[d86f0fc] | 1 | static double |
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| 2 | form_volume(double length_a, double b2a_ratio, double c2a_ratio) |
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[deb7ee0] | 3 | { |
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[ab2aea8] | 4 | double length_b = length_a * b2a_ratio; |
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| 5 | double length_c = length_a * c2a_ratio; |
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| 6 | double vol_shell = 2.0 * (length_a*length_b + length_a*length_c + length_b*length_c); |
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[deb7ee0] | 7 | return vol_shell; |
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| 8 | } |
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| 9 | |
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[71b751d] | 10 | static void |
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| 11 | Fq(double q, |
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| 12 | double *F1, |
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| 13 | double *F2, |
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[deb7ee0] | 14 | double sld, |
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| 15 | double solvent_sld, |
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[a807206] | 16 | double length_a, |
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[deb7ee0] | 17 | double b2a_ratio, |
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| 18 | double c2a_ratio) |
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| 19 | { |
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[ab2aea8] | 20 | const double length_b = length_a * b2a_ratio; |
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| 21 | const double length_c = length_a * c2a_ratio; |
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| 22 | const double a_half = 0.5 * length_a; |
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| 23 | const double b_half = 0.5 * length_b; |
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| 24 | const double c_half = 0.5 * length_c; |
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[deb7ee0] | 25 | |
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| 26 | //Integration limits to use in Gaussian quadrature |
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[ab2aea8] | 27 | const double v1a = 0.0; |
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| 28 | const double v1b = M_PI_2; //theta integration limits |
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| 29 | const double v2a = 0.0; |
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| 30 | const double v2b = M_PI_2; //phi integration limits |
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[74768cb] | 31 | |
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[71b751d] | 32 | double outer_sum_F1 = 0.0; |
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| 33 | double outer_sum_F2 = 0.0; |
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[74768cb] | 34 | for(int i=0; i<GAUSS_N; i++) { |
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| 35 | const double theta = 0.5 * ( GAUSS_Z[i]*(v1b-v1a) + v1a + v1b ); |
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[deb7ee0] | 36 | |
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[ab2aea8] | 37 | double sin_theta, cos_theta; |
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| 38 | double sin_c, cos_c; |
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| 39 | SINCOS(theta, sin_theta, cos_theta); |
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| 40 | SINCOS(q*c_half*cos_theta, sin_c, cos_c); |
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[deb7ee0] | 41 | |
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| 42 | // To check potential problems if denominator goes to zero here !!! |
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[ab2aea8] | 43 | const double termAL_theta = 8.0 * cos_c / (q*q*sin_theta*sin_theta); |
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| 44 | const double termAT_theta = 8.0 * sin_c / (q*q*sin_theta*cos_theta); |
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| 45 | |
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[71b751d] | 46 | double inner_sum_F1 = 0.0; |
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| 47 | double inner_sum_F2 = 0.0; |
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[74768cb] | 48 | for(int j=0; j<GAUSS_N; j++) { |
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| 49 | const double phi = 0.5 * ( GAUSS_Z[j]*(v2b-v2a) + v2a + v2b ); |
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[deb7ee0] | 50 | |
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[ab2aea8] | 51 | double sin_phi, cos_phi; |
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| 52 | double sin_a, cos_a; |
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| 53 | double sin_b, cos_b; |
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| 54 | SINCOS(phi, sin_phi, cos_phi); |
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| 55 | SINCOS(q*a_half*sin_theta*sin_phi, sin_a, cos_a); |
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| 56 | SINCOS(q*b_half*sin_theta*cos_phi, sin_b, cos_b); |
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[deb7ee0] | 57 | |
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| 58 | // Amplitude AL from eqn. (7c) |
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[ab2aea8] | 59 | const double AL = termAL_theta |
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| 60 | * sin_a*sin_b / (sin_phi*cos_phi); |
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[deb7ee0] | 61 | |
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| 62 | // Amplitude AT from eqn. (9) |
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[ab2aea8] | 63 | const double AT = termAT_theta |
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| 64 | * ( cos_a*sin_b/cos_phi + cos_b*sin_a/sin_phi ); |
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[deb7ee0] | 65 | |
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[71b751d] | 66 | inner_sum_F1 += GAUSS_W[j] * (AL+AT); |
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| 67 | inner_sum_F2 += GAUSS_W[j] * square(AL+AT); |
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[ab2aea8] | 68 | } |
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[deb7ee0] | 69 | |
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[71b751d] | 70 | inner_sum_F1 *= 0.5 * (v2b-v2a); |
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| 71 | inner_sum_F2 *= 0.5 * (v2b-v2a); |
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| 72 | outer_sum_F1 += GAUSS_W[i] * inner_sum_F1 * sin_theta; |
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| 73 | outer_sum_F2 += GAUSS_W[i] * inner_sum_F2 * sin_theta; |
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[deb7ee0] | 74 | } |
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| 75 | |
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[71b751d] | 76 | outer_sum_F1 *= 0.5*(v1b-v1a); |
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| 77 | outer_sum_F2 *= 0.5*(v1b-v1a); |
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[deb7ee0] | 78 | |
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| 79 | // Normalize as in Eqn. (15) without the volume factor (as cancels with (V*DelRho)^2 normalization) |
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| 80 | // The factor 2 is due to the different theta integration limit (pi/2 instead of pi) |
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[71b751d] | 81 | const double form_avg = outer_sum_F1/M_PI_2; |
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| 82 | const double form_squared_avg = outer_sum_F2/M_PI_2; |
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[deb7ee0] | 83 | |
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| 84 | // Multiply by contrast^2. Factor corresponding to volume^2 cancels with previous normalization. |
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[71b751d] | 85 | const double contrast = sld - solvent_sld; |
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[deb7ee0] | 86 | |
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| 87 | // Convert from [1e-12 A-1] to [cm-1] |
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[71b751d] | 88 | *F1 = 1e-2 * contrast * form_avg; |
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| 89 | *F2 = 1e-4 * contrast * contrast * form_squared_avg; |
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[deb7ee0] | 90 | } |
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