The electric field of a plane electromagnetic wave is given by
\( \overrightarrow E = {E_0}{{\widehat i + \widehat j} \over {\sqrt 2 }}\cos \left( {kz + \omega t} \right) \)
At t = 0, a positively charged particle is at the point (x, y, z) = \( \left( {0,0,{\pi \over k}} \right) \).
If its instantaneous velocity at (t = 0) is \( {v_0}\widehat k \) , the force acting on it due to the wave is :