def eval(self,**kwargs):
""" evaluate the link
Parameters
----------
applywav :boolean
Apply waveform to H
force : list
Force the computation (['sig','ray','Ct','H']) AND save (replace previous computations)
alg : 1|'old'|'exp'|'exp2'
version of run for signature
si_progress: bollean ( False)
display progression bar for signatures
diffraction : boolean (False)
takes into consideration diffraction points
ra_number_mirror_cf : int
rays.to3D number of ceil/floor reflexions
ra_ceil_H: float, (default [])
ceil height .
If [] : Layout max ceil height
If 0 : only floor reflection (outdoor case)
If -1 : neither ceil nor floor reflection (2D case)
ra_vectorized: boolean (True)
if True used the (2015 new) vectorized approach to determine 2drays
Returns
-------
ak : ndarray
alpha_k
tk : ndarray
tau_k
Notes
-----
update self.ak and self.tk
self.ak : ndarray
alpha_k
self.tk : ndarray
tau_k
Examples
--------
.. plot::
:include-source:
>>> from pylayers.simul.link import *
>>> L=DLink(verbose=False)
>>> aktk = L.eval()
See Also
--------
pylayers.antprop.signature
pylayers.antprop.rays
Experimental
------------
alg = 2015 | 20152 (best)
vectorized signature research
si_reverb : number of reverb in source/target cycle if alg=2015
"""
defaults={ 'applywav':True,
'si_progress':False,
'diffraction':True,
'ra_vectorized':True,
'ra_ceil_H':[],
'ra_number_mirror_cf':1,
'force':[],
'alg':1,
'si_reverb':4,
'threshold':0.1,
'verbose':[],
}
for key, value in defaults.items():
if key not in kwargs:
kwargs[key]=value
if 'cutoff' not in kwargs:
kwargs['cutoff']=self.cutoff
else:
self.cutoff=kwargs['cutoff']
if 'force' in kwargs:
if not isinstance(kwargs['force'],list):
if kwargs['force'] == True :
kwargs['force'] = ['sig','ray','Ct','H']
else :
kwargs['force'] = []
if kwargs['verbose'] != []:
self.verbose=kwargs['verbose']
# must be placed after all the init !!!!
if self.verbose :
print "checkh5"
self.checkh5()
############
# Signatures
############
if self.verbose :
print "Start Signatures"
tic = time.time()
Si = Signatures(self.L,self.ca,self.cb,cutoff=kwargs['cutoff'])
if (self.dexist['sig']['exist'] and not ('sig' in kwargs['force'])):
self.load(Si,self.dexist['sig']['grpname'])
if self.verbose :
print "load signature"
else :
if kwargs['alg']==1:
Si.run(cutoff=kwargs['cutoff'],
diffraction=kwargs['diffraction'],
threshold=kwargs['threshold'],
progress=kwargs['si_progress'])
if self.verbose :
print "default algorithm"
if kwargs['alg']=='exp':
TMP=Si.run_exp(cutoff=kwargs['cutoff'],
cutoffbound=kwargs['si_reverb'])
if self.verbose :
print "experimental (ex 2015)"
if kwargs['alg']=='exp2':
TMP=Si.run_exp2(cutoff=kwargs['cutoff'],
cutoffbound=kwargs['si_reverb'])
if self.verbose :
print "algo exp2 ( ex 20152)"
#Si.run6(diffraction=kwargs['diffraction'])
# save sig
self.save(Si,'sig',self.dexist['sig']['grpname'],force = kwargs['force'])
self.Si = Si
toc = time.time()
if self.verbose :
print "Stop signature",toc-tic
############
# Rays
############
if self.verbose :
print "Start Rays"
tic = time.time()
R = Rays(self.a,self.b)
if self.dexist['ray']['exist'] and not ('ray' in kwargs['force']):
self.load(R,self.dexist['ray']['grpname'])
else :
# perform computation ...
# ... with vetorized ray evaluation approach
if kwargs['ra_vectorized']:
r2d = Si.raysv(self.a,self.b)
# ... or with original and slow approach ( to be removed in a near future)
else :
r2d = Si.rays(self.a,self.b)
if kwargs['ra_ceil_H'] == []:
ceilheight = self.L.maxheight
else:
ceilheight = kwargs['ra_ceil_H']
R = r2d.to3D(self.L,H=ceilheight, N=kwargs['ra_number_mirror_cf'])
R.locbas(self.L)
# ...and save
R.fillinter(self.L)
C = Ctilde()
C = R.eval(self.fGHz)
self.save(R,'ray',self.dexist['ray']['grpname'],force = kwargs['force'])
self.R = R
toc = time.time()
if self.verbose :
print "Stop rays",toc-tic
if self.R.nray == 0:
raise NameError('No rays have been found. Try to re-run the simulation with a higher S.cutoff ')
############
# Ctilde
############
if self.dexist['Ct']['exist'] and not ('Ct' in kwargs['force']):
C=Ctilde()
self.load(C,self.dexist['Ct']['grpname'])
else :
#if not hasattr(R,'I'):
# Ctilde...
# Find an other criteria in order to decide whether the R has
# already been evaluated
#pdb.set_trace()
C = R.eval(self.fGHz)
# ...save Ct
self.save(C,'Ct',self.dexist['Ct']['grpname'],force = kwargs['force'])
self.C = C
############
# H
############
H = Tchannel()
if self.dexist['H']['exist'] and not ('H' in kwargs['force']):
self.load(H,self.dexist['H']['grpname'])
else :
# Ctilde antenna
Cl=C.locbas(Tt=self.Ta, Tr=self.Tb)
#T channel
H = C.prop2tran(a=self.Aa,b=self.Ab,Friis=True,debug=True)
self.save(H,'H',self.dexist['H']['grpname'],force = kwargs['force'])
self.H = H
if kwargs['applywav']:
if self.H.isFriis:
self.ir = self.H.get_cir(self.wav.sf)
else:
self.ir = self.H.get_cir(self.wav.sfg)
return self.H.ak, self.H.tk
def eval(self,**kwargs):
""" Evaluate the link
Parameters
----------
applywav :boolean
Apply waveform to H
force : list
Force the computation (['sig','ray','Ct','H']) AND save (replace previous computations)
si_algo : str ('old'|'new')
signature.run algo type
'old' : call propaths2
'new' : call procone2
alg : 5 | 7
version of run for signature
si_mt: boolean
Multi thread version of algo version 7
si_progress: bollean ( False)
display progression bar for signatures
diffraction : boolean (False)
takes into consideration diffraction points
ra_number_mirror_cf : int
rays.to3D number of ceil/floor reflexions
ra_ceil_height_meter: float,
ceil height
ra_vectorized: boolean (True)
if True used the (2015 new) vectorized approach to determine 2drays
Returns
-------
ak : ndarray
alpha_k
tk : ndarray
tau_k
Notes
-----
update self.ak and self.tk
self.ak : ndarray
alpha_k
self.tk : ndarray
tau_k
Examples
--------
.. plot::
:include-source:
>>> from pylayers.simul.link import *
>>> L=DLink(verbose=False)
>>> aktk = L.eval()
See Also
--------
pylayers.antprop.signature
pylayers.antprop.rays
Experimental
------------
alg = 2015 | 20152 (best)
vectorized signature research
si_reverb : number of reverb in source/target cycle if alg=2015
"""
defaults={ 'applywav':True,
'si_algo':'old',
'si_mt':False,
'si_progress':False,
'diffraction':False,
'ra_vectorized':False,
'ra_ceil_height_meter':3,
'ra_number_mirror_cf':1,
'force':[],
'alg':7,
'si_reverb':4,
'threshold':0.1,
}
for key, value in defaults.items():
if key not in kwargs:
kwargs[key]=value
if 'cutoff' not in kwargs:
kwargs['cutoff']=self.cutoff
else:
self.cutoff=kwargs['cutoff']
if 'force' in kwargs:
if not isinstance(kwargs['force'],list):
if kwargs['force'] == True :
kwargs['force'] = ['sig','ray','Ct','H']
else :
kwargs['force'] = []
# must be placed after all the init !!!!
self.checkh5()
############
# Signatures
############
Si = Signatures(self.L,self.ca,self.cb,cutoff=kwargs['cutoff'])
if (self.dexist['sig']['exist'] and not ('sig' in kwargs['force'])):
self.load(Si,self.dexist['sig']['grpname'])
else :
if kwargs['alg']==2015:
TMP=Si.run2015(cutoff=kwargs['cutoff'],
cutoffbound=kwargs['si_reverb'])
if kwargs['alg']==20152:
TMP=Si.run2015_2(cutoff=kwargs['cutoff'],
cutoffbound=kwargs['si_reverb'])
if kwargs['alg']==5:
Si.run5(cutoff=kwargs['cutoff'],
algo=kwargs['si_algo'],
diffraction=kwargs['diffraction'],
progress=kwargs['si_progress'])
if kwargs['alg']==7:
if kwargs['si_mt']==7:
Si.run7mt(cutoff=kwargs['cutoff'],
algo=kwargs['si_algo'],
diffraction=kwargs['diffraction'],
threshold=kwargs['threshold'],
progress=kwargs['si_progress'])
else :
Si.run7(cutoff=kwargs['cutoff'],
algo=kwargs['si_algo'],
diffraction=kwargs['diffraction'],
threshold=kwargs['threshold'],
progress=kwargs['si_progress'])
#Si.run6(diffraction=kwargs['diffraction'])
# save sig
self.save(Si,'sig',self.dexist['sig']['grpname'],force = kwargs['force'])
self.Si = Si
############
# Rays
############
R = Rays(self.a,self.b)
if self.dexist['ray']['exist'] and not ('ray' in kwargs['force']):
self.load(R,self.dexist['ray']['grpname'])
else :
# perform computation ...
# ... with vetorized ray evaluation approach
if kwargs['ra_vectorized']:
r2d = Si.raysv(self.a,self.b)
# ... or with original and slow approach ( to be removed in a near future)
else :
r2d = Si.rays(self.a,self.b)
R = r2d.to3D(self.L,H=self.L.maxheight, N=kwargs['ra_number_mirror_cf'])
R.locbas(self.L)
# ...and save
self.save(R,'ray',self.dexist['ray']['grpname'],force = kwargs['force'])
self.R = R
if self.R.nray == 0:
raise NameError('No rays have been found. Try to re-run the simulation with a higher S.cutoff ')
############
# Ctilde
############
C=Ctilde()
if self.dexist['Ct']['exist'] and not ('Ct' in kwargs['force']):
self.load(C,self.dexist['Ct']['grpname'])
else :
R.fillinter(self.L)
# Ctilde...
C = R.eval(self.fGHz)
# ...save Ct
self.save(C,'Ct',self.dexist['Ct']['grpname'],force = kwargs['force'])
self.C = C
############
# H
############
H = Tchannel()
if self.dexist['H']['exist'] and not ('H' in kwargs['force']):
self.load(H,self.dexist['H']['grpname'])
else :
# Ctilde antenna
Cl=C.locbas(Tt=self.Ta, Tr=self.Tb)
#T channel
H = C.prop2tran(a=self.Aa,b=self.Ab,Friis=True,debug=True)
self.save(H,'H',self.dexist['H']['grpname'],force = kwargs['force'])
self.H = H
if kwargs['applywav']:
if self.H.isFriis:
self.ir = self.H.applywavB(self.wav.sf)
else:
self.ir = self.H.applywavB(self.wav.sfg)
return self.H.ak, self.H.tk
def __init__(self, **kwargs):
""" deterministic link evaluation
Parameters
----------
L : Layout
Layout to be used
a : np.ndarray (3,)
position of a device dev_a
b : np.ndarray (3,)
position of a device dev_b
Aa : Antenna
Antenna of device dev_a
Ab : Antenna
Antenna of device dev_b
Ta : np.ndarray (3,3)
Rotation matrice of Antenna of device dev_a relative to global Layout scene
Tb : np.ndarray (3,3)
Rotation matrice of Antenna of device dev_b relative to global Layout scene
fGHz : np.ndarray (Nf,)
frequency range of Nf points used for evaluation of channel
wav : Waveform
Waveform to be applied on the channel
save_idx : int
number to identify the h5 file generated
Advanced (change only if you really know what you do !)
save_opt : list (['sig','ray','Ct','H'])
information to be saved in the Links h5 file. Should never be Modified !
force_create : Boolean (False)
forcecreating the h5py file (if already exist, will be erased)
Notes
-----
All simulations are stored into a unique file in your <PyProject>/output directory
using the following convention:
Links_<save_idx>_<LayoutFilename>.h5
where
<save_idx> is an integer number to distinguish different links simulations
and <LayoutFilename> is the Layout used for the link simulation.
Dataset organisation:
Links_<idx>_<Layout_name>.h5
|
|/sig/si_ID#0/
| /si_ID#1/
| ...
|
|/ray/ray_ID#0/
| /ray_ID#1/
| ...
|
|/Ct/Ct_ID#0/
| /Ct_ID#1/
| ...
|
|/H/H_ID#0/
| /H_ID#1/
| ...
|
|
|p_map
|c_map
|f_map
|A_map
|T_map
Roots Dataset :
c_map : Cycles (Nc x 3)
p_map : Positions (Np x 3)
f_map : Frequency (Nf x 3)
T_map : Rotation matrices (Nt x 3)
A_map : Antenna name (Na x 3)
Groups and subgroups:
Signature identifier (si_ID#N):
ca_cb_cutoff
Ray identifier (ray_ID#N):
cutoff_ua_ub
Ctilde identifier (Ct_ID#N):
ua_ub_uf
H identifier (H_ID#N):
ua_ub_uf_uTa_uTb_uAa_uAb
with
ca : cycle number of a
cb : cycle number of b
cutoff : signature.run cutoff
ua : indice of a position in 'p_map' position dataset
ub : indice of a position in 'p_map' position dataset
uf : indice of freq position in 'f_map' frequency dataset
uTa : indice of a position in 'T_map' Rotation dataset
uTb : indice of a position in 'T_map' Rotation dataset
uAa : indice of a position in 'A_map' Antenna name dataset
uAb : indice of b position in 'A_map' Antenna name dataset
Examples
--------
>>> from pylayers.simul.link import *
>>> L = DLink(verbose=False)
>>> aktk = L.eval()
"""
Link.__init__(self)
defaults={ 'L':Layout(),
'a':np.array(()),
'b':np.array(()),
'Aa':Antenna(typ='Omni'),
'Ab':Antenna(typ='Omni'),
'Ta':np.eye(3),
'Tb':np.eye(3),
'fGHz':[],
'wav':wvf.Waveform(),
'cutoff':3,
'save_opt':['sig','ray','Ct','H'],
'save_idx':0,
'force_create':False,
'verbose':True,
'graph':'tcvirw'
}
self._ca=-1
self._cb=-1
specset = ['a','b','Aa','Ab','Ta','Tb','L','fGHz','wav']
# set default attribute
for key, value in defaults.items():
if key not in kwargs:
if key in specset :
setattr(self,'_'+key,value)
else :
setattr(self,key,value)
else :
if key in specset :
setattr(self,'_'+key,kwargs[key])
else :
setattr(self,key,kwargs[key])
force=self.force_create
delattr(self,'force_create')
if self.fGHz == []:
self.initfreq()
else :
pass
try:
self._Lname = self._L.filename
except:
self._L=Layout(self._L)
self._Lname = self._L.filename
###########
# Transmitter and Receiver positions
###########
self.tx = RadioNode(name = '',
typ = 'tx',
_fileini = 'radiotx.ini',
)
self.rx = RadioNode(name = '',
typ = 'rx',
_fileini = 'radiorx.ini',
)
self.filename = 'Links_' + str(self.save_idx) + '_' + self._Lname + '.h5'
filenameh5 = pyu.getlong(self.filename,pstruc['DIRLNK'])
# check if save file alreasdy exists
if not os.path.exists(filenameh5) or force:
print 'Links save file for ' + self.L.filename + ' does not exist.'
print 'Creating file. You\'ll see this message only once per Layout'
self.save_init(filenameh5)
# dictionnary data exists
self.dexist={'sig':{'exist':False,'grpname':''},
'ray':{'exist':False,'grpname':''},
'Ct':{'exist':False,'grpname':''},
'H':{'exist':False,'grpname':''}
}
try:
self.L.dumpr()
except:
print('This is the first time the Layout is used. Graphs have to be built. Please Wait')
self.L.build(graph=self.graph)
self.L.dumpw()
#self.L.build()
###########
# init pos & cycles
#
# If a and b are not specified
# they are chosen as center of gravity of cycle 0
#
###########
if len(self.a)==0:
self.ca = 1
# self.a = self.L.cy2pt(self.ca)
else:
if len(kwargs['a']) ==2:
a=np.r_[kwargs['a'],1.0]
else:
a=kwargs['a']
self.a = a
# self.ca = self.L.pt2cy(self.a)
if len(self.b)==0:
if len(self.L.Gt.node)>2:
self.cb = 2
else:
self.cb = 1
# self.b = self.L.cy2pt(self.cb)
else:
if len(kwargs['b']) ==2:
b=np.r_[kwargs['b'],1.0]
else:
b=kwargs['b']
self.b = b
# self.cb = self.L.pt2cy(self.b)
###########
# init freq
# TODO Check where it is used redundant with fGHz
###########
#self.fmin = self.fGHz[0]
#self.fmax = self.fGHz[-1]
#self.fstep = self.fGHz[1]-self.fGHz[0]
self.Si = Signatures(self.L,self.ca,self.cb,cutoff=self.cutoff)
self.R = Rays(self.a,self.b)
self.C = Ctilde()
self.H = Tchannel()
def eval(self,**kwargs):
""" evaluate the link
Parameters
----------
applywav :boolean
Apply waveform to H
force : list
Force the computation (['sig','ray','Ct','H']) AND save (replace previous computations)
si_algo : str ('old'|'new')
signature.run algo type
'old' : call propaths2
'new' : call procone2
alg : 5|7
version of run for signature
si_mt: boolean
Multi thread version of algo version 7
si_progress: bollean ( False)
display progression bar for signatures
diffraction : boolean (False)
takes into consideration diffraction points
ra_number_mirror_cf : int
rays.to3D number of ceil/floor reflexions
ra_ceil_H: float, (default [])
ceil height .
If [] : Layout max ceil height
ra_vectorized: boolean (True)
if True used the (2015 new) vectorized approach to determine 2drays
Returns
-------
ak : ndarray
alpha_k
tk : ndarray
tau_k
Notes
-----
update self.ak and self.tk
self.ak : ndarray
alpha_k
self.tk : ndarray
tau_k
Examples
--------
.. plot::
:include-source:
>>> from pylayers.simul.link import *
>>> L=DLink(verbose=False)
>>> aktk = L.eval()
See Also
--------
pylayers.antprop.signature
pylayers.antprop.rays
Experimental
------------
alg = 2015 | 20152 (best)
vectorized signature research
si_reverb : number of reverb in source/target cycle if alg=2015
"""
defaults={ 'applywav':True,
'si_algo':'old',
'si_mt':False,
'si_progress':False,
'diffraction':True,
'ra_vectorized':True,
'ra_ceil_H':[],
'ra_number_mirror_cf':1,
'force':[],
'alg':7,
'si_reverb':4,
'threshold':0.1,
'verbose':[],
}
for key, value in defaults.items():
if key not in kwargs:
kwargs[key]=value
if 'cutoff' not in kwargs:
kwargs['cutoff']=self.cutoff
else:
self.cutoff=kwargs['cutoff']
if 'force' in kwargs:
if not isinstance(kwargs['force'],list):
if kwargs['force'] == True :
kwargs['force'] = ['sig','ray','Ct','H']
else :
kwargs['force'] = []
if kwargs['verbose'] != []:
self.verbose=kwargs['verbose']
# must be placed after all the init !!!!
if self.verbose :
print "checkh5"
self.checkh5()
############
# Signatures
############
if self.verbose :
print "Start Signatures"
tic = time.time()
Si = Signatures(self.L,self.ca,self.cb,cutoff=kwargs['cutoff'])
if (self.dexist['sig']['exist'] and not ('sig' in kwargs['force'])):
self.load(Si,self.dexist['sig']['grpname'])
if self.verbose :
print "load signature"
else :
if kwargs['alg']==2015:
TMP=Si.run2015(cutoff=kwargs['cutoff'],
cutoffbound=kwargs['si_reverb'])
if self.verbose :
print "algo 2015"
if kwargs['alg']==20152:
TMP=Si.run2015_2(cutoff=kwargs['cutoff'],
cutoffbound=kwargs['si_reverb'])
if self.verbose :
print "algo 20152"
if kwargs['alg']==5:
Si.run5(cutoff=kwargs['cutoff'],
algo=kwargs['si_algo'],
diffraction=kwargs['diffraction'],
progress=kwargs['si_progress'])
if self.verbose :
print "algo 5"
if kwargs['alg']==7:
if kwargs['si_mt']==7:
Si.run7mt(cutoff=kwargs['cutoff'],
algo=kwargs['si_algo'],
diffraction=kwargs['diffraction'],
threshold=kwargs['threshold'],
progress=kwargs['si_progress'])
if self.verbose :
print "algo 7 , si_mt"
else :
Si.run7(cutoff=kwargs['cutoff'],
algo=kwargs['si_algo'],
diffraction=kwargs['diffraction'],
threshold=kwargs['threshold'],
progress=kwargs['si_progress'])
if self.verbose :
print "algo 7"
#Si.run6(diffraction=kwargs['diffraction'])
# save sig
self.save(Si,'sig',self.dexist['sig']['grpname'],force = kwargs['force'])
self.Si = Si
toc = time.time()
if self.verbose :
print "Stop signature",toc-tic
############
# Rays
############
if self.verbose :
print "Start Rays"
tic = time.time()
R = Rays(self.a,self.b)
if self.dexist['ray']['exist'] and not ('ray' in kwargs['force']):
self.load(R,self.dexist['ray']['grpname'])
else :
# perform computation ...
# ... with vetorized ray evaluation approach
if kwargs['ra_vectorized']:
r2d = Si.raysv(self.a,self.b)
# ... or with original and slow approach ( to be removed in a near future)
else :
r2d = Si.rays(self.a,self.b)
if kwargs['ra_ceil_H'] == []:
ceilheight = self.L.maxheight
else:
ceilheight = kwargs['ra_ceil_H']
R = r2d.to3D(self.L,H=ceilheight, N=kwargs['ra_number_mirror_cf'])
R.locbas(self.L)
# ...and save
R.fillinter(self.L)
C=Ctilde()
C = R.eval(self.fGHz)
self.save(R,'ray',self.dexist['ray']['grpname'],force = kwargs['force'])
self.R = R
toc = time.time()
if self.verbose :
print "Stop rays",toc-tic
if self.R.nray == 0:
raise NameError('No rays have been found. Try to re-run the simulation with a higher S.cutoff ')
############
# Ctilde
############
if self.dexist['Ct']['exist'] and not ('Ct' in kwargs['force']):
C=Ctilde()
self.load(C,self.dexist['Ct']['grpname'])
else :
if not hasattr(R,'I'):
# Ctilde...
C = R.eval(self.fGHz)
# ...save Ct
self.save(C,'Ct',self.dexist['Ct']['grpname'],force = kwargs['force'])
self.C = C
############
# H
############
H = Tchannel()
if self.dexist['H']['exist'] and not ('H' in kwargs['force']):
self.load(H,self.dexist['H']['grpname'])
else :
# Ctilde antenna
Cl=C.locbas(Tt=self.Ta, Tr=self.Tb)
#T channel
H = C.prop2tran(a=self.Aa,b=self.Ab,Friis=True,debug=True)
self.save(H,'H',self.dexist['H']['grpname'],force = kwargs['force'])
self.H = H
if kwargs['applywav']:
if self.H.isFriis:
self.ir = self.H.get_cir(self.wav.sf)
else:
self.ir = self.H.get_cir(self.wav.sfg)
return self.H.ak, self.H.tk
def eval(self,**kwargs):
""" Evaluate the link
Parameters
----------
force : boolean
Force the computation (even if obj already exists) AND save (replace previous computations)
si_algo : str ('old'|'new')
signature.run algo type
ra_ceil_height_meter : int
rays.to3D ceil height in meters
ra_number_mirror_cf : int
rays.to3D number of ceil/floor reflexions
Returns
-------
ak : ndarray
alpha_k
tk : ndarray
tau_k
Notes
-----
update self.ak and self.tk
self.ak : ndarray
alpha_k
self.tk : ndarray
tau_k
Examples
--------
.. plot::
:include-source:
>>> from pylayers.simul.link import *
>>> L=DLink(verbose=False)
>>> aktk = L.eval()
See Also
--------
pylayers.antprop.signature
pylayers.antprop.rays
"""
defaults={ 'output':['sig','ray','Ct','H'],
'si_algo':'old',
'diffraction':False,
'ra_ceil_height_meter':3,
'ra_number_mirror_cf':1,
'force':False,
'alg':7,
'threshold':0.1,
}
for key, value in defaults.items():
if key not in kwargs:
kwargs[key]=value
self.checkh5()
if 'cutoff' not in kwargs:
kwargs['cutoff']=self.cutoff
############
# Signatures
############
Si = Signatures(self.L,self.ca,self.cb,cutoff=kwargs['cutoff'])
if self.dexist['sig']['exist'] and not kwargs['force']:
self.load(Si,self.dexist['sig']['grpname'])
else :
if kwargs['alg']==5:
Si.run5(cutoff=kwargs['cutoff'],algo=kwargs['si_algo'],diffraction=kwargs['diffraction'])
if kwargs['alg']==7:
Si.run7(cutoff=kwargs['cutoff'],
algo=kwargs['si_algo'],
diffraction=kwargs['diffraction'],
threshold=kwargs['threshold'])
#Si.run6(diffraction=kwargs['diffraction'])
# save sig
self.save(Si,'sig',self.dexist['sig']['grpname'],force = kwargs['force'])
self.Si = Si
############
# Rays
############
R = Rays(self.a,self.b)
if self.dexist['ray']['exist'] and not kwargs['force']:
self.load(R,self.dexist['ray']['grpname'])
else :
# perform computation ...
r2d = Si.rays(self.a,self.b)
R = r2d.to3D(self.L,H=kwargs['ra_ceil_height_meter'], N=kwargs['ra_number_mirror_cf'])
R.locbas(self.L)
# ...and save
self.save(R,'ray',self.dexist['ray']['grpname'],force = kwargs['force'])
self.R = R
if self.R.nray == 0:
raise NameError('No rays have been found. Try to re-run the simulation with a higher S.cutoff ')
############
# Ctilde
############
C=Ctilde()
if self.dexist['Ct']['exist'] and not kwargs['force']:
self.load(C,self.dexist['Ct']['grpname'])
else :
R.fillinter(self.L)
# Ctilde...
C = R.eval(self.fGHz)
# ...save Ct
self.save(C,'Ct',self.dexist['Ct']['grpname'],force = kwargs['force'])
self.C = C
############
# H
############
H=Tchannel()
if self.dexist['H']['exist'] and not kwargs['force']:
self.load(H,self.dexist['H']['grpname'])
else :
# Ctilde antenna
Cl=C.locbas(Tt=self.Ta, Tr=self.Tb)
#T channel
H = C.prop2tran(a=self.Aa,b=self.Ab,Friis=True)
self.save(H,'H',self.dexist['H']['grpname'],force = kwargs['force'])
self.H = H
return self.H.ak, self.H.tk
tx = array([759, 1114, 1.0]) rx = array([767, 1114, 1.5]) S.tx.clear() S.rx.clear() S.tx.point(tx) S.rx.point(rx) # get cycle from coordinates Ctx = S.L.pt2cy(S.tx.position[:, 0]) Crx = S.L.pt2cy(S.rx.position[:, 0]) fGHz = np.arange(2, 11, 0.1) wav = wvf.Waveform(fcGHz=5, bandGHz=3) # # Dans un sens # tic = time.time() Si1 = Signatures(S.L, Ctx, Crx) # Si1.run4(cutoff=5,algo='old') Si1.run(diffraction=False) toc = time.time() print "signature ", toc - tic tic = time.time() r2d = Si1.rays(tx, rx) print "2D rays ", tic - toc r3d1 = r2d.to3D(S.L) toc = time.time() print "3D rays ", toc - tic r3d1.locbas(S.L) tic = time.time() print "3D rays locbas", tic - toc r3d1.fillinter(S.L) toc = time.time()
S.L.build() tx=array([759,1114,1.0]) rx=array([767,1114,1.5]) S.tx.clear() S.rx.clear() S.tx.point(tx) S.rx.point(rx) # get cycle from coordinates Ctx = S.L.pt2cy(S.tx.position[:,0]) Crx = S.L.pt2cy(S.rx.position[:,0]) fGHz=np.arange(2,11,0.1) wav = wvf.Waveform(fcGHz=5,bandGHz=3) # # Dans un sens # Si1 = Signatures(S.L,Ctx,Crx) #Si1.run4(cutoff=5,algo='old') Si1.run5(diffraction=False) toc = time.time() print "signature ",toc-tic tic = time.time() r2d = Si1.rays(tx,rx) print "2D rays ",tic-toc r3d1 = r2d.to3D(S.L) toc = time.time() print "3D rays ",toc-tic r3d1.locbas(S.L) tic = time.time() print "3D rays locbas",tic-toc r3d1.fillinter(S.L) toc = time.time()
