|
1
|
|
|
# -*- coding: utf-8 -*- |
|
2
|
|
|
"""Pythonic wrappers for AACGM-V2 C functions. |
|
3
|
|
|
|
|
4
|
|
|
Functions |
|
5
|
|
|
-------------- |
|
6
|
|
|
test_time : Test the time and ensure it is a datetime.datetime object |
|
7
|
|
|
test_height : Test the height and see if it is appropriate for the method |
|
8
|
|
|
set_coeff_path : Set the coefficient paths using default or supplied values |
|
9
|
|
|
convert_latlon : Converts scalar location |
|
10
|
|
|
convert_latlon_arr : Converts array location |
|
11
|
|
|
get_aacgm_coord : Get scalar magnetic lat, lon, mlt from geographic location |
|
12
|
|
|
get_aacgm_coord_arr : Get array magnetic lat, lon, mlt from geographic location |
|
13
|
|
|
convert_str_to_bit : Convert human readible AACGM flag to bits |
|
14
|
|
|
convert_bool_to_bit : Convert boolian flags to bits |
|
15
|
|
|
convert_mlt : Get array mlt |
|
16
|
|
|
-------------- |
|
17
|
|
|
|
|
18
|
|
|
""" |
|
19
|
|
|
|
|
20
|
|
|
from __future__ import division, absolute_import, unicode_literals |
|
21
|
|
|
import datetime as dt |
|
22
|
|
|
import numpy as np |
|
23
|
|
|
import os |
|
24
|
|
|
import sys |
|
25
|
|
|
|
|
26
|
|
|
import aacgmv2 |
|
27
|
|
|
import aacgmv2._aacgmv2 as c_aacgmv2 |
|
28
|
|
|
from aacgmv2._aacgmv2 import TRACE, ALLOWTRACE, BADIDEA |
|
29
|
|
|
|
|
30
|
|
|
def test_time(dtime): |
|
31
|
|
|
""" Test the time input and ensure it is a dt.datetime object |
|
32
|
|
|
|
|
33
|
|
|
Parameters |
|
34
|
|
|
---------- |
|
35
|
|
|
dtime : (unknown) |
|
36
|
|
|
Time input in an untested format |
|
37
|
|
|
|
|
38
|
|
|
Returns |
|
39
|
|
|
------- |
|
40
|
|
|
dtime : (dt.datetime) |
|
41
|
|
|
Time as a datetime object |
|
42
|
|
|
|
|
43
|
|
|
Raises |
|
44
|
|
|
------ |
|
45
|
|
|
ValueError if time is not a dt.date or dt.datetime object |
|
46
|
|
|
|
|
47
|
|
|
""" |
|
48
|
|
|
if isinstance(dtime, dt.date): |
|
49
|
|
|
# Because datetime objects identify as both dt.date and dt.datetime, |
|
50
|
|
|
# you need an extra test here to ensure you don't lose the time |
|
51
|
|
|
# attributes |
|
52
|
|
|
if not isinstance(dtime, dt.datetime): |
|
53
|
|
|
dtime = dt.datetime.combine(dtime, dt.time(0)) |
|
54
|
|
|
elif not isinstance(dtime, dt.datetime): |
|
55
|
|
|
raise ValueError('time variable (dtime) must be a datetime object') |
|
56
|
|
|
|
|
57
|
|
|
return dtime |
|
58
|
|
|
|
|
59
|
|
|
|
|
60
|
|
|
def test_height(height, bit_code): |
|
61
|
|
|
""" Test the input height and ensure it is appropriate for the method |
|
62
|
|
|
|
|
63
|
|
|
Parameters |
|
64
|
|
|
---------- |
|
65
|
|
|
height : (float) |
|
66
|
|
|
Height to test in km |
|
67
|
|
|
bit_code : (int) |
|
68
|
|
|
Code string denoting method to use |
|
69
|
|
|
|
|
70
|
|
|
Returns |
|
71
|
|
|
------- |
|
72
|
|
|
good_height : (boolean) |
|
73
|
|
|
True if height and method are appropriate, False if not |
|
74
|
|
|
|
|
75
|
|
|
Notes |
|
76
|
|
|
----- |
|
77
|
|
|
Appropriate altitude ranges for the different methods are explored in |
|
78
|
|
|
Shepherd (2014). Summarized, they are: |
|
79
|
|
|
Coefficients: 0-2000 km |
|
80
|
|
|
Tracing: 0-1 Earth Radius |
|
81
|
|
|
|
|
82
|
|
|
Altitudes below zero will work, but will not provide a good representation |
|
83
|
|
|
of the magnetic field because it goes beyond the intended scope of these |
|
84
|
|
|
coordiantes. |
|
85
|
|
|
|
|
86
|
|
|
If you use the 'BADIDEA' code, you can bypass all constraints, but it |
|
87
|
|
|
is a Bad Idea! If you include a high enough altiutde, the code may hang. |
|
88
|
|
|
|
|
89
|
|
|
""" |
|
90
|
|
|
# Test for heights that are allowed but not within the intended scope |
|
91
|
|
|
# of the coordinate system. The routine will work, but the user should |
|
92
|
|
|
# be aware that the results are not as reliable |
|
93
|
|
|
if height < 0: |
|
94
|
|
|
aacgmv2.logger.warning('conversion not intended for altitudes < 0 km') |
|
95
|
|
|
|
|
96
|
|
|
# Test the conditions for using the coefficient method |
|
97
|
|
|
if(height > aacgmv2.high_alt_coeff and |
|
98
|
|
|
not (bit_code & (TRACE|ALLOWTRACE|BADIDEA))): |
|
99
|
|
|
estr = ''.join(['coefficients are not valid for altitudes above ', |
|
100
|
|
|
'{:.0f} km. You '.format(aacgmv2.high_alt_coeff), |
|
101
|
|
|
'must either use field-line tracing (trace=True or', |
|
102
|
|
|
' allowtrace=True) or indicate you know this is a', |
|
103
|
|
|
' bad idea']) |
|
104
|
|
|
aacgmv2.logger.error(estr) |
|
105
|
|
|
return False |
|
106
|
|
|
|
|
107
|
|
|
# Test the conditions for using the tracing method |
|
108
|
|
|
if height > aacgmv2.high_alt_trace and not (bit_code & BADIDEA): |
|
109
|
|
|
estr = ''.join(['these coordinates are not intended for the ', |
|
110
|
|
|
'magnetosphere! You must indicate that you know ', |
|
111
|
|
|
'this is a bad idea. If you continue, it is ', |
|
112
|
|
|
'possible that the code will hang.']) |
|
113
|
|
|
aacgmv2.logger.error(estr) |
|
114
|
|
|
return False |
|
115
|
|
|
|
|
116
|
|
|
return True |
|
117
|
|
|
|
|
118
|
|
|
def set_coeff_path(igrf_file=False, coeff_prefix=False): |
|
119
|
|
|
"""Sets the IGRF_COEFF and AACGMV_V2_DAT_PREFIX environment variables. |
|
120
|
|
|
|
|
121
|
|
|
Parameters |
|
122
|
|
|
----------- |
|
123
|
|
|
igrf_file : (str or bool) |
|
124
|
|
|
Full filename of IGRF coefficient file, True to use |
|
125
|
|
|
aacgmv2.IGRF_COEFFS, or False to leave as is. (default=False) |
|
126
|
|
|
coeff_prefix : (str or bool) |
|
127
|
|
|
Location and file prefix for aacgm coefficient files, True to use |
|
128
|
|
|
aacgmv2.AACGM_V2_DAT_PREFIX, or False to leave as is. (default=False) |
|
129
|
|
|
|
|
130
|
|
|
""" |
|
131
|
|
|
|
|
132
|
|
|
# Define coefficient file prefix if requested |
|
133
|
|
|
if coeff_prefix is not False: |
|
134
|
|
|
# Use the default value, if one was not supplied (allow None to |
|
135
|
|
|
# comply with depricated behaviour) |
|
136
|
|
|
if coeff_prefix is True or coeff_prefix is None: |
|
137
|
|
|
coeff_prefix = aacgmv2.AACGM_v2_DAT_PREFIX |
|
138
|
|
|
|
|
139
|
|
|
if hasattr(os, "unsetenv"): |
|
140
|
|
|
os.unsetenv('AACGM_v2_DAT_PREFIX') |
|
141
|
|
|
else: |
|
142
|
|
|
del os.environ['AACGM_v2_DAT_PREFIX'] |
|
143
|
|
|
os.environ['AACGM_v2_DAT_PREFIX'] = coeff_prefix |
|
144
|
|
|
|
|
145
|
|
|
# Define IGRF file if requested |
|
146
|
|
|
if igrf_file is not False: |
|
147
|
|
|
# Use the default value, if one was not supplied (allow None to |
|
148
|
|
|
# comply with depricated behaviour) |
|
149
|
|
|
if igrf_file is True or igrf_file is None: |
|
150
|
|
|
igrf_file = aacgmv2.IGRF_COEFFS |
|
151
|
|
|
|
|
152
|
|
|
if hasattr(os, "unsetenv"): |
|
153
|
|
|
os.unsetenv('IGRF_COEFFS') |
|
154
|
|
|
else: |
|
155
|
|
|
del os.environ['IGRF_COEFFS'] |
|
156
|
|
|
os.environ['IGRF_COEFFS'] = igrf_file |
|
157
|
|
|
|
|
158
|
|
|
return |
|
159
|
|
|
|
|
160
|
|
|
def convert_latlon(in_lat, in_lon, height, dtime, method_code="G2A"): |
|
161
|
|
|
"""Converts between geomagnetic coordinates and AACGM coordinates |
|
162
|
|
|
|
|
163
|
|
|
Parameters |
|
164
|
|
|
------------ |
|
165
|
|
|
in_lat : (float) |
|
166
|
|
|
Input latitude in degrees N (code specifies type of latitude) |
|
167
|
|
|
in_lon : (float) |
|
168
|
|
|
Input longitude in degrees E (code specifies type of longitude) |
|
169
|
|
|
height : (float) |
|
170
|
|
|
Altitude above the surface of the earth in km |
|
171
|
|
|
dtime : (datetime) |
|
172
|
|
|
Datetime for magnetic field |
|
173
|
|
|
method_code : (str or int) |
|
174
|
|
|
Bit code or string denoting which type(s) of conversion to perform |
|
175
|
|
|
G2A - geographic (geodetic) to AACGM-v2 |
|
176
|
|
|
A2G - AACGM-v2 to geographic (geodetic) |
|
177
|
|
|
TRACE - use field-line tracing, not coefficients |
|
178
|
|
|
ALLOWTRACE - use trace only above 2000 km |
|
179
|
|
|
BADIDEA - use coefficients above 2000 km |
|
180
|
|
|
GEOCENTRIC - assume inputs are geocentric w/ RE=6371.2 |
|
181
|
|
|
(default is "G2A") |
|
182
|
|
|
|
|
183
|
|
|
Returns |
|
184
|
|
|
------- |
|
185
|
|
|
out_lat : (float) |
|
186
|
|
|
Output latitude in degrees N |
|
187
|
|
|
out_lon : (float) |
|
188
|
|
|
Output longitude in degrees E |
|
189
|
|
|
out_r : (float) |
|
190
|
|
|
Geocentric radial distance (R_Earth) or altitude above the surface of |
|
191
|
|
|
the Earth (km) |
|
192
|
|
|
|
|
193
|
|
|
Raises |
|
194
|
|
|
------ |
|
195
|
|
|
ValueError if input is incorrect |
|
196
|
|
|
TypeError or RuntimeError if unable to set AACGMV2 datetime |
|
197
|
|
|
|
|
198
|
|
|
""" |
|
199
|
|
|
|
|
200
|
|
|
# Test time |
|
201
|
|
|
dtime = test_time(dtime) |
|
202
|
|
|
|
|
203
|
|
|
# Initialise output |
|
204
|
|
|
lat_out = np.nan |
|
205
|
|
|
lon_out = np.nan |
|
206
|
|
|
r_out = np.nan |
|
207
|
|
|
|
|
208
|
|
|
# Set the coordinate coversion method code in bits |
|
209
|
|
|
try: |
|
210
|
|
|
bit_code = convert_str_to_bit(method_code.upper()) |
|
211
|
|
|
except AttributeError: |
|
212
|
|
|
bit_code = method_code |
|
213
|
|
|
|
|
214
|
|
|
if not isinstance(bit_code, int): |
|
215
|
|
|
raise ValueError("unknown method code {:}".format(method_code)) |
|
216
|
|
|
|
|
217
|
|
|
# Test height that may or may not cause failure |
|
218
|
|
|
if not test_height(height, bit_code): |
|
219
|
|
|
return lat_out, lon_out, r_out |
|
220
|
|
|
|
|
221
|
|
|
# Test latitude range |
|
222
|
|
|
if abs(in_lat) > 90.0: |
|
223
|
|
|
# Allow latitudes with a small deviation from the maximum |
|
224
|
|
|
# (+/- 90 degrees) to be set to 90 |
|
225
|
|
|
if abs(in_lat) > 90.1: |
|
226
|
|
|
raise ValueError('unrealistic latitude') |
|
227
|
|
|
in_lat = np.sign(in_lat) * 90.0 |
|
228
|
|
|
|
|
229
|
|
|
# Constrain longitudes between -180 and 180 |
|
230
|
|
|
in_lon = ((in_lon + 180.0) % 360.0) - 180.0 |
|
231
|
|
|
|
|
232
|
|
|
# Set current date and time |
|
233
|
|
|
try: |
|
234
|
|
|
c_aacgmv2.set_datetime(dtime.year, dtime.month, dtime.day, dtime.hour, |
|
235
|
|
|
dtime.minute, dtime.second) |
|
236
|
|
|
except TypeError as terr: |
|
237
|
|
|
raise TypeError("unable to set time for {:}: {:}".format(dtime, terr)) |
|
238
|
|
|
except RuntimeError as rerr: |
|
239
|
|
|
raise RuntimeError("unable to set time for {:}: {:}".format(dtime, |
|
240
|
|
|
rerr)) |
|
241
|
|
|
|
|
242
|
|
|
# convert location |
|
243
|
|
|
try: |
|
244
|
|
|
lat_out, lon_out, r_out = c_aacgmv2.convert(in_lat, in_lon, height, |
|
245
|
|
|
bit_code) |
|
246
|
|
|
except: |
|
247
|
|
|
err = sys.exc_info()[0] |
|
248
|
|
|
estr = "unable to perform conversion at {:.1f},".format(in_lat) |
|
249
|
|
|
estr = "{:s}{:.1f} {:.1f} km, {:} ".format(estr, in_lon, height, dtime) |
|
250
|
|
|
estr = "{:s}using method {:}: {:}".format(estr, bit_code, err) |
|
251
|
|
|
aacgmv2.logger.warning(estr) |
|
252
|
|
|
pass |
|
253
|
|
|
|
|
254
|
|
|
return lat_out, lon_out, r_out |
|
255
|
|
|
|
|
256
|
|
|
def convert_latlon_arr(in_lat, in_lon, height, dtime, method_code="G2A"): |
|
257
|
|
|
"""Converts between geomagnetic coordinates and AACGM coordinates. |
|
258
|
|
|
|
|
259
|
|
|
Parameters |
|
260
|
|
|
------------ |
|
261
|
|
|
in_lat : (np.ndarray or list or float) |
|
262
|
|
|
Input latitude in degrees N (method_code specifies type of latitude) |
|
263
|
|
|
in_lon : (np.ndarray or list or float) |
|
264
|
|
|
Input longitude in degrees E (method_code specifies type of longitude) |
|
265
|
|
|
height : (np.ndarray or list or float) |
|
266
|
|
|
Altitude above the surface of the earth in km |
|
267
|
|
|
dtime : (datetime) |
|
268
|
|
|
Single datetime object for magnetic field |
|
269
|
|
|
method_code : (int or str) |
|
270
|
|
|
Bit code or string denoting which type(s) of conversion to perform |
|
271
|
|
|
G2A - geographic (geodetic) to AACGM-v2 |
|
272
|
|
|
A2G - AACGM-v2 to geographic (geodetic) |
|
273
|
|
|
TRACE - use field-line tracing, not coefficients |
|
274
|
|
|
ALLOWTRACE - use trace only above 2000 km |
|
275
|
|
|
BADIDEA - use coefficients above 2000 km |
|
276
|
|
|
GEOCENTRIC - assume inputs are geocentric w/ RE=6371.2 |
|
277
|
|
|
(default = "G2A") |
|
278
|
|
|
|
|
279
|
|
|
Returns |
|
280
|
|
|
------- |
|
281
|
|
|
out_lat : (np.ndarray) |
|
282
|
|
|
Output latitudes in degrees N |
|
283
|
|
|
out_lon : (np.ndarray) |
|
284
|
|
|
Output longitudes in degrees E |
|
285
|
|
|
out_r : (np.ndarray) |
|
286
|
|
|
Geocentric radial distance (R_Earth) or altitude above the surface of |
|
287
|
|
|
the Earth (km) |
|
288
|
|
|
|
|
289
|
|
|
Raises |
|
290
|
|
|
------ |
|
291
|
|
|
ValueError if input is incorrect |
|
292
|
|
|
TypeError or RuntimeError if unable to set AACGMV2 datetime |
|
293
|
|
|
|
|
294
|
|
|
Notes |
|
295
|
|
|
------- |
|
296
|
|
|
At least one of in_lat, in_lon, and height must be a list or array. |
|
297
|
|
|
|
|
298
|
|
|
""" |
|
299
|
|
|
|
|
300
|
|
|
# Recast the data as numpy arrays |
|
301
|
|
|
in_lat = np.array(in_lat) |
|
302
|
|
|
in_lon = np.array(in_lon) |
|
303
|
|
|
height = np.array(height) |
|
304
|
|
|
|
|
305
|
|
|
# If one or two of these elements is a float or int, create an array |
|
306
|
|
|
test_array = np.array([len(in_lat.shape), len(in_lon.shape), |
|
307
|
|
|
len(height.shape)]) |
|
308
|
|
|
if test_array.min() == 0: |
|
309
|
|
|
if test_array.max() == 0: |
|
310
|
|
|
aacgmv2.logger.warning("for a single location, consider using " \ |
|
311
|
|
|
"convert_latlon or get_aacgm_coord") |
|
312
|
|
|
in_lat = np.array([in_lat]) |
|
313
|
|
|
in_lon = np.array([in_lon]) |
|
314
|
|
|
height = np.array([height]) |
|
315
|
|
|
else: |
|
316
|
|
|
imax = test_array.argmax() |
|
317
|
|
|
max_shape = in_lat.shape if imax == 0 else (in_lon.shape \ |
|
318
|
|
|
if imax == 1 else height.shape) |
|
319
|
|
|
if not test_array[0]: |
|
320
|
|
|
in_lat = np.full(shape=max_shape, fill_value=in_lat) |
|
321
|
|
|
if not test_array[1]: |
|
322
|
|
|
in_lon = np.full(shape=max_shape, fill_value=in_lon) |
|
323
|
|
|
if not test_array[2]: |
|
324
|
|
|
height = np.full(shape=max_shape, fill_value=height) |
|
325
|
|
|
|
|
326
|
|
|
# Ensure that lat, lon, and height are the same length or if the lengths |
|
327
|
|
|
# differ that the different ones contain only a single value |
|
328
|
|
|
if not (in_lat.shape == in_lon.shape and in_lat.shape == height.shape): |
|
329
|
|
|
shape_dict = {'lat': in_lat.shape, 'lon': in_lon.shape, |
|
330
|
|
|
'height': height.shape} |
|
331
|
|
|
ulen = np.unique(shape_dict.values()) |
|
332
|
|
|
array_key = [kk for i, kk in enumerate(shape_dict.keys()) |
|
333
|
|
|
if shape_dict[kk] != (1,)] |
|
334
|
|
|
if len(array_key) == 3: |
|
335
|
|
|
raise ValueError('lat, lon, and height arrays are mismatched') |
|
336
|
|
|
elif len(array_key) == 2: |
|
337
|
|
|
if shape_dict[array_key[0]] == shape_dict[array_dict[1]]: |
|
|
|
|
|
|
338
|
|
|
raise ValueError('{:s} and {:s} arrays are mismatched'.format(\ |
|
339
|
|
|
*array_key)) |
|
340
|
|
|
|
|
341
|
|
|
# Test time |
|
342
|
|
|
dtime = test_time(dtime) |
|
343
|
|
|
|
|
344
|
|
|
# Initialise output |
|
345
|
|
|
lat_out = np.full(shape=in_lat.shape, fill_value=np.nan) |
|
346
|
|
|
lon_out = np.full(shape=in_lon.shape, fill_value=np.nan) |
|
347
|
|
|
r_out = np.full(shape=height.shape, fill_value=np.nan) |
|
348
|
|
|
|
|
349
|
|
|
# Test and set the conversion method code |
|
350
|
|
|
try: |
|
351
|
|
|
bit_code = convert_str_to_bit(method_code.upper()) |
|
352
|
|
|
except AttributeError: |
|
353
|
|
|
bit_code = method_code |
|
354
|
|
|
|
|
355
|
|
|
if not isinstance(bit_code, int): |
|
356
|
|
|
raise ValueError("unknown method code {:}".format(method_code)) |
|
357
|
|
|
|
|
358
|
|
|
# Test height |
|
359
|
|
|
if not test_height(np.nanmax(height), bit_code): |
|
360
|
|
|
return lat_out, lon_out, r_out |
|
361
|
|
|
|
|
362
|
|
|
# Test latitude range |
|
363
|
|
|
if np.abs(in_lat).max() > 90.0: |
|
364
|
|
|
if np.abs(in_lat).max() > 90.1: |
|
365
|
|
|
raise ValueError('unrealistic latitude') |
|
366
|
|
|
in_lat = np.clip(in_lat, -90.0, 90.0) |
|
367
|
|
|
|
|
368
|
|
|
# Constrain longitudes between -180 and 180 |
|
369
|
|
|
in_lon = ((in_lon + 180.0) % 360.0) - 180.0 |
|
370
|
|
|
|
|
371
|
|
|
|
|
372
|
|
|
# Set current date and time |
|
373
|
|
|
try: |
|
374
|
|
|
c_aacgmv2.set_datetime(dtime.year, dtime.month, dtime.day, dtime.hour, |
|
375
|
|
|
dtime.minute, dtime.second) |
|
376
|
|
|
except TypeError as terr: |
|
377
|
|
|
raise TypeError("unable to set time for {:}: {:}".format(dtime, terr)) |
|
378
|
|
|
except RuntimeError as rerr: |
|
379
|
|
|
raise RuntimeError("unable to set time for {:}: {:}".format(dtime, |
|
380
|
|
|
rerr)) |
|
381
|
|
|
|
|
382
|
|
|
# Vectorise the AACGM C routine |
|
383
|
|
|
convert_vectorised = np.vectorize(c_aacgmv2.convert) |
|
384
|
|
|
|
|
385
|
|
|
# convert |
|
386
|
|
|
try: |
|
387
|
|
|
lat_out, lon_out, r_out = convert_vectorised(in_lat, in_lon, height, |
|
388
|
|
|
bit_code) |
|
389
|
|
|
|
|
390
|
|
|
except: |
|
391
|
|
|
err = sys.exc_info()[0] |
|
392
|
|
|
estr = "unable to perform vector conversion at {:} using ".format(dtime) |
|
393
|
|
|
estr = "{:s}method {:}: {:}".format(estr, bit_code, err) |
|
394
|
|
|
aacgmv2.logger.warning(estr) |
|
395
|
|
|
pass |
|
396
|
|
|
|
|
397
|
|
|
return lat_out, lon_out, r_out |
|
398
|
|
|
|
|
399
|
|
|
def get_aacgm_coord(glat, glon, height, dtime, method="TRACE"): |
|
400
|
|
|
"""Get AACGM latitude, longitude, and magnetic local time |
|
401
|
|
|
|
|
402
|
|
|
Parameters |
|
403
|
|
|
------------ |
|
404
|
|
|
glat : (float) |
|
405
|
|
|
Geodetic latitude in degrees N |
|
406
|
|
|
glon : (float) |
|
407
|
|
|
Geodetic longitude in degrees E |
|
408
|
|
|
height : (float) |
|
409
|
|
|
Altitude above the surface of the earth in km |
|
410
|
|
|
dtime : (datetime) |
|
411
|
|
|
Date and time to calculate magnetic location |
|
412
|
|
|
method : (str) |
|
413
|
|
|
String denoting which type(s) of conversion to perform |
|
414
|
|
|
TRACE - use field-line tracing, not coefficients |
|
415
|
|
|
ALLOWTRACE - use trace only above 2000 km |
|
416
|
|
|
BADIDEA - use coefficients above 2000 km |
|
417
|
|
|
GEOCENTRIC - assume inputs are geocentric w/ RE=6371.2 |
|
418
|
|
|
(default = "TRACE") |
|
419
|
|
|
|
|
420
|
|
|
Returns |
|
421
|
|
|
------- |
|
422
|
|
|
mlat : (float) |
|
423
|
|
|
magnetic latitude in degrees N |
|
424
|
|
|
mlon : (float) |
|
425
|
|
|
magnetic longitude in degrees E |
|
426
|
|
|
mlt : (float) |
|
427
|
|
|
magnetic local time in hours |
|
428
|
|
|
|
|
429
|
|
|
""" |
|
430
|
|
|
# Initialize method code |
|
431
|
|
|
method_code = "G2A|{:s}".format(method) |
|
432
|
|
|
|
|
433
|
|
|
# Get magnetic lat and lon. |
|
434
|
|
|
mlat, mlon, _ = convert_latlon(glat, glon, height, dtime, |
|
435
|
|
|
method_code=method_code) |
|
436
|
|
|
|
|
437
|
|
|
# Get magnetic local time |
|
438
|
|
|
mlt = np.nan if np.isnan(mlon) else convert_mlt(mlon, dtime, m2a=False) |
|
439
|
|
|
|
|
440
|
|
|
return mlat, mlon, mlt |
|
441
|
|
|
|
|
442
|
|
|
|
|
443
|
|
|
def get_aacgm_coord_arr(glat, glon, height, dtime, method="TRACE"): |
|
444
|
|
|
"""Get AACGM latitude, longitude, and magnetic local time |
|
445
|
|
|
|
|
446
|
|
|
Parameters |
|
447
|
|
|
------------ |
|
448
|
|
|
glat : (np.array or list) |
|
449
|
|
|
Geodetic latitude in degrees N |
|
450
|
|
|
glon : (np.array or list) |
|
451
|
|
|
Geodetic longitude in degrees E |
|
452
|
|
|
height : (np.array or list) |
|
453
|
|
|
Altitude above the surface of the earth in km |
|
454
|
|
|
dtime : (datetime) |
|
455
|
|
|
Date and time to calculate magnetic location |
|
456
|
|
|
method : (str) |
|
457
|
|
|
String denoting which type(s) of conversion to perform |
|
458
|
|
|
TRACE - use field-line tracing, not coefficients |
|
459
|
|
|
ALLOWTRACE - use trace only above 2000 km |
|
460
|
|
|
BADIDEA - use coefficients above 2000 km |
|
461
|
|
|
GEOCENTRIC - assume inputs are geocentric w/ RE=6371.2 |
|
462
|
|
|
(default = "TRACE") |
|
463
|
|
|
(default = "TRACE") |
|
464
|
|
|
|
|
465
|
|
|
Returns |
|
466
|
|
|
------- |
|
467
|
|
|
mlat : (float) |
|
468
|
|
|
magnetic latitude in degrees N |
|
469
|
|
|
mlon : (float) |
|
470
|
|
|
magnetic longitude in degrees E |
|
471
|
|
|
mlt : (float) |
|
472
|
|
|
magnetic local time in hours |
|
473
|
|
|
|
|
474
|
|
|
""" |
|
475
|
|
|
# Initialize method code |
|
476
|
|
|
method_code = "G2A|{:s}".format(method) |
|
477
|
|
|
|
|
478
|
|
|
# Get magnetic lat and lon. |
|
479
|
|
|
mlat, mlon, _ = convert_latlon_arr(glat, glon, height, dtime, |
|
480
|
|
|
method_code=method_code) |
|
481
|
|
|
|
|
482
|
|
|
if np.all(np.isnan(mlon)): |
|
483
|
|
|
mlt = np.full(shape=mlat.shape, fill_value=np.nan) |
|
484
|
|
|
else: |
|
485
|
|
|
# Get magnetic local time |
|
486
|
|
|
mlt = convert_mlt(mlon, dtime, m2a=False) |
|
487
|
|
|
|
|
488
|
|
|
return mlat, mlon, mlt |
|
489
|
|
|
|
|
490
|
|
|
def convert_str_to_bit(method_code): |
|
491
|
|
|
"""convert string code specification to bit code specification |
|
492
|
|
|
|
|
493
|
|
|
Parameters |
|
494
|
|
|
------------ |
|
495
|
|
|
method_code : (str) |
|
496
|
|
|
Bitwise code for passing options into converter (default=0) |
|
497
|
|
|
G2A - geographic (geodetic) to AACGM-v2 |
|
498
|
|
|
A2G - AACGM-v2 to geographic (geodetic) |
|
499
|
|
|
TRACE - use field-line tracing, not coefficients |
|
500
|
|
|
ALLOWTRACE - use trace only above 2000 km |
|
501
|
|
|
BADIDEA - use coefficients above 2000 km |
|
502
|
|
|
GEOCENTRIC - assume inputs are geocentric w/ RE=6371.2 |
|
503
|
|
|
|
|
504
|
|
|
Returns |
|
505
|
|
|
-------- |
|
506
|
|
|
bit_code : (int) |
|
507
|
|
|
Method code specification in bits |
|
508
|
|
|
|
|
509
|
|
|
Notes |
|
510
|
|
|
-------- |
|
511
|
|
|
Multiple codes should be seperated by pipes '|'. Invalid parts of the code |
|
512
|
|
|
are ignored and no code defaults to 'G2A'. |
|
513
|
|
|
|
|
514
|
|
|
""" |
|
515
|
|
|
|
|
516
|
|
|
convert_code = {"G2A": c_aacgmv2.G2A, "A2G": c_aacgmv2.A2G, |
|
517
|
|
|
"TRACE": c_aacgmv2.TRACE, "BADIDEA": c_aacgmv2.BADIDEA, |
|
518
|
|
|
"GEOCENTRIC": c_aacgmv2.GEOCENTRIC, |
|
519
|
|
|
"ALLOWTRACE": c_aacgmv2.ALLOWTRACE} |
|
520
|
|
|
|
|
521
|
|
|
# Force upper case, remove any spaces, and split along pipes |
|
522
|
|
|
method_codes = method_code.upper().replace(" ", "").split("|") |
|
523
|
|
|
|
|
524
|
|
|
# Add the valid parts of the code, invalid elements are ignored |
|
525
|
|
|
bit_code = sum([convert_code[k] for k in method_codes |
|
526
|
|
|
if k in convert_code.keys()]) |
|
527
|
|
|
|
|
528
|
|
|
return bit_code |
|
529
|
|
|
|
|
530
|
|
|
def convert_bool_to_bit(a2g=False, trace=False, allowtrace=False, |
|
531
|
|
|
badidea=False, geocentric=False): |
|
532
|
|
|
"""convert boolian flags to bit code specification |
|
533
|
|
|
|
|
534
|
|
|
Parameters |
|
535
|
|
|
---------- |
|
536
|
|
|
a2g : (bool) |
|
537
|
|
|
True for AACGM-v2 to geographic (geodetic), False otherwise |
|
538
|
|
|
(default=False) |
|
539
|
|
|
trace : (bool) |
|
540
|
|
|
If True, use field-line tracing, not coefficients (default=False) |
|
541
|
|
|
allowtrace : (bool) |
|
542
|
|
|
If True, use trace only above 2000 km (default=False) |
|
543
|
|
|
badidea : (bool) |
|
544
|
|
|
If True, use coefficients above 2000 km (default=False) |
|
545
|
|
|
geocentric : (bool) |
|
546
|
|
|
True for geodetic, False for geocentric w/RE=6371.2 (default=False) |
|
547
|
|
|
|
|
548
|
|
|
Returns |
|
549
|
|
|
-------- |
|
550
|
|
|
bit_code : (int) |
|
551
|
|
|
code specification in bits |
|
552
|
|
|
|
|
553
|
|
|
""" |
|
554
|
|
|
|
|
555
|
|
|
bit_code = c_aacgmv2.A2G if a2g else c_aacgmv2.G2A |
|
556
|
|
|
|
|
557
|
|
|
if trace: |
|
558
|
|
|
bit_code += c_aacgmv2.TRACE |
|
559
|
|
|
if allowtrace: |
|
560
|
|
|
bit_code += c_aacgmv2.ALLOWTRACE |
|
561
|
|
|
if badidea: |
|
562
|
|
|
bit_code += c_aacgmv2.BADIDEA |
|
563
|
|
|
if geocentric: |
|
564
|
|
|
bit_code += c_aacgmv2.GEOCENTRIC |
|
565
|
|
|
|
|
566
|
|
|
return bit_code |
|
567
|
|
|
|
|
568
|
|
|
def convert_mlt(arr, dtime, m2a=False): |
|
569
|
|
|
"""Converts between magnetic local time (MLT) and AACGM-v2 longitude |
|
570
|
|
|
|
|
571
|
|
|
Parameters |
|
572
|
|
|
------------ |
|
573
|
|
|
arr : (array_line or float) |
|
574
|
|
|
Magnetic longitudes (degrees E) or MLTs (hours) to convert |
|
575
|
|
|
dtime : (datetime.datetime) |
|
576
|
|
|
Date and time for MLT conversion in Universal Time (UT). |
|
577
|
|
|
m2a : (bool) |
|
578
|
|
|
Convert MLT to AACGM-v2 longitude (True) or magnetic longitude to MLT |
|
579
|
|
|
(False). (default=False) |
|
580
|
|
|
|
|
581
|
|
|
Returns |
|
582
|
|
|
-------- |
|
583
|
|
|
out : (np.ndarray) |
|
584
|
|
|
Converted coordinates/MLT in degrees E or hours (as appropriate) |
|
585
|
|
|
|
|
586
|
|
|
Notes |
|
587
|
|
|
------- |
|
588
|
|
|
This routine previously based on Laundal et al. 2016, but now uses the |
|
589
|
|
|
improved calculation available in AACGM-V2.4. |
|
590
|
|
|
|
|
591
|
|
|
""" |
|
592
|
|
|
|
|
593
|
|
|
# Test time |
|
594
|
|
|
dtime = test_time(dtime) |
|
595
|
|
|
|
|
596
|
|
|
# Calculate desired location, C routines set date and time |
|
597
|
|
|
if m2a: |
|
598
|
|
|
# Get the magnetic longitude |
|
599
|
|
|
inv_vectorised = np.vectorize(c_aacgmv2.inv_mlt_convert) |
|
600
|
|
|
out = inv_vectorised(dtime.year, dtime.month, dtime.day, dtime.hour, |
|
601
|
|
|
dtime.minute, dtime.second, arr) |
|
602
|
|
|
else: |
|
603
|
|
|
# Get magnetic local time |
|
604
|
|
|
mlt_vectorised = np.vectorize(c_aacgmv2.mlt_convert) |
|
605
|
|
|
out = mlt_vectorised(dtime.year, dtime.month, dtime.day, dtime.hour, |
|
606
|
|
|
dtime.minute, dtime.second, arr) |
|
607
|
|
|
|
|
608
|
|
|
if hasattr(out, "shape") and out.shape == (): |
|
609
|
|
|
out = float(out) |
|
610
|
|
|
|
|
611
|
|
|
return out |
|
612
|
|
|
|