# -*- coding: utf-8 -*-
"""
========================================================================
Transforming positions and velocities to and from a Galactocentric frame
========================================================================

This document shows a few examples of how to use and customize the
`~astropy.coordinates.Galactocentric` frame to transform Heliocentric sky
positions, distance, proper motions, and radial velocities to a Galactocentric,
Cartesian frame, and the same in reverse.

The main configurable parameters of the `~astropy.coordinates.Galactocentric`
frame control the position and velocity of the solar system barycenter within
the Galaxy. These are specified by setting the ICRS coordinates of the
Galactic center, the distance to the Galactic center (the sun-galactic center
line is always assumed to be the x-axis of the Galactocentric frame), and the
Cartesian 3-velocity of the sun in the Galactocentric frame. We'll first
demonstrate how to customize these values, then show how to set the solar motion
instead by inputting the proper motion of Sgr A*.

Note that, for brevity, we may refer to the solar system barycenter as just "the
sun" in the examples below.


*By: Adrian Price-Whelan*

*License: BSD*


"""

##############################################################################
# Make `print` work the same in all versions of Python, set up numpy,
# matplotlib, and use a nicer set of plot parameters:

import numpy as np
import matplotlib.pyplot as plt
from astropy.visualization import astropy_mpl_style
plt.style.use(astropy_mpl_style)


##############################################################################
# Import the necessary astropy subpackages

import astropy.coordinates as coord
import astropy.units as u

##############################################################################
# Let's first define a barycentric coordinate and velocity in the ICRS frame.
# We'll use the data for the star HD 39881 from the `Simbad
# <simbad.harvard.edu/simbad/>`_ database:

c1 = coord.SkyCoord(ra=89.014303*u.degree, dec=13.924912*u.degree,
                    distance=(37.59*u.mas).to(u.pc, u.parallax()),
                    pm_ra_cosdec=372.72*u.mas/u.yr,
                    pm_dec=-483.69*u.mas/u.yr,
                    radial_velocity=0.37*u.km/u.s,
                    frame='icrs')

##############################################################################
# This is a high proper-motion star; suppose we'd like to transform its position
# and velocity to a Galactocentric frame to see if it has a large 3D velocity
# as well. To use the Astropy default solar position and motion parameters, we
# can simply do:

gc1 = c1.transform_to(coord.Galactocentric)

##############################################################################
# From here, we can access the components of the resulting
# `~astropy.coordinates.Galactocentric` instance to see the 3D Cartesian
# velocity components:

print(gc1.v_x, gc1.v_y, gc1.v_z)

##############################################################################
# The default parameters for the `~astropy.coordinates.Galactocentric` frame
# are detailed in the linked documentation, but we can modify the most commonly
# changes values using the keywords ``galcen_distance``, ``galcen_v_sun``, and
# ``z_sun`` which set the sun-Galactic center distance, the 3D velocity vector
# of the sun, and the height of the sun above the Galactic midplane,
# respectively. The velocity of the sun can be specified as an
# `~astropy.units.Quantity` object with velocity units and is interepreted as a
# Cartesian velocity, as in the example below. Note that, as with the positions,
# the Galactocentric frame is a right-handed system (i.e., the Sun is at negative
# x values) so ``v_x`` is opposite of the Galactocentric radial velocity:

v_sun = [11.1, 244, 7.25] * (u.km / u.s)  # [vx, vy, vz]
gc_frame = coord.Galactocentric(
    galcen_distance=8*u.kpc,
    galcen_v_sun=v_sun,
    z_sun=0*u.pc)

##############################################################################
# We can then transform to this frame instead, with our custom parameters:

gc2 = c1.transform_to(gc_frame)
print(gc2.v_x, gc2.v_y, gc2.v_z)

##############################################################################
# It's sometimes useful to specify the solar motion using the `proper motion
# of Sgr A* <https://arxiv.org/abs/astro-ph/0408107>`_ instead of Cartesian
# velocity components. With an assumed distance, we can convert proper motion
# components to Cartesian velocity components using `astropy.units`:

galcen_distance = 8*u.kpc
pm_gal_sgrA = [-6.379, -0.202] * u.mas/u.yr # from Reid & Brunthaler 2004
vy, vz = -(galcen_distance * pm_gal_sgrA).to(u.km/u.s, u.dimensionless_angles())

##############################################################################
# We still have to assume a line-of-sight velocity for the Galactic center,
# which we will again take to be 11 km/s:
vx = 11.1 * u.km/u.s
v_sun2 = u.Quantity([vx, vy, vz])  # List of Quantity -> a single Quantity

gc_frame2 = coord.Galactocentric(galcen_distance=galcen_distance,
                                 galcen_v_sun=v_sun2,
                                 z_sun=0*u.pc)
gc3 = c1.transform_to(gc_frame2)
print(gc3.v_x, gc3.v_y, gc3.v_z)

##############################################################################
# The transformations also work in the opposite direction. This can be useful
# for transforming simulated or theoretical data to observable quantities. As
# an example, we'll generate 4 theoretical circular orbits at different
# Galactocentric radii with the same circular velocity, and transform them to
# Heliocentric coordinates:

ring_distances = np.arange(10, 25+1, 5) * u.kpc
circ_velocity = 220 * u.km/u.s

phi_grid = np.linspace(90, 270, 512) * u.degree # grid of azimuths
ring_rep = coord.CylindricalRepresentation(
    rho=ring_distances[:,np.newaxis],
    phi=phi_grid[np.newaxis],
    z=np.zeros_like(ring_distances)[:,np.newaxis])

angular_velocity = (-circ_velocity / ring_distances).to(u.mas/u.yr,
                                                        u.dimensionless_angles())
ring_dif = coord.CylindricalDifferential(
    d_rho=np.zeros(phi_grid.shape)[np.newaxis]*u.km/u.s,
    d_phi=angular_velocity[:,np.newaxis],
    d_z=np.zeros(phi_grid.shape)[np.newaxis]*u.km/u.s
)

ring_rep = ring_rep.with_differentials(ring_dif)
gc_rings = coord.SkyCoord(ring_rep, frame=coord.Galactocentric)

##############################################################################
# First, let's visualize the geometry in Galactocentric coordinates. Here are
# the positions and velocities of the rings; note that in the velocity plot,
# the velocities of the 4 rings are identical and thus overlaid under the same
# curve:
fig,axes = plt.subplots(1, 2, figsize=(12,6))

# Positions
axes[0].plot(gc_rings.x.T, gc_rings.y.T, marker='None', linewidth=3)
axes[0].text(-8., 0, r'$\odot$', fontsize=20)

axes[0].set_xlim(-30, 30)
axes[0].set_ylim(-30, 30)

axes[0].set_xlabel('$x$ [kpc]')
axes[0].set_ylabel('$y$ [kpc]')

# Velocities
axes[1].plot(gc_rings.v_x.T, gc_rings.v_y.T, marker='None', linewidth=3)

axes[1].set_xlim(-250, 250)
axes[1].set_ylim(-250, 250)

axes[1].set_xlabel(f"$v_x$ [{(u.km / u.s).to_string('latex_inline')}]")
axes[1].set_ylabel(f"$v_y$ [{(u.km / u.s).to_string('latex_inline')}]")

fig.tight_layout()

plt.show()

##############################################################################
# Now we can transform to Galactic coordinates and visualize the rings in
# observable coordinates:
gal_rings = gc_rings.transform_to(coord.Galactic)

fig, ax = plt.subplots(1, 1, figsize=(8, 6))
for i in range(len(ring_distances)):
    ax.plot(gal_rings[i].l.degree, gal_rings[i].pm_l_cosb.value,
            label=str(ring_distances[i]), marker='None', linewidth=3)

ax.set_xlim(360, 0)

ax.set_xlabel('$l$ [deg]')
ax.set_ylabel(fr'$\mu_l \, \cos b$ [{(u.mas/u.yr).to_string("latex_inline")}]')

ax.legend()

plt.show()
