System boundary and work signs
A closed system exchanges energy but not mass. Here Q is positive into the gas; W is positive for work by the gas. Expansion gives positive boundary work; compression gives negative boundary work.
Check yourself: Which transfers cross the boundary, and which direction is positive?
State properties and the ideal-gas model
The ideal-gas equation pV = mRT uses absolute pressure and temperature. Ideal gases are compressible; do not impose constant density. Their internal energy depends only on temperature; heat and work depend on the path.
Check yourself: Have you confused a property difference with an energy transfer?
First-law accounting
With negligible kinetic and potential energy changes, ΔU = Q − W. Boundary work integrates resisting pressure over volume change. A quasistatic frictionless piston balances gas and resisting pressures.
Check yourself: Does the stated process justify using a constant pressure in W = pΔV?
Heat capacities and process constraints
For an ideal gas with constant specific heats, ΔU = m cᵥ ΔT and cₚ = cᵥ + R. For this model, constant-pressure heating with only boundary work gives Q = m cₚ ΔT. A rigid boundary instead eliminates displacement work, not necessarily every possible work mode.
Check yourself: Are there any shaft or electrical work transfers left after fixing the volume?
Adiabatic versus isothermal
Adiabatic means Q = 0; isothermal means constant temperature. Neither implies the other. Reversible adiabatic ideal-gas relations additionally need reversibility and an appropriate heat-capacity model; conservation alone is insufficient.
Check yourself: Which assumption supplies each process relation you intend to use?