There has recently been interest in the role of inverse bremsstrahlung, the
emission of photons by fast suprathermal ions in collisions with ambient e
lectrons possessing relatively low velocities, in tenuous plasmas in variou
s astrophysical contexts. This follows a long hiatus in the application of
suprathermal ion bremsstrahlung to astrophysical models since the early 197
0s. The potential importance of inverse bremsstrahlung relative to normal b
remsstrahlung, i.e., where ions are at rest, hinges upon the underlying vel
ocity distributions of the interacting species. Ln this paper, we identify
the conditions under which the inverse bremsstrahlung emissivity is signifi
cant relative to that for normal bremsstrahlung in shocked astrophysical pl
asmas. We determine that, since both observational and theoretical evidence
favors electron temperatures almost comparable to, and certainly not very
deficient relative to, proton temperatures in shocked plasmas, these enviro
nments generally render inverse bremsstrahlung at best a minor contributor
to the overall emission. Hence, inverse bremsstrahlung can be safely neglec
ted in most models invoking shock acceleration in discrete sources such as
supernova remnants. However, on scales greater than or similar to 100 pc di
stant from these sources, Coulomb collisional losses can deplete the cosmic
-ray electrons, rendering inverse bremsstrahlung, and perhaps bremsstrahlun
g from knock-on electrons, possibly detectable.