Mass `M` is distributed uniformly along a line of length `2L`. A particle of mass `m` is at a point that is at a distance `a` above the centre of the line on the its perpendicular bisector (Point `P` in figure). The gravitational force that the line exert on the particle is
A. `(GMm)/(sqrt(L^(2)+a^(2)))`
B. `(GMm)/(a(L^(2)+a^(2)))`
C. `(GMm)/(asqrt(L^(2)+a^(2)))`
D. `(GMm)/(a(L^(2)+a^(2))^(2))`