def vec2scalA(self, At, Ar, alpha=1.0):
"""
vec2scalA(self,At,Ar,alpha=1.0):
At = transmitter antenna
Ar = receiver antenna
Calculate ScalChannel by combining the propagation channel VectChannel
with realistic antennas transfer function
alpha : normalization factor
"""
Ftt, Ftp = At.Fsynth3(self.rang[:, 0], self.rang[:, 1])
Frt, Frp = Ar.Fsynth3(self.rang[:, 0], self.rang[:, 1])
Ftt = Ftt.transpose()
Ftp = Ftp.transpose()
Frt = Frt.transpose()
Frp = Frp.transpose()
Ftt = bs.FUsignal(At.fa, Ftt * alpha)
Ftp = bs.FUsignal(At.fa, Ftp * alpha)
Frt = bs.FUsignal(Ar.fa, Frt * alpha)
Frp = bs.FUsignal(Ar.fa, Frp * alpha)
scalch = ScalChannel(self, Ftt, Ftp, Frt, Frp)
return(scalch)
def VCg2VCl(VCg, Tt, Tr):
""" global reference frame to local reference frame
Parameters
----------
VCg : VectChannel global
Tt : Tx rotation matrix
Tr : Rx rotation matrix
Returns
-------
VCl : VectChannel (local)
"""
import copy
VCl = copy.deepcopy(VCg)
freq = VCl.freq
Rt, tangl = BTB_tx(VCg.tang, Tt)
Rr, rangl = BTB_rx(VCg.rang, Tr)
VCl.tang = tangl
VCl.rang = rangl
uf = np.ones(VCg.nfreq)
r0 = np.outer(Rr[0, 0, :], uf)
r1 = np.outer(Rr[0, 1, :], uf)
# print "shape r0 = ",np.shape(r0)
# print "shape VCg.Ctt.y = ",np.shape(VCg.Ctt.y)
# print "shape r1 = ",np.shape(r1)
# print "shape VCg.Cpt.y = ",np.shape(VCg.Cpt.y)
t00 = r0 * VCg.Ctt.y + r1 * VCg.Cpt.y
t01 = r0 * VCg.Ctp.y + r1 * VCg.Cpp.y
r0 = np.outer(Rr[1, 0, :], uf)
r1 = np.pouter(Rr[1, 1, :], uf)
t10 = r0 * VCg.Ctt.y + r1 * VCg.Cpt.y
t11 = r0 * VCg.Ctp.y + r1 * VCg.Cpp.y
r0 = np.outer(Rt[0, 0, :], uf)
r1 = np.outer(Rt[1, 0, :], uf)
Cttl = t00 * r0 + t01 * r1
Cptl = t10 * r0 + t11 * r1
r0 = np.outer(Rt[0, 1, :], uf)
r1 = np.outer(Rt[1, 1, :], uf)
Ctpl = t00 * r0 + t01 * r1
Cppl = t10 * r0 + t11 * r1
VCl.Ctt = bs.FUsignal(freq, Cttl)
VCl.Ctp = bs.FUsignal(freq, Ctpl)
VCl.Cpt = bs.FUsignal(freq, Cptl)
VCl.Cpp = bs.FUsignal(freq, Cppl)
return VCl
def __init__(self, d, fmin=2, fmax=11, Nf=180):
self.tauk = np.array([d / 0.3])
freq = np.linspace(fmin, fmax, Nf)
c1 = 1.0 / d * np.ones(len(freq))
c2 = zeros(len(freq))
c1.reshape(1, Nf)
c2.reshape(1, Nf)
self.freq = freq
self.Ctt = bs.FUsignal(freq, c1)
self.Ctp = bs.FUsignal(freq, c2)
self.Cpt = bs.FUsignal(freq, c2)
self.Cpp = bs.FUsignal(freq, c1)
self.tang = array([0])
self.rang = array([0])
self.nray = 1
def eval(self):
u""" evaluate waveform
The :math:`\lambda/4*\pi` factor which is necessary to get the proper budget
link ( from the Friis formula) is introduced in this function.
"""
if self['typ'] == 'generic':
[st, sf] = self.ip_generic()
#elif self['typ'] == 'mbofdm':
# [st,sf]=self.mbofdm()
elif self['typ'] == 'W1compensate':
[st, sf] = self.fromfile()
elif self['typ'] == 'W1offset':
[st, sf] = self.fromfile2()
else:
logging.critical('waveform typ not recognized, check your config \
file')
self.st = st
self.sf = sf
self.f = self.sf.x
ygamma = -1j * 0.3 / (4 * np.pi * self.f)
self.gamm = bs.FUsignal(x=self.f, y=ygamma)
self.sfg = self.sf * self.gamm
self.sfgh = self.sfg.symH(0)
self.stgh = self.sfgh.ifft(1)
def vec2scal(self):
""" calculate scalChannel from VectChannel and antenna
Returns
-------
slach : ScalChannel
"""
freq = self.freq
sh = np.shape(self.Ctt.y)
Ftt = bs.FUsignal(freq, np.ones(sh))
Ftp = bs.FUsignal(freq, np.zeros(sh))
Frt = bs.FUsignal(freq, np.ones(sh))
Frp = bs.FUsignal(freq, np.zeros(sh))
scalch = ScalChannel(self, Ftt, Ftp, Frt, Frp)
return(scalch)
def freqz(self,**kwargs):
""" freqz : evaluation of filter transfer function
The function evaluates an FUsignal
Parameters
----------
display : boolean
True
fsGHz : float
if set to 0 (relative frequency)
"""
defaults = {'display':True,
'fsGHz':0}
for k in defaults:
if k not in kwargs:
kwargs[k]=defaults[k]
(w,h) = si.freqz(self.b,self.a)
if kwargs['fsGHz']!=0:
fNGHz = kwargs['fsGHz']/2.
self.H = bs.FUsignal(w*fNGHz/np.pi,h)
xlabel = 'Frequency (GHz)'
else:
self.H = bs.FUsignal(w/np.pi,h)
xlabel = 'Relative frequency'
if kwargs['display']:
if 'fig' not in kwargs:
fig = plt.figure()
else:
fig = kwargs['fig']
ax1 = fig.add_subplot(211)
self.H.plot(typ=['l20'],xlabels=[xlabel],fig=fig,ax=ax1)
plt.grid()
ax2 = fig.add_subplot(212)
self.H.plot(typ=['d'],xlabels=[xlabel],fig=fig,ax=ax2)
plt.grid()
def eval(self):
""" evaluate waveform
The lambda/4*pi factor which is necessary to get the proper budget
link ( from the fris formula) is introduced in this function.
"""
if self.parameters['type'] == 'generic':
[st,sf]=self.ip_generic()
if self.parameters['type'] == 'mbofdm':
[st,sf]=self.mbofdm()
if self.parameters['type'] == 'file':
[st,sf]=self.fromfile()
self.st = st
self.sf = sf
self.f = self.sf.x
ygamma = -1j*0.3/(4*np.pi*self.f)
self.gamm = bs.FUsignal(self.f,ygamma)
self.sfg = self.sf*self.gamm
self.sfgh = self.sfg.symH(0)
self.stgh = self.sfgh.ifft(1)
def eval(self, fGHz=np.array([2.4])):
"""docstring for eval"""
print 'Rays evaluation'
self.I.eval(fGHz)
B = self.B.eval(fGHz)
B0 = self.B0.eval(fGHz)
# Ct : f x r x 2 x 2
Ct = np.zeros((self.I.nf, self.nray, 2, 2), dtype=complex)
# delays : ,r
self.delays = np.zeros((self.nray))
# dis : ,r
self.dis = np.zeros((self.nray))
#nf : number of frequency point
nf = self.I.nf
aod = np.empty((2, self.nray))
aoa = np.empty((2, self.nray))
# loop on interaction blocks
for l in self:
# l stands for the number of interactions
r = self[l]['nbrays']
# reshape in order to have a 1D list of index
# reshape ray index
rrl = self[l]['rays'].reshape(r * l, order='F')
# get the corresponding evaluated interactions
A = self.I.I[:, rrl, :, :].reshape(self.I.nf,
r,
l,
2,
2,
order='F')
Bl = B[:, rrl, :, :].reshape(self.I.nf, r, l, 2, 2, order='F')
B0l = B0[:, self[l]['rayidx'], :, :]
alpha = self.I.alpha[rrl].reshape(r, l, order='F')
gamma = self.I.gamma[rrl].reshape(r, l, order='F')
si0 = self.I.si0[rrl].reshape(r, l, order='F')
sout = self.I.sout[rrl].reshape(r, l, order='F')
aoa[:, self[l]['rayidx']] = self[l]['aoa']
aod[:, self[l]['rayidx']] = self[l]['aod']
try:
del Z
except:
pass
## loop on all the interactions of ray with l interactions
for i in range(0, l):
############################################
## # Divergence factor D
### not yet implementented
############################################
# if i == 0:
# D0=1./si0[:,1]
# rho1=si0[:,1]*alpha[:,i]
# rho2=si0[:,1]*alpha[:,i]*gamma[:,i]
# D=np.sqrt(
# ( (rho1 ) / (rho1 + sout[:,i]) )
# *( (rho2) / (rho2 + sout[:,i])))
# D=D*D0
# rho1=rho1+(sout[:,i]*alpha[:,i])
# rho2=rho2+(sout[:,i]*alpha[:,i]*gamma[:,i])
## gerer le loss
# if np.isnan(D).any():
# p=np.nonzero(np.isnan(D))[0]
# D[p]=1./sout[p,1]
# else :
# D=np.sqrt(
# ( (rho1 ) / (rho1 + sout[:,i]) )
# *( (rho2) / (rho2 + sout[:,i])))
# rho1=rho1+(sout[:,i]*alpha[:,i])
# rho2=rho2+(sout[:,i]*alpha[:,i]*gamma[:,i])
############################################
# A0 (X dot Y)
# | | |
# v v v
##########################
## B # I # B # I # B #
##########################
# \_____/ \______/
# | |
# Atmp(i) Atmp(i+1)
#
# Z=Atmp(i) dot Atmp(i+1)
X = A[:, :, i, :, :]
Y = Bl[:, :, i, :, :]
## Dot product interaction X Basis
Atmp = np.sum(X[..., :, :, np.newaxis] *
Y[..., np.newaxis, :, :],
axis=-2) #*D[np.newaxis,:,np.newaxis,np.newaxis]
if i == 0:
## First Baspdis added
A0 = B0l[:, :, :, :]
Z = np.sum(A0[..., :, :, np.newaxis] *
Atmp[..., np.newaxis, :, :],
axis=-2)
else:
# dot product previous interaction with latest
Z = np.sum(Z[..., :, :, np.newaxis] *
Atmp[..., np.newaxis, :, :],
axis=-2)
# fill the C tilde
Ct[:, self[l]['rayidx'], :, :] = Z[:, :, :, :]
# delay computation:
self[l]['dis'] = self.I.si0[self[l]['rays'][0, :]] + np.sum(
self.I.sout[self[l]['rays']], axis=0)
# Power losses due to distances
# will be removed once the divergence factor will be implemented
Ct[:,
self[l]['rayidx'], :, :] = Ct[:,
self[l]['rayidx'], :, :] * 1. / (
self[l]['dis'][np.newaxis, :,
np.newaxis,
np.newaxis])
self.delays[self[l]['rayidx']] = self[l]['dis'] / 0.3
self.dis[self[l]['rayidx']] = self[l]['dis']
# To be corrected in a future version
Ct = np.swapaxes(Ct, 1, 0)
c11 = Ct[:, :, 0, 0]
c12 = Ct[:, :, 0, 1]
c21 = Ct[:, :, 1, 0]
c22 = Ct[:, :, 1, 1]
Cn = Ctilde()
Cn.Cpp = bs.FUsignal(self.I.fGHz, c11)
Cn.Ctp = bs.FUsignal(self.I.fGHz, c12)
Cn.Cpt = bs.FUsignal(self.I.fGHz, c21)
Cn.Ctt = bs.FUsignal(self.I.fGHz, c22)
Cn.nfreq = self.I.nf
Cn.nray = self.nray
Cn.tauk = self.delays
Cn.fGHz = self.I.fGHz
# r x 2
Cn.tang = aod.T
# r x 2
Cn.rang = aoa.T
# add aoa and aod
return (Cn)
freq = Gt.I.f nfreq = Gt.I.nf nray = np.array(([Gt.nray])) Cr = np.swapaxes(Gt.Ctilde, 1, 0) #Cr=Gt.Ctilde.reshape(nray, nfreq,2,2) #Cr=np.transpose(Gt.Ctilde,(1,0,2,3)) c11 = Cr[:, :, 0, 0] c12 = Cr[:, :, 0, 1] c21 = Cr[:, :, 1, 0] c22 = Cr[:, :, 1, 1] Cn = Ctilde() Cn.Cpp = bs.FUsignal(freq, c11) Cn.Ctp = bs.FUsignal(freq, c12) Cn.Cpt = bs.FUsignal(freq, c21) Cn.Ctt = bs.FUsignal(freq, c22) Cn.nfreq = Gt.I.nf Cn.nray = Gt.nray Cn.tauk = Gt.delays r = 0 plotray(r) ### RECIPROCITY TEST #S2 = Simul() ## loading a layout #filestr = 'defstr'
def load(self, filefield, transpose=False):
""" load a Ctilde from a .field file
Load the three files .tauk .tang .rang which contain respectively
delay , angle of departure , angle of arrival.
Parameters
----------
filefield : string
transpose : boolean
default False
Examples
--------
>>> from pylayers.antprop.channel import *
>>> from pylayers.simul.simulem import *
>>> S=Simul()
>>> S.load('default.ini')
>>> C =Ctilde()
>>> C.load(pyu.getlong(S.dtud[1][1],'output'))
"""
filetauk = filefield.replace('.field', '.tauk')
filetang = filefield.replace('.field', '.tang')
filerang = filefield.replace('.field', '.rang')
try:
fo = open(filefield, "rb")
except:
raise NameError( "file "+ filefield+ " is unreachable")
# decode filename (*.field file obtained from evalfield simulation)
nray = stru.unpack('i', fo.read(4))[0]
print "nray : ", nray
nfreq = stru.unpack('i', fo.read(4))[0]
print "nfreq : ", nfreq
if nfreq == 0:
print " Error : incorrect number of frequency points in .field"
self.fail = True
return
n = nray * nfreq
buf = fo.read()
fo.close()
CMat = np.ndarray(shape=(n,8),buffer=buf)
c11 = CMat[:, 0] + CMat[:, 1]*1j
c12 = CMat[:, 2] + CMat[:, 3]*1j
c21 = CMat[:, 4] + CMat[:, 5]*1j
c22 = CMat[:, 6] + CMat[:, 7]*1j
c11 = c11.reshape(nray, nfreq)
c12 = c12.reshape(nray, nfreq)
c21 = c21.reshape(nray, nfreq)
c22 = c22.reshape(nray, nfreq)
if transpose:
c11 = c11.transpose()
c12 = c12.transpose()
c21 = c21.transpose()
c22 = c22.transpose()
#
# Temporary freq --> read filefreq
#
freq = np.linspace(2, 11, nfreq)
self.Ctt = bs.FUsignal(freq, c11)
self.Ctp = bs.FUsignal(freq, c12)
self.Cpt = bs.FUsignal(freq, c21)
self.Cpp = bs.FUsignal(freq, c22)
self.nfreq = nfreq
self.nray = nray
try:
fo = open(filetauk, "rb")
except:
self.fail = True
print "file ", filetauk, " is unreachable"
# decode filetauk
if not self.fail:
nray_tauk = stru.unpack('i', fo.read(4))[0]
print "nb rays in .tauk file: ", nray_tauk
buf = fo.read()
fo.close()
nray = len(buf) / 8
print "nb rays 2: ", nray
self.tauk = np.ndarray(shape=nray, buffer=buf)
if nray_tauk != nray:
print nray_tauk - nray
self.tauk = self.tauk
# decode the angular files (.tang and .rang)
try:
fo = open(filetang, "rb")
except:
self.fail = True
print "file ", filetang, " is unreachable"
if not self.fail:
nray_tang = stru.unpack('i', fo.read(4))[0]
buf = fo.read()
fo.close()
# coorectif Bug evalfield
tmp = np.ndarray(shape=(nray_tang, 2), buffer=buf)
self.tang = tmp[0:nray, :]
try:
fo = open(filerang, "rb")
except:
self.fail = True
print "file ", filerang, " is unreachable"
if not self.fail:
nray_rang = stru.unpack('i', fo.read(4))[0]
buf = fo.read()
fo.close()
# coorectif Bug evalfield
tmp = np.ndarray(shape=(nray_rang, 2), buffer=buf)
self.rang = tmp[0:nray, :]
def prop2tran(self,a='theta',b='theta'):
""" transform propagation channel into transmission channel
Parameters
----------
a : string or antenna array
polarization antenna a ( 'theta' | 'phi' | 'ant' )
: string or antenna array
polarization antenna b ( 'theta' | 'phi' | 'ant' )
0 : theta
1 : phi
Returns
-------
H : Tchannel(bs.FUDAsignal)
"""
freq = self.freq
nfreq = self.nfreq
nray = self.nray
sh = np.shape(self.Ctt.y)
if type(a)==str:
Fat = np.zeros(nray*nfreq).reshape((nray,nfreq))
Fap = np.zeros(nray*nfreq).reshape((nray,nfreq))
if a=='theta':
Fat = np.ones((nray,nfreq))
if a=='phi':
Fap = np.ones((nray,nfreq))
Fat = bs.FUsignal(self.freq,Fat)
Fap = bs.FUsignal(self.freq,Fap)
else:
Fat , Fap = a.Fsynth3(self.rang[:, 0],self.rang[:,1])
Fat = Fat.transpose()
Fap = Fap.transpose()
Fat = bs.FUsignal(a.fa,Fat)
Fap = bs.FUsignal(a.fa,Fap)
if type(b)==str:
Fbt = np.zeros(nray*nfreq).reshape((nray,nfreq))
Fbp = np.zeros(nray*nfreq).reshape((nray,nfreq))
if b=='theta':
Fbt = np.ones((nray,nfreq))
if b=='phi':
Fbp = np.ones((nray,nfreq))
Fbt = bs.FUsignal(self.freq,Fbt)
Fbp = bs.FUsignal(self.freq,Fbp)
else:
Fbt , Fbp = b.Fsynth3(self.rang[:, 0],self.rang[:,1])
# (nray,nfeq) needed
Fbt = Fbt.transpose()
Fbp = Fbp.transpose()
Fbt = bs.FUsignal(b.fa,Fbt)
Fbp = bs.FUsignal(b.fa,Fbp)
#pdb.set_trace()
t1 = self.Ctt * Fat + self.Cpt * Fap
t2 = self.Ctp * Fat + self.Cpp * Fap
alpha = t1 * Fbt + t2 * Fbp
H = Tchannel(alpha.x,alpha.y,self.tauk,self.tang,self.rang)
return(H)
