Changeset 43ff77c in sasmodels


Ignore:
Timestamp:
Apr 7, 2017 10:47:50 AM (8 years ago)
Author:
Paul Kienzle <pkienzle@…>
Branches:
master, core_shell_microgels, costrafo411, magnetic_model, ticket-1257-vesicle-product, ticket_1156, ticket_1265_superball, ticket_822_more_unit_tests
Children:
3a45c2c
Parents:
e2d6e3b (diff), b2f1d2f (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.
Message:

Merge branch 'master' into ticket-852-unit-tests

Files:
3 added
31 edited

Legend:

Unmodified
Added
Removed

  • .travis.yml

    rbec0e75 r01e551a  
    1 # Test Travis CL 
    2  
    31language: python 
    42python: 
    5   - "2.7" 
    6 # whitelist 
     3- '2.7' 
    74branches: 
    85  only: 
    9     - master 
    10 # command to install dependencies 
     6  - master 
    117virtualenv: 
    128  system_site_packages: true 
    139before_install: 
    14   - sudo apt-get update; 
    15   - sudo apt-get install python-numpy python-scipy 
    16 #  - sudo apt-get install opencl-headers 
    17  
     10- sudo apt-get update; 
     11- sudo apt-get install python-numpy python-scipy 
    1812install: 
    19 #  - pip install pyopencl 
    20   - pip install bumps 
    21   - pip install unittest-xml-reporting 
     13- pip install bumps 
     14- pip install unittest-xml-reporting 
    2215script: 
    23   - export WORKSPACE=/home/travis/build/SasView/sasmodels/ 
    24   - python -m sasmodels.model_test dll all 
     16- export WORKSPACE=/home/travis/build/SasView/sasmodels/ 
     17- python -m sasmodels.model_test dll all 
     18notifications: 
     19  slack: 
     20    secure: xNAUeSu1/it/x9Q2CSg79aw1LLc7d6mLpcqSCTeKROp71RhkFf8VjJnJm/lEbKHNC8yj5H9UHrz5DmzwJzI+6oMt4NdEeS6WvGhwGY/wCt2IcJKxw0vj1DAU04qFMS041Khwclo6jIqm76DloinXvmvsS+K/nSyQkF7q4egSlwA= 

  • sasmodels/compare.py

    r6e5c0b7 r43ff77c  
    546546    'f32': '32', 
    547547    'f64': '64', 
     548    'float16': '16', 
     549    'float32': '32', 
     550    'float64': '64', 
     551    'float128': '128', 
    548552    'longdouble': '128', 
    549553} 

  • sasmodels/core.py

    r5124c969 r650c6d2  
    250250        dtype = "longdouble" 
    251251    elif dtype == "half": 
    252         dtype = "f16" 
     252        dtype = "float16" 
    253253 
    254254    # Convert dtype string to numpy dtype. 

  • sasmodels/kerneldll.py

    r886fa25 rb2f1d2f  
    9797 
    9898if "SAS_COMPILER" in os.environ: 
    99     compiler = os.environ["SAS_COMPILER"] 
     99    COMPILER = os.environ["SAS_COMPILER"] 
    100100elif os.name == 'nt': 
    101     # If vcvarsall.bat has been called, then VCINSTALLDIR is in the environment 
    102     # and we can use the MSVC compiler.  Otherwise, if tinycc is available 
    103     # the use it.  Otherwise, hope that mingw is available. 
    104     if "VCINSTALLDIR" in os.environ: 
    105         compiler = "msvc" 
    106     elif tinycc: 
    107         compiler = "tinycc" 
     101    if tinycc is not None: 
     102        COMPILER = "tinycc" 
     103    elif "VCINSTALLDIR" in os.environ: 
     104        # If vcvarsall.bat has been called, then VCINSTALLDIR is in the environment 
     105        # and we can use the MSVC compiler.  Otherwise, if tinycc is available 
     106        # the use it.  Otherwise, hope that mingw is available. 
     107        COMPILER = "msvc" 
    108108    else: 
    109         compiler = "mingw" 
     109        COMPILER = "mingw" 
    110110else: 
    111     compiler = "unix" 
     111    COMPILER = "unix" 
    112112 
    113113ARCH = "" if ct.sizeof(ct.c_void_p) > 4 else "x86"  # 4 byte pointers on x86 
    114 if compiler == "unix": 
     114if COMPILER == "unix": 
    115115    # Generic unix compile 
    116116    # On mac users will need the X code command line tools installed 
    … …  
    123123        """unix compiler command""" 
    124124        return CC + [source, "-o", output, "-lm"] 
    125 elif compiler == "msvc": 
     125elif COMPILER == "msvc": 
    126126    # Call vcvarsall.bat before compiling to set path, headers, libs, etc. 
    127127    # MSVC compiler is available, so use it.  OpenMP requires a copy of 
    … …  
    139139        """MSVC compiler command""" 
    140140        return CC + ["/Tp%s"%source] + LN + ["/OUT:%s"%output] 
    141 elif compiler == "tinycc": 
     141elif COMPILER == "tinycc": 
    142142    # TinyCC compiler. 
    143143    CC = [tinycc.TCC] + "-shared -rdynamic -Wall".split() 
    … …  
    145145        """tinycc compiler command""" 
    146146        return CC + [source, "-o", output] 
    147 elif compiler == "mingw": 
     147elif COMPILER == "mingw": 
    148148    # MinGW compiler. 
    149149    CC = "gcc -shared -std=c99 -O2 -Wall".split() 

  • sasmodels/kernelpy.py

    rb397165 rdbfd471  
    235235            # exclude all q for that NaN.  Even better would be to have an 
    236236            # INVALID expression like the C models, but that is too expensive. 
    237             Iq = form() 
     237            Iq = np.asarray(form(), 'd') 
    238238            if np.isnan(Iq).any(): continue 
    239239 

  • sasmodels/models/hayter_msa.py

    ra807206 r5702f52  
    7474    ["radius_effective", "Ang", 20.75,   [0, inf],    "volume", "effective radius of charged sphere"], 
    7575    ["volfraction",   "None",     0.0192, [0, 0.74],   "", "volume fraction of spheres"], 
    76     ["charge",        "e",   19.0,    [0, inf],    "", "charge on sphere (in electrons)"], 
    77     ["temperature",   "K",  318.16,   [0, inf],    "", "temperature, in Kelvin, for Debye length calculation"], 
    78     ["concentration_salt",      "M",    0.0,    [-inf, inf], "", "conc of salt, moles/litre, 1:1 electolyte, for Debye length"], 
     76    ["charge",        "e",   19.0,    [0, 200],    "", "charge on sphere (in electrons)"], 
     77    ["temperature",   "K",  318.16,   [0, 450],    "", "temperature, in Kelvin, for Debye length calculation"], 
     78    ["concentration_salt",      "M",    0.0,    [0, inf], "", "conc of salt, moles/litre, 1:1 electolyte, for Debye length"], 
    7979    ["dielectconst",  "None",    71.08,   [-inf, inf], "", "dielectric constant (relative permittivity) of solvent, default water, for Debye length"] 
    8080    ] 

  • explore/angular_pd.py

    r12eb36b r8267e0b  
    4747 
    4848def draw_mesh_new(ax, theta, dtheta, phi, dphi, flow, radius=10., dist='gauss'): 
    49     theta_center = radians(theta) 
     49    theta_center = radians(90-theta) 
    5050    phi_center = radians(phi) 
    5151    flow_center = radians(flow) 
    … …  
    137137                              radius=11., dist=dist) 
    138138        if not axis.startswith('d'): 
    139             ax.view_init(elev=theta, azim=phi) 
     139            ax.view_init(elev=90-theta if use_new else theta, azim=phi) 
    140140        plt.gcf().canvas.draw() 
    141141 

  • sasmodels/kernel_header.c

    rdaeef4c rb00a646  
    148148inline double sas_sinx_x(double x) { return x==0 ? 1.0 : sin(x)/x; } 
    149149 
     150// To rotate from the canonical position to theta, phi, psi, first rotate by 
     151// psi about the major axis, oriented along z, which is a rotation in the 
     152// detector plane xy. Next rotate by theta about the y axis, aligning the major 
     153// axis in the xz plane. Finally, rotate by phi in the detector plane xy. 
     154// To compute the scattering, undo these rotations in reverse order: 
     155//     rotate in xy by -phi, rotate in xz by -theta, rotate in xy by -psi 
     156// The returned q is the length of the q vector and (xhat, yhat, zhat) is a unit 
     157// vector in the q direction. 
     158// To change between counterclockwise and clockwise rotation, change the 
     159// sign of phi and psi. 
     160 
    150161#if 1 
    151162//think cos(theta) should be sin(theta) in new coords, RKH 11Jan2017 
    … …  
    166177#endif 
    167178 
     179#if 1 
     180#define ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, xhat, yhat, zhat) do { \ 
     181    q = sqrt(qx*qx + qy*qy); \ 
     182    const double qxhat = qx/q; \ 
     183    const double qyhat = qy/q; \ 
     184    double sin_theta, cos_theta; \ 
     185    double sin_phi, cos_phi; \ 
     186    double sin_psi, cos_psi; \ 
     187    SINCOS(theta*M_PI_180, sin_theta, cos_theta); \ 
     188    SINCOS(phi*M_PI_180, sin_phi, cos_phi); \ 
     189    SINCOS(psi*M_PI_180, sin_psi, cos_psi); \ 
     190    xhat = qxhat*(-sin_phi*sin_psi + cos_theta*cos_phi*cos_psi) \ 
     191         + qyhat*( cos_phi*sin_psi + cos_theta*sin_phi*cos_psi); \ 
     192    yhat = qxhat*(-sin_phi*cos_psi - cos_theta*cos_phi*sin_psi) \ 
     193         + qyhat*( cos_phi*cos_psi - cos_theta*sin_phi*sin_psi); \ 
     194    zhat = qxhat*(-sin_theta*cos_phi) \ 
     195         + qyhat*(-sin_theta*sin_phi); \ 
     196    } while (0) 
     197#else 
     198// SasView 3.x definition of orientation 
    168199#define ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, cos_alpha, cos_mu, cos_nu) do { \ 
    169200    q = sqrt(qx*qx + qy*qy); \ 
    … …  
    180211    cos_nu = (-cos_phi*sin_psi*sin_theta + sin_phi*cos_psi)*qxhat + sin_psi*cos_theta*qyhat; \ 
    181212    } while (0) 
     213#endif 

  • sasmodels/models/barbell.py

    rfcb33e4 r0b56f38  
    8787* **Last Reviewed by:** Richard Heenan **Date:** January 4, 2017 
    8888""" 
    89 from numpy import inf 
     89from numpy import inf, sin, cos, pi 
    9090 
    9191name = "barbell" 
    … …  
    125125            phi_pd=15, phi_pd_n=0, 
    126126           ) 
     127q = 0.1 
     128# april 6 2017, rkh add unit tests, NOT compared with any other calc method, assume correct! 
     129qx = q*cos(pi/6.0) 
     130qy = q*sin(pi/6.0) 
     131tests = [[{}, 0.075, 25.5691260532], 
     132        [{'theta':80., 'phi':10.}, (qx, qy), 3.04233067789], 
     133        ] 
     134del qx, qy  # not necessary to delete, but cleaner 

  • sasmodels/models/bcc_paracrystal.c

    r4962519 r50beefe  
    9090    double theta, double phi, double psi) 
    9191{ 
    92     double q, cos_a1, cos_a2, cos_a3; 
    93     ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, cos_a3, cos_a2, cos_a1); 
     92    double q, zhat, yhat, xhat; 
     93    ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, xhat, yhat, zhat); 
    9494 
    95     const double a1 = +cos_a3 - cos_a1 + cos_a2; 
    96     const double a2 = +cos_a3 + cos_a1 - cos_a2; 
    97     const double a3 = -cos_a3 + cos_a1 + cos_a2; 
     95    const double a1 = +xhat - zhat + yhat; 
     96    const double a2 = +xhat + zhat - yhat; 
     97    const double a3 = -xhat + zhat + yhat; 
    9898 
    9999    const double qd = 0.5*q*dnn; 

  • sasmodels/models/bcc_paracrystal.py

    r925ad6e re2d6e3b  
    9999""" 
    100100 
    101 from numpy import inf 
     101from numpy import inf, pi 
    102102 
    103103name = "bcc_paracrystal" 
    … …  
    141141    psi_pd=15, psi_pd_n=0, 
    142142    ) 
     143# april 6 2017, rkh add unit tests, NOT compared with any other calc method, assume correct! 
     144# add 2d test later 
     145q =4.*pi/220. 
     146tests = [ 
     147    [{ }, 
     148     [0.001, q, 0.215268], [1.46601394721, 2.85851284174, 0.00866710287078]], 
     149] 

  • sasmodels/models/capped_cylinder.py

    rfcb33e4 r0b56f38  
    9191 
    9292""" 
    93 from numpy import inf 
     93from numpy import inf, sin, cos, pi 
    9494 
    9595name = "capped_cylinder" 
    … …  
    145145            theta_pd=15, theta_pd_n=45, 
    146146            phi_pd=15, phi_pd_n=1) 
     147q = 0.1 
     148# april 6 2017, rkh add unit tests, NOT compared with any other calc method, assume correct! 
     149qx = q*cos(pi/6.0) 
     150qy = q*sin(pi/6.0) 
     151tests = [[{}, 0.075, 26.0698570695], 
     152        [{'theta':80., 'phi':10.}, (qx, qy), 0.561811990502], 
     153        ] 
     154del qx, qy  # not necessary to delete, but cleaner 

  • sasmodels/models/core_shell_bicelle.c

    r592343f rb260926  
    3030 
    3131static double 
    32 bicelle_kernel(double qq, 
     32bicelle_kernel(double q, 
    3333              double rad, 
    3434              double radthick, 
    3535              double facthick, 
    36               double length, 
     36              double halflength, 
    3737              double rhoc, 
    3838              double rhoh, 
    … …  
    4242              double cos_alpha) 
    4343{ 
    44     double si1,si2,be1,be2; 
    45  
    4644    const double dr1 = rhoc-rhoh; 
    4745    const double dr2 = rhor-rhosolv; 
    4846    const double dr3 = rhoh-rhor; 
    49     const double vol1 = M_PI*rad*rad*(2.0*length); 
    50     const double vol2 = M_PI*(rad+radthick)*(rad+radthick)*2.0*(length+facthick); 
    51     const double vol3 = M_PI*rad*rad*2.0*(length+facthick); 
    52     double besarg1 = qq*rad*sin_alpha; 
    53     double besarg2 = qq*(rad+radthick)*sin_alpha; 
    54     double sinarg1 = qq*length*cos_alpha; 
    55     double sinarg2 = qq*(length+facthick)*cos_alpha; 
     47    const double vol1 = M_PI*square(rad)*2.0*(halflength); 
     48    const double vol2 = M_PI*square(rad+radthick)*2.0*(halflength+facthick); 
     49    const double vol3 = M_PI*square(rad)*2.0*(halflength+facthick); 
    5650 
    57     be1 = sas_2J1x_x(besarg1); 
    58     be2 = sas_2J1x_x(besarg2); 
    59     si1 = sas_sinx_x(sinarg1); 
    60     si2 = sas_sinx_x(sinarg2); 
     51    const double be1 = sas_2J1x_x(q*(rad)*sin_alpha); 
     52    const double be2 = sas_2J1x_x(q*(rad+radthick)*sin_alpha); 
     53    const double si1 = sas_sinx_x(q*(halflength)*cos_alpha); 
     54    const double si2 = sas_sinx_x(q*(halflength+facthick)*cos_alpha); 
    6155 
    6256    const double t = vol1*dr1*si1*be1 + 
    … …  
    6458                     vol3*dr3*si2*be1; 
    6559 
    66     const double retval = t*t*sin_alpha; 
     60    const double retval = t*t; 
    6761 
    6862    return retval; 
    … …  
    7165 
    7266static double 
    73 bicelle_integration(double qq, 
     67bicelle_integration(double q, 
    7468                   double rad, 
    7569                   double radthick, 
    … …  
    8377    // set up the integration end points 
    8478    const double uplim = M_PI_4; 
    85     const double halfheight = 0.5*length; 
     79    const double halflength = 0.5*length; 
    8680 
    8781    double summ = 0.0; 
    … …  
    9084        double sin_alpha, cos_alpha; // slots to hold sincos function output 
    9185        SINCOS(alpha, sin_alpha, cos_alpha); 
    92         double yyy = Gauss76Wt[i] * bicelle_kernel(qq, rad, radthick, facthick, 
    93                              halfheight, rhoc, rhoh, rhor, rhosolv, 
     86        double yyy = Gauss76Wt[i] * bicelle_kernel(q, rad, radthick, facthick, 
     87                             halflength, rhoc, rhoh, rhor, rhosolv, 
    9488                             sin_alpha, cos_alpha); 
    95         summ += yyy; 
     89        summ += yyy*sin_alpha; 
    9690    } 
    9791 
    … …  
    119113    double answer = bicelle_kernel(q, radius, thick_rim, thick_face, 
    120114                           0.5*length, core_sld, face_sld, rim_sld, 
    121                            solvent_sld, sin_alpha, cos_alpha) / fabs(sin_alpha); 
    122  
    123     answer *= 1.0e-4; 
    124  
    125     return answer; 
     115                           solvent_sld, sin_alpha, cos_alpha); 
     116    return 1.0e-4*answer; 
    126117} 
    127118 

  • sasmodels/models/core_shell_bicelle.py

    r3b9a526 r0b56f38  
    8888""" 
    8989 
    90 from numpy import inf, sin, cos 
     90from numpy import inf, sin, cos, pi 
    9191 
    9292name = "core_shell_bicelle" 
    … …  
    155155            theta=90, 
    156156            phi=0) 
     157q = 0.1 
     158# april 6 2017, rkh add unit tests, NOT compared with any other calc method, assume correct! 
     159qx = q*cos(pi/6.0) 
     160qy = q*sin(pi/6.0) 
     161tests = [[{}, 0.05, 7.4883545957], 
     162        [{'theta':80., 'phi':10.}, (qx, qy), 2.81048892474 ], 
     163        ] 
     164del qx, qy  # not necessary to delete, but cleaner 
    157165 
    158 #qx, qy = 0.4 * cos(pi/2.0), 0.5 * sin(0) 

  • sasmodels/models/core_shell_bicelle_elliptical.c

    r592343f rf4f85b3  
    3232} 
    3333 
    34 double  
    35                 Iq(double qq, 
    36                    double rad, 
    37                    double x_core, 
    38                    double radthick, 
    39                    double facthick, 
    40                    double length, 
    41                    double rhoc, 
    42                    double rhoh, 
    43                    double rhor, 
    44                    double rhosolv) 
     34double Iq(double q, 
     35          double rad, 
     36          double x_core, 
     37          double radthick, 
     38          double facthick, 
     39          double length, 
     40          double rhoc, 
     41          double rhoh, 
     42          double rhor, 
     43          double rhosolv) 
    4544{ 
    4645    double si1,si2,be1,be2; 
    … …  
    7473        const double sin_alpha = sqrt(1.0 - cos_alpha*cos_alpha); 
    7574        double inner_sum=0; 
    76         double sinarg1 = qq*halfheight*cos_alpha; 
    77         double sinarg2 = qq*(halfheight+facthick)*cos_alpha; 
     75        double sinarg1 = q*halfheight*cos_alpha; 
     76        double sinarg2 = q*(halfheight+facthick)*cos_alpha; 
    7877        si1 = sas_sinx_x(sinarg1); 
    7978        si2 = sas_sinx_x(sinarg2); 
    … …  
    8382            const double beta = ( Gauss76Z[j] +1.0)*M_PI_2; 
    8483            const double rr = sqrt(rA - rB*cos(beta)); 
    85             double besarg1 = qq*rr*sin_alpha; 
    86             double besarg2 = qq*(rr+radthick)*sin_alpha; 
     84            double besarg1 = q*rr*sin_alpha; 
     85            double besarg2 = q*(rr+radthick)*sin_alpha; 
    8786            be1 = sas_2J1x_x(besarg1); 
    8887            be2 = sas_2J1x_x(besarg2); 
    … …  
    114113{ 
    115114       // THIS NEEDS TESTING 
    116     double qq, cos_val, cos_mu, cos_nu; 
    117     ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, qq, cos_val, cos_mu, cos_nu); 
     115    double q, xhat, yhat, zhat; 
     116    ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, xhat, yhat, zhat); 
    118117    const double dr1 = rhoc-rhoh; 
    119118    const double dr2 = rhor-rhosolv; 
    … …  
    125124    const double vol3 = M_PI*rad*radius_major*2.0*(halfheight+facthick); 
    126125 
    127     // Compute:  r = sqrt((radius_major*cos_nu)^2 + (radius_minor*cos_mu)^2) 
     126    // Compute:  r = sqrt((radius_major*zhat)^2 + (radius_minor*yhat)^2) 
    128127    // Given:    radius_major = r_ratio * radius_minor   
    129128    // ASSUME the sin_alpha is included in the separate integration over orientation of rod angle 
    130     const double r = rad*sqrt(square(x_core*cos_nu) + cos_mu*cos_mu); 
    131     const double be1 = sas_2J1x_x( qq*r ); 
    132     const double be2 = sas_2J1x_x( qq*(r + radthick ) ); 
    133     const double si1 = sas_sinx_x( qq*halfheight*cos_val ); 
    134     const double si2 = sas_sinx_x( qq*(halfheight + facthick)*cos_val ); 
     129    const double rad_minor = rad; 
     130    const double rad_major = rad*x_core; 
     131    const double r_hat = sqrt(square(rad_major*xhat) + square(rad_minor*yhat)); 
     132    const double rshell_hat = sqrt(square((rad_major+radthick)*xhat) 
     133                                   + square((rad_minor+radthick)*yhat)); 
     134    const double be1 = sas_2J1x_x( q*r_hat ); 
     135    const double be2 = sas_2J1x_x( q*rshell_hat ); 
     136    const double si1 = sas_sinx_x( q*halfheight*zhat ); 
     137    const double si2 = sas_sinx_x( q*(halfheight + facthick)*zhat ); 
    135138    const double Aq = square( vol1*dr1*si1*be1 + vol2*dr2*si2*be2 +  vol3*dr3*si2*be1); 
    136139    //const double vol = form_volume(radius_minor, r_ratio, length); 

  • sasmodels/models/core_shell_bicelle_elliptical.py

    r3b9a526 r0b56f38  
    9999""" 
    100100 
    101 from numpy import inf, sin, cos 
     101from numpy import inf, sin, cos, pi 
    102102 
    103103name = "core_shell_bicelle_elliptical" 
    … …  
    150150            psi=0) 
    151151 
    152 #qx, qy = 0.4 * cos(pi/2.0), 0.5 * sin(0) 
     152q = 0.1 
     153# april 6 2017, rkh added a 2d unit test, NOT READY YET pull #890 branch assume correct! 
     154qx = q*cos(pi/6.0) 
     155qy = q*sin(pi/6.0) 
    153156 
    154157tests = [ 
    … …  
    159162    'sld_core':4.0, 'sld_face':7.0, 'sld_rim':1.0, 'sld_solvent':6.0, 'background':0.0}, 
    160163    0.015, 286.540286], 
    161 ] 
     164#    [{'theta':80., 'phi':10.}, (qx, qy), 7.88866563001 ], 
     165        ] 
     166 
     167del qx, qy  # not necessary to delete, but cleaner 

  • sasmodels/models/core_shell_cylinder.py

    rfcb33e4 r0b56f38  
    7373""" 
    7474 
    75 from numpy import pi, inf 
     75from numpy import pi, inf, sin, cos 
    7676 
    7777name = "core_shell_cylinder" 
    … …  
    151151            theta_pd=15, theta_pd_n=45, 
    152152            phi_pd=15, phi_pd_n=1) 
    153  
     153q = 0.1 
     154# april 6 2017, rkh add unit tests, NOT compared with any other calc method, assume correct! 
     155qx = q*cos(pi/6.0) 
     156qy = q*sin(pi/6.0) 
     157tests = [[{}, 0.075, 10.8552692237], 
     158        [{}, (qx, qy), 0.444618752741 ], 
     159        ] 
     160del qx, qy  # not necessary to delete, but cleaner 

  • sasmodels/models/core_shell_parallelepiped.c

    r1e7b0db0 r92dfe0c  
    134134    double psi) 
    135135{ 
    136     double q, cos_val_a, cos_val_b, cos_val_c; 
    137     ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, cos_val_c, cos_val_b, cos_val_a); 
     136    double q, zhat, yhat, xhat; 
     137    ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, xhat, yhat, zhat); 
    138138 
    139139    // cspkernel in csparallelepiped recoded here 
    … …  
    160160    double tc = length_a + 2.0*thick_rim_c; 
    161161    //handle arg=0 separately, as sin(t)/t -> 1 as t->0 
    162     double siA = sas_sinx_x(0.5*q*length_a*cos_val_a); 
    163     double siB = sas_sinx_x(0.5*q*length_b*cos_val_b); 
    164     double siC = sas_sinx_x(0.5*q*length_c*cos_val_c); 
    165     double siAt = sas_sinx_x(0.5*q*ta*cos_val_a); 
    166     double siBt = sas_sinx_x(0.5*q*tb*cos_val_b); 
    167     double siCt = sas_sinx_x(0.5*q*tc*cos_val_c); 
     162    double siA = sas_sinx_x(0.5*q*length_a*xhat); 
     163    double siB = sas_sinx_x(0.5*q*length_b*yhat); 
     164    double siC = sas_sinx_x(0.5*q*length_c*zhat); 
     165    double siAt = sas_sinx_x(0.5*q*ta*xhat); 
     166    double siBt = sas_sinx_x(0.5*q*tb*yhat); 
     167    double siCt = sas_sinx_x(0.5*q*tc*zhat); 
    168168     
    169169 

  • sasmodels/models/core_shell_parallelepiped.py

    rcb0dc22 r933af72  
    4848amplitudes of the core and shell, in the same manner as a core-shell model. 
    4949 
     50.. math:: 
     51 
     52    F_{a}(Q,\alpha,\beta)= 
     53    \left[\frac{\sin(Q(L_A+2t_A)/2\sin\alpha \sin\beta)}{Q(L_A+2t_A)/2\sin\alpha\sin\beta} 
     54    - \frac{\sin(QL_A/2\sin\alpha \sin\beta)}{QL_A/2\sin\alpha \sin\beta} \right] 
     55    \left[\frac{\sin(QL_B/2\sin\alpha \sin\beta)}{QL_B/2\sin\alpha \sin\beta} \right] 
     56    \left[\frac{\sin(QL_C/2\sin\alpha \sin\beta)}{QL_C/2\sin\alpha \sin\beta} \right] 
    5057 
    5158.. note:: 
    … …  
    5764 
    5865FITTING NOTES 
    59 If the scale is set equal to the particle volume fraction, |phi|, the returned 
     66If the scale is set equal to the particle volume fraction, $\phi$, the returned 
    6067value is the scattered intensity per unit volume, $I(q) = \phi P(q)$. 
    6168However, **no interparticle interference effects are included in this 

  • sasmodels/models/ellipsoid.c

    r130d4c7 r3b571ae  
    33double Iqxy(double qx, double qy, double sld, double sld_solvent, 
    44    double radius_polar, double radius_equatorial, double theta, double phi); 
    5  
    6 static double 
    7 _ellipsoid_kernel(double q, double radius_polar, double radius_equatorial, double cos_alpha) 
    8 { 
    9     double ratio = radius_polar/radius_equatorial; 
    10     // Using ratio v = Rp/Re, we can expand the following to match the 
    11     // form given in Guinier (1955) 
    12     //     r = Re * sqrt(1 + cos^2(T) (v^2 - 1)) 
    13     //       = Re * sqrt( (1 - cos^2(T)) + v^2 cos^2(T) ) 
    14     //       = Re * sqrt( sin^2(T) + v^2 cos^2(T) ) 
    15     //       = sqrt( Re^2 sin^2(T) + Rp^2 cos^2(T) ) 
    16     // 
    17     // Instead of using pythagoras we could pass in sin and cos; this may be 
    18     // slightly better for 2D which has already computed it, but it introduces 
    19     // an extra sqrt and square for 1-D not required by the current form, so 
    20     // leave it as is. 
    21     const double r = radius_equatorial 
    22                      * sqrt(1.0 + cos_alpha*cos_alpha*(ratio*ratio - 1.0)); 
    23     const double f = sas_3j1x_x(q*r); 
    24  
    25     return f*f; 
    26 } 
    275 
    286double form_volume(double radius_polar, double radius_equatorial) 
    … …  
    3715    double radius_equatorial) 
    3816{ 
     17    // Using ratio v = Rp/Re, we can implement the form given in Guinier (1955) 
     18    //     i(h) = int_0^pi/2 Phi^2(h a sqrt(cos^2 + v^2 sin^2) cos dT 
     19    //          = int_0^pi/2 Phi^2(h a sqrt((1-sin^2) + v^2 sin^2) cos dT 
     20    //          = int_0^pi/2 Phi^2(h a sqrt(1 + sin^2(v^2-1)) cos dT 
     21    // u-substitution of 
     22    //     u = sin, du = cos dT 
     23    //     i(h) = int_0^1 Phi^2(h a sqrt(1 + u^2(v^2-1)) du 
     24    const double v_square_minus_one = square(radius_polar/radius_equatorial) - 1.0; 
     25 
    3926    // translate a point in [-1,1] to a point in [0, 1] 
     27    // const double u = Gauss76Z[i]*(upper-lower)/2 + (upper+lower)/2; 
    4028    const double zm = 0.5; 
    4129    const double zb = 0.5; 
    4230    double total = 0.0; 
    4331    for (int i=0;i<76;i++) { 
    44         //const double cos_alpha = (Gauss76Z[i]*(upper-lower) + upper + lower)/2; 
    45         const double cos_alpha = Gauss76Z[i]*zm + zb; 
    46         total += Gauss76Wt[i] * _ellipsoid_kernel(q, radius_polar, radius_equatorial, cos_alpha); 
     32        const double u = Gauss76Z[i]*zm + zb; 
     33        const double r = radius_equatorial*sqrt(1.0 + u*u*v_square_minus_one); 
     34        const double f = sas_3j1x_x(q*r); 
     35        total += Gauss76Wt[i] * f * f; 
    4736    } 
    4837    // translate dx in [-1,1] to dx in [lower,upper] 
    … …  
    6251    double q, sin_alpha, cos_alpha; 
    6352    ORIENT_SYMMETRIC(qx, qy, theta, phi, q, sin_alpha, cos_alpha); 
    64     const double form = _ellipsoid_kernel(q, radius_polar, radius_equatorial, cos_alpha); 
     53    const double r = sqrt(square(radius_equatorial*sin_alpha) 
     54                          + square(radius_polar*cos_alpha)); 
     55    const double f = sas_3j1x_x(q*r); 
    6556    const double s = (sld - sld_solvent) * form_volume(radius_polar, radius_equatorial); 
    6657 
    67     return 1.0e-4 * form * s * s; 
     58    return 1.0e-4 * square(f * s); 
    6859} 
    6960 

  • sasmodels/models/ellipsoid.py

    r925ad6e r0b56f38  
    1818.. math:: 
    1919 
    20     F(q,\alpha) = \frac{3 \Delta \rho V (\sin[qr(R_p,R_e,\alpha)] 
    21                 - \cos[qr(R_p,R_e,\alpha)])} 
    22                 {[qr(R_p,R_e,\alpha)]^3} 
     20    F(q,\alpha) = \Delta \rho V \frac{3(\sin qr  - qr \cos qr)}{(qr)^3} 
    2321 
    24 and 
     22for 
    2523 
    2624.. math:: 
    2725 
    28     r(R_p,R_e,\alpha) = \left[ R_e^2 \sin^2 \alpha 
    29         + R_p^2 \cos^2 \alpha \right]^{1/2} 
     26    r = \left[ R_e^2 \sin^2 \alpha + R_p^2 \cos^2 \alpha \right]^{1/2} 
    3027 
    3128 
    3229$\alpha$ is the angle between the axis of the ellipsoid and $\vec q$, 
    33 $V = (4/3)\pi R_pR_e^2$ is the volume of the ellipsoid , $R_p$ is the polar radius along the 
    34 rotational axis of the ellipsoid, $R_e$ is the equatorial radius perpendicular 
    35 to the rotational axis of the ellipsoid and $\Delta \rho$ (contrast) is the 
    36 scattering length density difference between the scatterer and the solvent. 
     30$V = (4/3)\pi R_pR_e^2$ is the volume of the ellipsoid, $R_p$ is the polar 
     31radius along the rotational axis of the ellipsoid, $R_e$ is the equatorial 
     32radius perpendicular to the rotational axis of the ellipsoid and 
     33$\Delta \rho$ (contrast) is the scattering length density difference between 
     34the scatterer and the solvent. 
    3735 
    38 For randomly oriented particles: 
     36For randomly oriented particles use the orientational average, 
    3937 
    4038.. math:: 
    4139 
    42    F^2(q)=\int_{0}^{\pi/2}{F^2(q,\alpha)\sin(\alpha)d\alpha} 
     40   \langle F^2(q) \rangle = \int_{0}^{\pi/2}{F^2(q,\alpha)\sin(\alpha)\,d\alpha} 
    4341 
     42 
     43computed via substitution of $u=\sin(\alpha)$, $du=\cos(\alpha)\,d\alpha$ as 
     44 
     45.. math:: 
     46 
     47    \langle F^2(q) \rangle = \int_0^1{F^2(q, u)\,du} 
     48 
     49with 
     50 
     51.. math:: 
     52 
     53    r = R_e \left[ 1 + u^2\left(R_p^2/R_e^2 - 1\right)\right]^{1/2} 
    4454 
    4555To provide easy access to the orientation of the ellipsoid, we define 
    … …  
    4858:ref:`cylinder orientation figure <cylinder-angle-definition>`. 
    4959For the ellipsoid, $\theta$ is the angle between the rotational axis 
    50 and the $z$ -axis. 
     60and the $z$ -axis in the $xz$ plane followed by a rotation by $\phi$ 
     61in the $xy$ plane. 
    5162 
    5263NB: The 2nd virial coefficient of the solid ellipsoid is calculated based 
    … …  
    90101than 500. 
    91102 
     103Model was also tested against the triaxial ellipsoid model with equal major 
     104and minor equatorial radii.  It is also consistent with the cyclinder model 
     105with polar radius equal to length and equatorial radius equal to radius. 
     106 
    92107References 
    93108---------- 
    … …  
    96111*Structure Analysis by Small-Angle X-Ray and Neutron Scattering*, 
    97112Plenum Press, New York, 1987. 
     113 
     114Authorship and Verification 
     115---------------------------- 
     116 
     117* **Author:** NIST IGOR/DANSE **Date:** pre 2010 
     118* **Converted to sasmodels by:** Helen Park **Date:** July 9, 2014 
     119* **Last Modified by:** Paul Kienzle **Date:** March 22, 2017 
    98120""" 
    99121 
    100 from numpy import inf 
     122from numpy import inf, sin, cos, pi 
    101123 
    102124name = "ellipsoid" 
    … …  
    139161def ER(radius_polar, radius_equatorial): 
    140162    import numpy as np 
    141  
     163# see equation (26) in A.Isihara, J.Chem.Phys. 18(1950)1446-1449 
    142164    ee = np.empty_like(radius_polar) 
    143165    idx = radius_polar > radius_equatorial 
    … …  
    168190            theta_pd=15, theta_pd_n=45, 
    169191            phi_pd=15, phi_pd_n=1) 
     192q = 0.1 
     193# april 6 2017, rkh add unit tests, NOT compared with any other calc method, assume correct! 
     194qx = q*cos(pi/6.0) 
     195qy = q*sin(pi/6.0) 
     196tests = [[{}, 0.05, 54.8525847025], 
     197        [{'theta':80., 'phi':10.}, (qx, qy), 1.74134670026 ], 
     198        ] 
     199del qx, qy  # not necessary to delete, but cleaner 

  • sasmodels/models/elliptical_cylinder.c

    r592343f r61104c8  
    6767     double theta, double phi, double psi) 
    6868{ 
    69     double q, cos_val, cos_mu, cos_nu; 
    70     ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, cos_val, cos_mu, cos_nu); 
     69    double q, xhat, yhat, zhat; 
     70    ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, xhat, yhat, zhat); 
    7171 
    7272    // Compute:  r = sqrt((radius_major*cos_nu)^2 + (radius_minor*cos_mu)^2) 
    7373    // Given:    radius_major = r_ratio * radius_minor 
    74     const double r = radius_minor*sqrt(square(r_ratio*cos_nu) + cos_mu*cos_mu); 
     74    const double r = radius_minor*sqrt(square(r_ratio*xhat) + square(yhat)); 
    7575    const double be = sas_2J1x_x(q*r); 
    76     const double si = sas_sinx_x(q*0.5*length*cos_val); 
     76    const double si = sas_sinx_x(q*zhat*0.5*length); 
    7777    const double Aq = be * si; 
    7878    const double delrho = sld - solvent_sld; 

  • sasmodels/models/elliptical_cylinder.py

    rfcb33e4 r0b56f38  
    108108""" 
    109109 
    110 from numpy import pi, inf, sqrt 
     110from numpy import pi, inf, sqrt, sin, cos 
    111111 
    112112name = "elliptical_cylinder" 
    … …  
    149149                           + (length + radius) * (length + pi * radius)) 
    150150    return 0.5 * (ddd) ** (1. / 3.) 
     151q = 0.1 
     152# april 6 2017, rkh added a 2d unit test, NOT READY YET pull #890 branch assume correct! 
     153qx = q*cos(pi/6.0) 
     154qy = q*sin(pi/6.0) 
    151155 
    152156tests = [ 
    … …  
    158162      'sld_solvent':1.0, 'background':0.0}, 
    159163     0.001, 675.504402], 
     164#    [{'theta':80., 'phi':10.}, (qx, qy), 7.88866563001 ], 
    160165] 

  • sasmodels/models/fcc_paracrystal.c

    r4962519 r50beefe  
    9090    double theta, double phi, double psi) 
    9191{ 
    92     double q, cos_a1, cos_a2, cos_a3; 
    93     ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, cos_a3, cos_a2, cos_a1); 
     92    double q, zhat, yhat, xhat; 
     93    ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, xhat, yhat, zhat); 
    9494 
    95     const double a1 = cos_a2 + cos_a3; 
    96     const double a2 = cos_a3 + cos_a1; 
    97     const double a3 = cos_a2 + cos_a1; 
     95    const double a1 = yhat + xhat; 
     96    const double a2 = xhat + zhat; 
     97    const double a3 = yhat + zhat; 
    9898    const double qd = 0.5*q*dnn; 
    9999    const double arg = 0.5*square(qd*d_factor)*(a1*a1 + a2*a2 + a3*a3); 

  • sasmodels/models/fcc_paracrystal.py

    r925ad6e re2d6e3b  
    9090""" 
    9191 
    92 from numpy import inf 
     92from numpy import inf, pi 
    9393 
    9494name = "fcc_paracrystal" 
    … …  
    128128            psi_pd=15, psi_pd_n=0, 
    129129           ) 
     130# april 6 2017, rkh add unit tests, NOT compared with any other calc method, assume correct! 
     131# add 2d test later 
     132q =4.*pi/220. 
     133tests = [ 
     134    [{ }, 
     135     [0.001, q, 0.215268], [0.275164706668, 5.7776842567, 0.00958167119232]], 
     136] 

  • sasmodels/models/hollow_cylinder.py

    raea2e2a r0b56f38  
    6060""" 
    6161 
    62 from numpy import pi, inf 
     62from numpy import pi, inf, sin, cos 
    6363 
    6464name = "hollow_cylinder" 
    … …  
    129129            theta_pd=10, theta_pd_n=5, 
    130130           ) 
    131  
     131q = 0.1 
     132# april 6 2017, rkh added a 2d unit test, assume correct! 
     133qx = q*cos(pi/6.0) 
     134qy = q*sin(pi/6.0) 
    132135# Parameters for unit tests 
    133136tests = [ 
    134137    [{}, 0.00005, 1764.926], 
    135138    [{}, 'VR', 1.8], 
    136     [{}, 0.001, 1756.76] 
    137     ] 
     139    [{}, 0.001, 1756.76], 
     140    [{}, (qx, qy), 2.36885476192  ], 
     141        ] 
     142del qx, qy  # not necessary to delete, but cleaner 

  • sasmodels/models/parallelepiped.c

    r1e7b0db0 rd605080  
    6767    double psi) 
    6868{ 
    69     double q, cos_val_a, cos_val_b, cos_val_c; 
    70     ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, cos_val_c, cos_val_b, cos_val_a); 
     69    double q, xhat, yhat, zhat; 
     70    ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, xhat, yhat, zhat); 
    7171 
    72     const double siA = sas_sinx_x(0.5*q*length_a*cos_val_a); 
    73     const double siB = sas_sinx_x(0.5*q*length_b*cos_val_b); 
    74     const double siC = sas_sinx_x(0.5*q*length_c*cos_val_c); 
     72    const double siA = sas_sinx_x(0.5*length_a*q*xhat); 
     73    const double siB = sas_sinx_x(0.5*length_b*q*yhat); 
     74    const double siC = sas_sinx_x(0.5*length_c*q*zhat); 
    7575    const double V = form_volume(length_a, length_b, length_c); 
    7676    const double drho = (sld - solvent_sld); 

  • sasmodels/models/sc_paracrystal.c

    r4962519 r50beefe  
    111111          double psi) 
    112112{ 
    113     double q, cos_a1, cos_a2, cos_a3; 
    114     ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, cos_a3, cos_a2, cos_a1); 
     113    double q, zhat, yhat, xhat; 
     114    ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, xhat, yhat, zhat); 
    115115 
    116116    const double qd = q*dnn; 
    … …  
    118118    const double tanh_qd = tanh(arg); 
    119119    const double cosh_qd = cosh(arg); 
    120     const double Zq = tanh_qd/(1. - cos(qd*cos_a1)/cosh_qd) 
    121                     * tanh_qd/(1. - cos(qd*cos_a2)/cosh_qd) 
    122                     * tanh_qd/(1. - cos(qd*cos_a3)/cosh_qd); 
     120    const double Zq = tanh_qd/(1. - cos(qd*zhat)/cosh_qd) 
     121                    * tanh_qd/(1. - cos(qd*yhat)/cosh_qd) 
     122                    * tanh_qd/(1. - cos(qd*xhat)/cosh_qd); 
    123123 
    124124    const double Fq = sphere_form(q, radius, sphere_sld, solvent_sld)*Zq; 

  • sasmodels/models/stacked_disks.py

    rc3ccaec r0b56f38  
    103103""" 
    104104 
    105 from numpy import inf 
     105from numpy import inf, sin, cos, pi 
    106106 
    107107name = "stacked_disks" 
    … …  
    152152# After redefinition of spherical coordinates - 
    153153# tests had in old coords theta=0, phi=0; new coords theta=90, phi=0 
    154 # but should not matter here as so far all the tests are 1D not 2D 
     154q = 0.1 
     155# april 6 2017, rkh added a 2d unit test, assume correct! 
     156qx = q*cos(pi/6.0) 
     157qy = q*sin(pi/6.0) 
    155158tests = [ 
    156159# Accuracy tests based on content in test/utest_extra_models.py. 
    … …  
    186189    [{'thick_core': 10.0, 
    187190      'thick_layer': 15.0, 
     191      'radius': 100.0, 
     192      'n_stacking': 5, 
     193      'sigma_d': 0.0, 
     194      'sld_core': 4.0, 
     195      'sld_layer': -0.4, 
     196      'solvent_sd': 5.0, 
     197      'theta': 90.0, 
     198      'phi': 20.0, 
     199      'scale': 0.01, 
     200      'background': 0.001}, 
     201      (qx, qy), 0.0491167089952  ], 
     202    [{'thick_core': 10.0, 
     203      'thick_layer': 15.0, 
    188204      'radius': 3000.0, 
    189205      'n_stacking': 5, 
    … …  
    228244      'background': 0.001, 
    229245     }, ([0.4, 0.5]), [0.00105074, 0.00121761]], 
     246    [{'thick_core': 10.0, 
     247      'thick_layer': 15.0, 
     248      'radius': 3000.0, 
     249      'n_stacking': 1.0, 
     250      'sigma_d': 0.0, 
     251      'sld_core': 4.0, 
     252      'sld_layer': -0.4, 
     253      'solvent_sd': 5.0, 
     254      'theta': 90.0, 
     255      'phi': 20.0, 
     256      'scale': 0.01, 
     257      'background': 0.001, 
     258     }, (qx, qy), 0.0341738733124 ], 
    230259 
    231260    [{'thick_core': 10.0, 

  • sasmodels/models/triaxial_ellipsoid.c

    r925ad6e r68dd6a9  
    2020    double radius_polar) 
    2121{ 
    22     double sn, cn; 
    23     // translate a point in [-1,1] to a point in [0, 1] 
    24     const double zm = 0.5; 
    25     const double zb = 0.5; 
     22    const double pa = square(radius_equat_minor/radius_equat_major) - 1.0; 
     23    const double pc = square(radius_polar/radius_equat_major) - 1.0; 
     24    // translate a point in [-1,1] to a point in [0, pi/2] 
     25    const double zm = M_PI_4; 
     26    const double zb = M_PI_4; 
    2627    double outer = 0.0; 
    2728    for (int i=0;i<76;i++) { 
    28         //const double cos_alpha = (Gauss76Z[i]*(upper-lower) + upper + lower)/2; 
    29         const double x = 0.5*(Gauss76Z[i] + 1.0); 
    30         SINCOS(M_PI_2*x, sn, cn); 
    31         const double acosx2 = radius_equat_minor*radius_equat_minor*cn*cn; 
    32         const double bsinx2 = radius_equat_major*radius_equat_major*sn*sn; 
    33         const double c2 = radius_polar*radius_polar; 
     29        //const double u = Gauss76Z[i]*(upper-lower)/2 + (upper + lower)/2; 
     30        const double phi = Gauss76Z[i]*zm + zb; 
     31        const double pa_sinsq_phi = pa*square(sin(phi)); 
    3432 
    3533        double inner = 0.0; 
     34        const double um = 0.5; 
     35        const double ub = 0.5; 
    3636        for (int j=0;j<76;j++) { 
    37             const double ysq = square(Gauss76Z[j]*zm + zb); 
    38             const double t = q*sqrt(acosx2 + bsinx2*(1.0-ysq) + c2*ysq); 
    39             const double fq = sas_3j1x_x(t); 
    40             inner += Gauss76Wt[j] * fq * fq ; 
     37            // translate a point in [-1,1] to a point in [0, 1] 
     38            const double usq = square(Gauss76Z[j]*um + ub); 
     39            const double r = radius_equat_major*sqrt(pa_sinsq_phi*(1.0-usq) + 1.0 + pc*usq); 
     40            const double fq = sas_3j1x_x(q*r); 
     41            inner += Gauss76Wt[j] * fq * fq; 
    4142        } 
    42         outer += Gauss76Wt[i] * 0.5 * inner; 
     43        outer += Gauss76Wt[i] * inner;  // correcting for dx later 
    4344    } 
    44     // translate dx in [-1,1] to dx in [lower,upper] 
    45     const double fqsq = outer*zm; 
     45    // translate integration ranges from [-1,1] to [lower,upper] and normalize by 4 pi 
     46    const double fqsq = outer/4.0;  // = outer*um*zm*8.0/(4.0*M_PI); 
    4647    const double s = (sld - sld_solvent) * form_volume(radius_equat_minor, radius_equat_major, radius_polar); 
    4748    return 1.0e-4 * s * s * fqsq; 
    … …  
    5859    double psi) 
    5960{ 
    60     double q, calpha, cmu, cnu; 
    61     ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, calpha, cmu, cnu); 
     61    double q, xhat, yhat, zhat; 
     62    ORIENT_ASYMMETRIC(qx, qy, theta, phi, psi, q, xhat, yhat, zhat); 
    6263 
    63     const double t = q*sqrt(radius_equat_minor*radius_equat_minor*cnu*cnu 
    64                           + radius_equat_major*radius_equat_major*cmu*cmu 
    65                           + radius_polar*radius_polar*calpha*calpha); 
    66     const double fq = sas_3j1x_x(t); 
     64    const double r = sqrt(square(radius_equat_minor*xhat) 
     65                          + square(radius_equat_major*yhat) 
     66                          + square(radius_polar*zhat)); 
     67    const double fq = sas_3j1x_x(q*r); 
    6768    const double s = (sld - sld_solvent) * form_volume(radius_equat_minor, radius_equat_major, radius_polar); 
    6869 

  • sasmodels/models/triaxial_ellipsoid.py

    r925ad6e r0b56f38  
    22# Note: model title and parameter table are inserted automatically 
    33r""" 
    4 All three axes are of different lengths with $R_a \leq R_b \leq R_c$ 
    5 **Users should maintain this inequality for all calculations**. 
     4Definition 
     5---------- 
     6 
     7.. figure:: img/triaxial_ellipsoid_geometry.jpg 
     8 
     9    Ellipsoid with $R_a$ as *radius_equat_minor*, $R_b$ as *radius_equat_major* 
     10    and $R_c$ as *radius_polar*. 
     11 
     12Given an ellipsoid 
    613 
    714.. math:: 
    815 
    9     P(q) = \text{scale} V \left< F^2(q) \right> + \text{background} 
     16    \frac{X^2}{R_a^2} + \frac{Y^2}{R_b^2} + \frac{Z^2}{R_c^2} = 1 
    1017 
    11 where the volume $V = 4/3 \pi R_a R_b R_c$, and the averaging 
    12 $\left<\ldots\right>$ is applied over all orientations for 1D. 
    13  
    14 .. figure:: img/triaxial_ellipsoid_geometry.jpg 
    15  
    16     Ellipsoid schematic. 
    17  
    18 Definition 
    19 ---------- 
    20  
    21 The form factor calculated is 
     18the scattering for randomly oriented particles is defined by the average over all orientations $\Omega$ of: 
    2219 
    2320.. math:: 
    2421 
    25     P(q) = \frac{\text{scale}}{V}\int_0^1\int_0^1 
    26         \Phi^2(qR_a^2\cos^2( \pi x/2) + qR_b^2\sin^2(\pi y/2)(1-y^2) + R_c^2y^2) 
    27         dx dy 
     22    P(q) = \text{scale}(\Delta\rho)^2\frac{V}{4 \pi}\int_\Omega \Phi^2(qr) d\Omega + \text{background} 
    2823 
    2924where 
    … …  
    3126.. math:: 
    3227 
    33     \Phi(u) = 3 u^{-3} (\sin u - u \cos u) 
     28    \Phi(qr) &= 3 j_1(qr)/qr = 3 (\sin qr - qr \cos qr)/(qr)^3 \\ 
     29    r^2 &= R_a^2e^2 + R_b^2f^2 + R_c^2g^2 \\ 
     30    V &= \tfrac{4}{3} \pi R_a R_b R_c 
     31 
     32The $e$, $f$ and $g$ terms are the projections of the orientation vector on $X$, 
     33$Y$ and $Z$ respectively.  Keeping the orientation fixed at the canonical 
     34axes, we can integrate over the incident direction using polar angle 
     35$-\pi/2 \le \gamma \le \pi/2$ and equatorial angle $0 \le \phi \le 2\pi$ 
     36(as defined in ref [1]), 
     37 
     38 .. math:: 
     39 
     40     \langle\Phi^2\rangle = \int_0^{2\pi} \int_{-\pi/2}^{\pi/2} \Phi^2(qr) \cos \gamma\,d\gamma d\phi 
     41 
     42with $e = \cos\gamma \sin\phi$, $f = \cos\gamma \cos\phi$ and $g = \sin\gamma$. 
     43A little algebra yields 
     44 
     45.. math:: 
     46 
     47    r^2 = b^2(p_a \sin^2 \phi \cos^2 \gamma + 1 + p_c \sin^2 \gamma) 
     48 
     49for 
     50 
     51.. math:: 
     52 
     53    p_a = \frac{a^2}{b^2} - 1 \text{ and } p_c = \frac{c^2}{b^2} - 1 
     54 
     55Due to symmetry, the ranges can be restricted to a single quadrant 
     56$0 \le \gamma \le \pi/2$ and $0 \le \phi \le \pi/2$, scaling the resulting 
     57integral by 8. The computation is done using the substitution $u = \sin\gamma$, 
     58$du = \cos\gamma\,d\gamma$, giving 
     59 
     60.. math:: 
     61 
     62    \langle\Phi^2\rangle &= 8 \int_0^{\pi/2} \int_0^1 \Phi^2(qr) du d\phi \\ 
     63    r^2 &= b^2(p_a \sin^2(\phi)(1 - u^2) + 1 + p_c u^2) 
    3464 
    3565To provide easy access to the orientation of the triaxial ellipsoid, 
    … …  
    4979The radius-of-gyration for this system is  $R_g^2 = (R_a R_b R_c)^2/5$. 
    5080 
    51 The contrast is defined as SLD(ellipsoid) - SLD(solvent).  In the 
     81The contrast $\Delta\rho$ is defined as SLD(ellipsoid) - SLD(solvent).  In the 
    5282parameters, $R_a$ is the minor equatorial radius, $R_b$ is the major 
    5383equatorial radius, and $R_c$ is the polar radius of the ellipsoid. 
    … …  
    6999---------- 
    70100 
    71 L A Feigin and D I Svergun, *Structure Analysis by Small-Angle X-Ray 
    72 and Neutron Scattering*, Plenum, New York, 1987. 
     101[1] Finnigan, J.A., Jacobs, D.J., 1971. 
     102*Light scattering by ellipsoidal particles in solution*, 
     103J. Phys. D: Appl. Phys. 4, 72-77. doi:10.1088/0022-3727/4/1/310 
     104 
     105Authorship and Verification 
     106---------------------------- 
     107 
     108* **Author:** NIST IGOR/DANSE **Date:** pre 2010 
     109* **Last Modified by:** Paul Kienzle (improved calculation) **Date:** April 4, 2017 
     110* **Last Reviewed by:** Paul Kienzle &Richard Heenan **Date:**  April 4, 2017 
     111 
    73112""" 
    74113 
    75 from numpy import inf 
     114from numpy import inf, sin, cos, pi 
    76115 
    77116name = "triaxial_ellipsoid" 
    … …  
    91130               "Solvent scattering length density"], 
    92131              ["radius_equat_minor", "Ang", 20, [0, inf], "volume", 
    93                "Minor equatorial radius"], 
     132               "Minor equatorial radius, Ra"], 
    94133              ["radius_equat_major", "Ang", 400, [0, inf], "volume", 
    95                "Major equatorial radius"], 
     134               "Major equatorial radius, Rb"], 
    96135              ["radius_polar", "Ang", 10, [0, inf], "volume", 
    97                "Polar radius"], 
     136               "Polar radius, Rc"], 
    98137              ["theta", "degrees", 60, [-inf, inf], "orientation", 
    99138               "In plane angle"], 
    … …  
    112151    import numpy as np 
    113152    from .ellipsoid import ER as ellipsoid_ER 
     153     # now that radii can be in any size order, radii need sorting a,b,c where a~b and c is either much smaller or much larger 
     154     # also need some unit tests! 
     155     
    114156    return ellipsoid_ER(radius_polar, np.sqrt(radius_equat_minor * radius_equat_major)) 
    115157 
    … …  
    124166            phi_pd=15, phi_pd_n=1, 
    125167            psi_pd=15, psi_pd_n=1) 
     168q = 0.1 
     169# april 6 2017, rkh add unit tests, NOT compared with any other calc method, assume correct! 
     170# add 2d test after pull #890 
     171qx = q*cos(pi/6.0) 
     172qy = q*sin(pi/6.0) 
     173tests = [[{}, 0.05, 24.8839548033], 
     174#        [{'theta':80., 'phi':10.}, (qx, qy), 9999. ], 
     175        ] 
     176del qx, qy  # not necessary to delete, but cleaner 
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