Pre-Quantum Electrodynamics

Stokes' Theorem c.m.ic.stokes

\[ \int_{\cal S} ({\boldsymbol \nabla} \times {\bf v}) \cdot d{\bf a} = \oint_{\cal P} {\bf v} \cdot d{\bf l}. \label{Gr(1.57)} \]

Corollary 1: \(\int ({\boldsymbol \nabla} \times {\bf v}) \cdot d{\bf a}\) depends only on the boundary line and not on the particular surface used.

Corollary 2: \(\oint ({\boldsymbol \nabla} \times {\bf v}) \cdot d{\bf a}= 0\) for any closed surface, since the boundary shrinks to a point.


Author: Jean-Sébastien Caux

Created: 2022-02-07 Mon 08:02

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