The magnetic field vector of an electromagnetic wave is given by $B = {B_0}{{\widehat i + \widehat j} \over {\sqrt 2 }}\cos (kz - \omega t); where \widehat i,\widehat j represents unit vector along x and y-axis respectively. At t = 0s, two electric charges q1 of 4\pi coulomb and q2 of 2\pi coulomb located at \left( {0,0,{\pi \over k}} \right) and \left( {0,0,{{3\pi } \over k}} \right), respectively, have the same velocity of 0.5 c \widehat i$, (where c is the velocity of light). The ratio of the force acting on charge q1 to q2 is :-