  Static charged perfect fluid distributions have been studied. It is shown
that if the norm of the timelike Killing vector and the electrostatic potential
have the Weyl-Majumdar relation, then the background spatial metric is the
space of constant curvature, and the field equations reduces to a single
non-linear partial differential equation. Furthermore, if the linear equation
of state for the fluid is assumed, then this equation becomes a Helmholtz
equation on the space of constant curvature. Some explicit solutions are given.
