
---|
| 876 | the 1D model to the output of the software provided by the NIST (Kline, 2006). Figure |
---|
| 877 | 5 shows a comparison of the 1D output of our model and the output of the NIST |
---|
| 878 | software.</p> |
---|
| 879 | |
---|
| 880 | <p class=MsoNormal> </p> |
---|
| 881 | |
---|
| 882 | <p class=MsoNormal>Averaging over a distribution of orientation is done by |
---|
| 883 | evaluating equation 7. Since we have no other software to compare the |
---|
| 884 | implementation of the intensity for fully oriented ellipsoids, we can compare |
---|
| 885 | the result of averaging our 2D output using a uniform distribution <i>p(θ,</i><i><span |
---|
| 886 | style='font-family:"Arial","sans-serif"'>φ</span>)</i> = 1.0. Figure 6 shows the result of such a cross-check.</p> |
---|
| 887 | |
---|
| 888 | <p class=MsoNormal align=center style='text-align:center'><b><i><span |
---|
| 889 | style='color:#3366FF'> </span></i></b></p> |
---|
| 890 | |
---|
| 891 | <p class=MsoNormal>The discrepancy above q=0.3 Å<sup> -1</sup> is due to the |
---|
| 892 | way the form factors are calculated in the c-library provided by NIST. A numerical |
---|
| 893 | integration has to be performed to obtain P(q) for randomly oriented particles |
---|
| 894 | (equation 6). The NIST software performs that integration with a 76-point Gaussian |
---|
| 895 | quadrature rule, which will become imprecise at high q where the amplitude |
---|
| 896 | varies quickly as a function of q. The DANSE result shown has been obtained by |
---|
| 897 | summing over 501 equidistant points in <span style='font-family:"Arial","sans-serif"'>α</span>. |
---|
| 898 | Our result was found to be stable over the range of q shown for a number of |
---|
| 899 | points higher than 500.</p> |
---|
| 900 | |
---|
| 901 | <p class=MsoNormal style='page-break-after:avoid'><b><img width=573 height=315 |
---|
| 902 | id="Picture 16" src="../images/html/image015.jpg" |
---|
| 903 | alt="ellipsoid_1D_validation"></b></p> |
---|
| 904 | |
---|
| 905 | <p class=MsoCaption><a name="_Ref173222904">Figure </a>5: Comparison of the |
---|
| 906 | DANSE scattering intensity for an ellipsoid with the output of the NIST SANS |
---|
| 907 | analysis software. The parameters were set to: Scale=1.0, Radius_a=20 Å, Radius_b=400 |
---|
| 908 | Å, </p> |
---|
| 909 | |
---|
| 910 | <p class=MsoCaption>Contrast=3e-6 Å<sup> -2</sup>, and Background=0.01 cm<sup> |
---|
| 911 | -1</sup>.</p> |
---|
| 912 | |
---|
| 913 | <p class=MsoNormal><b> </b></p> |
---|
| 914 | |
---|
| 915 | |
---|
| 916 | <p class=MsoNormal style='page-break-after:avoid'><img width=573 height=315 |
---|
| 917 | id="Picture 17" src="../images/html/image016.jpg" |
---|
| 918 | alt="ellipsoid_2D_average"></p> |
---|
| 919 | |
---|
| 920 | <p class=MsoCaption><a name="_Ref173223004">Figure </a>6: Comparison of the |
---|
| 921 | intensity for uniformly distributed ellipsoids calculated from our 2D model and |
---|
| 922 | the intensity from the NIST SANS analysis software. The parameters used were: |
---|
| 923 | Scale=1.0, Radius_a=20 Å, Radius_b=400 Å, Contrast=3e-6 Å<sup> -2</sup>, and |
---|
| 924 | Background=0.0 cm<sup> -1</sup>.</p> |
---|
| 925 | |
---|
| 926 | <p class=MsoCaption> </p> |
---|
| 927 | |
---|
| 928 | <p class=MsoNormal><b> </b></p> |
---|
| 929 | |
---|
| 930 | <p class=MsoNormal><b> </b></p> |
---|
| 931 | |
---|
| 932 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 933 | style='font-size:14.0pt'>2.4.<span style='font:7.0pt "Times New Roman"'> |
---|
| 934 | </span></span></b><b><span style='font-size:14.0pt'><a name="CoreShellModel">CoreShell(Sphere)Model</a></span></b></p> |
---|
| 935 | |
---|
| 936 | <p class=MsoNormal> </p> |
---|
| 937 | |
---|
| 938 | <p class=MsoNormal>This model provides the form factor, P(<i>q</i>), for a |
---|
| 939 | monodisperse spherical particle with a core-shell structure. The form factor is |
---|
| 940 | normalized by the particle volume.</p> |
---|
| 941 | |
---|
| 942 | <p class=MsoNormal> </p> |
---|
| 943 | |
---|
| 944 | <p class=MsoNormal style='margin-left:.85in;text-indent:-.35in'><b>2.4.1.<span |
---|
| 945 | style='font:7.0pt "Times New Roman"'> </span></b><b>Definition</b></p> |
---|
| 946 | |
---|
| 947 | <p class=MsoNormal> </p> |
---|
| 948 | |
---|
| 949 | <p class=MsoNormal>The 1D scattering intensity is calculated in the following |
---|
| 950 | way (Guinier, 1955):</p> |
---|
| 951 | |
---|
| 952 | <p class=MsoNormal align=right style='text-align:right'><sub><img width=643 |
---|
| 953 | height=55 src="../images/html/image017.gif"></sub> (11)</p> |
---|
| 954 | |
---|
| 955 | <p class=MsoNormal>where <i>scale</i> is a scale factor, <i>V<sub>s</sub></i> |
---|
| 956 | is the volume of the outer shell, <i>V<sub>c</sub></i> is the volume of the |
---|
| 957 | core, <i>r<sub>s</sub></i> is the radius of the shell, <i>r<sub>c</sub></i> is |
---|
| 958 | the radius of the core, <i>ρ<sub>c</sub></i> is the scattering length |
---|
| 959 | density of the core, <i>ρ<sub>s</sub></i> is the scattering length density |
---|
| 960 | of the shell, ρ<sub>solv</sub> is the scattering length density of the |
---|
| 961 | solvent, and <i>bkg</i> is the background level.</p> |
---|
| 962 | |
---|
| 963 | <p class=MsoNormal> </p> |
---|
| 964 | |
---|
| 965 | <p class=MsoNormal>The 2D scattering intensity is the same as P(q) above, |
---|
| 966 | regardless of the orientation of the q vector.</p> |
---|
| 967 | |
---|
| 968 | <p class=MsoNormal> </p> |
---|
| 969 | |
---|
| 970 | <p class=MsoNormal>The returned value is scaled to units of [cm<sup>-1</sup>] |
---|
| 971 | and the parameters of the core-shell sphere model are the following:</p> |
---|
| 972 | |
---|
| 973 | <p class=MsoNormal> </p> |
---|
| 974 | |
---|
| 975 | <div align=center> |
---|
| 976 | |
---|
| 977 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 978 | style='border-collapse:collapse;border:none'> |
---|
| 979 | <tr style='height:18.8pt'> |
---|
| 980 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 981 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 982 | <p class=MsoBodyText>Parameter name</p> |
---|
| 983 | </td> |
---|
| 984 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 985 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 986 | <p class=MsoBodyText>Units</p> |
---|
| 987 | </td> |
---|
| 988 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 989 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 990 | <p class=MsoBodyText>Default value</p> |
---|
| 991 | </td> |
---|
| 992 | </tr> |
---|
| 993 | <tr style='height:18.8pt'> |
---|
| 994 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 995 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 996 | <p class=MsoBodyText>Scale</p> |
---|
| 997 | </td> |
---|
| 998 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 999 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1000 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1001 | <p class=MsoBodyText>None</p> |
---|
| 1002 | </td> |
---|
| 1003 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1004 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1005 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1006 | <p class=MsoBodyText>1.0</p> |
---|
| 1007 | </td> |
---|
| 1008 | </tr> |
---|
| 1009 | <tr style='height:18.8pt'> |
---|
| 1010 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1011 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1012 | <p class=MsoBodyText>Radius</p> |
---|
| 1013 | </td> |
---|
| 1014 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1015 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1016 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1017 | <p class=MsoBodyText>Å</p> |
---|
| 1018 | </td> |
---|
| 1019 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1020 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1021 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1022 | <p class=MsoBodyText>60</p> |
---|
| 1023 | </td> |
---|
| 1024 | </tr> |
---|
| 1025 | <tr style='height:18.8pt'> |
---|
| 1026 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1027 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1028 | <p class=MsoBodyText>Thickness</p> |
---|
| 1029 | </td> |
---|
| 1030 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1031 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1032 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1033 | <p class=MsoBodyText>Å</p> |
---|
| 1034 | </td> |
---|
| 1035 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1036 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1037 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1038 | <p class=MsoBodyText>10</p> |
---|
| 1039 | </td> |
---|
| 1040 | </tr> |
---|
| 1041 | <tr style='height:18.8pt'> |
---|
| 1042 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1043 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1044 | <p class=MsoBodyText>Core_sld</p> |
---|
| 1045 | </td> |
---|
| 1046 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1047 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1048 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1049 | <p class=MsoBodyText>Å<sup> -2</sup></p> |
---|
| 1050 | </td> |
---|
| 1051 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1052 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1053 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1054 | <p class=MsoBodyText>1e-6</p> |
---|
| 1055 | </td> |
---|
| 1056 | </tr> |
---|
| 1057 | <tr style='height:18.8pt'> |
---|
| 1058 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1059 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1060 | <p class=MsoBodyText>Shell_sld</p> |
---|
| 1061 | </td> |
---|
| 1062 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1063 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1064 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1065 | <p class=MsoBodyText>Å<sup> -2</sup></p> |
---|
| 1066 | </td> |
---|
| 1067 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1068 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1069 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1070 | <p class=MsoBodyText>2e-6</p> |
---|
| 1071 | </td> |
---|
| 1072 | </tr> |
---|
| 1073 | <tr style='height:18.8pt'> |
---|
| 1074 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1075 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1076 | <p class=MsoBodyText>Solvent_sld</p> |
---|
| 1077 | </td> |
---|
| 1078 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1079 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1080 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1081 | <p class=MsoBodyText>Å<sup> -2</sup></p> |
---|
| 1082 | </td> |
---|
| 1083 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1084 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1085 | padding:0in 5.4pt 0in 5.4pt;height:18.8pt'> |
---|
| 1086 | <p class=MsoBodyText>3e-6</p> |
---|
| 1087 | </td> |
---|
| 1088 | </tr> |
---|
| 1089 | <tr style='height:19.5pt'> |
---|
| 1090 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1091 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.5pt'> |
---|
| 1092 | <p class=MsoBodyText>Background</p> |
---|
| 1093 | </td> |
---|
| 1094 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1095 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1096 | padding:0in 5.4pt 0in 5.4pt;height:19.5pt'> |
---|
| 1097 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 1098 | </td> |
---|
| 1099 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1100 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1101 | padding:0in 5.4pt 0in 5.4pt;height:19.5pt'> |
---|
| 1102 | <p class=MsoBodyText>0.001</p> |
---|
| 1103 | </td> |
---|
| 1104 | </tr> |
---|
| 1105 | </table> |
---|
| 1106 | |
---|
| 1107 | </div> |
---|
| 1108 | |
---|
| 1109 | <p class=MsoNormal> </p> |
---|
| 1110 | |
---|
| 1111 | <p class=MsoNormal>Our model uses the form factor calculations implemented in a |
---|
| 1112 | c-library provided by the NIST Center for Neutron Research (Kline, 2006).</p> |
---|
| 1113 | |
---|
| 1114 | <p class=MsoNormal> </p> |
---|
| 1115 | |
---|
| 1116 | |
---|
| 1117 | <p class=MsoNormal style='margin-left:.85in;text-indent:-.35in'><b>2.4.2.<span |
---|
| 1118 | style='font:7.0pt "Times New Roman"'> </span></b><b>Validation |
---|
| 1119 | of the core-shell sphere model</b></p> |
---|
| 1120 | |
---|
| 1121 | <p class=MsoNormal> </p> |
---|
| 1122 | |
---|
| 1123 | <p class=MsoNormal>Validation of our code was done by comparing the output of |
---|
| 1124 | the 1D model to the output of the software provided by the NIST (Kline, 2006). |
---|
| 1125 | Figure 1 shows a comparison of the output of our model and the output of the |
---|
| 1126 | NIST software.</p> |
---|
| 1127 | |
---|
| 1128 | <p class=MsoNormal> </p> |
---|
| 1129 | |
---|
| 1130 | <p class=MsoBodyText align=center style='text-align:center;page-break-after: |
---|
| 1131 | avoid'><img width=573 height=315 id="Picture 19" |
---|
| 1132 | src="../images/html/image018.jpg" alt="core_shell_sphere_1D_validation"></p> |
---|
| 1133 | |
---|
| 1134 | <p class=MsoCaption>Figure 7: Comparison of the DANSE scattering intensity for |
---|
| 1135 | a core-shell sphere with the output of the NIST SANS analysis software. The |
---|
| 1136 | parameters were set to: Scale=1.0, Radius=60 Å, Contrast=1e-6 Å<sup> -2</sup>, |
---|
| 1137 | and Background=0.001 cm<sup> -1</sup>.</p> |
---|
| 1138 | |
---|
| 1139 | <p class=MsoBodyText> </p> |
---|
| 1140 | |
---|
| 1141 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 1142 | style='font-size:14.0pt'>2.5.<span style='font:7.0pt "Times New Roman"'> |
---|
| 1143 | </span></span></b><b><span style='font-size:14.0pt'><a name="CoreShellCylinderModel">CoreShellCylinderModel</a></span></b></p> |
---|
| 1144 | |
---|
| 1145 | <p class=MsoNormal> </p> |
---|
| 1146 | |
---|
| 1147 | <p class=MsoNormal>This model provides the form factor for a monodisperse, |
---|
| 1148 | circular cylinder with a core-shell scattering length density profile. The form |
---|
| 1149 | factor is normalized by the particle volume.</p> |
---|
| 1150 | |
---|
| 1151 | <p class=MsoNormal> </p> |
---|
| 1152 | |
---|
| 1153 | <p class=MsoNormal style='margin-left:.85in;text-indent:-.35in'><b>2.5.1.<span |
---|
| 1154 | style='font:7.0pt "Times New Roman"'> </span></b><b>Definition</b></p> |
---|
| 1155 | |
---|
| 1156 | <p class=MsoNormal> </p> |
---|
| 1157 | |
---|
| 1158 | <p class=MsoNormal>The output of the 2D scattering intensity function for |
---|
| 1159 | oriented core-shell cylinders is given by (Kline, 2006):</p> |
---|
| 1160 | |
---|
| 1161 | <p class=MsoNormal align=center style='text-align:center'><sub><img width=184 |
---|
| 1162 | height=45 src="../images/html/image019.gif"></sub> (12)</p> |
---|
| 1163 | |
---|
| 1164 | <p class=MsoNormal align=center style='text-align:center'><sub><img width=476 |
---|
| 1165 | height=93 src="../images/html/image020.gif"></sub> (13)</p> |
---|
| 1166 | |
---|
| 1167 | <p class=MsoNormal>where <span style='font-family:"Arial","sans-serif"'>α</span> |
---|
| 1168 | is the angle between the axis of the cylinder and the q-vector, <i>V<sub>s</sub></i> |
---|
| 1169 | is the volume of the outer shell, <i>V<sub>c</sub></i> is the volume of the |
---|
| 1170 | core, <i>L</i> is the length of the core, <i>r</i> is the radius of the core, <i>t</i> |
---|
| 1171 | is the thickness of the shell, <i>ρ<sub>c</sub></i> is the scattering |
---|
| 1172 | length density of the core, <i>ρ<sub>s</sub></i> is the scattering length |
---|
| 1173 | density of the shell, ρ<sub>solv</sub> is the scattering length density of |
---|
| 1174 | the solvent, and <i>bkg</i> is the background level. The outer radius of the |
---|
| 1175 | shell is given by <i>r+t</i> and the total length of the outer shell is given |
---|
| 1176 | by <i>L+2t</i>. J<sub>1</sub> is the first order Bessel function.</p> |
---|
| 1177 | |
---|
| 1178 | <p class=MsoNormal> </p> |
---|
| 1179 | |
---|
| 1180 | <p class=MsoNormal>To provide easy access to the orientation of the core-shell cylinder, |
---|
| 1181 | we define the axis of the cylinder using two angles θ and <span |
---|
| 1182 | style='font-family:"Arial","sans-serif"'>φ</span>. Similarly to the case |
---|
| 1183 | of the cylinder, those angles are defined on Figure 2.</p> |
---|
| 1184 | |
---|
| 1185 | <p class=MsoNormal> </p> |
---|
| 1186 | |
---|
| 1187 | <p class=MsoNormal>The returned value is scaled to units of [cm<sup>-1</sup>] |
---|
| 1188 | and the parameters of the core-shell cylinder model are the following:</p> |
---|
| 1189 | |
---|
| 1190 | <p class=MsoNormal> </p> |
---|
| 1191 | |
---|
| 1192 | <div align=center> |
---|
| 1193 | |
---|
| 1194 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 1195 | style='border-collapse:collapse;border:none'> |
---|
| 1196 | <tr style='height:19.25pt'> |
---|
| 1197 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1198 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1199 | <p class=MsoBodyText>Parameter name</p> |
---|
| 1200 | </td> |
---|
| 1201 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1202 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1203 | <p class=MsoBodyText>Units</p> |
---|
| 1204 | </td> |
---|
| 1205 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1206 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1207 | <p class=MsoBodyText>Default value</p> |
---|
| 1208 | </td> |
---|
| 1209 | </tr> |
---|
| 1210 | <tr style='height:19.25pt'> |
---|
| 1211 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1212 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1213 | <p class=MsoBodyText>Scale</p> |
---|
| 1214 | </td> |
---|
| 1215 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1216 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1217 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1218 | <p class=MsoBodyText>None</p> |
---|
| 1219 | </td> |
---|
| 1220 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1221 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1222 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1223 | <p class=MsoBodyText>1.0</p> |
---|
| 1224 | </td> |
---|
| 1225 | </tr> |
---|
| 1226 | <tr style='height:19.25pt'> |
---|
| 1227 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1228 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1229 | <p class=MsoBodyText>Radius</p> |
---|
| 1230 | </td> |
---|
| 1231 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1232 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1233 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1234 | <p class=MsoBodyText>Å</p> |
---|
| 1235 | </td> |
---|
| 1236 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1237 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1238 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1239 | <p class=MsoBodyText>20.0</p> |
---|
| 1240 | </td> |
---|
| 1241 | </tr> |
---|
| 1242 | <tr style='height:19.25pt'> |
---|
| 1243 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1244 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1245 | <p class=MsoBodyText>Thickness</p> |
---|
| 1246 | </td> |
---|
| 1247 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1248 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1249 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1250 | <p class=MsoBodyText>Å</p> |
---|
| 1251 | </td> |
---|
| 1252 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1253 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1254 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1255 | <p class=MsoBodyText>10.0</p> |
---|
| 1256 | </td> |
---|
| 1257 | </tr> |
---|
| 1258 | <tr style='height:19.25pt'> |
---|
| 1259 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1260 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1261 | <p class=MsoBodyText>Length</p> |
---|
| 1262 | </td> |
---|
| 1263 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1264 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1265 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1266 | <p class=MsoBodyText>Å</p> |
---|
| 1267 | </td> |
---|
| 1268 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1269 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1270 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1271 | <p class=MsoBodyText>400.0</p> |
---|
| 1272 | </td> |
---|
| 1273 | </tr> |
---|
| 1274 | <tr style='height:19.25pt'> |
---|
| 1275 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1276 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1277 | <p class=MsoBodyText>Core_sld</p> |
---|
| 1278 | </td> |
---|
| 1279 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1280 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1281 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1282 | <p class=MsoBodyText>Å<sup> -2</sup></p> |
---|
| 1283 | </td> |
---|
| 1284 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1285 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1286 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1287 | <p class=MsoBodyText>1e-6</p> |
---|
| 1288 | </td> |
---|
| 1289 | </tr> |
---|
| 1290 | <tr style='height:19.25pt'> |
---|
| 1291 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1292 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1293 | <p class=MsoBodyText>Shell_sld</p> |
---|
| 1294 | </td> |
---|
| 1295 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1296 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1297 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1298 | <p class=MsoBodyText>Å<sup> -2</sup></p> |
---|
| 1299 | </td> |
---|
| 1300 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1301 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1302 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1303 | <p class=MsoBodyText>4e-6</p> |
---|
| 1304 | </td> |
---|
| 1305 | </tr> |
---|
| 1306 | <tr style='height:19.25pt'> |
---|
| 1307 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1308 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1309 | <p class=MsoBodyText>Solvent_sld</p> |
---|
| 1310 | </td> |
---|
| 1311 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1312 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1313 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1314 | <p class=MsoBodyText>Å<sup> -2</sup></p> |
---|
| 1315 | </td> |
---|
| 1316 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1317 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1318 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1319 | <p class=MsoBodyText>1e-6</p> |
---|
| 1320 | </td> |
---|
| 1321 | </tr> |
---|
| 1322 | <tr style='height:19.25pt'> |
---|
| 1323 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1324 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1325 | <p class=MsoBodyText>Background</p> |
---|
| 1326 | </td> |
---|
| 1327 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1328 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1329 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1330 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 1331 | </td> |
---|
| 1332 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1333 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1334 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1335 | <p class=MsoBodyText>0.0</p> |
---|
| 1336 | </td> |
---|
| 1337 | </tr> |
---|
| 1338 | <tr style='height:19.25pt'> |
---|
| 1339 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1340 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1341 | <p class=MsoBodyText>Axis_theta</p> |
---|
| 1342 | </td> |
---|
| 1343 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1344 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1345 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1346 | <p class=MsoBodyText>Radian</p> |
---|
| 1347 | </td> |
---|
| 1348 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1349 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1350 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1351 | <p class=MsoBodyText>1.57</p> |
---|
| 1352 | </td> |
---|
| 1353 | </tr> |
---|
| 1354 | <tr style='height:20.0pt'> |
---|
| 1355 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1356 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:20.0pt'> |
---|
| 1357 | <p class=MsoBodyText>Axis_phi</p> |
---|
| 1358 | </td> |
---|
| 1359 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1360 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1361 | padding:0in 5.4pt 0in 5.4pt;height:20.0pt'> |
---|
| 1362 | <p class=MsoBodyText>Radian</p> |
---|
| 1363 | </td> |
---|
| 1364 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1365 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1366 | padding:0in 5.4pt 0in 5.4pt;height:20.0pt'> |
---|
| 1367 | <p class=MsoBodyText>0.0</p> |
---|
| 1368 | </td> |
---|
| 1369 | </tr> |
---|
| 1370 | </table> |
---|
| 1371 | |
---|
| 1372 | </div> |
---|
| 1373 | |
---|
| 1374 | <p class=MsoNormal> </p> |
---|
| 1375 | |
---|
| 1376 | <p class=MsoNormal>The output of the 1D scattering intensity function for |
---|
| 1377 | randomly oriented cylinders is then given by equation 6.</p> |
---|
| 1378 | |
---|
| 1379 | <p class=MsoNormal> </p> |
---|
| 1380 | |
---|
| 1381 | <p class=MsoNormal>The <i>axis_theta</i> and axis<i>_phi</i> parameters are not |
---|
| 1382 | used for the 1D output. Our implementation of the scattering kernel and the 1D |
---|
| 1383 | scattering intensity use the c-library from NIST.</p> |
---|
| 1384 | |
---|
| 1385 | <p class=MsoNormal> </p> |
---|
| 1386 | |
---|
| 1387 | <p class=MsoNormal style='margin-left:.85in;text-indent:-.35in'><b>2.5.2.<span |
---|
| 1388 | style='font:7.0pt "Times New Roman"'> </span></b><b>Validation |
---|
| 1389 | of the core-shell cylinder model</b></p> |
---|
| 1390 | |
---|
| 1391 | <p class=MsoNormal> </p> |
---|
| 1392 | |
---|
| 1393 | <p class=MsoNormal>Validation of our code was done by comparing the output of |
---|
| 1394 | the 1D model to the output of the software provided by the NIST (Kline, 2006). Figure |
---|
| 1395 | 8 shows a comparison of the 1D output of our model and the output of the NIST |
---|
| 1396 | software.</p> |
---|
| 1397 | |
---|
| 1398 | <p class=MsoNormal> </p> |
---|
| 1399 | |
---|
| 1400 | <p class=MsoNormal>Averaging over a distribution of orientation is done by |
---|
| 1401 | evaluating equation 7. Since we have no other software to compare the |
---|
| 1402 | implementation of the intensity for fully oriented core-shell cylinders, we can |
---|
| 1403 | compare the result of averaging our 2D output using a uniform distribution <i>p(θ,</i><i><span |
---|
| 1404 | style='font-family:"Arial","sans-serif"'>φ</span>)</i> = 1.0. Figure 9 shows the result of such a cross-check.</p> |
---|
| 1405 | |
---|
| 1406 | <p class=MsoNormal style='page-break-after:avoid'><img width=573 height=315 |
---|
| 1407 | id="Picture 22" src="../images/html/image021.jpg" |
---|
| 1408 | alt="core_shell_cylinder_1D_validation"></p> |
---|
| 1409 | |
---|
| 1410 | <p class=MsoCaption><a name="_Ref173307149">Figure </a>8: Comparison of the |
---|
| 1411 | DANSE scattering intensity for a core-shell cylinder with the output of the |
---|
| 1412 | NIST SANS analysis software. The parameters were set to: Scale=1.0, Radius=20 Å, |
---|
| 1413 | Thickness=10 Å, Length=400 Å, Core_sld=1e-6 Å<sup> -2</sup>, Shell_sld=4e-6 Å<sup> |
---|
| 1414 | -2</sup>, Solvent_sld=1e-6 Å<sup> -2</sup>, and Background=0.01 cm<sup> -1</sup>.</p> |
---|
| 1415 | |
---|
| 1416 | <p class=MsoCaption> </p> |
---|
| 1417 | |
---|
| 1418 | <p class=MsoNormal> </p> |
---|
| 1419 | |
---|
| 1420 | <p class=MsoNormal style='page-break-after:avoid'><img width=573 height=315 |
---|
| 1421 | id="Picture 23" src="../images/html/image022.jpg" |
---|
| 1422 | alt="core_shell_cylinder_2D_average"></p> |
---|
| 1423 | |
---|
| 1424 | <p class=MsoCaption><a name="_Ref173307204">Figure </a>9: Comparison of the |
---|
| 1425 | intensity for uniformly distributed core-shell cylinders calculated from our 2D |
---|
| 1426 | model and the intensity from the NIST SANS analysis software. The parameters |
---|
| 1427 | used were: Scale=1.0, Radius=20 Å, Thickness=10 Å, Length=400 Å, Core_sld=1e-6 Å<sup> |
---|
| 1428 | -2</sup>, Shell_sld=4e-6 Å<sup> -2</sup>, Solvent_sld=1e-6 Å<sup> -2</sup>, and |
---|
| 1429 | Background=0.0 cm<sup> -1</sup>.</p> |
---|
| 1430 | |
---|
| 1431 | <p class=MsoNormal> </p> |
---|
| 1432 | <p class=MsoNormal> </p> |
---|
| 1433 | |
---|
| 1434 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 1435 | style='font-size:14.0pt'>2.6.<span style='font:7.0pt "Times New Roman"'> |
---|
| 1436 | </span></span></b><b><span style='font-size:14.0pt'><a name="EllipticalCylinderModel">EllipticalCylinderModel</a></span></b></p> |
---|
| 1437 | |
---|
| 1438 | <p class=MsoNormal> </p> |
---|
| 1439 | |
---|
| 1440 | <p class=MsoNormal>This function calculates the scattering from an oriented |
---|
| 1441 | elliptical cylinder. The angles theta and phi define the orientation of the |
---|
| 1442 | axis of the cylinder. The angle psi is defined as the orientation of the major |
---|
| 1443 | axis of the ellipse with respect to the vector Q. A gaussian poydispersity can |
---|
| 1444 | be added to any (or all) of the orientation angles, and also for the minor |
---|
| 1445 | radius and the ratio of the ellipse radii.</p> |
---|
| 1446 | |
---|
| 1447 | <p class=MsoNormal>The function calculated is:</p> |
---|
| 1448 | |
---|
| 1449 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 1450 | style='position:relative;top:16.0pt'><img width=377 height=46 |
---|
| 1451 | src="../images/html/image023.gif"></span> </p> |
---|
| 1452 | |
---|
| 1453 | <p class=MsoNormal>with the functions:</p> |
---|
| 1454 | |
---|
| 1455 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 1456 | style='position:relative;top:39.0pt'><img width=297 height=114 |
---|
| 1457 | src="../images/html/image024.gif"></span> (13)</p> |
---|
| 1458 | |
---|
| 1459 | <p class=MsoNormal>and the angle psi is defined as the orientation of the major |
---|
| 1460 | axis of the ellipse with respect to the vector Q.</p> |
---|
| 1461 | |
---|
| 1462 | <p class=MsoNormal> </p> |
---|
| 1463 | |
---|
| 1464 | <p class=MsoNormal>The returned value is scaled to units of [cm<sup>-1</sup>] |
---|
| 1465 | and the parameters are the following:</p> |
---|
| 1466 | |
---|
| 1467 | <p class=MsoNormal> </p> |
---|
| 1468 | |
---|
| 1469 | <div align=center> |
---|
| 1470 | |
---|
| 1471 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 1472 | style='border-collapse:collapse;border:none'> |
---|
| 1473 | <tr style='height:19.25pt'> |
---|
| 1474 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1475 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1476 | <p class=MsoBodyText>Parameter name</p> |
---|
| 1477 | </td> |
---|
| 1478 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1479 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1480 | <p class=MsoBodyText>Units</p> |
---|
| 1481 | </td> |
---|
| 1482 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1483 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1484 | <p class=MsoBodyText>Default value</p> |
---|
| 1485 | </td> |
---|
| 1486 | </tr> |
---|
| 1487 | <tr style='height:19.25pt'> |
---|
| 1488 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1489 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1490 | <p class=MsoBodyText>scale</p> |
---|
| 1491 | </td> |
---|
| 1492 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1493 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1494 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1495 | <p class=MsoBodyText>None</p> |
---|
| 1496 | </td> |
---|
| 1497 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1498 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1499 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1500 | <p class=MsoBodyText>1.0</p> |
---|
| 1501 | </td> |
---|
| 1502 | </tr> |
---|
| 1503 | <tr style='height:19.25pt'> |
---|
| 1504 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1505 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1506 | <p class=MsoBodyText>r_minor</p> |
---|
| 1507 | </td> |
---|
| 1508 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1509 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1510 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1511 | <p class=MsoBodyText>Å</p> |
---|
| 1512 | </td> |
---|
| 1513 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1514 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1515 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1516 | <p class=MsoBodyText>20.0</p> |
---|
| 1517 | </td> |
---|
| 1518 | </tr> |
---|
| 1519 | <tr style='height:19.25pt'> |
---|
| 1520 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1521 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1522 | <p class=MsoBodyText>r_ratio</p> |
---|
| 1523 | </td> |
---|
| 1524 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1525 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1526 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1527 | <p class=MsoBodyText>Å</p> |
---|
| 1528 | </td> |
---|
| 1529 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1530 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1531 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1532 | <p class=MsoBodyText>1.5</p> |
---|
| 1533 | </td> |
---|
| 1534 | </tr> |
---|
| 1535 | <tr style='height:19.25pt'> |
---|
| 1536 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1537 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1538 | <p class=MsoBodyText>length</p> |
---|
| 1539 | </td> |
---|
| 1540 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1541 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1542 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1543 | <p class=MsoBodyText>Å</p> |
---|
| 1544 | </td> |
---|
| 1545 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1546 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1547 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1548 | <p class=MsoBodyText>400.0</p> |
---|
| 1549 | </td> |
---|
| 1550 | </tr> |
---|
| 1551 | <tr style='height:19.25pt'> |
---|
| 1552 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1553 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1554 | <p class=MsoBodyText>contrast</p> |
---|
| 1555 | </td> |
---|
| 1556 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1557 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1558 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1559 | <p class=MsoBodyText>Å<sup> -2</sup></p> |
---|
| 1560 | </td> |
---|
| 1561 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1562 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1563 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1564 | <p class=MsoBodyText>3e-6</p> |
---|
| 1565 | </td> |
---|
| 1566 | </tr> |
---|
| 1567 | <tr style='height:19.25pt'> |
---|
| 1568 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1569 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1570 | <p class=MsoBodyText>cyl_phi</p> |
---|
| 1571 | </td> |
---|
| 1572 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1573 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1574 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1575 | <p class=MsoBodyText>Å<sup> -2</sup></p> |
---|
| 1576 | </td> |
---|
| 1577 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1578 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1579 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1580 | <p class=MsoBodyText>0</p> |
---|
| 1581 | </td> |
---|
| 1582 | </tr> |
---|
| 1583 | <tr style='height:19.25pt'> |
---|
| 1584 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1585 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1586 | <p class=MsoBodyText>cyl_psi</p> |
---|
| 1587 | </td> |
---|
| 1588 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1589 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1590 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1591 | <p class=MsoBodyText>Å<sup> -2</sup></p> |
---|
| 1592 | </td> |
---|
| 1593 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1594 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1595 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1596 | <p class=MsoBodyText>0</p> |
---|
| 1597 | </td> |
---|
| 1598 | </tr> |
---|
| 1599 | <tr style='height:19.25pt'> |
---|
| 1600 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1601 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1602 | <p class=MsoBodyText>cyl_theta</p> |
---|
| 1603 | </td> |
---|
| 1604 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1605 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1606 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1607 | <p class=MsoBodyText>radian</p> |
---|
| 1608 | </td> |
---|
| 1609 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1610 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1611 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1612 | <p class=MsoBodyText>1.57</p> |
---|
| 1613 | </td> |
---|
| 1614 | </tr> |
---|
| 1615 | <tr style='height:19.25pt'> |
---|
| 1616 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1617 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1618 | <p class=MsoBodyText>background</p> |
---|
| 1619 | </td> |
---|
| 1620 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1621 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1622 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1623 | <p class=MsoBodyText> </p> |
---|
| 1624 | </td> |
---|
| 1625 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1626 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1627 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1628 | <p class=MsoBodyText>0</p> |
---|
| 1629 | </td> |
---|
| 1630 | </tr> |
---|
| 1631 | </table> |
---|
| 1632 | |
---|
| 1633 | </div> |
---|
| 1634 | |
---|
| 1635 | <p class=MsoNormal> </p> |
---|
| 1636 | |
---|
| 1637 | <p class=MsoNormal>REFERENCE</p> |
---|
| 1638 | |
---|
| 1639 | <p class=MsoNormal> </p> |
---|
| 1640 | |
---|
| 1641 | <p class=MsoNormal style='text-indent:.25in'>L. A. Feigin and D. I. Svergun |
---|
| 1642 | Structure Analysis by Small-Angle X-Ray and Neutron Scattering, Plenum, New |
---|
| 1643 | York, (1987).</p> |
---|
| 1644 | |
---|
| 1645 | <p class=MsoNormal> </p> |
---|
| 1646 | |
---|
| 1647 | <p class=MsoNormal style='margin-left:.25in;text-indent:-.25in'><b><span |
---|
| 1648 | style='font-size:14.0pt'>3.<span style='font:7.0pt "Times New Roman"'> |
---|
| 1649 | </span></span></b><b><span style='font-size:14.0pt'><a name="Shape-Independent">Shape-Independent</a></span></b></p> |
---|
| 1650 | |
---|
| 1651 | <p class=MsoBodyText> </p> |
---|
| 1652 | |
---|
| 1653 | <p class=MsoBodyText>The following are models used for shape-independent SANS |
---|
| 1654 | analysis.</p> |
---|
| 1655 | |
---|
| 1656 | <p class=MsoBodyText> </p> |
---|
| 1657 | |
---|
| 1658 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 1659 | style='font-size:14.0pt'>3.1.<span style='font:7.0pt "Times New Roman"'> |
---|
| 1660 | </span></span></b><b><span style='font-size:14.0pt'> <a name="Debye">Debye (Model)</a></span></b></p> |
---|
| 1661 | |
---|
| 1662 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 1663 | |
---|
| 1664 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'>The Debye |
---|
| 1665 | model is a form factor for a linear polymer chain. In addition to the radius of |
---|
| 1666 | gyration, Rg, a scale factor "scale", and a constant background term |
---|
| 1667 | are included in the calculation. </p> |
---|
| 1668 | |
---|
| 1669 | <p class=MsoNormal><span style='font-size:14.0pt'> </span></p> |
---|
| 1670 | |
---|
| 1671 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 1672 | style='font-size:14.0pt'><sub><img width=188 height=76 |
---|
| 1673 | src="../images/html/image025.gif"></sub></span></p> |
---|
| 1674 | |
---|
| 1675 | <p class=MsoNormal><span style='font-size:14.0pt'> </span></p> |
---|
| 1676 | |
---|
| 1677 | <div align=center> |
---|
| 1678 | |
---|
| 1679 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 1680 | style='border-collapse:collapse;border:none'> |
---|
| 1681 | <tr style='height:19.25pt'> |
---|
| 1682 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1683 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1684 | <p class=MsoBodyText>Parameter name</p> |
---|
| 1685 | </td> |
---|
| 1686 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1687 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1688 | <p class=MsoBodyText>Units</p> |
---|
| 1689 | </td> |
---|
| 1690 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1691 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1692 | <p class=MsoBodyText>Default value</p> |
---|
| 1693 | </td> |
---|
| 1694 | </tr> |
---|
| 1695 | <tr style='height:19.25pt'> |
---|
| 1696 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1697 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1698 | <p class=MsoBodyText>Scale</p> |
---|
| 1699 | </td> |
---|
| 1700 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1701 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1702 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1703 | <p class=MsoBodyText>None</p> |
---|
| 1704 | </td> |
---|
| 1705 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1706 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1707 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1708 | <p class=MsoBodyText>1.0</p> |
---|
| 1709 | </td> |
---|
| 1710 | </tr> |
---|
| 1711 | <tr style='height:19.25pt'> |
---|
| 1712 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1713 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1714 | <p class=MsoBodyText>Rg</p> |
---|
| 1715 | </td> |
---|
| 1716 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1717 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1718 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1719 | <p class=MsoBodyText>Å</p> |
---|
| 1720 | </td> |
---|
| 1721 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1722 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1723 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1724 | <p class=MsoBodyText>50.0</p> |
---|
| 1725 | </td> |
---|
| 1726 | </tr> |
---|
| 1727 | <tr style='height:19.25pt'> |
---|
| 1728 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1729 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1730 | <p class=MsoBodyText>Background</p> |
---|
| 1731 | </td> |
---|
| 1732 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1733 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1734 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1735 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 1736 | </td> |
---|
| 1737 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1738 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1739 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1740 | <p class=MsoBodyText>0.0</p> |
---|
| 1741 | </td> |
---|
| 1742 | </tr> |
---|
| 1743 | </table> |
---|
| 1744 | |
---|
| 1745 | </div> |
---|
| 1746 | |
---|
| 1747 | <p class=MsoNormal style='margin-left:.25in'> </p> |
---|
| 1748 | |
---|
| 1749 | <p class=MsoNormal style='margin-left:.25in'>Reference: Roe, R.-J., |
---|
| 1750 | "Methods of X-Ray and Neutron Scattering in Polymer Science", Oxford University Press, New York (2000).</p> |
---|
| 1751 | |
---|
| 1752 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 1753 | |
---|
| 1754 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 1755 | style='font-size:14.0pt'>3.2.<span style='font:7.0pt "Times New Roman"'> |
---|
| 1756 | </span></span></b><b><span style='font-size:14.0pt'> <a name="Lorentz">(Ornstein-Zernicke) |
---|
| 1757 | Lorentz (Model)</span></b></p> |
---|
| 1758 | |
---|
| 1759 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 1760 | |
---|
| 1761 | <p class=MsoNormal style='text-indent:.25in'>The Ornstein-Zernicke model is |
---|
| 1762 | defined by:</p> |
---|
| 1763 | |
---|
| 1764 | <p class=MsoNormal><span style='font-size:14.0pt'> </span></p> |
---|
| 1765 | |
---|
| 1766 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 1767 | style='font-size:14.0pt'><sub><img width=212 height=24 |
---|
| 1768 | src="../images/html/image026.gif"></sub></span></p> |
---|
| 1769 | |
---|
| 1770 | <p class=MsoNormal><span style='font-size:14.0pt'> </span></p> |
---|
| 1771 | |
---|
| 1772 | <p class=MsoNormal style='text-indent:.25in'>The parameter L is referred to as |
---|
| 1773 | the screening length.</p> |
---|
| 1774 | |
---|
| 1775 | <p class=MsoNormal><span style='font-size:14.0pt'> </span></p> |
---|
| 1776 | |
---|
| 1777 | <div align=center> |
---|
| 1778 | |
---|
| 1779 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 1780 | style='border-collapse:collapse;border:none'> |
---|
| 1781 | <tr style='height:19.25pt'> |
---|
| 1782 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1783 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1784 | <p class=MsoBodyText>Parameter name</p> |
---|
| 1785 | </td> |
---|
| 1786 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1787 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1788 | <p class=MsoBodyText>Units</p> |
---|
| 1789 | </td> |
---|
| 1790 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1791 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1792 | <p class=MsoBodyText>Default value</p> |
---|
| 1793 | </td> |
---|
| 1794 | </tr> |
---|
| 1795 | <tr style='height:19.25pt'> |
---|
| 1796 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1797 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1798 | <p class=MsoBodyText>Scale</p> |
---|
| 1799 | </td> |
---|
| 1800 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1801 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1802 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1803 | <p class=MsoBodyText>None</p> |
---|
| 1804 | </td> |
---|
| 1805 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1806 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1807 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1808 | <p class=MsoBodyText>1.0</p> |
---|
| 1809 | </td> |
---|
| 1810 | </tr> |
---|
| 1811 | <tr style='height:19.25pt'> |
---|
| 1812 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1813 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1814 | <p class=MsoBodyText>Length</p> |
---|
| 1815 | </td> |
---|
| 1816 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1817 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1818 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1819 | <p class=MsoBodyText>Å</p> |
---|
| 1820 | </td> |
---|
| 1821 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1822 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1823 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1824 | <p class=MsoBodyText>50.0</p> |
---|
| 1825 | </td> |
---|
| 1826 | </tr> |
---|
| 1827 | <tr style='height:19.25pt'> |
---|
| 1828 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1829 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1830 | <p class=MsoBodyText>Background</p> |
---|
| 1831 | </td> |
---|
| 1832 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1833 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1834 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1835 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 1836 | </td> |
---|
| 1837 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1838 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1839 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1840 | <p class=MsoBodyText>0.0</p> |
---|
| 1841 | </td> |
---|
| 1842 | </tr> |
---|
| 1843 | </table> |
---|
| 1844 | |
---|
| 1845 | </div> |
---|
| 1846 | |
---|
| 1847 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 1848 | |
---|
| 1849 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 1850 | |
---|
| 1851 | |
---|
| 1852 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 1853 | style='font-size:14.0pt'>3.3.<span style='font:7.0pt "Times New Roman"'> |
---|
| 1854 | </span></span></b><b><span style='font-size:14.0pt'> <a name="DAB_Model">DAB(Debye-Anderson-Brumberger)_ |
---|
| 1855 | Model)</a></span></b></p> |
---|
| 1856 | |
---|
| 1857 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'>Calculates the |
---|
| 1858 | scattering from a randomly distributed, two-phase system based on the |
---|
| 1859 | Debye-Anderson-Brumberger (DAB) model for such systems. The two-phase system is |
---|
| 1860 | characterized by a single length scale, the correlation length, which is a |
---|
| 1861 | measure of the average spacing between regions of phase 1 and phase 2. The |
---|
| 1862 | model also assumes smooth interfaces between the phases and hence exhibits |
---|
| 1863 | Porod behavior (I ~ Q<sup>-4</sup>) at large Q (Q*correlation length >> |
---|
| 1864 | 1). </p> |
---|
| 1865 | |
---|
| 1866 | <p class=MsoNormal style='text-indent:.25in'> </p> |
---|
| 1867 | |
---|
| 1868 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 1869 | style='font-size:14.0pt'><sub><img width=221 height=28 |
---|
| 1870 | src="../images/html/image027.gif"></sub></span></p> |
---|
| 1871 | |
---|
| 1872 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 1873 | style='font-size:14.0pt'> </span></p> |
---|
| 1874 | |
---|
| 1875 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'>The parameter |
---|
| 1876 | L is referred to as the correlation length.</p> |
---|
| 1877 | |
---|
| 1878 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 1879 | style='font-size:14.0pt'> </span></p> |
---|
| 1880 | |
---|
| 1881 | <div align=center> |
---|
| 1882 | |
---|
| 1883 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 1884 | style='border-collapse:collapse;border:none'> |
---|
| 1885 | <tr style='height:19.25pt'> |
---|
| 1886 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1887 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1888 | <p class=MsoBodyText>Parameter name</p> |
---|
| 1889 | </td> |
---|
| 1890 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1891 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1892 | <p class=MsoBodyText>Units</p> |
---|
| 1893 | </td> |
---|
| 1894 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1895 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1896 | <p class=MsoBodyText>Default value</p> |
---|
| 1897 | </td> |
---|
| 1898 | </tr> |
---|
| 1899 | <tr style='height:19.25pt'> |
---|
| 1900 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1901 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1902 | <p class=MsoBodyText>Scale</p> |
---|
| 1903 | </td> |
---|
| 1904 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1905 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1906 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1907 | <p class=MsoBodyText>None</p> |
---|
| 1908 | </td> |
---|
| 1909 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1910 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1911 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1912 | <p class=MsoBodyText>1.0</p> |
---|
| 1913 | </td> |
---|
| 1914 | </tr> |
---|
| 1915 | <tr style='height:19.25pt'> |
---|
| 1916 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1917 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1918 | <p class=MsoBodyText>Length</p> |
---|
| 1919 | </td> |
---|
| 1920 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1921 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1922 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1923 | <p class=MsoBodyText>Å</p> |
---|
| 1924 | </td> |
---|
| 1925 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1926 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1927 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1928 | <p class=MsoBodyText>50.0</p> |
---|
| 1929 | </td> |
---|
| 1930 | </tr> |
---|
| 1931 | <tr style='height:19.25pt'> |
---|
| 1932 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1933 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1934 | <p class=MsoBodyText>Background</p> |
---|
| 1935 | </td> |
---|
| 1936 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1937 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1938 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1939 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 1940 | </td> |
---|
| 1941 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 1942 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 1943 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1944 | <p class=MsoBodyText>0.0</p> |
---|
| 1945 | </td> |
---|
| 1946 | </tr> |
---|
| 1947 | </table> |
---|
| 1948 | |
---|
| 1949 | </div> |
---|
| 1950 | |
---|
| 1951 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 1952 | |
---|
| 1953 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'>References: </p> |
---|
| 1954 | |
---|
| 1955 | <p class=MsoNormal style='margin-left:.5in'>Debye, Anderson, Brumberger, |
---|
| 1956 | "Scattering by an Inhomogeneous Solid. II. The Correlation Function and |
---|
| 1957 | its Application", J. Appl. Phys. 28 (6), 679 (1957).</p> |
---|
| 1958 | |
---|
| 1959 | <p class=MsoNormal style='margin-left:.5in'> </p> |
---|
| 1960 | |
---|
| 1961 | <p class=MsoNormal style='margin-left:.5in'>Debye, Bueche, "Scattering by |
---|
| 1962 | an Inhomogeneous Solid", J. Appl. Phys. 20, 518 (1949).</p> |
---|
| 1963 | |
---|
| 1964 | <p class=MsoNormal> </p> |
---|
| 1965 | |
---|
| 1966 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 1967 | |
---|
| 1968 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 1969 | style='font-size:14.0pt'>3.4.<span style='font:7.0pt "Times New Roman"'> |
---|
| 1970 | </span></span></b><b><span style='font-size:14.0pt'> <a name="Power_Law">Power_Law</a></span></b></p> |
---|
| 1971 | |
---|
| 1972 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 1973 | |
---|
| 1974 | <p class=MsoNormal style='margin-left:.25in'>This model describes a power law |
---|
| 1975 | with background.</p> |
---|
| 1976 | |
---|
| 1977 | <p class=MsoNormal style='margin-left:.25in'><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 1978 | |
---|
| 1979 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 1980 | style='font-size:14.0pt'><sub><img width=161 height=24 |
---|
| 1981 | src="../images/html/image028.gif"></sub></span></p> |
---|
| 1982 | |
---|
| 1983 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 1984 | style='font-size:14.0pt'> </span></p> |
---|
| 1985 | |
---|
| 1986 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'>Note the minus |
---|
| 1987 | sign in front of the exponent.</p> |
---|
| 1988 | |
---|
| 1989 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 1990 | style='font-size:14.0pt'> </span></p> |
---|
| 1991 | |
---|
| 1992 | <div align=center> |
---|
| 1993 | |
---|
| 1994 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 1995 | style='border-collapse:collapse;border:none'> |
---|
| 1996 | <tr style='height:19.25pt'> |
---|
| 1997 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 1998 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 1999 | <p class=MsoBodyText>Parameter name</p> |
---|
| 2000 | </td> |
---|
| 2001 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2002 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2003 | <p class=MsoBodyText>Units</p> |
---|
| 2004 | </td> |
---|
| 2005 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2006 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2007 | <p class=MsoBodyText>Default value</p> |
---|
| 2008 | </td> |
---|
| 2009 | </tr> |
---|
| 2010 | <tr style='height:19.25pt'> |
---|
| 2011 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2012 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2013 | <p class=MsoBodyText>Scale</p> |
---|
| 2014 | </td> |
---|
| 2015 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2016 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2017 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2018 | <p class=MsoBodyText>None</p> |
---|
| 2019 | </td> |
---|
| 2020 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2021 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2022 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2023 | <p class=MsoBodyText>1.0</p> |
---|
| 2024 | </td> |
---|
| 2025 | </tr> |
---|
| 2026 | <tr style='height:19.25pt'> |
---|
| 2027 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2028 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2029 | <p class=MsoBodyText>m</p> |
---|
| 2030 | </td> |
---|
| 2031 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2032 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2033 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2034 | <p class=MsoBodyText>None</p> |
---|
| 2035 | </td> |
---|
| 2036 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2037 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2038 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2039 | <p class=MsoBodyText>4</p> |
---|
| 2040 | </td> |
---|
| 2041 | </tr> |
---|
| 2042 | <tr style='height:19.25pt'> |
---|
| 2043 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2044 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2045 | <p class=MsoBodyText>Background</p> |
---|
| 2046 | </td> |
---|
| 2047 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2048 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2049 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2050 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 2051 | </td> |
---|
| 2052 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2053 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2054 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2055 | <p class=MsoBodyText>0.0</p> |
---|
| 2056 | </td> |
---|
| 2057 | </tr> |
---|
| 2058 | </table> |
---|
| 2059 | |
---|
| 2060 | </div> |
---|
| 2061 | |
---|
| 2062 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2063 | |
---|
| 2064 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2065 | |
---|
| 2066 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 2067 | style='font-size:14.0pt'>3.5.<span style='font:7.0pt "Times New Roman"'> |
---|
| 2068 | </span></span></b><b><span style='font-size:14.0pt'><a name="Teubner Strey"> Teubner Strey (Model) </a></span></b></p> |
---|
| 2069 | |
---|
| 2070 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2071 | |
---|
| 2072 | <p class=MsoNormal style='margin-left:.25in'>This function calculates the |
---|
| 2073 | scattered intensity of a two-component system using the Teubner-Strey model.</p> |
---|
| 2074 | |
---|
| 2075 | <p class=MsoNormal style='margin-left:.25in'><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2076 | |
---|
| 2077 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 2078 | style='font-size:14.0pt'><sub><img width=213 height=45 |
---|
| 2079 | src="../images/html/image029.gif"></sub></span></p> |
---|
| 2080 | |
---|
| 2081 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 2082 | style='font-size:14.0pt'> </span></p> |
---|
| 2083 | |
---|
| 2084 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 2085 | style='font-size:14.0pt'> </span></p> |
---|
| 2086 | |
---|
| 2087 | <div align=center> |
---|
| 2088 | |
---|
| 2089 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 2090 | style='border-collapse:collapse;border:none'> |
---|
| 2091 | <tr style='height:19.25pt'> |
---|
| 2092 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2093 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2094 | <p class=MsoBodyText>Parameter name</p> |
---|
| 2095 | </td> |
---|
| 2096 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2097 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2098 | <p class=MsoBodyText>Units</p> |
---|
| 2099 | </td> |
---|
| 2100 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2101 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2102 | <p class=MsoBodyText>Default value</p> |
---|
| 2103 | </td> |
---|
| 2104 | </tr> |
---|
| 2105 | <tr style='height:19.25pt'> |
---|
| 2106 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2107 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2108 | <p class=MsoBodyText>A</p> |
---|
| 2109 | </td> |
---|
| 2110 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2111 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2112 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2113 | <p class=MsoBodyText>None</p> |
---|
| 2114 | </td> |
---|
| 2115 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2116 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2117 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2118 | <p class=MsoBodyText>0.1</p> |
---|
| 2119 | </td> |
---|
| 2120 | </tr> |
---|
| 2121 | <tr style='height:19.25pt'> |
---|
| 2122 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2123 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2124 | <p class=MsoBodyText>C1</p> |
---|
| 2125 | </td> |
---|
| 2126 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2127 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2128 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2129 | <p class=MsoBodyText>None</p> |
---|
| 2130 | </td> |
---|
| 2131 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2132 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2133 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2134 | <p class=MsoBodyText>-30.0</p> |
---|
| 2135 | </td> |
---|
| 2136 | </tr> |
---|
| 2137 | <tr style='height:19.25pt'> |
---|
| 2138 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2139 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2140 | <p class=MsoBodyText>C2</p> |
---|
| 2141 | </td> |
---|
| 2142 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2143 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2144 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2145 | <p class=MsoBodyText>None</p> |
---|
| 2146 | </td> |
---|
| 2147 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2148 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2149 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2150 | <p class=MsoBodyText>5000.0</p> |
---|
| 2151 | </td> |
---|
| 2152 | </tr> |
---|
| 2153 | <tr style='height:19.25pt'> |
---|
| 2154 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2155 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2156 | <p class=MsoBodyText>Background</p> |
---|
| 2157 | </td> |
---|
| 2158 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2159 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2160 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2161 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 2162 | </td> |
---|
| 2163 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2164 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2165 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2166 | <p class=MsoBodyText>0.0</p> |
---|
| 2167 | </td> |
---|
| 2168 | </tr> |
---|
| 2169 | </table> |
---|
| 2170 | |
---|
| 2171 | </div> |
---|
| 2172 | |
---|
| 2173 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2174 | |
---|
| 2175 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'>References: </p> |
---|
| 2176 | |
---|
| 2177 | <p class=MsoNormal style='margin-left:.5in'>Teubner, M; Strey, R. J. Chem. |
---|
| 2178 | Phys., 87, 3195 (1987).</p> |
---|
| 2179 | |
---|
| 2180 | <p class=MsoNormal style='margin-left:.5in'> </p> |
---|
| 2181 | |
---|
| 2182 | <p class=MsoNormal style='margin-left:.5in'>Schubert, K-V., Strey, R., Kline, |
---|
| 2183 | S. R. and E. W. Kaler, J. Chem. Phys., 101, 5343 (1994).</p> |
---|
| 2184 | |
---|
| 2185 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2186 | |
---|
| 2187 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2188 | |
---|
| 2189 | |
---|
| 2190 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 2191 | style='font-size:14.0pt'>3.6.<span style='font:7.0pt "Times New Roman"'> |
---|
| 2192 | </span></span></b><b><span style='font-size:14.0pt'><a name="Number Density Fractal"> Number Density Fractal (Model)</a></span></b></p> |
---|
| 2193 | |
---|
| 2194 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2195 | |
---|
| 2196 | <p class=MsoNormal style='margin-left:.25in'>Calculates the scattering from |
---|
| 2197 | fractal-like aggregates built from spherical building blocks following the |
---|
| 2198 | Texiera reference. The value returned is in cm<sup>-1</sup>.</p> |
---|
| 2199 | |
---|
| 2200 | <p class=MsoNormal style='margin-left:.25in'> </p> |
---|
| 2201 | |
---|
| 2202 | |
---|
| 2203 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 2204 | style='font-size:14.0pt'><sub><img width=380 height=188 |
---|
| 2205 | src="../images/html/image030.gif"></sub></span></p> |
---|
| 2206 | |
---|
| 2207 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2208 | |
---|
| 2209 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'>The scale |
---|
| 2210 | parameter is the volume fraction of the building blocks, R<sub>0</sub> is the |
---|
| 2211 | radius of the building block, D<sub>f</sub> is the fractal dimension, ξ is |
---|
| 2212 | the correlation length, <i>ρ<sub>solvent</sub></i> is the scattering |
---|
| 2213 | length density of the solvent, and <i>ρ<sub>block</sub></i> is the |
---|
| 2214 | scattering length density of the building blocks. </p> |
---|
| 2215 | |
---|
| 2216 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'> </p> |
---|
| 2217 | |
---|
| 2218 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 2219 | style='font-size:14.0pt'> </span></p> |
---|
| 2220 | |
---|
| 2221 | <div align=center> |
---|
| 2222 | |
---|
| 2223 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 2224 | style='border-collapse:collapse;border:none'> |
---|
| 2225 | <tr style='height:19.25pt'> |
---|
| 2226 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2227 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2228 | <p class=MsoBodyText>Parameter name</p> |
---|
| 2229 | </td> |
---|
| 2230 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2231 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2232 | <p class=MsoBodyText>Units</p> |
---|
| 2233 | </td> |
---|
| 2234 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2235 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2236 | <p class=MsoBodyText>Default value</p> |
---|
| 2237 | </td> |
---|
| 2238 | </tr> |
---|
| 2239 | <tr style='height:19.25pt'> |
---|
| 2240 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2241 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2242 | <p class=MsoBodyText>Scale</p> |
---|
| 2243 | </td> |
---|
| 2244 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2245 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2246 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2247 | <p class=MsoBodyText>None</p> |
---|
| 2248 | </td> |
---|
| 2249 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2250 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2251 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2252 | <p class=MsoBodyText>0.05</p> |
---|
| 2253 | </td> |
---|
| 2254 | </tr> |
---|
| 2255 | <tr style='height:19.25pt'> |
---|
| 2256 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2257 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2258 | <p class=MsoBodyText>Radius</p> |
---|
| 2259 | </td> |
---|
| 2260 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2261 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2262 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2263 | <p class=MsoBodyText>Å</p> |
---|
| 2264 | </td> |
---|
| 2265 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2266 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2267 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2268 | <p class=MsoBodyText>5.0</p> |
---|
| 2269 | </td> |
---|
| 2270 | </tr> |
---|
| 2271 | <tr style='height:19.25pt'> |
---|
| 2272 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2273 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2274 | <p class=MsoBodyText>Fractal_dim</p> |
---|
| 2275 | </td> |
---|
| 2276 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2277 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2278 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2279 | <p class=MsoBodyText>None</p> |
---|
| 2280 | </td> |
---|
| 2281 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2282 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2283 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2284 | <p class=MsoBodyText>2</p> |
---|
| 2285 | </td> |
---|
| 2286 | </tr> |
---|
| 2287 | <tr style='height:19.25pt'> |
---|
| 2288 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2289 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2290 | <p class=MsoBodyText>Corr_length</p> |
---|
| 2291 | </td> |
---|
| 2292 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2293 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2294 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2295 | <p class=MsoBodyText>Å</p> |
---|
| 2296 | </td> |
---|
| 2297 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2298 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2299 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2300 | <p class=MsoBodyText>100.0</p> |
---|
| 2301 | </td> |
---|
| 2302 | </tr> |
---|
| 2303 | <tr style='height:19.25pt'> |
---|
| 2304 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2305 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2306 | <p class=MsoBodyText>Block_sld</p> |
---|
| 2307 | </td> |
---|
| 2308 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2309 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2310 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2311 | <p class=MsoBodyText>Å<sup>-2</sup></p> |
---|
| 2312 | </td> |
---|
| 2313 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2314 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2315 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2316 | <p class=MsoBodyText>2e-6</p> |
---|
| 2317 | </td> |
---|
| 2318 | </tr> |
---|
| 2319 | <tr style='height:19.25pt'> |
---|
| 2320 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2321 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2322 | <p class=MsoBodyText>Solvent_sld</p> |
---|
| 2323 | </td> |
---|
| 2324 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2325 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2326 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2327 | <p class=MsoBodyText>Å<sup>-2</sup></p> |
---|
| 2328 | </td> |
---|
| 2329 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2330 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2331 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2332 | <p class=MsoBodyText>6e-6</p> |
---|
| 2333 | </td> |
---|
| 2334 | </tr> |
---|
| 2335 | <tr style='height:19.25pt'> |
---|
| 2336 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2337 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2338 | <p class=MsoBodyText>Background</p> |
---|
| 2339 | </td> |
---|
| 2340 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2341 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2342 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2343 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 2344 | </td> |
---|
| 2345 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2346 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2347 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2348 | <p class=MsoBodyText>0.0</p> |
---|
| 2349 | </td> |
---|
| 2350 | </tr> |
---|
| 2351 | </table> |
---|
| 2352 | |
---|
| 2353 | </div> |
---|
| 2354 | |
---|
| 2355 | |
---|
| 2356 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'> </p> |
---|
| 2357 | |
---|
| 2358 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'>References: </p> |
---|
| 2359 | |
---|
| 2360 | <p class=MsoNormal style='margin-left:.25in;text-indent:.25in;text-autospace: |
---|
| 2361 | none'>J. Teixeira, (1988) J. Appl. Cryst., vol. 21, p781-785</p> |
---|
| 2362 | |
---|
| 2363 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2364 | |
---|
| 2365 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2366 | |
---|
| 2367 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 2368 | style='font-size:14.0pt'>3.7.<span style='font:7.0pt "Times New Roman"'> |
---|
| 2369 | </span></span></b><b><span style='font-size:14.0pt'> <a name="BEPolyelectrolyte">BEPolyelectrolyte Model</a></span></b></p> |
---|
| 2370 | |
---|
| 2371 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2372 | |
---|
| 2373 | <p class=MsoNormal style='margin-left:.25in'>Calculates the structure factor of |
---|
| 2374 | a polyelectrolyte solution with the RPA expression derived by Borue and |
---|
| 2375 | Erukhimovich. The value returned is in cm<sup>-1</sup>.</p> |
---|
| 2376 | |
---|
| 2377 | <p class=MsoNormal style='margin-left:.25in'> </p> |
---|
| 2378 | |
---|
| 2379 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 2380 | style='font-size:14.0pt'><sub><img width=365 height=125 |
---|
| 2381 | src="../images/html/image031.gif"></sub></span></p> |
---|
| 2382 | |
---|
| 2383 | <p class=MsoNormal style='margin-left:.25in'> </p> |
---|
| 2384 | |
---|
| 2385 | <p class=MsoNormal style='margin-left:.25in'>K is a contrast factor of the |
---|
| 2386 | polymer, L<sub>b</sub> is the Bjerrum length, h is the virial parameter, b is |
---|
| 2387 | the monomer length, C<sub>s</sub> is the concentration of monovalent salt, |
---|
| 2388 | α is the ionization degree, C<sub>a</sub> is the polymer molar |
---|
| 2389 | concentration, and bck is the incoherent background.</p> |
---|
| 2390 | |
---|
| 2391 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2392 | |
---|
| 2393 | <div align=center> |
---|
| 2394 | |
---|
| 2395 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 2396 | style='border-collapse:collapse;border:none'> |
---|
| 2397 | <tr style='height:19.25pt'> |
---|
| 2398 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2399 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2400 | <p class=MsoBodyText>Parameter name</p> |
---|
| 2401 | </td> |
---|
| 2402 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2403 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2404 | <p class=MsoBodyText>Units</p> |
---|
| 2405 | </td> |
---|
| 2406 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2407 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2408 | <p class=MsoBodyText>Default value</p> |
---|
| 2409 | </td> |
---|
| 2410 | </tr> |
---|
| 2411 | <tr style='height:19.25pt'> |
---|
| 2412 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2413 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2414 | <p class=MsoBodyText>K</p> |
---|
| 2415 | </td> |
---|
| 2416 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2417 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2418 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2419 | <p class=MsoBodyText>Barns = 10<sup>-24</sup> cm<sup>2</sup></p> |
---|
| 2420 | </td> |
---|
| 2421 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2422 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2423 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2424 | <p class=MsoBodyText>10</p> |
---|
| 2425 | </td> |
---|
| 2426 | </tr> |
---|
| 2427 | <tr style='height:19.25pt'> |
---|
| 2428 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2429 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2430 | <p class=MsoBodyText>L<sub>b</sub></p> |
---|
| 2431 | </td> |
---|
| 2432 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2433 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2434 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2435 | <p class=MsoBodyText>Å</p> |
---|
| 2436 | </td> |
---|
| 2437 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2438 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2439 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2440 | <p class=MsoBodyText>7.1</p> |
---|
| 2441 | </td> |
---|
| 2442 | </tr> |
---|
| 2443 | <tr style='height:19.25pt'> |
---|
| 2444 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2445 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2446 | <p class=MsoBodyText>h</p> |
---|
| 2447 | </td> |
---|
| 2448 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2449 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2450 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2451 | <p class=MsoBodyText>Å<sup>-3</sup></p> |
---|
| 2452 | </td> |
---|
| 2453 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2454 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2455 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2456 | <p class=MsoBodyText>12</p> |
---|
| 2457 | </td> |
---|
| 2458 | </tr> |
---|
| 2459 | <tr style='height:19.25pt'> |
---|
| 2460 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2461 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2462 | <p class=MsoBodyText>b</p> |
---|
| 2463 | </td> |
---|
| 2464 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2465 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2466 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2467 | <p class=MsoBodyText>Å</p> |
---|
| 2468 | </td> |
---|
| 2469 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2470 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2471 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2472 | <p class=MsoBodyText>10</p> |
---|
| 2473 | </td> |
---|
| 2474 | </tr> |
---|
| 2475 | <tr style='height:19.25pt'> |
---|
| 2476 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2477 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2478 | <p class=MsoBodyText>Cs</p> |
---|
| 2479 | </td> |
---|
| 2480 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2481 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2482 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2483 | <p class=MsoBodyText>Mol/L</p> |
---|
| 2484 | </td> |
---|
| 2485 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2486 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2487 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2488 | <p class=MsoBodyText>0</p> |
---|
| 2489 | </td> |
---|
| 2490 | </tr> |
---|
| 2491 | <tr style='height:19.25pt'> |
---|
| 2492 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2493 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2494 | <p class=MsoBodyText>Alpha</p> |
---|
| 2495 | </td> |
---|
| 2496 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2497 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2498 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2499 | <p class=MsoBodyText>None</p> |
---|
| 2500 | </td> |
---|
| 2501 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2502 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2503 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2504 | <p class=MsoBodyText>0.05</p> |
---|
| 2505 | </td> |
---|
| 2506 | </tr> |
---|
| 2507 | <tr style='height:19.25pt'> |
---|
| 2508 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2509 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2510 | <p class=MsoBodyText>Ca</p> |
---|
| 2511 | </td> |
---|
| 2512 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2513 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2514 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2515 | <p class=MsoBodyText>Mol/L</p> |
---|
| 2516 | </td> |
---|
| 2517 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2518 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2519 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2520 | <p class=MsoBodyText>0.7</p> |
---|
| 2521 | </td> |
---|
| 2522 | </tr> |
---|
| 2523 | <tr style='height:19.25pt'> |
---|
| 2524 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2525 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2526 | <p class=MsoBodyText>Background</p> |
---|
| 2527 | </td> |
---|
| 2528 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2529 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2530 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2531 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 2532 | </td> |
---|
| 2533 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2534 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2535 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2536 | <p class=MsoBodyText>0.0</p> |
---|
| 2537 | </td> |
---|
| 2538 | </tr> |
---|
| 2539 | </table> |
---|
| 2540 | |
---|
| 2541 | </div> |
---|
| 2542 | |
---|
| 2543 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2544 | |
---|
| 2545 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'>References: </p> |
---|
| 2546 | |
---|
| 2547 | <p class=MsoNormal style='margin-left:.5in;text-autospace:none'>Borue, V. Y., |
---|
| 2548 | Erukhimovich, I. Y. Macromolecules 21, 3240 (1988).</p> |
---|
| 2549 | |
---|
| 2550 | <p class=MsoNormal style='margin-left:.5in;text-autospace:none'><span lang=FR>Joanny, |
---|
| 2551 | J.-F., Leibler, L. Journal de Physique 51, 545 (1990).</span></p> |
---|
| 2552 | |
---|
| 2553 | <p class=MsoNormal style='margin-left:.5in;text-autospace:none'><span lang=FR>Moussaid, |
---|
| 2554 | A., Schosseler, F., Munch, J.-P., Candau, S. J. Journal de Physique II France </span></p> |
---|
| 2555 | |
---|
| 2556 | <p class=MsoNormal style='margin-left:.5in;text-autospace:none'>3, 573 (1993).</p> |
---|
| 2557 | |
---|
| 2558 | <p class=MsoNormal style='margin-left:.5in;text-autospace:none'>Raphaël, E., |
---|
| 2559 | Joanny, J.-F., Europhysics Letters 11, 179 (1990).</p> |
---|
| 2560 | |
---|
| 2561 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'> </p> |
---|
| 2562 | |
---|
| 2563 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2564 | |
---|
| 2565 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 2566 | style='font-size:14.0pt'>3.8.<span style='font:7.0pt "Times New Roman"'> |
---|
| 2567 | </span></span></b><b><span style='font-size:14.0pt'><a name="Guinier"> Guinier (Model)</a></span></b></p> |
---|
| 2568 | |
---|
| 2569 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2570 | |
---|
| 2571 | <p class=MsoNormal style='margin-left:.25in'>A Guinier analysis is done by linearizing |
---|
| 2572 | the data at low q by plotting it as log(I) versus Q<sup>2</sup>. The Guinier |
---|
| 2573 | radius R<sub>g</sub> can be obtained by fitting the following model:</p> |
---|
| 2574 | |
---|
| 2575 | <p class=MsoNormal style='margin-left:.25in'> </p> |
---|
| 2576 | |
---|
| 2577 | <p class=MsoNormal align=center style='margin-left:.25in;text-align:center'><span |
---|
| 2578 | style='font-size:14.0pt'><sub><img width=183 height=28 |
---|
| 2579 | src="../images/html/image032.gif"></sub></span></p> |
---|
| 2580 | |
---|
| 2581 | <p class=MsoNormal align=center style='margin-left:.25in;text-align:center'><b><span |
---|
| 2582 | style='font-size:14.0pt'> </span></b></p> |
---|
| 2583 | |
---|
| 2584 | <div align=center> |
---|
| 2585 | |
---|
| 2586 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 2587 | style='border-collapse:collapse;border:none'> |
---|
| 2588 | <tr style='height:19.25pt'> |
---|
| 2589 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2590 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2591 | <p class=MsoBodyText>Parameter name</p> |
---|
| 2592 | </td> |
---|
| 2593 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2594 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2595 | <p class=MsoBodyText>Units</p> |
---|
| 2596 | </td> |
---|
| 2597 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2598 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2599 | <p class=MsoBodyText>Default value</p> |
---|
| 2600 | </td> |
---|
| 2601 | </tr> |
---|
| 2602 | <tr style='height:19.25pt'> |
---|
| 2603 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2604 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2605 | <p class=MsoBodyText>scale</p> |
---|
| 2606 | </td> |
---|
| 2607 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2608 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2609 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2610 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 2611 | </td> |
---|
| 2612 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2613 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2614 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2615 | <p class=MsoBodyText>1.0</p> |
---|
| 2616 | </td> |
---|
| 2617 | </tr> |
---|
| 2618 | <tr style='height:19.25pt'> |
---|
| 2619 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2620 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2621 | <p class=MsoBodyText>Rg</p> |
---|
| 2622 | </td> |
---|
| 2623 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2624 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2625 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2626 | <p class=MsoBodyText>Å</p> |
---|
| 2627 | </td> |
---|
| 2628 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2629 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2630 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
[b570686] | 2631 | <p class=MsoBodyText>60</p> |
---|
[5973b566] | 2632 | </td> |
---|
| 2633 | </tr> |
---|
| 2634 | </table> |
---|
| 2635 | |
---|
| 2636 | </div> |
---|
| 2637 | |
---|
| 2638 | <p class=MsoNormal style='margin-left:.25in'><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2639 | <p class=MsoNormal style='margin-left:.25in'><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2640 | <p class=MsoNormal style='margin-left:.25in'><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2641 | |
---|
| 2642 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 2643 | style='font-size:14.0pt'>3.9.<span style='font:7.0pt "Times New Roman"'> |
---|
| 2644 | </span></span></b><b><span style='font-size:14.0pt'> <a name="PorodModel">PorodModel</a></span></b></p> |
---|
| 2645 | |
---|
| 2646 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2647 | |
---|
| 2648 | <p class=MsoNormal style='margin-left:.25in'>A Porod analysis is done by |
---|
| 2649 | linearizing the data at high q by plotting it as log(I) versus log(Q). In the |
---|
| 2650 | high q region we can fit the following model: </p> |
---|
| 2651 | |
---|
| 2652 | <p class=MsoNormal style='margin-left:.25in'> </p> |
---|
| 2653 | |
---|
| 2654 | <p class=MsoNormal align=center style='margin-left:.25in;text-align:center'><span |
---|
| 2655 | style='font-size:14.0pt'><sub><img width=368 height=25 |
---|
| 2656 | src="../images/html/image033.gif"></sub></span></p> |
---|
| 2657 | |
---|
| 2658 | <p class=MsoNormal align=center style='margin-left:.25in;text-align:center'><span |
---|
| 2659 | style='font-size:14.0pt'> </span></p> |
---|
| 2660 | |
---|
| 2661 | <p class=MsoNormal style='margin-left:.25in'>C is the scale factor and Sv is |
---|
| 2662 | the specific surface area of the sample and <span style='font-family:"Arial","sans-serif"'>Δ</span>ρ |
---|
| 2663 | is the contrast factor. </p> |
---|
| 2664 | |
---|
| 2665 | <p class=MsoNormal style='margin-left:.25in'> </p> |
---|
| 2666 | |
---|
| 2667 | <p class=MsoNormal style='margin-left:.25in'>The background term is added for |
---|
| 2668 | data analysis.</p> |
---|
| 2669 | |
---|
| 2670 | <p class=MsoNormal align=center style='margin-left:.25in;text-align:center'><b><span |
---|
| 2671 | style='font-size:14.0pt'> </span></b></p> |
---|
| 2672 | |
---|
| 2673 | <div align=center> |
---|
| 2674 | |
---|
| 2675 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 2676 | style='border-collapse:collapse;border:none'> |
---|
| 2677 | <tr style='height:19.25pt'> |
---|
| 2678 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2679 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2680 | <p class=MsoBodyText>Parameter name</p> |
---|
| 2681 | </td> |
---|
| 2682 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2683 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2684 | <p class=MsoBodyText>Units</p> |
---|
| 2685 | </td> |
---|
| 2686 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2687 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2688 | <p class=MsoBodyText>Default value</p> |
---|
| 2689 | </td> |
---|
| 2690 | </tr> |
---|
| 2691 | <tr style='height:19.25pt'> |
---|
| 2692 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2693 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2694 | <p class=MsoBodyText>Scale</p> |
---|
| 2695 | </td> |
---|
| 2696 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2697 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2698 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2699 | <p class=MsoBodyText>Å<sup>-4</sup></p> |
---|
| 2700 | </td> |
---|
| 2701 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2702 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2703 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2704 | <p class=MsoBodyText>0.1</p> |
---|
| 2705 | </td> |
---|
| 2706 | </tr> |
---|
| 2707 | <tr style='height:19.25pt'> |
---|
| 2708 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2709 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2710 | <p class=MsoBodyText>Background</p> |
---|
| 2711 | </td> |
---|
| 2712 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2713 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2714 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2715 | <p class=MsoBodyText>cm<sup>-1</sup></p> |
---|
| 2716 | </td> |
---|
| 2717 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2718 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2719 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2720 | <p class=MsoBodyText>0</p> |
---|
| 2721 | </td> |
---|
| 2722 | </tr> |
---|
| 2723 | </table> |
---|
| 2724 | |
---|
| 2725 | </div> |
---|
| 2726 | |
---|
| 2727 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2728 | |
---|
| 2729 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2730 | |
---|
| 2731 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2732 | |
---|
| 2733 | |
---|
| 2734 | |
---|
| 2735 | |
---|
| 2736 | <p class=MsoNormal style='margin-left:.25in;text-indent:-.25in'><b><span |
---|
| 2737 | style='font-size:14.0pt'>4.<span style='font:7.0pt "Times New Roman"'> |
---|
| 2738 | </span></span></b><b><span style='font-size:14.0pt'><a name="Customized Models">Customized Models</a></span></b></p> |
---|
| 2739 | |
---|
| 2740 | <p class=MsoBodyText> </p> |
---|
| 2741 | |
---|
| 2742 | <p class=MsoBodyText>These models are defined by users (See SansView tutorial for details). </p> |
---|
| 2743 | |
---|
| 2744 | <p class=MsoBodyText> </p> |
---|
| 2745 | |
---|
| 2746 | <p class=MsoNormal style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 2747 | style='font-size:14.0pt'>4.1.<span style='font:7.0pt "Times New Roman"'> |
---|
| 2748 | </span></span></b><b><span style='font-size:14.0pt'> <a name="A+Bcos(2x)+Csin(2x)">A+Bcos(2x)+Csin(2x)</a></span></b></p> |
---|
| 2749 | |
---|
| 2750 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 2751 | |
---|
| 2752 | <p class=MsoNormal style='margin-left:.25in;text-autospace:none'>This function, as an example function, calculates intensity = A + Bcos(2Q) + Csin(2Q). </p> |
---|
| 2753 | |
---|
| 2754 | |
---|
| 2755 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
| 2756 | <p class=MsoListParagraphCxSpMiddle style='margin-left:.25in;text-indent:-.25in'><b><span |
---|
| 2757 | style='font-size:14.0pt'>5.<span style='font:7.0pt "Times New Roman"'> |
---|
| 2758 | </span></span></b><b><span style='font-size:14.0pt'><a name="Structure Factors">Structure Factors</a></span></b></p> |
---|
| 2759 | |
---|
| 2760 | <p class=MsoListParagraphCxSpMiddle style='margin-left:.25in'> </p> |
---|
| 2761 | |
---|
| 2762 | <p class=MsoListParagraphCxSpLast style='margin-left:.25in'>The information in |
---|
| 2763 | this section is originated from NIST SANS IgorPro package.</p> |
---|
| 2764 | |
---|
| 2765 | <p class=MsoBodyText> </p> |
---|
| 2766 | |
---|
| 2767 | <p class=MsoListParagraph style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 2768 | style='font-size:14.0pt'>5.1.<span style='font:7.0pt "Times New Roman"'> |
---|
| 2769 | </span></span></b><b><span style='font-size:14.0pt'> <a name="HardSphereStructure">HardSphere Structure</a></span></b></p> |
---|
| 2770 | |
---|
| 2771 | <p class=MsoNormal> </p> |
---|
| 2772 | |
---|
| 2773 | <p class=MsoNormal>This calculates the interparticle structure factor for |
---|
| 2774 | monodisperse spherical particles interacting through hard sphere (excluded |
---|
| 2775 | volume) interactions. The calculation uses the Percus-Yevick closure where the |
---|
| 2776 | interparticle potential is: </p> |
---|
| 2777 | |
---|
| 2778 | <p class=MsoNormal> </p> |
---|
| 2779 | |
---|
| 2780 | <p class=MsoNormal align=center style='margin-left:.25in;text-align:center'><span |
---|
| 2781 | style='font-size:14.0pt;position:relative;top:15.0pt'><img width=122 height=48 |
---|
| 2782 | src="../images/html/image034.gif"></span></p> |
---|
| 2783 | |
---|
| 2784 | <p class=MsoNormal align=center style='margin-left:.25in;text-align:center'><span |
---|
| 2785 | style='font-size:14.0pt;position:relative;top:7.0pt'> </span></p> |
---|
| 2786 | |
---|
| 2787 | <p class=MsoNormal><span style='position:relative;top:7.0pt'>where r is the |
---|
| 2788 | distance from the center of the sphere of a radius R.</span></p> |
---|
| 2789 | |
---|
| 2790 | <p class=MsoNormal> </p> |
---|
| 2791 | |
---|
| 2792 | <p class=MsoNormal> </p> |
---|
| 2793 | |
---|
| 2794 | <div align=center> |
---|
| 2795 | |
---|
| 2796 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 2797 | style='border-collapse:collapse;border:none'> |
---|
| 2798 | <tr style='height:19.25pt'> |
---|
| 2799 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2800 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2801 | <p class=MsoBodyText>Parameter name</p> |
---|
| 2802 | </td> |
---|
| 2803 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2804 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2805 | <p class=MsoBodyText>Units</p> |
---|
| 2806 | </td> |
---|
| 2807 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2808 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2809 | <p class=MsoBodyText>Default value</p> |
---|
| 2810 | </td> |
---|
| 2811 | </tr> |
---|
| 2812 | <tr style='height:19.25pt'> |
---|
| 2813 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2814 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2815 | <p class=MsoBodyText>radius</p> |
---|
| 2816 | </td> |
---|
| 2817 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2818 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2819 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2820 | <p class=MsoBodyText>Å</p> |
---|
| 2821 | </td> |
---|
| 2822 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2823 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2824 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2825 | <p class=MsoBodyText>50.0</p> |
---|
| 2826 | </td> |
---|
| 2827 | </tr> |
---|
| 2828 | <tr style='height:19.25pt'> |
---|
| 2829 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2830 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2831 | <p class=MsoBodyText>volfraction</p> |
---|
| 2832 | </td> |
---|
| 2833 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2834 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2835 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2836 | <p class=MsoBodyText> </p> |
---|
| 2837 | </td> |
---|
| 2838 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2839 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2840 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2841 | <p class=MsoBodyText>0.2</p> |
---|
| 2842 | </td> |
---|
| 2843 | </tr> |
---|
| 2844 | </table> |
---|
| 2845 | |
---|
| 2846 | </div> |
---|
| 2847 | |
---|
| 2848 | <p class=MsoNormal><img width=579 height=273 id="Picture 43" |
---|
| 2849 | src="../images/html/image035.gif"></p> |
---|
| 2850 | |
---|
| 2851 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 2852 | |
---|
| 2853 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 2854 | |
---|
| 2855 | <p class=MsoNormal style='text-autospace:none'>References: </p> |
---|
| 2856 | |
---|
| 2857 | <p class=MsoNormal style='margin-left:.5in;text-autospace:none'>Percus, J. K.; |
---|
| 2858 | Yevick, J. Phys. Rev. 110, 1. (1958).</p> |
---|
| 2859 | |
---|
| 2860 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 2861 | |
---|
| 2862 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 2863 | |
---|
| 2864 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 2865 | |
---|
| 2866 | <p class=MsoListParagraph style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 2867 | style='font-size:14.0pt'>5.2.<span style='font:7.0pt "Times New Roman"'> |
---|
| 2868 | </span></span></b><b><span style='font-size:14.0pt'><a name="SquareWellStructure"> SquareWell Structure</a></span></b></p> |
---|
| 2869 | |
---|
| 2870 | <p class=MsoNormal> </p> |
---|
| 2871 | |
---|
| 2872 | <p class=MsoNormal>This calculates the interparticle structure factor for a |
---|
| 2873 | squar well fluid spherical particles The mean spherical approximation (MSA) |
---|
| 2874 | closure was used for this calculation, and is not the most appropriate closure |
---|
| 2875 | for an attractive interparticle potential. This solution has been compared to |
---|
| 2876 | Monte Carlo simulations for a square well fluid, showing this calculation to be |
---|
| 2877 | limited in applicability to well depths e < 1.5 kT and volume fractions f |
---|
| 2878 | < 0.08.</p> |
---|
| 2879 | |
---|
| 2880 | <p class=MsoNormal> </p> |
---|
| 2881 | |
---|
| 2882 | <p class=MsoNormal>Positive well depths correspond to an attractive potential |
---|
| 2883 | well. Negative well depths correspond to a potential "shoulder", |
---|
| 2884 | which may or may not be physically reasonable.</p> |
---|
| 2885 | |
---|
| 2886 | <p class=MsoNormal> </p> |
---|
| 2887 | |
---|
| 2888 | <p class=MsoNormal>The well width (l) is defined as multiples of the particle |
---|
| 2889 | diameter (2*R)</p> |
---|
| 2890 | |
---|
| 2891 | <p class=MsoNormal> </p> |
---|
| 2892 | |
---|
| 2893 | <p class=MsoNormal>The interaction potential is:</p> |
---|
| 2894 | |
---|
| 2895 | <p class=MsoNormal align=center style='margin-left:.25in;text-align:center'><span |
---|
| 2896 | style='font-size:14.0pt;position:relative;top:22.0pt'><img width=174 height=67 |
---|
| 2897 | src="../images/html/image036.gif"></span></p> |
---|
| 2898 | |
---|
| 2899 | <p class=MsoNormal align=center style='margin-left:.25in;text-align:center'><span |
---|
| 2900 | style='font-size:14.0pt;position:relative;top:7.0pt'> </span></p> |
---|
| 2901 | |
---|
| 2902 | <p class=MsoNormal><span style='position:relative;top:7.0pt'>where r is the |
---|
| 2903 | distance from the center of the sphere of a radius R.</span></p> |
---|
| 2904 | |
---|
| 2905 | <p class=MsoNormal> </p> |
---|
| 2906 | |
---|
| 2907 | <p class=MsoNormal> </p> |
---|
| 2908 | |
---|
| 2909 | <div align=center> |
---|
| 2910 | |
---|
| 2911 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 2912 | style='margin-left:-1.5pt;border-collapse:collapse;border:none'> |
---|
| 2913 | <tr style='height:19.25pt'> |
---|
| 2914 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 2915 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2916 | <p class=MsoBodyText>Parameter name</p> |
---|
| 2917 | </td> |
---|
| 2918 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2919 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2920 | <p class=MsoBodyText>Units</p> |
---|
| 2921 | </td> |
---|
| 2922 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 2923 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2924 | <p class=MsoBodyText>Default value</p> |
---|
| 2925 | </td> |
---|
| 2926 | </tr> |
---|
| 2927 | <tr style='height:19.25pt'> |
---|
| 2928 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 2929 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2930 | <p class=MsoBodyText>radius</p> |
---|
| 2931 | </td> |
---|
| 2932 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2933 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2934 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2935 | <p class=MsoBodyText>Å</p> |
---|
| 2936 | </td> |
---|
| 2937 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2938 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2939 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2940 | <p class=MsoBodyText>50.0</p> |
---|
| 2941 | </td> |
---|
| 2942 | </tr> |
---|
| 2943 | <tr style='height:19.25pt'> |
---|
| 2944 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 2945 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2946 | <p class=MsoBodyText>volfraction</p> |
---|
| 2947 | </td> |
---|
| 2948 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2949 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2950 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2951 | <p class=MsoBodyText> </p> |
---|
| 2952 | </td> |
---|
| 2953 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2954 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2955 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2956 | <p class=MsoBodyText>0.2</p> |
---|
| 2957 | </td> |
---|
| 2958 | </tr> |
---|
| 2959 | <tr style='height:19.25pt'> |
---|
| 2960 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 2961 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2962 | <p class=MsoBodyText>welldepth</p> |
---|
| 2963 | </td> |
---|
| 2964 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2965 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2966 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2967 | <p class=MsoBodyText>kT</p> |
---|
| 2968 | </td> |
---|
| 2969 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2970 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2971 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2972 | <p class=MsoBodyText>1.5</p> |
---|
| 2973 | </td> |
---|
| 2974 | </tr> |
---|
| 2975 | <tr style='height:19.25pt'> |
---|
| 2976 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 2977 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2978 | <p class=MsoBodyText>wellwidth</p> |
---|
| 2979 | </td> |
---|
| 2980 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2981 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2982 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2983 | <p class=MsoBodyText>diameters</p> |
---|
| 2984 | </td> |
---|
| 2985 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 2986 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 2987 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 2988 | <p class=MsoBodyText>1.2</p> |
---|
| 2989 | </td> |
---|
| 2990 | </tr> |
---|
| 2991 | </table> |
---|
| 2992 | |
---|
| 2993 | </div> |
---|
| 2994 | |
---|
| 2995 | <p class=MsoNormal> </p> |
---|
| 2996 | |
---|
| 2997 | <p class=MsoNormal><img width=546 height=296 id="Picture 53" |
---|
| 2998 | src="../images/html/image037.gif"></p> |
---|
| 2999 | |
---|
| 3000 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 3001 | |
---|
| 3002 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 3003 | |
---|
| 3004 | <p class=MsoNormal style='text-autospace:none'>References: </p> |
---|
| 3005 | |
---|
| 3006 | <p class=MsoNormal style='margin-left:.5in;text-autospace:none'>Sharma, R. V.; |
---|
| 3007 | Sharma, K. C. Physica, 89A, 213. (1977).</p> |
---|
| 3008 | |
---|
| 3009 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 3010 | |
---|
| 3011 | <p class=MsoListParagraph style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 3012 | style='font-size:14.0pt'>5.3.<span style='font:7.0pt "Times New Roman"'> |
---|
| 3013 | </span></span></b><b><span style='font-size:14.0pt'><a name="HayterMSAStructure"> HayterMSA Structure</a></span></b></p> |
---|
| 3014 | |
---|
| 3015 | <p class=MsoNormal> </p> |
---|
| 3016 | |
---|
| 3017 | <p class=MsoNormal>This calculates the Structure factor (the Fourier transform |
---|
| 3018 | of the pair correlation function g(r)) for a system of charged, spheroidal |
---|
| 3019 | objects in a dielectric medium. When combined with an appropriate form factor |
---|
| 3020 | (such as sphere, core+shell, ellipsoid etc
), this allows for inclusion of the |
---|
| 3021 | interparticle interference effects due to screened coulomb repulsion between |
---|
| 3022 | charged particles. This routine only works for charged particles. If the |
---|
| 3023 | charge is set to zero the routine will self destruct. For non-charged |
---|
| 3024 | particles use a hard sphere potential.</p> |
---|
| 3025 | |
---|
| 3026 | <p class=MsoNormal> </p> |
---|
| 3027 | |
---|
| 3028 | <p class=MsoNormal>The salt concentration is used to compute the ionic strength |
---|
| 3029 | of the solution which in turn is used to compute the Debye screening length. |
---|
| 3030 | At present there is no provision for entering the ionic strength directly nor |
---|
| 3031 | for use of any multivalent salts. The counterions are also assumed to be monovalent.</p> |
---|
| 3032 | |
---|
| 3033 | <p class=MsoNormal> </p> |
---|
| 3034 | |
---|
| 3035 | <p class=MsoNormal> </p> |
---|
| 3036 | |
---|
| 3037 | <div align=center> |
---|
| 3038 | |
---|
| 3039 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 3040 | style='margin-left:-1.5pt;border-collapse:collapse;border:none'> |
---|
| 3041 | <tr style='height:19.25pt'> |
---|
| 3042 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 3043 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3044 | <p class=MsoBodyText>Parameter name</p> |
---|
| 3045 | </td> |
---|
| 3046 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 3047 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3048 | <p class=MsoBodyText>Units</p> |
---|
| 3049 | </td> |
---|
| 3050 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 3051 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3052 | <p class=MsoBodyText>Default value</p> |
---|
| 3053 | </td> |
---|
| 3054 | </tr> |
---|
| 3055 | <tr style='height:19.25pt'> |
---|
| 3056 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 3057 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3058 | <p class=MsoBodyText>radius</p> |
---|
| 3059 | </td> |
---|
| 3060 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3061 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3062 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3063 | <p class=MsoBodyText>Å</p> |
---|
| 3064 | </td> |
---|
| 3065 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3066 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3067 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3068 | <p class=MsoBodyText>20.8</p> |
---|
| 3069 | </td> |
---|
| 3070 | </tr> |
---|
| 3071 | <tr style='height:19.25pt'> |
---|
| 3072 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 3073 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3074 | <p class=MsoBodyText>charge</p> |
---|
| 3075 | </td> |
---|
| 3076 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3077 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3078 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3079 | <p class=MsoBodyText> </p> |
---|
| 3080 | </td> |
---|
| 3081 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3082 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3083 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3084 | <p class=MsoBodyText>19</p> |
---|
| 3085 | </td> |
---|
| 3086 | </tr> |
---|
| 3087 | <tr style='height:19.25pt'> |
---|
| 3088 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 3089 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3090 | <p class=MsoBodyText>volfraction</p> |
---|
| 3091 | </td> |
---|
| 3092 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3093 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3094 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3095 | <p class=MsoBodyText> </p> |
---|
| 3096 | </td> |
---|
| 3097 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3098 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3099 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3100 | <p class=MsoBodyText>0.2</p> |
---|
| 3101 | </td> |
---|
| 3102 | </tr> |
---|
| 3103 | <tr style='height:19.25pt'> |
---|
| 3104 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 3105 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3106 | <p class=MsoBodyText>temperature</p> |
---|
| 3107 | </td> |
---|
| 3108 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3109 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3110 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3111 | <p class=MsoBodyText>K</p> |
---|
| 3112 | </td> |
---|
| 3113 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3114 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3115 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3116 | <p class=MsoBodyText>318</p> |
---|
| 3117 | </td> |
---|
| 3118 | </tr> |
---|
| 3119 | <tr style='height:19.25pt'> |
---|
| 3120 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 3121 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3122 | <p class=MsoBodyText>salt conc</p> |
---|
| 3123 | </td> |
---|
| 3124 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3125 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3126 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3127 | <p class=MsoBodyText>M</p> |
---|
| 3128 | </td> |
---|
| 3129 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3130 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3131 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3132 | <p class=MsoBodyText>0</p> |
---|
| 3133 | </td> |
---|
| 3134 | </tr> |
---|
| 3135 | <tr style='height:19.25pt'> |
---|
| 3136 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 3137 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3138 | <p class=MsoBodyText>dielectconst</p> |
---|
| 3139 | </td> |
---|
| 3140 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3141 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3142 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3143 | <p class=MsoBodyText> </p> |
---|
| 3144 | </td> |
---|
| 3145 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3146 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3147 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3148 | <p class=MsoBodyText>71.1</p> |
---|
| 3149 | </td> |
---|
| 3150 | </tr> |
---|
| 3151 | </table> |
---|
| 3152 | |
---|
| 3153 | </div> |
---|
| 3154 | |
---|
| 3155 | <p class=MsoNormal> </p> |
---|
| 3156 | |
---|
| 3157 | <p class=MsoNormal><img width=548 height=354 id="Picture 56" |
---|
| 3158 | src="../images/html/image038.gif"></p> |
---|
| 3159 | |
---|
| 3160 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 3161 | |
---|
| 3162 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 3163 | |
---|
| 3164 | <p class=MsoNormal style='text-autospace:none'>References: </p> |
---|
| 3165 | |
---|
| 3166 | <p class=MsoNormal style='text-indent:.5in;text-autospace:none'>JP Hansen and |
---|
| 3167 | JB Hayter, Molecular Physics 46, 651-656 (1982).</p> |
---|
| 3168 | |
---|
| 3169 | <p class=MsoNormal style='text-autospace:none'> JB Hayter and J |
---|
| 3170 | Penfold, Molecular Physics 42, 109-118 (1981).</p> |
---|
| 3171 | |
---|
| 3172 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 3173 | |
---|
| 3174 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
| 3175 | |
---|
| 3176 | <p class=MsoListParagraph style='margin-left:.55in;text-indent:-.3in'><b><span |
---|
| 3177 | style='font-size:14.0pt'>5.4.<span style='font:7.0pt "Times New Roman"'> |
---|
| 3178 | </span></span></b><b><span style='font-size:14.0pt'><a name="StickyHSStructure"> StickyHS Structure</a></span></b></p> |
---|
| 3179 | |
---|
| 3180 | <p class=MsoNormal> </p> |
---|
| 3181 | |
---|
| 3182 | <p class=MsoNormal>This calculates the interparticle structure factor for a |
---|
| 3183 | hard sphere fluid with a narrow attractive well. A perturbative solution of the |
---|
| 3184 | Percus-Yevick closure is used. The strength of the attractive well is described |
---|
| 3185 | in terms of "stickiness" as defined below. The returned value is a |
---|
| 3186 | dimensionless structure factor, S(q).</p> |
---|
| 3187 | |
---|
| 3188 | <p class=MsoNormal> </p> |
---|
| 3189 | |
---|
| 3190 | <p class=MsoNormal>The perturb (perturbation parameter), epsilon, should be |
---|
| 3191 | held between 0.01 and 0.1. It is best to hold the perturbation parameter fixed |
---|
| 3192 | and let the "stickiness" vary to adjust the interaction strength. The |
---|
| 3193 | stickiness, tau, is defined in equation 21 and is a function of both the |
---|
| 3194 | perturbation parameter and the interaction strength. Tau and epsilon are |
---|
| 3195 | defined in terms of the hard sphere diameter (sigma = 2R), the width of the |
---|
| 3196 | square well, delta (same units as R), and the depth of the well, u<sub>o</sub>, |
---|
| 3197 | in units of kT. From the definition, it is clear that smaller tau mean stronger |
---|
| 3198 | attraction.</p> |
---|
| 3199 | |
---|
| 3200 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 3201 | style='font-size:14.0pt;position:relative;top:22.0pt'><img width=135 height=67 |
---|
| 3202 | src="../images/html/image039.gif"></span></p> |
---|
| 3203 | |
---|
| 3204 | <p class=MsoNormal align=center style='text-align:center'><span |
---|
| 3205 | style='font-size:14.0pt;position:relative;top:27.0pt'> </span></p> |
---|
| 3206 | |
---|
| 3207 | <p class=MsoNormal>where the interaction potential is</p> |
---|
| 3208 | |
---|
| 3209 | <p class=MsoNormal align=center style='margin-left:.25in;text-align:center'><span |
---|
| 3210 | style='font-size:14.0pt;position:relative;top:23.0pt'><img width=186 height=69 |
---|
| 3211 | src="../images/html/image040.gif"></span></p> |
---|
| 3212 | |
---|
| 3213 | <p class=MsoNormal>The Percus-Yevick (PY) closure was used for this |
---|
| 3214 | calculation, and is an adequate closure for an attractive interparticle |
---|
| 3215 | potential. This solution has been compared to Monte Carlo simulations for a |
---|
| 3216 | square well fluid, with good agreement.</p> |
---|
| 3217 | |
---|
| 3218 | <p class=MsoNormal> </p> |
---|
| 3219 | |
---|
| 3220 | <p class=MsoNormal>The true particle volume fraction, f, is not equal to h, |
---|
| 3221 | which appears in most of the reference. The two are related in equation (24) of |
---|
| 3222 | the reference. The reference also describes the relationship between this |
---|
| 3223 | perturbation solution and the original sticky hard sphere (or adhesive sphere) |
---|
| 3224 | model by Baxter.</p> |
---|
| 3225 | |
---|
| 3226 | <p class=MsoNormal> </p> |
---|
| 3227 | |
---|
| 3228 | <p class=MsoNormal>NOTES: The calculation can go haywire for certain |
---|
| 3229 | combinations of the input parameters, producing unphysical solutions - in this |
---|
| 3230 | case errors are reported to the command window and the S(q) is set to -1 (it |
---|
| 3231 | will disappear on a log-log plot). Use tight bounds to keep the parameters to |
---|
| 3232 | values that you know are physical (test them) and keep nudging them until the |
---|
| 3233 | optimization does not hit the constraints.</p> |
---|
| 3234 | |
---|
| 3235 | <p class=MsoNormal> </p> |
---|
| 3236 | |
---|
| 3237 | <div align=center> |
---|
| 3238 | |
---|
| 3239 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
| 3240 | style='margin-left:-1.5pt;border-collapse:collapse;border:none'> |
---|
| 3241 | <tr style='height:19.25pt'> |
---|
| 3242 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 3243 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3244 | <p class=MsoBodyText>Parameter name</p> |
---|
| 3245 | </td> |
---|
| 3246 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 3247 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3248 | <p class=MsoBodyText>Units</p> |
---|
| 3249 | </td> |
---|
| 3250 | <td width=143 valign=top style='width:107.0pt;border:solid windowtext 1.0pt; |
---|
| 3251 | border-left:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3252 | <p class=MsoBodyText>Default value</p> |
---|
| 3253 | </td> |
---|
| 3254 | </tr> |
---|
| 3255 | <tr style='height:19.25pt'> |
---|
| 3256 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 3257 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3258 | <p class=MsoBodyText>radius</p> |
---|
| 3259 | </td> |
---|
| 3260 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3261 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3262 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3263 | <p class=MsoBodyText>Å</p> |
---|
| 3264 | </td> |
---|
| 3265 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3266 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3267 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3268 | <p class=MsoBodyText>20.8</p> |
---|
| 3269 | </td> |
---|
| 3270 | </tr> |
---|
| 3271 | <tr style='height:19.25pt'> |
---|
| 3272 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 3273 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3274 | <p class=MsoBodyText>perturb </p> |
---|
| 3275 | </td> |
---|
| 3276 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3277 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3278 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3279 | <p class=MsoBodyText> </p> |
---|
| 3280 | </td> |
---|
| 3281 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3282 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3283 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3284 | <p class=MsoBodyText>0.05</p> |
---|
| 3285 | </td> |
---|
| 3286 | </tr> |
---|
| 3287 | <tr style='height:19.25pt'> |
---|
| 3288 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 3289 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3290 | <p class=MsoBodyText>volfraction</p> |
---|
| 3291 | </td> |
---|
| 3292 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3293 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3294 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3295 | <p class=MsoBodyText> </p> |
---|
| 3296 | </td> |
---|
| 3297 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
| 3298 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
| 3299 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3300 | <p class=MsoBodyText>0.1</p> |
---|
| 3301 | </td> |
---|
| 3302 | </tr> |
---|
| 3303 | <tr style='height:19.25pt'> |
---|
| 3304 | <td width=145 valign=top style='width:108.5pt;border:solid windowtext 1.0pt; |
---|
| 3305 | border-top:none;padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
| 3306 | <p class=MsoBodyText>stickiness</p> |
---|
| 3307 | </td> |
---|
| 3308 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
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| 3311 | <p class=MsoBodyText>K</p> |
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| 3316 | <p class=MsoBodyText>0.2</p> |
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| 3332 | <p class=MsoNormal style='text-autospace:none'>References: </p> |
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| 3333 | |
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| 3334 | <p class=MsoNormal style='text-indent:.5in;text-autospace:none'>Menon, S. V. |
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| 3335 | G., Manohar, C. and K. Srinivas Rao J. Chem. Phys., 95(12), 9186-9190 (1991).</p> |
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| 3344 | <p class=MsoBodyText><b><span style='font-size:14.0pt'><a name="References">References</a></span></b></p> |
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| 3345 | |
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| 3346 | <p class=MsoBodyText>Feigin, L. A, and D. I. Svergun (1987) "Structure |
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| 3347 | Analysis by Small-Angle X-Ray and Neutron Scattering", Plenum Press, New York.</p> |
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| 3348 | |
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| 3349 | <p class=MsoBodyText>Guinier, A. and G. Fournet (1955) "Small-Angle |
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| 3350 | Scattering of X-Rays", John Wiley and Sons, New York.</p> |
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| 3351 | |
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| 3352 | <p class=MsoBodyText>Kline, S. R. (2006) <i>J Appl. Cryst.</i> <b>39</b>(6), |
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| 3353 | 895.</p> |
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| 3354 | |
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| 3355 | <p class=MsoBodyText>Hansen, S., (1990)<i> J. Appl. Cryst. </i>23, 344-346.</p> |
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| 3356 | |
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| 3357 | <p class=MsoBodyText>Henderson, S.J. (1996) <i>Biophys. J. </i>70, 1618-1627</p> |
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| 3358 | |
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| 3359 | <p class=MsoBodyText>Stöckel, P., May, R., Strell, I., Cejka, Z., Hoppe, W., |
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| 3360 | Heumann, H., Zillig, W. and Crespi, H. (1980) <i>Eur. J. Biochem. </i>112, |
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| 3361 | 411-417.</p> |
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| 3362 | |
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| 3363 | <p class=MsoBodyText>McAlister, B.C. and Grady, B.P., (1998) J. Appl. Cryst. 31, |
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| 3364 | 594-599.</p> |
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| 3365 | |
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| 3366 | <p class=MsoBodyText>Porod, G. (1982) in Small Angle X-ray Scattering, editors |
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| 3367 | Glatter, O. and Kratky, O., Academic Press.</p> |
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