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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>2.1.1.1. Barbell</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-cylinder.html">2.1.1. Cylinder 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="capped_cylinder.html">2.1.1.2. Capped cylinder</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="barbell"> |
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52 | <span id="id1"></span><h1>2.1.1.1. Barbell<a class="headerlink" href="#barbell" title="Permalink to this headline">¶</a></h1> |
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53 | <p>Cylinder with spherical end caps</p> |
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54 | <table border="1" class="docutils"> |
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55 | <colgroup> |
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56 | <col width="16%" /> |
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57 | <col width="48%" /> |
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58 | <col width="17%" /> |
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59 | <col width="19%" /> |
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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>Barbell 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>bell_radius</td> |
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90 | <td>Spherical bell radius</td> |
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91 | <td>â«</td> |
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92 | <td>40</td> |
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93 | </tr> |
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94 | <tr class="row-odd"><td>radius</td> |
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95 | <td>Cylindrical bar radius</td> |
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96 | <td>â«</td> |
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97 | <td>20</td> |
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98 | </tr> |
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99 | <tr class="row-even"><td>length</td> |
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100 | <td>Cylinder bar length</td> |
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101 | <td>â«</td> |
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102 | <td>400</td> |
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103 | </tr> |
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104 | <tr class="row-odd"><td>theta</td> |
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105 | <td>In 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 | <tr class="row-even"><td>phi</td> |
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110 | <td>Out of plane angle</td> |
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111 | <td>degree</td> |
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112 | <td>60</td> |
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113 | </tr> |
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114 | </tbody> |
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115 | </table> |
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116 | <p>The returned value is scaled to units of cm<sup>-1</sup>.</p> |
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117 | <p>Calculates the scattering from a barbell-shaped cylinder (This model simply |
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118 | becomes the DumBellModel when the length of the cylinder, <em>L</em>, is set to zero). |
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119 | That is, a sphereocylinder with spherical end caps that have a radius larger |
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120 | than that of the cylinder and the center of the end cap radius lies outside |
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121 | of the cylinder. All dimensions of the BarBell are considered to be |
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122 | monodisperse. See the diagram for the details of the geometry and restrictions |
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123 | on parameter values.</p> |
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124 | <div class="section" id="definition"> |
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125 | <h2>Definition<a class="headerlink" href="#definition" title="Permalink to this headline">¶</a></h2> |
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126 | <p>The returned value is scaled to units of cm<sup>-1</sup>sr<sup>-1</sup>, absolute scale.</p> |
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127 | <p>The barbell geometry is defined as</p> |
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128 | <img alt="../_images/barbell_geometry.jpg" src="../_images/barbell_geometry.jpg" /> |
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129 | <p>where <em>r</em> is the radius of the cylinder. All other parameters are as defined |
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130 | in the diagram.</p> |
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131 | <p>Since the end cap radius |
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132 | <em>R</em> >= <em>r</em> and by definition for this geometry <em>h</em> < 0, <em>h</em> is then |
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133 | defined by <em>r</em> and <em>R</em> as</p> |
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134 | <p><em>h</em> = -1 * sqrt(<em>R</em><sup>2</sup> - <em>r</em><sup>2</sup>)</p> |
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135 | <p>The scattered intensity <em>I(q)</em> is calculated as</p> |
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136 | <div class="math"> |
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137 | \[\begin{split}I(Q) = \frac{(\Delta \rho)^2}{V} \left< A^2(Q)\right>\end{split}\]</div> |
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138 | <p>where the amplitude <em>A(q)</em> is given as</p> |
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139 | <div class="math"> |
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140 | \[\begin{split}A(Q) =&\ \pi r^2L |
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141 | {\sin\left(\tfrac12 QL\cos\theta\right) |
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142 | \over \tfrac12 QL\cos\theta} |
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143 | {2 J_1(Qr\sin\theta) \over Qr\sin\theta} \\ |
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144 | &\ + 4 \pi R^3 \int_{-h/R}^1 dt |
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145 | \cos\left[ Q\cos\theta |
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146 | \left(Rt + h + {\tfrac12} L\right)\right] |
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147 | \times (1-t^2) |
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148 | {J_1\left[QR\sin\theta \left(1-t^2\right)^{1/2}\right] |
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149 | \over QR\sin\theta \left(1-t^2\right)^{1/2}}\end{split}\]</div> |
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150 | <p>The < > brackets denote an average of the structure over all orientations. |
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151 | <<em>A</em> <sup>2</sup><em>(q)</em>> is then the form factor, <em>P(q)</em>. The scale factor is |
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152 | equivalent to the volume fraction of cylinders, each of volume, <em>V</em>. Contrast |
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153 | is the difference of scattering length densities of the cylinder and the |
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154 | surrounding solvent.</p> |
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155 | <p>The volume of the barbell is</p> |
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156 | <div class="math"> |
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157 | \[V = \pi r_c^2 L + 2\pi\left(\tfrac23R^3 + R^2h-\tfrac13h^3\right)\]</div> |
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158 | <p>and its radius-of-gyration is</p> |
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159 | <div class="math"> |
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160 | \[\begin{split}R_g^2 =&\ \left[ \tfrac{12}{5}R^5 |
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161 | + R^4\left(6h+\tfrac32 L\right) |
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162 | + R^2\left(4h^2 + L^2 + 4Lh\right) |
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163 | + R^2\left(3Lh^2 + \tfrac32 L^2h\right) \right. \\ |
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164 | &\ \left. + \tfrac25 h^5 - \tfrac12 Lh^4 - \tfrac12 L^2h^3 |
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165 | + \tfrac14 L^3r^2 + \tfrac32 Lr^4 \right] |
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166 | \left( 4R^3 6R^2h - 2h^3 + 3r^2L \right)^{-1}\end{split}\]</div> |
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167 | <p><strong>The requirement that</strong> <em>R</em> >= <em>r</em> <strong>is not enforced in the model!</strong> It is |
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168 | up to you to restrict this during analysis.</p> |
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169 | <p>This example dataset is produced by running the Macro PlotBarbell(), |
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170 | using 200 data points, <em>qmin</em> = 0.001 â«<sup>-1</sup>, <em>qmax</em> = 0.7 â«<sup>-1</sup>, |
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171 | <em>sld</em> = 4e-6 â«<sup>-2</sup> and the default model values.</p> |
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172 | <img alt="../_images/barbell_1d.jpg" src="../_images/barbell_1d.jpg" /> |
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173 | <p><em>Figure. 1D plot using the default values (w/256 data point).</em></p> |
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174 | <p>For 2D data: The 2D scattering intensity is calculated similar to the 2D |
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175 | cylinder model. For example, for Ξ = 45 deg and Ï = 0 deg with |
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176 | default values for other parameters</p> |
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177 | <img alt="../_images/barbell_2d.jpg" src="../_images/barbell_2d.jpg" /> |
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178 | <p><em>Figure. 2D plot (w/(256X265) data points).</em></p> |
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179 | <img alt="../_images/orientation.jpg" src="../_images/orientation.jpg" /> |
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180 | <p>Figure. Definition of the angles for oriented 2D barbells.</p> |
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181 | <img alt="../_images/orientation2.jpg" src="../_images/orientation2.jpg" /> |
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182 | <p><em>Figure. Examples of the angles for oriented pp against the detector plane.</em></p> |
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183 | </div> |
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184 | <div class="section" id="reference"> |
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185 | <h2>REFERENCE<a class="headerlink" href="#reference" title="Permalink to this headline">¶</a></h2> |
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186 | <p>H Kaya, <em>J. Appl. Cryst.</em>, 37 (2004) 37 223-230</p> |
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187 | <p>H Kaya and N R deSouza, <em>J. Appl. Cryst.</em>, 37 (2004) 508-509 (addenda and errata)</p> |
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188 | </div> |
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189 | </div> |
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190 | |
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194 | |
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195 | <p> |
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196 | «  <a href="../ref/models/shape-cylinder.html">2.1.1. Cylinder Functions</a> |
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197 |   ::   |
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199 |   ::   |
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200 | <a href="capped_cylinder.html">2.1.1.2. Capped cylinder</a>  Â» |
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