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32 | <body> |
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33 | <div class="header"><h1 class="heading"><a href="../index.html"> |
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34 | <span>Home</span></a></h1> |
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35 | <h2 class="heading"><span>2.1.2.1. Ellipsoid</span></h2> |
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36 | </div> |
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37 | <div class="topnav"> |
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38 | |
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39 | <p> |
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40 | «  <a href="../ref/models/shape-ellipsoid.html">2.1.2. Ellipsoid Functions</a> |
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41 |   ::   |
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42 | <a class="uplink" href="../index.html">Contents</a> |
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43 |   ::   |
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44 | <a href="triaxial_ellipsoid.html">2.1.2.2. Triaxial ellipsoid</a>  Â» |
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45 | </p> |
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46 | |
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47 | </div> |
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48 | <div class="content"> |
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49 | |
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50 | |
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51 | <div class="section" id="ellipsoid"> |
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52 | <span id="id1"></span><h1>2.1.2.1. Ellipsoid<a class="headerlink" href="#ellipsoid" title="Permalink to this headline">¶</a></h1> |
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53 | <p>Ellipsoid of revolution with uniform scattering length density.</p> |
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54 | <table border="1" class="docutils"> |
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55 | <colgroup> |
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56 | <col width="15%" /> |
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57 | <col width="49%" /> |
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58 | <col width="17%" /> |
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59 | <col width="18%" /> |
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60 | </colgroup> |
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61 | <thead valign="bottom"> |
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62 | <tr class="row-odd"><th class="head">Parameter</th> |
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63 | <th class="head">Description</th> |
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64 | <th class="head">Units</th> |
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65 | <th class="head">Default value</th> |
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66 | </tr> |
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67 | </thead> |
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68 | <tbody valign="top"> |
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69 | <tr class="row-even"><td>scale</td> |
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70 | <td>Source intensity</td> |
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71 | <td>None</td> |
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72 | <td>1</td> |
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73 | </tr> |
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74 | <tr class="row-odd"><td>background</td> |
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75 | <td>Source background</td> |
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76 | <td>cm<sup>-1</sup></td> |
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77 | <td>0</td> |
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78 | </tr> |
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79 | <tr class="row-even"><td>sld</td> |
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80 | <td>Ellipsoid scattering length density</td> |
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81 | <td>10<sup>-6</sup>â«<sup>-2</sup></td> |
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82 | <td>4</td> |
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83 | </tr> |
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84 | <tr class="row-odd"><td>solvent_sld</td> |
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85 | <td>Solvent scattering length density</td> |
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86 | <td>10<sup>-6</sup>â«<sup>-2</sup></td> |
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87 | <td>1</td> |
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88 | </tr> |
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89 | <tr class="row-even"><td>rpolar</td> |
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90 | <td>Polar radius</td> |
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91 | <td>â«</td> |
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92 | <td>20</td> |
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93 | </tr> |
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94 | <tr class="row-odd"><td>requatorial</td> |
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95 | <td>Equatorial radius</td> |
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96 | <td>â«</td> |
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97 | <td>400</td> |
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98 | </tr> |
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99 | <tr class="row-even"><td>theta</td> |
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100 | <td>In plane angle</td> |
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101 | <td>degree</td> |
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102 | <td>60</td> |
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103 | </tr> |
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104 | <tr class="row-odd"><td>phi</td> |
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105 | <td>Out of plane angle</td> |
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106 | <td>degree</td> |
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107 | <td>60</td> |
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108 | </tr> |
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109 | </tbody> |
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110 | </table> |
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111 | <p>The returned value is scaled to units of cm<sup>-1</sup>.</p> |
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112 | <p>The form factor is normalized by the particle volume.</p> |
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113 | <div class="section" id="definition"> |
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114 | <h2>Definition<a class="headerlink" href="#definition" title="Permalink to this headline">¶</a></h2> |
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115 | <p>The output of the 2D scattering intensity function for oriented ellipsoids |
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116 | is given by (Feigin, 1987)</p> |
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117 | <div class="math"> |
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118 | \[P(Q,\alpha) = {\text{scale} \over V} F^2(Q) + \text{background}\]</div> |
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119 | <p>where</p> |
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120 | <div class="math"> |
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121 | \[F(Q) = {3 (\Delta rho)) V (\sin[Qr(R_p,R_e,\alpha)] |
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122 | - \cos[Qr(R_p,R_e,\alpha)]) |
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123 | \over [Qr(R_p,R_e,\alpha)]^3 }\]</div> |
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124 | <p>and</p> |
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125 | <div class="math"> |
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126 | \[r(R_p,R_e,\alpha) = \left[ R_e^2 \sin^2 \alpha |
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127 | + R_p^2 \cos^2 \alpha \right]^{1/2}\]</div> |
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128 | <p><span class="math">\(\alpha\)</span> is the angle between the axis of the ellipsoid and <span class="math">\(\vec q\)</span>, |
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129 | <span class="math">\(V\)</span> is the volume of the ellipsoid, <span class="math">\(R_p\)</span> is the polar radius along the |
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130 | rotational axis of the ellipsoid, <span class="math">\(R_e\)</span> is the equatorial radius perpendicular |
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131 | to the rotational axis of the ellipsoid and <span class="math">\(\Delta \rho\)</span> (contrast) is the |
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132 | scattering length density difference between the scatterer and the solvent.</p> |
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133 | <p>To provide easy access to the orientation of the ellipsoid, we define |
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134 | the rotation axis of the ellipsoid using two angles <span class="math">\(\theta\)</span> and <span class="math">\(\phi\)</span>. |
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135 | These angles are defined in the |
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136 | <a class="reference internal" href="cylinder.html#cylinder-orientation"><em>cylinder orientation figure</em></a>. |
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137 | For the ellipsoid, <span class="math">\(\theta\)</span> is the angle between the rotational axis |
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138 | and the $z$-axis.</p> |
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139 | <p>NB: The 2nd virial coefficient of the solid ellipsoid is calculated based |
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140 | on the <span class="math">\(R_p\)</span> and <span class="math">\(R_e\)</span> values, and used as the effective radius for |
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141 | <span class="math">\(S(Q)\)</span> when <span class="math">\(P(Q) \cdot S(Q)\)</span> is applied.</p> |
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142 | <div class="figure" id="ellipsoid-1d"> |
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143 | <img alt="../_images/ellipsoid_1d.JPG" src="../_images/ellipsoid_1d.JPG" /> |
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144 | <p class="caption">Figure 1: The output of the 1D scattering intensity function for randomly oriented |
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145 | ellipsoids given by the equation above.</p> |
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146 | </div> |
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147 | <p>The <span class="math">\(\theta\)</span> and <span class="math">\(\phi\)</span> parameters are not used for the 1D output. Our |
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148 | implementation of the scattering kernel and the 1D scattering intensity |
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149 | use the c-library from NIST.</p> |
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150 | <div class="figure" id="ellipsoid-geometry"> |
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151 | <img alt="../_images/ellipsoid_geometry.JPG" src="../_images/ellipsoid_geometry.JPG" /> |
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152 | <p class="caption">Figure 2: The angles for oriented ellipsoid.</p> |
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153 | </div> |
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154 | </div> |
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155 | <div class="section" id="validation"> |
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156 | <h2>Validation<a class="headerlink" href="#validation" title="Permalink to this headline">¶</a></h2> |
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157 | <p>Validation of our code was done by comparing the output of the 1D model |
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158 | to the output of the software provided by the NIST (Kline, 2006). |
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159 | below shows a comparison of |
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160 | the 1D output of our model and the output of the NIST software.</p> |
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161 | <div class="figure" id="ellipsoid-comparison-1d"> |
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162 | <img alt="../_images/ellipsoid_comparison_1d.jpg" src="../_images/ellipsoid_comparison_1d.jpg" /> |
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163 | <p class="caption">Figure 3: Comparison of the SasView scattering intensity for an ellipsoid |
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164 | with the output of the NIST SANS analysis software. The parameters |
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165 | were set to: <em>scale</em> = 1.0, <em>rpolar</em> = 20 â«, |
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166 | <em>requatorial</em> =400 â«, <em>contrast</em> = 3e-6 â«<sup>-2</sup>, |
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167 | and <em>background</em> = 0.01 cm<sup>-1</sup>.</p> |
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168 | </div> |
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169 | <p>Averaging over a distribution of orientation is done by evaluating the |
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170 | equation above. Since we have no other software to compare the |
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171 | implementation of the intensity for fully oriented ellipsoids, we can |
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172 | compare the result of averaging our 2D output using a uniform distribution |
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173 | <span class="math">\(p(\theta,\phi) = 1.0\)</span>. <a class="pageref" href="#ellipsoid-comparison-2d">Figure 4</a> |
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174 | shows the result of such a cross-check.</p> |
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175 | <div class="figure" id="ellipsoid-comparison-2d"> |
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176 | <img alt="../_images/ellipsoid_comparison_2d.jpg" src="../_images/ellipsoid_comparison_2d.jpg" /> |
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177 | <p class="caption">Figure 4: Comparison of the intensity for uniformly distributed ellipsoids |
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178 | calculated from our 2D model and the intensity from the NIST SANS |
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179 | analysis software. The parameters used were: <em>scale</em> = 1.0, |
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180 | <em>rpolar</em> = 20 â«, <em>requatorial</em> = 400 â«, |
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181 | <em>contrast</em> = 3e-6 â«<sup>-2</sup>, and <em>background</em> = 0.0 cm<sup>-1</sup>.</p> |
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182 | </div> |
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183 | <p>The discrepancy above <em>q</em> = 0.3 cm<sup>-1</sup> is due to the way the form factors |
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184 | are calculated in the c-library provided by NIST. A numerical integration |
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185 | has to be performed to obtain <span class="math">\(P(Q)\)</span> for randomly oriented particles. |
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186 | The NIST software performs that integration with a 76-point Gaussian |
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187 | quadrature rule, which will become imprecise at high <span class="math">\(Q\)</span> where the amplitude |
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188 | varies quickly as a function of <span class="math">\(Q\)</span>. The SasView result shown has been |
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189 | obtained by summing over 501 equidistant points. Our result was found |
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190 | to be stable over the range of <span class="math">\(Q\)</span> shown for a number of points higher |
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191 | than 500.</p> |
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192 | <p>REFERENCE</p> |
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193 | <p>L A Feigin and D I Svergun. <em>Structure Analysis by Small-Angle X-Ray and Neutron Scattering</em>, Plenum, |
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194 | New York, 1987.</p> |
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195 | </div> |
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196 | </div> |
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197 | |
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198 | |
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199 | </div> |
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200 | <div class="bottomnav"> |
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201 | |
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202 | <p> |
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203 | «  <a href="../ref/models/shape-ellipsoid.html">2.1.2. Ellipsoid Functions</a> |
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204 |   ::   |
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205 | <a class="uplink" href="../index.html">Contents</a> |
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206 |   ::   |
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207 | <a href="triaxial_ellipsoid.html">2.1.2.2. Triaxial ellipsoid</a>  Â» |
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208 | </p> |
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