Four identical point masses, each of mass \(m\) and carrying charge \(+q\) are placed at the corners of a square of sides 'a' on a frictionless plain surface. If the particles are released simultaneously, the kinetic energy of the system when they are infinitely far apart is
(A) \(\frac{q^{2}}{a}(2 \sqrt{2}+1)\)
(B) \(\frac{q^{2}}{a}(\sqrt{2}+2)\)
(C) \(\frac{q^{2}}{a}(\sqrt{2}+4)\)
(D) \(\frac{q^{2}}{a}(\sqrt{2}+1)\)