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One mole of an ideal monatomic gas undergoes a process described by the equation PV3 = constant. The heat capacity of the gas during this process is : |
\(\frac{3}{2}R\) \(\frac{5}{2}R\) \(2R\) \(R\) |
\(R\) |
PV3 = constant ; ⇒ n = 3 C = Cv + \(\frac{R}{1 - n}\) = \(\frac{R}{r - 1}\) + \(\frac{R}{1 - n}\) r = 5/3 ⇒ C = R |
