The relationship between atmospheric circulation and vorticity is fundamentally described by Stokes theorem. This theorem provides a general link between the line integral of a vector field around a closed curve and the surface integral of its curl over a surface bounded by that curve.
Stokes theorem states that the circulation around a closed curve $C$ is equal to the flux of the vorticity vector through any surface $S$ that has $C$ as its boundary:
$ \oint_C \mathbf{v} \cdot d\mathbf{l} = \iint_S (\nabla \times \mathbf{v}) \cdot d\mathbf{S} $
Substituting the definitions of circulation and vorticity, we get:
$ \Gamma = \iint_S \boldsymbol{\omega} \cdot d\mathbf{S} $
This equation establishes the most general relationship: circulation is the integrated measure of vorticity over a surface. This principle is crucial in understanding large-scale atmospheric motions and weather patterns.