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As Chuck Britton only slightly jocularly reminded us, the "acceleration of
gravity" commonly subsumes the centrifugal acceleration. It is a term
appropriate only to the laboratory frame on Earth's surface, a quantity
which can be measured by students in the lab. I guess Jim's point is that,
since it is not really a "purely" gravitational acceleration, we shouldn't
call it that.
However, in the context of the principle of equivalence, we
recognize that there is no real distinction between the two components in
the lab frame. There is no way to measure how much is "purely" gravitational
and how much is "fictitious". g (a vector quantity) is the gravitational
field in the laboratory. It manifests itself as the initial acceleration of
any body falling freely from rest in the laboratory frame.