We know that the work done by any thermodynamic process is, in general, found by the relation: W =- -SVP dv Using the ideal gas law (PV = nRT), derive relations for the amount of work done in a system during each of the processes listed below. You may assume a closed system, i.e. n is constant for all processes.

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Find the work for a system where temperature (T) is constant. (This is called an isothermal process)
W = P(V₂ - Vf)
W = 0
(V)
W = P(V₁ - V₂)
W = PV
W = - PV)
W = -nRT
W = nRT
W = nRT In
W
n(V)
= nRT In
Transcribed Image Text:Find the work for a system where temperature (T) is constant. (This is called an isothermal process) W = P(V₂ - Vf) W = 0 (V) W = P(V₁ - V₂) W = PV W = - PV) W = -nRT W = nRT W = nRT In W n(V) = nRT In
We know that the work done by any thermodynamic process is, in general, found by the relation:
-S¹P dv
W = -
Using the ideal gas law (PV = nRT), derive relations for the amount of work done in a system during each of the processes listed below. You may assume a closed system, i.e.n is
constant for all processes.
Transcribed Image Text:We know that the work done by any thermodynamic process is, in general, found by the relation: -S¹P dv W = - Using the ideal gas law (PV = nRT), derive relations for the amount of work done in a system during each of the processes listed below. You may assume a closed system, i.e.n is constant for all processes.
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