Q: Cp is always greater than Cv for a gas, which of the following statements provide, partly or wholly, the reason for this ?
(i) No work is done by a gas at constant volume
(ii) I When a gas absorbs heat at constant pressure, its volume must change
(iii) For the same change in temperature, the internal energy of a gas changes by a smaller amount at constant volume than at constant pressure
(iv) The internal energy of an ideal gas is a function only of its temperature
(a) (i), (ii)
(b) (ii), (iii)
(c) (iii), (iv)
(d) all
Ans: (a)
Sol:(a) When heat Q is supplied at constant volume
Q = Qv = ∆U = nCv∆T
When heat Q is supplied at constant pressure
Q = Qp = ∆U’ + ∆W
= n Cv (∆T)’ + ∆W
$\large C_v = \frac{Q}{n \Delta T} $
$\large C_p = \frac{Q}{n \Delta T’} $
(∆T)’ < (∆T) Hence, Cp > Cv