The spatial factor PHI(X) of the vibratory-state MWB ('multiple water-
bag') plasma potential phi = PHI(X) exp (-iomegat) in the vicinity of
its generating electric charge rho(X) exp(-iomegat) is proved to be th
e Poisson potential U(X) of rho plus an error function xi(X) whose mag
nitude can be rendered as small as desired, in relation to \PHI(X)\, b
y locating the recording point sufficiently close to the charge. How c
lose this should be is independent of rho, but depends quantitatively
on the MWB model and the frequency omega, and qualitatively on whether
the frequency of the vibrations is greater or less than the plasma fr
equency. A high vibration frequency reinforces accuracy in the Poisson
ian approximation. The question as to whether phi is weaker or stronge
r than U(X)) is tacked. Shielding efficiency is explored in the vibrat
ory state.