Prandtl normal-mode equation
= Prandtl normal-mode equation
{c}
{title2=$\nu v'''=i\alpha[(U-c)v'-U'v]$}
For a frozen real parallel profile and modes proportional to $e^{i\alpha(x-ct)}$, continuity eliminates tangential <velocity> and gives this third-order equation. Wall conditions are $v=v'=0$; outer tangential matching gives $v'\to0$, with bounded $v$. Real coefficients give the spectral symmetry $(\alpha,c)\mapsto(-\alpha,c^*)$. For positive real <wavenumber>, growth means $\operatorname{Im}c>0$.