This problem involves calculating the heat absorbed from the hot reservoir ($Q_H$) for a Carnot engine, given the work done per cycle ($W$) and the temperatures of the hot ($T_H$) and cold ($T_C$) reservoirs.
First, convert the given temperatures from Celsius to Kelvin (K):
The efficiency ($\eta$) of a Carnot engine depends only on the reservoir temperatures:
$ \eta = 1 - \frac{T_C}{T_H} $
Substitute the Kelvin temperatures:
$ \eta = 1 - \frac{400 \ K}{500 \ K} = 1 - \frac{4}{5} = 1 - 0.8 = 0.2 $
The efficiency of any heat engine is also defined as the ratio of work done ($W$) to the heat absorbed from the hot reservoir ($Q_H$):
$ \eta = \frac{W}{Q_H} $
Rearrange the formula to solve for $Q_H$:
$ Q_H = \frac{W}{\eta} $
Given $W = 1.04 \times 10^5 \ J$ and calculated $\eta = 0.2$:
$ Q_H = \frac{1.04 \times 10^5 \ J}{0.2} $
$ Q_H = 5.20 \times 10^5 \ J $
The heat absorbed from the hot reservoir per cycle is $5.20 \times 10^5 \ J$.
A thermodynamic system is taken through the cyclic process ABC as shown in the figure. The total work done by the system during the cycle $ABC$ is _________ $\text{J}$.

The internal energy of air in $4 m \times 4 m \times 3 m$ sized room at 1 atmospheric pressure will be ________ $\times 10^6$ J.
(Consider air as diatomic molecule)
A thermodynamic system is taken through the cyclic process ABC as shown in the figure. The total work done by the system during the cycle $ABC$ is _________ $\text{J}$.
