Geodesy utilities for MiniSky.
Provides bearing and great-circle
distance calculations on the WGS'84 ellipsoid (qdrdist, latlondist),
fast flat-earth approximations for short distances (the kwik* functions),
position projection from a reference position with bearing and distance
(qdrpos, kwikpos), local earth radius and gravity according to WGS'84,
and magnetic declination lookup from a WMM data table (magdec).
Matrix variants (suffixed with _matrix) operate on vectors of positions
and return results for every combination of the input positions.
rwgs84
Calculate the Earth radius from the WGS'84 ellipsoid.
Source code in packages/minisky/minisky/geo.py
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43 | def rwgs84(latd: q.LatitudeDeg) -> q.LengthM:
"""Calculate the Earth radius from the WGS'84 ellipsoid."""
lat = np.radians(latd)
a = _WGS84_SEMI_MAJOR_AXIS
b = _WGS84_SEMI_MINOR_AXIS
coslat = np.cos(lat)
sinlat = np.sin(lat)
an = a * a * coslat
bn = b * b * sinlat
ad = a * coslat
bd = b * sinlat
r = np.sqrt((an * an + bn * bn) / (ad * ad + bd * bd))
return r
|
rwgs84_matrix
Calculate the Earth radius from the WGS'84 ellipsoid (vectorized).
Source code in packages/minisky/minisky/geo.py
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65 | def rwgs84_matrix(latd: q.LatitudeDeg) -> q.LengthM[np.ndarray]:
"""Calculate the Earth radius from the WGS'84 ellipsoid (vectorized)."""
lat = np.radians(latd)
a = _WGS84_SEMI_MAJOR_AXIS
b = _WGS84_SEMI_MINOR_AXIS
coslat = np.cos(lat)
sinlat = np.sin(lat)
an = a * a * coslat
bn = b * b * sinlat
ad = a * coslat
bd = b * sinlat
anan = np.multiply(an, an)
bnbn = np.multiply(bn, bn)
adad = np.multiply(ad, ad)
bdbd = np.multiply(bd, bd)
r = np.sqrt(np.divide(anan + bnbn, adad + bdbd))
return r
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qdrdist
Calculate initial bearing and great-circle distance, using WGS'84.
The distance uses the WGS'84 earth radius at the average latitude of
the two positions, with a correction when the positions lie on
different hemispheres. Bearing formula from
http://www.movable-type.co.uk/scripts/latlong.html
Source code in packages/minisky/minisky/geo.py
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120 | def qdrdist(
latd1: q.LatitudeDeg,
lond1: q.LongitudeDeg,
latd2: q.LatitudeDeg,
lond2: q.LongitudeDeg,
) -> tuple[q.BearingDeg, q.DistanceM]:
"""Calculate initial bearing and great-circle distance, using WGS'84.
The distance uses the WGS'84 earth radius at the average latitude of
the two positions, with a correction when the positions lie on
different hemispheres. Bearing formula from
http://www.movable-type.co.uk/scripts/latlong.html
"""
# Check for hemisphere crossing,
# when simple average would not work
res1 = rwgs84(0.5 * (latd1 + latd2)) # same hemisphere
a = _WGS84_SEMI_MAJOR_AXIS
r1 = rwgs84(latd1)
r2 = rwgs84(latd2)
res2 = (
0.5
* (abs(latd1) * (r1 + a) + abs(latd2) * (r2 + a))
/ (np.maximum(0.000001, abs(latd1) + abs(latd2)))
) # different hemisphere
sw = latd1 * latd2 >= 0.0
r = sw * res1 + (1 - sw) * res2
lat1 = np.radians(latd1)
lon1 = np.radians(lond1)
lat2 = np.radians(latd2)
lon2 = np.radians(lond2)
# Corrected to avoid "nan" at westward direction
d = r * np.arccos(
np.cos(lat1) * np.cos(lat2) * np.cos(lon2 - lon1) + np.sin(lat1) * np.sin(lat2)
)
coslat1 = np.cos(lat1)
coslat2 = np.cos(lat2)
qdr = np.degrees(
np.arctan2(
np.sin(lon2 - lon1) * coslat2,
coslat1 * np.sin(lat2) - np.sin(lat1) * coslat2 * np.cos(lon2 - lon1),
)
)
return qdr, d
|
qdrdist_matrix
Calculate bearing and distance matrices between position vectors, using WGS'84.
Computes bearing and haversine distance for every combination of a
position in vectors 1 and a position in vectors 2.
Source code in packages/minisky/minisky/geo.py
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198 | def qdrdist_matrix(
lat1: q.LatitudeDeg,
lon1: q.LongitudeDeg,
lat2: q.LatitudeDeg,
lon2: q.LongitudeDeg,
) -> tuple[q.BearingDeg[np.ndarray], q.DistanceM[np.ndarray]]:
"""Calculate bearing and distance matrices between position vectors, using WGS'84.
Computes bearing and haversine distance for every combination of a
position in vectors 1 and a position in vectors 2.
"""
# Convert inputs to 2-D row arrays, so that .T gives column arrays and
# broadcasting yields a result for every combination of positions.
lat1 = np.atleast_2d(np.asarray(lat1))
lon1 = np.atleast_2d(np.asarray(lon1))
lat2 = np.atleast_2d(np.asarray(lat2))
lon2 = np.atleast_2d(np.asarray(lon2))
prodla = lat1.T * lat2
condition = prodla < 0
r = np.zeros(prodla.shape)
r = np.where(condition, r, rwgs84_matrix(0.5 * (lat1.T + lat2)))
a = _WGS84_SEMI_MAJOR_AXIS
r = np.where(
np.invert(condition),
r,
(
np.divide(
np.multiply(
0.5,
(
(np.multiply(abs(lat1), (rwgs84_matrix(lat1) + a))).T
+ np.multiply(abs(lat2), (rwgs84_matrix(lat2) + a))
),
),
(abs(lat1)).T + (abs(lat2) + (lat1 == 0.0) * 0.000001),
)
),
) # different hemisphere
diff_lat = lat2 - lat1.T
diff_lon = lon2 - lon1.T
sin1 = np.radians(diff_lat)
sin2 = np.radians(diff_lon)
sinlat1 = np.sin(np.radians(lat1))
sinlat2 = np.sin(np.radians(lat2))
coslat1 = np.cos(np.radians(lat1))
coslat2 = np.cos(np.radians(lat2))
sin21 = np.sin(sin2)
cos21 = np.cos(sin2)
y = np.multiply(sin21, coslat2)
x1 = np.multiply(coslat1.T, sinlat2)
x2 = np.multiply(sinlat1.T, coslat2)
x3 = np.multiply(x2, cos21)
x = x1 - x3
qdr = np.degrees(np.arctan2(y, x))
sin10 = np.abs(np.sin(sin1 / 2.0))
sin20 = np.abs(np.sin(sin2 / 2.0))
sin1sin1 = np.multiply(sin10, sin10)
sin2sin2 = np.multiply(sin20, sin20)
sqrt = sin1sin1 + np.multiply((coslat1.T * coslat2), sin2sin2)
dist_c = np.multiply(2.0, np.arctan2(np.sqrt(sqrt), np.sqrt(1 - sqrt)))
dist = np.multiply(r, dist_c)
return qdr, dist
|
latlondist
Calculates only distance using haversine notation of the same formulae
and average r from wgs'84.
Source code in packages/minisky/minisky/geo.py
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238 | def latlondist(
latd1: q.LatitudeDeg,
lond1: q.LongitudeDeg,
latd2: q.LatitudeDeg,
lond2: q.LongitudeDeg,
) -> q.DistanceM:
"""Calculates only distance using haversine notation of the same formulae
and average r from wgs'84.
"""
res1 = rwgs84(0.5 * (latd1 + latd2)) # same hemisphere
# res2 :different hemisphere
a = _WGS84_SEMI_MAJOR_AXIS
r1 = rwgs84(latd1)
r2 = rwgs84(latd2)
res2 = (
0.5 * (abs(latd1) * (r1 + a) + abs(latd2) * (r2 + a)) / (abs(latd1) + abs(latd2))
) # different hemisphere
sw = latd1 * latd2 >= 0.0
r = sw * res1 + (1 - sw) * res2
lat1 = np.radians(latd1)
lon1 = np.radians(lond1)
lat2 = np.radians(latd2)
lon2 = np.radians(lond2)
sin1 = np.sin(0.5 * (lat2 - lat1))
sin2 = np.sin(0.5 * (lon2 - lon1))
coslat1 = np.cos(lat1)
coslat2 = np.cos(lat2)
root = sin1 * sin1 + coslat1 * coslat2 * sin2 * sin2
d = 2.0 * r * np.arctan2(np.sqrt(root), np.sqrt(1.0 - root))
return d
|
latlondist_matrix
Calculates distance matrix using haversine formulae and average r from wgs'84.
Source code in packages/minisky/minisky/geo.py
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297 | def latlondist_matrix(
lat1: q.LatitudeDeg,
lon1: q.LongitudeDeg,
lat2: q.LatitudeDeg,
lon2: q.LongitudeDeg,
) -> q.DistanceM[np.ndarray]:
"""Calculates distance matrix using haversine formulae and average r from wgs'84."""
# Convert inputs to 2-D row arrays, so that .T gives column arrays and
# broadcasting yields a result for every combination of positions.
lat1 = np.atleast_2d(np.asarray(lat1))
lon1 = np.atleast_2d(np.asarray(lon1))
lat2 = np.atleast_2d(np.asarray(lat2))
lon2 = np.atleast_2d(np.asarray(lon2))
prodla = lat1.T * lat2
condition = prodla < 0
r = np.zeros(prodla.shape)
r = np.where(condition, r, rwgs84_matrix(0.5 * (lat1.T + lat2)))
a = _WGS84_SEMI_MAJOR_AXIS
r = np.where(
np.invert(condition),
r,
(
np.divide(
np.multiply(
0.5,
(
(np.multiply(abs(lat1), (rwgs84_matrix(lat1) + a))).T
+ np.multiply(abs(lat2), (rwgs84_matrix(lat2) + a))
),
),
(abs(lat1)).T + (abs(lat2)),
)
),
) # different hemisphere
diff_lat = lat2 - lat1.T
diff_lon = lon2 - lon1.T
sin1 = np.radians(diff_lat)
sin2 = np.radians(diff_lon)
coslat1 = np.cos(np.radians(lat1))
coslat2 = np.cos(np.radians(lat2))
sin10 = np.sin(sin1 / 2)
sin20 = np.sin(sin2 / 2)
sin1sin1 = np.multiply(sin10, sin10)
sin2sin2 = np.multiply(sin20, sin20)
root = sin1sin1 + np.multiply((coslat1.T * coslat2), sin2sin2)
dist_c = np.multiply(2, np.arctan2(np.sqrt(root), np.sqrt(1.0 - root)))
dist = np.multiply(r, dist_c)
return dist
|
wgsg
Gravity acceleration at a given latitude according to WGS'84.
Source code in packages/minisky/minisky/geo.py
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309 | def wgsg(latd: q.LatitudeDeg) -> q.GravitationalAccelerationMps2:
"""Gravity acceleration at a given latitude according to WGS'84."""
geq = 9.7803 # m/s2 g at equator
e2 = 6.694e-3 # eccentricity
k = 0.001932 # derived from flattening f, 1/f = 298.257223563
sinlat = np.sin(np.radians(latd))
g = geq * (1.0 + k * sinlat * sinlat) / np.sqrt(1.0 - e2 * sinlat * sinlat)
return g
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qdrpos
Calculate vector with positions from vectors of reference position,
bearing and distance.
Great-circle projection using the WGS'84 earth radius at the reference
latitude. Ref for qdrpos:
http://www.movable-type.co.uk/scripts/latlong.html
Source code in packages/minisky/minisky/geo.py
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339 | def qdrpos(
latd1: q.LatitudeDeg,
lond1: q.LongitudeDeg,
qdr: q.BearingDeg,
dist: q.DistanceM,
) -> tuple[q.LatitudeDeg, q.LongitudeDeg]:
"""Calculate vector with positions from vectors of reference position,
bearing and distance.
Great-circle projection using the WGS'84 earth radius at the reference
latitude. Ref for qdrpos:
http://www.movable-type.co.uk/scripts/latlong.html
"""
R = rwgs84(latd1)
lat1 = np.radians(latd1)
lon1 = np.radians(lond1)
lat2 = np.arcsin(
np.sin(lat1) * np.cos(dist / R) + np.cos(lat1) * np.sin(dist / R) * np.cos(np.radians(qdr))
)
lon2 = lon1 + np.arctan2(
np.sin(np.radians(qdr)) * np.sin(dist / R) * np.cos(lat1),
np.cos(dist / R) - np.sin(lat1) * np.sin(lat2),
)
return np.degrees(lat2), np.degrees(lon2)
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kwikdist
Quick and dirty distance calculation.
Equirectangular (flat-earth) approximation with the mean earth radius;
fast, but accurate for short distances only.
Source code in packages/minisky/minisky/geo.py
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363 | def kwikdist(
lata: q.LatitudeDeg,
lona: q.LongitudeDeg,
latb: q.LatitudeDeg,
lonb: q.LongitudeDeg,
) -> q.DistanceM:
"""Quick and dirty distance calculation.
Equirectangular (flat-earth) approximation with the mean earth radius;
fast, but accurate for short distances only.
"""
re = _MEAN_EARTH_RADIUS
dlat = np.radians(latb - lata)
dlon = np.radians(((lonb - lona) + 180) % 360 - 180)
cavelat = np.cos(np.radians(lata + latb) * 0.5)
dangle = np.sqrt(dlat * dlat + dlon * dlon * cavelat * cavelat)
dist = re * dangle
return dist
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kwikdist_matrix
Quick and dirty distance matrix between two sets of positions.
Equirectangular (flat-earth) approximation with the mean earth radius;
fast, but accurate for short distances only.
Source code in packages/minisky/minisky/geo.py
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390 | def kwikdist_matrix(
lata: q.LatitudeDeg[np.ndarray],
lona: q.LongitudeDeg[np.ndarray],
latb: q.LatitudeDeg[np.ndarray],
lonb: q.LongitudeDeg[np.ndarray],
) -> q.DistanceM[np.ndarray]:
"""Quick and dirty distance matrix between two sets of positions.
Equirectangular (flat-earth) approximation with the mean earth radius;
fast, but accurate for short distances only.
"""
re = _MEAN_EARTH_RADIUS
dlat = np.radians(latb - lata.T)
dlon = np.radians(((lonb - lona.T) + 180) % 360 - 180)
cavelat = np.cos(np.radians(lata + latb.T) * 0.5)
dangle = np.sqrt(
np.multiply(dlat, dlat)
+ np.multiply(np.multiply(dlon, dlon), np.multiply(cavelat, cavelat))
)
dist = re * dangle
return dist
|
kwikqdrdist
Quick bearing/distance using a flat-earth approximation.
Uses the mean earth radius and does not work well close to the poles.
Bearings are normalized to [0, 360).
Source code in packages/minisky/minisky/geo.py
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417 | def kwikqdrdist(
lata: q.LatitudeDeg,
lona: q.LongitudeDeg,
latb: q.LatitudeDeg,
lonb: q.LongitudeDeg,
) -> tuple[q.BearingDeg, q.DistanceM]:
"""Quick bearing/distance using a flat-earth approximation.
Uses the mean earth radius and does not work well close to the poles.
Bearings are normalized to [0, 360).
"""
re = _MEAN_EARTH_RADIUS
dlat = np.radians(latb - lata)
dlon = np.radians(((lonb - lona) + 180) % 360 - 180)
cavelat = np.cos(np.radians(lata + latb) * 0.5)
dangle = np.sqrt(dlat * dlat + dlon * dlon * cavelat * cavelat)
dist = re * dangle
qdr = np.degrees(np.arctan2(dlon * cavelat, dlat)) % 360.0
return qdr, dist
|
kwikqdrdist_matrix
Quick bearing/distance matrices using a flat-earth approximation.
Uses the mean earth radius and does not work well close to the poles.
Bearings are normalized to [0, 360).
Source code in packages/minisky/minisky/geo.py
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447 | def kwikqdrdist_matrix(
lata: q.LatitudeDeg[np.ndarray],
lona: q.LongitudeDeg[np.ndarray],
latb: q.LatitudeDeg[np.ndarray],
lonb: q.LongitudeDeg[np.ndarray],
) -> tuple[q.BearingDeg[np.ndarray], q.DistanceM[np.ndarray]]:
"""Quick bearing/distance matrices using a flat-earth approximation.
Uses the mean earth radius and does not work well close to the poles.
Bearings are normalized to [0, 360).
"""
re = _MEAN_EARTH_RADIUS
dlat = np.radians(latb - lata.T)
dlon = np.radians(((lonb - lona.T) + 180) % 360 - 180)
cavelat = np.cos(np.radians(latb + lata.T) * 0.5)
dangle = np.sqrt(
np.multiply(dlat, dlat)
+ np.multiply(np.multiply(dlon, dlon), np.multiply(cavelat, cavelat))
)
dist = re * dangle
qdr = np.degrees(np.arctan2(np.multiply(dlon, cavelat), dlat)) % 360.0
return qdr, dist
|
kwikpos
Fast, but quick and dirty, position calculation from vectors of reference position,
bearing and distance using flat earth approximation.
Use for flat earth purposes e.g. flat display.
Longitude is wrapped to [-180, 180).
Source code in packages/minisky/minisky/geo.py
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472 | def kwikpos(
latd1: q.LatitudeDeg,
lond1: q.LongitudeDeg,
qdr: q.BearingDeg,
dist: q.DistanceM,
) -> tuple[q.LatitudeDeg, q.LongitudeDeg]:
"""Fast, but quick and dirty, position calculation from vectors of reference position,
bearing and distance using flat earth approximation.
Use for flat earth purposes e.g. flat display.
Longitude is wrapped to [-180, 180).
"""
dx = dist * np.sin(np.radians(qdr))
dy = dist * np.cos(np.radians(qdr))
dlat = dy / _METERS_PER_LATITUDE_DEGREE
dlon = dx / np.maximum(0.01, _METERS_PER_LATITUDE_DEGREE * np.cos(np.radians(latd1)))
latd2 = latd1 + dlat
lond2 = ((lond1 + dlon) + 180) % 360 - 180
return latd2, lond2
|
magdec
Gives magnetic declination (also called magnetic variation) at a given
position, interpolated linearly from the bundled global data table.
In:
latd, lond [deg] Position at which the magnetic declination is
evaluated (floats)
Out:
d_hdg [deg] Magnetic declination, the angle of difference
between true North and magnetic North. For instance,
if the declination at a certain point were 10 deg W
(10 deg), then a compass at that location pointing
north (magnetic) would actually align 10 deg W of
true North. True North would be 10 deg E relative to
the magnetic North direction given by the compass.
Declination varies with location and slowly changes
in time. Referenced from
https://www.ngdc.noaa.gov/geomag/calculators/help/igrfgridHelp.html
In short, magnetic heading = true heading - d_hdg,
(Reminder MTV : M = T - V)
or, true heading = magnetic heading + d_hdg.
Created by : Yaofu Zhou
Modified by J.M. Hoekstra
Reason: Segmentation fault caused by Scipy's BiVariateSpline interpolation
for some data on some machines, so it was changed to linear interpolation.
Difference in methods has been inspected: it is way less than the inaccuracy
of the actual data. Axes were regularly spaced at one degree. The direct
manual linear interpolation is also about 6 times faster.
Source code in packages/minisky/minisky/geo.py
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524 | def magdec(latd: q.LatitudeDeg[float], lond: q.LongitudeDeg[float]) -> q.AngleDeg[float]:
"""
Gives magnetic declination (also called magnetic variation) at a given
position, interpolated linearly from the bundled global data table.
In:
latd, lond [deg] Position at which the magnetic declination is
evaluated (floats)
Out:
d_hdg [deg] Magnetic declination, the angle of difference
between true North and magnetic North. For instance,
if the declination at a certain point were 10 deg W
(10 deg), then a compass at that location pointing
north (magnetic) would actually align 10 deg W of
true North. True North would be 10 deg E relative to
the magnetic North direction given by the compass.
Declination varies with location and slowly changes
in time. Referenced from
https://www.ngdc.noaa.gov/geomag/calculators/help/igrfgridHelp.html
In short, magnetic heading = true heading - d_hdg,
(Reminder MTV : M = T - V)
or, true heading = magnetic heading + d_hdg.
Created by : Yaofu Zhou
Modified by J.M. Hoekstra
Reason: Segmentation fault caused by Scipy's BiVariateSpline interpolation
for some data on some machines, so it was changed to linear interpolation.
Difference in methods has been inspected: it is way less than the inaccuracy
of the actual data. Axes were regularly spaced at one degree. The direct
manual linear interpolation is also about 6 times faster.
"""
decl_lat_lon = load_magnetic_declination()
# Use fact that whole degrees are used as ticks on both lat & lon axis
i_lat = min(max(0, int(90.0 - latd)), 180)
f_lat = (90.0 - latd) - int(90.0 - latd)
i_lon = min(max(0, int(lond + 180)), 360)
f_lon = lond + 180.0 - int(lond + 180)
# 2D linear interpolation
declon0 = (
decl_lat_lon[i_lat, i_lon] * (1.0 - f_lat)
+ f_lat * decl_lat_lon[min(180, i_lat + 1), i_lon]
)
declon1 = (
decl_lat_lon[i_lat, i_lon + 1] * (1.0 - f_lat)
+ f_lat * decl_lat_lon[min(180, i_lat + 1), min(i_lon + 1, 360)]
)
d_hdg = declon0 * (1.0 - f_lon) + f_lon * declon1
return d_hdg
|
load_magnetic_declination
cached
Called by Init
Read magnetic declination (also called magnetic variation) datafile
based on the data table calculated from the NOAA webpage
https://www.ngdc.noaa.gov/geomag/calculators/magcalc.shtml#igrfgrid
with the following input:
Southern most lat: 90 S
Northern most lat: 90 N
Lat Step Size: 1.0
Western most long: 180 W
Eastern most long: 179 E
Lon Step Size: 1.0
Elevation: Mean sea level 0 Feet
Magnetic component: Declination
Model: WMM (2019-2024)
Start Date: 2020 09 20
End Date: 2020 09 20
Step size: 1.0
Result format: CSV
The grid size can be adjusted but the (1 deg by 1 deg) size should suffice
for practical purpose, as long as the the grids cover the entire Earth
surface. The interpolation is performed at sea-level, but no significant
difference would be noticed up to FL600 or beyond.
See docstring of geo.magdec() for more information.
Based on original version created by : Yaofu Zhou
Modified to read at init and use linear interpolation by J.M. Hoekstra
Source code in packages/minisky/minisky/geo.py
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584 | @cache
def load_magnetic_declination() -> q.AngleDeg[np.ndarray]:
"""
Called by Init
Read magnetic declination (also called magnetic variation) datafile
based on the data table calculated from the NOAA webpage
https://www.ngdc.noaa.gov/geomag/calculators/magcalc.shtml#igrfgrid
with the following input:
Southern most lat: 90 S
Northern most lat: 90 N
Lat Step Size: 1.0
Western most long: 180 W
Eastern most long: 179 E
Lon Step Size: 1.0
Elevation: Mean sea level 0 Feet
Magnetic component: Declination
Model: WMM (2019-2024)
Start Date: 2020 09 20
End Date: 2020 09 20
Step size: 1.0
Result format: CSV
The grid size can be adjusted but the (1 deg by 1 deg) size should suffice
for practical purpose, as long as the the grids cover the entire Earth
surface. The interpolation is performed at sea-level, but no significant
difference would be noticed up to FL600 or beyond.
See docstring of geo.magdec() for more information.
Based on original version created by : Yaofu Zhou
Modified to read at init and use linear interpolation by J.M. Hoekstra"""
# Columns:
# (1) Date in decimal years
# (2) Latitude in decimal Degrees
# (3) Longitude in decimal Degrees
# (4) Elevation in km Mean Sea Level
# (5) Declination in Degree
# (6) Declination_sv in Degree
# (7) Declination_uncertainty in Degree
#
# lat : 89 ... -90
# Lon: -180 ... 179
file_path = data("navigation") / "geo_declination_data.csv"
df = pd.read_csv(file_path, comment="#", header=None)
decl = np.asarray(df[4], dtype=float)
decl_lat_lon = decl.reshape((180, 360))
# Source data stops at +89°; extend the grid to +90° by reusing that row.
decl_lat_lon = np.vstack((decl_lat_lon[0:1, :], decl_lat_lon))
# Add a column for longitude = 180 degrees (same as longitude = -180 degrees)
decl_lat_lon = np.hstack((decl_lat_lon, decl_lat_lon[:, 0:1]))
# Result is a 181x361 table for
# lat = 90 ... -90 (rows)
# lon = -180 ... 180 (columns)
decl_lat_lon.setflags(write=False)
return decl_lat_lon
|