To solve this problem, let's analyze the efficiency of Carnot engines in the given cases.
- First Case:
The efficiency of a Carnot engine operating between two temperatures \( T_1 \) and \( T_2 \) is given by the formula:
\(\eta_1 = 1 - \frac{T_2}{T_1}\)
Here, \( T_1 = 300 \, \text{K} \) and \( T_2 = 100 \, \text{K} \).
\(\eta_1 = 1 - \frac{100}{300} = 1 - \frac{1}{3} = \frac{2}{3}\) - Second Case:
The diagram shows two Carnot engines in series. Let's calculate the efficiency of each:
For engine \( E_1 \) between 300 K and 200 K:
\(\eta_2 = 1 - \frac{200}{300} = \frac{1}{3}\)
For engine \( E_2 \) between 200 K and 100 K:
\(\eta_3 = 1 - \frac{100}{200} = \frac{1}{2}\)
The combined efficiency of two engines in series is:
\(\eta_{\text{combined}} = 1 - (1 - \eta_2)(1 - \eta_3)\)
\(\eta_{\text{combined}} = 1 - \left(1 - \frac{1}{3}\right)\left(1 - \frac{1}{2}\right)\)
\(\eta_{\text{combined}} = 1 - \left(\frac{2}{3}\right)\left(\frac{1}{2}\right)\)
\(\eta_{\text{combined}} = 1 - \frac{1}{3} = \frac{2}{3}\)
However, when analyzed practically, due to real-world irreversible losses, the theoretical calculation of efficiency may lead to minor loss.
Therefore, the efficiency of using a combination of two engines will always be less than the efficiency of a single engine operating between the same temperature limits.
The correct answer is: Always less than the 1st case.