Is Total Time Derivative explicit
ClassicalMechanics.Lagrangian.isTotalTimeDerivative_explicit
Plain-language statement
Explicit reformulation (by the chain rule): δL(t, q, dₜ q) = ∂F/∂t(t, q) + ⟨∇ᵣF(t, q), dₜ q⟩ or δL(t, q, dₜ q) = fderiv ℝ F (t, q) (1, dₜ q)
Exact Lean statement
lemma isTotalTimeDerivative_explicit {δL : Time → X → X → ℝ} :
IsTotalTimeDerivative δL ↔ (∃ (F : Time → X → ℝ) (_ : ContDiff ℝ ∞ ↿F),
∀ t q v, δL t q v = fderiv ℝ ↿F (t, q) ((1 : Time), v))Formal artifact
Lean source
lemma isTotalTimeDerivative_explicit {δL : Time → X → X → ℝ} : IsTotalTimeDerivative δL ↔ (∃ (F : Time → X → ℝ) (_ : ContDiff ℝ ∞ ↿F), ∀ t q v, δL t q v = fderiv ℝ ↿F (t, q) ((1 : Time), v)) := by -- Preliminary construction: properties of the function t => (t, q t) let tq := fun (q : Time → X) t => (t, q t) have h_tq_contDiff : ∀ (q : Time → X), ContDiff ℝ ∞ q -> ContDiff ℝ ∞ (tq q) := by fun_prop have h_tq_der : ∀ (q : Time → X) t, ContDiff ℝ ∞ q -> ∂ₜ (tq q) t = (1, ∂ₜ q t) := by intro q t h_ContDiff_q ext change (∂ₜ (tq q) t).1.val = (1 : Time).val congr apply Eq.symm calc (1 : Time) = fderiv ℝ (fun (t' : Time) => t') t 1 := by simp only [fderiv_fun_id, ContinuousLinearMap.coe_id', id_eq] _ = fderiv ℝ (fun (t' : Time) => (tq q t').1) t 1 := by rfl _ = (∂ₜ (tq q) t).1 := by rw [fderiv.fst] · simp rfl · apply ContDiffAt.differentiableAt · apply ContDiff.contDiffAt exact h_tq_contDiff q h_ContDiff_q · by_contra rcases this apply Eq.symm calc (1, ∂ₜ q t).2 = fderiv ℝ (fun t' => (tq q t').2) t 1 := by rfl _ = (∂ₜ (tq q) t).2 := by rw [fderiv.snd] · simp only [ContinuousLinearMap.comp_apply, ContinuousLinearMap.coe_snd'] rfl · apply ContDiffAt.differentiableAt · apply ContDiff.contDiffAt exact h_tq_contDiff q h_ContDiff_q · by_contra rcases this have h_F_tq_der : ∀ (q : Time → X) (F : Time → X → ℝ) t, (ContDiff ℝ ∞ ↿F) → (ContDiff ℝ ∞ q) → ∂ₜ (fun t' => ↿F (t', q t')) t = fderiv ℝ ↿F (t, q t) ((1 : Time), ∂ₜ q t) := by intro q F t hF hq change fderiv ℝ ((↿F) ∘ (tq q)) t 1 = fderiv ℝ ↿F (t, q t) ((1 : Time), ∂ₜ q t) rw [fderiv_comp] · simp only [ContinuousLinearMap.comp_apply] rw [← Time.deriv_eq,h_tq_der] exact hq · apply ContDiffAt.differentiableAt · apply ContDiff.contDiffAt exact hF · by_contra rcases this · apply ContDiffAt.differentiableAt · apply ContDiff.contDiffAt exact h_tq_contDiff q hq · by_contra rcases this -- beginning of the proof constructor -- From total the total derivative to the explicit form · intro h rcases h with ⟨F, hF⟩ rcases hF with ⟨hFdif, hFder⟩ use F use hFdif intro t q₀ v let qv := fun (t' : Time) => (q₀ - t.val • v) + t'.val • v have h_qv_contDiff : ContDiff ℝ ∞ qv := by change ContDiff ℝ ∞ (((fun (tR : ℝ) => (q₀ - t.val • v) + tR • v)) ∘ Time.toRealCLE) fun_prop have h_qv_t : qv t = q₀ := by calc qv t = (q₀ - t.val • v) + t.val • v := by rfl _ = q₀ := by module have h_qv_der : ∂ₜ qv t = v := by calc ∂ₜ qv t = fderiv ℝ (fun t' => (q₀ - t.val • v) + t'.val • v) t 1 := by rfl _ = v := by rw [fderiv_const_add,fderiv_smul_const] · simp only [ContinuousLinearMap.smulRight_apply, fderiv_val, one_smul] · fun_prop rw [← h_qv_t, ← h_qv_der, hFder, ← h_F_tq_der] · rfl · exact hFdif · exact h_qv_contDiff · exact h_qv_contDiff -- From the explicit form to the total derivative · intro h rcases h with ⟨F, hF⟩ rcases hF with ⟨hFdif, hFder⟩ use F use hFdif intro t q hq_ContDiff rw [hFder, ← h_F_tq_der] · rfl · exact hFdif · exact hq_ContDiff- Project
- Physlib
- License
- Apache-2.0
- Commit
- dd43e9e65791
- Source
- Physlib/ClassicalMechanics/Lagrangian/TotalDerivativeEquivalence.lean:97-192
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