  A generalized Euler equation of fluid dynamics is derived for describing
many-body states of quantum mechanics. The Eulerian Eq. can be viewed as
representing the interaction of two substates, where each substate has its own
velocity and pressure fields. These field quantities are given by maps of the
wavefunction. For one-body systems, the Eulerian Eq. can model either a fluid
or particle description of quantum states. The generalized Euler Eq. is shown
to be the gradient of an equation representing the total-energy of the two
substates, having two energy fields. This total-energy Eq. is a generalization
of the Bernoulli Eq. of fluid dynamics. The total-energy Eq., along with a
continuity-equation, is equivalent to the time-dependent Schroedinger Eq. An
equation is also derived that is equivalent to the main equation of Bohmian
mechanics with additional identifications: The quantum potential of Bohmian
mechanics is given as a sum of a kinetic energy and pressure fields. Also, the
time derivative of the wavefunction phase is replaced by an energy field. In
the formalism, field quantities are identified from their placement in
equations of classical mechanics and separately, by definitions that involve
the wavefunction and operators of quantum mechanics. This approach yields,
unintended, and unknown energy and pressure fields. These fields, however, are
shown to satisfy a continuity Eq., an equation that is equivalent to the other
equation of Bohmian mechanics. It is also demonstrated that energy conservation
holds for both of these energy fields, if the wavefunction is a
linear-combination of eigenvectors, where the eigenvectors can be
nondegenerate. A detailed investigation is given on the possible behavior, or
source, of an electron that has one of the velocity fields. Alternate formulae
for this velocity fields are also considered.
