The functionals of the Kohn and Sil variational principles of atomic c
ollision theory contain second-order spatial derivatives of the wave-f
unction. Ipso facto the 'second-order'' generalised Euler-Lagrange dif
ferential equation is a necessary condition for these functionals to y
ield a stationary value. To illustrate this we provide a classical pre
scription for the time-dependent and time-independent quantum potentia
l scattering problems, generalising the latter to the three-body probl
em. As practical examples where the presence of second-order derivativ
es in the Lagrangian density makes a non-trivial contribution to the e
quations of motion, we consider the optimisation of translation factor
s in a trial wave-function using the Sil variational principle and the
optimisation of a variable charge using the Kohn variational principl
e. As further examples of Lagrangian densities where second-order deri
vatives may occur we briefly mention electromagnetism and relativistic
quantum mechanics.