Changes in / [e481a39:3f12f59] in sasmodels


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  • doc/conf.py

    r4a21670c r22975f0  
    233233 
    234234numfig = True 
     235#numfig_format = {"figure": "Fig. %s", "table": "Table %s", "code-block": "Program %s"} 

  • sasmodels/compare.py

    r72a081d r98d6cfc  
    6969    -accuracy=Low accuracy of the resolution calculation Low, Mid, High, Xhigh 
    7070    -edit starts the parameter explorer 
     71    -default/-demo* use demo vs default parameters 
    7172 
    7273Any two calculation engines can be selected for comparison: 
    … …  
    631632    'hist', 'nohist', 
    632633    'edit', 
     634    'demo', 'default', 
    633635    ]) 
    634636VALUE_OPTIONS = [ 
    … …  
    654656 
    655657 
    656 def get_demo_pars(model_info): 
     658def get_pars(model_info, use_demo=False): 
    657659    """ 
    658660    Extract demo parameters from the model definition. 
    … …  
    670672 
    671673    # Plug in values given in demo 
    672     pars.update(model_info['demo']) 
     674    if use_demo: 
     675        pars.update(model_info['demo']) 
    673676    return pars 
    674677 
    … …  
    727730        'rel_err'   : True, 
    728731        'explore'   : False, 
     732        'use_demo'  : True, 
    729733    } 
    730734    engines = [] 
    … …  
    765769        elif arg == '-sasview': engines.append(arg[1:]) 
    766770        elif arg == '-edit':    opts['explore'] = True 
     771        elif arg == '-demo':    opts['use_demo'] = True 
     772        elif arg == '-default':    opts['use_demo'] = False 
    767773    # pylint: enable=bad-whitespace 
    768774 
    … …  
    782788    # Get demo parameters from model definition, or use default parameters 
    783789    # if model does not define demo parameters 
    784     pars = get_demo_pars(model_info) 
     790    pars = get_pars(model_info, opts['use_demo']) 
     791 
    785792 
    786793    # Fill in parameters given on the command line 

  • sasmodels/models/core_shell_ellipsoid_xt.py

    r29172aa r3556ad7  
    8989parameters = [ 
    9090    ["equat_core",    "Ang",       20,   [0, inf],    "volume",      "Equatorial radius of core"], 
    91     ["x_core",        "None",       3,   [0, inf],    "volume",      "Polar radius of core"], 
    92     ["t_shell",       "Ang",       30,   [0, inf],    "volume",      "Equatorial radius of shell"], 
    93     ["x_polar_shell", "",           1,   [0, inf],    "volume",      "Polar radius of shell"], 
     91    ["x_core",        "None",       3,   [0, inf],    "volume",      "axial ratio of core, X = r_polar/r_equatorial"], 
     92    ["t_shell",       "Ang",       30,   [0, inf],    "volume",      "thickness of shell at equator"], 
     93    ["x_polar_shell", "",           1,   [0, inf],    "volume",      "ratio of thickness of shell at pole to that at equator"], 
    9494    ["sld_core",      "1e-6/Ang^2", 2,   [-inf, inf], "",            "Core scattering length density"], 
    9595    ["sld_shell",     "1e-6/Ang^2", 1,   [-inf, inf], "",            "Shell scattering length density"], 

  • sasmodels/models/core_shell_sphere.py

    raa2edb2 r3556ad7  
    1919    V_s(\rho_s-\rho_{solv})\frac{\sin(qr_s)-qr_s\cos(qr_s)}{(qr_s)^3}\right] 
    2020 
    21 where $V_s$ is the volume of the outer shell, $V_c$ is 
    22 the volume of the core, $r_s$ is the radius of the shell, $r_c$ is the radius of the 
     21where $V_s$ is the volume of the whole particle, $V_c$ is 
     22the volume of the core, $r_s$ = $radius$ + $thickness$ is the radius of the particle, $r_c$ is the radius of the 
    2323core, $\rho_c$ is the scattering length density of the core, $\rho_s$ is the scattering length 
    2424density of the shell, $\rho_{solv}$ is the scattering length density of the solvent. 
    … …  
    3030effective radius for $S(Q)$ when $P(Q) \cdot S(Q)$ is applied. 
    3131 
    32 Reference 
    33 --------- 
     32References 
     33---------- 
    3434 
    3535A Guinier and G Fournet, *Small-Angle Scattering of X-Rays*, John Wiley and Sons, New York, (1955) 
    … …  
    4949title = "Form factor for a monodisperse spherical particle with particle with a core-shell structure." 
    5050description = """ 
    51     F^2(q) = 3/V_s [V_c (core_sld-shell_sld) (sin(q*radius)-q*radius*cos(q*radius))/(q*radius)^3  
    52                    + V_s (shell_sld-solvent_sld) (sin(q*r_s)-q*r_s*cos(q*r_s))/(q*r_s)^3] 
     51    F^2(q) = 3/V_s [V_c (sld_core-sld_shell) (sin(q*radius)-q*radius*cos(q*radius))/(q*radius)^3  
     52                   + V_s (sld_shell-sld_solvent) (sin(q*r_s)-q*r_s*cos(q*r_s))/(q*r_s)^3] 
    5353 
    5454            V_s: Volume of the sphere shell 
    … …  
    6262parameters = [["radius",      "Ang",        60.0, [0, inf],    "volume", "Sphere core radius"], 
    6363              ["thickness",   "Ang",        10.0, [0, inf],    "volume", "Sphere shell thickness"], 
    64               ["core_sld",    "1e-6/Ang^2", 1.0,  [-inf, inf], "",       "Sphere core scattering length density"], 
    65               ["shell_sld",   "1e-6/Ang^2", 2.0,  [-inf, inf], "",       "Sphere shell scattering length density"], 
    66               ["solvent_sld", "1e-6/Ang^2", 3.0,  [-inf, inf],  "",      "Solvent scattering length density"]] 
     64              ["sld_core",    "1e-6/Ang^2", 1.0,  [-inf, inf], "",       "core scattering length density"], 
     65              ["sld_shell",   "1e-6/Ang^2", 2.0,  [-inf, inf], "",       "shell scattering length density"], 
     66              ["sld_solvent", "1e-6/Ang^2", 3.0,  [-inf, inf],  "",      "Solvent scattering length density"]] 
    6767# pylint: enable=bad-whitespace, line-too-long 
    6868 
    … …  
    7070 
    7171demo = dict(scale=1, background=0, radius=60, thickness=10, 
    72             core_sld=1.0, shell_sld=2.0, solvent_sld=0.0) 
     72            sld_core=1.0, sld_shell=2.0, sld_solvent=0.0) 
    7373 
    7474oldname = 'CoreShellModel' 
    75 oldpars = {} 
     75oldpars = dict( sld_core='core_sld', 
     76               sld_shell='shell_sld', 
     77               sld_solvent='solvent_sld') 
    7678 
    7779def ER(radius, thickness): 
    … …  
    99101         [{'radius': 60.0, 
    100102           'thickness': 10.0, 
    101            'core_sld': 1.0, 
    102            'shell_sld':2.0, 
    103            'solvent_sld':3.0, 
     103           'sld_core': 1.0, 
     104           'sld_shell':2.0, 
     105           'sld_solvent':3.0, 
    104106           'background':0.0 
    105107          }, 0.4, 0.000698838]] 

  • sasmodels/models/cylinder.py

    r5933c7f r6ef4293  
    3131To provide easy access to the orientation of the cylinder, we define the 
    3232axis of the cylinder using two angles $\theta$ and $\phi$. Those angles 
    33 are defined in :numref:`figure #<cylinder-angle-definition>`. 
     33are defined in :numref:`cylinder-angle-definition`. 
    3434 
    3535.. _cylinder-angle-definition: 

  • sasmodels/models/ellipsoid.py

    r43b7eea r3556ad7  
    22# Note: model title and parameter table are inserted automatically 
    33r""" 
    4 The form factor is normalized by the particle volume. 
     4The form factor is normalized by the particle volume  
    55 
    66Definition 
    … …  
    3131 
    3232$\alpha$ is the angle between the axis of the ellipsoid and $\vec q$, 
    33 $V$ is the volume of the ellipsoid, $R_p$ is the polar radius along the 
     33$V = (4/3)\pi R_pR_e^2$ is the volume of the ellipsoid , $R_p$ is the polar radius along the 
    3434rotational axis of the ellipsoid, $R_e$ is the equatorial radius perpendicular 
    3535to the rotational axis of the ellipsoid and $\Delta \rho$ (contrast) is the 
    … …  
    4141:ref:`cylinder orientation figure <cylinder-angle-definition>`. 
    4242For the ellipsoid, $\theta$ is the angle between the rotational axis 
    43 and the $z$-axis. 
     43and the $z$ -axis. 
    4444 
    4545NB: The 2nd virial coefficient of the solid ellipsoid is calculated based 
    … …  
    5454.. figure:: img/ellipsoid_angle_projection.jpg 
    5555 
    56     The angles for oriented ellipsoid. 
     56    The angles for oriented ellipsoid, shown here as oblate, $a$ = $R_p$ and $b$ = $R_e$ 
    5757 
    5858Validation 
    … …  
    7474    calculated from our 2D model and the intensity from the NIST SANS 
    7575    analysis software. The parameters used were: *scale* = 1.0, 
    76     *rpolar* = 20 |Ang|, *requatorial* = 400 |Ang|, 
     76    *r_polar* = 20 |Ang|, *r_equatorial* = 400 |Ang|, 
    7777    *contrast* = 3e-6 |Ang^-2|, and *background* = 0.0 |cm^-1|. 
    7878 
    … …  
    102102description = """\ 
    103103P(q.alpha)= scale*f(q)^2 + background, where f(q)= 3*(sld 
    104         - solvent_sld)*V*[sin(q*r(Rp,Re,alpha)) 
     104        - sld_solvent)*V*[sin(q*r(Rp,Re,alpha)) 
    105105        -q*r*cos(qr(Rp,Re,alpha))] 
    106106        /[qr(Rp,Re,alpha)]^3" 
    … …  
    110110 
    111111        sld: SLD of the ellipsoid 
    112         solvent_sld: SLD of the solvent 
     112        sld_solvent: SLD of the solvent 
    113113        V: volume of the ellipsoid 
    114114        Rp: polar radius of the ellipsoid 
    … …  
    120120parameters = [["sld", "1e-6/Ang^2", 4, [-inf, inf], "", 
    121121               "Ellipsoid scattering length density"], 
    122               ["solvent_sld", "1e-6/Ang^2", 1, [-inf, inf], "", 
     122              ["sld_solvent", "1e-6/Ang^2", 1, [-inf, inf], "", 
    123123               "Solvent scattering length density"], 
    124               ["rpolar", "Ang", 20, [0, inf], "volume", 
     124              ["r_polar", "Ang", 20, [0, inf], "volume", 
    125125               "Polar radius"], 
    126               ["requatorial", "Ang", 400, [0, inf], "volume", 
     126              ["r_equatorial", "Ang", 400, [0, inf], "volume", 
    127127               "Equatorial radius"], 
    128128              ["theta", "degrees", 60, [-inf, inf], "orientation", 
    … …  
    134134source = ["lib/sph_j1c.c", "lib/gauss76.c", "ellipsoid.c"] 
    135135 
    136 def ER(rpolar, requatorial): 
     136def ER(r_polar, r_equatorial): 
    137137    import numpy as np 
    138138 
    139     ee = np.empty_like(rpolar) 
    140     idx = rpolar > requatorial 
    141     ee[idx] = (rpolar[idx] ** 2 - requatorial[idx] ** 2) / rpolar[idx] ** 2 
    142     idx = rpolar < requatorial 
    143     ee[idx] = (requatorial[idx] ** 2 - rpolar[idx] ** 2) / requatorial[idx] ** 2 
    144     idx = rpolar == requatorial 
    145     ee[idx] = 2 * rpolar[idx] 
    146     valid = (rpolar * requatorial != 0) 
     139    ee = np.empty_like(r_polar) 
     140    idx = r_polar > r_equatorial 
     141    ee[idx] = (r_polar[idx] ** 2 - r_equatorial[idx] ** 2) / r_polar[idx] ** 2 
     142    idx = r_polar < r_equatorial 
     143    ee[idx] = (r_equatorial[idx] ** 2 - r_polar[idx] ** 2) / r_equatorial[idx] ** 2 
     144    idx = r_polar == r_equatorial 
     145    ee[idx] = 2 * r_polar[idx] 
     146    valid = (r_polar * r_equatorial != 0) 
    147147    bd = 1.0 - ee[valid] 
    148148    e1 = np.sqrt(ee[valid]) 
    … …  
    152152    delta = 0.75 * b1 * b2 
    153153 
    154     ddd = np.zeros_like(rpolar) 
    155     ddd[valid] = 2.0 * (delta + 1.0) * rpolar * requatorial ** 2 
     154    ddd = np.zeros_like(r_polar) 
     155    ddd[valid] = 2.0 * (delta + 1.0) * r_polar * r_equatorial ** 2 
    156156    return 0.5 * ddd ** (1.0 / 3.0) 
    157157 
    158158 
    159159demo = dict(scale=1, background=0, 
    160             sld=6, solvent_sld=1, 
    161             rpolar=50, requatorial=30, 
     160            sld=6, sld_solvent=1, 
     161            r_polar=50, r_equatorial=30, 
    162162            theta=30, phi=15, 
    163             rpolar_pd=.2, rpolar_pd_n=15, 
    164             requatorial_pd=.2, requatorial_pd_n=15, 
     163            r_polar_pd=.2, r_polar_pd_n=15, 
     164            r_equatorial_pd=.2, r_equatorial_pd_n=15, 
    165165            theta_pd=15, theta_pd_n=45, 
    166166            phi_pd=15, phi_pd_n=1) 
    167167oldname = 'EllipsoidModel' 
    168168oldpars = dict(theta='axis_theta', phi='axis_phi', 
    169                sld='sldEll', solvent_sld='sldSolv', 
    170                rpolar='radius_a', requatorial='radius_b') 
     169               sld='sldEll', sld_solvent='sldSolv', 
     170               r_polar='radius_a', r_equatorial='radius_b') 

  • sasmodels/models/parallelepiped.py

    r5933c7f r6ef4293  
    77---------- 
    88 
    9 | This model calculates the scattering from a rectangular parallelepiped (:numref:`Figure #<parallelepiped-image>`). 
     9| This model calculates the scattering from a rectangular parallelepiped (:numref:`parallelepiped-image`). 
    1010| If you need to apply polydispersity, see also :ref:`rectangular-prism`. 
    1111 

  • sasmodels/models/triaxial_ellipsoid.py

    r5933c7f r6ef4293  
    3636we define the axis of the cylinder using the angles $\theta$, $\phi$ 
    3737and $\psi$. These angles are defined on 
    38 :numref:`figure #<triaxial-ellipsoid-angles>`. 
     38:numref:`triaxial-ellipsoid-angles`. 
    3939The angle $\psi$ is the rotational angle around its own $c$ axis 
    4040against the $q$ plane. For example, $\psi = 0$ when the 
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