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.