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101 | </head> |
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102 | |
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103 | <body lang=EN-US link=blue vlink=purple> |
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104 | |
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105 | <div class=Section1> |
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106 | |
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107 | <p class=MsoListParagraphCxSpFirst style='text-indent:-.25in;line-height:normal'><span |
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108 | style='font-family:Symbol'>·<span style='font:7.0pt "Times New Roman"'> |
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109 | </span></span><b><span style='font-family:"Times New Roman","serif"'><a |
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110 | href="#invariant">Scattering Invariant</a></span></b></p> |
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111 | |
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112 | <p class=MsoListParagraphCxSpMiddle style='text-indent:-.25in;line-height:normal'><span |
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113 | style='font-family:Symbol'>·<span style='font:7.0pt "Times New Roman"'> |
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114 | </span></span><a href="#volume"><b><span style='font-family:"Times New Roman","serif"'>Volume |
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115 | Fraction</span></b></a></p> |
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116 | |
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117 | <p class=MsoListParagraphCxSpMiddle style='text-indent:-.25in;line-height:normal'><span |
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118 | style='font-family:Symbol'>·<span style='font:7.0pt "Times New Roman"'> |
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119 | </span></span><a href="#surface"><b><span style='font-family:"Times New Roman","serif"'>Specific |
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120 | Surface Area</span></b></a></p> |
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121 | |
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122 | <p class=MsoListParagraphCxSpLast style='text-indent:-.25in;line-height:normal'><span |
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123 | style='font-family:Symbol'>·<span style='font:7.0pt "Times New Roman"'> |
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124 | </span></span><a href="#howto"><b><span style='font-family:"Times New Roman","serif"'>How |
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125 | to Compute</span></b></a></p> |
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126 | |
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127 | <p class=MsoNormal style='line-height:normal'><b><span style='font-family:"Times New Roman","serif"'>The |
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128 | scattering <a name=invariant>invariant</a> (Q*)</span></b><span |
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129 | style='font-family:"Times New Roman","serif"'> </span></p> |
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130 | |
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131 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> </span></p> |
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132 | |
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133 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'>The |
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134 | scattering invariant (Q*) is a model-independent quantity that can be easily |
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135 | calculated from </span></p> |
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136 | |
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137 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'>scattering |
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138 | data. For two phase systems, the scattering invariant, Q*, is defined as the |
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139 | integral of</span></p> |
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140 | |
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141 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> the |
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142 | square of the wave transfer (q) multiplied by the scattering cross section over |
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143 | the full range of q. </span></p> |
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144 | |
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145 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'>Q* |
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146 | is given by the following equation, </span></p> |
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147 | |
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148 | <p class=MsoNormal style='line-height:normal'> |
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149 | |
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150 | <table cellpadding=0 cellspacing=0 align=left> |
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151 | <tr> |
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152 | <td width=2 height=4></td> |
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153 | </tr> |
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154 | <tr> |
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155 | <td></td> |
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156 | <td><img width=127 height=35 src="image001.gif"></td> |
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157 | </tr> |
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158 | </table> |
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159 | |
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160 | <span style='font-family:"Times New Roman","serif"'> </span></p> |
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161 | |
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162 | <p class=MsoNormal style='line-height:150%'><span style='font-family:"Times New Roman","serif"'> </span></p> |
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163 | |
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164 | <br clear=ALL> |
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165 | |
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166 | <p class=MsoNormal style='line-height:150%'><span style='font-family:"Times New Roman","serif"'>This |
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167 | model independent quantity (Q*) is calculated from the scattering data that can |
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168 | be used to determine the volume fraction and the specific area of the sample |
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169 | under consideration. These quantities are useful in their own right |
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170 | and can be used in further analysis. With this scattering invariant module |
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171 | users will also be able to determine the consistency of those properties |
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172 | between data. There is no real data defined from zero to infinity, there |
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173 | usually have limited range. Q* is not really computed from zero to infinity. |
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174 | Our maximum q range is 1e-5 ~ 10 (1/A). The lower and/or higher q range than |
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175 | data given can be extrapolated by fitting some data nearby.</span></p> |
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176 | |
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177 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'>The |
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178 | scattering invariant is computed as follow:</span></p> |
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179 | |
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180 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.25in;line-height:normal'><span |
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181 | style='font-family:"Arial","sans-serif"'><span style='font:7.0pt "Times New Roman"'> |
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182 | </span></span><i><span style='font-family:"Times New Roman","serif"'>I(q)</span></i><span |
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183 | style='font-family:"Times New Roman","serif"'> = <i>I(q)</i> w/o background : |
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184 | If the data includes a background, user sets the value to subtract the background |
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185 | for the Q* computation.</span></p> |
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186 | |
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187 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.25in;line-height:normal'><span |
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188 | style='font-family:"Arial","sans-serif"'><span style='font:7.0pt "Times New Roman"'> |
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189 | </span></span><span style='font-family:"Times New Roman","serif"'>Reset<i> |
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190 | I(q) </i></span><span style='font-family:"Times New Roman","serif"'>= <i>I(q)* |
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191 | scaling factor </i>, delta<i>I(q) = </i>delta<i>I(q)*scaling factor</i> : If |
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192 | non-zero scaling factor is given, it will be considered.</span></p> |
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193 | |
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194 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.25in;line-height:normal'><span |
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195 | style='font-family:"Arial","sans-serif"'><span style='font:7.0pt "Times New Roman"'> |
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196 | </span></span><span style='font-family:"Times New Roman","serif"'> Invariant:</span></p> |
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197 | |
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198 | <p class=MsoNormal style='margin-left:.25in;line-height:normal'> |
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199 | |
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200 | <table cellpadding=0 cellspacing=0 align=left> |
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201 | <tr> |
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202 | <td width=45 height=12></td> |
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203 | </tr> |
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204 | <tr> |
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205 | <td></td> |
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206 | <td><img width=127 height=35 src="image001.gif"></td> |
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207 | </tr> |
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208 | </table> |
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209 | |
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210 | <span style='font-family:"Times New Roman","serif"'> </span></p> |
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211 | |
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212 | <br clear=ALL> |
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213 | |
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214 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> </span></p> |
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215 | |
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216 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.5in;line-height:normal'><span |
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217 | style='font-family:"Times New Roman","serif"'> where, <i>g =q</i> |
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218 | for the pinhole geometry and <i>g =<sub> </sub>q<sub>v</sub></i>(the slit |
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219 | height) for the slit geometry which can be given in data or as a value.</span></p> |
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220 | |
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221 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.25in;line-height:normal'><span |
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222 | style='font-family:"Arial","sans-serif"'><span style='font:7.0pt "Times New Roman"'> |
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223 | </span></span><span style='font-family:"Times New Roman","serif"'> Higher |
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224 | q-region (>= qmax in data): </span></p> |
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225 | |
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226 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> Power |
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227 | law (w/o background term) function = C/q<sup>4</sup> will be used </span></p> |
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228 | |
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229 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.5in;line-height:normal'><span |
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230 | style='font-family:"Times New Roman","serif"'> where the constant |
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231 | C(=2pi(delta(rho))S<sub>v</sub>) is to be found by fitting part of data with |
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232 | the range of q<sub>N-m</sub> to q<sub>N</sub> (m<N).</span></p> |
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233 | |
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234 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.25in;line-height:normal'><span |
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235 | style='font-family:"Arial","sans-serif"'><span style='font:7.0pt "Times New Roman"'> |
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236 | </span></span><span style='font-family:"Times New Roman","serif"'> Lower |
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237 | q-region (<= qmin in data): </span></p> |
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238 | |
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239 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> Guinier |
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240 | function = <i>I<sub>0</sub>exp(-R<sub>g</sub><sup>2</sup>q<sup>2</sup>/3)</i> |
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241 | where I<sub>0</sub> and R<sub>g</sub> are obtained by fitting, </span></p> |
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242 | |
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243 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> similarly |
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244 | to the high q region above.</span></p> |
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245 | |
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246 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> Power |
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247 | law can also be used.</span></p> |
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248 | |
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249 | <p class=MsoNormal><span style='font-family:"Times New Roman","serif"'> </span><b>The |
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250 | <a name=volume>volume </a>fraction</b>: </p> |
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251 | |
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252 | <p class=MsoNormal style='line-height:normal'><span style='position:absolute; |
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253 | z-index:3;margin-left:1px;margin-top:9px;width:161px;height:47px'><img |
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254 | width=161 height=47 src="image002.gif"></span><span |
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255 | style='font-family:"Times New Roman","serif"'> </span></p> |
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256 | |
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257 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> </span></p> |
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258 | |
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259 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'>where |
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260 | delta(rho) is the SLD contrast of which value is given by users.</span></p> |
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261 | |
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262 | <p class=MsoNormal style='line-height:normal'><span style='position:absolute; |
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263 | z-index:4;margin-left:1px;margin-top:29px;width:101px;height:45px'><img |
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264 | width=101 height=45 src="image003.gif"></span><span |
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265 | style='font-family:"Times New Roman","serif"'>Thus, </span></p> |
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266 | |
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267 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> </span></p> |
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268 | |
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269 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> </span></p> |
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270 | |
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271 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> where |
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272 | 0 =< <i>A</i> =<1/4 in order for these values to be physically valid.</span></p> |
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273 | |
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274 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> </span></p> |
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275 | |
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276 | <p class=MsoNormal style='line-height:normal'><b><span style='font-family:"Times New Roman","serif"'>The |
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277 | <a name=surface>specific surface area </a>:</span></b></p> |
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278 | |
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279 | <p class=MsoNormal style='line-height:normal'> |
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280 | |
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281 | <table cellpadding=0 cellspacing=0 align=left> |
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282 | <tr> |
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283 | <td width=1 height=3></td> |
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284 | </tr> |
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285 | <tr> |
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286 | <td></td> |
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287 | <td><img width=184 height=47 src="image004.gif"></td> |
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288 | </tr> |
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289 | </table> |
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290 | |
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291 | <b><span style='font-family:"Times New Roman","serif"'> </span></b></p> |
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292 | |
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293 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> </span></p> |
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294 | |
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295 | <br clear=ALL> |
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296 | |
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297 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> where |
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298 | <i>A</i> and <i>Q<sup>*</sup></i> are obtained from previous sections, and the |
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299 | Porod constant <i>C<sub>p</sub></i> is given by users. </span></p> |
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300 | |
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301 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> </span></p> |
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302 | |
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303 | <p class=MsoNormal style='line-height:normal'><b><span style='font-family:"Times New Roman","serif"'>Definitions:</span></b><span |
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304 | style='font-family:"Times New Roman","serif"'> </span></p> |
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305 | |
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306 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'>Q : |
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307 | the magnitude of neutron (or X-ray) momentum transfer vector.</span></p> |
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308 | |
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309 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'>I(Q): |
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310 | the scattering intensity as a function of the momentum transfer Q.</span></p> |
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311 | |
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312 | <p class=MsoNormal style='line-height:150%'><span style='font-family:"Times New Roman","serif"'>Invariant |
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313 | total is the sum of the invariant calculated from datas q range and the |
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314 | invariant resulting from extrapolation at low q range and at high q range if |
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315 | considered.</span></p> |
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316 | |
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317 | <p class=MsoNormal style='line-height:150%'><span style='font-family:"Times New Roman","serif"'> </span></p> |
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318 | |
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319 | <p class=MsoNormal style='line-height:normal'><a name=reference><b><span |
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320 | style='font-family:"Times New Roman","serif"'>Reference</span></b></a><b><span |
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321 | style='font-family:"Times New Roman","serif"'>: </span></b></p> |
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322 | |
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323 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'>Porod's |
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324 | chapter (2) from O. Glatter and O. Kratky, "Small Angle X-Ray |
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325 | Scattering", Academic Press, New York, 1982</span></p> |
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326 | |
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327 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'>Otto's |
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328 | web page: </span><a href="http://physchem.kfunigraz.ac.at/sm/"><span |
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329 | style='font-family:"Times New Roman","serif"'>http://physchem.kfunigraz.ac.at/sm/</span></a><span |
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330 | style='font-family:"Times New Roman","serif"'> </span></p> |
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331 | |
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332 | <p class=MsoNormal style='line-height:normal'><a name=howto><b><span |
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333 | style='font-family:"Times New Roman","serif"'>HowTo</span></b></a><b><span |
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334 | style='font-family:"Times New Roman","serif"'>:</span></b></p> |
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335 | |
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336 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.5in;line-height:normal'><span |
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337 | style='font-family:"Times New Roman","serif"'><span style='font:7.0pt "Times New Roman"'> |
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338 | </span>i)<span style='font:7.0pt "Times New Roman"'> |
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339 | </span></span><span style='font-family:"Times New Roman","serif"'>Loading data |
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340 | to the panel: Open the data file from File in the menu bar. Select loaded data |
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341 | from a plot panel by highlighting that it until its color turns yellow. Then |
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342 | right click on that the data and selects the option Compute Invariant. The |
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343 | application automatically computes the invariant value if the data loaded is |
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344 | valid.</span></p> |
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345 | |
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346 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.5in;line-height:normal'><span |
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347 | style='font-family:"Times New Roman","serif"'><span style='font:7.0pt "Times New Roman"'> |
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348 | </span>ii)<span style='font:7.0pt "Times New Roman"'> |
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349 | </span></span><span style='font-family:"Times New Roman","serif"'>To subtract a |
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350 | background or/and to rescale the data, type the values in Customized Input |
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351 | box. </span></p> |
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352 | |
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353 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.5in;line-height:normal'><span |
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354 | style='font-family:"Times New Roman","serif"'><span style='font:7.0pt "Times New Roman"'> |
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355 | </span>iii)<span style='font:7.0pt "Times New Roman"'> |
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356 | </span></span><span style='font-family:"Times New Roman","serif"'>If you want |
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357 | to calculate the volume fraction and the specific surface area, type the |
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358 | optional inputs in the customized input box, and then press Compute button.</span></p> |
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359 | |
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360 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.5in;line-height:normal'><span |
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361 | style='font-family:"Times New Roman","serif"'><span style='font:7.0pt "Times New Roman"'> |
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362 | </span>iv)<span style='font:7.0pt "Times New Roman"'> |
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363 | </span></span><span style='font-family:"Times New Roman","serif"'>The invariant |
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364 | can also be calculated including the outside of the data Q range: To include |
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365 | the lower Q and/or the higher Q range, check in the enable extrapolation check |
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366 | box in Extrapolation box. If the power low is chosen, the power (exponent) |
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367 | can be either held or fitted by checking the corresponding radio button. The |
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368 | Npts that is being used for the extrapolation can be specified.</span></p> |
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369 | |
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370 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.5in;line-height:normal'><span |
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371 | style='font-family:"Times New Roman","serif"'><span style='font:7.0pt "Times New Roman"'> |
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372 | </span>v)<span style='font:7.0pt "Times New Roman"'> |
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373 | </span></span><span style='font-family:"Times New Roman","serif"'>If the |
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374 | invariant calculated from the extrapolated region is too large, it will be warn |
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375 | in red at the top of the panel, which means that your data is not proper to |
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376 | calculate the invariant.</span></p> |
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377 | |
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378 | <p class=MsoNormal style='margin-left:.5in;text-indent:-.5in;line-height:normal'><span |
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379 | style='font-family:"Times New Roman","serif"'><span style='font:7.0pt "Times New Roman"'> |
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380 | </span>vi)<span style='font:7.0pt "Times New Roman"'> |
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381 | </span></span><span style='font-family:"Times New Roman","serif"'>The details |
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382 | of the calculation is available by clicking the Details button in the middle |
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383 | of the panel. </span></p> |
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384 | |
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385 | <p class=MsoNormal align=center style='text-align:center;line-height:normal'><span |
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386 | style='font-family:"Times New Roman","serif"'><img border=0 width=572 |
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387 | height=449 id="Object 4" src="image005.gif"></span></p> |
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388 | |
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389 | <p class=MsoNormal style='line-height:normal'><span style='font-family:"Times New Roman","serif"'> </span></p> |
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390 | |
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391 | </div> |
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392 | |
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393 | </body> |
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394 | |
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395 | </html> |
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