Let's solve this problem step-by-step using the concepts of thermodynamics related to the Carnot engine.
The efficiency (\( \eta \)) of a Carnot engine is given by the formula:
where \( T_{\text{sink}} \) is the temperature of the sink and \( T_{\text{source}} \) is the temperature of the source. All temperatures need to be in Kelvin.
Given:
We need to find the original source temperature (\( T_{\text{source, initial}} \)) using the formula:
Rearranging gives:
Next, we need to increase the efficiency by 50% of the original efficiency. This means the new efficiency (\( \eta_{\text{new}} \)) will be:
We now set up the equation for the new efficiency:
Solving for the new source temperature (\( T_{\text{source, new}} \)) gives:
Thus, the temperature of the source needs to be increased by:
Therefore, the correct answer is 250 K.
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 \( R = 8 \, \text{J/molK} \)):
