Write the geometric vector as V=∑iVi′ei′(t). A rotating orthonormal basis obeys e˙i′=Ω×ei′. The product rule gives the transport identityBoth terms must be expressed in the same basis before adding them. If R(t) maps rotating components into inertial components, the precise component equation is d(RV′)/dt=R(V˙′+Ω′×V′). The printed expression suppresses this basis conversion.
(dtdV)inertial=(dtdV)rotating+Ω×V.
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