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One litre of hydrogen at 27°C and 106 dyne cm-2 pressure expands isothermally until its volume in doubled and then adiabatically until redoubled. Find the final temperature, pressure and work done in each case, γ = 1.4.

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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.

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