Given :
P1 = 106 dyne cm-2
V1 = 103 cm3 = 1 litre
T1 = 27°C = 300 K
V2 = 2V1 = 2000 cm3 for isothermal expansion
T2 = ?
For adiabatic expansion P2 = ?
V1' = 2000 cm3
V2' = 21' = 4000 cm3
(a) For isothermal expansion :
P2V2 = P1V1
or P2 = \(\frac{P_1V_1}{V_2}\)
= \(\frac{10^6\times10^3}{2\times10^3}\)
= 5 × 105 dyne cm-2
T2 = T1 for isothermal expansion = 300 K = 27°C Work done during isothermal expansion is given by
Wiso = 2.303 RT log10 \((\frac{V_2}{V_1})\)
or Wiso = 2.303 P1V1 log10\((\frac{V_2}{V_1})\) \((\frac{V_2}{V_1})\)
or Wiso = 2.303 × 106 × 103log10
or Wiso = 2.303 × 109 × 0.3010
or Wiso = 6.93 × 108 erg.
(b) For adiabatic expansion:
P2 = P1\((\frac{V_1'}{V_2'})^γ\)
= 106\((\frac{2000}{4000})^{1.4}\)
or P2 = 106 ×\((\frac{1}{2})^{1.4}\)
or P2 = 1.895 × 105 dyne cm-2
From relation T1V1γ−1 = 22γ−1, we get
T2 = T1\((\frac{V_1}{V_2})^{γ-1}\)
= 300 \((\frac{1}{2})^{1.4}\)
= 227.4K = −45.6°C
Work done during adiabatic expansion is given by
Wadi = (T1 − T2 )\(\frac{R}{1-γ}\)
\(= \frac{P_1V_1-P_2V_2}{γ-1}\)
\(= \frac{10^6\times2\times10^3-1.895\times10^5\times4\times10^3}{1.4-1}\)
or Wadi = \( \frac{20\times10^8-1.895\times4\times10^8}{0.4}\)
or Wadi = 31.05 × 108 erg.