Right answer is (d) \(\sum_{k=-\infty}^{\infty}|c_k|^2\)
The explanation: The average power of a periodic signal x(t) is given as
The average power of a periodic signal x(t) is given as \(\frac{1}{T_p} \int_{t_0}^{t_0+T_p}|x(t)|^2 dt\)
=\(\frac{1}{T_p} \int_{t_0}^{t_0+T_p}x(t).x^* (t) dt\)
=\(\frac{1}{T_p} \int_{t_0}^{t_0+T_p}x(t).\sum_{k=-\infty}^{\infty} c_k * e^{-j2πkF_0 t} dt\)
By interchanging the positions of integral and summation and by applying the integration, we get
=\(\sum_{k=-\infty}^{\infty}|c_k |^2\)