Deepak Patra
Sol. P base 1 = Initial Pressure V base 1 = Initial Volume P base 2 = Final Pressure V base 2 = Final Volume
Given, V base 2 = 2V base 1, Isothermal workdone = nRT base 1 Ln(V base 2/V base 1)
Adiabatic workdone = P base 1V base 1 – P base 2V base 2/γ – 1
Given that workdone in both cases is same
Hence nRT base 1 Ln (V base 2/V base 1) = P base 1V base 1 – P base 2V base 2/γ – 1 ⇒ (γ – 1) In (V base 2/V base 1) = P base 1V base 1 – P base 2V base 2/nRT base 1
⇒ (γ – 1) In (V base 2/V base 1) = nRT base 1 – nRT base 2/nRT base 1 ⇒ (γ – 1) In 2 = T base 1 – T base 1/T base 1 …(i) [∴V base 2/2V base 1]
We know TV^ γ – 1 = const. in adiabatic Process.
T base 1V base 1^γ – 1 = T base 2V base 2^γ – 1, or T base 1 (V base 1)^γ – 1 = T base 2 * (2)^γ – 1 * (V base 1)^γ – 1
Or, T base 1 = 2^γ – 1 or T base 2 or T base 2 = T base 1^1-γ …(ii)
From (i) & (ii)
(γ – 1) In 2 = T base 1 – T base 1 * 2^1-γ/T base 1 ⇒ (γ – 1) In2 = 1 – 2^1-γ