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Question: A Carnot engine works between ice point and steam point. In order to increase the efficiency of the ...

A Carnot engine works between ice point and steam point. In order to increase the efficiency of the engine by 20  %20\;\% , its source temperature will have to be changed by
(A) 29.5  K29.5\;K increase
(B) 29.5  K29.5\;K decrease
(C) 37.5C{37.5^\circ }C increase
(D) 29.5C{29.5^\circ }C decrease

Explanation

Solution

We will use the given conditions to obtain the efficiency of the engine. Then we shall increase the obtained efficiency by 20  %20\;\% . This efficiency is obtained when the source temperature has been raised which can be obtained by the same formula used to find the efficiency.

Formula used
η=1T1T2\eta = 1 - \dfrac{{{T_1}}}{{{T_2}}}
where T1{T_1} is the temperature of the sink and T2{T_2} is the temperature of the source.

Complete Step by step solution
The efficiency of a Carnot cycle is given by
η=1T1T2\eta = 1 - \dfrac{{{T_1}}}{{{T_2}}}
where T1{T_1} is the lower temperature and T2{T_2} is the higher temperature.
Here both the temperatures must be in Kelvin. Thus T1{T_1} here is the temperature at which ice melts which is 273  K273\;K and T2{T_2} is the temperature at which water starts boiling off into steam which is 373  K373\;K .
Thus substituting the values of the temperatures in the efficiency formula, we get,
η=1273  K373  K\Rightarrow \eta = 1 - \dfrac{{273\;K}}{{373\;K}}
Upon further solving we get,
η=10.7319\Rightarrow \eta = 1 - 0.7319
η=0.2681\Rightarrow \eta = 0.2681
It is given that the efficiency is to be increased by 20  %20\;\% . Therefore the new efficiency after the increase is 120  %120\;\% of the original efficiency of the Carnot engine.
ηnew=120100×0.2681\Rightarrow {\eta _{new}} = \dfrac{{120}}{{100}} \times 0.2681
ηnew=0.3217\Rightarrow {\eta _{new}} = 0.3217
This is the new efficiency of the engine. In the question, it is said that the source temperature needs to be changed. Therefore the sink temperature should remain the same. Thus the sink temperature T1{T_1} remains 273  K273\;K . However, the higher temperature of the source which was previously T2{T_2} needs to be changed to T3{T_3} .
Applying the formula of efficiency of the Carnot engine, we get
ηnew=1T1T3\Rightarrow {\eta _{new}} = 1 - \dfrac{{{T_1}}}{{{T_3}}}
Substituting the respective values, we get,
0.3217=1273  KT3\Rightarrow 0.3217 = 1 - \dfrac{{273\;K}}{{{T_3}}}
Upon rearranging the equation we get,
273  KT3=10.3217\Rightarrow \dfrac{{273\;K}}{{{T_3}}} = 1 - 0.3217
273  KT3=0.6783\Rightarrow \dfrac{{273\;K}}{{{T_3}}} = 0.6783
On rearranging the terms, we get,
T3=273  K0.6783\Rightarrow {T_3} = \dfrac{{273\;K}}{{0.6783}}
T3=402.48  K\Rightarrow {T_3} = 402.48\;K
Therefore we can see that the source temperature has increased.
We need to find the amount by which it has increased. Thus we will subtract the initial source temperature from the newly obtained final source temperature, i.e. T3T2{T_3} - {T_2} .
T3T2=402.48  K373  K\Rightarrow {T_3} - {T_2} = 402.48\;K - 373\;K
T3T2=29.48  K\Rightarrow {T_3} - {T_2} = 29.48\;K
Thus the correct answer is option (A).

Note
Here in the options provided, we have both temperatures in Kelvin and Celsius scales. It should be known that both these scales have the same difference in one unit change in their temperatures. This means that 1C{1^\circ }C rise or fall in temperature would mean the same when the temperature is increased or decreased by 1  K1\;K .