Kelvin-Helmholtz instability (source code)

= Kelvin-Helmholtz instability
{c}
{wiki=Kelvin–Helmholtz_instability}

For a planar vortex sheet separating equal-density streams of velocities $U_1$ and $U_2$, a mode of nonzero <wavenumber> $k$ has complex growth exponent
$$
\sigma=-ik\frac{U_1+U_2}{2}
\mathbin{\pm}\frac{|k|\,|U_1-U_2|}{2}.
$$
One sign has positive <growth rate>, so every nonzero wavenumber is unstable in the inviscid zero-thickness model.