Changeset 6da1d76 in sasmodels
- Timestamp:
- Oct 3, 2018 3:00:10 PM (6 years ago)
- Branches:
- master, core_shell_microgels, magnetic_model, ticket-1257-vesicle-product, ticket_1156, ticket_1265_superball, ticket_822_more_unit_tests
- Children:
- 17695aa
- Parents:
- 0535624 (diff), a1ec908 (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. - Files:
-
- 14 edited
Legend:
- Unmodified
- Added
- Removed
-
doc/guide/plugin.rst
rf796469 r2015f02 423 423 calculations, but instead rely on numerical integration to compute the 424 424 appropriately smeared pattern. 425 426 Each .py file also contains a function:: 427 428 def random(): 429 ... 430 431 This function provides a model-specific random parameter set which shows model 432 features in the USANS to SANS range. For example, core-shell sphere sets the 433 outer radius of the sphere logarithmically in `[20, 20,000]`, which sets the Q 434 value for the transition from flat to falling. It then uses a beta distribution 435 to set the percentage of the shape which is shell, giving a preference for very 436 thin or very thick shells (but never 0% or 100%). Using `-sets=10` in sascomp 437 should show a reasonable variety of curves over the default sascomp q range. 438 The parameter set is returned as a dictionary of `{parameter: value, ...}`. 439 Any model parameters not included in the dictionary will default according to 440 the code in the `_randomize_one()` function from sasmodels/compare.py. 425 441 426 442 Python Models -
sasmodels/__init__.py
re65c3ba ra1ec908 14 14 defining new models. 15 15 """ 16 __version__ = "0.9 7"16 __version__ = "0.98" 17 17 18 18 def data_files(): -
sasmodels/custom/__init__.py
r0f48f1e rd321747 12 12 import sys 13 13 import os 14 from os.path import basename, splitext 14 from os.path import basename, splitext, join as joinpath, exists, dirname 15 15 16 16 try: … … 18 18 from importlib.util import spec_from_file_location, module_from_spec # type: ignore 19 19 def load_module_from_path(fullname, path): 20 # type: (str, str) -> "module" 20 21 """load module from *path* as *fullname*""" 21 22 spec = spec_from_file_location(fullname, os.path.expanduser(path)) … … 27 28 import imp 28 29 def load_module_from_path(fullname, path): 30 # type: (str, str) -> "module" 29 31 """load module from *path* as *fullname*""" 30 32 # Clear out old definitions, if any … … 37 39 return module 38 40 41 _MODULE_CACHE = {} # type: Dict[str, Tuple("module", int)] 42 _MODULE_DEPENDS = {} # type: Dict[str, List[str]] 43 _MODULE_DEPENDS_STACK = [] # type: List[str] 39 44 def load_custom_kernel_module(path): 45 # type: str -> "module" 40 46 """load SAS kernel from *path* as *sasmodels.custom.modelname*""" 41 47 # Pull off the last .ext if it exists; there may be others 42 48 name = basename(splitext(path)[0]) 43 # Placing the model in the 'sasmodels.custom' name space. 44 kernel_module = load_module_from_path('sasmodels.custom.'+name, 45 os.path.expanduser(path)) 46 return kernel_module 49 path = os.path.expanduser(path) 50 51 # Reload module if necessary. 52 if need_reload(path): 53 # Assume the module file is the only dependency 54 _MODULE_DEPENDS[path] = set([path]) 55 56 # Load the module while pushing it onto the dependency stack. If 57 # this triggers any submodules, then they will add their dependencies 58 # to this module as the "working_on" parent. Pop the stack when the 59 # module is loaded. 60 _MODULE_DEPENDS_STACK.append(path) 61 module = load_module_from_path('sasmodels.custom.'+name, path) 62 _MODULE_DEPENDS_STACK.pop() 63 64 # Include external C code in the dependencies. We are looking 65 # for module.source and assuming that it is a list of C source files 66 # relative to the module itself. Any files that do not exist, 67 # such as those in the standard libraries, will be ignored. 68 # TODO: look in builtin module path for standard c sources 69 # TODO: share code with generate.model_sources 70 c_sources = getattr(module, 'source', None) 71 if isinstance(c_sources, (list, tuple)): 72 _MODULE_DEPENDS[path].update(_find_sources(path, c_sources)) 73 74 # Cache the module, and tag it with the newest timestamp 75 timestamp = max(os.path.getmtime(f) for f in _MODULE_DEPENDS[path]) 76 _MODULE_CACHE[path] = module, timestamp 77 78 #print("loading", os.path.basename(path), _MODULE_CACHE[path][1], 79 # [os.path.basename(p) for p in _MODULE_DEPENDS[path]]) 80 81 # Add path and all its dependence to the parent module, if there is one. 82 if _MODULE_DEPENDS_STACK: 83 working_on = _MODULE_DEPENDS_STACK[-1] 84 _MODULE_DEPENDS[working_on].update(_MODULE_DEPENDS[path]) 85 86 return _MODULE_CACHE[path][0] 87 88 def need_reload(path): 89 # type: str -> bool 90 """ 91 Return True if any path dependencies have a timestamp newer than the time 92 when the path was most recently loaded. 93 """ 94 # TODO: fails if a dependency has a modification time in the future 95 # If the newest dependency has a time stamp in the future, then this 96 # will be recorded as the cached time. When a second dependency 97 # is updated to the current time stamp, it will still be considered 98 # older than the current build and the reload will not be triggered. 99 # Could instead treat all future times as 0 here and in the code above 100 # which records the newest timestamp. This will force a reload when 101 # the future time is reached, but other than that should perform 102 # correctly. Probably not worth the extra code... 103 _, cache_time = _MODULE_CACHE.get(path, (None, -1)) 104 depends = _MODULE_DEPENDS.get(path, [path]) 105 #print("reload", any(cache_time < os.path.getmtime(p) for p in depends)) 106 #for f in depends: print(">>> ", f, os.path.getmtime(f)) 107 return any(cache_time < os.path.getmtime(p) for p in depends) 108 109 def _find_sources(path, source_list): 110 # type: (str, List[str]) -> List[str] 111 """ 112 Return a list of the sources relative to base file; ignore any that 113 are not found. 114 """ 115 root = dirname(path) 116 found = [] 117 for source_name in source_list: 118 source_path = joinpath(root, source_name) 119 if exists(source_path): 120 found.append(source_path) 121 return found -
sasmodels/kernelpy.py
r108e70e r91bd550 37 37 self.info = model_info 38 38 self.dtype = np.dtype('d') 39 logger.info("load python model " + self.info.name)40 39 41 40 def make_kernel(self, q_vectors): -
sasmodels/modelinfo.py
r0535624 r6da1d76 824 824 info.structure_factor = structure_factor 825 825 info.profile_axes = getattr(kernel_module, 'profile_axes', ['x', 'y']) 826 # Note: custom.load_custom_kernel_module assumes the C sources are defined 827 # by this attribute. 826 828 info.source = getattr(kernel_module, 'source', []) 827 829 info.c_code = getattr(kernel_module, 'c_code', None) -
sasmodels/models/bcc_paracrystal.py
r2d81cfe rda7b26b 1 1 r""" 2 .. warning:: This model and this model description are under review following 3 concerns raised by SasView users. If you need to use this model, 4 please email help@sasview.org for the latest situation. *The 5 SasView Developers. September 2018.* 6 2 7 Definition 3 8 ---------- … … 13 18 14 19 I(q) = \frac{\text{scale}}{V_p} V_\text{lattice} P(q) Z(q) 15 16 20 17 21 where *scale* is the volume fraction of spheres, $V_p$ is the volume of the … … 97 101 98 102 Authorship and Verification 99 --------------------------- -103 --------------------------- 100 104 101 105 * **Author:** NIST IGOR/DANSE **Date:** pre 2010 -
sasmodels/models/be_polyelectrolyte.py
ref07e95 rca77fc1 1 1 r""" 2 .. note:: Please read the Validation section below. 3 2 4 Definition 3 5 ---------- … … 11 13 12 14 I(q) = K\frac{q^2+k^2}{4\pi L_b\alpha ^2} 13 \frac{1}{1+r_{0}^ 2(q^2+k^2)(q^2-12hC_a/b^2)} + background15 \frac{1}{1+r_{0}^4(q^2+k^2)(q^2-12hC_a/b^2)} + background 14 16 15 17 k^2 = 4\pi L_b(2C_s + \alpha C_a) 16 18 17 r_{0}^2 = \frac{ 1}{\alpha \sqrt{C_a} \left( b/\sqrt{48\pi L_b}\right)}19 r_{0}^2 = \frac{b}{\alpha \sqrt{C_a 48\pi L_b}} 18 20 19 21 where 20 22 21 23 $K$ is the contrast factor for the polymer which is defined differently than in 22 other models and is given in barns where $1 barn = 10^{-24}cm^2$. $K$ is24 other models and is given in barns where 1 $barn = 10^{-24}$ $cm^2$. $K$ is 23 25 defined as: 24 26 … … 29 31 a = b_p - (v_p/v_s) b_s 30 32 31 where $b_p$ and $b_s$ are sum of the scattering lengths of the atoms 32 constituting the monomer of the polymer and the sum of the scattering lengths 33 of the atoms constituting the solvent molecules respectively, and $v_p$ and 34 $v_s$ are the partial molar volume of the polymer and the solvent respectively 35 36 $L_b$ is the Bjerrum length(|Ang|) - **Note:** This parameter needs to be 37 kept constant for a given solvent and temperature! 38 39 $h$ is the virial parameter (|Ang^3|/mol) - **Note:** See [#Borue]_ for the 40 correct interpretation of this parameter. It incorporates second and third 41 virial coefficients and can be Negative. 42 43 $b$ is the monomer length(|Ang|), $C_s$ is the concentration of monovalent 44 salt(mol/L), $\alpha$ is the ionization degree (ionization degree : ratio of 45 charged monomers to total number of monomers), $C_a$ is the polymer molar 46 concentration(mol/L), and $background$ is the incoherent background. 33 where: 34 35 - $b_p$ and $b_s$ are **sum of the scattering lengths of the atoms** 36 constituting the polymer monomer and the solvent molecules, respectively. 37 38 - $v_p$ and $v_s$ are the partial molar volume of the polymer and the 39 solvent, respectively. 40 41 - $L_b$ is the Bjerrum length (|Ang|) - **Note:** This parameter needs to be 42 kept constant for a given solvent and temperature! 43 44 - $h$ is the virial parameter (|Ang^3|) - **Note:** See [#Borue]_ for the 45 correct interpretation of this parameter. It incorporates second and third 46 virial coefficients and can be *negative*. 47 48 - $b$ is the monomer length (|Ang|). 49 50 - $C_s$ is the concentration of monovalent salt(1/|Ang^3| - internally converted from mol/L). 51 52 - $\alpha$ is the degree of ionization (the ratio of charged monomers to the total 53 number of monomers) 54 55 - $C_a$ is the polymer molar concentration (1/|Ang^3| - internally converted from mol/L) 56 57 - $background$ is the incoherent background. 47 58 48 59 For 2D data the scattering intensity is calculated in the same way as 1D, … … 52 63 53 64 q = \sqrt{q_x^2 + q_y^2} 65 66 Validation 67 ---------- 68 69 As of the last revision, this code is believed to be correct. However it 70 needs further validation and should be used with caution at this time. The 71 history of this code goes back to a 1998 implementation. It was recently noted 72 that in that implementation, while both the polymer concentration and salt 73 concentration were converted from experimental units of mol/L to more 74 dimensionally useful units of 1/|Ang^3|, only the converted version of the 75 polymer concentration was actually being used in the calculation while the 76 unconverted salt concentration (still in apparent units of mol/L) was being 77 used. This was carried through to Sasmodels as used for SasView 4.1 (though 78 the line of code converting the salt concentration to the new units was removed 79 somewhere along the line). Simple dimensional analysis of the calculation shows 80 that the converted salt concentration should be used, which the original code 81 suggests was the intention, so this has now been corrected (for SasView 4.2). 82 Once better validation has been performed this note will be removed. 54 83 55 84 References … … 66 95 67 96 * **Author:** NIST IGOR/DANSE **Date:** pre 2010 68 * **Last Modified by:** Paul Kienzle **Date:** July 24, 201669 * **Last Reviewed by:** Paul Butler and Richard Heenan **Date:** October 07, 201697 * **Last Modified by:** Paul Butler **Date:** September 25, 2018 98 * **Last Reviewed by:** Paul Butler **Date:** September 25, 2018 70 99 """ 71 100 … … 92 121 ["contrast_factor", "barns", 10.0, [-inf, inf], "", "Contrast factor of the polymer"], 93 122 ["bjerrum_length", "Ang", 7.1, [0, inf], "", "Bjerrum length"], 94 ["virial_param", "Ang^3 /mol", 12.0, [-inf, inf], "", "Virial parameter"],123 ["virial_param", "Ang^3", 12.0, [-inf, inf], "", "Virial parameter"], 95 124 ["monomer_length", "Ang", 10.0, [0, inf], "", "Monomer length"], 96 125 ["salt_concentration", "mol/L", 0.0, [-inf, inf], "", "Concentration of monovalent salt"], … … 102 131 103 132 def Iq(q, 104 contrast_factor =10.0,105 bjerrum_length =7.1,106 virial_param =12.0,107 monomer_length =10.0,108 salt_concentration =0.0,109 ionization_degree =0.05,110 polymer_concentration =0.7):133 contrast_factor, 134 bjerrum_length, 135 virial_param, 136 monomer_length, 137 salt_concentration, 138 ionization_degree, 139 polymer_concentration): 111 140 """ 112 :param q: Input q-value 113 :param contrast_factor: Contrast factor of the polymer 114 :param bjerrum_length: Bjerrum length 115 :param virial_param: Virial parameter 116 :param monomer_length: Monomer length 117 :param salt_concentration: Concentration of monovalent salt 118 :param ionization_degree: Degree of ionization 119 :param polymer_concentration: Polymer molar concentration 120 :return: 1-D intensity 141 :params: see parameter table 142 :return: 1-D form factor for polyelectrolytes in low salt 143 144 parameter names, units, default values, and behavior (volume, sld etc) are 145 defined in the parameter table. The concentrations are converted from 146 experimental mol/L to dimensionaly useful 1/A3 in first two lines 121 147 """ 122 148 123 concentration = polymer_concentration * 6.022136e-4 124 125 k_square = 4.0 * pi * bjerrum_length * (2*salt_concentration + 126 ionization_degree * concentration) 127 128 r0_square = 1.0/ionization_degree/sqrt(concentration) * \ 149 concentration_pol = polymer_concentration * 6.022136e-4 150 concentration_salt = salt_concentration * 6.022136e-4 151 152 k_square = 4.0 * pi * bjerrum_length * (2*concentration_salt + 153 ionization_degree * concentration_pol) 154 155 r0_square = 1.0/ionization_degree/sqrt(concentration_pol) * \ 129 156 (monomer_length/sqrt((48.0*pi*bjerrum_length))) 130 157 … … 133 160 134 161 term2 = 1.0 + r0_square**2 * (q**2 + k_square) * \ 135 (q**2 - (12.0 * virial_param * concentration /(monomer_length**2)))162 (q**2 - (12.0 * virial_param * concentration_pol/(monomer_length**2))) 136 163 137 164 return term1/term2 … … 174 201 175 202 # Accuracy tests based on content in test/utest_other_models.py 203 # Note that these should some day be validated beyond this self validation 204 # (circular reasoning). -- i.e. the "good value," at least for those with 205 # non zero salt concentrations, were obtained by running the current 206 # model in SasView and copying the appropriate result here. 207 # PDB -- Sep 26, 2018 176 208 [{'contrast_factor': 10.0, 177 209 'bjerrum_length': 7.1, … … 184 216 }, 0.001, 0.0948379], 185 217 186 # Additional tests with larger range of parameters187 218 [{'contrast_factor': 10.0, 188 219 'bjerrum_length': 100.0, 189 220 'virial_param': 3.0, 190 'monomer_length': 1.0,191 'salt_concentration': 10.0,192 'ionization_degree': 2.0,193 'polymer_concentration': 10.0,221 'monomer_length': 5.0, 222 'salt_concentration': 1.0, 223 'ionization_degree': 0.1, 224 'polymer_concentration': 1.0, 194 225 'background': 0.0, 195 }, 0.1, -3.75693800588],226 }, 0.1, 0.253469484], 196 227 197 228 [{'contrast_factor': 10.0, 198 229 'bjerrum_length': 100.0, 199 230 'virial_param': 3.0, 200 'monomer_length': 1.0,201 'salt_concentration': 10.0,202 'ionization_degree': 2.0,203 'polymer_concentration': 10.0,204 'background': 100.0205 }, 5.0, 100.029142149],231 'monomer_length': 5.0, 232 'salt_concentration': 1.0, 233 'ionization_degree': 0.1, 234 'polymer_concentration': 1.0, 235 'background': 1.0, 236 }, 0.05, 1.738358122], 206 237 207 238 [{'contrast_factor': 100.0, 208 239 'bjerrum_length': 10.0, 209 'virial_param': 180.0,210 'monomer_length': 1.0,240 'virial_param': 12.0, 241 'monomer_length': 10.0, 211 242 'salt_concentration': 0.1, 212 243 'ionization_degree': 0.5, 213 244 'polymer_concentration': 0.1, 214 'background': 0.0,215 }, 200., 1.80664667511e-06],245 'background': 0.01, 246 }, 0.5, 0.012881893], 216 247 ] -
sasmodels/models/fcc_paracrystal.py
r2d81cfe rda7b26b 3 3 #note - calculation requires double precision 4 4 r""" 5 .. warning:: This model and this model description are under review following 6 concerns raised by SasView users. If you need to use this model, 7 please email help@sasview.org for the latest situation. *The 8 SasView Developers. September 2018.* 9 10 Definition 11 ---------- 12 5 13 Calculates the scattering from a **face-centered cubic lattice** with 6 14 paracrystalline distortion. Thermal vibrations are considered to be … … 8 16 Paracrystalline distortion is assumed to be isotropic and characterized by 9 17 a Gaussian distribution. 10 11 Definition12 ----------13 18 14 19 The scattering intensity $I(q)$ is calculated as … … 23 28 is the paracrystalline structure factor for a face-centered cubic structure. 24 29 25 Equation (1) of the 1990 reference is used to calculate $Z(q)$, using 26 equations (23)-(25) from the 1987 paper for $Z1$, $Z2$, and $Z3$. 30 Equation (1) of the 1990 reference\ [#CIT1990]_ is used to calculate $Z(q)$, 31 using equations (23)-(25) from the 1987 paper\ [#CIT1987]_ for $Z1$, $Z2$, and 32 $Z3$. 27 33 28 34 The lattice correction (the occupied volume of the lattice) for a … … 88 94 ---------- 89 95 90 Hideki Matsuoka et. al. *Physical Review B*, 36 (1987) 1754-1765 91 (Original Paper) 96 .. [#CIT1987] Hideki Matsuoka et. al. *Physical Review B*, 36 (1987) 1754-1765 97 (Original Paper) 98 .. [#CIT1990] Hideki Matsuoka et. al. *Physical Review B*, 41 (1990) 3854 -3856 99 (Corrections to FCC and BCC lattice structure calculation) 92 100 93 Hideki Matsuoka et. al. *Physical Review B*, 41 (1990) 3854 -3856 94 (Corrections to FCC and BCC lattice structure calculation) 101 Authorship and Verification 102 --------------------------- 103 104 * **Author:** NIST IGOR/DANSE **Date:** pre 2010 105 * **Last Modified by:** Paul Butler **Date:** September 29, 2016 106 * **Last Reviewed by:** Richard Heenan **Date:** March 21, 2016 95 107 """ 96 108 -
sasmodels/models/sc_paracrystal.py
r2d81cfe rda7b26b 1 1 r""" 2 .. warning:: This model and this model description are under review following 3 concerns raised by SasView users. If you need to use this model, 4 please email help@sasview.org for the latest situation. *The 5 SasView Developers. September 2018.* 6 7 Definition 8 ---------- 9 2 10 Calculates the scattering from a **simple cubic lattice** with 3 11 paracrystalline distortion. Thermal vibrations are considered to be … … 5 13 Paracrystalline distortion is assumed to be isotropic and characterized 6 14 by a Gaussian distribution. 7 8 Definition9 ----------10 15 11 16 The scattering intensity $I(q)$ is calculated as … … 20 25 $Z(q)$ is the paracrystalline structure factor for a simple cubic structure. 21 26 22 Equation (16) of the 1987 reference is used to calculate $Z(q)$, using 23 equations (13)-(15) from the 1987 paper for Z1, Z2, and Z3. 27 Equation (16) of the 1987 reference\ [#CIT1987]_ is used to calculate $Z(q)$, 28 using equations (13)-(15) from the 1987 paper\ [#CIT1987]_ for $Z1$, $Z2$, and 29 $Z3$. 24 30 25 31 The lattice correction (the occupied volume of the lattice) for a simple cubic … … 91 97 Reference 92 98 --------- 93 Hideki Matsuoka et. al. *Physical Review B,* 36 (1987) 1754-176594 (Original Paper)95 99 96 Hideki Matsuoka et. al. *Physical Review B,* 41 (1990) 3854 -3856 97 (Corrections to FCC and BCC lattice structure calculation) 100 .. [#CIT1987] Hideki Matsuoka et. al. *Physical Review B*, 36 (1987) 1754-1765 101 (Original Paper) 102 .. [#CIT1990] Hideki Matsuoka et. al. *Physical Review B*, 41 (1990) 3854 -3856 103 (Corrections to FCC and BCC lattice structure calculation) 104 105 Authorship and Verification 106 --------------------------- 107 108 * **Author:** NIST IGOR/DANSE **Date:** pre 2010 109 * **Last Modified by:** Paul Butler **Date:** September 29, 2016 110 * **Last Reviewed by:** Richard Heenan **Date:** March 21, 2016 98 111 """ 99 112 -
sasmodels/sasview_model.py
r0535624 r6da1d76 62 62 #: set of defined models (standard and custom) 63 63 MODELS = {} # type: Dict[str, SasviewModelType] 64 # TODO: remove unused MODEL_BY_PATH cache once sasview no longer references it 64 65 #: custom model {path: model} mapping so we can check timestamps 65 66 MODEL_BY_PATH = {} # type: Dict[str, SasviewModelType] 67 #: Track modules that we have loaded so we can determine whether the model 68 #: has changed since we last reloaded. 69 _CACHED_MODULE = {} # type: Dict[str, "module"] 66 70 67 71 def find_model(modelname): … … 106 110 Load a custom model given the model path. 107 111 """ 108 model = MODEL_BY_PATH.get(path, None)109 if model is not None and model.timestamp == getmtime(path):110 #logger.info("Model already loaded %s", path)111 return model112 113 112 #logger.info("Loading model %s", path) 113 114 # Load the kernel module. This may already be cached by the loader, so 115 # only requires checking the timestamps of the dependents. 114 116 kernel_module = custom.load_custom_kernel_module(path) 115 if hasattr(kernel_module, 'Model'): 116 model = kernel_module.Model 117 118 # Check if the module has changed since we last looked. 119 reloaded = kernel_module != _CACHED_MODULE.get(path, None) 120 _CACHED_MODULE[path] = kernel_module 121 122 # Turn the module into a model. We need to do this in even if the 123 # model has already been loaded so that we can determine the model 124 # name and retrieve it from the MODELS cache. 125 model = getattr(kernel_module, 'Model', None) 126 if model is not None: 117 127 # Old style models do not set the name in the class attributes, so 118 128 # set it here; this name will be overridden when the object is created … … 127 137 model_info = modelinfo.make_model_info(kernel_module) 128 138 model = make_model_from_info(model_info) 129 model.timestamp = getmtime(path)130 139 131 140 # If a model name already exists and we are loading a different model, … … 143 152 _previous_name, model.name, model.filename) 144 153 145 MODELS[model.name] = model 146 MODEL_BY_PATH[path] = model 147 return model 154 # Only update the model if the module has changed 155 if reloaded or model.name not in MODELS: 156 MODELS[model.name] = model 157 158 return MODELS[model.name] 148 159 149 160 -
sasmodels/compare.py
rbd7630d rb6dab59 1151 1151 'rel_err' : True, 1152 1152 'explore' : False, 1153 'use_demo' : True,1153 'use_demo' : False, 1154 1154 'zero' : False, 1155 1155 'html' : False, -
sasmodels/direct_model.py
r7b9e4dd rb6d1d52 31 31 from . import resolution2d 32 32 from .details import make_kernel_args, dispersion_mesh 33 from .modelinfo import DEFAULT_BACKGROUND34 33 35 34 # pylint: disable=unused-import … … 350 349 351 350 # Need to pull background out of resolution for multiple scattering 352 background = pars.get('background', DEFAULT_BACKGROUND) 351 default_background = self._model.info.parameters.common_parameters[1].default 352 background = pars.get('background', default_background) 353 353 pars = pars.copy() 354 354 pars['background'] = 0. -
sasmodels/generate.py
r6e45516 rb6dab59 968 968 pars = model_info.parameters.kernel_parameters 969 969 else: 970 pars = model_info.parameters.COMMON + model_info.parameters.kernel_parameters 970 pars = (model_info.parameters.common_parameters 971 + model_info.parameters.kernel_parameters) 971 972 partable = make_partable(pars) 972 973 subst = dict(id=model_info.id.replace('_', '-'), -
sasmodels/models/hardsphere.py
r2d81cfe rb6dab59 171 171 # VR defaults to 1.0 172 172 173 demo = dict(radius_effective=200, volfraction=0.2,174 radius_effective_pd=0.1, radius_effective_pd_n=40)175 173 # Q=0.001 is in the Taylor series, low Q part, so add Q=0.1, 176 174 # assuming double precision sasview is correct
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