Kirchhoff ellipse — where it appears
Named by 2 essays across one field — each of them below, with the objects they name alongside it.
The shape a vortex keeps
Outside a circular patch of uniform vorticity the flow is exactly the point vortex's — not nearly, exactly — so replacing one by the other looks free. It is not. The patch has a shape, the shape has a rotation rate of its own, and there is a strain above which no shape exists at all.
Past three, an ellipse is a shear layer
Kirchhoff's elliptical vortex turns for ever without changing shape, and Love showed in 1893 that it stops being stable at an aspect ratio of exactly three. Computed, that threshold turns out to be the first of a sequence — a new way of coming apart every one and a half aspect ratios — and the sequence ends somewhere recognisable. A long enough ellipse is a strip of vorticity, and it comes apart the way a shear layer does, at a rate Rayleigh found for the strip.
Named alongside it
The objects these essays reach for when they reach for this one.
Contour dynamicsEquilibriumModel limitTwo-dimensional flowVortex patchVorticityCirculationGrowth rateKelvin helmholtzMultipolePoint vortexRegularisation