Chapter 12: Problem 28
The internal energy \(U\) is a unique function of any state because of change in \(U\) (A) does not depend upon path. (B) depends upon path. (C) corresponds to an adiabatic process. (D) corresponds to an isothermal process.
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Chapter 12: Problem 28
The internal energy \(U\) is a unique function of any state because of change in \(U\) (A) does not depend upon path. (B) depends upon path. (C) corresponds to an adiabatic process. (D) corresponds to an isothermal process.
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The net work done on the gas in the cycle \(A B C D A\) is \([2009]\) (A) Zero (B) \(276 R\) (C) \(1076 R\) (D) \(1904 R\)
Equal amount of same gas in two similar cylinders, \(A\) and \(B\), compressed to same final volume from same initial volume one adiabatically and another isothermally, respectively, then (A) final pressure in \(A\) is more than in \(B\). (B) final pressure in \(B\) is greater than in \(A\). (C) final pressure in both equal. (D) for the gas, value of \(\gamma=\frac{C_{p}}{C_{V}}\) is required.
When a given quantity of an ideal monoatomic gas is at pressure \(P\) and absolute temperature \(T\), then the adiabatic bulk modulus of the gas will be (A) \(P\) (B) \(\frac{5}{3} P\) (C) \(T\) (D) \(\frac{5 T}{2}\)
An ideal heat engine working between temperatures \(T_{H}\) and \(T_{L}\) has efficiency \(\eta .\) If both the temperature are raised by \(100 \mathrm{~K}\) each, the new efficiency of the heat engine will be (A) equal to \(\eta\). (B) greater than \(\eta\). (C) less than \(\eta\). (D) greater or less than \(\eta\) depending upon the nature of the working substance.
Two moles of an ideal gas at \(300 \mathrm{~K}\) were cooled at constant volume so that the pressure is reduced to half the initial value. As a result of heating at constant pressure, the gas has expanded till it attains the original temperature. The total heat absorbed by gas, if \(R\) is the gas constant (A) \(150 R\) (B) \(300 R\) (C) \(75 R\) (D) \(100 R\)
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