Equation Of Motion unique
ClassicalMechanics.DampedHarmonicOscillator.equationOfMotion_unique
Plain-language statement
Any two smooth solutions of the damped equation of motion with the same initial position and velocity are equal.
Exact Lean statement
lemma equationOfMotion_unique (x y : Time → EuclideanSpace ℝ (Fin 1))
(hx : ContDiff ℝ ∞ x) (hy : ContDiff ℝ ∞ y)
(hEOMx : S.EquationOfMotion x) (hEOMy : S.EquationOfMotion y)
(h0 : x 0 = y 0) (hv0 : ∂ₜ x 0 = ∂ₜ y 0) :
x = yFormal artifact
Lean source
lemma equationOfMotion_unique (x y : Time → EuclideanSpace ℝ (Fin 1)) (hx : ContDiff ℝ ∞ x) (hy : ContDiff ℝ ∞ y) (hEOMx : S.EquationOfMotion x) (hEOMy : S.EquationOfMotion y) (h0 : x 0 = y 0) (hv0 : ∂ₜ x 0 = ∂ₜ y 0) : x = y := by have hIC : (fun τ : ℝ => (x (Time.toRealCLE.symm τ), ∂ₜ x (Time.toRealCLE.symm τ))) 0 = (fun τ : ℝ => (y (Time.toRealCLE.symm τ), ∂ₜ y (Time.toRealCLE.symm τ))) 0 := by have h00 : Time.toRealCLE.symm (0 : ℝ) = (0 : Time) := map_zero Time.toRealCLE.symm simp only [h00, h0, hv0] have hEq := ODE_solution_unique_univ (v := fun _ p => S.phaseVectorField p) (s := fun _ => Set.univ) (t₀ := (0 : ℝ)) (f := fun τ : ℝ => (x (Time.toRealCLE.symm τ), ∂ₜ x (Time.toRealCLE.symm τ))) (g := fun τ : ℝ => (y (Time.toRealCLE.symm τ), ∂ₜ y (Time.toRealCLE.symm τ))) (fun _ => S.phaseVectorField.lipschitz.lipschitzOnWith) (fun τ => ⟨S.phaseCurve_hasDerivAt x hx hEOMx τ, Set.mem_univ _⟩) (fun τ => ⟨S.phaseCurve_hasDerivAt y hy hEOMy τ, Set.mem_univ _⟩) hIC funext t have h1 := congrFun hEq (Time.toRealCLE t) simp only [ContinuousLinearEquiv.symm_apply_apply] at h1 exact (Prod.ext_iff.mp h1).1- Project
- Physlib
- License
- Apache-2.0
- Commit
- dd43e9e65791
- Source
- Physlib/ClassicalMechanics/DampedHarmonicOscillator/Solution.lean:527-547
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