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Python DataIO.findZero方法代码示例

本文整理汇总了Python中cc.tools.io.DataIO.findZero方法的典型用法代码示例。如果您正苦于以下问题:Python DataIO.findZero方法的具体用法?Python DataIO.findZero怎么用?Python DataIO.findZero使用的例子?那么恭喜您, 这里精选的方法代码示例或许可以为您提供帮助。您也可以进一步了解该方法所在cc.tools.io.DataIO的用法示例。


在下文中一共展示了DataIO.findZero方法的2个代码示例,这些例子默认根据受欢迎程度排序。您可以为喜欢或者感觉有用的代码点赞,您的评价将有助于系统推荐出更棒的Python代码示例。

示例1: read

# 需要导入模块: from cc.tools.io import DataIO [as 别名]
# 或者: from cc.tools.io.DataIO import findZero [as 别名]
 def read(self): 
 
     '''
     Read the collision rates file. Assumes GASTRoNOoM format.
     
     To read ALI/MCP collision rates (which are in the Lamda format), make
     use of the LamdaReader, which redefines this method. The other retrieval
     methods remain valid.        
     
     Each transition is stored as an index, and gives upper and lower level
     index as well as the collision rate.
     
     '''
     
     #-- Read the collis file which is just one long column. Assumes there is
     #   at least one zero value for padding! 
     collis = np.loadtxt(self.fn)
     self['pars'] = dict()
     
     #-- The number of transitions is given by the number of non-zero values
     #   in the beginning of the file. 
     ntrans = DataIO.findZero(0,collis)
     n0 = DataIO.findNumber(ntrans,collis)-ntrans
     
     #-- The number of temperatures in the file can be calculated now
     ntemp = (len(collis)-2*(ntrans+n0))/(ntrans+n0+1)
     
     #-- Prep the coll_trans array and add indices for coll_trans
     dtype = [('index',int),('lup',int),('llow',int),('rates',np.ndarray)]
     self['coll_trans'] = np.empty(shape=(ntrans,),dtype=dtype)
     self['coll_trans']['index'] = range(1,ntrans+1)
     
     #-- Add the level indices
     self['coll_trans']['lup'] = collis[:ntrans]
     self['coll_trans']['llow'] = collis[ntrans+n0:2*ntrans+n0]
     
     #-- Retrieve the temperatures. 
     start_i = 2*(ntrans+n0)
     Tgrid = [collis[start_i+i*(ntrans + n0 + 1)] for i in range(ntemp)]
     
     #-- Check if any of them is zero, and 
     #   readjust ntemp (sometimes a 0 temp with 0 rates is present in file)
     Tgrid_real = [Ti for Ti in Tgrid if Ti != 0.]
     ntemp_real = len(Tgrid_real)
     
     #-- Retrieve rates and insert into array. Loop for ntemp, and ignore
     #   rates if T is 0 there.
     rates = np.empty(shape=(ntrans,ntemp_real))
     start_i = start_i + 1
     for i,Ti in enumerate(Tgrid):
         if Ti == 0.0: continue
         this_i = start_i+i*(ntrans + n0 + 1)
         rates[:,i] = collis[this_i:this_i+ntrans]
     
     #-- Save into coll_trans array
     for i in range(ntrans):
         self['coll_trans']['rates'][i] = rates[i,:]
         
     #-- Save additional information
     self['pars']['ncoll_trans'] = ntrans
     self['pars']['ncoll_temp'] = ntemp_real
     self['coll_temp'] = np.array(Tgrid_real)
开发者ID:IvS-KULeuven,项目名称:ComboCode,代码行数:64,代码来源:CollisReader.py

示例2: read

# 需要导入模块: from cc.tools.io import DataIO [as 别名]
# 或者: from cc.tools.io.DataIO import findZero [as 别名]
 def read(self):
      
     '''
     Read the MOLECULE_radiat file and set a dictionary for the instance
     with all the information. 
     
     Done on creation of an instance of the class.
     
     '''
     
     #-- Read the radiat file which is just one long column
     radiat = np.loadtxt(self.fn)
     
     #-- If nline wasn't given, find out now. 
     if self.nline is None:
         nline = DataIO.findZero(0,radiat)
         
         #-- Check if this is a good nline. If not, there's likely no zeroes
         #   (and the above function found the 0-energy level or an ny-0). 
         if len(radiat) < 4*nline+2*self.ny:
             #-- But there might still be zeroes for ny: this is always the 
             #   first non-zero energy level
             ienergy = DataIO.findNumber(nline,radiat)
             
             #-- Find the ny-zeroes, but this might be end of file: no zeroes
             n0_nyi = DataIO.findZero(ienergy,radiat)
             if n0_nyi == len(radiat):
                 n0_ny = 0
             
             #-- Otherwise, continue. We do have ny-zeroes
             else:   
                 n0_nyj = DataIO.findNumber(n0_nyi,radiat)
                 n0_ny = n0_nyj-n0_nyi
             self.nline = (len(radiat)-2*(self.ny+n0_ny))/4
         else:
             self.nline = nline
         self['pars']['nline'] = self.nline
         
     #-- Prep the transition array
     dtype = [('index',int),('lup',int),('llow',int),('frequency',float),\
              ('einsteinA',float)]
     self['trans'] = np.empty(shape=(self.nline,),dtype=dtype)
     self['trans']['index'] = range(1,self.nline+1)
     
     #-- Prep the level array
     dtype = [('index',int),('weight',float),('energy',float)]
     self['level'] = np.empty(shape=(self.ny,),dtype=dtype)
     self['level']['index'] = range(1,self.ny+1)
     
     #-- The number of values per property is either nline or ny
     nvals = [self.nline,self.nline,self.ny,self.ny,self.nline,self.nline]
     
     #-- Numbers are padded with zeroes at end. The amount of padding is 
     #   unknown. if total length is equal to sum of all step sizes, reading 
     #   radiat is very simple.
     if sum(nvals) == len(radiat):
         n0_nline = 0
         n0_ny = 0
         
     #-- Otherwise a more elaborate method must be used to determine the 
     #   amount of zero-padding that is used for each nline and ny.
     else:
         #-- Einstein A is never 0, so this is easy.
         n0_nline = DataIO.findNumber(self.nline,radiat)-self.nline
         
         #-- Two nline-sized blocks, one ny-sized block. Because the first
         #   energy level might be 0 cm^-1, this is not the real n0_ny
         start_i = 2*(self.nline+n0_nline)+self.ny
         n0_ny1 = DataIO.findNumber(start_i,radiat)-start_i
         
         #-- Second ny-sized block gives the real n0_ny, since llow can never
         #   be zero:
         start_i = DataIO.findZero(start_i+n0_ny1,radiat)
         n0_ny = DataIO.findNumber(start_i,radiat)-start_i
         
     #-- Collect property names, types and number of zero-padding
     props = ['einsteinA','frequency','weight','energy','llow','lup']
     ptypes = ['trans','trans','level','level','trans','trans']
     n0s = [n0_nline,n0_nline,n0_ny,n0_ny,n0_nline,n0_nline]
     
     #-- Save the data into the arrays
     for i,(nval,ptype,prop) in enumerate(zip(nvals,ptypes,props)):
         #-- Determine starting index for this block
         start_i = sum(nvals[:i])+sum(n0s[:i])
         
         #-- Retrieve information
         self[ptype][prop] = radiat[start_i:start_i+nval]
开发者ID:IvS-KULeuven,项目名称:ComboCode,代码行数:89,代码来源:RadiatReader.py


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