(d) Electric field $E = \frac{V}{l} - \frac{iR}{l}\ (R =$ Resistance of wire)
Magnetic field at the surface of wire $B = \frac{\mu_{0}i}{2\pi a}\ (a =$ radius of wire)
Hence poynting vector, directed radially inward is given
By $S = \frac{EB}{\mu_{0}} = \frac{iR}{\mu_{0}l}.\frac{\mu_{0}i}{2\pi a} = \frac{i^{2}R}{2\pi al}$