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Question

Physics Question on Thermodynamics

A Carnot engine is operating between a hot body and cold body maintained at temperature T1T_1 and T2T_2 respectively. Consider the following three cases : The temperature of the hot body is changed to T1+ΔTT_1 + \Delta T and cold body is at T2T_2 : The temperature of the hot body is at T1T_1 and cold body is changed to T2+ΔTT_2 + \Delta T : The temperature of the hot body is at T1T_1 and cold body is changed to T2ΔTT_2 - \Delta T

A

The efficiency of the Carnot cycle is highest for case -I

B

The efficiency of the Carnot cycle is highest for case -II

C

The efficiency of the Carnot cycle is highest for case -III

D

The efficiency of case -II is higher than case -III

Answer

The efficiency of the Carnot cycle is highest for case -III

Explanation

Solution

We know that efficiency of Carnot engine is given by relation
η=T1T2T1\eta=\frac{T_{1}-T_{2}}{T_{1}}
Hence in
ηI=(T1+ΔT)T2T1+ΔT\eta_{ I } =\frac{\left(T_{1}+\Delta T\right)-T_{2}}{T_{1}+\Delta T}
=(T1T2)+ΔTT1+ΔT=\frac{\left(T_{1}-T_{2}\right)+\Delta T}{T_{1}+\Delta T}
ηII=T1(T2+ΔT)T1\eta_{ II } =\frac{T_{1}-\left(T_{2}+\Delta T\right)}{T_{1}}
ηIII=T1(T2ΔT)T1\eta_{ III } =\frac{T_{1}-\left(T_{2}-\Delta T\right)}{T_{1}}
=(T1T2)+ΔTT1=\frac{\left(T_{1}-T_{2}\right)+\Delta T}{T_{1}}
So, from above efficiences we can conclude the order as
ηIII>ηII>ηI\eta_{ III }>\eta_{ II }>\eta_{ I }