  We derive the complete expression for the Brans Class I exterior spacetime
explicitly in terms of the energy and pressures profiles of a stationary
spherisymmetric gravity source. This novel and generic expression is achieved
in a parsimonious manner, requiring only a subset of the Brans-Dicke field
equation and the scalar equation. For distant orbiting test particles, this
expression promptly provides a simple, closed and exact formula of the
[textgreek]<LaTeX>\textgreek{g}</LaTeX> Eddington parameter, which reads
{\gamma}_{exact}=(({\omega}+1+({\omega}+2){\Theta})/({\omega}+2+({\omega}+1){\Theta})),
where {\Theta} is the ratio of the star's "total pressure" integral over its
energy integral. This non-perturbative result reproduces the usual
Post-Newtonian (({\omega}+1)/({\omega}+2)) expression in the case of a
"Newtonian star", in which the pressure is negligible with respect to the
energy density. Furthermore, it converges to the General Relativity value
({\gamma}_{GR}=1) as the star's equation of state approaches that of
ultra-relativistic matter (in which case {\Theta} approaches 1), a behavior
consistent with broader studies on scalar-tensor gravity. Our derivation
underscores the essence of these results involving (1) the key relevant portion
of the Brans-Dicke field equations, (2) the uniqueness of the Brans Class I
vacuum solution for the non-phantom action, viz. {\omega}>-3/2, and (3) the
involvement of only two free parameters in this solution, hence requiring two
quantities (energy and pressure integrals) of the mass source to fully
characterize the solution. From a practical standpoint, it elucidates how a
given stellar interior structure model determines the star's exterior
gravitational field and impacts the motions of light objects (such as planets
and accretion disks) orbiting it.
