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Project-declaredLean 4.32.0 · mathlib@81a5d257c8e4

Kinetic Term eq sum

Electromagnetism.ElectromagneticPotential.kineticTerm_eq_sum

Project documentation

The kinetic energy from an electromagnetic potential. -/ noncomputable def kineticTerm {d} (𝓕 : FreeSpace) (A : ElectromagneticPotential d) : SpaceTime d → ℝ := fun x => - 1/(4 * 𝓕.μ₀) * {η' d | μ μ' ⊗ η' d | ν ν' ⊗ A.toFieldStrength x | μ ν ⊗ A.toFieldStrength x | μ' ν'}ᵀ.toField /-! ### A.1. Lorentz invariance of the kinetic term We show that the kine...

Exact Lean statement

lemma kineticTerm_eq_sum {d} {𝓕 : FreeSpace} (A : ElectromagneticPotential d) (x : SpaceTime d) :
    A.kineticTerm 𝓕 x =
    - 1/(4 * 𝓕.μ₀) * ∑ μ, ∑ ν, ∑ μ', ∑ ν', η μ μ' * η ν ν' *
      (Lorentz.CoVector.basis.tensorProduct Lorentz.Vector.basis).repr (A.toFieldStrength x) (μ, ν)
      * (Lorentz.CoVector.basis.tensorProduct Lorentz.Vector.basis).repr
        (A.toFieldStrength x) (μ', ν')

Formal artifact

Lean source

Canonical source
Full Lean sourceLean 4
lemma kineticTerm_eq_sum {d} {𝓕 : FreeSpace} (A : ElectromagneticPotential d) (x : SpaceTime d) :    A.kineticTerm 𝓕 x =    - 1/(4 * 𝓕.μ₀) * ∑ μ, ∑ ν, ∑ μ', ∑ ν', η μ μ' * η ν ν' *      (Lorentz.CoVector.basis.tensorProduct Lorentz.Vector.basis).repr (A.toFieldStrength x) (μ, ν)      * (Lorentz.CoVector.basis.tensorProduct Lorentz.Vector.basis).repr        (A.toFieldStrength x) (μ', ν') := by  rw [kineticTerm]  rw [toField_eq_repr]  rw [contrT_basis_repr_apply_eq_fin]  conv_lhs =>    enter [2, 2, μ]    rw [contrT_basis_repr_apply_eq_fin]    enter [2, ν]    rw [prodT_basis_repr_apply]    enter [1]    rw [contrT_basis_repr_apply_eq_fin]    enter [2, μ']    rw [contrT_basis_repr_apply_eq_fin]    enter [2, ν']    rw [prodT_basis_repr_apply]    enter [1]    rw [prodT_basis_repr_apply]    enter [1]    simp only [Tensorial.self_toTensor_apply]    rw [coMetric_repr_apply_eq_minkowskiMatrix]    change η μ' μ  conv_lhs =>    enter [2, 2, μ, 2, ν, 1, 2, μ', 2, ν', 1, 2]    simp only [Tensorial.self_toTensor_apply]    rw [coMetric_repr_apply_eq_minkowskiMatrix]    change η (ν') (ν)  conv_lhs =>    enter [2, 2, μ, 2, ν, 1, 2, μ', 2, ν', 2]    rw [toFieldStrength_tensor_basis_eq_basis]    change ((Lorentz.Vector.basis.tensorProduct Lorentz.Vector.basis).repr (A.toFieldStrength x))      (μ', ν')  conv_lhs =>    enter [2, 2, μ, 2, ν, 2]    rw [toFieldStrength_tensor_basis_eq_basis]    change ((Lorentz.Vector.basis.tensorProduct Lorentz.Vector.basis).repr (A.toFieldStrength x))      (μ, ν)  conv_lhs =>    enter [2, 2, μ]    enter [2, ν]    rw [Finset.sum_mul]    enter [2, μ']    rw [Finset.sum_mul]    enter [2, ν']    simp  conv_lhs => enter [2, 2, μ]; rw [Finset.sum_comm]  conv_lhs => rw [Finset.sum_comm]  conv_lhs => enter [2, 2, μ', 2, ν]; rw [Finset.sum_comm]  conv_lhs => enter [2, 2, μ']; rw [Finset.sum_comm]  rfl
Project
Physlib
License
Apache-2.0
Commit
dd43e9e65791
Source
Physlib/Electromagnetism/Dynamics/KineticTerm.lean:117-170

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