In more general problems the gas can push weights, springs or other bodies. In every case the first law is the same: every form of energy (kinetic energy of a weight, elastic energy of a spring, gravitational potential energy, thermal energy of a second body) enters the balance.
The typical set-up is a vertical cylinder with a piston of mass and area . The gas pressure is constant because the piston is in mechanical equilibrium at every instant: the weight of the piston adds to the push of the atmosphere.
When the gas receives heat and lifts the piston by , the energy balance of the gas includes three “outflows” for work:
- lifting the piston: ;
- work against the atmosphere: ;
- the increase in internal energy of the gas: .
Balance with a heavy piston
with the geometric constraint and the equation of state .
The two auxiliary conditions (geometric constraint and equation of state) close the system: they allow , and to be linked and hence the required unknown to be solved for.
In this chapter we have seen that energy conservation alone (with the work of the atmosphere included) allows a great variety of irreversible thermodynamic problems to be solved: the gas expands abruptly, two bodies reach thermal equilibrium, the piston rises — all without ever imagining a path on the - diagram. But questions remain that the first law cannot answer: why does heat always flow from hot to cold? Which transformations are reversible? To answer these a new quantity is needed, entropy.
A quantitative case (a vertical piston being lifted) is worked out in Lifting a vertical piston.
Links
Topics: Thermodynamics Concepts: First law of thermodynamics · Internal energy · Gravitational potential energy Skills: Bubble energy balance Objects: Ideal gas · Piston and cylinder
Related exercises: Nitrogen heated in a rigid cylinder · Lifting a vertical piston · Heating under the piston