2.7
An ideal gas obeys the equation pV = nRT, with its internal energy solely dependent on temperature.
To connect this molecular picture to experimental setups, consider the same gas contained in a cylinder with a movable piston placed within a constant-temperature bath.
Reducing the external pressure slowly expands the gas, slightly lowering the temperature. As a result, heat is transferred from the bath into the gas, maintaining a constant temperature.
In this reversible isothermal expansion, the internal energy change is zero, meaning heat equals work done.
Substituting the equation of state, which is the general relationship among pressure, volume, and temperature, into the pressure–volume work expression and integrating it relates the work done to the volume changes during an isothermal reversible expansion.
For adiabatic expansion, where no heat is transferred, the work done equals the internal energy change.
If expansion is reversible, equating work and internal energy and substituting the ideal gas relation for pressure, links the temperature and volume changes.
Integrating this equation and rearranging it relates the initial and final temperature and volumes of the gas.
A perfect gas obeys the equation of state pV = nRT. The internal energy of a perfect gas remains unaffected by volume alterations. Therefore, the inte…
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