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Project-declaredLean 4.32.0 · mathlib@81a5d257c8e4

Kinetic Energy eq translational add body Angular Velocity

RigidBodyMotion.kineticEnergy_eq_translational_add_bodyAngularVelocity

Project documentation

König's theorem in the body frame. The total kinetic energy M.kineticEnergy t, formed from the lab-frame point velocities, splits at the centre of mass (centerOfMass = 0) as T = ½ M ⟪V, V⟫ + rotationalKineticEnergy ω_body. The rotational energy is a frame-independent scalar, so it is evaluated here from the body-frame angular velocity ω_body...

Exact Lean statement

theorem kineticEnergy_eq_translational_add_bodyAngularVelocity (M : RigidBodyMotion 3) (t : Time)
    (h : M.mass ≠ 0) (hR : DifferentiableAt ℝ (fun s => (M.orientation s).1) t)
    (hc : M.centerOfMass = 0) :
    M.kineticEnergy t
      = (1 / (2 : ℝ)) * M.mass * (⟪M.centerOfMassVelocity t, M.centerOfMassVelocity t⟫_ℝ)
        + M.toRigidBody.rotationalKineticEnergy (M.bodyAngularVelocity t)

Formal artifact

Lean source

Canonical source
Full Lean sourceLean 4
theorem kineticEnergy_eq_translational_add_bodyAngularVelocity (M : RigidBodyMotion 3) (t : Time)    (h : M.mass  0) (hR : DifferentiableAt  (fun s => (M.orientation s).1) t)    (hc : M.centerOfMass = 0) :    M.kineticEnergy t      = (1 / (2 : )) * M.mass * (⟪M.centerOfMassVelocity t, M.centerOfMassVelocity t⟫_)        + M.toRigidBody.rotationalKineticEnergy (M.bodyAngularVelocity t) := by  rw [M.kineticEnergy_eq_translational_add_rotational t h,    RigidBody.rotationalKineticEnergy_eq_integral]  congr 1  congr 2  ext y  have hy : (fun j => (y : Fin 3  ) j - M.centerOfMass j) = (y : Fin 3  ) := by    simp [hc]  simp only [cmap_apply, ContMDiffMap.coeFn_mk]  rw [hy, M.deriv_orientation_mulVec_eq_orientation_bodyAngularVelocity_cross (y : Fin 3  ) t hR,    Matrix.dotProduct_mulVec_orthogonal (mul_eq_one_comm.mp (M.orientation_mul_transpose t))]
Project
Physlib
License
Apache-2.0
Commit
dd43e9e65791
Source
Physlib/ClassicalMechanics/RigidBody/KineticEnergy.lean:180-195

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