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Duplicate from elonmuskceo/shiny-orbit-simulation
Browse filesCo-authored-by: Elon Musk <elonmuskceo@users.noreply.huggingface.co>
- .gitattributes +33 -0
- Dockerfile +22 -0
- README.md +11 -0
- app.py +229 -0
- requirements.txt +6 -0
- simulation.py +203 -0
- www/coords.png +0 -0
.gitattributes
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*.7z filter=lfs diff=lfs merge=lfs -text
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*.pb filter=lfs diff=lfs merge=lfs -text
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*.rar filter=lfs diff=lfs merge=lfs -text
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*.safetensors filter=lfs diff=lfs merge=lfs -text
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saved_model/**/* filter=lfs diff=lfs merge=lfs -text
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*.tar.* filter=lfs diff=lfs merge=lfs -text
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*.tflite filter=lfs diff=lfs merge=lfs -text
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*tfevents* filter=lfs diff=lfs merge=lfs -text
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Dockerfile
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FROM ubuntu:kinetic
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# Doesn't usually have an "upgrade"
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RUN apt-get update \
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&& DEBIAN_FRONTEND=noninteractive \
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apt-get install --no-install-recommends --assume-yes \
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build-essential \
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python3 \
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python3-dev \
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python3-pip
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COPY requirements.txt .
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RUN pip install -r requirements.txt
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COPY . .
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ENTRYPOINT ["/bin/sh", "-c"]
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EXPOSE 7860
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CMD ["shiny run --port 7860 --host 0.0.0.0 app.py"]
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README.md
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---
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title: Shiny Orbit Simulation
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emoji: 🪐
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colorFrom: green
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colorTo: green
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sdk: docker
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pinned: false
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duplicated_from: elonmuskceo/shiny-orbit-simulation
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---
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Check out the configuration reference at https://huggingface.co/docs/hub/spaces-config-reference
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app.py
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from pathlib import Path
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| 2 |
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from simulation import Body, Simulation, nbody_solve, spherical_to_cartesian
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| 3 |
+
import matplotlib.pyplot as plt
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| 4 |
+
import astropy.units as u
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| 5 |
+
import numpy as np
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| 6 |
+
|
| 7 |
+
from shiny import App, reactive, render, ui
|
| 8 |
+
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| 9 |
+
# This application adapted from RK4 Orbit Integrator tutorial in Python for Astronomers
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| 10 |
+
# https://prappleizer.github.io/
|
| 11 |
+
|
| 12 |
+
|
| 13 |
+
def panel_box(*args, **kwargs):
|
| 14 |
+
return ui.div(
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| 15 |
+
ui.div(*args, class_="card-body"),
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| 16 |
+
**kwargs,
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| 17 |
+
class_="card mb-3",
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| 18 |
+
)
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| 19 |
+
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| 20 |
+
|
| 21 |
+
app_ui = ui.page_fluid(
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| 22 |
+
{"class": "p-4"},
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| 23 |
+
ui.row(
|
| 24 |
+
ui.column(
|
| 25 |
+
4,
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| 26 |
+
panel_box(
|
| 27 |
+
ui.input_slider("days", "Simulation duration (days)", 0, 200, value=60),
|
| 28 |
+
ui.input_slider(
|
| 29 |
+
"step_size",
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| 30 |
+
"Simulation time step (hours)",
|
| 31 |
+
0,
|
| 32 |
+
24,
|
| 33 |
+
value=4,
|
| 34 |
+
step=0.5,
|
| 35 |
+
),
|
| 36 |
+
ui.input_action_button(
|
| 37 |
+
"run", "Run simulation", class_="btn-primary w-100"
|
| 38 |
+
),
|
| 39 |
+
),
|
| 40 |
+
ui.navset_tab_card(
|
| 41 |
+
ui.nav(
|
| 42 |
+
"Earth",
|
| 43 |
+
ui.input_checkbox("earth", "Enable", True),
|
| 44 |
+
ui.panel_conditional(
|
| 45 |
+
"input.earth",
|
| 46 |
+
ui.input_numeric(
|
| 47 |
+
"earth_mass",
|
| 48 |
+
"Mass (10^22 kg)",
|
| 49 |
+
597.216,
|
| 50 |
+
),
|
| 51 |
+
ui.input_slider(
|
| 52 |
+
"earth_speed",
|
| 53 |
+
"Speed (km/s)",
|
| 54 |
+
0,
|
| 55 |
+
1,
|
| 56 |
+
value=0.0126,
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| 57 |
+
step=0.001,
|
| 58 |
+
),
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| 59 |
+
ui.input_slider("earth_theta", "Angle (5)", 0, 360, value=270),
|
| 60 |
+
ui.input_slider("earth_phi", "5", 0, 180, value=90),
|
| 61 |
+
),
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| 62 |
+
),
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| 63 |
+
ui.nav(
|
| 64 |
+
"Moon",
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| 65 |
+
ui.input_checkbox("moon", "Enable", True),
|
| 66 |
+
ui.panel_conditional(
|
| 67 |
+
"input.moon",
|
| 68 |
+
ui.input_numeric("moon_mass", "Mass (10^22 kg)", 7.347),
|
| 69 |
+
ui.input_slider(
|
| 70 |
+
"moon_speed", "Speed (km/s)", 0, 2, value=1.022, step=0.001
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| 71 |
+
),
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| 72 |
+
ui.input_slider("moon_theta", "Angle (5)", 0, 360, value=90),
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| 73 |
+
ui.input_slider("moon_phi", "5", 0, 180, value=90),
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| 74 |
+
),
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| 75 |
+
),
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| 76 |
+
ui.nav(
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| 77 |
+
"Planet X",
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| 78 |
+
ui.input_checkbox("planetx", "Enable", False),
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| 79 |
+
ui.output_ui("planetx_controls"),
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| 80 |
+
ui.panel_conditional(
|
| 81 |
+
"input.planetx",
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| 82 |
+
ui.input_numeric("planetx_mass", "Mass (10^22 kg)", 7.347),
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| 83 |
+
ui.input_slider(
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| 84 |
+
"planetx_speed",
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| 85 |
+
"Speed (km/s)",
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| 86 |
+
0,
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| 87 |
+
2,
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| 88 |
+
value=1.022,
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| 89 |
+
step=0.001,
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| 90 |
+
),
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| 91 |
+
ui.input_slider("planetx_theta", "Angle (5)", 0, 360, 270),
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| 92 |
+
ui.input_slider("planetx_phi", "5", 0, 180, 90),
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| 93 |
+
),
|
| 94 |
+
),
|
| 95 |
+
),
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| 96 |
+
),
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| 97 |
+
ui.column(
|
| 98 |
+
8,
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| 99 |
+
ui.output_plot("orbits", width="500px", height="500px"),
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| 100 |
+
ui.img(src="coords.png", style="width: 100%; max-width: 250px;"),
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| 101 |
+
),
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| 102 |
+
),
|
| 103 |
+
)
|
| 104 |
+
|
| 105 |
+
|
| 106 |
+
def server(input, output, session):
|
| 107 |
+
def earth_body():
|
| 108 |
+
v = spherical_to_cartesian(
|
| 109 |
+
input.earth_theta(), input.earth_phi(), input.earth_speed()
|
| 110 |
+
)
|
| 111 |
+
|
| 112 |
+
return Body(
|
| 113 |
+
mass=input.earth_mass() * 10e21 * u.kg,
|
| 114 |
+
x_vec=np.array([0, 0, 0]) * u.km,
|
| 115 |
+
v_vec=np.array(v) * u.km / u.s,
|
| 116 |
+
name="Earth",
|
| 117 |
+
)
|
| 118 |
+
|
| 119 |
+
def moon_body():
|
| 120 |
+
v = spherical_to_cartesian(
|
| 121 |
+
input.moon_theta(), input.moon_phi(), input.moon_speed()
|
| 122 |
+
)
|
| 123 |
+
|
| 124 |
+
return Body(
|
| 125 |
+
mass=input.moon_mass() * 10e21 * u.kg,
|
| 126 |
+
x_vec=np.array([3.84e5, 0, 0]) * u.km,
|
| 127 |
+
v_vec=np.array(v) * u.km / u.s,
|
| 128 |
+
name="Moon",
|
| 129 |
+
)
|
| 130 |
+
|
| 131 |
+
def planetx_body():
|
| 132 |
+
v = spherical_to_cartesian(
|
| 133 |
+
input.planetx_theta(), input.planetx_phi(), input.planetx_speed()
|
| 134 |
+
)
|
| 135 |
+
|
| 136 |
+
return Body(
|
| 137 |
+
mass=input.planetx_mass() * 10e21 * u.kg,
|
| 138 |
+
x_vec=np.array([-3.84e5, 0, 0]) * u.km,
|
| 139 |
+
v_vec=np.array(v) * u.km / u.s,
|
| 140 |
+
name="Planet X",
|
| 141 |
+
)
|
| 142 |
+
|
| 143 |
+
def simulation():
|
| 144 |
+
bodies = []
|
| 145 |
+
if input.earth():
|
| 146 |
+
bodies.append(earth_body())
|
| 147 |
+
if input.moon():
|
| 148 |
+
bodies.append(moon_body())
|
| 149 |
+
if input.planetx():
|
| 150 |
+
bodies.append(planetx_body())
|
| 151 |
+
|
| 152 |
+
simulation_ = Simulation(bodies)
|
| 153 |
+
simulation_.set_diff_eq(nbody_solve)
|
| 154 |
+
|
| 155 |
+
return simulation_
|
| 156 |
+
|
| 157 |
+
has_run = False
|
| 158 |
+
|
| 159 |
+
@output
|
| 160 |
+
@render.plot
|
| 161 |
+
@reactive.event(input.run, ignore_none=False)
|
| 162 |
+
def orbits():
|
| 163 |
+
return make_orbit_plot()
|
| 164 |
+
|
| 165 |
+
def make_orbit_plot():
|
| 166 |
+
sim = simulation()
|
| 167 |
+
n_steps = input.days() * 24 / input.step_size()
|
| 168 |
+
with ui.Progress(min=1, max=n_steps) as p:
|
| 169 |
+
sim.run(input.days() * u.day, input.step_size() * u.hr, progress=p)
|
| 170 |
+
|
| 171 |
+
sim_hist = sim.history
|
| 172 |
+
end_idx = len(sim_hist) - 1
|
| 173 |
+
|
| 174 |
+
fig = plt.figure()
|
| 175 |
+
|
| 176 |
+
ax = plt.axes(projection="3d")
|
| 177 |
+
|
| 178 |
+
n_bodies = int(sim_hist.shape[1] / 6)
|
| 179 |
+
for i in range(0, n_bodies):
|
| 180 |
+
ax.scatter3D(
|
| 181 |
+
sim_hist[end_idx, i * 6],
|
| 182 |
+
sim_hist[end_idx, i * 6 + 1],
|
| 183 |
+
sim_hist[end_idx, i * 6 + 2],
|
| 184 |
+
s=50,
|
| 185 |
+
)
|
| 186 |
+
ax.plot3D(
|
| 187 |
+
sim_hist[:, i * 6],
|
| 188 |
+
sim_hist[:, i * 6 + 1],
|
| 189 |
+
sim_hist[:, i * 6 + 2],
|
| 190 |
+
)
|
| 191 |
+
|
| 192 |
+
ax.view_init(30, 20)
|
| 193 |
+
set_axes_equal(ax)
|
| 194 |
+
|
| 195 |
+
return fig
|
| 196 |
+
|
| 197 |
+
|
| 198 |
+
www_dir = Path(__file__).parent / "www"
|
| 199 |
+
app = App(app_ui, server, static_assets=www_dir)
|
| 200 |
+
|
| 201 |
+
|
| 202 |
+
# https://stackoverflow.com/a/31364297/412655
|
| 203 |
+
def set_axes_equal(ax):
|
| 204 |
+
"""Make axes of 3D plot have equal scale so that spheres appear as spheres,
|
| 205 |
+
cubes as cubes, etc.. This is one possible solution to Matplotlib's
|
| 206 |
+
ax.set_aspect('equal') and ax.axis('equal') not working for 3D.
|
| 207 |
+
|
| 208 |
+
Input
|
| 209 |
+
ax: a matplotlib axis, e.g., as output from plt.gca().
|
| 210 |
+
"""
|
| 211 |
+
|
| 212 |
+
x_limits = ax.get_xlim3d()
|
| 213 |
+
y_limits = ax.get_ylim3d()
|
| 214 |
+
z_limits = ax.get_zlim3d()
|
| 215 |
+
|
| 216 |
+
x_range = abs(x_limits[1] - x_limits[0])
|
| 217 |
+
x_middle = np.mean(x_limits)
|
| 218 |
+
y_range = abs(y_limits[1] - y_limits[0])
|
| 219 |
+
y_middle = np.mean(y_limits)
|
| 220 |
+
z_range = abs(z_limits[1] - z_limits[0])
|
| 221 |
+
z_middle = np.mean(z_limits)
|
| 222 |
+
|
| 223 |
+
# The plot bounding box is a sphere in the sense of the infinity
|
| 224 |
+
# norm, hence I call half the max range the plot radius.
|
| 225 |
+
plot_radius = 0.5 * max([x_range, y_range, z_range])
|
| 226 |
+
|
| 227 |
+
ax.set_xlim3d([x_middle - plot_radius, x_middle + plot_radius])
|
| 228 |
+
ax.set_ylim3d([y_middle - plot_radius, y_middle + plot_radius])
|
| 229 |
+
ax.set_zlim3d([z_middle - plot_radius, z_middle + plot_radius])
|
requirements.txt
ADDED
|
@@ -0,0 +1,6 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
astropy==5.1
|
| 2 |
+
Jinja2
|
| 3 |
+
matplotlib
|
| 4 |
+
pandas
|
| 5 |
+
numpy
|
| 6 |
+
shiny
|
simulation.py
ADDED
|
@@ -0,0 +1,203 @@
|
|
|
|
|
|
|
|
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|
|
|
|
|
|
|
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|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
from typing import Any
|
| 2 |
+
import numpy as np
|
| 3 |
+
import astropy.constants as c
|
| 4 |
+
import time
|
| 5 |
+
|
| 6 |
+
# Adapted from Python for Astronomers: An Introduction to Scientific Computing
|
| 7 |
+
# by Imad Pasha & Christopher Agostino
|
| 8 |
+
# https://prappleizer.github.io/Tutorials/RK4/RK4_Tutorial.html
|
| 9 |
+
|
| 10 |
+
# Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International License
|
| 11 |
+
# http://creativecommons.org/licenses/by-nc-sa/4.0/
|
| 12 |
+
|
| 13 |
+
|
| 14 |
+
class Body:
|
| 15 |
+
def __init__(self, mass, x_vec, v_vec, name=None, has_units=True):
|
| 16 |
+
"""
|
| 17 |
+
spawn instance of the Body class, which is used in Simulations.
|
| 18 |
+
|
| 19 |
+
:param: mass | mass of particle. if has_units=True, an Astropy Quantity, otherwise a float
|
| 20 |
+
:param: x_vec | a vector len(3) containing the x, y, z initial positions of the body.
|
| 21 |
+
the array can be unitless if has_units=False, or be of the form np.array([0,0,0])*u.km
|
| 22 |
+
:param: v_vec | vector len(3) containing the v_x, v_y, v_z initial velocities of the body.
|
| 23 |
+
:param: name | string containing a name, used for plotting later
|
| 24 |
+
:param: has_units | defines how the code treats the problem, as unit-ed, or unitless.
|
| 25 |
+
"""
|
| 26 |
+
self.name = name
|
| 27 |
+
self.has_units = has_units
|
| 28 |
+
if self.has_units:
|
| 29 |
+
self.mass = mass.cgs
|
| 30 |
+
self.x_vec = x_vec.cgs.value
|
| 31 |
+
self.v_vec = v_vec.cgs.value
|
| 32 |
+
else:
|
| 33 |
+
self.mass = mass
|
| 34 |
+
self.x_vec = x_vec
|
| 35 |
+
self.v_vec = v_vec
|
| 36 |
+
|
| 37 |
+
def return_vec(self):
|
| 38 |
+
"""
|
| 39 |
+
Concatenates the x and v vector into 1 vector 'y' used in RK formalism.
|
| 40 |
+
"""
|
| 41 |
+
return np.concatenate((self.x_vec, self.v_vec))
|
| 42 |
+
|
| 43 |
+
def return_mass(self):
|
| 44 |
+
"""
|
| 45 |
+
handler to strip the mass units if present (after converting to cgs) or return float
|
| 46 |
+
"""
|
| 47 |
+
if self.has_units:
|
| 48 |
+
return self.mass.cgs.value
|
| 49 |
+
else:
|
| 50 |
+
return self.mass
|
| 51 |
+
|
| 52 |
+
def return_name(self):
|
| 53 |
+
return self.name
|
| 54 |
+
|
| 55 |
+
|
| 56 |
+
class Simulation:
|
| 57 |
+
def __init__(self, bodies, has_units=True):
|
| 58 |
+
"""
|
| 59 |
+
Initializes instance of Simulation object.
|
| 60 |
+
-------------------------------------------
|
| 61 |
+
Params:
|
| 62 |
+
bodies (list): a list of Body() objects
|
| 63 |
+
has_units (bool): set whether bodies entered have units or not.
|
| 64 |
+
"""
|
| 65 |
+
self.has_units = has_units
|
| 66 |
+
self.bodies = bodies
|
| 67 |
+
self.N_bodies = len(self.bodies)
|
| 68 |
+
self.nDim = 6.0
|
| 69 |
+
self.quant_vec = np.concatenate(np.array([i.return_vec() for i in self.bodies]))
|
| 70 |
+
self.mass_vec = np.array([i.return_mass() for i in self.bodies])
|
| 71 |
+
self.name_vec = [i.return_name() for i in self.bodies]
|
| 72 |
+
|
| 73 |
+
def set_diff_eq(self, calc_diff_eqs, **kwargs):
|
| 74 |
+
"""
|
| 75 |
+
Method which assigns an external solver function as the diff-eq solver for RK4.
|
| 76 |
+
For N-body or gravitational setups, this is the function which calculates accelerations.
|
| 77 |
+
---------------------------------
|
| 78 |
+
Params:
|
| 79 |
+
calc_diff_eqs: A function which returns a [y] vector for RK4
|
| 80 |
+
**kwargs: Any additional inputs/hyperparameters the external function requires
|
| 81 |
+
"""
|
| 82 |
+
self.diff_eq_kwargs = kwargs
|
| 83 |
+
self.calc_diff_eqs = calc_diff_eqs
|
| 84 |
+
|
| 85 |
+
def rk4(self, t, dt):
|
| 86 |
+
"""
|
| 87 |
+
RK4 integrator. Calculates the K values and returns a new y vector
|
| 88 |
+
--------------------------------
|
| 89 |
+
Params:
|
| 90 |
+
t: a time. Only used if the diff eq depends on time (gravity doesn't).
|
| 91 |
+
dt: timestep. Non adaptive in this case
|
| 92 |
+
"""
|
| 93 |
+
k1 = dt * self.calc_diff_eqs(
|
| 94 |
+
t, self.quant_vec, self.mass_vec, **self.diff_eq_kwargs
|
| 95 |
+
)
|
| 96 |
+
k2 = dt * self.calc_diff_eqs(
|
| 97 |
+
t + 0.5 * dt,
|
| 98 |
+
self.quant_vec + 0.5 * k1,
|
| 99 |
+
self.mass_vec,
|
| 100 |
+
**self.diff_eq_kwargs,
|
| 101 |
+
)
|
| 102 |
+
k3 = dt * self.calc_diff_eqs(
|
| 103 |
+
t + 0.5 * dt,
|
| 104 |
+
self.quant_vec + 0.5 * k2,
|
| 105 |
+
self.mass_vec,
|
| 106 |
+
**self.diff_eq_kwargs,
|
| 107 |
+
)
|
| 108 |
+
k4 = dt * self.calc_diff_eqs(
|
| 109 |
+
t + dt, self.quant_vec + k2, self.mass_vec, **self.diff_eq_kwargs
|
| 110 |
+
)
|
| 111 |
+
|
| 112 |
+
y_new = self.quant_vec + ((k1 + 2 * k2 + 2 * k3 + k4) / 6.0)
|
| 113 |
+
|
| 114 |
+
return y_new
|
| 115 |
+
|
| 116 |
+
def run(self, T, dt, t0=0, progress=None):
|
| 117 |
+
"""
|
| 118 |
+
Method which runs the simulation on a given set of bodies.
|
| 119 |
+
---------------------
|
| 120 |
+
Params:
|
| 121 |
+
T: total time (in simulation units) to run the simulation. Can have units or not, just set has_units appropriately.
|
| 122 |
+
dt: timestep (in simulation units) to advance the simulation. Same as above
|
| 123 |
+
t0 (optional): set a non-zero start time to the simulation.
|
| 124 |
+
progress (optional): A shiny.ui.Progress object which will be used to send progress updates.
|
| 125 |
+
|
| 126 |
+
Returns:
|
| 127 |
+
None, but leaves an attribute history accessed via
|
| 128 |
+
'simulation.history' which contains all y vectors for the simulation.
|
| 129 |
+
These are of shape (Nstep,Nbodies * 6), so the x and y positions of particle 1 are
|
| 130 |
+
simulation.history[:,0], simulation.history[:,1], while the same for particle 2 are
|
| 131 |
+
simulation.history[:,6], simulation.history[:,7]. Velocities are also extractable.
|
| 132 |
+
"""
|
| 133 |
+
if not hasattr(self, "calc_diff_eqs"):
|
| 134 |
+
raise AttributeError("You must set a diff eq solver first.")
|
| 135 |
+
if self.has_units:
|
| 136 |
+
try:
|
| 137 |
+
_ = t0.unit
|
| 138 |
+
except:
|
| 139 |
+
t0 = (t0 * T.unit).cgs.value
|
| 140 |
+
T = T.cgs.value
|
| 141 |
+
dt = dt.cgs.value
|
| 142 |
+
|
| 143 |
+
self.history: Any = [self.quant_vec]
|
| 144 |
+
clock_time = t0
|
| 145 |
+
nsteps = int((T - t0) / dt)
|
| 146 |
+
start_time = time.time()
|
| 147 |
+
for step in range(nsteps):
|
| 148 |
+
if progress is not None and step % 5 == 0:
|
| 149 |
+
progress.set(
|
| 150 |
+
step,
|
| 151 |
+
message=f"Integrating step = {step} / {nsteps}",
|
| 152 |
+
detail=f"Elapsed time = {round(clock_time/1e6, 1)}",
|
| 153 |
+
)
|
| 154 |
+
y_new = self.rk4(0, dt)
|
| 155 |
+
self.history.append(y_new)
|
| 156 |
+
self.quant_vec = y_new
|
| 157 |
+
clock_time += dt
|
| 158 |
+
runtime = time.time() - start_time
|
| 159 |
+
self.history = np.array(self.history)
|
| 160 |
+
|
| 161 |
+
|
| 162 |
+
def nbody_solve(t, y, masses):
|
| 163 |
+
N_bodies = int(len(y) / 6)
|
| 164 |
+
solved_vector = np.zeros(y.size)
|
| 165 |
+
for i in range(N_bodies):
|
| 166 |
+
ioffset = i * 6
|
| 167 |
+
for j in range(N_bodies):
|
| 168 |
+
joffset = j * 6
|
| 169 |
+
solved_vector[ioffset] = y[ioffset + 3]
|
| 170 |
+
solved_vector[ioffset + 1] = y[ioffset + 4]
|
| 171 |
+
solved_vector[ioffset + 2] = y[ioffset + 5]
|
| 172 |
+
if i != j:
|
| 173 |
+
dx = y[ioffset] - y[joffset]
|
| 174 |
+
dy = y[ioffset + 1] - y[joffset + 1]
|
| 175 |
+
dz = y[ioffset + 2] - y[joffset + 2]
|
| 176 |
+
r = (dx**2 + dy**2 + dz**2) ** 0.5
|
| 177 |
+
ax = (-c.G.cgs * masses[j] / r**3) * dx
|
| 178 |
+
ay = (-c.G.cgs * masses[j] / r**3) * dy
|
| 179 |
+
az = (-c.G.cgs * masses[j] / r**3) * dz
|
| 180 |
+
ax = ax.value
|
| 181 |
+
ay = ay.value
|
| 182 |
+
az = az.value
|
| 183 |
+
solved_vector[ioffset + 3] += ax
|
| 184 |
+
solved_vector[ioffset + 4] += ay
|
| 185 |
+
solved_vector[ioffset + 5] += az
|
| 186 |
+
return solved_vector
|
| 187 |
+
|
| 188 |
+
|
| 189 |
+
def spherical_to_cartesian(
|
| 190 |
+
theta: float, phi: float, rho: float
|
| 191 |
+
) -> tuple[float, float, float]:
|
| 192 |
+
x = rho * sind(phi) * cosd(theta)
|
| 193 |
+
y = rho * sind(phi) * sind(theta)
|
| 194 |
+
z = rho * cosd(phi)
|
| 195 |
+
return (x, y, z)
|
| 196 |
+
|
| 197 |
+
|
| 198 |
+
def cosd(x):
|
| 199 |
+
return np.cos(x / 180 * np.pi)
|
| 200 |
+
|
| 201 |
+
|
| 202 |
+
def sind(x):
|
| 203 |
+
return np.sin(x / 180 * np.pi)
|
www/coords.png
ADDED
|