19.2.3 Isothermal Process

FIGURE 19.8 shows an isothermal process. Here we need to know the pressure as a function of volume before we can integrate Equation 19.8. From the ideal-gas law, p=nRT/V. Thus the work on the gas as the volume changes from Vi to Vf is

W=−∫ViVfp dV=−∫ViVfnRTVdV=−nRT∫ViVfdVV (19.11)

where we could take the T outside the integral because temperature is constant during an isothermal process. This is a straightforward integration, giving

W=−nRT∫ViVfdVV=−nRT ln V|ViVf=−nRT(ln Vf−ln Vi)=−nRT ln(VfVi) (19.12)

Because nRT=piVi=pfVf during an isothermal process, the work is:

W=−nRT ln(VfVi)=−piVi ln(VfVi)=−pfVf ln(VfVi)(isothermal process) (19.13)

Which version of Equation 19.13 is easiest to use will depend on the information you’re given. The pressure, volume, and temperature must be in SI units.

FIGURE 19.8 An isothermal process.

The figure illustrates a pressure versus volume graph.
FIGURE 19.8 Full Alternative Text

EXAMPLE 19.2 The work of an isothermal compression

A cylinder contains 7.0 g of nitrogen gas. How much work must be done to compress the gas at a constant temperature of 80°C until the volume is halved?

MODEL This is an isothermal ideal-gas process.

SOLVE Nitrogen gas is N2, with molar mass Mmol = 0.028 kg/mol=28 g/mol, so 7.0 g is 0.25 mol of gas. The temperature is T=353 K. Although we don’t know the actual volume, we do know that Vf=12Vi. The volume ratio is all we need to calculate the work:

W=−nRT ln(VfVi)=−(0.25 mol)(8.31 J/mol K)(353 K)ln(1/2)=508 J

REVIEW The work is positive because a force from the environment pushes the piston inward to compress the gas.