We derive an expression for the effective gravitational mass for any closed
spacelike 2-surface. This effective gravitational energy is defined direct
ly through the geometrical quantity of the freely falling a-surface and thu
s is well adapted to intuitive expectation that the gravitational mass shou
ld be determined by the motion of a test body moving freely in the gravitat
ional field. We find that this effective gravitational mass has a reasonabl
e positive value for a small sphere in the non-vacuum space-times and can b
e negative for the vacuum case. Further, this effective gravitational energ
y is compared with the quasi-local energy based on the (2 + 2) formalism of
General Relativity. Although some gauge freedoms exist, analytic expressio
ns of the quasi-local energy for vacuum cases are the same as the effective
gravitational mass. Especially, we see that the contribution from the cosm
ological constant is the same in general cases.