As with mechanics problems, every thermodynamics problem can be represented with a bubble diagram: one bubble for each type of energy, with the initial (state A) and final (state B) values written inside, and arrows indicating the transfers.

Bubble = type of energy. Arrow = transfer.

In the thermodynamic case the typical bubbles are: the internal energy of the gas Eint,gas=f2nRTE_\text{int,gas} = \frac{f}{2}nRT, the thermal energy of any second body or thermostat EtermE_\text{term}, the energy of the atmosphere EatmE_\text{atm} and the mechanical energy EmeccE_\text{mecc} of weights or machines. The arrows are the three exchanges of the first law: heat QQ to a thermostat, work LgasL_\text{gas} to mechanical parts, work LatmL_\text{atm} to the atmosphere.

Exchange diagram for a thermodynamics problem. The gas exchanges heat QQ with the thermostat, work LgasL_\text{gas} with mechanical parts (weights, machines) and work LatmL_\text{atm} with the atmosphere. The total energy of the system is conserved.

The advantage of the diagram is the same as in mechanics: it makes visible at a glance which exchanges are present and which are zero. In the three typical problems that follow, the strategy is always to zero out the arrows that are absent (for example Lgas=0L_\text{gas}=0 at constant volume, Q=0Q=0 in an insulated container) and keep only the relevant terms.

Connections

Topics: Termodinamica Concepts: Primo principio della termodinamica · Energia interna Skills: Bilancio energetico a bolle Methods: Diagramma a bolle di scambio energetico Objects: Gas ideale

Related exercises: Nitrogen heated in a rigid cylinder · Heating under the piston · Heat as a substance?