In recent work it has been shown that there can be substantial transie
nt growth in the energy of small perturbations to plane Poiseuille and
Couette flows if the Reynolds number is below the critical value pred
icted by linear stability analysis. This growth, which may be as large
as O(1000), occurs in the absence of nonlinear effects and can be exp
lained by the non-normality of the governing linear operator - that is
, the nonorthogonality of the associated eigenfunctions. In this paper
we study various aspects of this energy growth for two- and three-dim
ensional Poiseuille and Couette flows using energy methods, linear sta
bility analysis, and a direct numerical procedure for computing the tr
ansient growth. We examine conditions for no energy growth, the depend
ence of the growth on the streamwise and spanwise wavenumbers, the tim
e dependence of the growth, and the effects of degenerate eigenvalues.
We show that the maximum transient growth behaves like O(R2), where R
is the Reynolds number. We derive conditions for no energy growth by
applying the Hille-Yosida theorem to the governing linear operator and
show that these conditions yield the same results as those derived by
energy methods, which can be applied to perturbations of arbitrary am
plitude. These results emphasize the fact that subcritical transition
can occur for Poiseuille and Couette flows because the governing linea
r operator is non-normal.