(d) A series resonance circuit admits maximum current, as
$P = i^{2}R$
So, power dissipated is maximum at resonance.
So, frequency of the source at which maximum power is dissipated in the circuit is
$v = \frac{1}{2\pi\sqrt{LC}}$
$= \frac{1}{2 \times 3.14\sqrt{25 \times 10^{- 3} \times 400 \times 10^{- 6}}}$
$= \frac{1}{2 \times 3.14\sqrt{10^{- 5}}} = 50.3\ Hz$