  Color transparency (CT) in high momentum transfer $(e,e' \vec p)$ reactions
is explored. The spin of the proton and photon are treated explicitly, hence
the name ``Vector CT". The Dirac distorted wave impulse approximation is used
as a starting point; then CT effects are embedded. A hadronic basis is used to
describe the struck proton as a wavepacket of physical baryon resonances. The
effects of the wavepacket expansion on the normal component of the ejectile
polarization, which vanishes in the limit of full CT, are investigated. This
formalism is also applied to study CT effects in total cross sections,
individual separated nuclear response functions, Fermi motion of the initial
nucleon, non-zero size of the initial wavepacket and the effects of
relativistic lower components. We show that including CT reduces the violations
of current conservation (CC), a typical problem in calculations of this kind.
The energy dependence of the normal polarization in $(e,e' \vec p)$ reactions
is found to be slow. However, a measurement of the normal transverse response
in a heavy nucleus, such as $^{208}Pb$ seems to afford the opportunity to see
CT at quite low momentum transfers. The effects of Fermi motion are
investigated, and choosing the momentum of the struck nucleon to be large leads
to significant violations of CC.
