Create app.py
Browse files
app.py
ADDED
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| 1 |
+
import os
|
| 2 |
+
import tempfile
|
| 3 |
+
from dataclasses import dataclass, field
|
| 4 |
+
|
| 5 |
+
import gradio as gr
|
| 6 |
+
import matplotlib.pyplot as plt
|
| 7 |
+
import numpy as np
|
| 8 |
+
from matplotlib.animation import FuncAnimation
|
| 9 |
+
|
| 10 |
+
|
| 11 |
+
# -----------------------------
|
| 12 |
+
# Core physics data structures
|
| 13 |
+
# -----------------------------
|
| 14 |
+
@dataclass
|
| 15 |
+
class Body:
|
| 16 |
+
name: str
|
| 17 |
+
mass: float
|
| 18 |
+
position: np.ndarray
|
| 19 |
+
velocity: np.ndarray
|
| 20 |
+
color: str = "white"
|
| 21 |
+
size: float = 8.0
|
| 22 |
+
acceleration: np.ndarray = field(default_factory=lambda: np.zeros(2, dtype=float))
|
| 23 |
+
trail: list = field(default_factory=list)
|
| 24 |
+
|
| 25 |
+
def __post_init__(self):
|
| 26 |
+
self.position = np.array(self.position, dtype=float)
|
| 27 |
+
self.velocity = np.array(self.velocity, dtype=float)
|
| 28 |
+
self.acceleration = np.array(self.acceleration, dtype=float)
|
| 29 |
+
|
| 30 |
+
def record_position(self):
|
| 31 |
+
self.trail.append(self.position.copy())
|
| 32 |
+
|
| 33 |
+
|
| 34 |
+
# -----------------------------
|
| 35 |
+
# Physics engine
|
| 36 |
+
# -----------------------------
|
| 37 |
+
def compute_accelerations(bodies, G=1.0, softening=1e-3):
|
| 38 |
+
n = len(bodies)
|
| 39 |
+
accelerations = [np.zeros(2, dtype=float) for _ in range(n)]
|
| 40 |
+
|
| 41 |
+
for i in range(n):
|
| 42 |
+
for j in range(n):
|
| 43 |
+
if i == j:
|
| 44 |
+
continue
|
| 45 |
+
|
| 46 |
+
displacement = bodies[j].position - bodies[i].position
|
| 47 |
+
distance_sq = np.dot(displacement, displacement) + softening**2
|
| 48 |
+
distance = np.sqrt(distance_sq)
|
| 49 |
+
|
| 50 |
+
accelerations[i] += G * bodies[j].mass * displacement / (distance_sq * distance)
|
| 51 |
+
|
| 52 |
+
return accelerations
|
| 53 |
+
|
| 54 |
+
|
| 55 |
+
def step_velocity_verlet(bodies, dt, G=1.0, softening=1e-3):
|
| 56 |
+
old_accelerations = compute_accelerations(bodies, G=G, softening=softening)
|
| 57 |
+
|
| 58 |
+
for body, acc in zip(bodies, old_accelerations):
|
| 59 |
+
body.acceleration = acc
|
| 60 |
+
body.position = body.position + body.velocity * dt + 0.5 * acc * dt**2
|
| 61 |
+
|
| 62 |
+
new_accelerations = compute_accelerations(bodies, G=G, softening=softening)
|
| 63 |
+
|
| 64 |
+
for body, old_acc, new_acc in zip(bodies, old_accelerations, new_accelerations):
|
| 65 |
+
body.velocity = body.velocity + 0.5 * (old_acc + new_acc) * dt
|
| 66 |
+
body.acceleration = new_acc
|
| 67 |
+
body.record_position()
|
| 68 |
+
|
| 69 |
+
|
| 70 |
+
class SimulationVV:
|
| 71 |
+
def __init__(self, bodies, dt=0.001, G=1.0, softening=1e-3):
|
| 72 |
+
self.bodies = bodies
|
| 73 |
+
self.dt = dt
|
| 74 |
+
self.G = G
|
| 75 |
+
self.softening = softening
|
| 76 |
+
self.time = 0.0
|
| 77 |
+
|
| 78 |
+
for body in self.bodies:
|
| 79 |
+
if len(body.trail) == 0:
|
| 80 |
+
body.record_position()
|
| 81 |
+
|
| 82 |
+
def step(self):
|
| 83 |
+
step_velocity_verlet(
|
| 84 |
+
self.bodies,
|
| 85 |
+
dt=self.dt,
|
| 86 |
+
G=self.G,
|
| 87 |
+
softening=self.softening,
|
| 88 |
+
)
|
| 89 |
+
self.time += self.dt
|
| 90 |
+
|
| 91 |
+
|
| 92 |
+
# -----------------------------
|
| 93 |
+
# Diagnostics
|
| 94 |
+
# -----------------------------
|
| 95 |
+
def compute_kinetic_energy(bodies):
|
| 96 |
+
total_ke = 0.0
|
| 97 |
+
for body in bodies:
|
| 98 |
+
total_ke += 0.5 * body.mass * np.dot(body.velocity, body.velocity)
|
| 99 |
+
return total_ke
|
| 100 |
+
|
| 101 |
+
|
| 102 |
+
def compute_potential_energy(bodies, G=1.0, softening=1e-3):
|
| 103 |
+
total_pe = 0.0
|
| 104 |
+
n = len(bodies)
|
| 105 |
+
|
| 106 |
+
for i in range(n):
|
| 107 |
+
for j in range(i + 1, n):
|
| 108 |
+
displacement = bodies[j].position - bodies[i].position
|
| 109 |
+
distance = np.sqrt(np.dot(displacement, displacement) + softening**2)
|
| 110 |
+
total_pe += -G * bodies[i].mass * bodies[j].mass / distance
|
| 111 |
+
|
| 112 |
+
return total_pe
|
| 113 |
+
|
| 114 |
+
|
| 115 |
+
# -----------------------------
|
| 116 |
+
# Presets
|
| 117 |
+
# -----------------------------
|
| 118 |
+
def make_two_body_system(G=1.0):
|
| 119 |
+
M = 1000.0
|
| 120 |
+
r = 1.0
|
| 121 |
+
v = np.sqrt(G * M / r)
|
| 122 |
+
|
| 123 |
+
sun = Body(
|
| 124 |
+
name="Sun",
|
| 125 |
+
mass=M,
|
| 126 |
+
position=[0.0, 0.0],
|
| 127 |
+
velocity=[0.0, 0.0],
|
| 128 |
+
color="gold",
|
| 129 |
+
size=18,
|
| 130 |
+
)
|
| 131 |
+
|
| 132 |
+
earth = Body(
|
| 133 |
+
name="Earth",
|
| 134 |
+
mass=1.0,
|
| 135 |
+
position=[r, 0.0],
|
| 136 |
+
velocity=[0.0, v],
|
| 137 |
+
color="deepskyblue",
|
| 138 |
+
size=8,
|
| 139 |
+
)
|
| 140 |
+
|
| 141 |
+
return [sun, earth]
|
| 142 |
+
|
| 143 |
+
|
| 144 |
+
def make_three_body_system():
|
| 145 |
+
body1 = Body(
|
| 146 |
+
name="Body 1",
|
| 147 |
+
mass=500.0,
|
| 148 |
+
position=[-0.8, 0.0],
|
| 149 |
+
velocity=[0.0, -10.0],
|
| 150 |
+
color="orange",
|
| 151 |
+
size=14,
|
| 152 |
+
)
|
| 153 |
+
|
| 154 |
+
body2 = Body(
|
| 155 |
+
name="Body 2",
|
| 156 |
+
mass=500.0,
|
| 157 |
+
position=[0.8, 0.0],
|
| 158 |
+
velocity=[0.0, 10.0],
|
| 159 |
+
color="cyan",
|
| 160 |
+
size=14,
|
| 161 |
+
)
|
| 162 |
+
|
| 163 |
+
body3 = Body(
|
| 164 |
+
name="Body 3",
|
| 165 |
+
mass=5.0,
|
| 166 |
+
position=[0.0, 1.2],
|
| 167 |
+
velocity=[18.0, 0.0],
|
| 168 |
+
color="magenta",
|
| 169 |
+
size=8,
|
| 170 |
+
)
|
| 171 |
+
|
| 172 |
+
return [body1, body2, body3]
|
| 173 |
+
|
| 174 |
+
|
| 175 |
+
def make_custom_two_body(central_mass, orbit_radius, planet_mass, planet_speed, tangential_direction):
|
| 176 |
+
sun = Body(
|
| 177 |
+
name="Central Body",
|
| 178 |
+
mass=central_mass,
|
| 179 |
+
position=[0.0, 0.0],
|
| 180 |
+
velocity=[0.0, 0.0],
|
| 181 |
+
color="gold",
|
| 182 |
+
size=18,
|
| 183 |
+
)
|
| 184 |
+
|
| 185 |
+
vy = planet_speed if tangential_direction == "Counterclockwise" else -planet_speed
|
| 186 |
+
|
| 187 |
+
planet = Body(
|
| 188 |
+
name="Planet",
|
| 189 |
+
mass=planet_mass,
|
| 190 |
+
position=[orbit_radius, 0.0],
|
| 191 |
+
velocity=[0.0, vy],
|
| 192 |
+
color="deepskyblue",
|
| 193 |
+
size=8,
|
| 194 |
+
)
|
| 195 |
+
|
| 196 |
+
return [sun, planet]
|
| 197 |
+
|
| 198 |
+
|
| 199 |
+
# -----------------------------
|
| 200 |
+
# Rendering
|
| 201 |
+
# -----------------------------
|
| 202 |
+
def simulate_system(
|
| 203 |
+
preset,
|
| 204 |
+
dt,
|
| 205 |
+
frames,
|
| 206 |
+
steps_per_frame,
|
| 207 |
+
G,
|
| 208 |
+
softening,
|
| 209 |
+
trail_length,
|
| 210 |
+
central_mass,
|
| 211 |
+
orbit_radius,
|
| 212 |
+
planet_mass,
|
| 213 |
+
planet_speed,
|
| 214 |
+
tangential_direction,
|
| 215 |
+
):
|
| 216 |
+
if preset == "Two-Body Circular Orbit":
|
| 217 |
+
bodies = make_two_body_system(G=G)
|
| 218 |
+
elif preset == "Three-Body Chaotic System":
|
| 219 |
+
bodies = make_three_body_system()
|
| 220 |
+
else:
|
| 221 |
+
bodies = make_custom_two_body(
|
| 222 |
+
central_mass=central_mass,
|
| 223 |
+
orbit_radius=orbit_radius,
|
| 224 |
+
planet_mass=planet_mass,
|
| 225 |
+
planet_speed=planet_speed,
|
| 226 |
+
tangential_direction=tangential_direction,
|
| 227 |
+
)
|
| 228 |
+
|
| 229 |
+
sim = SimulationVV(bodies, dt=dt, G=G, softening=softening)
|
| 230 |
+
|
| 231 |
+
kinetic_history = []
|
| 232 |
+
potential_history = []
|
| 233 |
+
total_history = []
|
| 234 |
+
|
| 235 |
+
fig, (ax_orbit, ax_energy) = plt.subplots(1, 2, figsize=(14, 6))
|
| 236 |
+
fig.patch.set_facecolor("#0f1117")
|
| 237 |
+
ax_orbit.set_facecolor("black")
|
| 238 |
+
ax_energy.set_facecolor("white")
|
| 239 |
+
|
| 240 |
+
max_range = max(2.5, orbit_radius * 1.8)
|
| 241 |
+
ax_orbit.set_xlim(-max_range, max_range)
|
| 242 |
+
ax_orbit.set_ylim(-max_range, max_range)
|
| 243 |
+
ax_orbit.set_aspect("equal")
|
| 244 |
+
ax_orbit.set_title("Orbital Dynamics", color="white", fontsize=14)
|
| 245 |
+
ax_orbit.tick_params(colors="white")
|
| 246 |
+
for spine in ax_orbit.spines.values():
|
| 247 |
+
spine.set_color("white")
|
| 248 |
+
ax_orbit.grid(alpha=0.15, color="white")
|
| 249 |
+
|
| 250 |
+
ax_energy.set_title("Energy Diagnostics", fontsize=14)
|
| 251 |
+
ax_energy.set_xlabel("Frame")
|
| 252 |
+
ax_energy.set_ylabel("Energy")
|
| 253 |
+
ax_energy.grid(alpha=0.3)
|
| 254 |
+
|
| 255 |
+
scatters = []
|
| 256 |
+
trail_lines = []
|
| 257 |
+
|
| 258 |
+
for body in sim.bodies:
|
| 259 |
+
scatter = ax_orbit.scatter([], [], color=body.color, s=body.size * 18, edgecolors="white", linewidths=0.5)
|
| 260 |
+
line, = ax_orbit.plot([], [], color=body.color, alpha=0.7, linewidth=1.5)
|
| 261 |
+
scatters.append(scatter)
|
| 262 |
+
trail_lines.append(line)
|
| 263 |
+
|
| 264 |
+
ke_line, = ax_energy.plot([], [], label="Kinetic Energy", linewidth=2)
|
| 265 |
+
pe_line, = ax_energy.plot([], [], label="Potential Energy", linewidth=2)
|
| 266 |
+
te_line, = ax_energy.plot([], [], label="Total Energy", linewidth=2)
|
| 267 |
+
ax_energy.legend()
|
| 268 |
+
|
| 269 |
+
def init():
|
| 270 |
+
for scatter, line in zip(scatters, trail_lines):
|
| 271 |
+
scatter.set_offsets(np.array([[np.nan, np.nan]]))
|
| 272 |
+
line.set_data([], [])
|
| 273 |
+
ke_line.set_data([], [])
|
| 274 |
+
pe_line.set_data([], [])
|
| 275 |
+
te_line.set_data([], [])
|
| 276 |
+
return scatters + trail_lines + [ke_line, pe_line, te_line]
|
| 277 |
+
|
| 278 |
+
def update(_frame):
|
| 279 |
+
for _ in range(steps_per_frame):
|
| 280 |
+
sim.step()
|
| 281 |
+
|
| 282 |
+
ke = compute_kinetic_energy(sim.bodies)
|
| 283 |
+
pe = compute_potential_energy(sim.bodies, G=G, softening=softening)
|
| 284 |
+
kinetic_history.append(ke)
|
| 285 |
+
potential_history.append(pe)
|
| 286 |
+
total_history.append(ke + pe)
|
| 287 |
+
|
| 288 |
+
for i, body in enumerate(sim.bodies):
|
| 289 |
+
scatters[i].set_offsets(body.position.reshape(1, 2))
|
| 290 |
+
trail = np.array(body.trail[-trail_length:])
|
| 291 |
+
if len(trail) > 1:
|
| 292 |
+
trail_lines[i].set_data(trail[:, 0], trail[:, 1])
|
| 293 |
+
|
| 294 |
+
x = np.arange(len(total_history))
|
| 295 |
+
ke_line.set_data(x, kinetic_history)
|
| 296 |
+
pe_line.set_data(x, potential_history)
|
| 297 |
+
te_line.set_data(x, total_history)
|
| 298 |
+
|
| 299 |
+
ax_energy.relim()
|
| 300 |
+
ax_energy.autoscale_view()
|
| 301 |
+
|
| 302 |
+
return scatters + trail_lines + [ke_line, pe_line, te_line]
|
| 303 |
+
|
| 304 |
+
anim = FuncAnimation(
|
| 305 |
+
fig,
|
| 306 |
+
update,
|
| 307 |
+
frames=frames,
|
| 308 |
+
init_func=init,
|
| 309 |
+
interval=40,
|
| 310 |
+
blit=False,
|
| 311 |
+
)
|
| 312 |
+
|
| 313 |
+
temp_dir = tempfile.mkdtemp()
|
| 314 |
+
output_path = os.path.join(temp_dir, "nbody_simulation.gif")
|
| 315 |
+
anim.save(output_path, writer="pillow", fps=20)
|
| 316 |
+
plt.close(fig)
|
| 317 |
+
|
| 318 |
+
return output_path
|
| 319 |
+
|
| 320 |
+
|
| 321 |
+
# -----------------------------
|
| 322 |
+
# Gradio UI
|
| 323 |
+
# -----------------------------
|
| 324 |
+
DESCRIPTION = """
|
| 325 |
+
## N-Body Orbital Physics Lab
|
| 326 |
+
|
| 327 |
+
Explore Newtonian gravity with an interactive **Velocity Verlet** simulation.
|
| 328 |
+
|
| 329 |
+
### Included
|
| 330 |
+
- Two-body circular orbit
|
| 331 |
+
- Three-body chaotic dynamics
|
| 332 |
+
- Custom two-body experiment mode
|
| 333 |
+
- Energy diagnostics
|
| 334 |
+
- Adjustable timestep, softening, and trail length
|
| 335 |
+
"""
|
| 336 |
+
|
| 337 |
+
with gr.Blocks(title="N-Body Orbital Physics Lab", theme=gr.themes.Soft()) as demo:
|
| 338 |
+
gr.Markdown("# 🪐 N-Body Orbital Physics Lab")
|
| 339 |
+
gr.Markdown(DESCRIPTION)
|
| 340 |
+
|
| 341 |
+
with gr.Row():
|
| 342 |
+
with gr.Column():
|
| 343 |
+
preset = gr.Dropdown(
|
| 344 |
+
choices=[
|
| 345 |
+
"Two-Body Circular Orbit",
|
| 346 |
+
"Three-Body Chaotic System",
|
| 347 |
+
"Custom Two-Body Experiment",
|
| 348 |
+
],
|
| 349 |
+
value="Two-Body Circular Orbit",
|
| 350 |
+
label="Preset",
|
| 351 |
+
)
|
| 352 |
+
|
| 353 |
+
dt = gr.Slider(0.0001, 0.005, value=0.0005, step=0.0001, label="Time Step (dt)")
|
| 354 |
+
frames = gr.Slider(100, 400, value=250, step=50, label="Rendered Frames")
|
| 355 |
+
steps_per_frame = gr.Slider(1, 8, value=4, step=1, label="Physics Steps per Frame")
|
| 356 |
+
G = gr.Slider(0.1, 5.0, value=1.0, step=0.1, label="Gravitational Constant (G)")
|
| 357 |
+
softening = gr.Slider(0.0001, 0.05, value=0.001, step=0.0001, label="Softening")
|
| 358 |
+
trail_length = gr.Slider(20, 300, value=100, step=10, label="Trail Length")
|
| 359 |
+
|
| 360 |
+
gr.Markdown("### Custom Two-Body Controls")
|
| 361 |
+
central_mass = gr.Slider(100, 5000, value=1000, step=50, label="Central Mass")
|
| 362 |
+
orbit_radius = gr.Slider(0.5, 3.0, value=1.0, step=0.1, label="Orbit Radius")
|
| 363 |
+
planet_mass = gr.Slider(0.1, 20.0, value=1.0, step=0.1, label="Planet Mass")
|
| 364 |
+
planet_speed = gr.Slider(1.0, 80.0, value=31.6, step=0.1, label="Planet Tangential Speed")
|
| 365 |
+
tangential_direction = gr.Radio(
|
| 366 |
+
choices=["Counterclockwise", "Clockwise"],
|
| 367 |
+
value="Counterclockwise",
|
| 368 |
+
label="Orbit Direction",
|
| 369 |
+
)
|
| 370 |
+
|
| 371 |
+
run_button = gr.Button("Run Simulation", variant="primary")
|
| 372 |
+
|
| 373 |
+
with gr.Column():
|
| 374 |
+
output_gif = gr.Image(label="Simulation Output", type="filepath")
|
| 375 |
+
|
| 376 |
+
run_button.click(
|
| 377 |
+
fn=simulate_system,
|
| 378 |
+
inputs=[
|
| 379 |
+
preset,
|
| 380 |
+
dt,
|
| 381 |
+
frames,
|
| 382 |
+
steps_per_frame,
|
| 383 |
+
G,
|
| 384 |
+
softening,
|
| 385 |
+
trail_length,
|
| 386 |
+
central_mass,
|
| 387 |
+
orbit_radius,
|
| 388 |
+
planet_mass,
|
| 389 |
+
planet_speed,
|
| 390 |
+
tangential_direction,
|
| 391 |
+
],
|
| 392 |
+
outputs=output_gif,
|
| 393 |
+
)
|
| 394 |
+
|
| 395 |
+
if __name__ == "__main__":
|
| 396 |
+
demo.launch()
|