1 | double form_volume(double length_a, double b2a_ratio, double c2a_ratio, double thickness); |
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2 | double Iq(double q, double sld, double solvent_sld, double length_a, |
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3 | double b2a_ratio, double c2a_ratio, double thickness); |
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4 | |
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5 | double form_volume(double length_a, double b2a_ratio, double c2a_ratio, double thickness) |
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6 | { |
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7 | double length_b = length_a * b2a_ratio; |
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8 | double length_c = length_a * c2a_ratio; |
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9 | double a_core = length_a - 2.0*thickness; |
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10 | double b_core = length_b - 2.0*thickness; |
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11 | double c_core = length_c - 2.0*thickness; |
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12 | double vol_core = a_core * b_core * c_core; |
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13 | double vol_total = length_a * length_b * length_c; |
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14 | double vol_shell = vol_total - vol_core; |
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15 | return vol_shell; |
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16 | } |
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17 | |
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18 | double Iq(double q, |
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19 | double sld, |
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20 | double solvent_sld, |
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21 | double length_a, |
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22 | double b2a_ratio, |
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23 | double c2a_ratio, |
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24 | double thickness) |
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25 | { |
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26 | const double length_b = length_a * b2a_ratio; |
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27 | const double length_c = length_a * c2a_ratio; |
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28 | const double a_half = 0.5 * length_a; |
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29 | const double b_half = 0.5 * length_b; |
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30 | const double c_half = 0.5 * length_c; |
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31 | const double vol_total = length_a * length_b * length_c; |
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32 | const double vol_core = 8.0 * (a_half-thickness) * (b_half-thickness) * (c_half-thickness); |
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33 | |
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34 | //Integration limits to use in Gaussian quadrature |
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35 | const double v1a = 0.0; |
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36 | const double v1b = M_PI_2; //theta integration limits |
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37 | const double v2a = 0.0; |
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38 | const double v2b = M_PI_2; //phi integration limits |
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39 | |
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40 | double outer_sum = 0.0; |
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41 | for(int i=0; i<76; i++) { |
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42 | |
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43 | const double theta = 0.5 * ( Gauss76Z[i]*(v1b-v1a) + v1a + v1b ); |
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44 | double sin_theta, cos_theta; |
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45 | SINCOS(theta, sin_theta, cos_theta); |
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46 | |
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47 | const double termC1 = sas_sinx_x(q * c_half * cos(theta)); |
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48 | const double termC2 = sas_sinx_x(q * (c_half-thickness)*cos(theta)); |
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49 | |
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50 | double inner_sum = 0.0; |
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51 | for(int j=0; j<76; j++) { |
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52 | |
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53 | const double phi = 0.5 * ( Gauss76Z[j]*(v2b-v2a) + v2a + v2b ); |
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54 | double sin_phi, cos_phi; |
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55 | SINCOS(phi, sin_phi, cos_phi); |
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56 | |
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57 | // Amplitude AP from eqn. (13), rewritten to avoid round-off effects when arg=0 |
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58 | |
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59 | const double termA1 = sas_sinx_x(q * a_half * sin_theta * sin_phi); |
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60 | const double termA2 = sas_sinx_x(q * (a_half-thickness) * sin_theta * sin_phi); |
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61 | |
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62 | const double termB1 = sas_sinx_x(q * b_half * sin_theta * cos_phi); |
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63 | const double termB2 = sas_sinx_x(q * (b_half-thickness) * sin_theta * cos_phi); |
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64 | |
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65 | const double AP1 = vol_total * termA1 * termB1 * termC1; |
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66 | const double AP2 = vol_core * termA2 * termB2 * termC2; |
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67 | |
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68 | inner_sum += Gauss76Wt[j] * square(AP1-AP2); |
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69 | } |
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70 | inner_sum *= 0.5 * (v2b-v2a); |
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71 | |
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72 | outer_sum += Gauss76Wt[i] * inner_sum * sin(theta); |
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73 | } |
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74 | outer_sum *= 0.5*(v1b-v1a); |
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75 | |
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76 | // Normalize as in Eqn. (15) without the volume factor (as cancels with (V*DelRho)^2 normalization) |
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77 | // The factor 2 is due to the different theta integration limit (pi/2 instead of pi) |
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78 | const double form = outer_sum/M_PI_2; |
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79 | |
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80 | // Multiply by contrast^2. Factor corresponding to volume^2 cancels with previous normalization. |
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81 | const double delrho = sld - solvent_sld; |
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82 | |
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83 | // Convert from [1e-12 A-1] to [cm-1] |
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84 | return 1.0e-4 * delrho * delrho * form; |
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85 | } |
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