"""Benchmark plants xdot = f(x, u), y = h(x). Every plant is torch-batched: ``f(x, u)`` takes ``x`` of shape (B, nx) and ``u`` of shape (B, nu) and returns (B, nx); ``h(x)`` returns the measured coordinates ``x[:, sensors]``. There is no scalar/numpy path. Physical parameters are plain attributes listed in ``PARAMS``, so a mismatched plant is ``plant.perturbed(rel)`` and nothing else changes. The input enters each plant in a different way (more than additive forcing): additive (vdp, fhn, rossler, lorenz), state-dependent gain (duffing), bilinear (bioreactor), matrix-valued G(x) (two_link_arm, cartpole), distributed (quad_tank, highway_traffic). ``SaturatingActuator`` additionally makes any plant non-affine in u. """ from __future__ import annotations import math import torch REGISTRY: dict = {} def register(name): def deco(cls): REGISTRY[name] = cls cls.name = name return cls return deco def _pos(v, eps: float = 1e-6): """Smooth positive part, C-infinity, equal to v for v >> sqrt(eps).""" return 0.5 * (v + torch.sqrt(v * v + eps)) class Plant: nx: int = 0 nu: int = 1 PARAMS: dict = {} # name -> nominal value (scalars only) NOT_PERTURBED: tuple = () # parameters that are operating conditions, not plant physics DEFAULT_SENSORS: tuple = (0,) name = "plant" def __init__(self, sensors=None, **params): unknown = set(params) - set(self.PARAMS) if unknown: raise ValueError(f"{self.name}: unknown parameters {sorted(unknown)}") for k, v in self.PARAMS.items(): setattr(self, k, float(params.get(k, v))) self.sensors = tuple(self.DEFAULT_SENSORS if sensors is None else sensors) self.ny = len(self.sensors) # -- interface ------------------------------------------------------------- def f(self, x: torch.Tensor, u: torch.Tensor) -> torch.Tensor: raise NotImplementedError def h(self, x: torch.Tensor) -> torch.Tensor: return x[:, list(self.sensors)] # Incomplete knowledge: the part of f a modeller would plausibly have, with one # physically identified term missing or simplified (UNMODELLED says which). Every # model-based component (filters, model-based KKL, the phase-1 PDE term) gets this # model when system.knowledge = partial; the real plant keeps f. UNMODELLED: str = "" def f_known(self, x: torch.Tensor, u: torch.Tensor) -> torch.Tensor: raise NotImplementedError(f"{self.name}: no partial-knowledge model defined") # -- helpers --------------------------------------------------------------- def params(self) -> dict: return {k: getattr(self, k) for k in self.PARAMS} def perturbed(self, rel: float) -> "Plant": """The same plant with every physical parameter off nominal by exp(+-rel). Signs alternate over the sorted parameter names, so the perturbation is deterministic and never a pure rescaling of time. """ p, sign = {}, 1.0 for k in sorted(self.PARAMS): if k in self.NOT_PERTURBED: p[k] = getattr(self, k) continue p[k] = getattr(self, k) * math.exp(sign * rel) sign = -sign return type(self)(sensors=self.sensors, **p) def input_gain(self, x: torch.Tensor) -> torch.Tensor: """G(x) = f(x, 1) - f(x, 0), shape (B, nx). Exact for input-affine plants.""" one = torch.ones(x.shape[0], self.nu, dtype=x.dtype, device=x.device) return self.f(x, one) - self.f(x, 0 * one) # --------------------------------------------------------------------------- # 2-D plants # --------------------------------------------------------------------------- @register("vdp") class VanDerPol(Plant): """x1' = x2, x2' = mu (1 - x1^2) x2 - x1 + u, y = x1.""" nx = 2 PARAMS = {"mu": 1.0} def f(self, x, u): x1, x2 = x[:, 0], x[:, 1] return torch.stack([x2, self.mu * (1 - x1 ** 2) * x2 - x1 + u[:, 0]], 1) UNMODELLED = "the nonlinear damping law mu (1 - x1^2) x2 (model: undamped oscillator)" def f_known(self, x, u): return torch.stack([x[:, 1], -x[:, 0] + u[:, 0]], 1) @register("duffing") class Duffing(Plant): """Reversed Duffing with state-dependent input gain. x1' = x2, x2' = -x1 - x1^3 + (1 + kappa x1^2) u, y = x1. """ nx = 2 PARAMS = {"kappa": 0.5} def f(self, x, u): x1, x2 = x[:, 0], x[:, 1] return torch.stack([x2, -x1 - x1 ** 3 + (1 + self.kappa * x1 ** 2) * u[:, 0]], 1) UNMODELLED = "the cubic stiffness -x1^3 (model: linear spring)" def f_known(self, x, u): x1, x2 = x[:, 0], x[:, 1] return torch.stack([x2, -x1 + (1 + self.kappa * x1 ** 2) * u[:, 0]], 1) @register("fhn") class FitzHughNagumo(Plant): """v' = v - v^3/3 - w + I + u, w' = eps (v + a - b w), y = v.""" nx = 2 PARAMS = {"a": 0.7, "b": 0.8, "eps": 0.08, "I_ext": 0.5} def f(self, x, u): v, w = x[:, 0], x[:, 1] return torch.stack([v - v ** 3 / 3 - w + self.I_ext + u[:, 0], self.eps * (v + self.a - self.b * w)], 1) UNMODELLED = "the recovery leak -eps b w" def f_known(self, x, u): v, w = x[:, 0], x[:, 1] return torch.stack([v - v ** 3 / 3 - w + self.I_ext + u[:, 0], self.eps * (v + self.a)], 1) @register("bioreactor") class Bioreactor(Plant): """Continuous stirred bioreactor, bilinear in (state, input). x1' = (mu(x2) - D) x1, x2' = -mu(x2) x1 / Y + D (x2f - x2), D = D_nom + u, mu(s) = mu_max s / (Ks + s) on the smooth positive part of s, y = x2 (substrate). Measuring substrate rather than biomass is both the standard instrument and the observable choice (empirical observability index 0.70 against 0.056). """ nx = 2 PARAMS = {"mu_max": 1.0, "Ks": 1.0, "Y": 0.4, "x2f": 4.0, "D_nom": 0.3} # feed concentration and dilution set point are the operating point, not the # biology: perturbing them by e^0.5 moved the biomass equilibrium from 1.4 to 3.4, # outside the envelope (every mismatch-50 episode was rejected) NOT_PERTURBED = ("x2f", "D_nom") DEFAULT_SENSORS = (1,) def f(self, x, u): x1, x2 = x[:, 0], x[:, 1] D = self.D_nom + u[:, 0] sp = _pos(x2) mu = self.mu_max * sp / (self.Ks + sp) return torch.stack([(mu - D) * x1, -mu * x1 / self.Y + D * (self.x2f - x2)], 1) UNMODELLED = "Monod saturation of the growth rate (model: first-order kinetics mu_max s / Ks)" def f_known(self, x, u): x1, x2 = x[:, 0], x[:, 1] D = self.D_nom + u[:, 0] mu = self.mu_max * _pos(x2) / self.Ks return torch.stack([(mu - D) * x1, -mu * x1 / self.Y + D * (self.x2f - x2)], 1) # --------------------------------------------------------------------------- # 3-D chaotic plants # --------------------------------------------------------------------------- @register("rossler") class Rossler(Plant): """x1' = -(x2 + x3), x2' = x1 + a x2 + u, x3' = b + x3 (x1 - c), y = x2.""" nx = 3 PARAMS = {"a": 0.1, "b": 0.1, "c": 14.0} DEFAULT_SENSORS = (1,) def f(self, x, u): x1, x2, x3 = x[:, 0], x[:, 1], x[:, 2] return torch.stack([-(x2 + x3), x1 + self.a * x2 + u[:, 0], self.b + x3 * (x1 - self.c)], 1) UNMODELLED = "the folding nonlinearity x1 x3" def f_known(self, x, u): x1, x2, x3 = x[:, 0], x[:, 1], x[:, 2] return torch.stack([-(x2 + x3), x1 + self.a * x2 + u[:, 0], self.b - self.c * x3], 1) @register("lorenz") class Lorenz(Plant): """sigma (x2 - x1), x1 (rho - x3) - x2 + u, x1 x2 - beta x3, y = x2.""" nx = 3 PARAMS = {"sigma": 10.0, "rho": 28.0, "beta": 8.0 / 3.0} DEFAULT_SENSORS = (1,) def f(self, x, u): x1, x2, x3 = x[:, 0], x[:, 1], x[:, 2] return torch.stack([self.sigma * (x2 - x1), x1 * (self.rho - x3) - x2 + u[:, 0], x1 * x2 - self.beta * x3], 1) UNMODELLED = "the coupling -x1 x3 in the measured equation" def f_known(self, x, u): x1, x2, x3 = x[:, 0], x[:, 1], x[:, 2] return torch.stack([self.sigma * (x2 - x1), self.rho * x1 - x2 + u[:, 0], x1 * x2 - self.beta * x3], 1) # --------------------------------------------------------------------------- # 4-D and 5-D plants # --------------------------------------------------------------------------- @register("quad_tank") class QuadrupleTank(Plant): """Quadruple-tank process (Johansson, IEEE TCST 2000), non-minimum-phase setting. The two lower levels are measured, the upper two are not. One scalar command drives both pumps differentially, v1 = v1n + u, v2 = v2n - u/2. sqrt is taken on a smooth positive part so Jacobians stay finite as h -> 0. """ nx = 4 PARAMS = {"A1": 28.0, "A2": 32.0, "A3": 28.0, "A4": 32.0, "a1": 0.071, "a2": 0.057, "a3": 0.071, "a4": 0.057, "gam1": 0.43, "gam2": 0.34, "k1": 3.33, "k2": 3.35, "v1n": 3.0, "v2n": 3.0, "g": 981.0} # g is a constant of nature and v1n, v2n are the operating point (nominal pump # voltages): perturbing them moved tank 2's equilibrium from 10.9 to 29.3 cm at # rel = 0.3, outside the envelope, so every mismatch episode was rejected NOT_PERTURBED = ("g", "v1n", "v2n") DEFAULT_SENSORS = (0, 1) def f(self, x, u): uu = u[:, 0] v1, v2 = self.v1n + uu, self.v2n - 0.5 * uu c = math.sqrt(2.0 * self.g) s = [torch.sqrt(_pos(x[:, i]) + 1e-6) for i in range(4)] d1 = (-self.a1 * c * s[0] + self.a3 * c * s[2] + self.gam1 * self.k1 * v1) / self.A1 d2 = (-self.a2 * c * s[1] + self.a4 * c * s[3] + self.gam2 * self.k2 * v2) / self.A2 d3 = (-self.a3 * c * s[2] + (1 - self.gam2) * self.k2 * v2) / self.A3 d4 = (-self.a4 * c * s[3] + (1 - self.gam1) * self.k1 * v1) / self.A4 return torch.stack([d1, d2, d3, d4], 1) UNMODELLED = "the square-root orifice law (model: flows linearised at the nominal equilibrium)" H_OP = (11.66, 10.9, 5.36, 3.3) # nominal zero-input equilibrium (cm) def f_known(self, x, u): uu = u[:, 0] v1, v2 = self.v1n + uu, self.v2n - 0.5 * uu c = math.sqrt(2.0 * self.g) s = [math.sqrt(h0) + (x[:, i] - h0) / (2 * math.sqrt(h0)) for i, h0 in enumerate(self.H_OP)] d1 = (-self.a1 * c * s[0] + self.a3 * c * s[2] + self.gam1 * self.k1 * v1) / self.A1 d2 = (-self.a2 * c * s[1] + self.a4 * c * s[3] + self.gam2 * self.k2 * v2) / self.A2 d3 = (-self.a3 * c * s[2] + (1 - self.gam2) * self.k2 * v2) / self.A3 d4 = (-self.a4 * c * s[3] + (1 - self.gam1) * self.k1 * v1) / self.A4 return torch.stack([d1, d2, d3, d4], 1) @register("cartpole") class CartPole(Plant): """Cart-pole about the upright equilibrium, pole-balancing loop closed. States (x, v, th, om); cart position and pole angle are measured. Only the pole states are fed back (gain K_bal in input units): a full LQR drives every initial condition to the same origin and makes the plant unobservable as a benchmark. u is an exogenous command on top of the balancing loop. th is smoothly limited. """ nx = 4 PARAMS = {"mc": 1.0, "mp": 0.1, "l": 0.5, "g": 9.81, "kd_v": 0.05, "kd_w": 0.02, "f_scale": 5.0} DEFAULT_SENSORS = (0, 2) TH_MAX = 0.6 K_BAL = (0.0, 0.0, -9.889688, -2.181384) def f(self, x, u): v, th, om = x[:, 1], x[:, 2], x[:, 3] th_s = self.TH_MAX * torch.tanh(th / self.TH_MAX) s, c = torch.sin(th_s), torch.cos(th_s) k1, k2, k3, k4 = self.K_BAL F = self.f_scale * (u[:, 0] - (k1 * x[:, 0] + k2 * v + k3 * th_s + k4 * om)) den = self.mc + self.mp * s * s av = (F + self.mp * s * (self.l * om * om - self.g * c)) / den - self.kd_v * v aw = (((self.mc + self.mp) * self.g * s - c * (F + self.mp * self.l * om * om * s)) / (self.l * den)) - self.kd_w * om return torch.stack([v, av, om, aw], 1) UNMODELLED = "large-angle pendulum terms (model: small-angle sin th = th, cos th = 1, no om^2)" def f_known(self, x, u): v, th, om = x[:, 1], x[:, 2], x[:, 3] th_s = self.TH_MAX * torch.tanh(th / self.TH_MAX) k1, k2, k3, k4 = self.K_BAL F = self.f_scale * (u[:, 0] - (k1 * x[:, 0] + k2 * v + k3 * th_s + k4 * om)) av = (F - self.mp * self.g * th_s) / self.mc - self.kd_v * v aw = ((self.mc + self.mp) * self.g * th_s - F) / (self.l * self.mc) - self.kd_w * om return torch.stack([v, av, om, aw], 1) @register("two_link_arm") class TwoLinkArm(Plant): """Lightly damped planar two-link arm with gravity, torque on joint 1. x = (q1, q2, dq1, dq2), both joint angles measured, G(x) = M(q)^{-1} e1. Damping is light (kd = 0.05): heavy damping collapses every trajectory onto the hanging equilibrium and destroys reconstructibility. """ nx = 4 PARAMS = {"m1": 1.0, "m2": 1.0, "l1": 1.0, "lc1": 0.5, "lc2": 0.5, "I1": 0.083, "I2": 0.083, "g": 9.81, "kd": 0.05} DEFAULT_SENSORS = (0, 1) def f(self, x, u): q1, q2, dq1, dq2 = x[:, 0], x[:, 1], x[:, 2], x[:, 3] a = self.m1 * self.lc1 ** 2 + self.I1 + self.m2 * (self.l1 ** 2 + self.lc2 ** 2) + self.I2 b = self.m2 * self.l1 * self.lc2 d = self.m2 * self.lc2 ** 2 + self.I2 g1 = (self.m1 * self.lc1 + self.m2 * self.l1) * self.g g2 = self.m2 * self.lc2 * self.g c2, s2 = torch.cos(q2), torch.sin(q2) m11, m12, m22 = a + 2 * b * c2, d + b * c2, d + 0 * c2 det = m11 * m22 - m12 ** 2 hh = b * s2 r1 = u[:, 0] + hh * dq2 * (2 * dq1 + dq2) - g1 * torch.cos(q1) \ - g2 * torch.cos(q1 + q2) - self.kd * dq1 r2 = -hh * dq1 ** 2 - g2 * torch.cos(q1 + q2) - self.kd * dq2 return torch.stack([dq1, dq2, (m22 * r1 - m12 * r2) / det, (-m12 * r1 + m11 * r2) / det], 1) UNMODELLED = "Coriolis and centrifugal terms (model: M(q) qdd = tau - g(q) - kd qd)" def f_known(self, x, u): q1, q2, dq1, dq2 = x[:, 0], x[:, 1], x[:, 2], x[:, 3] a = self.m1 * self.lc1 ** 2 + self.I1 + self.m2 * (self.l1 ** 2 + self.lc2 ** 2) + self.I2 b = self.m2 * self.l1 * self.lc2 d = self.m2 * self.lc2 ** 2 + self.I2 g1 = (self.m1 * self.lc1 + self.m2 * self.l1) * self.g g2 = self.m2 * self.lc2 * self.g c2 = torch.cos(q2) m11, m12, m22 = a + 2 * b * c2, d + b * c2, d + 0 * c2 det = m11 * m22 - m12 ** 2 r1 = u[:, 0] - g1 * torch.cos(q1) - g2 * torch.cos(q1 + q2) - self.kd * dq1 r2 = -g2 * torch.cos(q1 + q2) - self.kd * dq2 return torch.stack([dq1, dq2, (m22 * r1 - m12 * r2) / det, (-m12 * r1 + m11 * r2) / det], 1) @register("highway_traffic") class HighwayTraffic(Plant): """Five-cell Greenshields freeway, ramp inflow on cell 3 is the input. Three loop detectors (cells 1, 3, 5); with the downstream detector alone the chain is a five-fold differentiator and effectively unobservable. """ nx = 5 PARAMS = {"v_free": 30.0, "rho_max": 0.25, "L": 500.0, "u_main_base": 1.2, "u_ramp_base": 0.3} # demand is an operating condition: scaling it by e^{0.3} pushed the road past capacity # into congestion, where the Greenshields model used here is not valid NOT_PERTURBED = ("u_main_base", "u_ramp_base") DEFAULT_SENSORS = (0, 2, 4) def f(self, x, u): q = self.v_free * (x - x ** 2 / self.rho_max) # cell outflows inflow = torch.cat([torch.full_like(x[:, :1], self.u_main_base), q[:, :-1]], 1) z = torch.zeros_like(x[:, :1]) ramp = torch.cat([z, z, self.u_ramp_base + u[:, :1], z, z], 1) # no in-place: vmap-safe return (inflow - q + ramp) / self.L UNMODELLED = "congestion in the fundamental diagram (model: free-flow q = v_free rho)" def f_known(self, x, u): q = self.v_free * x inflow = torch.cat([torch.full_like(x[:, :1], self.u_main_base), q[:, :-1]], 1) z = torch.zeros_like(x[:, :1]) ramp = torch.cat([z, z, self.u_ramp_base + u[:, :1], z, z], 1) return (inflow - q + ramp) / self.L # --------------------------------------------------------------------------- # Non-affine actuator # --------------------------------------------------------------------------- class SaturatingActuator(Plant): r"""Make an input-affine plant non-affine in u (DC-motor form). u_eff = u_bar tanh((u - k (x_j - x_ref)) / u_bar), f(x, u) = f0(x) + G(x) u_eff The actuator saturates and is opposed by a back-EMF term on the state it drives, so u and x are inseparable. The back-EMF acts on the deviation from the operating point x_ref (the IC-box centre, near but not at the equilibrium for bioreactor and quad_tank): the archive used the absolute state, which moved the bioreactor's dilution rate to D = -0.16 at zero input, a physically different plant. Model-based baselines differentiate this exact map; only the input structure changes. The back-EMF must not change the plant's character: a system YAML may fix ``j`` / ``k`` where the automatic design would (two_link_arm: non-collocated, pumps energy; rossler: k = a cancels the term that makes it chaotic). """ def __init__(self, base: Plant, u_bar: float, k: float, j: int, x_ref: float): self.base, self.u_bar, self.k, self.j, self.x_ref = base, float(u_bar), float(k), int(j), float(x_ref) self.nx, self.nu, self.ny = base.nx, base.nu, base.ny self.sensors = base.sensors self.name = base.name self.PARAMS = base.PARAMS def f(self, x, u): zero = torch.zeros_like(u) f0 = self.base.f(x, zero) g = self.base.f(x, zero + 1) - f0 ue = self.u_bar * torch.tanh((u[:, 0] - self.k * (x[:, self.j] - self.x_ref)) / self.u_bar) return f0 + g * ue[:, None] def h(self, x): return self.base.h(x) def params(self): return self.base.params() def perturbed(self, rel): return SaturatingActuator(self.base.perturbed(rel), self.u_bar, self.k, self.j, self.x_ref) def actuator_design(base: Plant, box: torch.Tensor, u_bar: float, j: int = None) -> tuple: """(k, j, x_ref): j is the state the input pushes hardest over the IC box (unless given); the back-EMF gain makes k * half-span(x_j) = u_bar / 2, i.e. the actuator enters saturation inside the operating set rather than staying linear.""" gen = torch.Generator().manual_seed(0) lo, hi = box[:, 0], box[:, 1] X = lo + (hi - lo) * torch.rand(512, base.nx, generator=gen, dtype=torch.float64) if j is None: j = int(base.input_gain(X).abs().mean(0).argmax()) j = int(j) half = float(hi[j] - lo[j]) / 2 return 0.5 * u_bar / max(half, 1e-6), j, float(lo[j] + hi[j]) / 2 class KnownPart(Plant): """The modeller's model under incomplete knowledge: ``base.f_known`` in place of f.""" def __init__(self, base: Plant): self.base, self.nx, self.nu = base, base.nx, base.nu self.sensors, self.ny, self.name = base.sensors, base.ny, base.name + "/known" self.PARAMS = {} def f(self, x, u): return self.base.f_known(x, u) def params(self): return self.base.params() def build_plant(scfg: dict, perturb: float = 0.0, knowledge: str = "full") -> Plant: """Construct the plant described by a system config section. ``knowledge='partial'`` returns the modeller's model (``f_known``, see Plant.UNMODELLED); the actuator model is known in either case.""" mk = lambda: REGISTRY[scfg["plant"]](sensors=scfg.get("sensors"), **scfg.get("params", {})) base = mk().perturbed(perturb) if perturb else mk() if knowledge == "partial": base = KnownPart(base) elif knowledge != "full": raise ValueError(f"knowledge must be 'full' or 'partial', not {knowledge!r}") act = scfg.get("actuator") or {} if act.get("kind", "affine") == "saturating": u_bar = float(act.get("u_bar", 2.0)) * float(scfg.get("u_scale", 1.0)) k, j, xr = actuator_design(mk(), torch.tensor(scfg["ic_box"], dtype=torch.float64), u_bar, act.get("j")) k = float(act.get("k", k)) # YAML override (reason given there) return SaturatingActuator(base, u_bar, k, j, xr) return base