🧄Curl and Vector Cross-Product Identity in General Coordinates

The solution demonstrates how tensor notation translates complex vector calculus operations into component-based index contractions. Crucially, the curl ( ×v\nabla \times v ) is generalized to arbitrary coordinates by replacing the Cartesian Levi-Civita symbol with the contravariant Levi-Civita tensor density (ηabc)\left(\eta^{a b c}\right), resulting in (×v)c=ηabcavb(\nabla \times v)^c=\eta^{a b c} \partial_a v_b. This formula is clean because the symmetry of the Christoffel symbols ensures they cancel out when contracted with the antisymmetric ηabc\eta^{a b c}. Finally, the complex vector identity v×(×w)+w×(×v)v \times(\nabla \times w)+w \times(\nabla \times v) is expressed in covariant components by nesting the tensor form of the curl inside the tensor form of the cross product, requiring multiple applications of the metric ( g ) and the η\eta tensor to manage all index raising and lowering.

Last updated

Was this helpful?