more
This commit is contained in:
parent
aa0b61405b
commit
82c6e962db
2
http.go
2
http.go
|
@ -29,9 +29,11 @@ func TelemRouter(log *slog.Logger, broker *JBroker) http.Handler {
|
||||||
w.Write([]byte(skylab.SkylabDefinitions))
|
w.Write([]byte(skylab.SkylabDefinitions))
|
||||||
})
|
})
|
||||||
|
|
||||||
|
// heartbeat request.
|
||||||
r.Get("/ping", func(w http.ResponseWriter, r *http.Request) {
|
r.Get("/ping", func(w http.ResponseWriter, r *http.Request) {
|
||||||
w.Write([]byte("pong"))
|
w.Write([]byte("pong"))
|
||||||
})
|
})
|
||||||
|
|
||||||
r.Mount("/api/v1", apiV1(broker))
|
r.Mount("/api/v1", apiV1(broker))
|
||||||
|
|
||||||
// To future residents - you can add new API calls/systems in /api/v2
|
// To future residents - you can add new API calls/systems in /api/v2
|
||||||
|
|
|
@ -1,11 +1,12 @@
|
||||||
# hyperspeed forward and backwards analytics engine
|
# hyperspeed forward and backwards analytics engine
|
||||||
|
|
||||||
import numpy.typing as npt
|
|
||||||
from scipy.integrate import solve_bvp, solve_ivp
|
|
||||||
|
|
||||||
from jax import jit, grad, vmap
|
import numpy as np
|
||||||
|
|
||||||
import jax.numpy as np
|
from numba import jit
|
||||||
|
|
||||||
|
|
||||||
|
# import jax.numpy as np
|
||||||
|
|
||||||
|
|
||||||
# TODO: define 3d vector space - x,y,z oriented around car/world?
|
# TODO: define 3d vector space - x,y,z oriented around car/world?
|
||||||
|
@ -70,7 +71,7 @@ def make_cubic(a, b, c, d):
|
||||||
"""returns a simple cubic function"""
|
"""returns a simple cubic function"""
|
||||||
|
|
||||||
def poly(x):
|
def poly(x):
|
||||||
return a + b * x + c * (x**2) + (x**3) / d
|
return a + b * x + c * (x ** 2) + (x ** 3) / d
|
||||||
|
|
||||||
return jit(poly)
|
return jit(poly)
|
||||||
|
|
||||||
|
@ -484,16 +485,18 @@ def helio_vector(vec, jme):
|
||||||
)
|
)
|
||||||
|
|
||||||
|
|
||||||
def solar_position(timestamp, latitude, longitude):
|
def solar_position(timestamp, latitude, longitude, elevation):
|
||||||
"""Calculate the position of the sun at a given location and time.
|
"""Calculate the position of the sun at a given location and time.
|
||||||
|
|
||||||
Args:
|
Args:
|
||||||
timestamp (array-like): The timestamp(s) to calculate.
|
timestamp (array-like): The timestamp(s) at each point.
|
||||||
|
latitude (array-like): The latitude(s) of each point.
|
||||||
|
longitude (array-like): The longitude(s) of each point.
|
||||||
|
elevation (array-like): The elevation of each point.
|
||||||
|
|
||||||
Returns:
|
Returns:
|
||||||
ndarray: An array containing the altitude and azimuth for each timestamp.
|
ndarray: An array containing the altitude and azimuth for each point.
|
||||||
"""
|
"""
|
||||||
timestamp = np.array(timestamp)
|
|
||||||
jd = timestamp / 86400.0 + 2440587.5
|
jd = timestamp / 86400.0 + 2440587.5
|
||||||
jc = (jd - 2451545) / 36525
|
jc = (jd - 2451545) / 36525
|
||||||
|
|
||||||
|
@ -509,7 +512,7 @@ def solar_position(timestamp, latitude, longitude):
|
||||||
# heliocentric longitude
|
# heliocentric longitude
|
||||||
l_rad = np.zeros_like(timestamp)
|
l_rad = np.zeros_like(timestamp)
|
||||||
for idx, vec in enumerate(HELIO_L):
|
for idx, vec in enumerate(HELIO_L):
|
||||||
l_rad = l_rad + helio_vector(vec, jme) * jme**idx
|
l_rad = l_rad + helio_vector(vec, jme) * jme ** idx
|
||||||
|
|
||||||
l_rad = l_rad / 10e8
|
l_rad = l_rad / 10e8
|
||||||
l_deg = np.rad2deg(l_rad) % 360
|
l_deg = np.rad2deg(l_rad) % 360
|
||||||
|
@ -517,14 +520,14 @@ def solar_position(timestamp, latitude, longitude):
|
||||||
# heliocentric latitude
|
# heliocentric latitude
|
||||||
b_rad = np.zeros_like(timestamp)
|
b_rad = np.zeros_like(timestamp)
|
||||||
for idx, vec in enumerate(HELIO_B):
|
for idx, vec in enumerate(HELIO_B):
|
||||||
b_rad = b_rad + helio_vector(vec, jme) * jme**idx
|
b_rad = b_rad + helio_vector(vec, jme) * jme ** idx
|
||||||
b_rad = b_rad / 10e8
|
b_rad = b_rad / 10e8
|
||||||
b_deg = np.rad2deg(b_rad) % 360
|
b_deg = np.rad2deg(b_rad) % 360
|
||||||
|
|
||||||
# heliocentric radius
|
# heliocentric radius
|
||||||
r_rad = np.zeros_like(timestamp)
|
r_rad = np.zeros_like(timestamp)
|
||||||
for idx, vec in enumerate(HELIO_R):
|
for idx, vec in enumerate(HELIO_R):
|
||||||
r_rad = r_rad + helio_vector(vec, jme) * jme**idx
|
r_rad = r_rad + helio_vector(vec, jme) * jme ** idx
|
||||||
r_rad = r_rad / 10e8
|
r_rad = r_rad / 10e8
|
||||||
r_deg = np.rad2deg(r_rad) % 360
|
r_deg = np.rad2deg(r_rad) % 360
|
||||||
|
|
||||||
|
@ -532,7 +535,7 @@ def solar_position(timestamp, latitude, longitude):
|
||||||
beta = -1 * b_deg
|
beta = -1 * b_deg
|
||||||
|
|
||||||
def cubic_poly(a, b, c, d):
|
def cubic_poly(a, b, c, d):
|
||||||
return a + b * jce + c * jce**2 + (jce**3) / d
|
return a + b * jce + c * jce ** 2 + (jce ** 3) / d
|
||||||
|
|
||||||
X0 = cubic_poly(297.85036, 445267.111480, -0.0019142, 189474)
|
X0 = cubic_poly(297.85036, 445267.111480, -0.0019142, 189474)
|
||||||
X1 = cubic_poly(357.52772, 35999.050340, -0.0001603, -300000)
|
X1 = cubic_poly(357.52772, 35999.050340, -0.0001603, -300000)
|
||||||
|
@ -544,19 +547,19 @@ def solar_position(timestamp, latitude, longitude):
|
||||||
|
|
||||||
nut = NUTATION_ABCD_ARRAY
|
nut = NUTATION_ABCD_ARRAY
|
||||||
|
|
||||||
## TODO: these are gross - use loops instead of broadcasting?
|
# TODO: these are gross - use loops instead of broadcasting?
|
||||||
|
# FIXME: use guvectorize, treat jce as a scalar.
|
||||||
d_psi = (nut[:, 0] + jce[..., np.newaxis] * nut[:, 1]) * np.sin(
|
d_psi = (nut[:, 0] + jce[..., np.newaxis] * nut[:, 1]) * np.sin(
|
||||||
np.sum(X[:, np.newaxis, :] * NUTATION_YTERM_ARRAY[np.newaxis, ...], axis=2)
|
np.sum(X[:, np.newaxis, :] * NUTATION_YTERM_ARRAY[np.newaxis, ...], axis=2)
|
||||||
)
|
)
|
||||||
d_psi = np.sum(d_psi, axis=-1) / 36, 000, 000
|
d_psi = np.sum(d_psi, axis=-1) / 36, 000, 000
|
||||||
|
|
||||||
|
|
||||||
d_epsilon = (nut[:, 2] + jce[..., np.newaxis] * nut[:, 3]) * np.cos(
|
d_epsilon = (nut[:, 2] + jce[..., np.newaxis] * nut[:, 3]) * np.cos(
|
||||||
np.sum(X[:, np.newaxis, :] * NUTATION_YTERM_ARRAY[np.newaxis, ...], axis=2)
|
np.sum(X[:, np.newaxis, :] * NUTATION_YTERM_ARRAY[np.newaxis, ...], axis=2)
|
||||||
)
|
)
|
||||||
d_epsilon = np.sum(d_epsilon, axis=-1) / 36, 000, 000
|
d_epsilon = np.sum(d_epsilon, axis=-1) / 36, 000, 000
|
||||||
|
|
||||||
u = jme[:, np.newaxis] / 10 * np.arange(0,10).reshape((1,-1))
|
u = jme[:, np.newaxis] / 10 * np.arange(0, 10).reshape((1, -1))
|
||||||
epsilon_0 = np.array(
|
epsilon_0 = np.array(
|
||||||
[
|
[
|
||||||
84381.448,
|
84381.448,
|
||||||
|
@ -576,3 +579,38 @@ def solar_position(timestamp, latitude, longitude):
|
||||||
d_tau = -20.4898 / (3600 * r_deg)
|
d_tau = -20.4898 / (3600 * r_deg)
|
||||||
sun_longitude = theta + d_psi + d_tau
|
sun_longitude = theta + d_psi + d_tau
|
||||||
|
|
||||||
|
v_0 = 280.46061837 + 360.98564736629 * (jd - 2451545) + 0.000387933 * jc ** 2 - jc ** 3 / 38710000
|
||||||
|
v_0 = v_0 % 360
|
||||||
|
|
||||||
|
v = v_0 + d_psi * np.cos(np.deg2rad(epsilon))
|
||||||
|
|
||||||
|
alpha = np.arctan2(np.sin(np.radians(sun_longitude)) *
|
||||||
|
np.cos(np.radians(epsilon)) -
|
||||||
|
np.tan(np.radians(beta)) *
|
||||||
|
np.sin(np.radians(epsilon)),
|
||||||
|
np.cos(np.radians(sun_longitude)))
|
||||||
|
alpha_deg = np.rad2deg(alpha) % 360
|
||||||
|
delta = np.arcsin(
|
||||||
|
np.sin(np.radians(beta)) *
|
||||||
|
np.cos(np.radians(epsilon)) +
|
||||||
|
np.cos(np.radians(beta)) *
|
||||||
|
np.sin(np.radians(epsilon)) *
|
||||||
|
np.cos(np.radians(sun_longitude))
|
||||||
|
)
|
||||||
|
delta_deg = np.rad2deg(delta) % 360
|
||||||
|
|
||||||
|
h = v + latitude - alpha_deg
|
||||||
|
|
||||||
|
xi_deg = 8.794 / (3600 * r_deg)
|
||||||
|
u = np.arctan(0.99664719 * np.tan(latitude))
|
||||||
|
|
||||||
|
x = np.cos(u) + elevation / 6378140 * np.cos(latitude)
|
||||||
|
|
||||||
|
y = 0.99664719 * np.sin(u) + elevation / 6378140 * np.sin(latitude)
|
||||||
|
|
||||||
|
d_alpha = np.arctan2(-1 * x * np.sin(np.radians(xi_deg)) * np.sin(np.radians(h)), np.cos(delta))
|
||||||
|
d_alpha = np.rad2deg(d_alpha)
|
||||||
|
alpha_prime = alpha_deg + d_alpha
|
||||||
|
delta_prime = np.arctan2((np.sin(delta) - y * np.sin(np.radians(xi_deg))) * np.cos(np.radians(d_alpha)),
|
||||||
|
np.cos(delta) - x * np.sin(np.radians(xi_deg)) * np.cos(np.radians(h)))
|
||||||
|
topo_local_hour_angle_deg = h - d_alpha
|
||||||
|
|
Loading…
Reference in a new issue