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csst-sims
csst_mci_sim
Commits
9928a062
Commit
9928a062
authored
Oct 25, 2024
by
Yan Zhaojun
Browse files
Delete earthshine.py
parent
580aee74
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1
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csst_mci_sim/earthshine.py
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580aee74
import
numpy
as
np
import
julian
from
datetime
import
datetime
from
astropy.time
import
Time
from
astropy.coordinates
import
get_sun
from
astropy.coordinates
import
SkyCoord
import
astropy.coordinates
as
coord
import
pandas
as
pd
from
astropy
import
units
as
u
from
scipy.interpolate
import
interp1d
from
scipy
import
interpolate
import
ctypes
def
transRaDec2D
(
ra
,
dec
):
# radec转为竞天程序里的ob, 赤道坐标系下的笛卡尔三维坐标xyz.
x1
=
np
.
cos
(
dec
/
57.2957795
)
*
np
.
cos
(
ra
/
57.2957795
)
y1
=
np
.
cos
(
dec
/
57.2957795
)
*
np
.
sin
(
ra
/
57.2957795
)
z1
=
np
.
sin
(
dec
/
57.2957795
)
return
np
.
array
([
x1
,
y1
,
z1
])
def
earth_angle
(
time_jd
,
x_sat
,
y_sat
,
z_sat
,
ra_obj
,
dec_obj
):
ra_sat
=
np
.
arctan2
(
y_sat
,
x_sat
)
/
np
.
pi
*
180
dec_sat
=
np
.
arctan2
(
z_sat
,
np
.
sqrt
(
x_sat
**
2
+
y_sat
**
2
))
/
np
.
pi
*
180
radec_sat
=
SkyCoord
(
ra
=
ra_sat
*
u
.
degree
,
dec
=
dec_sat
*
u
.
degree
,
frame
=
'gcrs'
)
lb_sat
=
radec_sat
.
transform_to
(
'geocentrictrueecliptic'
)
# get the obj location
radec_obj
=
SkyCoord
(
ra
=
ra_obj
*
u
.
degree
,
dec
=
dec_obj
*
u
.
degree
,
frame
=
'gcrs'
)
lb_obj
=
radec_obj
.
transform_to
(
'geocentrictrueecliptic'
)
# calculate the angle between sub-satellite point and the earth side
earth_radius
=
6371
# km
sat_height
=
np
.
sqrt
(
x_sat
**
2
+
y_sat
**
2
+
z_sat
**
2
)
angle_a
=
np
.
arcsin
(
earth_radius
/
sat_height
)
/
np
.
pi
*
180
# calculate the angle between satellite position and the target position
angle_b
=
lb_sat
.
separation
(
lb_obj
)
# calculat the earth angle
angle
=
180
-
angle_a
-
angle_b
.
degree
return
angle
###############################################################################
def
ill2flux
(
E
,
path
):
# use template from sky_bkg (background_spec_hst.dat)
filename
=
path
+
'MCI_inputData/refs/background_spec_hst.dat'
cat_spec
=
pd
.
read_csv
(
filename
,
sep
=
'\s+'
,
header
=
None
,
comment
=
'#'
)
wave0
=
cat_spec
[
0
].
values
# A
spec0
=
cat_spec
[
2
].
values
# erg/s/cm^2/A/arcsec^2
# convert erg/s/cm^2/A/arcsec^2 to erg/s/cm^2/A/sr
flux1
=
spec0
/
(
1
/
4.25452e10
)
# convert erg/s/cm^2/A/sr to W/m^2/sr/um
flux2
=
flux1
*
10
# 对接收面积积分,输出单位 W/m^2/nm
D
=
2
# meter
f
=
28
# meter, 焦距,转换关系来源于王维notes.
flux3
=
flux2
*
np
.
pi
*
D
**
2
/
4
/
f
**
2
/
10
**
3
f
=
interp1d
(
wave0
,
flux3
)
wave_range
=
np
.
arange
(
3800
,
7800
)
flux3_mean
=
f
(
wave_range
)
delta_lamba
=
0.1
# nm
E0
=
np
.
sum
(
flux3_mean
*
delta_lamba
)
factor
=
E
/
E0
spec_scaled
=
factor
*
spec0
return
wave0
,
spec_scaled
##############################################################
def
earthshine
(
path
,
time_jd
,
x_sat
,
y_sat
,
z_sat
,
ra
,
dec
):
# EarthShine from straylight
sl
=
StrayLight
(
path
,
jtime
=
time_jd
,
sat
=
np
.
array
(
[
x_sat
,
y_sat
,
z_sat
]),
radec
=
np
.
array
([(
ra
*
u
.
degree
).
value
,
(
dec
*
u
.
degree
).
value
]))
earth_e
=
sl
.
caculateEarthShineFilter
(
filter
=
'r'
)
angle_earth
=
earth_angle
(
time_jd
,
x_sat
,
y_sat
,
z_sat
,
ra
,
dec
)
if
angle_earth
<
0
:
earth_e
=
0
earthshine_wave0
,
earthshine_flux0
=
ill2flux
(
earth_e
,
path
)
# sample as mci wavelength
wave_mci
=
np
.
linspace
(
2500
,
11000
,
8501
)
# np.arange(2500, 11000, 1)
f2
=
interp1d
(
earthshine_wave0
,
earthshine_flux0
)
earthshine
=
f2
(
wave_mci
)
return
earthshine
#################################################################
class
StrayLight
(
object
):
def
__init__
(
self
,
path
,
jtime
=
2460843.
,
sat
=
np
.
array
([
0
,
0
,
0
]),
radec
=
np
.
array
([
0
,
0
])):
self
.
path
=
path
self
.
jtime
=
jtime
self
.
sat
=
sat
self
.
equator
=
coord
.
SkyCoord
(
radec
[
0
]
*
u
.
degree
,
radec
[
1
]
*
u
.
degree
,
frame
=
'icrs'
)
self
.
ecliptic
=
self
.
equator
.
transform_to
(
'barycentrictrueecliptic'
)
self
.
pointing
=
transRaDec2D
(
radec
[
0
],
radec
[
1
])
self
.
slcdll
=
ctypes
.
CDLL
(
self
.
path
+
'MCI_inputData/refs/libstraylight.so'
)
# dylib
self
.
slcdll
.
Calculate
.
argtypes
=
[
ctypes
.
c_double
,
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
c_char_p
]
self
.
slcdll
.
PointSource
.
argtypes
=
[
ctypes
.
c_double
,
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
c_char_p
]
self
.
slcdll
.
EarthShine
.
argtypes
=
[
ctypes
.
c_double
,
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
POINTER
(
ctypes
.
c_double
)]
self
.
slcdll
.
Zodiacal
.
argtypes
=
[
ctypes
.
c_double
,
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
POINTER
(
ctypes
.
c_double
)]
self
.
slcdll
.
ComposeY
.
argtypes
=
[
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
POINTER
(
ctypes
.
c_double
),
ctypes
.
POINTER
(
ctypes
.
c_double
)]
self
.
slcdll
.
Init
.
argtypes
=
[
ctypes
.
c_char_p
,
ctypes
.
c_char_p
,
ctypes
.
c_char_p
,
ctypes
.
c_char_p
]
self
.
deFn
=
self
.
path
+
"MCI_inputData/refs/DE405"
self
.
PSTFn
=
self
.
path
+
"MCI_inputData/refs/PST"
self
.
RFn
=
self
.
path
+
"MCI_inputData/refs/R"
self
.
ZolFn
=
self
.
path
+
"MCI_inputData/refs/Zodiacal"
self
.
brightStarTabFn
=
self
.
path
+
"MCI_inputData/refs/BrightGaia_with_csst_mag"
self
.
slcdll
.
Init
(
str
.
encode
(
self
.
deFn
),
str
.
encode
(
self
.
PSTFn
),
str
.
encode
(
self
.
RFn
),
str
.
encode
(
self
.
ZolFn
))
# def caculateStarLightFilter(self, filter='i'):
# filterIndex = {'nuv': 0, 'u': 1, 'g': 2,
# 'r': 3, 'i': 4, 'z': 5, 'y': 6}
# sat = (ctypes.c_double*3)()
# sat[:] = self.sat
# ob = (ctypes.c_double*3)()
# ob[:] = self.pointing
# py1 = (ctypes.c_double*3)()
# py2 = (ctypes.c_double*3)()
# self.slcdll.ComposeY(ob, py1, py2)
# star_e1 = (ctypes.c_double*7)()
# self.slcdll.PointSource(self.jtime, sat, ob, py1,
# star_e1, str.encode(self.brightStarTabFn))
# star_e2 = (ctypes.c_double*7)()
# self.slcdll.PointSource(self.jtime, sat, ob, py2,
# star_e2, str.encode(self.brightStarTabFn))
# band_star_e1 = star_e1[:][filterIndex[filter]]
# band_star_e2 = star_e2[:][filterIndex[filter]]
# return max(band_star_e1, band_star_e2)
###############################################################################
def
caculateEarthShineFilter
(
self
,
filter
=
'i'
):
filterIndex
=
{
'nuv'
:
0
,
'u'
:
1
,
'g'
:
2
,
'r'
:
3
,
'i'
:
4
,
'z'
:
5
,
'y'
:
6
}
sat
=
(
ctypes
.
c_double
*
3
)()
sat
[:]
=
self
.
sat
ob
=
(
ctypes
.
c_double
*
3
)()
ob
[:]
=
self
.
pointing
py1
=
(
ctypes
.
c_double
*
3
)()
py2
=
(
ctypes
.
c_double
*
3
)()
self
.
slcdll
.
ComposeY
(
ob
,
py1
,
py2
)
earth_e1
=
(
ctypes
.
c_double
*
7
)()
self
.
slcdll
.
EarthShine
(
self
.
jtime
,
sat
,
ob
,
py1
,
earth_e1
)
# e[7]代表7个波段的照度
earth_e2
=
(
ctypes
.
c_double
*
7
)()
self
.
slcdll
.
EarthShine
(
self
.
jtime
,
sat
,
ob
,
py2
,
earth_e2
)
band_earth_e1
=
earth_e1
[:][
filterIndex
[
filter
]]
band_earth_e2
=
earth_e2
[:][
filterIndex
[
filter
]]
return
max
(
band_earth_e1
,
band_earth_e2
)
###############################################################################
### test
# path='/home/yan/MCI/'
# time_jd = 2460417.59979167
# x_sat = -4722.543136
# y_sat = -1478.219213
# z_sat = 4595.402769
# ra = 116.18081536720157
# dec= 39.42316681016602
# earthshine0=earthshine(path,time_jd, x_sat, y_sat, z_sat, ra, dec)
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