In Newtonian notion force between to masses m1 and m2 separated

by a distance d is simply G m1 m2/d^2. This is an example of a theory

which accepts action at a distance. A second example is Coulomb's

law which states how two point charges interact with each other.

These laws do not specify when the effect of a source located

at the `source point' will be felt at a particular `field point'. The

interactions are assumed to be `instantaneous'.

Einstein's gravity however does not admit this principle.

How, then, in Einstein's gravity, gravitational attraction propagates

locally, by the local deformations of space-time.

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