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Same dispersion relation as in spatial case. i.e. \omega=\alpha U – i \alpha^2\epsilon
Expansions assumed around neutral curve, then small imaginary dw can be related to small imaginary da
Note that modes with negative \alpha_i here represent decaying upstream propagating modes
TS mode is damped in left figure
Taking into account non-parallel effects for TS-waves. Assume that U(x,y) and V(x,y) is the base flow.
Normalization condition is integral of weighted x-variation
Generalizations of optimals to spatially developing, non-parallel flow
3D disturbances that corresponds to streaks and streamwise vorticies
Expand u_0 in eigenfunctions of A*A, operating repeatedly with A*A will result bring out \lambda_1
Identify the action of the adjoint in the integrals resulting from the integration by parts