(i) The e.m. wave carries energy which is due to electric field vector and magnetic field vector. In e.m. wave $$E$$ and $$B$$ vary from point to point and from moment to moment. Let $$E$$ and $$B$$ be their time average. The energy density due to the electric field $$E$$ is
$$u_E = \dfrac{1}{2} \in_0 E^2$$
The energy density due to magnetic field $$B$$ is $$u B = \dfrac{1}{2}\dfrac{B^2}{\mu_0}$$
Total average energy density of em wave
$$u_{av}=uE+uB=\dfrac{1}{2}\in_0E^2+\dfrac{1}{2}\dfrac{B^2}{\mu_0}$$ ...(i)
Let the em wave be propagation along z-direction. The electric field vector and magnetic field vectors be represented by
$$E=E_0\sin (kz-wt)$$
$$B= B_0\sin (kz-wt)$$
The time average value of $$E^2$$ over complete cycle $$= E_0^2/2$$
and time average value of $$B^2$$ over complete cycle $$= B_0^2/2$$
$$\therefore u_{av} = \dfrac{1}{2} \in_0 \dfrac{E_0^2}{2} + \dfrac{1}{2}\mu_0\left(\dfrac{B_0^2}{2}\right) = \dfrac{1}{4} \in_0 E_0^2 + \dfrac{B_0^2}{4\mu_0}$$
(ii) we know that $$E_0 = cB_0$$ and $$c = \dfrac{1}{\sqrt{\mu_0\in_0}}$$.
$$\therefore \dfrac{1}{4} \dfrac{B_0^2}{\mu_0} = \dfrac{1}{4} \dfrac{E_0^2/c^2}{\mu_0} = \dfrac{E_0^2}{4\mu_0} \times \mu_0 \in_0 = \dfrac{1}{4} \in_0 E_0^2$$
$$\therefore uB = uE$$
Hence, $$u_{av} = \dfrac{1}{4} \in_0 E^2_0 + \dfrac{1}{4} \dfrac{B_0^2}{\mu_0} = \dfrac{1}{4} \in_0 E_0^2 + \dfrac{1}{4}\in_0 E^2_0=\dfrac{1}{4}\in_0E_0^2=\dfrac{1}{2}\dfrac{B^2_0}{\mu_0}$$
Time average intensity of the wave
$$I_{av} = u_{av}c=\dfrac{1}{2} \in E_0^2c=\dfrac{1}{2}\in_0cE_0^2$$
Hence, the correct option is $$(C)$$