371328
If the source and sink temperature are \(411^\circ C\) and \(69^\circ C\) respectively and the engine extracts \(1000\;J\) of heat in each cycle, then area enclosed by the PV diagram is
371329
In a heat engine, the temperature of the working substance at the end of the cycle is
1 Equal to that at the beginning
2 More than that at the beginning
3 Less than that at the beginning
4 Determined by the amount of heat rejected at the sink
Explanation:
Internal energy is a function of \((T)\). As internal energy is a state function the working substance final temperature must be equal to intial temperature.
PHXI12:THERMODYNAMICS
371330
If the temperature of the sink is decreased, the efficiency of heat engine
1 First increases then decreases
2 Increases
3 Decreases
4 Remains unchanged
Explanation:
\(\eta=\left(1-\dfrac{0}{T_{2}}\right)=1\)
PHXI12:THERMODYNAMICS
371331
Heat engine rejects some heat to the sink. This heat
371328
If the source and sink temperature are \(411^\circ C\) and \(69^\circ C\) respectively and the engine extracts \(1000\;J\) of heat in each cycle, then area enclosed by the PV diagram is
371329
In a heat engine, the temperature of the working substance at the end of the cycle is
1 Equal to that at the beginning
2 More than that at the beginning
3 Less than that at the beginning
4 Determined by the amount of heat rejected at the sink
Explanation:
Internal energy is a function of \((T)\). As internal energy is a state function the working substance final temperature must be equal to intial temperature.
PHXI12:THERMODYNAMICS
371330
If the temperature of the sink is decreased, the efficiency of heat engine
1 First increases then decreases
2 Increases
3 Decreases
4 Remains unchanged
Explanation:
\(\eta=\left(1-\dfrac{0}{T_{2}}\right)=1\)
PHXI12:THERMODYNAMICS
371331
Heat engine rejects some heat to the sink. This heat
371328
If the source and sink temperature are \(411^\circ C\) and \(69^\circ C\) respectively and the engine extracts \(1000\;J\) of heat in each cycle, then area enclosed by the PV diagram is
371329
In a heat engine, the temperature of the working substance at the end of the cycle is
1 Equal to that at the beginning
2 More than that at the beginning
3 Less than that at the beginning
4 Determined by the amount of heat rejected at the sink
Explanation:
Internal energy is a function of \((T)\). As internal energy is a state function the working substance final temperature must be equal to intial temperature.
PHXI12:THERMODYNAMICS
371330
If the temperature of the sink is decreased, the efficiency of heat engine
1 First increases then decreases
2 Increases
3 Decreases
4 Remains unchanged
Explanation:
\(\eta=\left(1-\dfrac{0}{T_{2}}\right)=1\)
PHXI12:THERMODYNAMICS
371331
Heat engine rejects some heat to the sink. This heat
371328
If the source and sink temperature are \(411^\circ C\) and \(69^\circ C\) respectively and the engine extracts \(1000\;J\) of heat in each cycle, then area enclosed by the PV diagram is
371329
In a heat engine, the temperature of the working substance at the end of the cycle is
1 Equal to that at the beginning
2 More than that at the beginning
3 Less than that at the beginning
4 Determined by the amount of heat rejected at the sink
Explanation:
Internal energy is a function of \((T)\). As internal energy is a state function the working substance final temperature must be equal to intial temperature.
PHXI12:THERMODYNAMICS
371330
If the temperature of the sink is decreased, the efficiency of heat engine
1 First increases then decreases
2 Increases
3 Decreases
4 Remains unchanged
Explanation:
\(\eta=\left(1-\dfrac{0}{T_{2}}\right)=1\)
PHXI12:THERMODYNAMICS
371331
Heat engine rejects some heat to the sink. This heat