Thermodynamic Processes

Learn about isothermal, adiabatic, isobaric and isochoric processes in an easy and clear way.

1. What Is a Thermodynamic Process?

A thermodynamic process is any change that takes a system from one state to another. During a process, one or more state variables like pressure, volume, or temperature change.

The nature of a process depends on which quantities are kept constant and how the system interacts with the surroundings.

2. Quasi-Static Process (Slow Process)

A quasi-static process is one that happens extremely slowly so the system stays in near-equilibrium at every stage. It is an idealised process but helps us calculate work and other quantities accurately.

2.1. Why Quasi-Static is Important

Most thermodynamic equations assume a quasi-static process. This ensures pressure and temperature are well-defined at every instant.

3. Isothermal Process

An isothermal process is one in which temperature remains constant throughout (\( \Delta T = 0 \)). Heat flows in or out to maintain the temperature during expansion or compression.

3.1. Key Features

  • Temperature is constant.
  • Internal energy remains constant for an ideal gas.
  • Work done is higher compared to adiabatic expansion.

3.2. Equation for Isothermal Expansion

\( PV = \text{constant} \)

\( W = nRT \ln \left( \dfrac{V_2}{V_1} \right) \)

4. Adiabatic Process

An adiabatic process is one in which no heat is exchanged with the surroundings (\( \Delta Q = 0 \)). Any change in internal energy comes only from work done.

4.1. Key Features

  • No heat enters or leaves the system.
  • Temperature changes during the process.
  • Expansion cools the gas; compression heats it.

4.2. Equation for Adiabatic Process

\( PV^{\gamma} = \text{constant} \)

Where \( \gamma = \dfrac{C_p}{C_v} \).

5. Isobaric Process

An isobaric process is a process in which pressure remains constant (\( P = \text{constant} \)).

This often occurs when a gas is heated or cooled while the piston can freely move.

5.1. Key Features

  • Pressure stays constant.
  • Heat supplied does both work and increases internal energy.

5.2. Work Done in Isobaric Process

\( W = P (V_2 - V_1) \)

6. Isochoric (Isovolumetric) Process

An isochoric process is one in which the volume remains constant (\( V = \text{constant} \)).

Since the volume does not change, no work is done (\( W = 0 \)).

6.1. Key Features

  • Volume remains fixed.
  • All heat added goes into increasing internal energy.
  • Often happens in closed, rigid containers.

6.2. Relation in Isochoric Process

\( \Delta Q = \Delta U \)

7. Reversible and Irreversible Processes

Real processes are usually irreversible due to friction, turbulence, or rapid changes. Reversible processes are ideal and happen infinitely slowly.

7.1. Reversible Process

A reversible process can be reversed by an infinitesimal change in a variable. It is quasi-static and involves no losses.

7.2. Irreversible Process

An irreversible process happens quickly, involves heat losses, and cannot be exactly reversed. Most real-life processes fall into this category.

8. Examples of Thermodynamic Processes in Daily Life

  • Air in a bicycle pump gets hotter during compression (adiabatic).
  • Boiling water at constant pressure (isobaric).
  • Gas heating in a rigid container (isochoric).
  • Melting ice-water system maintained at constant temperature (isothermal).