| """Tier-3 physical systems: held out of training to support a generalisation |
| claim ("converges on systems it never trained on").""" |
|
|
| from __future__ import annotations |
|
|
| import numpy as np |
|
|
| from physix.systems.base import PhysicalSystem, SystemTier |
|
|
|
|
| class ProjectileWithDrag(PhysicalSystem): |
| """2-D projectile with quadratic air drag. |
| |
| Equations of motion:: |
| |
| d2x/dt2 = -k * |v| * vx |
| d2y/dt2 = -g - k * |v| * vy |
| |
| where ``|v| = sqrt(vx**2 + vy**2)``. |
| """ |
|
|
| system_id: str = "projectile_drag" |
| tier: SystemTier = SystemTier.TIER_3 |
| state_variables: tuple[str, ...] = ("x", "y", "vx", "vy") |
| duration: float = 5.0 |
| hint_template: str = ( |
| "Projectile launched at angle {angle_deg:.0f} degrees with initial " |
| "speed {v0:.1f} m/s. Air drag is non-negligible." |
| ) |
|
|
| def sample_parameters(self, rng: np.random.Generator) -> dict[str, float]: |
| return { |
| "g": 9.81, |
| "k": float(rng.uniform(0.005, 0.02)), |
| } |
|
|
| def sample_initial_conditions(self, rng: np.random.Generator) -> dict[str, float]: |
| speed = float(rng.uniform(15.0, 30.0)) |
| angle = float(rng.uniform(np.deg2rad(30.0), np.deg2rad(70.0))) |
| return { |
| "x": 0.0, |
| "y": 0.0, |
| "vx": float(speed * np.cos(angle)), |
| "vy": float(speed * np.sin(angle)), |
| } |
|
|
| def rhs( |
| self, |
| t: float, |
| state: np.ndarray, |
| params: dict[str, float], |
| ) -> np.ndarray: |
| _x, _y, vx, vy = state |
| speed = float(np.sqrt(vx * vx + vy * vy)) |
| return np.array( |
| [ |
| vx, |
| vy, |
| -params["k"] * speed * vx, |
| -params["g"] - params["k"] * speed * vy, |
| ], |
| dtype=float, |
| ) |
|
|
| def ground_truth_equation(self) -> str: |
| |
| |
| return ( |
| "d2x/dt2 = -k*sqrt(vx**2 + vy**2)*vx; " |
| "d2y/dt2 = -g - k*sqrt(vx**2 + vy**2)*vy" |
| ) |
|
|
| def hint(self, parameters: dict[str, float]) -> str: |
| ic = self.initial_conditions |
| if not ic: |
| return self.hint_template |
| v0 = float(np.sqrt(ic["vx"] ** 2 + ic["vy"] ** 2)) |
| angle_deg = float(np.rad2deg(np.arctan2(ic["vy"], ic["vx"]))) |
| return self.hint_template.format(angle_deg=angle_deg, v0=v0) |
|
|
|
|
| class ChargedInBField(PhysicalSystem): |
| """Charged particle in a uniform magnetic field along z (circular motion). |
| |
| Equations of motion (assuming B = B_z * ẑ and v in xy-plane):: |
| |
| d2x/dt2 = (q*B/m) * vy |
| d2y/dt2 = -(q*B/m) * vx |
| """ |
|
|
| system_id: str = "charged_b_field" |
| tier: SystemTier = SystemTier.TIER_3 |
| state_variables: tuple[str, ...] = ("x", "y", "vx", "vy") |
| hint_template: str = ( |
| "Charged particle in a uniform magnetic field. Charge-to-mass ratio " |
| "q/m = {qm:.2f}, field strength {B:.2f} T." |
| ) |
|
|
| def sample_parameters(self, rng: np.random.Generator) -> dict[str, float]: |
| return { |
| "q": float(rng.choice([-1.0, 1.0])), |
| "m": float(rng.uniform(0.5, 2.0)), |
| "B": float(rng.uniform(0.5, 2.0)), |
| } |
|
|
| def sample_initial_conditions(self, rng: np.random.Generator) -> dict[str, float]: |
| return { |
| "x": 0.0, |
| "y": 0.0, |
| "vx": float(rng.uniform(0.5, 2.0)), |
| "vy": float(rng.uniform(-2.0, 2.0)), |
| } |
|
|
| def rhs( |
| self, |
| t: float, |
| state: np.ndarray, |
| params: dict[str, float], |
| ) -> np.ndarray: |
| _x, _y, vx, vy = state |
| omega = params["q"] * params["B"] / params["m"] |
| return np.array([vx, vy, omega * vy, -omega * vx], dtype=float) |
|
|
| def ground_truth_equation(self) -> str: |
| return ( |
| "d2x/dt2 = (q*B/m)*vy; " |
| "d2y/dt2 = -(q*B/m)*vx" |
| ) |
|
|
| def hint(self, parameters: dict[str, float]) -> str: |
| qm = parameters["q"] / parameters["m"] |
| return self.hint_template.format(qm=qm, B=parameters["B"]) |
|
|