⚛ Physics LabThermodynamics · v0.31 beta

THERMODYNAMICS · IDEAL GASES

Thermodynamic Transformations and the First Law

Follow an ideal gas through a reversible isothermal, isobaric, isochoric or adiabatic transformation. Explore pressure, volume, temperature, work, heat, internal energy and entropy.

Physical Parameters

mol
K
m³
m³
K
dimensionless
m²
s

The process is quasi-static and reversible, with equilibrium at every stage. Duration parametrizes the path; it does not represent a measured process rate.

Examples: Isothermal: expansion · Isothermal: compression · Isobaric: heating · Isochoric: heating · Adiabatic: expansion · Adiabatic: compression · Monatomic gas · Isochoric: cooling

Simulation: Cylinder and Piston

The cylinder dimensions are to scale: width and height use the same metric scale. The gas is modeled as an ideal system in equilibrium.

Volume V—
Pressure p—
Temperature T—
Work W (by the gas)—
Heat Q (to the gas)—
Internal Energy Change ΔU—
Entropy Change ΔS—
Residual Q − W − ΔU—

First law: ΔU = Q − W. Work W is positive when the gas expands.

Synchronized Graphs

The first graph is a pressure–volume (p–V) state diagram; the others show evolution along the path. Select a point or enter an exact time.

Selected Time: 0 s

p–V Diagram: Reversible Path

● Start ● End ● Selected State

Pressure vs. Time

Temperature vs. Time

First Law: Q, W, ΔU vs. Time

● W (work by gas) ● Q (heat to gas) ● ΔU (internal energy)

Entropy Change vs. Time

Data Table

Model Assumptions and Limitations

Ideal gas with constant heat capacities and amount of substance undergoing a quasi-static, reversible process.

Gas pressure and external pressure differ only infinitesimally along the path: this is not a rapid compression, shock wave or irreversible transformation.

Reversible heat exchange requires a thermal environment that follows the gas temperature. The animation time does not determine an actual heat flow rate.

No frictional losses, chemical reactions or phase changes.

THERMODYNAMICS EXPLAINED

Step-by-Step Calculations

by Andrea Minini