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Topic: Finding Work for Reversible Adiabatic Expansions  (Read 7536 times)

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Offline emeraldcrystal

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Finding Work for Reversible Adiabatic Expansions
« on: January 25, 2009, 01:05:08 AM »

Offline Donaldson Tan

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Re: Finding Work for Reversible Adiabatic Expansions
« Reply #1 on: January 26, 2009, 10:09:32 AM »
Work done by the gas
= integration from Vinitial to Vfinal P dV
= integration from Vinitial to Vfinal {nRT/V} dV

This is an isoentropic process involving a perfect gas,
=> PVγ = Constant
=> Given that P = nRT/V, then (nRT/V)Vγ = Constant
=> TVγ-1 = Constant/nR = Constant K for a fixed mass of gas.
=> T = K/Vγ-1

K = TinitialVinitialγ-1

Hence, work done by gas
= integration from Vinitial to Vfinal {nRT/V} dV
= integration from Vinitial to Vfinal (nR/V)*(K/Vγ-1) dV
= integration from Vinitial to Vfinal (nRK/Vγ) dV
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Offline listerineman

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Re: Finding Work for Reversible Adiabatic Expansions
« Reply #2 on: February 02, 2010, 11:20:13 PM »
But doesn't that equation for work only apply to an isothermal process? This equation is for a constant temperature.
= integration from Vinitial to Vfinal {nRT/V} dV

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