Thermodynamic Processes

01Thermodynamic Processes

Constant pressure

This section covers constant-pressure changes, work done, their p–V representation and application of the first law.

Non-flow processes

In a non-flow process, gas does not flow across the boundary of the system, so the system is closed. The gas is treated as ideal and obeys

pV=nRTpV=nRT

For an ideal gas, intermolecular forces are neglected. There is therefore no intermolecular potential-energy contribution to the internal energy, so changes in internal energy are associated with changes in molecular kinetic energy and temperature.

Constant pressure change

A constant-pressure process is also called an isobaric process. The pressure remains unchanged while the volume and temperature can change.

Heating a gas at constant pressure causes it to expand. Its volume and temperature increase, and the gas does positive work on its surroundings.

Cooling at constant pressure causes the volume and temperature to decrease, so work is done on the gas.

On a ppVV diagram, a constant-pressure change is represented by a horizontal line.

Vpp= constantV1V2

Work and the first law

For a volume change ΔV\Delta V at constant pressure pp, the work done by the system is

W=pΔVW=p\Delta V

Using Q=ΔU+WQ=\Delta U+W gives

Q=ΔU+pΔVQ=\Delta U+p\Delta V
Change ΔV\Delta V WW Temperature
Heating and expansion Positive Positive Increases
Cooling and compression Negative Negative Decreases

Exam Tip: At constant pressure, calculate ΔV\Delta V as final volume minus initial volume. This automatically gives the correct sign for W=pΔVW=p\Delta V.

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