Isochoric Process: Definition, Formulas, and Examples Easily Explained

Isochoric Process: Definition, Formulas, and Examples Easily Explained

An isochoric ( also called isovolumetric) process is a thermodynamic process that takes place at constant volume.

This means that the system does not experience changes in its volume throughout the transformation.

Relationship between pressure and temperature

In an ideal gas, if the volume remains constant, it is true that:

\[ \frac{P}{T} = \text{constant} \]

That is, the pressure is directly proportional to the absolute temperature.

Physical interpretation:
As the temperature increases, the gas particles move faster and collide more frequently and intensely against the walls of the vessel, causing an increase in pressure.

Graphical representation

Isochoric transformations are represented by isochores:

  • In a P–V diagram → vertical line (constant volume)

  • In a P–T diagram → increasing straight line

  • In a V–T diagram → horizontal line

Work in an isochoric process

The work in thermodynamics is given by:

\[ W = P \cdot \Delta V \]

As in this process:

\[ \Delta V = 0 \]

Then:

\[ W = 0 \]

Conclusion:
An isochoric process does not perform mechanical work.

First Law of Thermodynamics

The first law establishes:

\[ \Delta U = Q - W \]

Since there is no work:

\[ \Delta U = Q \]

Interpretation:
All the energy transferred in the form of heat is converted into variation of the internal energy of the system.

Internal energy in an ideal gas

In an ideal gas:

The internal energy depends solely on the temperature.

Therefore, any change in internal energy implies a change in temperature.

Heat in an isochoric process

If the amount of gas remains constant, the heat exchanged is calculated as:

\[ Q = n \cdot C_v \cdot \Delta T \]

where:

  • n = number of moles

  • Cv = molar specific heat at constant volume

  • ΔT = temperature variation

Examples of isochoric processes

Ideal example

A gas contained in a rigid, closed, non-deformable container to which heat is supplied.

Example in applied thermodynamics

In the Otto cycle (ideal model of gasoline engines), there are two isochoric transformations:

  • Heat input (combustion)

  • Heat transfer

Comparison with other processes

Process Constant magnitude Main feature
Isochoric Volume No work (W = 0)
Isothermal Temperature Constant internal energy
Isobaric Pressure Non-Zero Work
Adiabatic Heat (Q = 0) No heat exchange

Final Key Idea

In an isochoric process:

  • Volume does not change

  • No work is done

  • All the heat exchanged is transformed into internal energy

  • Pressure and temperature are directly related

Author:
Publication Date: February 26, 2020
Last Revision: March 17, 2026