Changeset 50a77df in sasview for src/sas/models
- Timestamp:
- Mar 15, 2016 11:18:39 AM (9 years ago)
- Branches:
- master, ESS_GUI, ESS_GUI_Docs, ESS_GUI_batch_fitting, ESS_GUI_bumps_abstraction, ESS_GUI_iss1116, ESS_GUI_iss879, ESS_GUI_iss959, ESS_GUI_opencl, ESS_GUI_ordering, ESS_GUI_sync_sascalc, costrafo411, magnetic_scatt, release-4.1.1, release-4.1.2, release-4.2.2, release_4.0.1, ticket-1009, ticket-1094-headless, ticket-1242-2d-resolution, ticket-1243, ticket-1249, ticket885, unittest-saveload
- Children:
- f66d9d1
- Parents:
- 02098e3 (diff), 0b63c6e (diff)
Note: this is a merge changeset, the changes displayed below correspond to the merge itself.
Use the (diff) links above to see all the changes relative to each parent. - Location:
- src/sas/models
- Files:
-
- 3 edited
Legend:
- Unmodified
- Added
- Removed
-
src/sas/models/c_extension/c_models/barbell.cpp
r79492222 rdb46d13 30 30 #include "barbell.h" 31 31 } 32 33 // Convenience parameter structure 34 typedef struct { 35 double scale; 36 double rad_bar; 37 double len_bar; 38 double rad_bell; 39 double sld_barbell; 40 double sld_solv; 41 double background; 42 double theta; 43 double phi; 44 } BarBellParameters; 32 45 33 46 BarBellModel :: BarBellModel() { … … 46 59 } 47 60 48 double bar 2d_kernel(double dp[], double q, double alpha) {61 double barbell2d_kernel(double dp[], double q, double alpha) { 49 62 int j; 50 63 double Pi; … … 113 126 return answer; 114 127 } 128 129 /** 130 * Function to evaluate 2D scattering function 131 * @param pars: parameters of the BarBell 132 * @param q: q-value 133 * @param q_x: q_x / q 134 * @param q_y: q_y / q 135 * @return: function value 136 */ 137 static double barbell_analytical_2D_scaled(BarBellParameters *pars, double q, double q_x, double q_y) { 138 double cyl_x, cyl_y;//, cyl_z; 139 //double q_z; 140 double alpha, cos_val; 141 double answer; 142 double dp[7]; 143 //convert angle degree to radian 144 double pi = 4.0*atan(1.0); 145 double theta = pars->theta * pi/180.0; 146 double phi = pars->phi * pi/180.0; 147 148 dp[0] = pars->scale; 149 dp[1] = pars->rad_bar; 150 dp[2] = pars->len_bar; 151 dp[3] = pars->rad_bell; 152 dp[4] = pars->sld_barbell; 153 dp[5] = pars->sld_solv; 154 dp[6] = pars->background; 155 156 157 //double Pi = 4.0*atan(1.0); 158 // Cylinder orientation 159 cyl_x = cos(theta) * cos(phi); 160 cyl_y = sin(theta); 161 //cyl_z = -cos(theta) * sin(phi); 162 163 // q vector 164 //q_z = 0; 165 166 // Compute the angle btw vector q and the 167 // axis of the cylinder 168 cos_val = cyl_x*q_x + cyl_y*q_y;// + cyl_z*q_z; 169 170 // The following test should always pass 171 if (fabs(cos_val)>1.0) { 172 printf("cyl_ana_2D: Unexpected error: cos(alpha)>1\n"); 173 return 0; 174 } 175 176 // Note: cos(alpha) = 0 and 1 will get an 177 // undefined value from CylKernel 178 alpha = acos( cos_val ); 179 180 answer = barbell2d_kernel(dp, q, alpha); 181 182 183 return answer; 184 185 } 186 187 /** 188 * Function to evaluate 2D scattering function 189 * @param pars: parameters of the BarBell 190 * @param q: q-value 191 * @return: function value 192 */ 193 static double barbell_analytical_2DXY(BarBellParameters *pars, double qx, double qy){ 194 double q; 195 q = sqrt(qx*qx+qy*qy); 196 return barbell_analytical_2D_scaled(pars, q, qx/q, qy/q); 197 } 198 115 199 /** 116 200 * Function to evaluate 1D scattering function … … 190 274 */ 191 275 double BarBellModel :: operator()(double qx, double qy) { 192 double dp[7]; 193 194 // Fill parameter array for IGOR library 195 // Add the background after averaging 196 dp[0] = scale(); 197 dp[1] = rad_bar(); 198 dp[2] = len_bar(); 199 dp[3] = rad_bell(); 200 dp[4] = sld_barbell(); 201 dp[5] = sld_solv(); 202 dp[6] = 0.0; 203 204 double _theta = theta(); 205 double _phi = phi(); 276 BarBellParameters dp; 277 278 // Fill parameter array for IGOR library 279 // Add the background after averaging 280 dp.scale = scale(); 281 dp.rad_bar = rad_bar(); 282 dp.len_bar = len_bar(); 283 dp.rad_bell = rad_bell(); 284 dp.sld_barbell = sld_barbell(); 285 dp.sld_solv = sld_solv(); 286 dp.background = 0.0; 287 dp.theta = theta(); 288 dp.phi = phi(); 206 289 207 290 // Get the dispersion points for the rad_bar … … 237 320 // Loop over radius weight points 238 321 for(size_t i=0; i<weights_rad_bar.size(); i++) { 239 dp [1]= weights_rad_bar[i].value;322 dp.rad_bar = weights_rad_bar[i].value; 240 323 for(size_t j=0; j<weights_len_bar.size(); j++) { 241 dp [2]= weights_len_bar[j].value;324 dp.len_bar = weights_len_bar[j].value; 242 325 for(size_t k=0; k<weights_rad_bell.size(); k++) { 243 dp [3]= weights_rad_bell[k].value;326 dp.rad_bell = weights_rad_bell[k].value; 244 327 // Average over theta distribution 245 328 for(size_t l=0; l< weights_theta.size(); l++) { 246 _theta = weights_theta[l].value;329 dp.theta = weights_theta[l].value; 247 330 // Average over phi distribution 248 331 for(size_t m=0; m< weights_phi.size(); m++) { 249 _phi = weights_phi[m].value;332 dp.phi = weights_phi[m].value; 250 333 //Un-normalize Form by volume 251 hDist = sqrt(fabs(dp[3]*dp[3]-dp[1]*dp[1])); 252 vol_i = pi*dp[1]*dp[1]*dp[2]+2.0*pi*(2.0*dp[3]*dp[3]*dp[3]/3.0 253 +dp[3]*dp[3]*hDist-hDist*hDist*hDist/3.0); 254 255 const double q = sqrt(qx*qx+qy*qy); 256 //convert angle degree to radian 257 const double pi = 4.0*atan(1.0); 258 259 // Cylinder orientation 260 const double cyl_x = cos(_theta * pi/180.0) * cos(_phi * pi/180.0); 261 const double cyl_y = sin(_theta * pi/180.0); 262 263 // Compute the angle btw vector q and the 264 // axis of the cylinder (assume qz = 0) 265 const double cos_val = cyl_x*qx + cyl_y*qy; 266 267 // The following test should always pass 268 if (fabs(cos_val)>1.0) { 269 return 0; 270 } 271 272 // Note: cos(alpha) = 0 and 1 will get an 273 // undefined value from CylKernel 274 const double alpha = acos( cos_val ); 275 276 // Call the IGOR library function to get the kernel 277 const double output = bar2d_kernel(dp, q, alpha)/sin(alpha); 278 334 hDist = -sqrt(fabs(dp.rad_bell*dp.rad_bell-dp.rad_bar*dp.rad_bar)); 335 vol_i = pi*dp.rad_bar*dp.rad_bar*dp.len_bar+2.0*pi/3.0*((dp.rad_bell-hDist)*(dp.rad_bell-hDist)* 336 (2*dp.rad_bell+hDist)); 279 337 double _ptvalue = weights_rad_bar[i].weight 280 338 * weights_len_bar[j].weight … … 283 341 * weights_phi[m].weight 284 342 * vol_i 285 * output; 343 * barbell_analytical_2DXY(&dp, qx, qy); 344 //* output; 286 345 //* pow(weights_rad[i].value,3.0); 287 346 -
src/sas/models/smearing_2d.py
rfd5ac0d rb699768 240 240 dz = numpy.sqrt(z) 241 241 242 from sas. dataloader import Data2D242 from sas.sascalc.dataloader import Data2D 243 243 #for i in range(10): print i, 0.001 + i*0.008/9.0 244 244 #for i in range(100): print i, int(math.floor( (i/ (100/9.0)) )) -
src/sas/models/dispersion_models.py
rfd5ac0d r0e4e554 154 154 c_models.set_dispersion_weights(self.cdisp, values, weights) 155 155 156 models = {"gaussian":GaussianDispersion, "rectangula ":RectangleDispersion,156 models = {"gaussian":GaussianDispersion, "rectangular":RectangleDispersion, 157 157 "array":ArrayDispersion, "schulz":SchulzDispersion, 158 158 "lognormal":LogNormalDispersion}
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