Coriolis and centrifugal rotating-frame acceleration
For a frame rotating at constant Ω about a common inertial origin, a_inertial=a_rot+2Ω×v_rot+Ω×(Ω×r).
Key knowledge
For a frame rotating at constant Ω about a common inertial origin, a_inertial=a_rot+2Ω×v_rot+Ω×(Ω×r). Newton's law in that rotating frame therefore includes the inertial forces −2mΩ×v_rot and −mΩ×(Ω×r).
Values and equations
m a_rot=F_real−2mΩ×v_rot−mΩ×(Ω×r)
- m
- Mass kg
- a_rot
- Rotating-frame acceleration m s⁻²
- F_real
- Physical resultant force N
- Ω
- Constant angular-velocity vector rad s⁻¹
- v_rot
- Rotating velocity m s⁻¹
- r
- Position relative to common origin m
Conditions and scope
- Classical motion, constant angular velocity and a shared nonaccelerating origin.
- Time-varying rotation adds −mΩ̇×r and acceleration of the origin adds −ma_origin; they are excluded from this displayed constant-rotation model. Inertial forces depend on frame choice.
Sources · 1
References
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Evidence and review
Newtonian Dynamics: Rotating reference frames: Equations 406–414: vector time derivatives and inertial/rotating acceleration relation.
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Entry details
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- physics-rotating-frame-acceleration
- Revision
- university-core.1
- Structured reference record
- University core expansion