Time and Dates (astropy.time
)¶
Introduction¶
The astropy.time
package provides functionality for manipulating times and
dates. Specific emphasis is placed on supporting time scales (e.g., UTC, TAI,
UT1, TDB) and time representations (e.g., JD, MJD, ISO 8601) that are used in
astronomy and required to calculate, for example, sidereal times and barycentric
corrections. The astropy.time
package is based on fast and memory efficient
PyERFA wrappers around the ERFA time and calendar routines.
All time manipulations and arithmetic operations are done internally using two
64-bit floats to represent time. Floating point algorithms from [1] are used so
that the Time
object maintains sub-nanosecond precision over times spanning
the age of the universe.
Getting Started¶
The usual way to use astropy.time
is to create a Time
object by
supplying one or more input time values as well as the time format and time
scale of those values. The input time(s) can either be a single scalar like
"2010-01-01 00:00:00"
or a list or a numpy
array of values as shown
below. In general, any output values have the same shape (scalar or array) as
the input.
Examples¶
To create a Time
object:
>>> import numpy as np
>>> from astropy.time import Time
>>> times = ['1999-01-01T00:00:00.123456789', '2010-01-01T00:00:00']
>>> t = Time(times, format='isot', scale='utc')
>>> t
<Time object: scale='utc' format='isot' value=['1999-01-01T00:00:00.123' '2010-01-01T00:00:00.000']>
>>> t[1]
<Time object: scale='utc' format='isot' value=2010-01-01T00:00:00.000>
The format
argument specifies how to interpret the input values (e.g., ISO,
JD, or Unix time). The scale
argument specifies the time scale for the
values (e.g., UTC, TT, or UT1). The scale
argument is optional and defaults
to UTC except for Time from Epoch Formats.
We could have written the above as:
>>> t = Time(times, format='isot')
When the format of the input can be unambiguously determined, the
format
argument is not required, so we can then simplify even further:
>>> t = Time(times)
Now we can get the representation of these times in the JD and MJD
formats by requesting the corresponding Time
attributes:
>>> t.jd
array([2451179.50000143, 2455197.5 ])
>>> t.mjd
array([51179.00000143, 55197. ])
The full power of output representation is available via the
to_value
method which also allows controlling the
subformat. For instance, using numpy.longdouble
as the output type
for higher precision:
>>> t.to_value('mjd', 'long')
array([51179.00000143, 55197. ], dtype=float128)
The default representation can be changed by setting the format
attribute:
>>> t.format = 'fits'
>>> t
<Time object: scale='utc' format='fits' value=['1999-01-01T00:00:00.123'
'2010-01-01T00:00:00.000']>
>>> t.format = 'isot'
We can also convert to a different time scale, for instance from UTC to
TT. This uses the same attribute mechanism as above but now returns a new
Time
object:
>>> t2 = t.tt
>>> t2
<Time object: scale='tt' format='isot' value=['1999-01-01T00:01:04.307' '2010-01-01T00:01:06.184']>
>>> t2.jd
array([2451179.5007443 , 2455197.50076602])
Note that both the ISO (ISOT) and JD representations of t2
are different
than for t
because they are expressed relative to the TT time scale. Of
course, from the numbers or strings you would not be able to tell this was the
case:
>>> print(t2.fits)
['1999-01-01T00:01:04.307' '2010-01-01T00:01:06.184']
You can set the time values in place using the usual numpy
array setting
item syntax:
>>> t2 = t.tt.copy() # Copy required if transformed Time will be modified
>>> t2[1] = '2014-12-25'
>>> print(t2)
['1999-01-01T00:01:04.307' '2014-12-25T00:00:00.000']
The Time
object also has support for missing values, which is particularly
useful for Table Operations such as joining and stacking:
>>> t2[0] = np.ma.masked # Declare that first time is missing or invalid
>>> print(t2)
[-- '2014-12-25T00:00:00.000']
Finally, some further examples of what is possible. For details, see the API documentation below.
>>> dt = t[1] - t[0]
>>> dt
<TimeDelta object: scale='tai' format='jd' value=4018.00002172>
Here, note the conversion of the timescale to TAI. Time differences can only have scales in which one day is always equal to 86400 seconds.
>>> import numpy as np
>>> t[0] + dt * np.linspace(0., 1., 12)
<Time object: scale='utc' format='isot' value=['1999-01-01T00:00:00.123' '2000-01-01T06:32:43.930'
'2000-12-31T13:05:27.737' '2001-12-31T19:38:11.544'
'2003-01-01T02:10:55.351' '2004-01-01T08:43:39.158'
'2004-12-31T15:16:22.965' '2005-12-31T21:49:06.772'
'2007-01-01T04:21:49.579' '2008-01-01T10:54:33.386'
'2008-12-31T17:27:17.193' '2010-01-01T00:00:00.000']>
>>> t.sidereal_time('apparent', 'greenwich')
<Longitude [6.68050179, 6.70281947] hourangle>
You can also use time-based Quantity
for time arithmetic:
>>> import astropy.units as u
>>> Time("2020-01-01") + 5 * u.day
<Time object: scale='utc' format='iso' value=2020-01-06 00:00:00.000>
As of v5.1, Time
objects can also be passed directly to
numpy.linspace
to create even-sampled time arrays, including support for
non-scalar start
and/or stop
points - given compatible shapes.
>>> stop = ['1999-01-05T00:00:00.123456789', '2010-05-01T00:00:00']
>>> tstp = Time(stop, format='isot', scale='utc')
>>> np.linspace(t, tstp, 4, endpoint=False)
<Time object: scale='utc' format='isot' value=[['1999-01-01T00:00:00.123' '2010-01-01T00:00:00.000']
['1999-01-02T00:00:00.123' '2010-01-31T00:00:00.000']
['1999-01-03T00:00:00.123' '2010-03-02T00:00:00.000']
['1999-01-04T00:00:00.123' '2010-04-01T00:00:00.000']]>
Using astropy.time
¶
Time Object Basics¶
In astropy.time
a “time” is a single instant of time which is
independent of the way the time is represented (the “format”) and the time
“scale” which specifies the offset and scaling relation of the unit of time.
There is no distinction made between a “date” and a “time” since both concepts
(as loosely defined in common usage) are just different representations of a
moment in time.
Time Format¶
The time format specifies how an instant of time is represented. The currently
available formats are can be found in the Time.FORMATS
dict and are listed
in the table below. Each of these formats is implemented as a class that derives
from the base TimeFormat
class. This class structure can
be adapted and extended by users for specialized time formats not supplied in
astropy.time
.
Format |
Class |
Example Argument |
---|---|---|
byear |
1950.0 |
|
byear_str |
‘B1950.0’ |
|
cxcsec |
63072064.184 |
|
datetime |
datetime(2000, 1, 2, 12, 0, 0) |
|
decimalyear |
2000.45 |
|
fits |
‘2000-01-01T00:00:00.000’ |
|
gps |
630720013.0 |
|
iso |
‘2000-01-01 00:00:00.000’ |
|
isot |
‘2000-01-01T00:00:00.000’ |
|
jd |
2451544.5 |
|
jyear |
2000.0 |
|
jyear_str |
‘J2000.0’ |
|
mjd |
51544.0 |
|
plot_date |
730120.0003703703 |
|
unix |
946684800.0 |
|
unix_tai |
946684800.0 |
|
yday |
2000:001:00:00:00.000 |
|
ymdhms |
{‘year’: 2010, ‘month’: 3, ‘day’: 1} |
|
datetime64 |
np.datetime64(‘2000-01-01T01:01:01’) |
Note
The TimeFITS
format implements most
of the FITS standard [2], including support for the LOCAL
timescale.
Note, though, that FITS supports some deprecated names for timescales;
these are translated to the formal names upon initialization. Furthermore,
any specific realization information, such as UT(NIST)
is stored only as
long as the time scale is not changed.
Changing Format¶
The default representation can be changed by setting the format
attribute:
>>> t = Time('2000-01-02')
>>> t.format = 'jd'
>>> t
<Time object: scale='utc' format='jd' value=2451545.5>
Be aware that when changing format, the current output subformat (see section below) may not exist in the new format. In this case, the subformat will not be preserved:
>>> t = Time('2000-01-02', format='fits', out_subfmt='longdate')
>>> t.value
'+02000-01-02'
>>> t.format = 'iso'
>>> t.out_subfmt
u'*'
>>> t.format = 'fits'
>>> t.value
'2000-01-02T00:00:00.000'
Subformat¶
Many of the available time format classes support the concept of a subformat. This allows for variations on the basic theme of a format in both the input parsing/validation and the output.
- The table below illustrates available subformats for the string formats
iso
,fits
, andyday
formats:
Format |
Subformat |
Input / Output |
---|---|---|
|
date_hms |
2001-01-02 03:04:05.678 |
|
date_hm |
2001-01-02 03:04 |
|
date |
2001-01-02 |
|
date_hms |
2001-01-02T03:04:05.678 |
|
longdate_hms |
+02001-01-02T03:04:05.678 |
|
longdate |
+02001-01-02 |
|
date_hms |
2001:032:03:04:05.678 |
|
date_hm |
2001:032:03:04 |
|
date |
2001:032 |
Numerical formats such as mjd
, jyear
, or cxcsec
all support the
subformats: 'float'
, 'long'
, 'decimal'
, 'str'
, and 'bytes'
.
Here, 'long'
uses numpy.longdouble
for somewhat enhanced precision (with
the enhancement depending on platform), and 'decimal'
instances of
decimal.Decimal
for full precision. For the 'str'
and 'bytes'
subformats, the number of digits is also chosen such that time values are
represented accurately.
When used on input, these formats allow creating a time using a single input
value that accurately captures the value to the full available precision in
Time
. Conversely, the single value on output using Time
to_value
or TimeDelta
to_value
can have higher precision than the standard 64-bit float:
>>> tm = Time('51544.000000000000001', format='mjd') # String input
>>> tm.mjd # float64 output loses last digit but Decimal gets it
51544.0
>>> tm.to_value('mjd', subfmt='decimal')
Decimal('51544.00000000000000099920072216264')
>>> tm.to_value('mjd', subfmt='str')
'51544.000000000000001'
The complete list of subformat options for the Time
formats that
have them is:
Format |
Subformats |
---|---|
|
float, long, decimal, str, bytes |
|
float, long, decimal, str, bytes |
|
date_hms, date_hm, date |
|
float, long, decimal, str, bytes |
|
date_hms, date, longdate_hms, longdate |
|
float, long, decimal, str, bytes |
|
date_hms, date_hm, date |
|
date_hms, date_hm, date |
|
float, long, decimal, str, bytes |
|
float, long, decimal, str, bytes |
|
float, long, decimal, str, bytes |
|
float, long, decimal, str, bytes |
|
float, long, decimal, str, bytes |
|
float, long, decimal, str, bytes |
|
date_hms, date_hm, date |
The complete list of subformat options for the TimeDelta
formats
that have them is:
Format |
Subformats |
---|---|
|
float, long, decimal, str, bytes |
|
float, long, decimal, str, bytes |
Time from Epoch Formats¶
The formats cxcsec
, gps
, unix
, and unix_tai
are special in that
they provide a floating point representation of the elapsed time in seconds
since a particular reference date. These formats have a intrinsic time scale
which is used to compute the elapsed seconds since the reference date.
Format |
Scale |
Reference date |
---|---|---|
|
TT |
|
|
UTC |
|
|
TAI |
|
|
TAI |
|
Unlike the other formats which default to UTC, if no scale
is provided when
initializing a Time
object then the above intrinsic scale is used.
This is done for computational efficiency.
Time Scale¶
The time scale (or time standard) is “a specification for measuring time: either the rate at which time passes; or points in time; or both” [3], [4].
>>> Time.SCALES
('tai', 'tcb', 'tcg', 'tdb', 'tt', 'ut1', 'utc', 'local')
Scale |
Description |
---|---|
tai |
International Atomic Time (TAI) |
tcb |
Barycentric Coordinate Time (TCB) |
tcg |
Geocentric Coordinate Time (TCG) |
tdb |
Barycentric Dynamical Time (TDB) |
tt |
Terrestrial Time (TT) |
ut1 |
Universal Time (UT1) |
utc |
Coordinated Universal Time (UTC) |
local |
Local Time Scale (LOCAL) |
Wikipedia time standard article
Note
The local
time scale is meant for free-running clocks or
simulation times (i.e., to represent a time without a properly defined
scale). This means it cannot be converted to any other time scale, and
arithmetic is possible only with Time
instances with scale local
and
with TimeDelta
instances with scale local
or None
.
The system of transformation between supported time scales (i.e., all but
local
) is shown in the figure below. Further details are provided in the
Convert time scale section.
Scalar or Array¶
A Time
object can hold either a single time value or an array of time values.
The distinction is made entirely by the form of the input time(s). If a Time
object holds a single value then any format outputs will be a single scalar
value, and likewise for arrays.
Example¶
Like other arrays and lists, Time
objects holding arrays are subscriptable,
returning scalar or array objects as appropriate:
>>> from astropy.time import Time
>>> t = Time(100.0, format='mjd')
>>> t.jd
2400100.5
>>> t = Time([100.0, 200.0, 300.], format='mjd')
>>> t.jd
array([2400100.5, 2400200.5, 2400300.5])
>>> t[:2]
<Time object: scale='utc' format='mjd' value=[100. 200.]>
>>> t[2]
<Time object: scale='utc' format='mjd' value=300.0>
>>> t = Time(np.arange(50000., 50003.)[:, np.newaxis],
... np.arange(0., 1., 0.5), format='mjd')
>>> t
<Time object: scale='utc' format='mjd' value=[[50000. 50000.5]
[50001. 50001.5]
[50002. 50002.5]]>
>>> t[0]
<Time object: scale='utc' format='mjd' value=[50000. 50000.5]>
NumPy Method Analogs and Applicable NumPy Functions¶
For Time
instances holding arrays, many of the same methods and attributes
that work on ndarray
instances can be used. For example, you can
reshape Time
instances and take specific parts using
reshape()
, ravel()
,
flatten()
, T
,
transpose()
, swapaxes()
,
diagonal()
, squeeze()
, or
take()
. Corresponding functions, as well as others
that affect the shape, such as atleast_1d
and rollaxis
, work
as expected. (The relevant functions have to be explicitly enabled in
astropy
source code; let us know if a numpy
function is not supported
that you think should work.)
Examples¶
To reshape Time
instances:
>>> t.reshape(2, 3)
<Time object: scale='utc' format='mjd' value=[[50000. 50000.5 50001. ]
[50001.5 50002. 50002.5]]>
>>> t.T
<Time object: scale='utc' format='mjd' value=[[50000. 50001. 50002. ]
[50000.5 50001.5 50002.5]]>
>>> np.roll(t, 1, axis=0)
<Time object: scale='utc' format='mjd' value=[[50002. 50002.5]
[50000. 50000.5]
[50001. 50001.5]]>
Note that similarly to the ndarray
methods, all but
flatten()
try to use new views of the data,
with the data copied only if that is impossible (as discussed, for example, in
the documentation for numpy
reshape()
).
Some arithmetic methods are supported as well: min()
,
max()
, ptp()
,
sort()
, argmin()
,
argmax()
, and argsort()
.
To apply arithmetic methods to Time
instances:
>> t.max()
<Time object: scale='utc' format='mjd' value=50002.5>
>> t.ptp(axis=0) # doctest: +FLOAT_CMP
<TimeDelta object: scale='tai' format='jd' value=[2. 2.]>
Inferring Input Format¶
The Time
class initializer will not accept ambiguous inputs, but it will make
automatic inferences in cases where the inputs are unambiguous. This can apply
when the times are supplied as objects, inputs for ymdhms
, or strings. In
the latter case it is not required to specify the format because the available
string formats have no overlap. However, if the format is known in advance the
string parsing will be faster if the format is provided.
Example¶
To infer input format:
>>> from datetime import datetime
>>> t = Time(datetime(2010, 1, 2, 1, 2, 3))
>>> t.format
'datetime'
>>> t = Time('2010-01-02 01:02:03')
>>> t.format
'iso'
Internal Representation¶
The Time
object maintains an internal representation of time as a pair of
double precision numbers expressing Julian days. The sum of the two numbers is
the Julian Date for that time relative to the given time scale. Users
requiring no better than microsecond precision over human time scales (~100
years) can safely ignore the internal representation details and skip this
section.
This representation is driven by the underlying ERFA C-library implementation.
The ERFA routines take care throughout to maintain overall precision of the
double pair. Users are free to choose the way in which total JD is
provided, though internally one part contains integer days and the
other the fraction of the day, as this ensures optimal accuracy for
all conversions. The internal JD pair is available via the jd1
and jd2
attributes:
>>> t = Time('2010-01-01 00:00:00', scale='utc')
>>> t.jd1, t.jd2
(2455198.0, -0.5)
>>> t2 = t.tai
>>> t2.jd1, t2.jd2
(2455198., -0.49960648148148146)
Creating a Time Object¶
The allowed Time
arguments to create a time object are listed below:
- valnumpy ndarray, list, str, or number
Data to initialize table.
- val2numpy ndarray, list, str, or number; optional
Data to initialize table.
- formatstr, optional
Format of input value(s).
- scalestr, optional
Time scale of input value(s).
- precisionint between 0 and 9 inclusive
Decimal precision when outputting seconds as floating point.
- in_subfmtstr
Unix glob to select subformats for parsing input times.
- out_subfmtstr
Unix glob to select subformat for output times.
- location
EarthLocation
or tuple, optional If a tuple, three
Quantity
items with length units for geocentric coordinates, or a longitude, latitude, and optional height for geodetic coordinates. Can be a single location, or one for each input time.
val¶
The val
argument specifies the input time or times and can be a single
string or number, or it can be a Python list or `numpy
array of strings or
numbers. To initialize a Time
object based on a specified time, it must be
present.
In most situations, you also need to specify the time scale via the
scale
argument. The Time
class will never guess the time scale,
so a concise example would be:
>>> t1 = Time(50100.0, scale='tt', format='mjd')
>>> t2 = Time('2010-01-01 00:00:00', scale='utc')
It is possible to create a new Time
object from one or more existing time
objects. In this case, the format and scale will be inferred from the
first object unless explicitly specified.
>>> Time([t1, t2])
<Time object: scale='tt' format='mjd' value=[50100. 55197.00076602]>
val2¶
The val2
argument is available for those situations where high precision is
required. Recall that the internal representation of time within astropy.time
is two double-precision numbers that when summed give the Julian date. If
provided, the val2
argument is used in combination with val
to set the
second of the internal time values. The exact interpretation of val2
is
determined by the input format class. All string-valued formats ignore val2
and all numeric inputs effectively add the two values in a way that maintains
the highest precision. For example:
>>> t = Time(100.0, 0.000001, format='mjd', scale='tt')
>>> t.jd, t.jd1, t.jd2
(2400100.500001, 2400101.0, -0.499999)
format¶
The `format
argument sets the time time format, and as mentioned it is
required unless the format can be unambiguously determined from the input times.
scale¶
The scale
argument sets the time scale and is required except for time
formats such as plot_date
(TimePlotDate
) and unix
(TimeUnix
). These formats represent the duration
in SI seconds since a fixed instant in time is independent of time scale. See
the Time from Epoch Formats for more details.
precision¶
The precision
setting affects string formats when outputting a value that
includes seconds. It must be an integer between 0 and 9. There is no effect
when inputting time values from strings. The default precision is 3. Note
that the limit of 9 digits is driven by the way that ERFA handles fractional
seconds. In practice this should should not be an issue.
>>> t = Time('B1950.0', precision=3)
>>> t.byear_str
'B1950.000'
>>> t.precision = 0
>>> t.byear_str
'B1950'
in_subfmt¶
The in_subfmt
argument provides a mechanism to select one or more
subformat values from the available subformats for input. Multiple
allowed subformats can be selected using Unix-style wildcard characters, in
particular *
and ?
, as documented in the Python fnmatch module.
The default value for in_subfmt
is *
which matches any available
subformat. This allows for convenient input of values with unknown or
heterogeneous subformat:
>>> Time(['2000:001', '2000:002:03:04', '2001:003:04:05:06.789'])
<Time object: scale='utc' format='yday'
value=['2000:001:00:00:00.000' '2000:002:03:04:00.000' '2001:003:04:05:06.789']>
You can explicitly specify in_subfmt
in order to strictly require a
certain subformat:
>>> t = Time('2000:002:03:04', in_subfmt='date_hm')
>>> t = Time('2000:002', in_subfmt='date_hm')
Traceback (most recent call last):
...
ValueError: Input values did not match any of the formats where the
format keyword is optional ['astropy_time', 'datetime',
'byear_str', 'iso', 'isot', 'jyear_str', 'yday']
out_subfmt¶
The out_subfmt
argument is similar to in_subfmt
except that it applies
to output formatting. In the case of multiple matching subformats, the first
matching subformat is used.
>>> Time('2000-01-01 02:03:04', out_subfmt='date').iso
'2000-01-01'
>>> Time('2000-01-01 02:03:04', out_subfmt='date_hms').iso
'2000-01-01 02:03:04.000'
>>> Time('2000-01-01 02:03:04', out_subfmt='date*').iso
'2000-01-01 02:03:04.000'
>>> Time('50814.123456789012345', format='mjd', out_subfmt='str').mjd
'50814.123456789012345'
See also the subformat section.
location¶
This optional parameter specifies the observer location, using an
EarthLocation
object or a tuple containing any form that can initialize one:
either a tuple with geocentric coordinates (X, Y, Z), or a tuple with geodetic
coordinates (longitude, latitude, height; with height defaulting to zero).
They are used for time scales that are sensitive to observer location
(currently, only TDB, which relies on the PyERFA routine erfa.dtdb
to
determine the time offset between TDB and TT), as well as for sidereal time if
no explicit longitude is given.
>>> t = Time('2001-03-22 00:01:44.732327132980', scale='utc',
... location=('120d', '40d'))
>>> t.sidereal_time('apparent', 'greenwich')
<Longitude 12. hourangle>
>>> t.sidereal_time('apparent')
<Longitude 20. hourangle>
Note
In future versions, we hope to add the possibility to add observatory objects and/or names.
Getting the Current Time¶
The current time can be determined as a Time
object using the
now
class method:
>>> nt = Time.now()
>>> ut = Time(datetime.utcnow(), scale='utc')
The two should be very close to each other.
Fast C-based Date String Parser¶
Time formats that are based on a date string representation of time, including
TimeISO
, TimeISOT
, and
TimeYearDayTime
, make use of a fast C-based date parser that
improves speed by a factor of 20 or more for large arrays of times.
The C parser is stricter than the Python-based parser (which relies on
strptime
). In particular fields like the month or day of year must
always have a fixed number of ASCII digits. As an example the Python parser will
accept 2000-1-2T3:04:5.23
while the C parser requires
2000-01-02T03:04:05.23
Use of the C parser is enabled by default except when the input subformat
in_subfmt
argument is different from the default value of '*'
. If the
fast C parser fails to parse the date values then the Time
initializer will
automatically fall through to the Python parser.
In rare cases where you need to explicitly control which parser gets used there
is a configuration item time.conf.use_fast_parser
that can be set. The
default is 'True'
, which means to try the fast parser and fall through to
Python parser if needed. Note that the configuration value is a string, not a
bool object.
For example to disable the C parser use:
>>> from astropy.time import conf
>>> date = '2000-1-2T3:04:5.23'
>>> t = Time(date, format='isot') # Succeeds by default
>>> with conf.set_temp('use_fast_parser', 'False'):
... t = Time(date, format='isot')
... print(t)
2000-01-02T03:04:05.230
To force the user of the C parser (for example in testing) use:
>>> with conf.set_temp('use_fast_parser', 'force'):
... try:
... t = Time(date, format='isot')
... except ValueError as err:
... print(err)
Input values did not match the format class isot:
ValueError: fast C time string parser failed: non-digit found where digit (0-9) required
Using Time Objects¶
The operations available with Time
objects include:
Get and set time value(s) for an array-valued
Time
object.Set missing (masked) values.
Get the representation of the time value(s) in a particular time format.
Get a new time object for the same time value(s) but referenced to a different time scale.
Calculate sidereal time and Earth rotation angle corresponding to the time value(s).
Do time arithmetic involving
Time
,TimeDelta
and/orQuantity
objects with units of time.
Get and Set Values¶
For an existing Time
object which is array-valued, you can use the
usual numpy
array item syntax to get either a single item or a subset
of items. The returned value is a Time
object with all the same
attributes.
Examples¶
To get an item or a subset of items:
>>> t = Time(['2001:020', '2001:040', '2001:060', '2001:080'],
... out_subfmt='date')
>>> print(t[1])
2001:040
>>> print(t[1:])
['2001:040' '2001:060' '2001:080']
>>> print(t[[2, 0]])
['2001:060' '2001:020']
You can also set values in place for an array-valued Time
object:
>>> t = Time(['2001:020', '2001:040', '2001:060', '2001:080'],
... out_subfmt='date')
>>> t[1] = '2010:001'
>>> print(t)
['2001:020' '2010:001' '2001:060' '2001:080']
>>> t[[2, 0]] = '1990:123'
>>> print(t)
['1990:123' '2010:001' '1990:123' '2001:080']
The new value (on the right hand side) when setting can be one of three possibilities:
Scalar string value or array of string values where each value is in a valid time format that can be automatically parsed and used to create a
Time
object.Value or array of values where each value has the same
format
as theTime
object being set. For instance, a float ornumpy
array of floats for an object withformat='unix'
.Time
object with identicallocation
(butscale
andformat
need not be the same). The right side value will be transformed so the timescale
matches.
Whenever any item is set, then the internal cache (see Caching) is cleared
along with the delta_tdb_tt
and/or delta_ut1_utc
transformation
offsets, if they have been set.
If it is required that the Time
object be immutable, then set the
writeable
attribute to False
. In this case, attempting to set a value will
raise a ValueError: Time object is read-only
. See the section on
Caching for an example.
Missing Values¶
The Time
and TimeDelta
objects support functionality for marking values as
missing or invalid. This is also known as masking, and is especially useful for
Table Operations such as joining and stacking.
Example¶
To set one or more items as missing, assign the special value
numpy.ma.masked
:
>>> t = Time(['2001:020', '2001:040', '2001:060', '2001:080'],
... out_subfmt='date')
>>> t[2] = np.ma.masked
>>> print(t)
['2001:020' '2001:040' -- '2001:080']
Note
The operation of setting an array element to numpy.ma.masked
(missing) overwrites the actual time data and therefore there is no way to
recover the original value. In this sense, the numpy.ma.masked
value
behaves just like any other valid Time
value when setting. This is
similar to how Pandas missing data works,
but somewhat different from NumPy masked arrays which
maintain a separate mask array and retain the underlying data. In the
Time
object the mask
attribute is read-only and cannot be directly set.
Once one or more values in the object are masked, any operations will
propagate those values as masked, and access to format attributes such
as unix
or value
will return a MaskedArray
object:
>>> t.unix
masked_array(data = [979948800.0 981676800.0 -- 985132800.0],
mask = [False False True False],
fill_value = 1e+20)
You can view the mask
, but note that it is read-only and
setting the mask is always done by setting the item to masked
.
>>> t.mask
array([False, False, True, False]...)
>>> t[:2] = np.ma.masked
Custom Format Classes and Missing Values¶
For advanced users who have written a custom time format via a
TimeFormat
subclass, it may be necessary to modify your
class if you wish to support missing values. For applications that
do not take advantage of missing values no changes are required.
Missing values in a TimeFormat
subclass object are marked by
setting the corresponding entries of the jd2
attribute to be numpy.nan
(but this is never done directly by the user). For most array operations and
numpy
functions the numpy.nan
entries are propagated as expected and
all is well. However, this is not always the case, and in particular the ERFA
routines do not generally support numpy.nan
values gracefully.
In cases where numpy.nan
is not acceptable, format class methods should use
the jd2_filled
property instead of jd2
. This replaces numpy.nan
with
0.0
. Since jd2
is always in the range -1 to +1, substituting 0.0
will allow functions to return “reasonable” values which will then be masked in
any subsequent outputs. See the value
property of the
TimeDecimalYear
format for any example.
Get Representation¶
Instants of time can be represented in different ways, for instance as an
ISO-format date string ('1999-07-23 04:31:00'
) or seconds since 1998.0
(49091460.0
) or Modified Julian Date (51382.187451574
).
The representation of a Time
object in a particular format is available
by getting the object attribute corresponding to the format name. The list of
available format names is in the time format section.
>>> t = Time('2010-01-01 00:00:00', format='iso', scale='utc')
>>> t.jd # JD representation of time in current scale (UTC)
2455197.5
>>> t.iso # ISO representation of time in current scale (UTC)
'2010-01-01 00:00:00.000'
>>> t.unix # seconds since 1970.0 (UTC)
1262304000.0
>>> t.datetime # Representation as datetime.datetime object
datetime.datetime(2010, 1, 1, 0, 0)
Example¶
To get the representation of a Time
object:
>>> import matplotlib.pyplot as plt
>>> jyear = np.linspace(2000, 2001, 20)
>>> t = Time(jyear, format='jyear')
>>> plt.plot_date(t.plot_date, jyear)
>>> plt.gcf().autofmt_xdate() # orient date labels at a slant
>>> plt.draw()
Convert Time Scale¶
A new Time
object for the same time value(s) but referenced to a new time
scale can be created getting the object attribute corresponding to the time
scale name. The list of available time scale names is in the time scale
section and in the figure below illustrating the network of time scale
transformations.
Examples¶
To create a Time
object with a new time scale:
>>> t = Time('2010-01-01 00:00:00', format='iso', scale='utc')
>>> t.tt # TT scale
<Time object: scale='tt' format='iso' value=2010-01-01 00:01:06.184>
>>> t.tai
<Time object: scale='tai' format='iso' value=2010-01-01 00:00:34.000>
In this process the format
and other object attributes like lon
,
lat
, and precision
are also propagated to the new object.
As noted in the Time Object Basics section, a Time
object can only be
changed by explicitly setting some of its elements. The process of changing the
time scale therefore begins by making a copy of the original object and then
converting the internal time values in the copy to the new time scale. The new
Time
object is returned by the attribute access.
Caching¶
The computations for transforming to different time scales or formats can be
time-consuming for large arrays. In order to avoid repeated computations, each
Time
or TimeDelta
instance caches such transformations internally:
>>> t = Time(np.arange(1e6), format='unix', scale='utc')
>>> time x = t.tt
CPU times: user 263 ms, sys: 4.02 ms, total: 267 ms
Wall time: 267 ms
>>> time x = t.tt
CPU times: user 28 µs, sys: 9 µs, total: 37 µs
Wall time: 32.9 µs
Actions such as changing the output precision or subformat will clear the cache. In order to explicitly clear the internal cache do:
>>> del t.cache
>>> time x = t.tt
CPU times: user 263 ms, sys: 4.02 ms, total: 267 ms
Wall time: 267 ms
In order to ensure consistency between the transformed (and cached) version and the original, the transformed object is set to be not writeable. For example:
>>> x = t.tt
>>> x[1] = '2000:001'
Traceback (most recent call last):
...
ValueError: Time object is read-only. Make a copy() or set "writeable" attribute to True.
If you require modifying the object then make a copy first, for example, x =
t.tt.copy()
.
Transformation Offsets¶
Time scale transformations that cross one of the orange circles in the image above require an additional offset time value that is model or observation dependent. See SOFA Time Scale and Calendar Tools for further details.
The two attributes delta_ut1_utc
and
delta_tdb_tt
provide a way to set
these offset times explicitly. These represent the time scale offsets
UT1 - UTC and TDB - TT, respectively. As an example:
>>> t = Time('2010-01-01 00:00:00', format='iso', scale='utc')
>>> t.delta_ut1_utc = 0.334 # Explicitly set one part of the transformation
>>> t.ut1.iso # ISO representation of time in UT1 scale
'2010-01-01 00:00:00.334'
For the UT1 to UTC offset, you have to interpolate the observed values provided
by the International Earth Rotation and Reference Systems (IERS) Service. astropy
will automatically download and use values
from the IERS which cover times spanning from 1973-Jan-01 through one year into
the future. In addition, the astropy
package is bundled with a data table of
values provided in Bulletin B, which cover the period from 1962 to shortly
before an astropy
release.
When the delta_ut1_utc
attribute is not set
explicitly, IERS values will be used (initiating a download of a few Mb
file the first time). For details about how IERS values are used in astropy
time and coordinates, and to understand how to control automatic downloads, see
IERS data access (astropy.utils.iers). The example below illustrates converting to the UT1
scale along with the auto-download feature:
>>> t = Time('2016:001')
>>> t.ut1
Downloading https://maia.usno.navy.mil/ser7/finals2000A.all
|==================================================================| 3.0M/3.0M (100.00%) 6s
<Time object: scale='ut1' format='yday' value=2016:001:00:00:00.082>
Note
The IERS_Auto
class contains machinery
to ensure that the IERS table is kept up to date by auto-downloading the
latest version as needed. This means that the IERS table is assured of
having the state-of-the-art definitive and predictive values for Earth
rotation. As a user it is your responsibility to understand the
accuracy of IERS predictions if your science depends on that. If you
request UT1-UTC
for times beyond the range of IERS table data then the
nearest available values will be provided.
In the case of the TDB to TT offset, most users need only provide the lon
and lat
values when creating the Time
object. If the
delta_tdb_tt
attribute is not explicitly set, then
the PyERFA routine erfa.dtdb
will be used to compute the TDB to TT
offset. Note that if lon
and lat
are not explicitly initialized,
values of 0.0 degrees for both will be used.
Example¶
The following code replicates an example in the SOFA Time Scale and Calendar Tools document. It does the transform from UTC to all supported time scales (TAI, TCB, TCG, TDB, TT, UT1, UTC). This requires an observer location (here, latitude and longitude).
>>> import astropy.units as u
>>> t = Time('2006-01-15 21:24:37.5', format='iso', scale='utc',
... location=(-155.933222*u.deg, 19.48125*u.deg))
>>> t.utc.iso
'2006-01-15 21:24:37.500'
>>> t.ut1.iso
'2006-01-15 21:24:37.834'
>>> t.tai.iso
'2006-01-15 21:25:10.500'
>>> t.tt.iso
'2006-01-15 21:25:42.684'
>>> t.tcg.iso
'2006-01-15 21:25:43.323'
>>> t.tdb.iso
'2006-01-15 21:25:42.684'
>>> t.tcb.iso
'2006-01-15 21:25:56.894'
Hashing¶
A user can generate a unique hash key for scalar (0-dimensional) Time
or
TimeDelta
objects. The key is based on a tuple of jd1
,
jd2
, scale
, and location
(if present, None
otherwise).
Note that two Time
objects with a different scale
can compare equally
but still have different hash keys. This a practical consideration driven
in by performance, but in most cases represents a desirable behavior.
Printing Time Arrays¶
If your times
array contains a lot of elements, the value
argument will
display all the elements of the Time
object t
when it is called or
printed. To control the number of elements to be displayed, set the
threshold
argument with np.printoptions
as follows:
>>> many_times = np.arange(1000)
>>> t = Time(many_times, format='cxcsec')
>>> with np.printoptions(threshold=10):
... print(repr(t))
... print(t.iso)
<Time object: scale='tt' format='cxcsec' value=[ 0. 1. 2. ... 997. 998. 999.]>
['1998-01-01 00:00:00.000' '1998-01-01 00:00:01.000'
'1998-01-01 00:00:02.000' ... '1998-01-01 00:16:37.000'
'1998-01-01 00:16:38.000' '1998-01-01 00:16:39.000']
Sidereal Time and Earth Rotation Angle¶
Apparent or mean sidereal time can be calculated using
sidereal_time()
. The method returns a Longitude
with units of hour angle, which by default is for the longitude corresponding to
the location with which the Time
object is initialized. Like the scale
transformations, ERFA C-library routines are used under the hood, which support
calculations following different IAU resolutions.
Similarly, one can calculate the Earth rotation angle with
earth_rotation_angle()
. Unlike sidereal time, which
is referred to the equinox and is a complicated function of both UT1 and
Terrestrial Time, the Earth rotation angle is referred to the Celestial
Intermediate Origin (CIO) and is a linear function of UT1 alone.
For the recent IAU precession models, as well as for the Earth rotation angle, the result includes the TIO locator (s’), which positions the Terrestrial Intermediate Origin on the equator of the Celestial Intermediate Pole (CIP) and is rigorously corrected for polar motion.
Example¶
To calculate sidereal time:
>>> t = Time('2006-01-15 21:24:37.5', scale='utc', location=('120d', '45d'))
>>> t.sidereal_time('mean')
<Longitude 13.08952187 hourangle>
>>> t.sidereal_time('apparent')
<Longitude 13.08950368 hourangle>
>>> t.earth_rotation_angle()
<Longitude 13.08436206 hourangle>
>>> t.sidereal_time('apparent', 'greenwich')
<Longitude 5.08950368 hourangle>
>>> t.sidereal_time('apparent', '-90d')
<Longitude 23.08950368 hourangle>
>>> t.sidereal_time('apparent', '-90d', 'IAU1994')
<Longitude 23.08950365 hourangle>
Time Deltas¶
Time arithmetic is supported using the TimeDelta
class. The following
operations are available:
Create a
TimeDelta
explicitly by instantiating a class object.Negate a
TimeDelta
or take its absolute value.Multiply or divide a
TimeDelta
by a constant or array.
The TimeDelta
class is derived from the Time
class and shares many of its
properties. One difference is that the time scale has to be one for which one
day is exactly 86400 seconds. Hence, the scale cannot be UTC.
Quantity
objects with time units can also be used in place of TimeDelta
.
The available time formats are:
Format |
Class |
---|---|
sec |
|
jd |
|
datetime |
Examples¶
Use of the TimeDelta
object is illustrated in the few examples below:
>>> t1 = Time('2010-01-01 00:00:00')
>>> t2 = Time('2010-02-01 00:00:00')
>>> dt = t2 - t1 # Difference between two Times
>>> dt
<TimeDelta object: scale='tai' format='jd' value=31.0>
>>> dt.sec
2678400.0
>>> from astropy.time import TimeDelta
>>> dt2 = TimeDelta(50.0, format='sec')
>>> t3 = t2 + dt2 # Add a TimeDelta to a Time
>>> t3.iso
'2010-02-01 00:00:50.000'
>>> t2 - dt2 # Subtract a TimeDelta from a Time
<Time object: scale='utc' format='iso' value=2010-01-31 23:59:10.000>
>>> dt + dt2
<TimeDelta object: scale='tai' format='jd' value=31.0005787037>
>>> import numpy as np
>>> t1 + dt * np.linspace(0, 1, 5)
<Time object: scale='utc' format='iso' value=['2010-01-01 00:00:00.000'
'2010-01-08 18:00:00.000' '2010-01-16 12:00:00.000' '2010-01-24 06:00:00.000'
'2010-02-01 00:00:00.000']>
>>> import astropy.units as u
>>> t1 + 1 * u.hour
<Time object: scale='utc' format='iso' value=2010-01-01 01:00:00.000>
# The now deprecated default assumes days for numeric inputs
>>> t1 + 5.0
<Time object: scale='utc' format='iso' value=2010-01-06 00:00:00.000>
TimeDeltaMissingUnitWarning: Numerical value without unit or explicit format passed to TimeDelta, assuming days
The TimeDelta
has a to_value
method which supports
controlling the type of the output representation by providing either a format
name and optional subformat or a valid astropy
unit:
>>> dt.to_value(u.hr)
744.0
>>> dt.to_value('jd', 'str')
'31.0'
Time Scales for Time Deltas¶
We have shown in the above that the difference between two UTC times is a
TimeDelta
with a scale of TAI. This is because a UTC time difference cannot be
uniquely defined unless the user knows the two times that were differenced
(because of leap seconds, a day does not always have 86400 seconds). For all
other time scales, the TimeDelta
inherits the scale of the first Time
object.
Examples¶
To get the time scale for a TimeDelta
object:
>>> t1 = Time('2010-01-01 00:00:00', scale='tcg')
>>> t2 = Time('2011-01-01 00:00:00', scale='tcg')
>>> dt = t2 - t1
>>> dt
<TimeDelta object: scale='tcg' format='jd' value=365.0>
When TimeDelta
objects are added or subtracted from Time
objects, scales
are converted appropriately, with the final scale being that of the Time
object:
>>> t2 + dt
<Time object: scale='tcg' format='iso' value=2012-01-01 00:00:00.000>
>>> t2.tai
<Time object: scale='tai' format='iso' value=2010-12-31 23:59:27.068>
>>> t2.tai + dt
<Time object: scale='tai' format='iso' value=2011-12-31 23:59:27.046>
TimeDelta
objects can be converted only to objects with compatible scales
(i.e., scales for which it is not necessary to know the times that were
differenced):
>>> dt.tt
<TimeDelta object: scale='tt' format='jd' value=364.999999746>
>>> dt.tdb
Traceback (most recent call last):
...
ScaleValueError: Cannot convert TimeDelta with scale 'tcg' to scale 'tdb'
TimeDelta
objects can also have an undefined scale, in which case it is
assumed that their scale matches that of the other Time
or TimeDelta
object (or is TAI in case of a UTC time):
>>> t2.tai + TimeDelta(365., format='jd', scale=None)
<Time object: scale='tai' format='iso' value=2011-12-31 23:59:27.068>
Note
Since internally Time
uses floating point numbers, round-off
errors can cause two times to be not strictly equal even if
mathematically they should be. For times in UTC in particular, this
can lead to surprising behavior, because when you add a
TimeDelta
, which cannot have a scale of UTC, the UTC time is
first converted to TAI, then the addition is done, and finally the
time is converted back to UTC. Hence, rounding errors can be
incurred, which means that even expected equalities may not hold:
>>> t = Time(2450000., 1e-6, format='jd')
>>> t + TimeDelta(0, format='jd') == t
False
Barycentric and Heliocentric Light Travel Time Corrections¶
The arrival times of photons at an observatory are not particularly useful for accurate timing work, such as eclipse/transit timing of binaries or exoplanets. This is because the changing location of the observatory causes photons to arrive early or late. The solution is to calculate the time the photon would have arrived at a standard location; either the Solar System barycenter or the heliocenter.
Example¶
Suppose you observed the dwarf nova IP Peg from Greenwich and have a list of
times in MJD form, in the UTC timescale. You then create appropriate Time
and
SkyCoord
objects and calculate light travel times to the barycenter as
follows:
>>> from astropy import time, coordinates as coord, units as u
>>> ip_peg = coord.SkyCoord("23:23:08.55", "+18:24:59.3",
... unit=(u.hourangle, u.deg), frame='icrs')
>>> greenwich = coord.EarthLocation.of_site('greenwich')
>>> times = time.Time([56325.95833333, 56325.978254], format='mjd',
... scale='utc', location=greenwich)
>>> ltt_bary = times.light_travel_time(ip_peg)
>>> ltt_bary
<TimeDelta object: scale='tdb' format='jd' value=[-0.0037715 -0.00377286]>
If you desire the light travel time to the heliocenter instead, then use:
>>> ltt_helio = times.light_travel_time(ip_peg, 'heliocentric')
>>> ltt_helio
<TimeDelta object: scale='tdb' format='jd' value=[-0.00376576 -0.00376712]>
The method returns an TimeDelta
object, which can be added to
your times to give the arrival time of the photons at the barycenter or
heliocenter. Here, you should be careful with the timescales used; for more
detailed information about timescales, see Time Scale.
The heliocenter is not a fixed point, and therefore the gravity continually changes at the heliocenter. Thus, the use of a relativistic timescale like TDB is not particularly appropriate, and, historically, times corrected to the heliocenter are given in the UTC timescale:
>>> times_heliocentre = times.utc + ltt_helio
Corrections to the barycenter are more precise than the heliocenter, because the barycenter is a fixed point where gravity is constant. For maximum accuracy you want to have your barycentric corrected times in a timescale that has always ticked at a uniform rate, and ideally one whose tick rate is related to the rate that a clock would tick at the barycenter. For this reason, barycentric corrected times normally use the TDB timescale:
>>> time_barycentre = times.tdb + ltt_bary
By default, the light travel time is calculated using the position and velocity of Earth and the Sun from ERFA routines, but you can also get more precise calculations using the JPL ephemerides (which are derived from dynamical models). An example using the JPL ephemerides is:
>>> ltt_bary_jpl = times.light_travel_time(ip_peg, ephemeris='jpl')
>>> ltt_bary_jpl
<TimeDelta object: scale='tdb' format='jd' value=[-0.0037715 -0.00377286]>
>>> (ltt_bary_jpl - ltt_bary).to(u.ms)
<Quantity [-0.00132325, -0.00132861] ms>
The difference between the built-in ephemerides and the JPL ephemerides is normally of the order of 1/100th of a millisecond, so the built-in ephemerides should be suitable for most purposes. For more details about what ephemerides are available, including the requirements for using JPL ephemerides, see Solar System Ephemerides.
Interaction with time-like Quantities¶
Where possible, Quantity
objects with units of time are treated as TimeDelta
objects with undefined scale (though necessarily with lower precision). They
can also be used as input in constructing Time
and TimeDelta
objects, and
TimeDelta
objects can be converted to Quantity
objects of arbitrary units
of time.
Examples¶
To use Quantity
objects with units of time:
>>> import astropy.units as u
>>> Time(10.*u.yr, format='gps') # time-valued quantities can be used for
... # for formats requiring a time offset
<Time object: scale='tai' format='gps' value=315576000.0>
>>> Time(10.*u.yr, 1.*u.s, format='gps')
<Time object: scale='tai' format='gps' value=315576001.0>
>>> Time(2000.*u.yr, format='jyear')
<Time object: scale='tt' format='jyear' value=2000.0>
>>> Time(2000.*u.yr, format='byear')
... # but not for Besselian year, which implies
... # a different time scale
...
Traceback (most recent call last):
...
ValueError: Input values did not match the format class byear:
ValueError: Cannot use Quantities for 'byear' format, as the interpretation would be ambiguous. Use float with Besselian year instead.
>>> TimeDelta(10.*u.yr) # With a quantity, no format is required
<TimeDelta object: scale='None' format='jd' value=3652.5>
>>> dt = TimeDelta([10., 20., 30.], format='jd')
>>> dt.to(u.hr) # can convert TimeDelta to a quantity
<Quantity [240., 480., 720.] h>
>>> dt > 400. * u.hr # and compare to quantities with units of time
array([False, True, True]...)
>>> dt + 1.*u.hr # can also add/subtract such quantities
<TimeDelta object: scale='None' format='jd' value=[10.04166667 20.04166667 30.04166667]>
>>> Time(50000., format='mjd', scale='utc') + 1.*u.hr
<Time object: scale='utc' format='mjd' value=50000.0416667>
>>> dt * 10.*u.km/u.s # for multiplication and division with a
... # Quantity, TimeDelta is converted
<Quantity [100., 200., 300.] d km / s>
>>> dt * 10.*u.Unit(1) # unless the Quantity is dimensionless
<TimeDelta object: scale='None' format='jd' value=[100. 200. 300.]>
Writing a Custom Format¶
Some applications may need a custom Time
format, and this capability is
available by making a new subclass of the TimeFormat
class.
When such a subclass is defined in your code, the format class and
corresponding name is automatically registered in the set of available time
formats.
Examples¶
The key elements of a new format class are illustrated by examining the
code for the jd
format (which is one of the most minimal):
class TimeJD(TimeFormat):
"""
Julian Date time format.
"""
name = 'jd' # Unique format name
def set_jds(self, val1, val2):
"""
Set the internal jd1 and jd2 values from the input val1, val2.
The input values are expected to conform to this format, as
validated by self._check_val_type(val1, val2) during __init__.
"""
self._check_scale(self._scale) # Validate scale.
self.jd1, self.jd2 = day_frac(val1, val2)
@property
def value(self):
"""
Return format ``value`` property from internal jd1, jd2
"""
return self.jd1 + self.jd2
As mentioned above, the _check_val_type(self, val1, val2)
method may need to be overridden to validate the inputs as conforming to the
format specification. By default this checks for valid float, float array, or
Quantity
inputs. In contrast, the iso
format class ensures the inputs
meet the ISO format specification for strings.
One special case that is relatively common and more convenient to implement is a
format that makes a small change to the date format. For instance, you could
insert T
in the yday
format with the following TimeYearDayTimeCustom
class. Notice how the subfmts
definition is modified slightly from the
standard TimeISO
class from which it inherits:
>>> from astropy.time import TimeISO
>>> class TimeYearDayTimeCustom(TimeISO):
... """
... Year, day-of-year and time as "<YYYY>-<DOY>T<HH>:<MM>:<SS.sss...>".
... The day-of-year (DOY) goes from 001 to 365 (366 in leap years).
... For example, 2000-001T00:00:00.000 is midnight on January 1, 2000.
... The allowed subformats are:
... - 'date_hms': date + hours, mins, secs (and optional fractional secs)
... - 'date_hm': date + hours, mins
... - 'date': date
... """
... name = 'yday_custom' # Unique format name
... subfmts = (('date_hms',
... '%Y-%jT%H:%M:%S',
... '{year:d}-{yday:03d}T{hour:02d}:{min:02d}:{sec:02d}'),
... ('date_hm',
... '%Y-%jT%H:%M',
... '{year:d}-{yday:03d}T{hour:02d}:{min:02d}'),
... ('date',
... '%Y-%j',
... '{year:d}-{yday:03d}'))
>>> t = Time('2000-01-01')
>>> t.yday_custom
'2000-001T00:00:00.000'
>>> t2 = Time('2016-001T00:00:00')
>>> t2.iso
'2016-01-01 00:00:00.000'
Another special case that is relatively common is a format that represents the
time since a particular epoch. The classic example is Unix time which is the
number of seconds since 1970-01-01 00:00:00 UTC, not counting leap seconds. What
if we wanted that value but do want to count leap seconds. This would be
done by using the TAI scale instead of the UTC scale. In this case we inherit
from the TimeFromEpoch
class and define a few class attributes:
>>> from astropy.time.formats import erfa, TimeFromEpoch
>>> class TimeUnixLeap(TimeFromEpoch):
... """
... Seconds from 1970-01-01 00:00:00 TAI. Similar to Unix time
... but this includes leap seconds.
... """
... name = 'unix_leap'
... unit = 1.0 / erfa.DAYSEC # in days (1 day == 86400 seconds)
... epoch_val = '1970-01-01 00:00:00'
... epoch_val2 = None
... epoch_scale = 'tai' # Scale for epoch_val class attribute
... epoch_format = 'iso' # Format for epoch_val class attribute
>>> t = Time('2000-01-01')
>>> t.unix_leap
946684832.0
>>> t.unix_leap - t.unix
32.0
Going beyond this will probably require looking at the astropy
code for more
guidance, but if you get stuck, the astropy
developers are more than happy
to help. If you write a format class that is widely useful we might want to
include it in the core!
Timezones¶
When a Time
object is constructed from a timezone-aware
datetime
, no timezone information is saved in the
Time
object. However, Time
objects can be
converted to timezone-aware datetime objects.
Example¶
To convert a Time
object to a timezone-aware datetime object:
>>> from datetime import datetime
>>> from astropy.time import Time, TimezoneInfo
>>> import astropy.units as u
>>> utc_plus_one_hour = TimezoneInfo(utc_offset=1*u.hour)
>>> dt_aware = datetime(2000, 1, 1, 0, 0, 0, tzinfo=utc_plus_one_hour)
>>> t = Time(dt_aware) # Loses timezone info, converts to UTC
>>> print(t) # will return UTC
1999-12-31 23:00:00
>>> print(t.to_datetime(timezone=utc_plus_one_hour)) # to timezone-aware datetime
2000-01-01 00:00:00+01:00
Timezone database packages, like pytz
for example, may be more convenient to use to create tzinfo
objects used to specify timezones rather than the TimezoneInfo
object.
Example¶
Using the dateutil package,
you can parse times in a wide variety of supported formats to generate a
datetime.datetime
object which can then be used to initialize a Time
object:
>>> from dateutil.parser import parse
>>> dtime = parse('2020-10-29T08:20:46.950+1100')
>>> Time(dtime)
<Time object: scale='utc' format='datetime' value=2020-10-28 21:20:46.950000>
Custom String Formats with strftime
and strptime
¶
The Time
object supports output string representation
using the format specification language defined in the Python standard library
for time.strftime
. This can be done using the strftime
method.
Examples¶
To get output string representation using the strftime
method:
>>> from astropy.time import Time
>>> t = Time('2018-01-01T10:12:58')
>>> t.strftime('%H:%M:%S %d %b %Y')
'10:12:58 01 Jan 2018'
Conversely, to create a Time
object from a custom date string
that can be parsed with Python standard library time.strptime
(using the same
format language linked above), use the strptime
class
method:
>>> from astropy.time import Time
>>> t = Time.strptime('23:59:60 30 June 2015', '%H:%M:%S %d %B %Y')
>>> t
<Time object: scale='utc' format='isot' value=2015-06-30T23:59:60.000>
Reference/API¶
astropy.time Package¶
Functions¶
|
If the current ERFA leap second table is out of date, try to update it. |
Classes¶
|
Configuration parameters for |
|
|
|
Represent and manipulate times and dates for astronomy. |
|
Base time class from which Time and TimeDelta inherit. |
|
Besselian Epoch year as floating point value(s) like 1950.0 |
|
Besselian Epoch year as string value(s) like 'B1950.0' |
|
Chandra X-ray Center seconds from 1998-01-01 00:00:00 TT. |
|
Represent date as Python standard library |
|
|
|
Time as a decimal year, with integer values corresponding to midnight of the first day of each year. |
|
Represent the time difference between two times. |
|
Time delta in datetime.timedelta |
|
Base class for time delta representations |
|
Time delta in Julian days (86400 SI seconds) |
Warning for missing unit or format in TimeDelta |
|
|
|
|
Time delta in SI seconds |
|
Base class for support floating point Besselian and Julian epoch dates |
|
Base class to support string Besselian and Julian epoch dates such as 'B1950.0' or 'J2000.0' respectively. |
|
FITS format: "[±Y]YYYY-MM-DD[THH:MM:SS[.sss]]". |
|
Base class for time representations. |
|
Base class for times that represent the interval from a particular epoch as a floating point multiple of a unit time interval (e.g. |
|
GPS time: seconds from 1980-01-06 00:00:00 UTC For example, 630720013.0 is midnight on January 1, 2000. |
|
ISO 8601 compliant date-time format "YYYY-MM-DD HH:MM:SS.sss...". |
|
ISO 8601 compliant date-time format "YYYY-MM-DDTHH:MM:SS.sss...". |
|
Container for meta information like name, description, format. |
|
Container for meta information like name, description, format. |
|
Julian Date time format. |
|
Julian Epoch year as floating point value(s) like 2000.0 |
|
Julian Epoch year as string value(s) like 'J2000.0' |
|
Modified Julian Date time format. |
|
|
|
Matplotlib |
|
Base class for string-like time representations. |
|
Base class for time formats that can uniquely create a time object without requiring an explicit format specifier. |
|
Unix time (UTC): seconds from 1970-01-01 00:00:00 UTC, ignoring leap seconds. |
|
Unix time (TAI): SI seconds elapsed since 1970-01-01 00:00:00 TAI (see caveats). |
|
ymdhms: A Time format to represent Time as year, month, day, hour, minute, second (thus the name ymdhms). |
|
Year, day-of-year and time as "YYYY:DOY:HH:MM:SS.sss...". |
|
Subclass of the |
Class Inheritance Diagram¶
Acknowledgments and Licenses¶
This package makes use of the PyERFA wrappers of the ERFA ANSI C library. The copyright of the ERFA software belongs to the NumFOCUS Foundation. The library is made available under the terms of the “BSD-three clauses” license.
The ERFA library is derived, with permission, from the International Astronomical Union’s “Standards of Fundamental Astronomy” (SOFA) library, available from http://www.iausofa.org.