During a reversible adiabatic expansion of an ideal gas, the pressure
and volume at any moment are related by PVγ = c where c and γ are
constants. Show that the work done by the gas in expanding from a
state (P1, V1) to a state (P2, V2) is
W PV P V = −
−
1 1 2 2
γ 1
"pV^{\\gamma} = \\text{const} \\; \\Rightarrow p_1V_1^{\\gamma} = p_2V_2^{\\gamma}"
For the ideal gas "pV = \\nu R T."
The work done by the gas is
"w = \\int\\limits_{V_1}^{V_2}p\\,dV = \\int\\limits_{V_1}^{V_2}\\dfrac{\\text{const}}{V^{\\gamma}}\\,dV =- \\text{const}\\cdot\\dfrac{1}{\\gamma-1}\\cdot \\dfrac{1}{V^{\\gamma-1}}\\Big |_{V_1}^{V_2} = \\text{const}\\cdot\\dfrac{1}{1-\\gamma}\\cdot \\left(\\dfrac{1}{V_2^{\\gamma-1}} - \\dfrac{1}{V_1^{\\gamma-1}} \\right) = \\Big| \\text{const} = p_1V_1^{\\gamma} = p_2V_2^{\\gamma} \\Big| = \\dfrac{1}{1-\\gamma}\\cdot \\left(\\dfrac{p_2V_2^{\\gamma}}{V_2^{\\gamma-1}} - \\dfrac{p_1V_1^{\\gamma}}{V_1^{\\gamma-1}} \\right) = \\dfrac{1}{1-\\gamma}\\cdot \\left(p_2V_2 - p_1V_1 \\right)"
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