B.4.2 (HL)—Gas work
- Syllabus
- First assessment 2025
- Objective
- —
- Level
- HL
Work from pressure and volume
For a constant-pressure change, the work done by the gas is
W=PΔV
Expansion has ΔV>0 and work done by the gas is positive in the first-law convention.
PV interpretation
On a pressure–volume diagram, work is the area under the process path. For constant pressure this is a rectangle; for changing pressure, use the area or integral specified by the model.
Units and direction
Use pressure in pascals and volume in cubic metres so PΔV is in joules. Compression gives ΔV<0, so work done by the gas is negative.
Worked example from the mapped local textbook
A gas expands at constant pressure 1.0×105Pa from 0.020m3 to 0.050m3.
W=PΔV=(1.0×105)(0.050−0.020)=3.0×103J
The work is positive because the gas expands and does work on its surroundings.
Common trap
Do not multiply pressure by the final volume alone. Work depends on the change in volume and on the process path.
The evidence uses direct numerical work calculations from pressure and initial/final volumes.
Calculate
Use W=PΔV for a constant-pressure process with pressure in Pa and volume change in m³. Expansion gives positive work by the gas. On a PV diagram, identify the area under the path and do not use final volume alone.
Using pressure times final volume or mixing kPa and m³ without conversion.
Representative question
Calculate, in J , the work done by the gas during this expansion.
WW=PΔV=11.2×103×(52.7−47.1)=62.7×103 J
Accept 66.1×103 J if 53 used
Accept 61.6×103 J if 52.6 used
Energy accounting
For a closed system, Q=ΔU+W. Gas work is linked to volume change by W=PΔV for constant pressure, and for a monatomic ideal gas ΔU=23nRΔT.
Entropy and direction
Entropy measures accessible microstates: S=kBlnΩ and, for a reversible thermal transfer, ΔS=ΔQ/T. The total entropy of an isolated system does not decrease; real processes are generally irreversible.
Gas processes and engines
Classify isovolumetric, isobaric, isothermal and adiabatic paths by what is fixed. Cyclic paths can run heat engines; net work is the signed PV-loop area.
Efficiency limits
η=QHWuseful=1−QHQC and no real engine can exceed ηC=1−TC/TH. Always state the sign convention, system boundary and reservoir temperatures.