(a) In isothermal compression, there is always an increase of heat which must flow out of the gas
$\mathrm{\Delta}Q = \mathrm{\Delta}U + \mathrm{\Delta}W \Rightarrow \mathrm{\Delta}Q = \mathrm{\Delta}W\ \lbrack\because\mathrm{\Delta}U = 0\rbrack$
$\Rightarrow \ \mathrm{\Delta}Q = - 1.5 \times 10^{4}J = \frac{1.5 \times 10^{4}}{4.18}cal = - 3.6 \times 10^{3}cal$