To solve this problem, we need to understand the working principle of a Carnot cycle, which is a theoretical thermodynamic cycle that provides insight into the efficiency of heat engines.
The Carnot efficiency \eta of an engine operating between two temperatures is given by the formula:
\eta = 1 - \frac{T_{2}}{T_{1}}
where:
Given temperatures:
Substituting these values into the efficiency formula, we get:
\eta = 1 - \frac{400}{500} = 1 - 0.8 = 0.2
This means the efficiency of the engine is 0.2 or 20%.
The engine absorbs 6\, kcal of heat at the higher temperature. The work done by the engine is the amount of heat absorbed multiplied by the efficiency:
\text{Work} = \eta \times \text{Heat Absorbed} = 0.2 \times 6\, \text{kcal} = 1.2\, \text{kcal}
Thus, the amount of heat converted into work is 1.2 kcal, which corresponds to the correct answer.
A real gas within a closed chamber at \( 27^\circ \text{C} \) undergoes the cyclic process as shown in the figure. The gas obeys the equation \( PV^3 = RT \) for the path A to B. The net work done in the complete cycle is (assuming \( R = 8 \, \text{J/molK} \)):
