
Efficiency of a Carnot engine is 50% and the temperature of the sink is 500K. If the temperature of source is kept constant and its efficiency raised to 60% then the required temperatures of the sink will be
(A) $100K$
(B) $600K$
(C) $400K$
(D) $500K$
Answer
573.6k+ views
Hint: Here we have to find the required temperature of the sink if efficiency of Carnot engine is \[50\% \] and the constant temperature of the source means sink is\[500{\text{ }}K\]. If efficiency of Carnot engine is raised to \[60\% \].
Efficiency is basically used for measuring how much work or energy we can conserve in a process. In other words, it is like comparing the output of the energy to the input of the energy in any given system.
Complete step by step solution:
When the efficiency of the Carnot engine is $50\% $, then the outlet temperature ${T_2}$ is $500K$ that is ${T_2} = 500K$
We know the efficiency formula that is
$\eta = 1 - \dfrac{{{T_2}}}{{{T_1}}}$
Here we the value of efficiency that is $50\% $ and the value of ${T_2}$ is $500K$ now substitute the values in above equation
$ \Rightarrow \dfrac{{50}}{{100}} = 1 - \dfrac{{500}}{{{T_1}}}$
Now we have to find the value of ${T_1}$ hence it to R.H.S so the equation becomes
$ \Rightarrow \dfrac{{500}}{{{T_1}}} = 1 - \dfrac{{50}}{{100}}$
Now take the L.C.M so we get
$ \Rightarrow \dfrac{{500}}{{{T_1}}} = \dfrac{{100 - 50}}{{100}}$
So after the further simplification we get
${T_1} = \dfrac{{500 \times 100}}{{50}}$
After calculating we get
${T_1} = 1000K$
Now after increase in the efficiency up to $60\% $ with the temperature ${T_1} = 1000K$
Then we know the efficiency formula
$\eta = 1 - \dfrac{{{T_2}}}{{{T_1}}}$
Now substitute the values in the above equation
$\dfrac{{60}}{{100}} = 1 - \dfrac{{{T_2}}}{{1000}}$
Here we have to find ${T_2}$so take it outside then the equation becomes
$\dfrac{{{T_2}}}{{1000}} = 1 - \dfrac{{60}}{{100}}$
Now take the LCM in R.H.S
$\dfrac{{{T_2}}}{{1000}} = \dfrac{{100 - 60}}{{100}}$
Now after further simplification we get
${T_2} = \dfrac{{1000 \times 40}}{{100}}$
After calculating we get
${T_2} = 400K$
It is the required temperature of sink.
Hence, the correct answer is option (C).
Note: A Carnot heat engine is a theoretical engine that operates on the Carnot cycle it is an ideal reversible heat engine especially as postulated in the statement of Carnot's principle of engine efficiency
Efficiency is basically used for measuring how much work or energy we can conserve in a process. In other words, it is like comparing the output of the energy to the input of the energy in any given system.
Complete step by step solution:
When the efficiency of the Carnot engine is $50\% $, then the outlet temperature ${T_2}$ is $500K$ that is ${T_2} = 500K$
We know the efficiency formula that is
$\eta = 1 - \dfrac{{{T_2}}}{{{T_1}}}$
Here we the value of efficiency that is $50\% $ and the value of ${T_2}$ is $500K$ now substitute the values in above equation
$ \Rightarrow \dfrac{{50}}{{100}} = 1 - \dfrac{{500}}{{{T_1}}}$
Now we have to find the value of ${T_1}$ hence it to R.H.S so the equation becomes
$ \Rightarrow \dfrac{{500}}{{{T_1}}} = 1 - \dfrac{{50}}{{100}}$
Now take the L.C.M so we get
$ \Rightarrow \dfrac{{500}}{{{T_1}}} = \dfrac{{100 - 50}}{{100}}$
So after the further simplification we get
${T_1} = \dfrac{{500 \times 100}}{{50}}$
After calculating we get
${T_1} = 1000K$
Now after increase in the efficiency up to $60\% $ with the temperature ${T_1} = 1000K$
Then we know the efficiency formula
$\eta = 1 - \dfrac{{{T_2}}}{{{T_1}}}$
Now substitute the values in the above equation
$\dfrac{{60}}{{100}} = 1 - \dfrac{{{T_2}}}{{1000}}$
Here we have to find ${T_2}$so take it outside then the equation becomes
$\dfrac{{{T_2}}}{{1000}} = 1 - \dfrac{{60}}{{100}}$
Now take the LCM in R.H.S
$\dfrac{{{T_2}}}{{1000}} = \dfrac{{100 - 60}}{{100}}$
Now after further simplification we get
${T_2} = \dfrac{{1000 \times 40}}{{100}}$
After calculating we get
${T_2} = 400K$
It is the required temperature of sink.
Hence, the correct answer is option (C).
Note: A Carnot heat engine is a theoretical engine that operates on the Carnot cycle it is an ideal reversible heat engine especially as postulated in the statement of Carnot's principle of engine efficiency
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