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Find the efficeincy of the thermodynamic cycle shown in figure for an ideal diatomic gas. |
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Answer» Let n be the number of moles of the gas and the temperature be `T_(0)` in the state A. Now, work done during the cycle `W=(1)/(2)xx(2V_(0)-V_(0))(2P_(0)-P_(0))=(1)/(2)P_(0)V_(0)` For the heat `(DeltaQ_(1))` given during the process `ArarrB`, we have `DeltaQ_(1)=DeltaW_(AB)+DeltaU_(AB)` `DeltaW_(AB)=` area under the straight line AB `=(1)/(2)(P_(0)+2P_(0))(2V_(0)-V_(0))=(3P_(0)V_(0))/(2)` Applying equation of state for the gas in the state A `&` B. `(P_(0)V_(0))/(T_(0))=((2P_(0))(2V_(0)))/(T_(B))rArrT_(B)=4T_(0)` `thereforeU_(AB)=nC_(v)DeltaT=n((5R)/(2))(4T_(0)-T_(0))` `=(15nRT_(2))/(2)=(15P_(0)V_(0))/(2)` `therefore DeltaQ_(1)=(3)/(2)P_(0)V_(0)+(15)/(2)P_(0)V_(0)=9P_(0)V_(0)` Obviously, the processes `BrarrC` and `CrarrA` involve the abstraction of heat from the gas. `"Efficiency"=("Work done per cycle")/("Total heat supplied per cycle")` i.e., `eta=((1)/(2)P_(0)V_(0))/(9P_(0)V_(0))=(1)/(18)` |
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