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Commit f65ab66f authored by Andreas Theodosiou's avatar Andreas Theodosiou :penguin:
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Merge branch 'develop' into 'master' 

Bump to version 0.4

See merge request !20
parents 733a63bf fe75bb7e
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Tags v0.4
1 merge request!20Bump to version 0.4
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drama/geo/derived_geo.py
+ 219
− 41
View file @ f65ab66f
import numpy as np
import scipy.interpolate as interpolate
import scipy.constants
from drama.geo import geometry as geom
from drama.geo.swath_geo import SingleSwath
class BistaticRadarGeometry(object):
"""This class calculates useful geometric relations.
"""
This class calculates useful geometric relations.
Parameters
----------
orbit_height :
orbit_height : float
orbit height above surface
r_planet :
r_planet : float
radious of planet, default's to Earth's
gm_planet :
gm_planet : float
mass of planet, default's to Earths
degrees :
degrees : bool
if set, everything is in degrees, defaults to False.
Returns
-------
"""
def __init__(self, par_file, companion_delay=None):
self.swth_t = SingleSwath(par_file=par_file)
......@@ -67,6 +65,11 @@ class BistaticRadarGeometry(object):
self.v_r[..., 0] = np.sum(self.swth_r.v_ecef.reshape(ashp) * self.swth_t.local_x, axis=-1)
self.v_r[..., 1] = np.sum(self.swth_r.v_ecef.reshape(ashp) * self.swth_t.local_y, axis=-1)
self.v_r[..., 2] = np.sum(self.swth_r.v_ecef.reshape(ashp) * self.swth_t.local_z, axis=-1)
# Now an additional line of sight for an antenna separated by a certain Baseline
r_r2 = self.r_r + self.antaxes_local[...,1] # this adds baseline along antenna axis_
r_r2_n = np.linalg.norm(r_r2, axis=2)
self.r_v_r2 = r_r2 / r_r2_n[:,:, np.newaxis]
# Magnitude (norm) of r_t and r_r
self.r_n_t = np.linalg.norm(self.r_t, axis=2)
self.r_n_r = np.linalg.norm(self.r_r, axis=2)
......@@ -105,16 +108,6 @@ class BistaticRadarGeometry(object):
self.set_lat(lat)
def set_lat(self, lat):
"""
Parameters
----------
lat :
Returns
-------
"""
self._lat = lat
mid_range = int(self.swth_t.lats.shape[1] / 2)
lats = self.swth_t.lats
......@@ -466,21 +459,30 @@ class BistaticRadarGeometry(object):
return np.stack([grad_x, grad_y], axis=-1)
def train_off_track_displacement(self, inc, dotr_s=1, ascending=True):
""" Calculates displacement of target in SAR image due to a motion induced
derivative of the bistatic range
"""
Calculates displacement of target in SAR image due to a motion induced
derivative of the bistatic range.
Parameters
----------
inc :
incident angle, in radians
dotr_s:
time derivative of bistatic range due to target motion
ascending :
(Default value = True)
inc : float | np.ndarray
Incident angle, in radians.
dotr_s: float
Time derivative of bistatic range due to target motion.
ascending : bool
If true, ascending orbit, else descending (Default value = True).
Returns
-------
tuple
Tuple containing the temporal offset, the offset in the azimuth
(cross-track) direction, and a tuple containing parameters related
to the derivatives. The latter contains three variables: the ratio
of the first derivative of the bistatic range wrt to the azimuth
distance to the second derivative, the derivate of the bistatic
range wrt to time, the 2nd derivate of the bistatic range wrt to and
an alternative expression for the temporal offset.
time
"""
# azimuth (time) shift
c1 = self.inc2sgrad_r_b(inc, ascending=ascending)[:, 0] / self.inc2sgrad_dot_r_b(inc, ascending=ascending)[:, 0]
......@@ -498,8 +500,8 @@ class BistaticRadarGeometry(object):
def k_ground(self, df, dta, f0=None, ascending=True):
if f0 is None:
f0 = self.conf.sar.f0
k0 = 2 * np.pi * f0 / 3e8
dk = df * 2 * np.pi / 3e8
k0 = 2 * np.pi * f0 / scipy.constants.c
dk = df * 2 * np.pi / scipy.constants.c
if ascending:
orbind = self.__asc_latind
else:
......@@ -508,13 +510,165 @@ class BistaticRadarGeometry(object):
v_r = self.v_r[orbind]
r_i = self.r_v_t[orbind]
r_s = self.r_v_r[orbind]
dr_i = (np.sum(r_i * v_t, axis=-1)[..., np.newaxis] * r_i - v_t) / bsgeo.r_n_t[orbind, ...,np.newaxis]
dr_s = (np.sum(r_s * v_r, axis=-1)[..., np.newaxis] * r_s - v_r) / bsgeo.r_n_r[orbind, ...,np.newaxis]
dr_i = (np.sum(r_i * v_t, axis=-1)[..., np.newaxis] * r_i - v_t) / self.r_n_t[orbind, ...,np.newaxis]
dr_s = (np.sum(r_s * v_r, axis=-1)[..., np.newaxis] * r_s - v_r) / self.r_n_r[orbind, ...,np.newaxis]
kv = (k0 + dk) * (r_i + r_s) + k0 * (dr_i + dr_s) * dta
return kv
def dk_ground_dt(self, f0=None, ascending=True):
"""
Derivative of bistatic wavenumber vector at the ground w.r.t. azimuth time.
Parameters
----------
f0 : float
Carrier frequency, defaults to value in conf file passed to initialize function.
ascending : bool
True for ascending.
Returns
-------
np.ndarray
The derivative w.r.t azimuth time.
"""
if f0 is None:
f0 = self.conf.sar.f0
k0 = 2 * np.pi * f0 / scipy.constants.c
if ascending:
orbind = self.__asc_latind
else:
orbind = self.__dsc_latind
v_t = self.v_t[orbind]
v_r = self.v_r[orbind]
r_i = self.r_v_t[orbind]
r_s = self.r_v_r[orbind]
dr_i = (np.sum(r_i * v_t, axis=-1)[..., np.newaxis] * r_i - v_t) / self.r_n_t[orbind, ...,np.newaxis]
dr_s = (np.sum(r_s * v_r, axis=-1)[..., np.newaxis] * r_s - v_r) / self.r_n_r[orbind, ...,np.newaxis]
dkvdt = k0 * (dr_i + dr_s)
return dkvdt
def dk_ground_df(self, ascending=True):
"""
Derivative of bistatic wavenumber vector at the ground w.r.t. frequency.
Parameters
----------
ascending : bool
True for ascending.
Returns
-------
np.ndarray
The derivative w.r.t frequency.
"""
if ascending:
orbind = self.__asc_latind
else:
orbind = self.__dsc_latind
r_i = self.r_v_t[orbind]
r_s = self.r_v_r[orbind]
dkvdf = 2 * np.pi / scipy.constants.c * (r_i + r_s)
return dkvdf
def dk_ground_dbati(self, f0=None, ascending=True):
"""
Derivative of bistatic wavenumber vector at the ground w.r.t. baseline
(or along-track position on receive antenna).
Parameters
----------
f0 : float
Carrier frequency, defaults to value in conf file passed to initialize function.
ascending : bool
True for ascending.
Returns
-------
np.ndarray
The derivative w.r.t the baseline.
"""
if f0 is None:
f0 = self.conf.sar.f0
k0 = 2 * np.pi * f0 / scipy.constants.c
if ascending:
orbind = self.__asc_latind
else:
orbind = self.__dsc_latind
#v_t = self.v_t[orbind]
#v_r = self.v_r[orbind]
#r_i = self.r_v_t[orbind]
r_s = self.r_v_r[orbind]
r_s2 = self.r_v_r2[orbind]
#dr_i = (np.sum(r_i * v_t, axis=-1)[..., np.newaxis] * r_i - v_t) / self.r_n_t[orbind, ...,np.newaxis]
#dr_s = (np.sum(r_s * v_r, axis=-1)[..., np.newaxis] * r_s - v_r) / self.r_n_r[orbind, ...,np.newaxis]
#dr_s2 = (np.sum(r_s2 * v_r, axis=-1)[..., np.newaxis] * r_s - v_r) / self.r_n_r[orbind, ...,np.newaxis]
dkvdbati = k0 * (r_s2 - r_s)
return dkvdbati
def bati2insarpar(self, inc, f0=None, ascending=True):
"""
Computes short-baseline InSAR paramters for a 1 m baseline along antenna
axis.
Parameters
----------
inc: float, np.ndarray
angle of incidence of incident wave, in radians
f0 : float
Carrier frequency, defaults to value in conf file passed to initialize function.
ascending : bool
True for ascending.
Returns
-------
dict
A dictionary with:
'dfdb': The frequency (spectral) shift, in Hz, per 1 m baseline
'dtdb': The ati lag per 1 m baseline
'dkzdb': The delta kz (i.e. 2\pi/h_amb) per 1 m baseline
'dkzdb_rar': The delta kz for the real-aperture interferometer,
i.e. without coregistration, which only applies if also no SAR
processing is done.
"""
if ascending:
orbind = self.__asc_latind
else:
orbind = self.__dsc_latind
dkdt = self.dk_ground_dt(f0=f0, ascending=ascending)
dkdf = self.dk_ground_df(ascending=ascending)
dkdbati = self.dk_ground_dbati(f0=f0, ascending=ascending)
A = np.zeros((dkdt.shape[0],2,2))
A[:, :, 0] = dkdf[:,0:2]
A[:, :, 1] = dkdt[:,0:2]
invA = np.linalg.inv(A)
b = - dkdbati[:, 0:2]
df_dt = np.einsum("...ij,...j->...i", invA, b)
# dkz of second antenna after alignment
dkz = dkdbati[:,2] + dkdt[:, 2] * df_dt[:,1] + dkdf[:, 2] * df_dt[:,0]
inc_m = self.swth_t.master_inc[orbind, :]
inc2dfdb = interpolate.interp1d(inc_m, df_dt[:,0],
"quadratic",
bounds_error=False,
fill_value=np.NaN)
inc2dtdb = interpolate.interp1d(inc_m, df_dt[:,1],
"quadratic",
bounds_error=False,
fill_value=np.NaN)
inc2dkzdb = interpolate.interp1d(inc_m, dkz,
"quadratic",
bounds_error=False,
fill_value=np.NaN)
inc2dkz0db = interpolate.interp1d(inc_m, dkdbati[:,2],
"quadratic",
bounds_error=False,
fill_value=np.NaN)
return {"dfdb": inc2dfdb(inc),
"dtdb": inc2dtdb(inc),
"dkzdb":inc2dkzdb(inc),
"dkzdb_rar":inc2dkz0db(inc)}
def inc2specsup(self, inc, mode='IWS', ascending=True, f0=None):
"""Short summary.
"""Calculate the spectral support from the incidence angle.
Parameters
----------
......@@ -523,7 +677,7 @@ class BistaticRadarGeometry(object):
mode : string
'IWS' (default).
ascending : bool
Self-explainatory.
True for ascending orbit, False for descending.
f0 : float
carrier frequency to superseed value read from config file.
......@@ -531,7 +685,6 @@ class BistaticRadarGeometry(object):
-------
dictionary
Corners of spectral support region and other goodies.
"""
if ascending:
orbind = self.__asc_latind
......@@ -549,7 +702,7 @@ class BistaticRadarGeometry(object):
sw = swath[0]
proc_bw = self.conf.IWS.proc_bw[sw]
pulse_bw = self.conf.IWS.pulse_bw[sw]
dta =proc_bw/(self.inc2ddot_r_b((inc))/(3e8/f0))
dta =proc_bw/(self.inc2ddot_r_b((inc))/(scipy.constants.c/f0))
v11 = self.k_ground(-pulse_bw/2, -dta/2, f0=f0, ascending=ascending)[inc_ind]
v21 = self.k_ground(pulse_bw/2, -dta/2, f0=f0, ascending=ascending)[inc_ind]
v12 = self.k_ground(-pulse_bw/2, dta/2, f0=f0, ascending=ascending)[inc_ind]
......@@ -562,7 +715,9 @@ class BistaticRadarGeometry(object):
def spectral_mask(self, inc, daz, mode='IWS', ascending=True, f0=None, drg=None,
baseband=False, Nx=128, Ny=128):
"""Short summary.
"""
Find the positions of the spectral support region for a set of incidence
angles and return the corresponding mask.
Parameters
----------
......@@ -590,9 +745,7 @@ class BistaticRadarGeometry(object):
-------
dictionary
Spectral support mask and kx and ky vectors.
"""
#from matplotlib.collections import PatchCollection
from matplotlib.path import Path
support = self.inc2specsup(inc, mode=mode, ascending=ascending, f0=f0)
verts = np.zeros((4 , 2))
......@@ -602,7 +755,7 @@ class BistaticRadarGeometry(object):
verts[3,:] = support['specsup'][2][0:2]
if drg is None:
drg = 3e8/2/support['pbw']/1.1/np.sin(support['inc'])
drg = scipy.constants.c/2/support['pbw']/1.1/np.sin(support['inc'])
if baseband:
kx = 2*np.pi * np.fft.fftshift(np.fft.fftfreq(256, drg))
ky = 2*np.pi * np.fft.fftshift(np.fft.fftfreq(256, daz))
......@@ -613,7 +766,7 @@ class BistaticRadarGeometry(object):
ky = 2*np.pi * np.fft.fftshift(np.fft.fftfreq(Ny, daz)) + support['center'][1]
kkx, kky = np.meshgrid(kx,ky)
poly_path=Path(verts)
mask = 1.0* poly_path.contains_points(np.stack((kkx.flatten(),kky.flatten()), axis=-1)).reshape(kkx.shape)
mask = 1.0 * poly_path.contains_points(np.stack((kkx.flatten(),kky.flatten()), axis=-1)).reshape(kkx.shape)
for amb in [-2,-1,1,2]:
mask_a = poly_path.contains_points(np.stack((kkx.flatten(),kky.flatten() + amb * 2*np.pi/daz), axis=-1)).reshape(kkx.shape)
mask = mask + 1.0 * mask_a
......@@ -682,3 +835,28 @@ if __name__ == '__main__':
plt.figure()
plt.imshow(np.fft.fftshift(np.real(np.fft.ifft2(np.fft.fft2(specmask["mask"])**2))), origin='lower')
plt.colorbar()
#%%
print(bsgeo.antaxes_sat[1000])
# print(bsgeo.antaxes_sat[3000])
print(bsgeo.antaxes_local[1500,200])
plt.figure()
plt.plot(bsgeo.antaxes_sat[:,0,1],label='x')
plt.plot(bsgeo.antaxes_sat[:,1,1],label='y')
plt.plot(bsgeo.antaxes_sat[:,2,1],label='z')
plt.legend()
plt.figure()
plt.plot(bsgeo.antaxes_local[3000,:,0,1],label='x')
plt.plot(bsgeo.antaxes_local[3000,:,1,1],label='y')
plt.plot(bsgeo.antaxes_local[3000,:,2,1],label='z')
plt.legend()
bsgeo.r_r.shape
#%%
inc = np.linspace(30,45)
atipar = bsgeo.bati2insarpar(np.radians(inc))
plt.figure()
plt.plot(inc,atipar["dtdb"]*9)
plt.figure()
plt.plot(inc,atipar["dfdb"]*9)
plt.figure()
plt.plot(inc, 2*np.pi/atipar["dkzdb"]/9)
plt.plot(inc, 2*np.pi/atipar["dkzdb_rar"]/9,"--")
setup.cfg
+ 1
− 1
View file @ f65ab66f
[metadata]
name = drama
version = 0.3
version = 0.4
author = Paco López-Dekker
author_email = F.LopezDekker@tudelft.nl
description = Delft Radar Modelling and perfornance Analysis (DRaMA)
......
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