The condition for a perfect fluid in the metric-affine extension of the Rie
mannian spacetime of general relativity is determined. The condition for a
pure perfect fluid without any additional interactions imposes a very stron
g restriction bn the continuity relation for the fluid. The effect of this
restriction is to remove both the torsion and the Weyl vectors from the fie
ld equations. This shows that for matter described entirely by a perfect fl
uid, the continuity relation for the fluid must take its general relativist
ic form. This results opens up an entirely new arena in gravitational physi
cs for the systematic investigation of various fluids with additional matte
r fields in metric-affine geometry. It is also shown for the case of symmet
ry breaking terms that break projective invariance of the Riemann scalar La
grangian that the restrictive condition on the perfect fluid can be relaxed
; however this method of extending fluids to the full metric-affine geometr
y, as is already known, will introduce unknown coupling constants into the
theory.