Question #40672

N MOLES OF A MONOATOMIC GAS IS CARRIED AROUND THE REVERSIBLE RECTANGULAR CYCLE ABCDA AS SHOWN IN THE DIAGRAM. THE TEMPERATURE AT A IS To . THE THERMODYNAMIC EFFICIENCY OF THE CYCLE IS :
1. 15 %
2. 20 %
3. 25 %
4. 50 %

Expert's answer

Answer on Question #40672, Physics, Molecular Physics

N MOLES OF A MONOATOMIC GAS IS CARRIED AROUND THE REVERSIBLE RECTANGULAR CYCLE ABCDA AS SHOWN IN THE DIAGRAM. THE TEMPERATURE AT A IS TO . THE THERMODYNAMIC EFFICIENCY OF THE CYCLE IS : 1. 15%15\% 2. 20%20\% 3. 25%25\% 4. 50%50\%

Solution


In any cyclic process, the net work done by the system is equal to the area enclosed by the cyclic thermodynamic path in a p-V diagram. So


Wnet=(pBpA)(VDVA)=(2p0p0)(2V0V0)=p0V0.W _ {n e t} = (p _ {B} - p _ {A}) (V _ {D} - V _ {A}) = (2 p _ {0} - p _ {0}) (2 V _ {0} - V _ {0}) = p _ {0} V _ {0}.


Total heat absorbed by the cycle is the sum of the heat absorbed along path AB and the heat absorbed along path BC:


QA=QAB+QBC.Q _ {A} = Q _ {A B} + Q _ {B C}.


The heat absorbed along path AB:


QAB=CVN(TBT0).Q _ {A B} = C _ {V} N (T _ {B} - T _ {0}).


From the ideal gas state equation:


TB=2p0V0NR,T _ {B} = \frac {2 p _ {0} \cdot V _ {0}}{N R},


and


T0=p0V0NR.T _ {0} = \frac {p _ {0} \cdot V _ {0}}{N R}.


The heat absorbed along path AB:


QAB=CVN(TBT0)=32RN(2p0V0NRp0V0NR)=32p0V0.Q _ {A B} = C _ {V} N (T _ {B} - T _ {0}) = \frac {3}{2} R N \left(\frac {2 p _ {0} \cdot V _ {0}}{N R} - \frac {p _ {0} \cdot V _ {0}}{N R}\right) = \frac {3}{2} p _ {0} \cdot V _ {0}.


The heat absorbed along path BC:


QBC=CPN(TCTB).Q _ {B C} = C _ {P} N (T _ {C} - T _ {B}).


From the ideal gas state equation:


TC=2p02V0NR.T _ {C} = \frac {2 p _ {0} \cdot 2 V _ {0}}{N R}.


The heat absorbed along path AB:


QBC=CPN(TCTB)=52RN(2p02V0NR2p0V0NR)=5p0V0.Q _ {B C} = C _ {P} N (T _ {C} - T _ {B}) = \frac {5}{2} R N \left(\frac {2 p _ {0} \cdot 2 V _ {0}}{N R} - \frac {2 p _ {0} \cdot V _ {0}}{N R}\right) = 5 p _ {0} \cdot V _ {0}.


Total heat absorbed by the cycle


QA=32p0V0+5p0V0=132p0V0.Q _ {A} = \frac {3}{2} p _ {0} \cdot V _ {0} + 5 p _ {0} \cdot V _ {0} = \frac {13}{2} p _ {0} \cdot V _ {0}.


Thermal efficiency of a cycle:


η=WnetQA=p0V0132p0V0=21315%.\eta = \frac {W _ {n e t}}{Q _ {A}} = \frac {p _ {0} \cdot V _ {0}}{\frac {13}{2} p _ {0} \cdot V _ {0}} = \frac {2}{13} \approx 15\%.


Answer: 1.15%1.15\% .

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