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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 |
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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"'> |
---|
404 | </span></span></b><b><span style='font-size:14.0pt'><a name="CylinderModel">CylinderModel</a></span></b></p> |
---|
405 | |
---|
406 | <p class=MsoNormal> </p> |
---|
407 | |
---|
408 | <p class=MsoNormal>This model provides the form factor for a monodisperse right |
---|
409 | circular cylinder with uniform scattering length density. The form factor is |
---|
410 | normalized by the particle volume.</p> |
---|
411 | |
---|
412 | <p class=MsoNormal> </p> |
---|
413 | |
---|
414 | <p class=MsoNormal style='margin-left:.85in;text-indent:-.35in'><b>2.2.1.<span |
---|
415 | style='font:7.0pt "Times New Roman"'> </span></b><b>Definition</b></p> |
---|
416 | |
---|
417 | <p class=MsoNormal> </p> |
---|
418 | |
---|
419 | <p class=MsoNormal>The output of the 2D scattering intensity function for |
---|
420 | oriented cylinders is given by (Guinier, 1955):</p> |
---|
421 | |
---|
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> |
---|
424 | |
---|
425 | <p class=MsoNormal align=center style='text-align:center'><sub><img width=373 |
---|
426 | height=45 src="../images/html/image007.gif"></sub> (5)</p> |
---|
427 | |
---|
428 | <p class=MsoNormal>where <span style='font-family:"Arial","sans-serif"'>α</span> |
---|
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 |
---|
433 | and the solvent. J<sub>1</sub> is the first order Bessel function.</p> |
---|
434 | |
---|
435 | <p class=MsoNormal> </p> |
---|
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" |
---|
444 | alt=angles></p> |
---|
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> |
---|
448 | |
---|
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> |
---|
454 | |
---|
455 | <p class=MsoNormal> </p> |
---|
456 | |
---|
457 | <div align=center> |
---|
458 | |
---|
459 | <table class=MsoTableGrid border=1 cellspacing=0 cellpadding=0 |
---|
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; |
---|
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; |
---|
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'> |
---|
2631 | <p class=MsoBodyText>0.1</p> |
---|
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: |
---|
3309 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
3310 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
3311 | <p class=MsoBodyText>K</p> |
---|
3312 | </td> |
---|
3313 | <td width=143 valign=top style='width:107.0pt;border-top:none;border-left: |
---|
3314 | none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1.0pt; |
---|
3315 | padding:0in 5.4pt 0in 5.4pt;height:19.25pt'> |
---|
3316 | <p class=MsoBodyText>0.2</p> |
---|
3317 | </td> |
---|
3318 | </tr> |
---|
3319 | </table> |
---|
3320 | |
---|
3321 | </div> |
---|
3322 | |
---|
3323 | <p class=MsoNormal> </p> |
---|
3324 | |
---|
3325 | <p class=MsoNormal><img width=524 height=359 id="Picture 111" |
---|
3326 | src="../images/html/image041.gif"></p> |
---|
3327 | |
---|
3328 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
3329 | |
---|
3330 | <p class=MsoNormal style='text-autospace:none'> </p> |
---|
3331 | |
---|
3332 | <p class=MsoNormal style='text-autospace:none'>References: </p> |
---|
3333 | |
---|
3334 | <p class=MsoNormal style='text-indent:.5in;text-autospace:none'>Menon, S. V. |
---|
3335 | G., Manohar, C. and K. Srinivas Rao J. Chem. Phys., 95(12), 9186-9190 (1991).</p> |
---|
3336 | |
---|
3337 | |
---|
3338 | |
---|
3339 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
3340 | |
---|
3341 | <p class=MsoNormal><b><span style='font-size:14.0pt'> </span></b></p> |
---|
3342 | |
---|
3343 | |
---|
3344 | <p class=MsoBodyText><b><span style='font-size:14.0pt'><a name="References">References</a></span></b></p> |
---|
3345 | |
---|
3346 | <p class=MsoBodyText>Feigin, L. A, and D. I. Svergun (1987) "Structure |
---|
3347 | Analysis by Small-Angle X-Ray and Neutron Scattering", Plenum Press, New York.</p> |
---|
3348 | |
---|
3349 | <p class=MsoBodyText>Guinier, A. and G. Fournet (1955) "Small-Angle |
---|
3350 | Scattering of X-Rays", John Wiley and Sons, New York.</p> |
---|
3351 | |
---|
3352 | <p class=MsoBodyText>Kline, S. R. (2006) <i>J Appl. Cryst.</i> <b>39</b>(6), |
---|
3353 | 895.</p> |
---|
3354 | |
---|
3355 | <p class=MsoBodyText>Hansen, S., (1990)<i> J. Appl. Cryst. </i>23, 344-346.</p> |
---|
3356 | |
---|
3357 | <p class=MsoBodyText>Henderson, S.J. (1996) <i>Biophys. J. </i>70, 1618-1627</p> |
---|
3358 | |
---|
3359 | <p class=MsoBodyText>Stöckel, P., May, R., Strell, I., Cejka, Z., Hoppe, W., |
---|
3360 | Heumann, H., Zillig, W. and Crespi, H. (1980) <i>Eur. J. Biochem. </i>112, |
---|
3361 | 411-417.</p> |
---|
3362 | |
---|
3363 | <p class=MsoBodyText>McAlister, B.C. and Grady, B.P., (1998) J. Appl. Cryst. 31, |
---|
3364 | 594-599.</p> |
---|
3365 | |
---|
3366 | <p class=MsoBodyText>Porod, G. (1982) in Small Angle X-ray Scattering, editors |
---|
3367 | Glatter, O. and Kratky, O., Academic Press.</p> |
---|
3368 | |
---|
3369 | <p class=MsoBodyText> </p> |
---|
3370 | |
---|
3371 | <p class=MsoNormal> </p> |
---|
3372 | |
---|
3373 | </div> |
---|
3374 | |
---|
3375 | </body> |
---|
3376 | |
---|
3377 | </html> |
---|