1 | /** |
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2 | This software was developed by the University of Tennessee as part of the |
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3 | Distributed Data Analysis of Neutron Scattering Experiments (DANSE) |
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4 | project funded by the US National Science Foundation. |
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5 | |
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6 | If you use DANSE applications to do scientific research that leads to |
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7 | publication, we ask that you acknowledge the use of the software with the |
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8 | following sentence: |
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9 | |
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10 | "This work benefited from DANSE software developed under NSF award DMR-0520547." |
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11 | |
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12 | copyright 2008, University of Tennessee |
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13 | */ |
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14 | |
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15 | /** |
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16 | * Scattering model classes |
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17 | * The classes use the IGOR library found in |
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18 | * sansmodels/src/libigor |
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19 | * |
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20 | * TODO: refactor so that we pull in the old sansmodels.c_extensions |
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21 | * TODO: add 2D function |
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22 | */ |
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23 | |
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24 | #include <math.h> |
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25 | #include "parameters.hh" |
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26 | #include <stdio.h> |
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27 | #include <stdlib.h> |
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28 | using namespace std; |
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29 | #include "lamellarPS.h" |
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30 | |
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31 | extern "C" { |
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32 | #include "libCylinder.h" |
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33 | } |
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34 | |
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35 | /*LamellarPS_kernel() was moved from libigor to get rid of polydipersity in del(thickness) that we provide from control panel. |
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36 | LamellarPSX : calculates the form factor of a lamellar structure - with S(q) effects included |
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37 | ------- |
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38 | ------- resolution effects ARE NOT included, but only a CONSTANT default value, not the real q-dependent resolution!! |
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39 | |
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40 | */ |
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41 | static double LamellarPS_kernel(double dp[], double q) |
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42 | { |
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43 | double scale,dd,del,sld_bi,sld_sol,contr,NN,Cp,bkg; //local variables of coefficient wave |
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44 | double inten, qval,Pq,Sq,alpha,temp,t1,t2,t3,dQ; |
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45 | double Pi,Euler,dQDefault,fii; |
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46 | int ii,NNint; |
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47 | Euler = 0.5772156649; // Euler's constant |
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48 | dQDefault = 0.0; //[=] 1/A, q-resolution, default value |
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49 | dQ = dQDefault; |
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50 | |
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51 | Pi = 4.0*atan(1.0); |
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52 | qval = q; |
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53 | |
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54 | scale = dp[0]; |
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55 | dd = dp[1]; |
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56 | del = dp[2]; |
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57 | sld_bi = dp[3]; |
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58 | sld_sol = dp[4]; |
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59 | NN = trunc(dp[5]); //be sure that NN is an integer |
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60 | Cp = dp[6]; |
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61 | bkg = dp[7]; |
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62 | |
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63 | contr = sld_bi - sld_sol; |
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64 | |
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65 | Pq = 2.0*contr*contr/qval/qval*(1.0-cos(qval*del)); |
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66 | |
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67 | NNint = (int)NN; //cast to an integer for the loop |
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68 | ii=0; |
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69 | Sq = 0.0; |
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70 | for(ii=1;ii<=(NNint-1);ii+=1) { |
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71 | |
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72 | fii = (double)ii; //do I really need to do this? |
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73 | |
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74 | temp = 0.0; |
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75 | alpha = Cp/4.0/Pi/Pi*(log(Pi*ii) + Euler); |
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76 | t1 = 2.0*dQ*dQ*dd*dd*alpha; |
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77 | t2 = 2.0*qval*qval*dd*dd*alpha; |
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78 | t3 = dQ*dQ*dd*dd*ii*ii; |
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79 | |
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80 | temp = 1.0-ii/NN; |
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81 | temp *= cos(dd*qval*ii/(1.0+t1)); |
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82 | temp *= exp(-1.0*(t2 + t3)/(2.0*(1.0+t1)) ); |
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83 | temp /= sqrt(1.0+t1); |
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84 | |
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85 | Sq += temp; |
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86 | } |
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87 | |
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88 | Sq *= 2.0; |
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89 | Sq += 1.0; |
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90 | |
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91 | inten = 2.0*Pi*scale*Pq*Sq/(dd*qval*qval); |
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92 | |
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93 | inten *= 1.0e8; // 1/A to 1/cm |
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94 | |
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95 | return(inten+bkg); |
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96 | } |
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97 | |
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98 | LamellarPSModel :: LamellarPSModel() { |
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99 | scale = Parameter(1.0); |
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100 | spacing = Parameter(400.0, true); |
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101 | spacing.set_min(0.0); |
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102 | delta = Parameter(30.0); |
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103 | delta.set_min(0.0); |
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104 | sld_bi = Parameter(6.3e-6); |
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105 | sld_sol = Parameter(1.0e-6); |
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106 | n_plates = Parameter(20.0); |
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107 | caille = Parameter(0.1); |
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108 | background = Parameter(0.0); |
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109 | |
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110 | } |
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111 | |
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112 | /** |
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113 | * Function to evaluate 1D scattering function |
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114 | * The NIST IGOR library is used for the actual calculation. |
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115 | * @param q: q-value |
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116 | * @return: function value |
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117 | */ |
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118 | double LamellarPSModel :: operator()(double q) { |
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119 | double dp[8]; |
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120 | |
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121 | // Fill parameter array for IGOR library |
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122 | // Add the background after averaging |
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123 | dp[0] = scale(); |
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124 | dp[1] = spacing(); |
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125 | dp[2] = delta(); |
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126 | dp[3] = sld_bi(); |
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127 | dp[4] = sld_sol(); |
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128 | dp[5] = n_plates(); |
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129 | dp[6] = caille(); |
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130 | dp[7] = 0.0; |
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131 | |
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132 | |
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133 | // Get the dispersion points for spacing and delta (thickness) |
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134 | vector<WeightPoint> weights_spacing; |
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135 | spacing.get_weights(weights_spacing); |
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136 | vector<WeightPoint> weights_delta; |
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137 | delta.get_weights(weights_delta); |
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138 | |
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139 | // Perform the computation, with all weight points |
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140 | double sum = 0.0; |
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141 | double norm = 0.0; |
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142 | |
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143 | // Loop over short_edgeA weight points |
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144 | for(int i=0; i< (int)weights_spacing.size(); i++) { |
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145 | dp[1] = weights_spacing[i].value; |
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146 | //for(int j=0; j< (int)weights_spacing.size(); j++) { BUGS fixed March 2015 |
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147 | for(int j=0; j< (int)weights_delta.size(); j++) { |
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148 | //dp[2] = weights_delta[i].value; BUG |
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149 | dp[2] = weights_delta[j].value; |
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150 | |
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151 | sum += weights_spacing[i].weight * weights_delta[j].weight * LamellarPS_kernel(dp, q); |
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152 | norm += weights_spacing[i].weight * weights_delta[j].weight; |
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153 | } |
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154 | } |
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155 | return sum/norm + background(); |
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156 | } |
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157 | /** |
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158 | * Function to evaluate 2D scattering function |
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159 | * @param q_x: value of Q along x |
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160 | * @param q_y: value of Q along y |
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161 | * @return: function value |
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162 | */ |
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163 | double LamellarPSModel :: operator()(double qx, double qy) { |
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164 | double q = sqrt(qx*qx + qy*qy); |
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165 | return (*this).operator()(q); |
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166 | } |
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167 | |
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168 | /** |
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169 | * Function to evaluate 2D scattering function |
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170 | * @param pars: parameters of the cylinder |
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171 | * @param q: q-value |
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172 | * @param phi: angle phi |
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173 | * @return: function value |
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174 | */ |
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175 | double LamellarPSModel :: evaluate_rphi(double q, double phi) { |
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176 | return (*this).operator()(q); |
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177 | } |
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178 | /** |
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179 | * Function to calculate effective radius |
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180 | * @return: effective radius value |
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181 | */ |
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182 | double LamellarPSModel :: calculate_ER() { |
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183 | //NOT implemented yet!!! |
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184 | return 0.0; |
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185 | } |
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186 | double LamellarPSModel :: calculate_VR() { |
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187 | return 1.0; |
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188 | } |
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