From 1747772fb0cbf4587749e491556b57ffae5d6480 Mon Sep 17 00:00:00 2001 From: ketiltrout Date: Wed, 24 Jul 2024 18:39:46 -0700 Subject: [PATCH] refactor(ephemeris): Use ch_ephem This re-imports stuff moved to `ch_ephem`. It both re-imports everything that was moved back into `ch_util.ephemeris` for backwards compatibility, but also removes references to `ch_util.epheremis` from the code, using the newly-exported versions of things directly. This PR requires both: * https://github.com/radiocosmology/caput/pull/271 * https://github.com/chime-experiment/ch_ephem/pull/1 Catalogs: All the catalogs have been moved to `ch_ephem`, which provides a standard interface to them via `ch_ephem.catalogs.load`. To make this change, `fluxcat.FluxCatalog.load` has been broken into two pieces. The new `fluxcat.FluxCatalog.load_dict` imports a catalog from an already-parsed JSON dict (which is what `ch_ephem` provides). The original `fluxcat.FluxCatalog.load` works as it used to, but tail-calls `load_dict` to do most of the importing. Position data: Position data (lat, lon, alt) is now obtained by fetching the parameter out of the `caput.time.Observer` objects provided by `ch_ephem`. The constants in `ch_util.ephemeris` are populated by doing this. Instrument geormetry: `ch_ephem` has also taken on the geometry data (rotation, roll, offset) that was in `tools` (where it's been re-imported from `ch_ephem`). Private objects deleted: I've also deleted a number of private objects which are no longer being used (i.e. objects whose names start with a leading underscore). Notable among these are the geometry constants from `ch_util.tools` and the unused`ch_util.tools._LAT_LON` which had position data for various instruments which differed from the position data provided by `ch_util.ephemeris`. Also removed are the long-deprectated `ch_util.ephemeris._get_chime` and `ch_util.ephemeris.transit_RA`. --- ch_util/cal_utils.py | 23 +- ch_util/catalogs/atnf_psrcat.json | 2569 -- ch_util/catalogs/hfb_target_list.json | 1582 - .../primary_calibrators_perley2016.json | 3223 -- .../catalogs/specfind_v2_5Jy_vollmer2009.json | 31141 ---------------- ch_util/chan_monitor.py | 22 +- ch_util/data_quality.py | 15 +- ch_util/ephemeris.py | 955 +- ch_util/finder.py | 33 +- ch_util/fluxcat.py | 46 +- ch_util/hfbcat.py | 21 +- ch_util/holography.py | 28 +- ch_util/plot.py | 4 +- ch_util/rfi.py | 10 +- ch_util/tools.py | 130 +- requirements.txt | 1 + setup.py | 5 - tests/test_ephemeris.py | 95 - 18 files changed, 241 insertions(+), 39662 deletions(-) delete mode 100644 ch_util/catalogs/atnf_psrcat.json delete mode 100644 ch_util/catalogs/hfb_target_list.json delete mode 100644 ch_util/catalogs/primary_calibrators_perley2016.json delete mode 100644 ch_util/catalogs/specfind_v2_5Jy_vollmer2009.json delete mode 100644 tests/test_ephemeris.py diff --git a/ch_util/cal_utils.py b/ch_util/cal_utils.py index 2f6f8d4f..fff0f351 100644 --- a/ch_util/cal_utils.py +++ b/ch_util/cal_utils.py @@ -17,9 +17,14 @@ from scipy.linalg import lstsq, inv from caput import memh5, time as ctime + from chimedb import dataset as ds from chimedb.dataset.utils import state_id_of_type, unique_unmasked_entry -from ch_util import ephemeris, tools + +from ch_ephem.observers import chime +import ch_ephem.sources + +from ch_util import tools # Set up logging logger = logging.getLogger(__name__) @@ -2474,13 +2479,13 @@ def thermal_amplitude(delta_T, freq): def _el_to_dec(el): """Convert from el = sin(zenith angle) to declination in degrees.""" - return np.degrees(np.arcsin(el)) + ephemeris.CHIMELATITUDE + return np.degrees(np.arcsin(el)) + chime.latitude def _dec_to_el(dec): """Convert from declination in degrees to el = sin(zenith angle).""" - return np.sin(np.radians(dec - ephemeris.CHIMELATITUDE)) + return np.sin(np.radians(dec - chime.latitude)) def get_reference_times_file( @@ -2691,10 +2696,10 @@ def get_reference_times_dataset_id( # The CHIME calibration sources _source_dict = { - "cyga": ephemeris.CygA, - "casa": ephemeris.CasA, - "taua": ephemeris.TauA, - "vira": ephemeris.VirA, + "cyga": ch_ephem.sources.CygA, + "casa": ch_ephem.sources.CasA, + "taua": ch_ephem.sources.TauA, + "vira": ch_ephem.sources.VirA, } # Get the set of gain IDs for each time stamp @@ -2728,9 +2733,7 @@ def get_reference_times_dataset_id( # Calculate the source transit time, and sanity check it source = _source_dict[d["source_name"]] - d["source_transit"] = ephemeris.transit_times( - source, d["gen_time"] - 24 * 3600.0 - ) + d["source_transit"] = chime.transit_times(source, d["gen_time"] - 24 * 3600.0) cal_diff_hours = (d["gen_time"] - d["source_transit"]) / 3600 if cal_diff_hours > 3: logger.warn( diff --git a/ch_util/catalogs/atnf_psrcat.json b/ch_util/catalogs/atnf_psrcat.json deleted file mode 100644 index aeb53534..00000000 --- a/ch_util/catalogs/atnf_psrcat.json +++ /dev/null @@ -1,2569 +0,0 @@ -{ - "B0329+54": { - "ra": 53.247539999999994, - "dec": 54.578702500000006, - "alternate_names": [ - "J0332+5434", - "B0329+54" - ], - "model": "CurvedPowerLaw", - "model_kwargs": { - "nparam": 3, - "freq_pivot": 600.0 - }, - "stats": { - "ndof": 4, - "chisq": 6.095237238185315 - }, - "param": [ - 0.9692717928383052, - -1.4613181794011147, - -0.358717917347395 - ], - "param_cov": [ - [ - 0.007445843145392445, - -0.00017327557241528216, - -0.002055990012580111 - ], - [ - -0.00017327557241528178, - 0.013684258886520962, - 0.002289940986873935 - ], - [ - -0.002055990012580111, - 0.0022899409868739353, - 0.00417852845977159 - ] - ], - "measurements": [ - [ - 50.0, - 4.16, - 2.08, - 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(1991)" - ] - ] - }, - "3C_441": { - "ra": 331.52049, - "dec": 29.48888, - "alternate_names": [ - "VLSS_J2206.0+2929", - "3C_441", - "3C_441.0", - "3CR_441", - "4C_29.65", - "B2_2203+29", - "B2.1_2203+29", - "B2.2_2203+29", - "BWE_2203+2914", - "CTD_164", - "CUL_2203+292", - "DA_573", - "GB6_B2203+2914", - "LHE_515", - "MITG_J220605+2929", - "NRAO_678", - "NVSS_J220604+292921", - "S1_2203+29", - "TXS_2203+292", - "VRO_29.22.02", - "WB_2203+2914", - "[HB91]_2203+292", - "87GB_220348.3+291422", - "WN_B2203.8+2914", - "[MMD97]_220349.46+291442.9" - ], - "model": "CurvedPowerLaw", - "model_kwargs": { - "freq_pivot": 600.0, - "nparam": 2 - }, - "stats": { - "chisq": 1.98320829427, - "ndof": 13 - }, - "param": [ - 5.03577400697, - -0.831831221963 - ], - "param_cov": [ - [ - 0.0710123654515, - -0.000453883874251 - ], - [ - -0.000453883874251, - 0.00125207662676 - ] - ], - "measurements": [ - [ - 74.0, - 27.3, - 5.5, - true, - "VLSS", - 2007.0, - "Cohen et al. 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(1990, 1991)" - ] - ] - }, - "4C_39.56": { - "ra": 275.3369, - "dec": 39.71242, - "alternate_names": [ - "WISE_J182120.89+394244.8", - "4C_39.56", - "B2_1819+39", - "B2.3_1819+39", - "B3_1819+396", - "BWE_1819+3941", - "CJ1_1819+396", - "DA_449", - "GB6_B1819+3941", - "LEDA_2820627", - "MITG_J182119+3942", - "NVSS_J182120+394245", - "OHIO_U_332.9", - "S4_1819+396", - "S4_1819+39", - "TXS_1819+396", - "WB_1819+3941", - "[PW82]_1819+39", - "87GB_181941.9+394113", - "WN_B1819.7+3941", - "[VV2000]_J182120.8+394245", - "[VV2003]_J182120.8+394245", - "[VV2006]_J182120.8+394245", - "[VV98]_J182120.8+394245", - "[VV2010]_J182120.8+394245" - ], - "model": "CurvedPowerLaw", - "model_kwargs": { - "freq_pivot": 600.0, - "nparam": 2 - }, - "stats": { - "chisq": 5.76525921286, - "ndof": 7 - }, - "param": [ - 5.02797034445, - -0.705301233544 - ], - "param_cov": [ - [ - 0.154928860455, - -0.0121921706737 - ], - [ - -0.0121921706737, - 0.00353334796229 - ] - ], - "measurements": [ - [ - 325.0, - 7.03, - 1.4, - true, - "WN", - null, - null - ], - [ - 365.0, - 6.96, - 1.4, - true, - "TXS", - 1991.0, - "Large et al. (1991)" - ], - [ - 408.0, - 6.33, - 1.3, - true, - "B2.3", - null, - null - ], - [ - 408.0, - 5.98, - 1.2, - true, - "B3", - 1985.0, - "Ficarra et al. (1985)" - ], - [ - 1400.0, - 3.51, - 0.7, - true, - "NVSS", - 1998.0, - "Condon et al. (1998)" - ], - [ - 1400.0, - 3.74, - 0.75, - true, - "WB", - 1992.0, - "White & Becker (1992)" - ], - [ - 4850.0, - 0.985, - 0.2, - true, - "GB6", - 1996.0, - "Gregory et al. (1996)" - ], - [ - 4850.0, - 1.22, - 0.24, - true, - "87GB", - 1991.0, - "Gregory & Condon (1991)" - ], - [ - 4850.0, - 0.958, - 0.19, - true, - "MITG", - 1991.0, - "Bennett et al. (1986), Langston et al. (1990), Griffith et al. (1990, 1991)" - ] - ] - }, - "PKS_2318-16": { - "ra": 350.25838, - "dec": -16.38474, - "alternate_names": [ - "VLSS_J2321.0-1623", - "CUL_2318-166", - "LEDA_2831700", - "MRC_2318-166", - "MSH_23-1-08", - "NVSS_J232102-162305", - "PKS_2318-16", - "PKS_J2321-1622", - "PKS_2318-166", - "PMN_J2321-1623", - "TXS_2318-166", - "WISH_B2318.4-1639", - "AT20G_J232102-162305" - ], - "model": "CurvedPowerLaw", - "model_kwargs": { - "freq_pivot": 600.0, - "nparam": 2 - }, - "stats": { - "chisq": 6.27490200814, - "ndof": 6 - }, - "param": [ - 5.02549786336, - -0.94991726291 - ], - "param_cov": [ - [ - 0.127999100671, - 0.000866374041369 - ], - [ - 0.000866374041369, - 0.00285282659213 - ] - ], - "measurements": [ - [ - 74.0, - 26.3, - 5.3, - true, - "VLSS", - 2007.0, - "Cohen et al. (2007)" - ], - [ - 160.0, - 18.5, - 3.7, - true, - "Culb", - 1995.0, - "Slee (1995)" - ], - [ - 325.0, - 9.68, - 1.9, - true, - "WISH", - 2002.0, - "de Breuck et al. (2002)" - ], - [ - 365.0, - 10.3, - 2.1, - true, - "TXS", - 1991.0, - "Large et al. (1991)" - ], - [ - 408.0, - 8.75, - 1.8, - true, - "MRC", - 1996.0, - "Douglas et al. (1996)" - ], - [ - 1400.0, - 2.36, - 0.47, - true, - "NVSS", - 1998.0, - "Condon et al. (1998)" - ], - [ - 2700.0, - 1.0, - 0.2, - true, - "PKS", - 1991.0, - "Otrupcek & Wright (1991)" - ], - [ - 4850.0, - 0.64, - 0.13, - true, - "PMN", - 1996.0, - "Wright et al. (1994, 1996), Griffith et al. (1994, 1995)" - ] - ] - } -} \ No newline at end of file diff --git a/ch_util/chan_monitor.py b/ch_util/chan_monitor.py index 5147fb35..37e0e844 100644 --- a/ch_util/chan_monitor.py +++ b/ch_util/chan_monitor.py @@ -5,8 +5,11 @@ import caput.time as ctime +from ch_ephem.observers import chime +import ch_ephem.sources + from chimedb import data_index -from ch_util import ephemeris, finder +from ch_util import finder # Corrections to transit times due to 2deg rotation of cylinders: TTCORR = {"CygA": -94.4, "CasA": 152.3, "TauA": -236.9, "VirA": -294.5} @@ -16,7 +19,7 @@ [[np.cos(CR), -np.sin(CR)], [np.sin(CR), np.cos(CR)]] ) # Cylinder rotation matrix C = 2.9979e8 -PHI = ephemeris.CHIMELATITUDE * np.pi / 180.0 # DRAO Latitue +PHI = chime.latitude * np.pi / 180.0 # DRAO Latitue SD = 24.0 * 3600.0 * ctime.SIDEREAL_S # Sidereal day _DEFAULT_NODE_SPOOF = {"scinet_online": "/scratch/k/krs/jrs65/chime/archive/online/"} @@ -88,12 +91,12 @@ def __init__( if self.source2 is not None: self.dec2 = self.source2._dec self.tt1 = ( - ephemeris.transit_times(self.source1, self.tm1[0], self.tm1[-1])[0] + chime.transit_times(self.source1, self.tm1[0], self.tm1[-1])[0] + TTCORR[self.source1.name] ) if self.source2 is not None: self.tt2 = ( - ephemeris.transit_times(self.source2, self.tm2[0], self.tm2[-1])[0] + chime.transit_times(self.source2, self.tm2[0], self.tm2[-1])[0] + TTCORR[self.source2.name] ) @@ -1135,7 +1138,12 @@ def get_sunfree_srcs(self, srcs=None): self.set_acq_list() if srcs is None: - srcs = [ephemeris.CygA, ephemeris.CasA, ephemeris.TauA, ephemeris.VirA] + srcs = [ + ch_ephem.sources.CygA, + ch_ephem.sources.CasA, + ch_ephem.sources.TauA, + ch_ephem.sources.VirA, + ] Ns = len(srcs) clr = [False] * Ns @@ -1145,7 +1153,7 @@ def get_sunfree_srcs(self, srcs=None): night_transit = np.array([]) for acq in self.night_acq_list: night_transit = np.append( - night_transit, ephemeris.transit_times(src, *acq[1]) + night_transit, chime.transit_times(src, *acq[1]) ) if night_transit.size: @@ -1154,7 +1162,7 @@ def get_sunfree_srcs(self, srcs=None): if src.name in ["CygA", "CasA"]: transit = np.array([]) for acq in self.acq_list: - transit = np.append(transit, ephemeris.transit_times(src, *acq[1])) + transit = np.append(transit, chime.transit_times(src, *acq[1])) if transit.size: clr[ii] = True diff --git a/ch_util/data_quality.py b/ch_util/data_quality.py index 21834a75..6260c68b 100644 --- a/ch_util/data_quality.py +++ b/ch_util/data_quality.py @@ -18,7 +18,6 @@ import caput.time as ctime -import ch_util.ephemeris as ch_eph from ch_util import andata from ch_util import tools from ch_util import ni_utils @@ -496,14 +495,16 @@ def _cut_daytime(visi, tmstp): Returns a list of arrays if multiple nights are present. """ + from ch_ephem.observers import chime + tstp = tmstp[1] - tmstp[0] # Get time step - risings = ch_eph.solar_rising(tmstp[0], tmstp[-1]) - settings = ch_eph.solar_setting(tmstp[0], tmstp[-1]) + risings = chime.solar_rising(tmstp[0], tmstp[-1]) + settings = chime.solar_setting(tmstp[0], tmstp[-1]) if len(risings) == 0 and len(settings) == 0: - next_rising = ch_eph.solar_rising(tmstp[-1]) - next_setting = ch_eph.solar_setting(tmstp[-1]) + next_rising = chime.solar_rising(tmstp[-1]) + next_setting = chime.solar_setting(tmstp[-1]) if next_setting < next_rising: # All data is in daylight time @@ -690,13 +691,15 @@ def _cut_sun_transit(cut_vis, tmstp, tcut=120.0): """ + from ch_ephem.observers import chime + # Start looking for transits tcut minutes before start time: st_time = tmstp[0] - tcut * 60.0 # Stop looking for transits tcut minutes after end time: end_time = tmstp[-1] + tcut * 60.0 # Find Sun transits between start time and end time: - sun_trans = ch_eph.solar_transit(st_time, end_time) + sun_trans = chime.solar_transit(st_time, end_time) cut_tmstp = tmstp # Time stamps to be cut tstp = tmstp[1] - tmstp[0] # Get time step diff --git a/ch_util/ephemeris.py b/ch_util/ephemeris.py index 395eeafe..71934d34 100644 --- a/ch_util/ephemeris.py +++ b/ch_util/ephemeris.py @@ -1,111 +1,13 @@ """ -Ephemeris routines +This module is deprecated. -The precession of the Earth's axis gives noticeable shifts in object -positions over the life time of CHIME. To minimise the effects of this we -need to be careful and consistent with our ephemeris calculations. -Historically Right Ascension has been given with respect to the Vernal -Equinox which has a significant (and unnecessary) precession in the origin of -the RA axis. To avoid this we use the new Celestial Intermediate Reference -System which does not suffer from this issue. - -Practically this means that when calculating RA, DEC coordinates for a source -position at a *given time* you must be careful to obtain CIRS coordinates -(and not equinox based ones). Internally using `ephemeris.object_coords` does -exactly that for you, so for any lookup of coordinates you should use that on -your requested body. - -Note that the actual coordinate positions of sources must be specified using -RA, DEC coordinates in ICRS (which is roughly equivalent to J2000). The -purpose of object_coords is to transform into new RA, DEC coordinates taking -into account the precession and nutation of the Earth's polar axis since -then. - -These kind of coordinate issues are tricky, confusing and hard to debug years -later, so if you're unsure you are recommended to seek some advice. - -Constants -========= - -:const:`CHIMELATITUDE` - CHIME's latitude [degrees]. -:const:`CHIMELONGITUDE` - CHIME's longitude [degrees]. -:const:`CHIMEALTITUDE` - CHIME's altitude [metres]. -:const:`SIDEREAL_S` - Number of SI seconds in a sidereal second [s/sidereal s]. You probably want - STELLAR_S instead. -:const:`STELLAR_S` - Number of SI seconds in a stellar second [s/stellar s]. -:const:`CasA` - :class:`skyfield.starlib.Star` representing Cassiopeia A. -:const:`CygA` - :class:`skyfield.starlib.Star` representing Cygnus A. -:const:`TauA` - :class:`skyfield.starlib.Star` representing Taurus A. -:const:`VirA` - :class:`skyfield.starlib.Star` representing Virgo A. - - -Telescope Instances -=================== - -- :const:`chime` - - -Ephemeris Functions -=================== - -- :py:meth:`skyfield_star_from_ra_dec` -- :py:meth:`transit_times` -- :py:meth:`solar_transit` -- :py:meth:`lunar_transit` -- :py:meth:`setting_times` -- :py:meth:`solar_setting` -- :py:meth:`lunar_setting` -- :py:meth:`rising_times` -- :py:meth:`solar_rising` -- :py:meth:`lunar_rising` -- :py:meth:`_is_skyfield_obj` -- :py:meth:`peak_RA` -- :py:meth:`get_source_dictionary` -- :py:meth:`lsa` - - -Time Utilities -============== - -- :py:meth:`ensure_unix` -- :py:meth:`chime_local_datetime` -- :py:meth:`unix_to_datetime` -- :py:meth:`datetime_to_unix` -- :py:meth:`datetime_to_timestr` -- :py:meth:`timestr_to_datetime` -- :py:meth:`unix_to_skyfield_time` -- :py:meth:`skyfield_time_to_unix` -- :py:meth:`time_of_day` -- :py:meth:`csd` -- :py:meth:`csd_to_unix` -- :py:meth:`unix_to_csd` -- :py:meth:`parse_date` - - -Miscellaneous Utilities -======================= - -- :py:meth:`galt_pointing_model_ha` -- :py:meth:`galt_pointing_model_dec` +For CHIME-specific stuff, use `ch_ephem`. +For instrument-independent stuff, use `caput`. """ -from datetime import datetime -from typing import Union -from numpy.core.multiarray import unravel_index +import warnings -# NOTE: Load Skyfield API but be sure to use skyfield_wrapper for loading data -import skyfield.api - -import numpy as np +warnings.warn("The ch_util.ephemeris module is deprecated.", DeprecationWarning) from caput.interferometry import sphdist from caput.time import ( @@ -125,283 +27,52 @@ STELLAR_S, ) -# Calvin derived the horizontal position of the center of the focal lines... -# ...and the elevation of the focal line from survey coordinates: -# All altitudes given in meters above sea level -CHIMELATITUDE = 49.3207092194 -CHIMELONGITUDE = -119.6236774310 -CHIMEALTITUDE = 555.372 - -# Calvin also positioned the GBO/TONE Outrigger similarly. -# GBO/TONE Outrigger -TONELATITUDE = 38.4292962636 -TONELONGITUDE = -79.8451625395 -TONEALTITUDE = 810.000 - -# Rough position for outriggers. -# These will be updated as positioning gets refined. -# https://bao.chimenet.ca/doc/documents/1727 -KKOLATITUDE = 49.41905 -KKOLONGITUDE = -120.5253 -KKOALTITUDE = 835 - -# Aliases for backwards compatibility -PCOLATITUDE = KKOLATITUDE -PCOLONGITUDE = KKOLONGITUDE -PCOALTITUDE = KKOALTITUDE - -GBOLATITUDE = 38.436122 -GBOLONGITUDE = -79.827922 -GBOALTITUDE = 2710 / 3.28084 - -HCOLATITUDE = 40.8171082 -HCOLONGITUDE = -121.4689584 -HCOALTITUDE = 3346 / 3.28084 - -# Create the Observer instances for CHIME and outriggers -chime = Observer( - lon=CHIMELONGITUDE, - lat=CHIMELATITUDE, - alt=CHIMEALTITUDE, - lsd_start=datetime(2013, 11, 15), -) - -tone = Observer( - lon=TONELONGITUDE, - lat=TONELATITUDE, - alt=TONEALTITUDE, - lsd_start=datetime(2013, 11, 15), -) - -kko = Observer( - lon=KKOLONGITUDE, - lat=KKOLATITUDE, - alt=KKOALTITUDE, - lsd_start=datetime(2013, 11, 15), -) - -gbo = Observer( - lon=GBOLONGITUDE, - lat=GBOLATITUDE, - alt=GBOALTITUDE, - lsd_start=datetime(2013, 11, 15), +from ch_ephem.coord import star_cirs as Star_cirs +from ch_ephem.coord import peak_ra as peak_RA +from ch_ephem.coord import ( + cirs_radec, + object_coords, + hadec_to_bmxy, + bmxy_to_hadec, + get_range_rate, ) +from ch_ephem.pointing import galt_pointing_model_ha, galt_pointing_model_dec +from ch_ephem.sources import get_source_dictionary, CasA, CygA, TauA, VirA +from ch_ephem.time import parse_date, utc_lst_to_mjd, chime_local_datetime +import ch_ephem.observers -hco = Observer( - lon=HCOLONGITUDE, - lat=HCOLATITUDE, - alt=HCOALTITUDE, - lsd_start=datetime(2013, 11, 15), -) - - -def _get_chime(): - import warnings - - warnings.warn("Use `ephemeris.chime` instead.", DeprecationWarning) - return chime - - -def galt_pointing_model_ha( - ha_in, dec_in, a=[-5.872, -0.5292, 5.458, -0.076, -0.707, 0.0, 0.0] -): - """Calculate pointing correction in hour angle for the Galt Telescope - See description of the pointing model by Lewis Knee CHIME document library - 754 https://bao.chimenet.ca/doc/documents/754 - - Parameters - ---------- - ha, dec : Skyfield Angle objects - Target hour angle and declination - - a : list of floats - List of coefficients (in arcmin) for the pointing model - (NOTE: it is very unlikely that a user will want to change these - from the defaults, which are taken from the pointing model as of - 2019-2-15) - - Returns - ------- - Skyfield Angle object - Angular offset in hour angle - """ - - from skyfield.positionlib import Angle - - ha = ha_in.radians - dec = dec_in.radians - - # hour angle pointing correction in arcmin - delta_ha_cos_dec = ( - a[0] - + a[1] * np.sin(dec) - + a[2] * np.cos(dec) - + a[3] * np.sin(ha) * np.sin(dec) - + a[4] * np.cos(ha) * np.sin(dec) - + a[5] * np.sin(ha) * np.cos(dec) - + a[6] * np.cos(ha) * np.cos(dec) - ) - - return Angle(degrees=(delta_ha_cos_dec / np.cos(dec)) / 60.0) - - -def galt_pointing_model_dec( - ha_in, dec_in, b=[1.081, 0.707, -0.076, 0.0, 0.0, 0.0, 0.0] -): - """Calculate pointing correction in declination for the Galt Telescope - See description of the pointing model by Lewis Knee CHIME document library - 754 https://bao.chimenet.ca/doc/documents/754 - - Parameters - ---------- - ha, dec : Skyfield Angle objects - Target hour angle and declination - - b : list of floats - List of coefficients (in arcmin) for the pointing model - (NOTE: it is very unlikely that a user will want to change these - from the defaults, which are taken from the pointing model as of - 2019-2-15) - - Returns - ------- - Skyfield Angle object - Angular offset in hour angle - """ +from .hfbcat import get_doppler_shifted_freq - from skyfield.positionlib import Angle +chime = ch_ephem.observers.get("chime") +CHIMELATITUDE = chime.latitude +CHIMELONGITUDE = chime.longitude +CHIMEALTITUDE = chime.altitude - ha = ha_in.radians - dec = dec_in.radians +tone = ch_ephem.observers.get("tone") +TONELATITUDE = tone.latitude +TONELONGITUDE = tone.longitude +TONEALTITUDE = tone.altitude - # declination pointing correction in arcmin - delta_dec = ( - b[0] - + b[1] * np.sin(ha) - + b[2] * np.cos(ha) - + b[3] * np.sin(dec) - + b[4] * np.cos(dec) - + b[5] * np.sin(dec) * np.cos(ha) - + b[6] * np.sin(dec) * np.sin(ha) - ) +kko = ch_ephem.observers.get("kko") +KKOLATITUDE = kko.latitude +KKOLONGITUDE = kko.longitude +KKOALTITUDE = kko.altitude - return Angle(degrees=delta_dec / 60.0) - - -def parse_date(datestring): - """Convert date string to a datetime object. - - Parameters - ---------- - datestring : string - Date as YYYYMMDD-AAA, where AAA is one of [UTC, PST, PDT] - - Returns - ------- - date : datetime - A python datetime object in UTC. - """ - from datetime import datetime, timedelta - import re - - rm = re.match("([0-9]{8})-([A-Z]{3})", datestring) - if rm is None: - msg = ( - "Wrong format for datestring: {0}.".format(datestring) - + "\nShould be YYYYMMDD-AAA, " - + "where AAA is one of [UTC,PST,PDT]" - ) - raise ValueError(msg) - - datestring = rm.group(1) - tzoffset = 0.0 - tz = rm.group(2) - - tzs = {"PDT": -7.0, "PST": -8.0, "EDT": -4.0, "EST": -5.0, "UTC": 0.0} - - if tz is not None: - try: - tzoffset = tzs[tz.upper()] - except KeyError: - print("Time zone {} not known. Known time zones:".format(tz)) - for key, value in tzs.items(): - print(key, value) - print("Using UTC{:+.1f}.".format(tzoffset)) - - return datetime.strptime(datestring, "%Y%m%d") - timedelta(hours=tzoffset) - - -def utc_lst_to_mjd(datestring, lst, obs=chime): - """Convert datetime string and LST to corresponding modified Julian Day - - Parameters - ---------- - datestring : string - Date as YYYYMMDD-AAA, where AAA is one of [UTC, PST, PDT] - lst : float - Local sidereal time at DRAO (CHIME) in decimal hours - obs : caput.Observer object - - Returns - ------- - mjd : float - Modified Julian Date corresponding to the given time. - """ - return ( - unix_to_skyfield_time( - obs.lsa_to_unix(lst * 360 / 24, datetime_to_unix(parse_date(datestring))) - ).tt - - 2400000.5 - ) - - -def solar_transit(start_time, end_time=None, obs=chime): - """Find the Solar transits between two times for CHIME. - - Parameters - ---------- - start_time : float (UNIX time) or datetime - Start time to find transits. - end_time : float (UNIX time) or datetime, optional - End time for finding transits. If `None` default, search for 24 hours - after start time. - - Returns - ------- - transit_times : array_like - Array of transit times (in UNIX time). - - """ - - planets = skyfield_wrapper.ephemeris - sun = planets["sun"] - return obs.transit_times(sun, start_time, end_time) - - -def lunar_transit(start_time, end_time=None, obs=chime): - """Find the Lunar transits between two times for CHIME. - - Parameters - ---------- - start_time : float (UNIX time) or datetime - Start time to find transits. - end_time : float (UNIX time) or datetime, optional - End time for finding transits. If `None` default, search for 24 hours - after start time. - - Returns - ------- - transit_times : array_like - Array of transit times (in UNIX time). +PCOLATITUDE = KKOLATITUDE +PCOLONGITUDE = KKOLONGITUDE +PCOALTITUDE = KKOALTITUDE - """ +gbo = ch_ephem.observers.get("gbo") +GBOLATITUDE = gbo.latitude +GBOLONGITUDE = gbo.longitude +GBOALTITUDE = gbo.altitude - planets = skyfield_wrapper.ephemeris - moon = planets["moon"] - return obs.transit_times(moon, start_time, end_time) +hco = ch_ephem.observers.get("hco") +HCOLATITUDE = hco.latitude +HCOLONGITUDE = hco.longitude +HCOALTITUDE = hco.altitude -# Create CHIME specific versions of various calls. lsa_to_unix = chime.lsa_to_unix unix_to_lsa = chime.unix_to_lsa unix_to_csd = chime.unix_to_lsd @@ -414,552 +85,26 @@ def lunar_transit(start_time, end_time=None, obs=chime): CSD_ZERO = chime.lsd_start_day -def transit_RA(time): - """No longer supported. Use `lsa` instead.""" - raise NotImplementedError( - "No longer supported. Use the better defined `lsa` instead." - ) - - -def chime_local_datetime(*args): - """Create a :class:`datetime.datetime` object in Canada/Pacific timezone. - - Parameters - ---------- - *args - Any valid arguments to the constructor of :class:`datetime.datetime` - except *tzinfo*. Local date and time at CHIME. - - Returns - ------- - dt : :class:`datetime.datetime` - Timezone naive date and time but converted to UTC. - - """ - - from pytz import timezone - - tz = timezone("Canada/Pacific") - dt_naive = datetime(*args) - if dt_naive.tzinfo: - msg = "Time zone should not be supplied." - raise ValueError(msg) - dt_aware = tz.localize(dt_naive) - return dt_aware.replace(tzinfo=None) - dt_aware.utcoffset() - - +# These are now caput.time.Observer methods def solar_setting(start_time, end_time=None, obs=chime): - """Find the Solar settings between two times for CHIME. - - Parameters - ---------- - start_time : float (UNIX time) or datetime - Start time to find settings. - end_time : float (UNIX time) or datetime, optional - End time for finding settings. If `None` default, search for 24 hours - after start time. - - Returns - ------- - setting_times : array_like - Array of setting times (in UNIX time). - - """ - - planets = skyfield_wrapper.ephemeris - sun = planets["sun"] - # Use 0.6 degrees for the angular diameter of the Sun to be conservative: - return obs.set_times(sun, start_time, end_time, diameter=0.6) + return obs.solar_setting(start_time, end_time) def lunar_setting(start_time, end_time=None, obs=chime): - """Find the Lunar settings between two times for CHIME. - - Parameters - ---------- - start_time : float (UNIX time) or datetime - Start time to find settings. - end_time : float (UNIX time) or datetime, optional - End time for finding settings. If `None` default, search for 24 hours - after start time. - - Returns - ------- - setting_times : array_like - Array of setting times (in UNIX time). - - """ - - planets = skyfield_wrapper.ephemeris - moon = planets["moon"] - # Use 0.6 degrees for the angular diameter of the Moon to be conservative: - return obs.set_times(moon, start_time, end_time, diameter=0.6) + return obs.lunar_setting(start_time, end_time) def solar_rising(start_time, end_time=None, obs=chime): - """Find the Solar risings between two times for CHIME. - - Parameters - ---------- - start_time : float (UNIX time) or datetime - Start time to find risings. - end_time : float (UNIX time) or datetime, optional - End time for finding risings. If `None` default, search for 24 hours - after start time. - - Returns - ------- - rising_times : array_like - Array of rising times (in UNIX time). - - """ - - planets = skyfield_wrapper.ephemeris - sun = planets["sun"] - # Use 0.6 degrees for the angular diameter of the Sun to be conservative: - return obs.rise_times(sun, start_time, end_time, diameter=0.6) + return obs.solar_rising(start_time, end_time) def lunar_rising(start_time, end_time=None, obs=chime): - """Find the Lunar risings between two times for CHIME. - - Parameters - ---------- - start_time : float (UNIX time) or datetime - Start time to find risings. - end_time : float (UNIX time) or datetime, optional - End time for finding risings. If `None` default, search for 24 hours after - start time. + return obs.lunar_rising(start_time, end_time) - Returns - ------- - rising_times : array_like - Array of rising times (in UNIX time). - - """ - - planets = skyfield_wrapper.ephemeris - moon = planets["moon"] - # Use 0.6 degrees for the angular diameter of the Moon to be conservative: - return obs.rise_times(moon, start_time, end_time, diameter=0.6) - - -def _is_skyfield_obj(body): - return ( - isinstance(body, skyfield.starlib.Star) - or isinstance(body, skyfield.vectorlib.VectorSum) - or isinstance(body, skyfield.jpllib.ChebyshevPosition) - ) - - -def Star_cirs(ra, dec, epoch): - """Wrapper for skyfield.api.star that creates a position given CIRS - coordinates observed from CHIME - - Parameters - ---------- - ra, dec : skyfield.api.Angle - RA and dec of the source in CIRS coordinates - epoch : skyfield.api.Time - Time of the observation - - Returns - ------- - body : skyfield.api.Star - Star object in ICRS coordinates - """ - - from skyfield.api import Star - - return cirs_radec(Star(ra=ra, dec=dec, epoch=epoch)) - - -def cirs_radec(body, date=None, deg=False, obs=chime): - """Converts a Skyfield body in CIRS coordinates at a given epoch to - ICRS coordinates observed from CHIME - - Parameters - ---------- - body : skyfield.api.Star - Skyfield Star object with positions in CIRS coordinates. - - Returns - ------- - new_body : skyfield.api.Star - Skyfield Star object with positions in ICRS coordinates - """ - - from skyfield.positionlib import Angle - from skyfield.api import Star - - ts = skyfield_wrapper.timescale - - epoch = ts.tt_jd(np.median(body.epoch)) - - pos = obs.skyfield_obs().at(epoch).observe(body) - - # Matrix CT transforms from CIRS to ICRF (https://rhodesmill.org/skyfield/time.html) - r_au, dec, ra = skyfield.functions.to_polar( - np.einsum("ij...,j...->i...", epoch.CT, pos.position.au) - ) - - return Star( - ra=Angle(radians=ra, preference="hours"), dec=Angle(radians=dec), epoch=epoch - ) - - -def object_coords(body, date=None, deg=False, obs=chime): - """Calculates the RA and DEC of the source. - - Gives the ICRS coordinates if no date is given (=J2000), or if a date is - specified gives the CIRS coordinates at that epoch. - - This also returns the *apparent* position, including abberation and - deflection by gravitational lensing. This shifts the positions by up to - 20 arcseconds. - - Parameters - ---------- - body : skyfield source - skyfield.starlib.Star or skyfield.vectorlib.VectorSum or - skyfield.jpllib.ChebyshevPosition body representing the source. - date : float - Unix time at which to determine ra of source If None, use Jan 01 - 2000. - deg : bool - Return RA ascension in degrees if True, radians if false (default). - obs : `caput.time.Observer` - An observer instance to use. If not supplied use `chime`. For many - calculations changing from this default will make little difference. - - Returns - ------- - ra, dec: float - Position of the source. - """ - - if date is None: # No date, get ICRS coords - if isinstance(body, skyfield.starlib.Star): - ra, dec = body.ra.radians, body.dec.radians - else: - raise ValueError( - "Body is not fixed, cannot calculate coordinates without a date." - ) - - else: # Calculate CIRS position with all corrections - date = unix_to_skyfield_time(date) - radec = obs.skyfield_obs().at(date).observe(body).apparent().cirs_radec(date) - - ra, dec = radec[0].radians, radec[1].radians - - # If requested, convert to degrees - if deg: - ra = np.degrees(ra) - dec = np.degrees(dec) - - # Return - return ra, dec - - -def hadec_to_bmxy(ha_cirs, dec_cirs): - """Convert CIRS hour angle and declination to CHIME/FRB beam-model XY coordinates. - - Parameters - ---------- - ha_cirs : array_like - The CIRS Hour Angle in degrees. - dec_cirs : array_like - The CIRS Declination in degrees. - - Returns - ------- - bmx, bmy : array_like - The CHIME/FRB beam model X and Y coordinates in degrees as defined in - the beam-model coordinate conventions: - https://chime-frb-open-data.github.io/beam-model/#coordinate-conventions - """ - - from caput.interferometry import rotate_ypr, sph_to_ground - - from ch_util.tools import _CHIME_ROT - - # Convert CIRS coordinates to CHIME "ground fixed" XYZ coordinates, - # which constitute a unit vector pointing towards the point of interest, - # i.e., telescope cartesian unit-sphere coordinates. - # chx: The EW coordinate (increases to the East) - # chy: The NS coordinate (increases to the North) - # chz: The vertical coordinate (increases to the sky) - chx, chy, chz = sph_to_ground( - np.deg2rad(ha_cirs), np.deg2rad(CHIMELATITUDE), np.deg2rad(dec_cirs) - ) - - # Correct for CHIME telescope rotation with respect to North - ypr = np.array([np.deg2rad(-_CHIME_ROT), 0, 0]) - chx_rot, chy_rot, chz_rot = rotate_ypr(ypr, chx, chy, chz) - - # Convert rotated CHIME "ground fixed" XYZ coordinates to spherical polar coordinates - # with the pole towards almost-North and using CHIME's meridian as the prime meridian. - # Note that the azimuthal angle theta in these spherical polar coordinates increases - # to the West (to ensure that phi and theta here have the same meaning as the variables - # with the same names in the beam_model package and DocLib #1203). - # phi (polar angle): almost-North = 0 deg; zenith = 90 deg; almost-South = 180 deg - # theta (azimuthal angle): almost-East = -90 deg; zenith = 0 deg; almost-West = +90 deg - phi = np.arccos(chy_rot) - theta = np.arctan2(-chx_rot, +chz_rot) - - # Convert polar angle and azimuth to CHIME/FRB beam model XY position - bmx = np.rad2deg(theta * np.sin(phi)) - bmy = np.rad2deg(np.pi / 2.0 - phi) - - return bmx, bmy - - -def bmxy_to_hadec(bmx, bmy): - """Convert CHIME/FRB beam-model XY coordinates to CIRS hour angle and declination. - - Parameters - ---------- - bmx, bmy : array_like - The CHIME/FRB beam model X and Y coordinates in degrees as defined in - the beam-model coordinate conventions: - https://chime-frb-open-data.github.io/beam-model/#coordinate-conventions - X is degrees west from the meridian - Y is degrees north from zenith - - Returns - ------- - ha_cirs : array_like - The CIRS Hour Angle in degrees. - dec_cirs : array_like - The CIRS Declination in degrees. - """ - import warnings - - from caput.interferometry import rotate_ypr, ground_to_sph - - from ch_util.tools import _CHIME_ROT - - # Convert CHIME/FRB beam model XY position to spherical polar coordinates - # with the pole towards almost-North and using CHIME's meridian as the prime - # meridian. Note that the CHIME/FRB beam model X coordinate increases westward - # and so does the azimuthal angle theta in these spherical polar coordinates - # (to ensure that phi and theta here have the same meaning as the variables - # with the same names in the beam_model package and DocLib #1203). - # phi (polar angle): almost-North = 0 deg; zenith = 90 deg; almost-South = 180 deg - # theta (azimuthal angle): almost-East = -90 deg; zenith = 0 deg; almost-West = +90 deg - phi = np.pi / 2.0 - np.deg2rad(bmy) - theta = np.deg2rad(bmx) / np.sin(phi) - - # Warn for input beam-model XY positions below the horizon - scalar_input = np.isscalar(theta) - theta = np.atleast_1d(theta) - if (theta < -1.0 * np.pi / 2.0).any() or (theta > np.pi / 2.0).any(): - warnings.warn("Input beam model XY coordinate(s) below horizon.") - if scalar_input: - theta = np.squeeze(theta) - - # Convert spherical polar coordinates to rotated CHIME "ground fixed" XYZ - # coordinates (i.e., cartesian unit-sphere coordinates, rotated to correct - # for the CHIME telescope's rotation with respect to North). - # chx_rot: The almost-EW coordinate (increases to the almost-East) - # chy_rot: The almost-NS coordinate (increases to the almost-North) - # chz_rot: The vertical coordinate (increases to the sky) - chx_rot = np.sin(phi) * np.sin(-theta) - chy_rot = np.cos(phi) - chz_rot = np.sin(phi) * np.cos(-theta) - - # Undo correction for CHIME telescope rotation with respect to North - ypr = np.array([np.deg2rad(_CHIME_ROT), 0, 0]) - chx, chy, chz = rotate_ypr(ypr, chx_rot, chy_rot, chz_rot) - - # Convert CHIME "ground fixed" XYZ coordinates to CIRS hour angle and declination - ha_cirs, dec_cirs = ground_to_sph(chx, chy, np.deg2rad(CHIMELATITUDE)) - - return np.rad2deg(ha_cirs), np.rad2deg(dec_cirs) - - -def peak_RA(body, date=None, deg=False): - """Calculates the RA where a source is expected to peak in the beam. - Note that this is not the same as the RA where the source is at - transit, since the pathfinder is rotated with respect to north. - - Parameters - ---------- - body : ephem.FixedBody - skyfield.starlib.Star or skyfield.vectorlib.VectorSum or - skyfield.jpllib.ChebyshevPosition or Ephemeris body - representing the source. - date : float - Unix time at which to determine ra of source - If None, use Jan 01 2000. - Ignored if body is not a skyfield object - deg : bool - Return RA ascension in degrees if True, - radians if false (default). - - Returns - ------- - peak_ra : float - RA when the transiting source peaks. - """ - - _PF_ROT = np.radians(1.986) # Pathfinder rotation from north. - _PF_LAT = np.radians(CHIMELATITUDE) # Latitude of pathfinder - - # Extract RA and dec of object - ra, dec = object_coords(body, date=date) - - # Estimate the RA at which the transiting source peaks - ra = ra + np.tan(_PF_ROT) * (dec - _PF_LAT) / np.cos(_PF_LAT) - - # If requested, convert to degrees - if deg: - ra = np.degrees(ra) - - # Return - return ra - - -# For backwards compatibility -def get_doppler_shifted_freq(*args, **kwargs): - """Deprecated. Use `ch_util.hfbcat.get_doppler_shifted_freq`.""" - from . import hfbcat - - import warnings - - warnings.warn( - "Use `ch_util.hfbcat.get_doppler_shifted_freq` instead.", DeprecationWarning - ) - - return hfbcat.get_doppler_shifted_freq(*args, **kwargs) - - -def get_range_rate( - source: skyfield.starlib.Star, - date: Union[float, list], - obs: Observer = chime, -) -> Union[float, np.array]: - """Calculate rate at which distance between observer and source changes. - - Parameters - ---------- - source - Position(s) on the sky. - date - Unix time(s) for which to calculate range rate. - obs - An Observer instance to use. If not supplied use `chime`. For many - calculations changing from this default will make little difference. - - Returns - ------- - range_rate - Rate (in m/s) at which the distance between the observer and source - changes (i.e., the velocity of observer in direction of source, but - positive for observer and source moving appart). If either `source` - or `date` contains multiple entries, `range_rate` will be an array. - Otherwise, `range_rate` will be a float. - - Notes - ----- - Only one of `source` and `date` can contain multiple entries. - - This routine uses an :class:`skyfield.positionlib.Apparent` object - (rather than an :class:`skyfield.positionlib.Astrometric` object) to find - the velocity of the observatory and the position of the source. This - accounts for the gravitational deflection and the aberration of light. - It is unclear if the latter should be taken into account for this Doppler - shift calculation, but its effects are negligible. - """ - - if hasattr(source.ra._degrees, "__iter__") and hasattr(date, "__iter__"): - raise ValueError( - "Only one of `source` and `date` can contain multiple entries." - ) - - # Convert unix times to skyfield times - date = unix_to_skyfield_time(date) - - # Create skyfield Apparent object of source position seen from observer - position = obs.skyfield_obs().at(date).observe(source).apparent() - - # Observer velocity vector in ICRS xyz coordinates in units of m/s - obs_vel_m_per_s = position.velocity.m_per_s - - # Normalized source position vector in ICRS xyz coordinates - source_pos_m = position.position.m - source_pos_norm = source_pos_m / np.linalg.norm(source_pos_m, axis=0) - - # Dot product of observer velocity and source position gives observer - # velocity in direction of source; flip sign to get range rate (positive - # for observer and source moving appart) - range_rate = -np.sum(obs_vel_m_per_s.T * source_pos_norm.T, axis=-1) - - return range_rate - - -def get_source_dictionary(*args): - """Returns a dictionary containing :class:`skyfield.starlib.Star` - objects for common radio point sources. This is useful for - obtaining the skyfield representation of a source from a string - containing its name. - - Parameters - ---------- - catalog_name : str - Name of the catalog. This must be the basename of the json file - in the `ch_util/catalogs` directory. Can take multiple catalogs, - with the first catalog favoured for any overlapping sources. - - Returns - ------- - src_dict : dictionary - Format is {'SOURCE_NAME': :class:`skyfield.starlib.Star`, ...} - - """ - - import os - import json - - src_dict = {} - for catalog_name in reversed(args): - path_to_catalog = os.path.join( - os.path.dirname(__file__), - "catalogs", - os.path.splitext(catalog_name)[0] + ".json", - ) - - with open(path_to_catalog, "r") as handler: - catalog = json.load(handler) - - for name, info in catalog.items(): - src_dict[name] = skyfield_star_from_ra_dec(info["ra"], info["dec"], name) - - return src_dict - - -# Common radio point sources -source_dictionary = get_source_dictionary( - "primary_calibrators_perley2016", - "specfind_v2_5Jy_vollmer2009", - "atnf_psrcat", - "hfb_target_list", -) - -#: :class:`skyfield.starlib.Star` representing Cassiopeia A. -CasA = source_dictionary["CAS_A"] - -#: :class:`skyfield.starlib.Star` representing Cygnus A. -CygA = source_dictionary["CYG_A"] - -#: :class:`skyfield.starlib.Star` representing Taurus A. -TauA = source_dictionary["TAU_A"] - -#: :class:`skyfield.starlib.Star` representing Virgo A. -VirA = source_dictionary["VIR_A"] +def solar_transit(start_time, end_time=None, obs=chime): + return obs.solar_transit(start_time, end_time) -if __name__ == "__main__": - import doctest - doctest.testmod() +def lunar_transit(start_time, end_time=None, obs=chime): + return obs.lunar_transit(start_time, end_time) diff --git a/ch_util/finder.py b/ch_util/finder.py index 6c90316a..3aca06be 100644 --- a/ch_util/finder.py +++ b/ch_util/finder.py @@ -48,9 +48,11 @@ import caput.time as ctime +from ch_ephem.observers import chime + import chimedb.core as db import chimedb.data_index as di -from . import layout, ephemeris +from . import layout from chimedb.dataflag import DataFlagType, DataFlag @@ -162,8 +164,8 @@ class Finder(object): Search for transits of a given source. - >>> from ch_util import ephemeris - >>> f.include_transits(ephemeris.CasA, time_delta=3600) + >>> import ch_ephem.sources + >>> f.include_transits(ch_ephem.sources.CasA, time_delta=3600) >>> f.print_results_summary() interval | acquisition | offset from start (s) | length (s) | N files 1 | 20140219T145849Z_abbot_corr | 452087.2 | 3600.0 | 2 @@ -279,7 +281,7 @@ def __init__(self, acqs=(), node_spoof=None): for i in self._acq_info: acqs.join(i) self._acqs = list(acqs) - self._time_range = (ephemeris.CSD_ZERO, time.time()) + self._time_range = (chime.lsd_start_day, time.time()) self._time_intervals = None self._time_exclusions = [] self._atmel_restrict = None @@ -959,11 +961,12 @@ def include_transits(self, body, time_delta=None): Examples -------- - >>> from ch_util import (finder, ephemeris) + >>> from ch_util import finder + >>> import ch_ephem.sources >>> from datetime import datetime >>> f = finder.Finder() >>> f.set_time_range(datetime(2014,02,20), datetime(2014,02,22)) - >>> f.include_transits(ephemeris.CasA, time_delta=3600) + >>> f.include_transits(ch_ephem.sources.CasA, time_delta=3600) >>> f.print_results_summary() interval | acquisition | offset from start (s) | length (s) | N files 1 | 20140219T145849Z_abbot_corr | 107430.9 | 3600.0 | 2 @@ -976,7 +979,7 @@ def include_transits(self, body, time_delta=None): if not time_delta: time_delta = self.min_interval * 2 - ttimes = ephemeris.transit_times(body, *self.time_range) + ttimes = chime.transit_times(body, *self.time_range) for ttime in ttimes: self.include_time_interval( ttime - time_delta / 2.0, ttime + time_delta / 2.0 @@ -1080,7 +1083,7 @@ def exclude_transits(self, body, time_delta): if not time_delta: time_delta = self.min_interval * 2 - ttimes = ephemeris.transit_times(body, *self.time_range) + ttimes = chime.transit_times(body, *self.time_range) for ttime in ttimes: self.exclude_time_interval( ttime - time_delta / 2.0, ttime + time_delta / 2.0 @@ -1089,23 +1092,23 @@ def exclude_transits(self, body, time_delta): def exclude_daytime(self): """Add time intervals to exclude all day time data.""" - rise_times = ephemeris.solar_rising( + rise_times = chime.solar_rising( self.time_range[0] - 24 * 3600.0, self.time_range[1] ) for rise_time in rise_times: - set_time = ephemeris.solar_setting(rise_time) + set_time = chime.solar_setting(rise_time) self.exclude_time_interval(rise_time, set_time) def exclude_nighttime(self): """Add time intervals to exclude all night time data.""" - set_times = ephemeris.solar_setting( + set_times = chime.solar_setting( self.time_range[0] - 24 * 3600.0, self.time_range[1] ) for set_time in set_times: - rise_time = ephemeris.solar_rising(set_time) + rise_time = chime.solar_rising(set_time) self.exclude_time_interval(set_time, rise_time) def exclude_sun(self, time_delta=4000.0, time_delta_rise_set=4000.0): @@ -1122,21 +1125,21 @@ def exclude_sun(self, time_delta=4000.0, time_delta_rise_set=4000.0): """ # Sunrise - rise_times = ephemeris.solar_rising( + rise_times = chime.solar_rising( self.time_range[0] - time_delta_rise_set, self.time_range[1] ) for rise_time in rise_times: self.exclude_time_interval(rise_time, rise_time + time_delta_rise_set) # Sunset - set_times = ephemeris.solar_setting( + set_times = chime.solar_setting( self.time_range[0], self.time_range[1] + time_delta_rise_set ) for set_time in set_times: self.exclude_time_interval(set_time - time_delta_rise_set, set_time) # Sun transit - transit_times = ephemeris.solar_transit( + transit_times = chime.solar_transit( self.time_range[0] - time_delta / 2.0, self.time_range[1] + time_delta / 2.0 ) for transit_time in transit_times: diff --git a/ch_util/fluxcat.py b/ch_util/fluxcat.py index b70e8651..6387b93b 100644 --- a/ch_util/fluxcat.py +++ b/ch_util/fluxcat.py @@ -24,7 +24,8 @@ from caput import misc import caput.time as ctime -from . import ephemeris +import ch_ephem.catalogs + from .tools import ensure_list # Define nominal frequency. Sources in catalog are ordered according to @@ -33,10 +34,10 @@ FREQ_NOMINAL = 600.0 # Define the source collections that should be loaded when this module is imported. -DIR_COLLECTIONS = os.path.join(os.path.dirname(__file__), "catalogs") +# These catalogs are provided by ch_ephem. DEFAULT_COLLECTIONS = [ - os.path.join(DIR_COLLECTIONS, "primary_calibrators_perley2016.json"), - os.path.join(DIR_COLLECTIONS, "specfind_v2_5Jy_vollmer2009.json"), + "primary_calibrators_perley2016", + "specfind_v2_5Jy_vollmer2009", ] @@ -1284,6 +1285,41 @@ def load(cls, filename, overwrite=0, set_globals=False, verbose=False): elif ext == ".pickle": collection_dict = pickle.load(fp) + return cls.load_dict( + collection_dict, collection_name, overwrite, set_globals, verbose + ) + + @classmethod + def load_dict( + cls, + collection_dict, + collection_name, + overwrite=0, + set_globals=False, + verbose=False, + ): + """ + Load the contents of a dict into the catalog. + + Parameters + ---------- + collection_dict : dict + keys are source names, values are the sources + collection_name : str + Name of the collection + overwrite : int between 0 and 2 + Action to take in the event that this source is already in the catalog: + - 0 - Return the existing entry. + - 1 - Add any measurements to the existing entry. + - 2 - Overwrite the existing entry. + Default is 0. + set_globals : bool + If True, this creates a variable in the global space + for each source in the file. Default is False. + verbose : bool + If True, print some basic info about the contents of + the file as it is loaded. Default is False. + """ # Add this to the list of files cls._collections[collection_name] = list(collection_dict.keys()) @@ -1470,4 +1506,4 @@ def _print_collection_summary(collection_name, source_names, verbose=True): # Load the default collections for col in DEFAULT_COLLECTIONS: - FluxCatalog.load(col) + FluxCatalog.load_dict(ch_ephem.catalogs.load(col), col) diff --git a/ch_util/hfbcat.py b/ch_util/hfbcat.py index 49e8ecc2..64855acc 100644 --- a/ch_util/hfbcat.py +++ b/ch_util/hfbcat.py @@ -5,19 +5,20 @@ from __future__ import annotations import os import numpy as np -from typing import TYPE_CHECKING, Union +from typing import TYPE_CHECKING, Optional, Union + +import ch_ephem.catalogs -from . import ephemeris from .fluxcat import FluxCatalog from .tools import ensure_list if TYPE_CHECKING: import skyfield.starlib.Star + import caput.time.Observer # Define the source collection that should be loaded when this module is imported. -HFB_COLLECTION = os.path.join( - os.path.dirname(__file__), "catalogs", "hfb_target_list.json" -) +# This is a catalog provided by ch_ephem. +HFB_COLLECTION = "hfb_target_list" class HFBCatalog(FluxCatalog): @@ -91,7 +92,7 @@ def get_doppler_shifted_freq( source: Union[skyfield.starlib.Star, str], date: Union[float, list], freq_rest: Union[float, list] = None, - obs: ephemeris.Observer = ephemeris.chime, + obs: Optional[caput.time.Observer] = None, ) -> np.array: """Calculate Doppler shifted frequency of spectral feature with rest frequency `freq_rest`, seen towards source `source` at time `date`, due to @@ -136,6 +137,10 @@ def get_doppler_shifted_freq( """ from scipy.constants import c as speed_of_light + from ch_ephem.coord import get_range_rate + + if obs is None: + from ch_ephem.observers import chime as obs # For source string inputs, get skyfield Star object from HFB catalog if isinstance(source, str): @@ -160,7 +165,7 @@ def get_doppler_shifted_freq( # Get rate at which the distance between the observer and source changes # (positive for observer and source moving appart) - range_rate = ephemeris.get_range_rate(source, date, obs) + range_rate = get_range_rate(source, date, obs) # Compute observed frequencies from rest frequencies # using relativistic Doppler effect @@ -171,4 +176,4 @@ def get_doppler_shifted_freq( # Load the HFB target list -HFBCatalog.load(HFB_COLLECTION) +HFBCatalog.load_dict(ch_ephem.catalogs.load(HFB_COLLECTION), HFB_COLLECTION) diff --git a/ch_util/holography.py b/ch_util/holography.py index 16ea84a8..fa6e3bb4 100644 --- a/ch_util/holography.py +++ b/ch_util/holography.py @@ -21,9 +21,11 @@ import peewee as pw import caput.time as ctime -from chimedb.core.orm import base_model -from ch_util import ephemeris +import ch_ephem +from ch_ephem.observers import chime + +from chimedb.core.orm import base_model # Global variables and constants. # ================================ @@ -109,9 +111,9 @@ def from_lst( Any notes on this observation. """ - start_time = ephemeris.lsa_to_unix( + start_time = chime.lsa_to_unix( start_lst * 360 / 24, - ctime.datetime_to_unix(ephemeris.parse_date(start_day)), + ctime.datetime_to_unix(ch_ephem.time.parse_date(start_day)), ) duration_unix = duration_lst * (3600.0) * ctime.SIDEREAL_S @@ -466,7 +468,7 @@ def check_for_duplicates(t, src, start_tol, ignore_src_mismatch=False): return None # DRAO longitude in hours - DRAO_lon = ephemeris.chime.longitude * 24.0 / 360.0 + DRAO_lon = chime.longitude * 24.0 / 360.0 if verbose: print(" ") @@ -563,7 +565,7 @@ def parse_ant_logs(cls, logs, return_post_report_params=False): from skyfield.positionlib import Angle - DRAO_lon = ephemeris.CHIMELONGITUDE * 24.0 / 360.0 + DRAO_lon = chime.longitude * 24.0 / 360.0 def sidlst_to_csd(sid, lst, sid_ref, t_ref): """ @@ -586,7 +588,9 @@ def sidlst_to_csd(sid, lst, sid_ref, t_ref): output : float CHIME sidereal day """ - csd_ref = int(ephemeris.csd(ctime.datetime_to_unix(t_ref.utc_datetime()))) + csd_ref = int( + chime.lsd_to_unix(ctime.datetime_to_unix(t_ref.utc_datetime())) + ) csd = sid - sid_ref + csd_ref return csd + lst / ctime.SIDEREAL_S / 24.0 @@ -684,13 +688,15 @@ def sidlst_to_csd(sid, lst, sid_ref, t_ref): ant_data["ha"] = Angle( radians=ha.radians - - ephemeris.galt_pointing_model_ha(ha, dec).radians, + - ch_ephem.pointing.galt_pointing_model_ha(ha, dec).radians, preference="hours", ) ant_data["dec_cirs"] = Angle( radians=dec.radians - - ephemeris.galt_pointing_model_dec(ha, dec).radians, + - ch_ephem.pointing.galt_pointing_model_dec( + ha, dec + ).radians, preference="degrees", ) @@ -702,7 +708,7 @@ def sidlst_to_csd(sid, lst, sid_ref, t_ref): ) ant_data["t"] = ctime.unix_to_skyfield_time( - ephemeris.csd_to_unix(ant_data["csd"]) + chime.lsd_to_unix(ant_data["csd"]) ) # Correct RA from equinox to CIRS coords (both in radians) @@ -718,7 +724,7 @@ def sidlst_to_csd(sid, lst, sid_ref, t_ref): preference="hours", ) - obs = ephemeris.Star_cirs( + obs = ch_ephem.coord.star_cirs( ra=ant_data["ra_cirs"], dec=ant_data["dec_cirs"], epoch=ant_data["t"], diff --git a/ch_util/plot.py b/ch_util/plot.py index b16d4a4c..2b9ee4f4 100644 --- a/ch_util/plot.py +++ b/ch_util/plot.py @@ -8,9 +8,9 @@ import scipy.signal as sig import caput.time as ctime +from ch_ephem.observers import chime from . import andata -from . import ephemeris def waterfall( @@ -435,7 +435,7 @@ def _full_day_shape(data, tmstp, date, n_bins=8640, axis="solar", ax=None): if in_range: sf_time = ctime.unix_to_skyfield_time(tmstp[ii]) sun = ctime.skyfield_wrapper.ephemeris["sun"] - obs = ephemeris.chime.skyfield_obs().at(sf_time) + obs = chime.skyfield_obs().at(sf_time) azim = obs.observe(sun).apparent().altaz()[1].radians in_start_range = (tmstp[ii] > start_range[0]) and ( diff --git a/ch_util/rfi.py b/ch_util/rfi.py index 4871b437..b5215c25 100644 --- a/ch_util/rfi.py +++ b/ch_util/rfi.py @@ -32,7 +32,9 @@ import numpy as np import scipy.signal as sig -from . import tools, ephemeris +from ch_ephem.observers import chime + +from . import tools # Set up logging logger = logging.getLogger(__name__) @@ -147,7 +149,7 @@ def flag_dataset( if "time" in data.index_map: timestamp = data.time[0] elif "ra" in data.index_map: - timestamp = ephemeris.csd_to_unix(data.attrs["lsd"]) + timestamp = chime.lsd_to_unix(data.attrs["lsd"]) freq_mask = frequency_mask(data.freq[:], timestamp=timestamp) auto_ii, auto_mask = np.logical_or(auto_mask, freq_mask[:, np.newaxis, np.newaxis]) @@ -245,7 +247,7 @@ def number_deviations( timestamp = data.time[0] elif "ra" in data.index_map: twidth = int(time_width * len(data.ra[:]) / 86164.0) + 1 - timestamp = ephemeris.csd_to_unix(data.attrs["lsd"]) + timestamp = chime.lsd_to_unix(data.attrs["lsd"]) else: raise TypeError( f"Expected data type with a `time` or `ra` axis. Got {type(data)}." @@ -417,7 +419,7 @@ def spectral_cut(data, fil_window=15, only_autos=False): if "time" in data.index_map: timestamp = data.time[0] elif "ra" in data.index_map: - timestamp = ephemeris.csd_to_unix(data.attrs["lsd"]) + timestamp = chime.lsd_to_unix(data.attrs["lsd"]) drawn_bool_mask = frequency_mask(data.freq[:], timestamp=timestamp) good_data = np.logical_not(drawn_bool_mask) diff --git a/ch_util/tools.py b/ch_util/tools.py index d649aaaf..3ffbc6f7 100644 --- a/ch_util/tools.py +++ b/ch_util/tools.py @@ -131,60 +131,25 @@ from caput import pfb from caput.interferometry import projected_distance, fringestop_phase -from ch_util import ephemeris - -# Currently the position between the Pathfinder and 26m have been -# calibrated with holography, but positions between CHIME and -# Pathfinder/26m have not (they were determined from high-res -# satellite images and are only approximate). We need to -# use CHIME holography data to constrain distance [x, y, z] between -# CHIME and 26m. I then recommend defining our coordinate system -# such that center of CHIME array is the origin (so leaving variable -# _CHIME_POS alone, and updating _PF_POS and _26M_POS appropriately.) - -# CHIME geometry -_CHIME_POS = [0.0, 0.0, 0.0] -# CHIME rotation from north. Anti-clockwise looking at the ground (degrees). -# See DocLib #695 for more information. -_CHIME_ROT = -0.071 - -# 26m geometry -_26M_POS = [254.162124, 21.853934, 18.93] -_26M_B = 2.14 # m +import ch_ephem.observers + +# All telescope geometry (rotation, roll, offsets) moved to ch_ephem/instruments.yaml +# +# To access them: +# +# >>> pathfinder = ch_ephem.observers.get("pathfinder") +# >>> PF_POS = pathfinder.offset +# >>> PF_ROT = pathfinder.rotation +# >>> PF_ROLL = pathfinder.roll +# +# etc. + +# Private data +# ============ -# Pathfinder geometry -_PF_POS = [373.754961, -54.649866, 0.0] -_PF_ROT = 1.986 # Pathfinder rotation from north (towards west) in degrees +_26M_B = 2.14 # m _PF_SPACE = 22.0 # Pathfinder cylinder spacing -# KKO geometry -_KKO_POS = [0.0, 0.0, 0.0] -_KKO_ROT = 0.6874 -_KKO_ROLL = 0.5888 -_PCO_POS = _KKO_POS -_PCO_ROT = _KKO_ROT # Aliases for backwards-compatibility -# KKO_ROT = rotation of cylinder axis from North. Anti-clockwise looking at the ground (degrees). -# KKO_ROLL = roll of cylinder toward east from Vertical. Anti-clockwise looking North along the focal line. -# See Doclib #1530 and #1121 for more information. - -# GBO geometry -_GBO_POS = [0.0, 0.0, 0.0] -_GBO_ROT = -27.3745 -_GBO_ROLL = -30.0871 - -# HCO geometry -_HCO_POS = [0.0, 0.0, 0.0] -_HCO_ROT = -0.8023 -_HCO_ROLL = 1.0556 - - -# Lat/Lon -_LAT_LON = { - "chime": [49.3207125, -119.623670], - "pathfinder": [49.3202245, -119.6183635], - "galt_26m": [49.320909, -119.620174], - "gbo_tone": [38.4292962636, -79.8451625395], -} # Classes # ======= @@ -442,8 +407,10 @@ class PathfinderAntenna(ArrayAntenna): Flag indicating that the antenna is powered. """ - _rotation = _PF_ROT - _offset = _PF_POS + _pathfinder = ch_ephem.observers.get("pathfinder") + + _rotation = _pathfinder.rotation + _offset = _pathfinder.offset # The delay relative to other inputs isn't really known. Set to NaN so we # don't make any mistakes @@ -455,17 +422,21 @@ class PathfinderAntenna(ArrayAntenna): class CHIMEAntenna(ArrayAntenna): """Antenna that is part of CHIME.""" - _rotation = _CHIME_ROT - _offset = _CHIME_POS + _chime = ch_ephem.observers.get("chime") + + _rotation = _chime.rotation + _offset = _chime.offset _delay = 0 # Treat CHIME antennas as defining the delay zero point class KKOAntenna(ArrayAntenna): """KKO outrigger antenna for the CHIME/FRB project.""" - _rotation = _KKO_ROT - _roll = _KKO_ROLL - _offset = _KKO_POS + _kko = ch_ephem.observers.get("kko") + + _rotation = _kko.rotation + _roll = _kko.roll + _offset = _kko.offset _delay = np.nan @@ -475,18 +446,22 @@ class KKOAntenna(ArrayAntenna): class GBOAntenna(ArrayAntenna): """GBO outrigger antenna for the CHIME/FRB project.""" - _rotation = _GBO_ROT - _roll = _GBO_ROLL - _offset = _GBO_POS + _gbo = ch_ephem.observers.get("gbo") + + _rotation = _gbo.rotation + _roll = _gbo.roll + _offset = _gbo.offset _delay = np.nan class HCOAntenna(ArrayAntenna): """HCRO outrigger antenna for the CHIME/FRB project.""" - _rotation = _HCO_ROT - _roll = _HCO_ROLL - _offset = _HCO_POS + _hco = ch_ephem.observers.get("hco") + + _rotation = _hco.rotation + _roll = _hco.roll + _offset = _hco.offset _delay = np.nan @@ -495,8 +470,10 @@ class TONEAntenna(ArrayAntenna): Let's allow for a global rotation and offset. """ - _rotation = 0.00 - _offset = [0.00, 0.00, 0.00] + _tone = ch_ephem.observers.get("tone") + + _rotation = _tone.rotation + _offset = _tone.offset _delay = np.nan @@ -871,11 +848,9 @@ def calibrate_temperature(raw): t : numpy array The temperature in degrees Kelvin. """ - import numpy - off = 150.0 r_t = 2000.0 * (8320.0 / (raw - off) - 1.0) - return 1.0 / (1.0 / 298.0 + numpy.log(r_t / 1.0e4) / 3950.0) + return 1.0 / (1.0 / 298.0 + np.log(r_t / 1.0e4) / 3950.0) def antenna_to_lna(graph, ant, pol): @@ -1559,8 +1534,8 @@ def change_chime_location(rotation=None, location=None, default=False): """ if default: - rotation = _CHIME_ROT - location = _CHIME_POS + rotation = ch_ephem.observers.chime.rotation + location = ch_ephem.observers.chime.offset if rotation is not None: CHIMEAntenna._rotation = rotation @@ -2302,7 +2277,7 @@ def fringestop_time( csd=False, inplace=False, static_delays=True, - obs=ephemeris.chime, + obs=None, ): """Fringestop timestream data to a fixed source. @@ -2337,6 +2312,9 @@ def fringestop_time( fringestopped_timestream : np.ndarray[nfreq, nprod, times] """ + if obs is None: + from ch_ephem.observers import chime as obs + # Check the shapes match nfeed = len(feeds) nprod = len(prod_map) if prod_map is not None else nfeed * (nfeed + 1) // 2 @@ -2471,7 +2449,7 @@ def delay( prod_map=None, csd=False, static_delays=True, - obs=ephemeris.chime, + obs=None, ): """Calculate the delay in a visibilities observing a given source. @@ -2504,9 +2482,13 @@ def delay( """ import scipy.constants + from ch_ephem.coord import object_coords + + if obs is None: + from ch_ephem.observers import chime as obs ra = (times % 1.0) * 360.0 if csd else obs.unix_to_lsa(times) - src_ra, src_dec = ephemeris.object_coords(src, times.mean(), obs=obs) + src_ra, src_dec = object_coords(src, times.mean(), obs=obs) ha = (np.radians(ra) - src_ra)[np.newaxis, :] latitude = np.radians(obs.latitude) # Get feed positions / c diff --git a/requirements.txt b/requirements.txt index b75f68e5..c7f45e68 100644 --- a/requirements.txt +++ b/requirements.txt @@ -2,6 +2,7 @@ chimedb @ git+https://github.com/chime-experiment/chimedb.git chimedb.data_index @ git+https://github.com/chime-experiment/chimedb_di.git chimedb.dataflag @ git+https://github.com/chime-experiment/chimedb_dataflag.git chimedb.dataset @ git+https://github.com/chime-experiment/chimedb_dataset.git +ch_ephem @ git+https://github.com/chime-experiment/ch_ephem.git matplotlib numpy >= 1.16,<2 scipy diff --git a/setup.py b/setup.py index 24ce8903..21e0a95c 100644 --- a/setup.py +++ b/setup.py @@ -2,10 +2,6 @@ import versioneer -ch_util_data = { - "ch_util": ["catalogs/*.json"], -} - # Load the PEP508 formatted requirements from the requirements.txt file. Needs # pip version > 19.0 with open("requirements.txt", "r") as fh: @@ -23,7 +19,6 @@ "chimedb.config @ git+ssh://git@github.com/chime-experiment/chimedb_config.git" ] }, - package_data=ch_util_data, # metadata for upload to PyPI author="CHIME collaboration", author_email="richard@phas.ubc.ca", diff --git a/tests/test_ephemeris.py b/tests/test_ephemeris.py deleted file mode 100644 index 3229b345..00000000 --- a/tests/test_ephemeris.py +++ /dev/null @@ -1,95 +0,0 @@ -"""Unit tests for ephemeris module.""" - -import os -from datetime import datetime - -import pytest -from pytest import approx -import numpy as np - -import caput.time as ctime -from ch_util import ephemeris - - -# Download the required Skyfield files from a mirror on a CHIME server. -# -# The upstream servers for the timescale and ephemeris data can be -# flaky. Use this to ensure a copy will be downloaded at the risk of it -# being potentially out of date. This is useful for things like CI -# servers, but otherwise letting Skyfield do it's downloading is a -# better idea. - -mirror_url = "https://bao.chimenet.ca/skyfield/" - -files = ["Leap_Second.dat", "finals2000A.all", "de421.bsp"] - -loader = ctime.skyfield_wrapper.load -for file in files: - if not os.path.exists(loader.path_to(file)): - loader.download(mirror_url + file) - - -def test_transit_delta_t(): - t_start = 21351.34 - t1 = ephemeris.transit_times(123.0, t_start)[0] - t2 = ephemeris.transit_times(125.0, t_start)[0] - delta = (t2 - t1) % 86400 - - assert delta == approx(8.0 * 60.0 * ephemeris.STELLAR_S, abs=0.1) - - -def test_transit_sources(): - # Check at an early time (this is close to the UNIX epoch) - t_start = 12315.123 - t1 = ephemeris.transit_times(350.8664, t_start)[0] # This is CasA's RA - t2 = ephemeris.transit_times(ephemeris.CasA, t_start)[0] - # Due to precession of the polar axis this only matches within ~30s - assert t1 == approx(t2, abs=30) - - # Check at an early time (this is close to the UNIX epoch) - t_start = datetime(2001, 1, 1) - t1 = ephemeris.transit_times(350.8664, t_start)[0] # This is CasA's RA - t2 = ephemeris.transit_times(ephemeris.CasA, t_start)[0] - # This is the J2000 epoch and so the precession should be ~0. - assert t1 == approx(t2, abs=0.1) - - -def test_transit_against_transit_ra(): - t_start = 65422.2 - ra = 234.54234 - t = ephemeris.transit_times(ra, t_start)[0] - ra_back_calculated = ephemeris.lsa(t) - - assert ra == approx(ra_back_calculated, abs=1e-2) - - -def test_csd(): - """Test CHIME sidereal day definition.""" - # csd_zero = 1384489290.908534 - # csd_zero = 1384489290.224582 - csd_zero = 1384489291.0995445 - et1 = ephemeris.datetime_to_unix(datetime(2013, 11, 14)) - - # Check the zero of CSD (1e-7 accuracy ~ 10 milliarcsec) - assert ephemeris.csd(csd_zero) == approx(0.0, abs=1e-6) - - # Check that the fractional part is equal to the transit RA - assert (360.0 * (ephemeris.csd(et1) % 1.0)) == approx( - ephemeris.chime.unix_to_lsa(et1), abs=1e-7 - ) - - # Check a specific precalculated CSD - csd1 = -1.1848449724498247 - - assert ephemeris.csd(et1) == approx(csd1, abs=1e-7) - - # Check vectorization - test_args = np.array([csd_zero, et1]) - test_ans = np.array([0.0, csd1]) - assert ephemeris.csd(test_args) == approx(test_ans, abs=1e-7) - - -def test_transit_RA(): - # transit RA is deprecated and should just throw an exception - with pytest.raises(NotImplementedError): - ephemeris.transit_RA(0.0)