Fix all dangling cross references in the docs
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@ -59,8 +59,8 @@ Changelog
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whether Earth satellites in orbit are in Earth’s shadow or not, thanks
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to a pull request from Jesse Coffey.
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* Added :func:`~skyfield.positionlib.position_of_radec()` to replace the
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poorly designed :func:`~skyfield.positionlib.position_from_radec()`.
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* Added :func:`~skyfield.positionlib.position_of_radec()`
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to replace the poorly designed ``position_from_radec()``.
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* Skyfield :class:`~skyfield.timelib.Time` objects now have microsecond
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internal accuracy, so round trips to and from Python datetimes should
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@ -187,7 +187,7 @@ Changelog
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`#296 <https://github.com/skyfielders/python-skyfield/issues/296>`_
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`#297 <https://github.com/skyfielders/python-skyfield/issues/297>`_
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* Added a :func:`~skyfield.almanac.rising_setting()` function for
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* Added a :func:`~skyfield.almanac.risings_and_settings()` function for
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computing rising and setting times.
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`#271 <https://github.com/skyfielders/python-skyfield/issues/271>`_
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@ -197,7 +197,7 @@ Changelog
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* Provided a constellation lookup routine through
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:func:`~skyfield.api.load_constellation_map()`.
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* Added :func:`~skyfield.positionlib.position_from_radec()`.
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* Added a ``position_from_radec()`` function.
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* Fixed the ``apparent()`` method in the case where a single observer
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position is observing an entire vector of target positions.
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@ -291,7 +291,7 @@ Changelog
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1.6 — 2018 July 25
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------------------
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* Both of the loader methods :meth:`~skyfield.iokit.Loader.load()` and
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* Both of the loader methods :meth:`~skyfield.iokit.Loader.open()` and
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:meth:`~skyfield.iokit.Loader.tle()` now accept not just URLs but also
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plain local file paths; they correctly re-download a remote file if
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“reload=True” is specified; and they allow specifying a different local
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@ -540,12 +540,13 @@ Changelog
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0.4
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---
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* To prevent confusion, the :meth:`~Time.astimezone()`
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and :meth:`~Time.utc_datetime()` methods
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* To prevent confusion, the :meth:`~skyfield.timelib.Time.astimezone()`
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and :meth:`~skyfield.timelib.Time.utc_datetime()` methods
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have been changed to return only a ``datetime`` object.
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If you also need a leap second flag returned,
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call the new methods :meth:`~Time.astimezone_and_leap_second()`
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and :meth:`~Time.utc_datetime_and_leap_second()`.
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call the new methods
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:meth:`~skyfield.timelib.Time.astimezone_and_leap_second()`
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and :meth:`~skyfield.timelib.Time.utc_datetime_and_leap_second()`.
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0.3
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---
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@ -10,4 +10,3 @@ satellite data and computing their positions with Skyfield.
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.. autoclass:: EarthSatellite
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:members:
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@ -135,10 +135,12 @@ The common API shared by planets, Earth locations, and Earth satellites.
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.. autosummary::
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VectorFunction
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VectorFunction.__add__
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VectorFunction.__sub__
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VectorFunction.at
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Either adding two vector functions ``v1 + v2`` or subtracting them ``v1 - v2``
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produces a new function of time that, when invoked with ``.at(t)``,
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returns the sum or difference of the vectors returned by the two functions.
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Planetary Ephemerides
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=====================
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@ -156,7 +158,10 @@ See :doc:`planets`.
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SpiceKernel.comments
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SpiceKernel.names
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SpiceKernel.decode
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SpiceKernel.__getitem__
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Kernels also support lookup using the Python ``kernel['Mars']`` syntax,
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in which case they return a function of time
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that returns vectors from the Solar System barycenter to the named body.
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Almanac
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=======
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@ -169,7 +174,6 @@ Routines to search for events like sunrise, sunset, and Moon phase.
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phase_angle
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fraction_illuminated
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find_discrete
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seasons
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sunrise_sunset
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dark_twilight_day
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@ -299,6 +303,15 @@ Constellations
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.. autofunction:: skyfield.api.load_constellation_map
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Searching
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=========
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.. currentmodule:: skyfield.searchlib
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.. autofunction:: find_discrete()
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.. autofunction:: find_maxima()
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.. autofunction:: find_minima()
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Osculating Orbital Elements
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===========================
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@ -3,8 +3,6 @@
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Earth Satellites
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==================
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.. currentmodule:: skyfield
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Skyfield is able to predict the positions of Earth satellites
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from the Two-Line Element (TLE) files published
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by organizations like `CelesTrak`_.
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@ -276,7 +274,7 @@ at which a particular satellite is overhead,
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you will probably want to learn more about its position at those times.
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The simplest form in which you can generate a satellite position
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is to call its :meth:`~skyfield.sgp4lib.EarthSatellite.at()` method,
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is to call its ``at()`` method,
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which will return an *x, y, z* position relative to the Earth’s center
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in the Geocentric Celestial Reference System.
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(GCRS coordinates are based on even more precise axes
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@ -598,7 +596,7 @@ Detecting Propagation Errors
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After building a satellite object,
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you can examine the *epoch* date and time
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when the TLE element set’s predictions are most accurate.
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The ``epoch`` attribute is a :class:`Time`,
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The ``epoch`` attribute is a :class:`~skyfield.timelib.Time`,
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so it supports all of the standard Skyfield date methods:
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.. testcode::
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@ -3,8 +3,6 @@
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Downloading and Using Data Files
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==================================
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.. currentmodule:: skyfield.api
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Your Skyfield programs will typically download two kinds of data file.
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First, Skyfield will need up-to-date tables about time —
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@ -67,7 +65,7 @@ and can start up without needing to access the network:
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Ready
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Most programs will run just fine using the default ``load()`` object
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provided in the :mod:`skyfield.api` module.
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provided in the ``skyfield.api`` module.
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But other programs may want to build their own loader
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so that they have the chance to specify non-default behavior.
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@ -2,8 +2,6 @@
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Planets, and Choosing an Ephemeris
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====================================
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.. currentmodule:: skyfield.api
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If you are interested in observing the planets,
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the Jet Propulsion Laboratory (JPL)
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has prepared long tables that predict the positions of the planets
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@ -12,7 +10,7 @@ A table of positions is called an *ephemeris*
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and those supplied by the JPL are of very high accuracy.
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You can ask Skyfield to download an ephemeris from the JPL
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by giving :func:`~skyfield.iokit.load()` a filename.
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by giving ``load()`` a filename.
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Or you can load an ephemeris that you’ve already saved to disk
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with :func:`~skyfield.iokit.load_file()`.
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@ -3,7 +3,7 @@
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Positions and Coordinates
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===========================
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.. currentmodule:: skyfield.api
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.. currentmodule:: skyfield.positionlib
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Skyfield is careful to distinguish the *position* of an object
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from the several choices of *coordinate*
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@ -258,7 +258,7 @@ Instead of using an acronym,
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Skyfield uses the class name :class:`Barycentric`
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for coordinates expressed in the ICRS.
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You can view the raw *x*, *y*, and *z* coordinates
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by asking Skyfield for their :attr:`~Barycentric.position` attribute:
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by asking Skyfield for their ``position`` attribute:
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.. testcode::
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@ -335,9 +335,9 @@ that we see in our sky:
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This light-delayed position is called the *astrometric* position,
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and is traditionally mapped on a star chart
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by the angles *right ascension* and *declination*
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that you can compute using the :meth:`~Position.radec()` method
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and display using their :meth:`~Angle.hstr()`
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and :meth:`~Angle.dstr()` methods:
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that you can compute using the :meth:`~ICRF.radec()` method
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and display using their :meth:`~skyfield.units.Angle.hstr()`
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and :meth:`~skyfield.units.Angle.dstr()` methods:
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.. testcode::
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@ -592,7 +592,7 @@ call the
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:meth:`~skyfield.positionlib.ICRF.separation_from()`
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method of one of the positions
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and pass it the other position as its argument.
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The result will be an :class:`~Angle` object.
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The result will be an :class:`~skyfield.units.Angle` object.
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If instead you want to know the distance between two positions,
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subtract the position you want to use as the starting point
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@ -14,10 +14,6 @@ that looks for a moment of position or alignment
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that fits some definition that you are looking for.
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The other is an “extremum” search
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where you want to know when a value reaches its maximum or minimum value.
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For the moment,
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this documentation page only discusses searching for events;
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check out the ``find_maxima()`` routine in the ``searchlib.py`` source code
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for how Skyfield searches for maximum or minimum values.
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Finding discrete events
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=======================
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@ -3,7 +3,7 @@
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Stars and Distant Objects
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===========================
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.. currentmodule:: skyfield.api
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.. currentmodule:: skyfield.starlib
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Skyfield can generate positions for stars or and other distant objects
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that you either load from a star catalog, or else for which you can
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@ -26,7 +26,7 @@ The supported time scales are:
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To specify a time,
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first build a :class:`Timescale` object
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by calling Skyfield’s :meth:`load.timescale()` routine.
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by calling Skyfield’s ``load.timescale()`` routine.
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This downloads several data files from international authorities —
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the United States Naval Observatory
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and the International Earth Rotation Service —
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@ -799,7 +799,8 @@ or invokes a computation that needs their value:
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this Julian date.
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You will typically never need to access these matrices yourself,
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as they are used automatically by the :meth:`Position.radec()`
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as they are used automatically
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by the :meth:`~skyfield.positionlib.ICRF.radec()`
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method when you use its ``epoch=`` parameter
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to ask for a right ascension and declination
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in the dynamical reference system,
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EPSILON = 0.001 / DAY_S
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def find_discrete(start_time, end_time, f, epsilon=EPSILON, num=12):
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"""Find the times when a function changes value.
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"""Find the times at which a discrete function of time changes value.
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Search between ``start_time`` and ``end_time``, which should both be
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:class:`~skyfield.timelib.Time` objects, for the occasions where the
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function ``f`` changes from one value to another. Use this to
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search for events like sunrise or moon phases.
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A tuple of two arrays is returned. The first array gives the times
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at which the input function changes, and the second array specifies
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the new value of the function at each corresponding time.
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This is an expensive operation as it needs to repeatedly call the
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function to narrow down the times that it changes. It continues
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searching until it knows each time to at least an accuracy of
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``epsilon`` Julian days. At each step, it creates an array of
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``num`` new points between the lower and upper bound that it has
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established for each transition. These two values can be changed to
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tune the behavior of the search.
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This routine is used to find instantaneous events like sunrise,
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transits, and the seasons. See :doc:`searches` for how to use it
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yourself.
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"""
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ts = start_time.ts
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return ts.tt_jd(ends), y
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def find_minima(start_time, end_time, f, epsilon=1.0 / DAY_S, num=12):
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"""Find the local minima in the values returned by a function of time.
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This routine is used to find events like minimum elongation. See
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:doc:`searches` for how to use it yourself.
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"""
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def g(t): return -f(t)
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g.rough_period = getattr(f, 'rough_period', None)
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g.step_days = getattr(f, 'step_days', None)
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return t, -y
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def find_maxima(start_time, end_time, f, epsilon=1.0 / DAY_S, num=12):
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"""Find the local maxima in the values returned by a function of time.
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This routine is used to find events like highest altitude and
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maximum elongation. See :doc:`searches` for how to use it yourself.
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"""
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# @@ @@_@@ @@_@@_@@_@@
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# / \ / \ / \
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# @@ @@ @@ @@ @@ @@
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class EarthSatellite(VectorFunction):
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"""An Earth satellite loaded from a TLE file and propagated with SGP4.
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An earth satellite object is a Skyfield vector function, so call its
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:meth:`~skyfield.vectorlib.VectorSum.at()` method to generate its
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position in the sky, or use addition and subtraction to combine it
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with other vectors.
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An earth satellite object is a Skyfield vector function, so you can
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either call its ``at()`` method to generate its position in the sky
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or else use addition and subtraction to combine it with other
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vectors.
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Satellite parameters are generally only accurate for a week or two
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around the *epoch* of the parameters, the date for which they were
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@ -95,6 +95,7 @@ class Distance(object):
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return Distance(au=length_of(self.au))
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def light_seconds(self):
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"""Return the length of this vector in light seconds."""
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return self.m / C
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def to(self, unit):
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