예제 #1
0
amp = 71
ang_mode = np.pi * 0.
mod = (1. - np.cos(ang_mode)) / 2.
print mod
#mod = 0.2
a = (amp - 2) * mod + 1
b = amp * (1 - mod) + 2 * mod - 1
nphi = 201
phi = np.linspace(0., 2. * np.pi, nphi)
#angmom = ort.angmom_fixed(ang_mode, phi)
angmom = ort.angmom_beta_phi(a, b, phi)

#print angmom

# calculate radar variables
alpha_cov = ort.avg_polcov(angmom, alpha_a, alpha_c)
avar_hh = alpha_cov[0]
avar_vv = alpha_cov[1]
avar_hv = alpha_cov[2]
acov_hh_vv = alpha_cov[3]
acov_hh_hv = alpha_cov[4]
acov_vv_hv = alpha_cov[5]
adp = alpha_cov[6]
zdr, ldr, kdp, rhohv, zh, rhoxh = ort.radar(wavl, avar_hh, avar_vv, avar_hv,
                                            acov_hh_vv, acov_hh_hv, acov_vv_hv,
                                            adp)

# compare to simultaneous tr
psi_dp = 0.5 * np.pi
svar_h, svar_v, scov_hv = ort.cov_sim(alpha_cov, psi_dp)
zdr_str, ldrj, kdpj, rhohv_str, zh_str, rhoxhj = ort.radar(
예제 #2
0
# compare to those with spherical inclusions
eps_mix = maxwell_garnett(eps_ice, vfrac_inc)
alpha_a_sp, alpha_a_sp, alpha_c_sp = sp.oblate_polz(eps_mix, dmax / 2.,
                                                    thick / 2.)

# set orientation distribution
amp = 18.
mod = 0.
a = (amp - 2) * mod + 1
b = amp * (1 - mod) + 2 * mod - 1

angmom = ort.angmom_beta(a, b)

# calculate radar variables
alp_cov_arr = ort.avg_polcov(angmom, alpha_a, alpha_c)
alp_cov_arr_sp = ort.avg_polcov(angmom, alpha_a_sp, alpha_c_sp)
zdr, ldr, kdp, rhohv, zh, rhoxh = ort.radar(wavl, alp_cov_arr)
zdr_sp, ldr_sp, kdp_sp, rhohv_sp, zh_sp, rhoxh = ort.radar(
    wavl, alp_cov_arr_sp)
#print zdr, ldr, kdp, rhohv, zh

# plot radar variables
fig = plt.figure(1)
ax = fig.add_subplot(2, 2, 1)
plt.plot(vfrac_inc, zdr, 'r-', lw=3.)
plt.plot(vfrac_inc, zdr_sp, 'b-', lw=3.)
#ax.set_ylim([0., 1.])
ax.set_xlim([0.05, 1.])

ax = fig.add_subplot(2, 2, 2)
예제 #3
0
w2 = 1. - w1

#a = 7.
#b = 7.
sig_deg = 180. * np.sqrt(2. / (b1 - 1.)) / np.pi
#sig_deg = 35.
print sig_deg
angmom1 = ort.angmom_beta(a1, b1)
angmom2 = ort.angmom_beta(a2, b2)
angmom = (w1 * np.array(angmom1) + w2 * np.array(angmom2))
angmom_g = ort.angmom_gauss(sig_deg)
print angmom_g
print angmom1

# calculate radar variables
avar_hh, avar_vv, avar_hv, acov_hh_vv, adp = ort.avg_polcov(
    angmom, alpha_a, alpha_c)
zdr, ldr, kdp, rhohv, zh = ort.radar(wavl, avar_hh, avar_vv, avar_hv,
                                     acov_hh_vv, adp)
print zdr, ldr, kdp, rhohv, zh

avar_hh, avar_vv, avar_hv, acov_hh_vv, adp = ort.avg_polcov(
    angmom_g, alpha_a, alpha_c)
zdr, ldr, kdp, rhohv, zh = ort.radar(wavl, avar_hh, avar_vv, avar_hv,
                                     acov_hh_vv, adp)
print zdr, ldr, kdp, rhohv, zh

# plot beta distribution
x = (1. - np.cos(np.linspace(fc(0.), fc(1.), 201))) / 2.
ang = np.arccos(1. - 2. * x) * 180. / np.pi
beta_av = (w1 * ort.beta_dist(x, a1, b1) + w2 * ort.beta_dist(x, a2, b2))
#plt.plot(x, beta_av, 'r--', lw=3.)
sigh_agg = np.log10(sigh_agg)
sigv_agg = np.log10(sigv_agg)
#print sigh_agg, zdr_agg, kdp_agg

# compare to isolated pristine crystals
#aobl_a, aobl_a, aobl_c = sp.oblate_polz(eps_ice, asp_inc/2., 1./2.)
aprl_c, aprl_a, aprl_a = sp.prolate_polz(eps_ice, 1. / 2., asp_inc / 2.)
vol_sph = np.pi / 6. * asp_inc**2.
#aobl_a = aobl_a/vol_sph
#aobl_c = aobl_c/vol_sph
aprl_a = aprl_a / vol_sph
aprl_c = aprl_c / vol_sph

angmom_pr = ort.angmom_beta(a_inc, b_inc)
#acov_arr = ort.avg_polcov(angmom_pr, aobl_a, aobl_c)
acov_arr = ort.avg_polcov(angmom_pr, aprl_a, aprl_c)
zdr, ldr, kdp, rhohv, zhh, rhoxh = ort.radar(wavl, acov_arr)
sigh = np.log10(k**2. * acov_arr[0])
sigv = np.log10(k**2. * acov_arr[1])

# plot radar variables
fig = plt.figure(1)
ax = fig.add_subplot(2, 2, 1)
plt.plot(vfrac_inc, zdr * vfrac_inc / vfrac_inc, 'r-', lw=3.)
plt.plot(vfrac_inc, zdr_agg, 'b-', lw=3.)
#ax.set_ylim([0., 1.])
#ax.set_xlim([0.05, 1.])

ax = fig.add_subplot(2, 2, 2)
plt.plot(vfrac_inc, np.log10(kdp) * vfrac_inc / vfrac_inc, 'r-', lw=3.)
plt.plot(vfrac_inc, np.log10(kdp_agg), 'b-', lw=3.)