From: Pascale Noyret Date: Tue, 21 Feb 2012 13:05:49 +0000 (+0000) Subject: version travail X-Git-Tag: LOGILAB~206 X-Git-Url: http://git.salome-platform.org/gitweb/?a=commitdiff_plain;h=c3bec282161de6c863d4126127b0f7f02077fb4e;p=tools%2Feficas.git version travail --- diff --git a/MAP/CMakeLists.txt b/MAP/CMakeLists.txt index e7e4546f..63a1fcdb 100644 --- a/MAP/CMakeLists.txt +++ b/MAP/CMakeLists.txt @@ -28,7 +28,7 @@ install ( FILES qtEficas_map.py style.py prefs_MAP.py configuration_MAP.py - catalogues_MAP.ini + #catalogues_MAP.ini s_poly_st_1_V1.py s_poly_st_1_V1_clefs_docu s_scc_st_2_V1.py diff --git a/MAP/cataDebut.py b/MAP/cataDebut.py new file mode 100644 index 00000000..eaa6dcc3 --- /dev/null +++ b/MAP/cataDebut.py @@ -0,0 +1,177 @@ +#)# -*- coding: utf-8 -*- +# +## -------------------------------------------------- +## debut entete +## -------------------------------------------------- +# +from Accas import * +import os +import sys +import types +from prefs_MAP import PATH_MAP + + +class Tuple: + def __init__(self,ntuple): + self.ntuple=ntuple + + def __convert__(self,valeur): + if type(valeur) == types.StringType: + return None + if len(valeur) != self.ntuple: + return None + return valeur + + def info(self): + return "Tuple de %s elements" % self.ntuple + + __repr__=info + __str__=info + +# +#CONTEXT.debug = 1 +JdC = JDC_CATA ( code = 'MAP', + execmodul = None, + #regles=(AU_MOINS_UN('DISPL',),A_CLASSER('RBM','DISPL')) + )# Fin JDC_CATA +# + + +specter_path=PROC(nom='specter_path',op=None, + path=SIMP(typ='Fichier',defaut='/home/A28637/SVN_MAP/trunk/vendor/PERFORM_20110225/perfect_dev/tools/bin/specter', statut='o', fr = '', ang = 'A class for the definition of a file', max=1,), + ) + + +residual_energy_model=PROC(nom='residual_energy_model',op=None, + access=SIMP(statut= 'o',typ = 'TXM', defaut="user", max=1), + beta=FACT(statut='o', max=1, fr = '', ang = 'A class for the definition of a numerical value', + value=SIMP(statut= 'o',typ = 'R', defaut=0.779, max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='None', max=1), + ), + short_doc=SIMP(statut= 'o',typ = 'TXM', defaut="The model which gives the total number of surviving point defects for cascades in iron up to 10 keV. ", max=1), + alpha=FACT(statut='o', max=1, fr = '', ang = 'A class for the definition of a numerical value', + value=SIMP(statut= 'o',typ = 'R', defaut=5.67, max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='None', max=1), + ), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + ) +mfvisc2_path=PROC(nom='mfvisc2_path',op=None, + path=SIMP(typ='Fichier',defaut='/home/A28637/SVN_MAP/trunk/vendor/PERFORM_20110225/perfect_dev/tools/bin/mfvisc', statut='o', fr = '', ang = 'A class for the definition of a file', max=1,), + ) + + +mfvisc2_parametrisation=PROC(nom='mfvisc2_parametrisation',op=None, + stop_if_solute_loss=FACT(statut='o', max=1, fr = '', ang = 'Choose Yes if you want the rate-theory calculation to stop when a solute loss (i.e. Cu or He in the case of RPV and INTERN respectively) is detected. Choose No otherwise.', + value=SIMP(statut= 'o',typ = 'TXM', defaut="No", max=1,into=['Yes', 'No']), + ), + bound_solute=FACT(statut='o', max=1, fr = '', ang = 'Choose Yes if you want the to artifically impose the solute conservation by imposing a null flux for concentrations at Nob.', + value=SIMP(statut= 'o',typ = 'TXM', defaut="Yes", max=1,into=['Yes', 'No']), + ), + numerical_scheme_i=FACT(statut='o', max=1, fr = '', ang = 'Numerical parameters scheme for interstitials', + No=FACT(statut='o', max=1, fr = '', ang = 'Number of discrete equations for species i', + value=SIMP(statut= 'o',typ = 'I', defaut=30, max=1,val_min=0), + ), + Nc=FACT(statut='o', max=1, fr = '', ang = 'Number of continuous equations for species i', + value=SIMP(statut= 'o',typ = 'I', defaut=300, max=1,val_min=0), + ), + M=FACT(statut='o', max=1, fr = '', ang = 'Step value for species i', + value=SIMP(statut= 'o',typ = 'I', defaut=30, max=1,val_min=0), + ), + kmet=FACT(statut='o', max=1, fr = '', ang = 'Step value for species i', + value=SIMP(statut= 'o',typ = 'I', defaut=97, max=1,val_min=0), + ), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + ), + numerical_scheme_b=FACT(statut='o', max=1, fr = '', ang = 'Numerical parameters scheme for the solute element', + No=FACT(statut='o', max=1, fr = '', ang = 'Number of discrete equations for species b', + value=SIMP(statut= 'o',typ = 'I', defaut=0, max=1,val_min=0), + ), + Nc=FACT(statut='o', max=1, fr = '', ang = 'Number of continuous equations for species b', + value=SIMP(statut= 'o',typ = 'I', defaut=0, max=1,val_min=0), + ), + M=FACT(statut='o', max=1, fr = '', ang = 'Step value for species b', + value=SIMP(statut= 'o',typ = 'I', defaut=0, max=1,val_min=0), + ), + kmet=FACT(statut='o', max=1, fr = '', ang = 'Step value for species b', + value=SIMP(statut= 'o',typ = 'I', defaut=0, max=1,val_min=0), + ), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + ), + access=SIMP(statut= 'o',typ = 'TXM', defaut="user", max=1), + solver_absolute_error=FACT(statut='o', max=1, fr = '', ang = 'Absolute error for the rate theory solver', + value=SIMP(statut= 'o',typ = 'R', defaut=0.0001, max=1,val_min=0), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='None', max=1), + ), + solver_relative_error=FACT(statut='o', max=1, fr = '', ang = 'Relative error for the rate theory solver', + value=SIMP(statut= 'o',typ = 'R', defaut=0.001, max=1,val_min=0), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='None', max=1), + ), + short_doc=SIMP(statut= 'o',typ = 'TXM', defaut="Parametrisation of the rate theory code", max=1), + numerical_scheme_v=FACT(statut='o', max=1, fr = '', ang = 'Numerical parameters scheme for vacancies', + No=FACT(statut='o', max=1, fr = '', ang = 'Number of discrete equations for species v', + value=SIMP(statut= 'o',typ = 'I', defaut=30, max=1,val_min=0), + ), + Nc=FACT(statut='o', max=1, fr = '', ang = 'Number of continuous equations for species v', + value=SIMP(statut= 'o',typ = 'I', defaut=300, max=1,val_min=0), + ), + M=FACT(statut='o', max=1, fr = '', ang = 'Step value for species v', + value=SIMP(statut= 'o',typ = 'I', defaut=30, max=1,val_min=0), + ), + kmet=FACT(statut='o', max=1, fr = '', ang = 'Step value for species v', + value=SIMP(statut= 'o',typ = 'I', defaut=55, max=1,val_min=0), + ), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + ), + bound_self_defects=FACT(statut='o', max=1, fr = '', ang = 'Choose Yes if you want the to artifically impose self defects conservation by imposing a null flux for concentrations at $(No+Nc)$. Choose stop to stop the calculation in case of leakage.', + value=SIMP(statut= 'o',typ = 'TXM', defaut="Stop", max=1,into=['Yes', 'No', 'Stop']), + ), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + ) +neutron_spectrum=PROC(nom='neutron_spectrum',op=None, + spectrum=FACT(statut='o', max=1, fr = '', ang = 'Neutron spectrum table', + values=SIMP(statut= 'o',typ = Tuple(2), defaut=[[0.0465, 21000000000000.0], [0.10000000000000001, 24300000000000.0], [0.20000000000000001, 27300000000000.0], [0.40000000000000002, 37800000000000.0], [0.80000000000000004, 46600000000000.0], [1.0, 16400000000000.0], [1.3999999999999999, 25800000000000.0], [2.5, 41200000000000.0]], min=1, max='**'), + ), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + spectrum_time=SIMP(statut= 'o',typ = 'TXM', defaut="None", max=1), + access=SIMP(statut= 'o',typ = 'TXM', defaut="user", max=1), + short_doc=SIMP(statut= 'o',typ = 'TXM', defaut="Data object containing the neutron spectrum table.", max=1), + ) +material_content=PROC(nom='material_content',op=None, + valeur=FACT(statut='o', max=1, fr = '', ang = 'Chemical composition of the steel', + Cu=SIMP(statut= 'o',typ = 'R', defaut=0.0, max=1,val_min=0.0,val_max=0.1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='atomic percent', max=1), + ), + ) +experimental_resolutions=PROC(nom='experimental_resolutions',op=None, + short_doc=SIMP(statut= 'o',typ = 'TXM', defaut="A base class for the minimum radius of interstitial and vacancy clusters taken into account in number densities calculations.", max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + R_min_V=FACT(statut='o', max=1, fr = '', ang = 'Minimum radius of vacancy clusters taken into account in number densities calculations.', + value=SIMP(statut= 'o',typ = 'R', defaut=0.0, max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='nm', max=1), + ), + access=SIMP(statut= 'o',typ = 'TXM', defaut="user", max=1), + interstitial_cluster_shape=FACT(statut='o', max=1, fr = '', ang = 'Choice for the shape of interstitials clusters, disks or spheres. This only impacts the calculation of the radius of the cluster and associated radial density.', + value=SIMP(statut= 'o',typ = 'TXM', defaut="disk", max=1,into=['disk', 'sphere']), + ), + R_min_B=FACT(statut='o', max=1, fr = '', ang = 'Minimum radius of copper precipitates taken into account in number densities calculations. ', + value=SIMP(statut= 'o',typ = 'R', defaut=0.0, max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='nm', max=1), + ), + R_min_I=FACT(statut='o', max=1, fr = '', ang = 'Minimum radius of interstitial clusters taken into account in number densities calculations. ', + value=SIMP(statut= 'o',typ = 'R', defaut=0.0, max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='nm', max=1), + ), + ) +damage_energy_model=PROC(nom='damage_energy_model',op=None, + a=SIMP(statut= 'o',typ = 'R', defaut=1.11787605409e-09, max=1), + elect=SIMP(statut= 'o',typ = 'R', defaut=4.8e-10, max=1), + r_bohr=SIMP(statut= 'o',typ = 'R', defaut=5.29e-09, max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + z_p=SIMP(statut= 'o',typ = 'R', defaut=26.0, max=1), + z_t=SIMP(statut= 'o',typ = 'R', defaut=26.0, max=1), + access=SIMP(statut= 'o',typ = 'TXM', defaut="expert", max=1), + short_doc=SIMP(statut= 'o',typ = 'TXM', defaut="Lindhard damage energy model", max=1), + m_p=SIMP(statut= 'o',typ = 'R', defaut=55.0, max=1), + m_t=SIMP(statut= 'o',typ = 'R', defaut=55.0, max=1), + ) + diff --git a/MAP/creeCataFromDict.py b/MAP/creeCataFromDict.py new file mode 100755 index 00000000..37dc9727 --- /dev/null +++ b/MAP/creeCataFromDict.py @@ -0,0 +1,42 @@ +#!/usr/bin/env python +# -*- coding: utf-8 -*- +import types +class CataMAP: + + def __init__(self,dict1,dict2): + self.cata="" + self.texte=self.readfile("cataDebut.py") + self.dictParam=dict1 + self.dictData=dict2 + self.traiteDico(self.dictParam) + + + def readfile(self,fn): + try: + texte=open(fn).read() + except: + print "Impossible ouvrir fichier %s" % filename + return texte + + + def traiteDico(self,dict): + for clef in dict.keys() : + d=dict[clef] + texteSIMP="=SIMP(typ=%s,statut=%s)\n,"%d + texteSIMp=clef+texteSIMP + print texteSIMP + + def execute(self): + contexte = globals() + try : + exec self.texte in contexte + except : + import traceback + traceback.print_exc() + + +if __name__ == "__main__" : + dicoParam={"p1":{"typ":"TXM","statut":"o"}} + dicoVal={"val1":{"typ":"R","statut":"o"}} + monCata=CataMAP(dicoParam,dicoVal) + print monCata.texte diff --git a/MAP/prefs_MAP.py b/MAP/prefs_MAP.py index b667b55a..aea6917c 100644 --- a/MAP/prefs_MAP.py +++ b/MAP/prefs_MAP.py @@ -56,12 +56,16 @@ MAP_DIRECTORY=os.getenv("MAP_DIRECTORY") catalogues = ( # (code, identifiant, catalogue, formatOut, formatIN) - ('MAP','s_Perfect_V1',os.path.join(repIni,'s_Perfect_V1.py'),'s_Perfect'), + ('MAP','V1',os.path.join(repIni,'s_Perfect_V1.py'),'Perfect'), ('MAP','V0',os.path.join(repIni,'s_DIC_V1.py'),'s_DIC'), ('MAP','V1',os.path.join(repIni,'s_DIC_V1.py'),'s_DIC','defaut'), ('MAP','V1',os.path.join(repIni,'s_scc_3d_analysis_V1.py'),'s_scc_3d','defaut'), + ('MAP','V1',os.path.join(repIni,'Essai/maquette.py'),'maquette','defaut'), + ('MAP','V1',os.path.join(repIni,'Essai/comp_c_image_3d.py'),'c_image_3d','defaut'), + ('MAP','V1',os.path.join(repIni,'Essai/c_pre_interface_mesh.py.py'),'c_pre_interface_mesh','defaut'), + ('MAP','V1',os.path.join(repIni,'Essai/c_post_distribution_properties.py'),'c_post_distribution_properties','defaut'), ) OpenTURNS_path='/local/noyret/Salome/V6_main/tools/install/Openturns_tool-0150-py266-r272-ro144-rp208-sw204-xm278-la331-gr2263-dox173_patch-tbb30/lib/python2.6/site-packages' -sys.path[:0]=[INSTALLDIR, OpenTURNS_path] +sys.path[:0]=[repIni,INSTALLDIR, OpenTURNS_path] diff --git a/MAP/s_Perfect_V1.py b/MAP/s_Perfect_V1.py index 1d45aa4f..eaa6dcc3 100644 --- a/MAP/s_Perfect_V1.py +++ b/MAP/s_Perfect_V1.py @@ -7,6 +7,7 @@ from Accas import * import os import sys +import types from prefs_MAP import PATH_MAP @@ -34,197 +35,143 @@ JdC = JDC_CATA ( code = 'MAP', #regles=(AU_MOINS_UN('DISPL',),A_CLASSER('RBM','DISPL')) )# Fin JDC_CATA # -specter_path=PROC(nom="specter_path",op= None, - path = SIMP ( typ = 'TXM', defaut=PATH_MAP+"perfect_dev/tools/bin/specter", - statut='o', fr = "", ang = "specter_path ", max=1, - ), -) -residual_energy_model=PROC(nom="residual_energy_model",op= None, - beta = FACT (statut='o', max=1, - ang = "total number of surviving point defects for cascades in iron up", - name= SIMP(statut= "f",typ = 'TXM', ang = "",max=1), - value=SIMP(statut= "o",typ = 'R', defaut=0.779, max=1), - unit= SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - alpha = FACT (statut='o', max=1, - name= SIMP(statut= "f",typ = 'TXM', ang = "",max=1), - value=SIMP(statut= "o",typ = 'R', defaut=5.67, ang = "",max=1,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), -) -mfvisc2_path=PROC(nom="mfvisc2_path",op= None, - path = SIMP ( typ = 'TXM', defaut=PATH_MAP+"perfect_dev/tools/bin/mfvisc", - statut='o', fr = "", ang = "specter_path ", max=1, - ), -) -mfvisc2_parametrisation=PROC(nom="mfvisc2_parametrisation",op= None, - stop_if_solute_loss=SIMP (statut= "f",typ = 'TXM', - ang = "Yes if you want the rate-theory calculation to stop when a solute loss is detected", - defaut="No",into=("Yes","No") - ), - bound_solute=SIMP (statut= "f",typ = 'TXM', - ang = "Yes if you want the to artifically impose the solute conservation by imposing a null flux for concentrations at Nob", - defaut="Yes",into=("Yes","No") - ), - numerical_scheme_i = FACT (statut='o', max=1, - ang="Numerical parameters scheme for interstitial", - No=FACT(statut='o', max=1, - ang='Number of discrete equations for species i', - name=SIMP(statut= "f", typ = 'TXM', defaut='No_i', ang = "",max=1,), - value=SIMP(statut= "o",typ = 'I', defaut=30,into=(30,), ang = "",max=1,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - Nc=FACT(statut='o', max=1, - ang='Number of continous equations for species i', - name=SIMP(statut= "f", typ = 'TXM', defaut='Nc_i', ang = "",max=1,), - value=SIMP(statut= "o",typ = 'I', defaut=300, ang = "",max=1,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - M=FACT(statut='o', max=1, ang='Step value for species i', - name=SIMP(statut= "f", typ = 'TXM', defaut='M_i', max=1,), - value=SIMP(statut= "o",typ = 'I', defaut=50, max=1,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - kmet=FACT(statut='o', max=1, ang='Step value for species i', - name=SIMP(statut= "f", typ = 'TXM', defaut='kmet_i', max=1,), - value=SIMP(statut= "o",typ = 'I', defaut=97, max=1,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - species=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - numerical_scheme_b = FACT (statut='o', max=1, - ang="Numerical parameters scheme for the solute element", - No=FACT(statut='o', max=1, - ang='Number of discrete equations for species b', - name=SIMP(statut= "f", typ = 'TXM', defaut='No_b', ang = "",max=1,), - value=SIMP(statut= "o",typ = 'I', defaut=0, ang = "",max=1,val_min=0,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - Nc=FACT(statut='o', max=1, - ang='Number of continous equations for species b', - name=SIMP(statut= "f", typ = 'TXM', defaut='Nc_b', ang = "",max=1,), - value=SIMP(statut= "o",typ = 'I', defaut=0, ang = "",max=1,val_min=0,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - M=FACT(statut='o', max=1, ang='Step value for species b', - name=SIMP(statut= "f", typ = 'TXM', defaut='M_b', max=1,), - value=SIMP(statut= "o",typ = 'I', defaut=0, max=1,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - kmet=FACT(statut='o', max=1, ang='Step value for species b', - name=SIMP(statut= "f", typ = 'TXM', defaut='kmet_b', max=1,), - value=SIMP(statut= "o",typ = 'I', defaut=0, max=1,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - species=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - numerical_scheme_v = FACT (statut='o', max=1, - ang="Numerical parameters scheme for vacancies", - No=FACT(statut='o', max=1, - ang='Number of discrete equations for species v', - name=SIMP(statut= "f", typ = 'TXM', defaut='No_v', ang = "",max=1,), - value=SIMP(statut= "o",typ = 'I', defaut=30, ang = "",max=1,val_min=0,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - Nc=FACT(statut='o', max=1, - ang='Number of continous equations for species v', - name=SIMP(statut= "f", typ = 'TXM', defaut='Nc_v', ang = "",max=1,), - value=SIMP(statut= "o",typ = 'I', defaut=300, ang = "",max=1,val_min=0,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - M=FACT(statut='o', max=1, ang='Step value for species v', - name=SIMP(statut= "f", typ = 'TXM', defaut='M_v', max=1,), - value=SIMP(statut= "o",typ = 'I', defaut=30, max=1,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - kmet=FACT(statut='o', max=1, ang='Step value for species v', - name=SIMP(statut= "f", typ = 'TXM', defaut='kmet_v', max=1,), - value=SIMP(statut= "o",typ = 'I', defaut=55, max=1,), - unit=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - species=SIMP (statut= "f",typ = 'TXM', ang = "",max=1), - ), - ignore_Helium = SIMP (statut= "f",typ = 'TXM', ang = "",max=1, - defaut="Yes",into=("Yes","No"),), - bound_self_defects = SIMP (statut= "f",typ = 'TXM', max=1, - ang="Yes if you want the to artifically impose self defects conservation by imposing a null flux for concentrations at $(No+Nc)$. Choose 'stop' to stop the calculation in case of leakage.", - defaut="Stop",into=("Yes","No","Stop"),) -) - -operating_conditions=PROC(nom="operating_conditions",op= None, - - relative_time_increments=SIMP (statut= "o",typ = 'R', min=3, max='**', - ang="Relative time increments for the LONG_TERM computation", - defaut=(1e-10, 1.0000000000000001e-09, 3e-09, 1e-08, 2.9999999999999997e-08, 9.9999999999999995e-08, 2.9999999999999999e-07, 9.9999999999999995e-07, 3.0000000000000001e-06, 1.0000000000000001e-05, 3.0000000000000001e-05, 0.0001, 0.00029999999999999997, 0.001, 0.0030000000000000001, 0.01, 0.029999999999999999, 0.10000000000000001, 0.29999999999999999, 1.0), - ), - rescaling_NRT_damage_rate=FACT(statut='o', max=1, - ang="rescaling NRT damage rate (dpa/s)", - value=SIMP(statut= "o",typ = 'R', defaut=0.0, val_min=0,), - unit=SIMP (statut= "f",typ = 'TXM', defaut='dpa_per_s',into=('dpa_per_s',)), +specter_path=PROC(nom='specter_path',op=None, + path=SIMP(typ='Fichier',defaut='/home/A28637/SVN_MAP/trunk/vendor/PERFORM_20110225/perfect_dev/tools/bin/specter', statut='o', fr = '', ang = 'A class for the definition of a file', max=1,), + ) + + +residual_energy_model=PROC(nom='residual_energy_model',op=None, + access=SIMP(statut= 'o',typ = 'TXM', defaut="user", max=1), + beta=FACT(statut='o', max=1, fr = '', ang = 'A class for the definition of a numerical value', + value=SIMP(statut= 'o',typ = 'R', defaut=0.779, max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='None', max=1), + ), + short_doc=SIMP(statut= 'o',typ = 'TXM', defaut="The model which gives the total number of surviving point defects for cascades in iron up to 10 keV. ", max=1), + alpha=FACT(statut='o', max=1, fr = '', ang = 'A class for the definition of a numerical value', + value=SIMP(statut= 'o',typ = 'R', defaut=5.67, max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='None', max=1), + ), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + ) +mfvisc2_path=PROC(nom='mfvisc2_path',op=None, + path=SIMP(typ='Fichier',defaut='/home/A28637/SVN_MAP/trunk/vendor/PERFORM_20110225/perfect_dev/tools/bin/mfvisc', statut='o', fr = '', ang = 'A class for the definition of a file', max=1,), + ) + + +mfvisc2_parametrisation=PROC(nom='mfvisc2_parametrisation',op=None, + stop_if_solute_loss=FACT(statut='o', max=1, fr = '', ang = 'Choose Yes if you want the rate-theory calculation to stop when a solute loss (i.e. Cu or He in the case of RPV and INTERN respectively) is detected. Choose No otherwise.', + value=SIMP(statut= 'o',typ = 'TXM', defaut="No", max=1,into=['Yes', 'No']), + ), + bound_solute=FACT(statut='o', max=1, fr = '', ang = 'Choose Yes if you want the to artifically impose the solute conservation by imposing a null flux for concentrations at Nob.', + value=SIMP(statut= 'o',typ = 'TXM', defaut="Yes", max=1,into=['Yes', 'No']), + ), + numerical_scheme_i=FACT(statut='o', max=1, fr = '', ang = 'Numerical parameters scheme for interstitials', + No=FACT(statut='o', max=1, fr = '', ang = 'Number of discrete equations for species i', + value=SIMP(statut= 'o',typ = 'I', defaut=30, max=1,val_min=0), + ), + Nc=FACT(statut='o', max=1, fr = '', ang = 'Number of continuous equations for species i', + value=SIMP(statut= 'o',typ = 'I', defaut=300, max=1,val_min=0), + ), + M=FACT(statut='o', max=1, fr = '', ang = 'Step value for species i', + value=SIMP(statut= 'o',typ = 'I', defaut=30, max=1,val_min=0), + ), + kmet=FACT(statut='o', max=1, fr = '', ang = 'Step value for species i', + value=SIMP(statut= 'o',typ = 'I', defaut=97, max=1,val_min=0), + ), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + ), + numerical_scheme_b=FACT(statut='o', max=1, fr = '', ang = 'Numerical parameters scheme for the solute element', + No=FACT(statut='o', max=1, fr = '', ang = 'Number of discrete equations for species b', + value=SIMP(statut= 'o',typ = 'I', defaut=0, max=1,val_min=0), + ), + Nc=FACT(statut='o', max=1, fr = '', ang = 'Number of continuous equations for species b', + value=SIMP(statut= 'o',typ = 'I', defaut=0, max=1,val_min=0), + ), + M=FACT(statut='o', max=1, fr = '', ang = 'Step value for species b', + value=SIMP(statut= 'o',typ = 'I', defaut=0, max=1,val_min=0), + ), + kmet=FACT(statut='o', max=1, fr = '', ang = 'Step value for species b', + value=SIMP(statut= 'o',typ = 'I', defaut=0, max=1,val_min=0), + ), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + ), + access=SIMP(statut= 'o',typ = 'TXM', defaut="user", max=1), + solver_absolute_error=FACT(statut='o', max=1, fr = '', ang = 'Absolute error for the rate theory solver', + value=SIMP(statut= 'o',typ = 'R', defaut=0.0001, max=1,val_min=0), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='None', max=1), + ), + solver_relative_error=FACT(statut='o', max=1, fr = '', ang = 'Relative error for the rate theory solver', + value=SIMP(statut= 'o',typ = 'R', defaut=0.001, max=1,val_min=0), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='None', max=1), + ), + short_doc=SIMP(statut= 'o',typ = 'TXM', defaut="Parametrisation of the rate theory code", max=1), + numerical_scheme_v=FACT(statut='o', max=1, fr = '', ang = 'Numerical parameters scheme for vacancies', + No=FACT(statut='o', max=1, fr = '', ang = 'Number of discrete equations for species v', + value=SIMP(statut= 'o',typ = 'I', defaut=30, max=1,val_min=0), + ), + Nc=FACT(statut='o', max=1, fr = '', ang = 'Number of continuous equations for species v', + value=SIMP(statut= 'o',typ = 'I', defaut=300, max=1,val_min=0), + ), + M=FACT(statut='o', max=1, fr = '', ang = 'Step value for species v', + value=SIMP(statut= 'o',typ = 'I', defaut=30, max=1,val_min=0), + ), + kmet=FACT(statut='o', max=1, fr = '', ang = 'Step value for species v', + value=SIMP(statut= 'o',typ = 'I', defaut=55, max=1,val_min=0), + ), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + ), + bound_self_defects=FACT(statut='o', max=1, fr = '', ang = 'Choose Yes if you want the to artifically impose self defects conservation by imposing a null flux for concentrations at $(No+Nc)$. Choose stop to stop the calculation in case of leakage.', + value=SIMP(statut= 'o',typ = 'TXM', defaut="Stop", max=1,into=['Yes', 'No', 'Stop']), + ), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + ) +neutron_spectrum=PROC(nom='neutron_spectrum',op=None, + spectrum=FACT(statut='o', max=1, fr = '', ang = 'Neutron spectrum table', + values=SIMP(statut= 'o',typ = Tuple(2), defaut=[[0.0465, 21000000000000.0], [0.10000000000000001, 24300000000000.0], [0.20000000000000001, 27300000000000.0], [0.40000000000000002, 37800000000000.0], [0.80000000000000004, 46600000000000.0], [1.0, 16400000000000.0], [1.3999999999999999, 25800000000000.0], [2.5, 41200000000000.0]], min=1, max='**'), + ), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + spectrum_time=SIMP(statut= 'o',typ = 'TXM', defaut="None", max=1), + access=SIMP(statut= 'o',typ = 'TXM', defaut="user", max=1), + short_doc=SIMP(statut= 'o',typ = 'TXM', defaut="Data object containing the neutron spectrum table.", max=1), + ) +material_content=PROC(nom='material_content',op=None, + valeur=FACT(statut='o', max=1, fr = '', ang = 'Chemical composition of the steel', + Cu=SIMP(statut= 'o',typ = 'R', defaut=0.0, max=1,val_min=0.0,val_max=0.1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='atomic percent', max=1), ), - flux_cut_off_energy=FACT(statut='o', max=1, - ang="Energy threshold for the calculation of the flux", - value=SIMP(statut= "o",typ = 'R', defaut=1.0, val_min=0,), - unit=SIMP (statut= "f",typ = 'TXM', defaut='MeV',into=('MeV',)), - ), - toughness_calculation_time_index = SIMP (statut= "o",typ = 'R', defaut=-1,into=(-1,),), - temp_irrad=FACT(statut='o', max=1, - ang="Energy threshold for the calculation of the flux", - name=SIMP(statut= "f", typ = 'TXM', defaut='T', max=1,), - value=SIMP(statut= "o",typ = 'R', defaut=573.0, val_min=0,), - unit=SIMP (statut= "f",typ = 'TXM', defaut='K',into=('K',)), - ), - time_irrad=FACT(statut='o', max=1, - unit=SIMP(statut= "f", typ = 'TXM', defaut='s', max=1,), - value=SIMP(statut= "o",typ = 'R', defaut=100000.0, val_min=0,), - ), - rescaling_flux=FACT(statut='o', max=1, - unit=SIMP(statut= "f", typ = 'TXM', defaut='n_per_cm2_per_s', max=1,), - value=SIMP(statut= "o",typ = 'R', defaut=0.0, val_min=0,), - ), -) - -bcc_crystal=PROC(nom="bcc_crystal",op= None, - lattice_parameter=FACT(statut='o', max=1, - unit=SIMP(statut= "f", typ = 'TXM', defaut='angstrom', max=1,), - value=SIMP(statut= "o",typ = 'R', defaut=2.87, ), - ), - atomic_volume=FACT(statut='o', max=1, - unit=SIMP(statut= "f", typ = 'TXM', defaut='m3', max=1,), - value=SIMP(statut= "o",typ = 'R', defaut=1.18199515e-29, ), - ), - structure=SIMP (statut= "f",typ = 'TXM', defaut='bcc',into=('bcc','fcc'), - ang='Crystalline structure of the considered alloy'), - atomic_density=FACT(statut='o', max=1, - unit=SIMP(statut= "f", typ = 'TXM', defaut='at_per_m3', max=1,), - value=SIMP(statut= "o",typ = 'R', defaut=8.46027160095e+28, ), - ), -) - -neutron_spectrum=PROC(nom="neutron_spectrum",op= None, - spectrum=SIMP(statut= "o",typ = 'R',max='**', defaut=(0.0465, 21000000000000.0, 0.10000000000000001, 24300000000000.0, 0.20000000000000001, 27300000000000.0, 0.40000000000000002, 37800000000000.0, 0.80000000000000004, 46600000000000.0, 1.0, 16400000000000.0, 1.3999999999999999, 25800000000000.0, 2.5, 41200000000000.0)), - - spectrum_description=SIMP(statut= "f", typ = 'TXM', max=1,), -) - -diffusion_model=PROC(nom="diffusion_model",op=None, - mv=FACT(statut='o', max=1, - value=SIMP(statut= "o",typ = 'R', defaut=5., ), - unit=SIMP(statut= "f", typ = 'TXM', defaut='atomic percent', max=1,), -) -) - - - - - - - - - - - - + ) +experimental_resolutions=PROC(nom='experimental_resolutions',op=None, + short_doc=SIMP(statut= 'o',typ = 'TXM', defaut="A base class for the minimum radius of interstitial and vacancy clusters taken into account in number densities calculations.", max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + R_min_V=FACT(statut='o', max=1, fr = '', ang = 'Minimum radius of vacancy clusters taken into account in number densities calculations.', + value=SIMP(statut= 'o',typ = 'R', defaut=0.0, max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='nm', max=1), + ), + access=SIMP(statut= 'o',typ = 'TXM', defaut="user", max=1), + interstitial_cluster_shape=FACT(statut='o', max=1, fr = '', ang = 'Choice for the shape of interstitials clusters, disks or spheres. This only impacts the calculation of the radius of the cluster and associated radial density.', + value=SIMP(statut= 'o',typ = 'TXM', defaut="disk", max=1,into=['disk', 'sphere']), + ), + R_min_B=FACT(statut='o', max=1, fr = '', ang = 'Minimum radius of copper precipitates taken into account in number densities calculations. ', + value=SIMP(statut= 'o',typ = 'R', defaut=0.0, max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='nm', max=1), + ), + R_min_I=FACT(statut='o', max=1, fr = '', ang = 'Minimum radius of interstitial clusters taken into account in number densities calculations. ', + value=SIMP(statut= 'o',typ = 'R', defaut=0.0, max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut='nm', max=1), + ), + ) +damage_energy_model=PROC(nom='damage_energy_model',op=None, + a=SIMP(statut= 'o',typ = 'R', defaut=1.11787605409e-09, max=1), + elect=SIMP(statut= 'o',typ = 'R', defaut=4.8e-10, max=1), + r_bohr=SIMP(statut= 'o',typ = 'R', defaut=5.29e-09, max=1), + unit=SIMP(statut= 'o',typ = 'TXM', defaut="", max=1), + z_p=SIMP(statut= 'o',typ = 'R', defaut=26.0, max=1), + z_t=SIMP(statut= 'o',typ = 'R', defaut=26.0, max=1), + access=SIMP(statut= 'o',typ = 'TXM', defaut="expert", max=1), + short_doc=SIMP(statut= 'o',typ = 'TXM', defaut="Lindhard damage energy model", max=1), + m_p=SIMP(statut= 'o',typ = 'R', defaut=55.0, max=1), + m_t=SIMP(statut= 'o',typ = 'R', defaut=55.0, max=1), + )