 Excess dissipation of a Burgers vortex

The swirl viscous dissipation of a steady Burgers vortex, integrated per unit length and per unit density, is $\nu \int {\omega }_z^{2}dA=\alpha {\Gamma }^2/(8\pi )$. It remains finite as kinematic viscosity tends to zero at fixed strain and circulation. This is excess over the background strain: the uniform strain itself has infinite total viscous dissipation over an infinite cross-section.