A formalism of classical mechanics is given for time-dependent many-body states of quantum
mechanics, describing both fluid flow and point mass trajectories. The familiar equations of
energy, motion, and those of Lagrangian mechanics are obtained. An energy and continuity
equation is demonstrated to be equivalent to the real and imaginary parts of the time dependent
Schroedinger equation, respectively, where the Schroedinger equation is in density matrix form.
For certain stationary states, using Lagrangian mechanics and a Hamiltonian function for
quantum mechanics, equations for point-mass trajectories are obtained. For 1-body states and
fluid flows, the energy equation and equations of motion are the Bernoulli and Euler equations
of fluid mechanics, respectively. Generalizations of the energy and Euler equations are
derived to obtain equations that are in the same form as they are in classical mechanics. The
fluid flow type is compressible, inviscid, irrotational, with the nonclassical element of local
variable mass. Over all space mass is conserved. The variable mass is a necessary condition for
the fluid flow to agree with the zero orbital angular momentum for s states of hydrogen. Cross
flows are examined, where velocity directions are changed without changing the kinetic energy.
For one-electron atoms, the velocity modification gives closed orbits for trajectories, and
mass conservation, vortexes, and density stratification for fluid flows. For many body states,
Under certain conditions, and by hypotheses, Euler equations of orbital-flows are
obtained. One-body Schroedinger equations that are a generalization of the Hartree-Fock
equations are also obtained. These equations contain a quantum Coulomb's law, involving the
2-body pair function of reduced density matrix theory that replace the charge densities.