If three particles each of mass $M$ are placed at the three corners of an equilateral triangle of side $a$, the forces exerted by this system on another particle of mass $M$ placed (i) at the mid point of a side and (ii) at the centre of the triangle are respectively
(a) 0,0
(b) $\frac{4 G M^{2}}{3 a^{2}}, 0$
(c) $0, \frac{4 G M^{2}}{3 a^{2}}$
(d) $\frac{3 G M^{2}}{a^{2}}, \frac{G M^{2}}{a^{2}}$