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dda_si_integration_funcs.py
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dda_si_integration_funcs.py
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import numpy
import misc
import ott_funcs
# # gshank integrates the 6 sommerfeld integrals from start to
# # infinity (until convergence) in lambda. at the break point, bk,
# # the step increment may be changed from dela to delb. shank's
# # algorithm to accelerate convergence of a slowly converging series
# # is used
# # void gshank( complex double start, complex double dela, complex double *sum,
# # int nans, complex double *seed, int ibk, complex double bk, complex double delb )
def gshank(start, dela, suminc, nans, seed, ibk, bk, delb, zph, rho, k1, k2, jh): # return suminc
# # start = A_0
# # dela = delta before break point
# # suminc = increment of integral
# # nans = number of functions
# # seed = S_0
# # ibk = flag if path contains a break point (1 or 0)
# # bk = break point (d*) in the path
# # delb = delta after break point
# # jh = flag 1 or 0, respectively for Bessel or Hankel function forms
#
# # complex double q1[6][20], q2[6][20], ans1[6], ans2[6];
#suminc = suminc_start
q1 = numpy.zeros([6, 20], dtype=numpy.complex128)
q2 = numpy.zeros([6, 20], dtype=numpy.complex128)
ans1 = numpy.zeros([6, 1], dtype=numpy.complex128)
# # constants
MAXH = 20
CRIT = 1E-4
rbk = numpy.real(bk)
delt = dela
if ibk == 0:
ibx = 1
else:
ibx = 0
#brk = False # TODO: Where should it be assigned?
# for( i = 0; i < nans; i++ )
# # ans2[i]=seed[i];
ans2 = seed
b = start
# for( intx = 1; intx <= MAXH; intx++ )
for intx in numpy.arange(1, MAXH + 1): # TODO: test interval
inx = intx - 1 # inx=intx-1
a = b
b = b + delt # b += del
if (ibx == 0) and (numpy.real(b) >= rbk):
# hit break point. reset seed and start over.
ibx = 1
b = bk
delt = delb
suminc = rom1(nans, 2, zph, rho, k1, k2, a, b, jh) # rom1(nans,sum,2)
if ibx != 2:
# for( i = 0; i < nans; i++ )
# ans2[i] += sum[i];
ans2 = ans2 + suminc
intx = 0
continue
# # for( i = 0; i < nans; i++ )
# # ans2[i]=ans1[i]+sum[i];
ans2 = ans1 + suminc
intx = 0
continue
# end # } /* if( (ibx == 0) && (creal(b) >= rbk) ) */
suminc = rom1(nans, 2, zph, rho, k1, k2, a, b, jh) # rom1(nans,sum,2);
# # for( i = 0; i < nans; i++ )
# # ans1[i] = ans2[i]+sum[i];
ans1 = ans2 + suminc
a = b
b = b + delt # b += del;
# # if( (ibx == 0) && (creal(b) >= rbk) )
if (ibx == 0) and (numpy.real(b) >= rbk):
# hit break point. reset seed and start over.
ibx = 2
b = bk
delt = delb
suminc = rom1(nans, 2, zph, rho, k1, k2, a, b, jh) # rom1(nans,sum,2);
if ibx != 2:
# for( i = 0; i < nans; i++ )
# ans2[i] += sum[i];
ans2 = ans2 + suminc
intx = 0
continue
# for( i = 0; i < nans; i++ )
# ans2[i] = ans1[i]+sum[i];
ans2 = ans1 + suminc
intx = 0
continue
# end # } /* if( (ibx == 0) && (creal(b) >= rbk) ) */
suminc = rom1(nans, 2, zph, rho, k1, k2, a, b, jh) # rom1(nans,sum,2);
# for( i = 0; i < nans; i++ )
# ans2[i]=ans1[i]+sum[i];
ans2 = ans1 + suminc
den = 0
for j in numpy.arange(nans): # for( i = 0; i < nans; i++ )
as1 = ans1[j] # as1=ans1[i];
as2 = ans2[j] # as2=ans2[i];
if intx >= 2:
# for( j = 1; j < intx; j++ )
for k in numpy.arange(1, intx):
km = k - 1 # jm=j-1;
aa = q2[j, km] # aa=q2[i][jm];
a1 = q1[j, km] + as1 - 2. * aa # a1=q1[i][jm]+as1-2.*aa;
# if( (creal(a1) != 0.) or (cimag(a1) != 0.) ):
if (numpy.real(a1) != 0.) or (numpy.imag(a1) != 0.):
a2 = aa - q1[j, km] # a2=aa-q1[i][jm];
a1 = q1[j, km] - a2 * a2 / a1 # a1=q1[i][jm]-a2*a2/a1;
else:
a1 = q1[j, km] # a1=q1[i][jm];
a2 = aa + as2 - 2 * as1
# if( (creal(a2) != 0.) || (cimag(a2) != 0.) )
if (numpy.real(a2) != 0) or (numpy.imag(a2) != 0):
a2 = aa - (as1 - aa) * (as1 - aa) / a2
else:
a2 = aa
q1[j, km] = as1 # q1[i][jm]=as1;
q2[j, km] = as2 # q2[i][jm]=as2;
as1 = a1
as2 = a2
# end # } /* for( j = 1; i < intx; i++ ) */
# end # } /* if(intx >= 2) */
q1[j, intx - 1] = as1 # q1[i][intx-1]=as1;
q2[j, intx - 1] = as2 # q2[i][intx-1]=as2;
# amg=fabs(creal(as2))+fabs(cimag(as2));
amg = numpy.abs(numpy.real(as2)) + numpy.abs(numpy.imag(as2))
if amg > den:
den = amg
# end # } /* for( i = 0; i < nans; i++ ) */
denm = 1E-3 * den * CRIT # denm=1.e-3*den*CRIT;
km = intx - 3 # jm=intx-3;
if km < 1:
km = 1
# #for( j = jm-1; j < intx; j++ )
for k in numpy.arange(km - 1, intx):
brk = False # brk = FALSE;
# for (i = 0; i < nans; i++ )
for j in numpy.arange(nans):
a1 = q2[j, k] # a1=q2[i][j];
den = (numpy.abs(numpy.real(a1)) + numpy.abs(
numpy.imag(a1))) * CRIT # den=(fabs(creal(a1))+fabs(cimag(a1)))*CRIT;
if den < denm:
den = denm
a1 = q1[j, k] - a1 # a1=q1[i][j]-a1;
amg = numpy.abs(numpy.real(a1) + numpy.abs(numpy.imag(a1)))
if amg > den:
brk = True # brk = TRUE;
break
# end # } /* for( i = 0; i < nans; i++ ) */
if brk:
break
# end # } /* for( j = jm-1; j < intx; j++ ) */
if not brk: # if( ! brk )
# for( i = 0; i < nans; i++ )
# sum[i]=.5*(q1[i][inx]+q2[i][inx]);
suminc = .5 * (q1[:, inx] + q2[:, inx])
return suminc
# end # } /* for( intx = 1; intx <= maxh; intx++ ) */
raise Exception("Did not converge! :(")
# # /* No convergence */
# # abort_on_error(-6);
# # TODO: handle error
# % rom1 integrates the 6 sommerfeld integrals from a to b in lambda.
# % the method of variable interval width romberg integration is used.
# % void rom1( int n, complex double *sum, int nx )
def rom1(n, nx, zph, rho, k1, k2, a, b, jh):
# % n = number of functions?
# % nx = ?
# % static double z, ze, s, ep, zend, dz=0., dzot=0., tr, ti;
# % static complex double t00, t11, t02;
# % static complex double g1[6], g2[6], g3[6], g4[6], g5[6], t01[6], t10[6], t20[6];
dz = 0
dzot = 0
t01 = numpy.zeros([n], dtype=numpy.complex128)
t10 = numpy.zeros([n], dtype=numpy.complex128)
t20 = numpy.zeros([n], dtype=numpy.complex128)
# % constants
NM = 131072
CRIT = 1E-4
NTS = 4
lstep = 0
z = 0
ze = 1
s = 1
ep = s / (1E4 * NM) # ep=s/(1.e4*NM)
zend = ze - ep
# % for( i = 0; i < n; i++ )
# % sum[i]=CPLX_00;
suminc = numpy.zeros([n])
ns = nx
nt = 0
g1 = saoa(z, zph, rho, k1, k2, a, b, jh) # saoa(z,g1)
jump = 0 # jump = FALSE;
while True: # while( TRUE )
if not jump: # if( ! jump )
dz = s / ns
if (z + dz) > ze:
dz = ze - z
if dz <= ep:
return suminc
dzot = dz * .5
g3 = saoa(z + dzot, zph, rho, k1, k2, a, b, jh) # saoa(z+dzot,g3)
g5 = saoa(z + dz, zph, rho, k1, k2, a, b, jh) # saoa(z+dz,g5)
# /* if( ! jump ) */
nogo = 0 # nogo = FALSE;
# % for( i = 0; i < n; i++ )
# % {
# % t00=(g1[i]+g5[i])*dzot;
# % t01[i]=(t00+dz*g3[i])*.5;
# % t10[i]=(4.*t01[i]-t00)/3.;
# %
# % /* test convergence of 3 point romberg result */
# % test( creal(t01[i]), creal(t10[i]), &tr, cimag(t01[i]), cimag(t10[i]), &ti, 0. );
# % if( (tr > CRIT) || (ti > CRIT) )
# % nogo = TRUE;
# % }
for j in numpy.arange(n):
t00 = (g1[j] + g5[j]) * dzot
t01[j] = (t00 + dz * g3[j]) * .5
t10[j] = (4 * t01[j] - t00) / 3
# test convergence of 3 point romberg result
# test( creal(t01[i]), creal(t10[i]), &tr, cimag(t01[i]), cimag(t10[i]), &ti, 0. );
tr, ti = test(numpy.real(t01[j]), numpy.real(t10[j]), numpy.imag(t01[j]), numpy.imag(t10[j]), 0)
if (tr > CRIT) or (ti > CRIT):
nogo = 0 # nogo=TRUE TODO: TEST WHY NOT 1
if not nogo: # if( ! nogo ):
# for( i = 0; i < n; i++ )
# sum[i] += t10[i];
suminc = suminc + t10
nt += 2 # nt += 2
z += dz # z += dz
if z > zend:
return suminc
# for( i = 0; i < n; i++ )
# g1[i]=g5[i];
g1 = g5
if (nt >= NTS) and (ns > nx):
ns /= 2
nt = 1
jump = 0 # jump = FALSE
continue
# } /* if( ! nogo ) */
g2 = saoa(z + dz * .25, zph, rho, k1, k2, a, b, jh) # saoa(z+dz*.25,g2)
g4 = saoa(z + dz * .75, zph, rho, k1, k2, a, b, jh) # saoa(z+dz*.75,g4)
nogo = 0 # nogo=FALSE;
# % for( i = 0; i < n; i++ )
# % {
# % t02=(t01[i]+dzot*(g2[i]+g4[i]))*.5;
# % t11=(4.*t02-t01[i])/3.;
# % t20[i]=(16.*t11-t10[i])/15.;
# %
# % /* test convergence of 5 point romberg result */
# % test( creal(t11), creal(t20[i]), &tr, cimag(t11), cimag(t20[i]), &ti, 0. );
# % if( (tr > CRIT) || (ti > CRIT) )
# % nogo = TRUE;
# % }
for j in numpy.arange(n):
t02 = (t01[j] + dzot * (g2[j] + g4[j])) * .5
t11 = (4 * t02 - t01[j]) / 3
t20[j] = (16 * t11 - t10[j]) / 15 # TODO: TEST WHY I NOT J
# test convergence of 5 point romberg result
tr, ti = test(numpy.real(t11), numpy.real(t20[j]), numpy.imag(t11), numpy.imag(t20[j]),
0) # TODO: TEST WHY I NOT J
if (tr > CRIT) or (ti > CRIT):
nogo = 1 # nogo = TRUE;
if not nogo: # if( ! nogo )
# for( i = 0; i < n; i++ )
# sum[i] += t20[i];
suminc = suminc + t20
nt += 1 # nt++
z += dz # z += dz
if z > zend:
return suminc
# for( i = 0; i < n; i++ )
# g1[i]=g5[i];
g1 = g5
if (nt >= NTS) and (ns > nx):
ns /= 2
nt = 1
jump = 0 # jump = FALSE;
continue
# end % } /* if( ! nogo ) */
nt = 0
if ns < NM:
ns *= 2 # ns *= 2;
dz = s / ns
dzot = dz * .5
# % for( i = 0; i < n; i++ )
# % {
# % g5[i]=g3[i];
# % g3[i]=g2[i];
# % }
g5 = g3
g3 = g2
jump = 1 # jump = TRUE;
continue
# end % } /* if(ns < nm) */
if not lstep: # if( ! lstep )
lstep = 1 # lstep = TRUE;
t00, t11 = lambd(z, a, b) # lambda( z, &t00, &t11 );
# % for( i = 0; i < n; i++ )
# % sum[i] += t20[i];
suminc = suminc + t20
nt += 1 # nt++
z += dz # z += dz
if z > zend:
return suminc
# % for( i = 0; i < n; i++ )
# % g1[i]=g5[i];
g1 = g5
if (nt >= NTS) and (ns > nx):
ns /= 2 # ns /= 2;
nt = 1
jump = 0 # jump = FALSE;
# end %% } /* while( TRUE ) */
# % saoa computes the integrand for each of the 6 sommerfeld */
# % integrals for source and observer above ground */
# %void saoa( double t, complex double *ans)
def saoa(t, zph, rho, k1, k2, a, b, jh):
# % double xlr, sign;
# % static complex double xl, dxl, cgam1, cgam2, b0, b0p, com, dgam, den1, den2;
pow2 = misc.power_function(2)
pow4 = misc.power_function(4)
pow6 = misc.power_function(6)
tsmag = 100 * k1 * numpy.conj(k1)
cksm = pow2(k2) / (pow2(k1) + pow2(k2)) # cksm=ck2sq/(ck1sq+ck2sq);
ct1 = .5 * (pow2(k1) - pow2(k2)) # ct1=.5*(ck1sq-ck2sq)
# % erv=ck1sq*ck1sq;
# % ezv=ck2sq*ck2sq;
# % ct2=.125*(erv-ezv);
ct2 = .125 * (pow4(k1) - pow4(k2))
# % erv *= ck1sq;
# % ezv *= ck2sq;
# % ct3=.0625*(erv-ezv);
ct3 = .0625 * (pow6(k1) - pow6(k2))
xl, dxl = lambd(t, a, b) # lambda(t, &xl, &dxl);
if jh == 0:
# bessel function form
b0, b0p = ott_funcs.bessel0(xl * rho) # bessel(xl*rho, &b0, &b0p);
b0 *= 2. # b0 *=2.
b0p *= 2. # b0p *=2.
cgam1 = numpy.sqrt(pow2(xl) - pow2(k1)) # cgam1=csqrt(xl*xl-ck1sq)
cgam2 = numpy.sqrt(pow2(xl) - pow2(k2)) # cgam2=csqrt(xl*xl-ck2sq)
if numpy.real(cgam1) == 0: # if(creal(cgam1) == 0.):
cgam1 = numpy.abs(numpy.imag(cgam1)) * 1j # cgam1=cmplx(0.,-fabs(cimag(cgam1)))
if numpy.real(cgam2) == 0: # if(creal(cgam2) == 0.):
cgam2 = numpy.abs(numpy.imag(cgam2)) * 1j # cgam2=cmplx(0.,-fabs(cimag(cgam2)))
else:
# hankel function form
b0, b0p = ott_funcs.hankel0(xl * rho) # hankel(xl*rho, &b0, &b0p);
com = xl - k1 # com=xl-ck1;
cgam1 = numpy.sqrt(xl + k1) * numpy.sqrt(com) # cgam1=csqrt(xl+ck1)*csqrt(com);
if (numpy.real(com) < 0) and (numpy.imag(com) >= 0): # if(creal(com) < 0. && cimag(com) >= 0.)
cgam1 = -cgam1
com = xl - k2 # com=xl-ck2;
cgam2 = numpy.sqrt(xl + k2) * numpy.sqrt(com) # cgam2=csqrt(xl+ck2)*csqrt(com);
if (numpy.real(com) < 0) and (numpy.imag(com) >= 0): # if(creal(com) < 0. && cimag(com) >= 0.)
cgam2 = -cgam2
xlr = xl * numpy.conj(xl)
if xlr >= tsmag:
if numpy.imag(xl) >= 0:
xlr = numpy.real(xl)
if xlr >= k2:
if (xlr <= numpy.realk1): # if(xlr <= ck1r):
dgam = cgam2 - cgam1
else:
sign = 1
dgam = 1 / (pow2(xl)) # dgam=1./(xl*xl)
dgam = sign * ((ct3 * dgam + ct2) * dgam + ct1) / xl
else:
sign = -1
dgam = 1 / pow2(xl) # dgam=1./(xl*xl)
dgam = sign * ((ct3 * dgam + ct2) * dgam + ct1) / xl
# /* if(xlr >= ck2) */
# /* if(cimag(xl) >= 0.) */
else:
sign = 1
dgam = 1 / pow2(xl) # dgam=1./(xl*xl)
dgam = sign * ((ct3 * dgam + ct2) * dgam + ct1) / xl
# % /* if(xlr < tsmag) */
else:
dgam = cgam2 - cgam1
den2 = cksm * dgam / (
cgam2 * (pow2(k1) * cgam2 + pow2(k2) * cgam1)) # den2=cksm*dgam/(cgam2*(ck1sq*cgam2+ck2sq*cgam1))
den1 = 1 / (cgam1 + cgam2) - cksm / cgam2
com = dxl * xl * numpy.exp(-cgam2 * zph)
answer = numpy.zeros([6], dtype=numpy.complex128)
answer[5] = com * b0 * den1 / k1 # ans[5] = com*b0*den1/ck1
com = com * den2 # com *= den2
if rho != 0: # if(rho != 0.)
b0p /= rho
answer[0] = -com * xl * (b0p + b0 * xl) # ans[0]=-com*xl*(b0p+b0*xl)
answer[3] = com * xl * b0p # ans[3]=com*xl*b0p
else:
answer[0] = -com * xl * xl * .5 # ans[0]=-com*xl*xl*.5
answer[3] = answer[0] # ans[3]=ans[0]
answer[1] = com * cgam2 * cgam2 * b0 # ans[1]=com*cgam2*cgam2*b0
answer[2] = -answer[3] * cgam2 * rho # ans[2]=-ans[3]*cgam2*rho
answer[4] = com * b0 # ans[4]=com*b0
return answer
def evlua(zph, rho, k1, k2):
# radiating dipole, k
# receiving dipole, j
# zph = z_j + z_k
# rho = radial coordinate for cylindrical system
# k1 = wave number in slab medium
# k2 = wave number in top medium
# int i, jump;
# static double del, slope, rmis;
# static complex double cp1, cp2, cp3, bk, delta, delta2, sum[6], ans[6];
pow2 = misc.power_function(2)
conj_e = 1
bk = 0
# suminc = zeros(6,1);
answer = numpy.zeros([6])
tkmag = 100 * numpy.abs(k1)
delt = zph
if rho > delt:
delt = rho
if zph >= 2 * rho:
# bessel function form of sommerfeld integrals
jh = 0
a = 0
delt = 1 / delt
if delt > tkmag:
b = .1 * (1 - 1j) * tkmag # b=cmplx(.1*tkmag,-.1*tkmag);
suminc = rom1(6, 2, zph, rho, k1, k2, a, b, jh)
a = b
b = delt * (1 - 1j)
answer = rom1(6, 2, zph, rho, k1, k2, a, b, jh)
# for i = 0; i < 6; i++ )
# sum[i] += ans[i];
# end
suminc = suminc + answer
else:
b = delt * (1 - 1j)
suminc = rom1(6, 2, zph, rho, k1, k2, a, b, jh)
delta = .2 * numpy.pi * delt
answer = gshank(b, delta, answer, 6, suminc, 0, b, b, zph, rho, k1, k2,
jh) # gshank(b,delta,ans,6,sum,0,b,b);
answer[5] = answer[5] * k1 # ans[5] *= k1;
if conj_e:
# conjugate since nec uses exp(+jwt)
erv = numpy.conj(pow2(k1) * answer[2]) # *erv=conj(ck1sq*ans[2]);
ezv = numpy.conj(pow2(k1) * (answer[1] + pow2(k2) * answer[4])) # *ezv=conj(ck1sq*(ans[1]+ck2sq*ans[4]));
erh = numpy.conj(pow2(k2) * (answer[0] + answer[5])) # *erh=conj(ck2sq*(ans[0]+ans[5]));
eph = -numpy.conj(pow2(k2) * (answer[3] + answer[5])) # *eph=-conj(ck2sq*(ans[3]+ans[5]));
else:
# unconjugated
erv = pow2(k1) * answer[2] # *erv=conj(ck1sq*ans[2]);
ezv = pow2(k1) * (answer[1] + pow2(k2) * answer[3]) # *ezv=conj(ck1sq*(ans[1]+ck2sq*ans[4]));
erh = pow2(k2) * (answer[0] + answer[5]) # *erh=conj(ck2sq*(ans[0]+ans[5]));
eph = -pow2(k2) * (answer[3] + answer[5]) # *eph=-conj(ck2sq*(ans[3]+ans[5]));
return erv, ezv, erh, eph
# # } /* if(zph >= 2.*rho) */
else:
# hankel function form of sommerfeld integrals
jh = 1
cp1 = .4 * k2 * 1j # cp1=cmplx(0.0,.4*ck2);
cp2 = .6 * k2 - .2 * k2 * 1j # cp2=cmplx(.6*ck2,-.2*ck2);
cp3 = 1.02 * k2 - .2 * k2 * 1j # cp3=cmplx(1.02*ck2,-.2*ck2);
a = cp1
b = cp2
suminc = rom1(6, 2, zph, rho, k1, k2, a, b, jh)
a = cp2
b = cp3
answer = rom1(6, 2, zph, rho, k1, k2, a, b, jh)
# for( i = 0; i < 6; i++ )
# sum[i]=-(sum[i]+ans[i]);
suminc = -(suminc + answer)
# path from imaginary axis to -infinity
if zph > .001 * rho:
slope = rho / zph
else:
slope = 1000
delt = .2 * numpy.pi / delt
delta = (-1 + slope * 1j) * delt / numpy.sqrt(1 + pow2(slope))
delta2 = -numpy.conj(delta)
answer = gshank(cp1, delta, answer, 6, suminc, 0, bk, bk, zph, rho, k1, k2,
jh) # gshank(cp1,delta,ans,6,sum,0,bk,bk);
rmis = rho * (numpy.real(k1) - k2)
jump = 0; # jump = FALSE;
if (rmis >= 2 * k2) and (rho >= 1E-10):
if (zph >= 1E-10):
bk = (-zph + rho * 1j) * (k1 - cp3) # bk=cmplx(-zph,rho)*(ck1-cp3);
rmis = -numpy.real(bk) / numpy.abs(numpy.imag(bk)) # rmis=-creal(bk)/fabs(cimag(bk));
if (rmis > 4 * rho / zph):
jump = 1 # jump = TRUE;
if not jump: # if( ! jump )
# integrate up between branch cuts, then to + infinity
cp1 = k1 - (.1 + .2 * 1j) # cp1=ck1-(.1+.2fj);
cp2 = cp1 + .2
bk = delt * 1j # bk=cmplx(0.,del);
suminc = gshank(cp1, bk, suminc, 6, answer, 0, bk, bk, zph, rho, k1, k2,
jh) # gshank(cp1,bk,sum,6,ans,0,bk,bk);
a = cp1
b = cp2
answer = rom1(6, 1, zph, rho, k1, k2, a, b, jh)
# for( i = 0; i < 6; i++ )
# ans[i] -= sum[i];
answer = answer - suminc
suminc = gshank(cp3, bk, suminc, 6, answer, 0, bk, bk, zph, rho, k1, k2,
jh) # gshank(cp3,bk,sum,6,ans,0,bk,bk);
answer = gshank(cp2, delta2, answer, 6, suminc, 0, bk, bk, zph, rho, k1, k2,
jh) # gshank(cp2,delta2,ans,6,sum,0,bk,bk);
jump = 1 # jump = TRUE;
# /* if( (rmis >= 2.*ck2) || (rho >= 1.e-10) ) */
else:
jump = 0 # jump = FALSE;
if not jump: # ( ! jump )
##{
# integrate below branch points, then to + infinity
# for( i = 0; i < 6; i++ )
# sum[i]=-ans[i];
suminc = -answer
rmis = numpy.real(k1) * 1.01 # rmis=creal(ck1)*1.01;
# if( (ck2+1.) > rmis )
# rmis=ck2+1.;
if (k2 + 1) > rmis:
rmis = k2 + 1
bk = rmis + .99 * numpy.imag(k1) * 1j # bk=cmplx(rmis,.99*cimag(ck1));
delta = bk - cp3
delta = delta * delt / numpy.abs(delta) # delta *= del/cabs(delta);
answer = gshank(cp3, delta, answer, 6, suminc, 1, bk, delta2, zph, rho, k1, k2,
jh) # gshank(cp3,delta,ans,6,sum,1,bk,delta2);
# /* if( ! jump ) */
answer[5] = answer[5] * k1 # ans[5] *= ck1;
if conj_e:
# conjugate since nec uses exp(+jwt)
erv = numpy.conj(pow2(k1) * answer[2]) # *erv=conj(ck1sq*ans[2]);
ezv = numpy.conj(pow2(k1) * (answer[1] + pow2(k2) * answer[4])) # *ezv=conj(ck1sq*(ans[1]+ck2sq*ans[4]));
erh = numpy.conj(pow2(k2) * (answer[0] + answer[5])) # *erh=conj(ck2sq*(ans[0]+ans[5]));
eph = -numpy.conj(pow2(k2) * (answer[3] + answer[5])) # *eph=-conj(ck2sq*(ans[3]+ans[5]));
else:
# unconjugated
erv = pow2(k1) * answer[2]
ezv = pow2(k1) * (answer[1] + pow2(k2) * answer[4])
erh = pow2(k2) * (answer[0] + answer[5])
eph = -pow2(k2) * (answer[3] + answer[5])
return erv, ezv, erh, eph
def precalc_Somm(r, k1, k2, use_mex=False):
# r: dipole coordinates
# k1: wave number in substrate
# k2: wave number in upper medium, e.g., air, water etc.
pow2 = misc.power_function(2)
# global use_mex
N = r.shape[0]
zr = numpy.zeros([N * N, 2])
ix = 0
for j in numpy.arange(N):
# sprintf('precalc zph rho. %d of %d',j,N)
for k in numpy.arange(N):
r_j = r[j, :]
r_k = r[k, :]
zph = r_j[2] + r_k[2]
rho = numpy.sqrt(pow2(r_j[0] - r_k[0]) + pow2(r_j[1] - r_k[1]))
# round to 4 decimal places
# zph = round2(zph,.0001);
# rho = round2(rho,.0001);
zr[ix, :] = numpy.asarray([zph, rho]) # TODO: Get rid of asarray
ix += 1
zr0 = zr
#zr, m, n = numpy.unique(zr, return_index=True, return_inverse=True)
zr, m, n = misc.unique_rows(zr, return_index=True, return_inverse=True)
L = zr.shape[0]
S = numpy.zeros([L, 4], dtype=numpy.complex128)
for j in numpy.arange(L):
# sprintf('precalc S. %d of %d',j,L)
if use_mex:
raise Exception("Some unknown function")
# I = somm(numpy.real(k1), numpy.imag(k1),k2,zr[j,1],zr[j,2])
# IV_rho = I[1] + 1j*I[2]
# IV_z = I[3] + 1j*I[4]
# IH_rho = I[5] + 1j*I[6]
# IH_phi = I[7] + 1j*I[8]
else:
IV_rho, IV_z, IH_rho, IH_phi = evlua(zph, rho, k1, k2)
S[j, :] = [IV_rho, IV_z, IH_rho, IH_phi]
return S, n
# void test( double f1r, double f2r, double *tr,
# double f1i, double f2i, double *ti, double dmin )
def test(f1r, f2r, f1i, f2i, dmin):
den = numpy.abs(f2r)
tr = numpy.abs(f2i)
if den < tr:
den = tr
if den < dmin:
den = dmin
if den < 1E-37:
tr = 0
ti = 0
return tr, ti
tr = numpy.abs((f1r - f2r) / den)
ti = numpy.abs((f1i - f2i) / den)
return tr, ti
# void lambda( double t, complex double *xlam, complex double *dxlam )
# {
# *dxlam=b-a;
# *xlam=a+*dxlam*t;
# return;
# }
def lambd(t, a, b):
# a = start of integration interval
# b = ed of integration interval
dxlam = b - a
xlam = a + dxlam * t
return xlam, dxlam