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But the question is about the Earth's gravity. Properly that is
the force
that the Earth exerts on the body.
That's "proper" in Newtonian physics, but we know better now and have
for nearly a hundred years.
I'm not saying that we shouldn't teach the antiquated, but still
useful concept that bodies attract each other by virtue of their mass
and separation, but we shouldn't actively work against eventual
better understanding by pretending that centrifugal effects are
merely unfortunate "corrections" to "real" gravitational forces.
Indeed, the modern perspective is simple, practical, and easily
explained: The "gravitational force" in *any* reference frame is m
times the local value of g and the way you find the local value of g
is by dropping an object and measuring its acceleration.
John Mallinckrodt
Cal Poly Pomona
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