Derive expression for Joule’s Coefficient.

Website can be closed on 12th to 14th Jan 2025 due to server maintainance work.


Joule’s coefficient (or Joule-Thomson coefficient) measures the change in temperature of a gas when it expands or is compressed at constant enthalpy. It is a critical concept in thermodynamics, especially in refrigeration and air conditioning. Understanding Joule’s coefficient helps predict how gases behave under varying pressure and temperature conditions during expansion or compression processes. This assignment will derive the expression for Joule’s coefficient, explaining its significance and applications.


The Joule-Thomson coefficient (μ) is defined as the rate of change of temperature (T) with respect to pressure (P) during a throttling process at constant enthalpy (H). Mathematically, it is expressed as:

μ = (∂T/∂P)H

  • Refrigeration and Air Conditioning: Joule’s coefficient is vital for understanding the cooling effect produced during the expansion of refrigerants.
  • Natural Gas Processing: It assists in designing processes for natural gas extraction and processing by predicting temperature changes during pressure changes.

To derive the expression for Joule’s coefficient, we start from the first law of thermodynamics and the concept of enthalpy.

The first law states that the change in internal energy (dU) is equal to the heat added to the system (dQ) minus the work done by the system (dW):

dU = dQ – dW

Enthalpy (H) is defined as:

H = U + PV

Differentiating this gives:

dH = dU + d(PV)

Using the product rule, we have:

d(PV) = PdV + VdP

Substituting this back into the enthalpy equation gives:

dH = dU + PdV + VdP

From the first law, we know:

dU = dQ – dW

For an ideal gas undergoing a throttling process, we assume no heat exchange with the surroundings, so dQ = 0 and:

dU = -dW

In this case, dW = PdV, so we rewrite dU as:

dU = -PdV

Now we can substitute dU back into the equation for dH:

dH = -PdV + PdV + VdP = VdP

Since we consider a process at constant enthalpy (dH = 0):

0 = VdP

This indicates that during the throttling process, pressure changes occur without changing enthalpy.

To express the relationship between temperature and pressure, we can use the Maxwell relation, which links changes in enthalpy with pressure and temperature for an ideal gas. The following relationship holds for an ideal gas:

dH = Cp dT

Thus, we have:

Cp dT = VdP

Dividing both sides by dP gives:

(dT/dP) = V/Cp

Now, we can write the expression for the Joule-Thomson coefficient as:

μ = (∂T/∂P)H = V/Cp

This expression indicates that the Joule-Thomson coefficient is directly related to the specific volume of the gas and inversely related to its heat capacity at constant pressure.


  1. Cooling Effect: For gases with a positive Joule-Thomson coefficient, expansion leads to cooling, making them suitable for refrigeration applications.
  2. Heating Effect: For gases with a negative coefficient, expansion results in heating, which must be managed in various industrial processes.
  3. Applications in Natural Gas: Understanding Joule’s coefficient is crucial for processing natural gas, as it helps predict how the gas will behave under pressure changes.
  4. Thermodynamic Processes: Joule’s coefficient is essential in analyzing various thermodynamic processes, including throttling processes in turbines and compressors.

Joule’s coefficient is a fundamental concept in thermodynamics that quantifies the temperature change of a gas during expansion or compression at constant enthalpy. By deriving the expression for the Joule-Thomson coefficient, we gain insights into gas behavior during throttling processes and its implications in refrigeration, air conditioning, and other industrial applications. Understanding this coefficient is essential for engineers and scientists working with gases and designing systems that rely on their thermodynamic properties.


  1. Cengel, Y. A., & Boles, M. A. (2015). Thermodynamics: An Engineering Approach. McGraw-Hill Education.
  2. Sonntag, C. E., & Borgnakke, C. (2013). Introduction to Thermal Systems Engineering: Thermodynamics, Fluid Mechanics, and Heat Transfer. Wiley.
  3. Moran, M. J., & Shapiro, H. N. (2006). Fundamentals of Engineering Thermodynamics. Wiley.

Leave a Comment

Your email address will not be published. Required fields are marked *

Scroll to Top