The efficiency of a Carnot engine is given by:
$\eta = 1 - \frac{T_L}{T_H}$
where:
When $T_H = T_L$, the efficiency is $\eta = 1 - \frac{T_L}{T_L} = 0$. This means the graph should start at the point $(T_L, 0)$.
As $T_H$ increases, the efficiency increases.
However, the efficiency can never exceed 1. As $T_H$ approaches infinity, the efficiency approaches 1.
Therefore, the graph should asymptotically approach $\eta = 1$.
Rearranging the efficiency equation, we get:
$\eta = 1-\frac{T_L}{T_H} $ $1 - \eta = \frac{T_L}{T_H} $ $T_H = \frac{T_L}{1-\eta}$
The correct answer is (B)
In 1st case, Carnot engine operates between temperatures 300 K and 100 K. In 2nd case, as shown in the figure, a combination of two engines is used. The efficiency of this combination (in 2nd case) will be: