Question:

\(∆U^Θ\) of combustion of methane is – \(X\ kJ \ mol^{–1}\). The value of \(∆H^Θ\) is

Updated On: Jan 20, 2026
  • \(= ∆U^Θ\)
  • \(>∆U^Θ\)
  • \(<∆U^Θ\)
  • \(=0\)
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The Correct Option is C

Solution and Explanation

The given problem is about finding the relationship between the change in internal energy (\(∆U^Θ\)) and the change in enthalpy (\(∆H^Θ\)) for the combustion of methane. Understanding these thermodynamic concepts is crucial:

  1. In thermodynamics, the relationship between the change in enthalpy (\(∆H\)) and the change in internal energy (\(∆U\)) is given by: \(∆H = ∆U + ∆n_gRT\), where \(\Delta n_g\) represents the change in the number of moles of gas, \(R\) is the universal gas constant, and \(T\) is the temperature in Kelvin.
  2. For the combustion of methane (\(CH_4\)), the balanced chemical reaction is: \(CH_4 (g) + 2O_2 (g) \rightarrow CO_2 (g) + 2H_2O (l)\).
  3. Count the gaseous molecules involved:
    • In reactants: 1 mole of CH4 + 2 moles of O2 = 3 moles of gas.
    • In products: 1 mole of CO2 = 1 mole of gas.
  4. The change in the number of moles of gas, \(∆n_g\), is calculated as: \(∆n_g = \text{moles of gaseous products} - \text{moles of gaseous reactants} = 1 - 3 = -2\).
  5. Given \(∆n_g\) is negative, this implies a decrease in the number of gaseous moles during the reaction.
  6. Substitute \(∆n_g\) in the formula: \(∆H = ∆U + (-2)RT\).
  7. Since \(RT\) is positive (as \(R\) and \(T\) are positive constants), the term \(-2RT\) will reduce the value of \(∆H\), making \(∆H\) less than \(∆U\).
  8. Therefore, the correct relationship is: \(∆H^Θ < ∆U^Θ\).

Thus, the correct answer is \(<∆U^Θ\).

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Concepts Used:

Thermodynamics

Thermodynamics in physics is a branch that deals with heat, work and temperature, and their relation to energy, radiation and physical properties of matter.

Important Terms

System

A thermodynamic system is a specific portion of matter with a definite boundary on which our attention is focused. The system boundary may be real or imaginary, fixed or deformable.

There are three types of systems:

  • Isolated System – An isolated system cannot exchange both energy and mass with its surroundings. The universe is considered an isolated system.
  • Closed System – Across the boundary of the closed system, the transfer of energy takes place but the transfer of mass doesn’t take place. Refrigerators and compression of gas in the piston-cylinder assembly are examples of closed systems.
  • Open System – In an open system, the mass and energy both may be transferred between the system and surroundings. A steam turbine is an example of an open system.

Thermodynamic Process

A system undergoes a thermodynamic process when there is some energetic change within the system that is associated with changes in pressure, volume and internal energy.

There are four types of thermodynamic process that have their unique properties, and they are:

  • Adiabatic Process – A process in which no heat transfer takes place.
  • Isochoric Process – A thermodynamic process taking place at constant volume is known as the isochoric process.
  • Isobaric Process – A process in which no change in pressure occurs.
  • Isothermal Process – A process in which no change in temperature occurs.

Laws of Thermodynamics

Zeroth Law of Thermodynamics

The Zeroth law of thermodynamics states that if two bodies are individually in equilibrium with a separate third body, then the first two bodies are also in thermal equilibrium with each other.

First Law of Thermodynamics 

The First law of thermodynamics is a version of the law of conservation of energy, adapted for thermodynamic processes, distinguishing three kinds of transfer of energy, as heat, as thermodynamic work, and as energy associated with matter transfer, and relating them to a function of a body's state, called internal energy.

Second Law of Thermodynamics 

The Second law of thermodynamics is a physical law of thermodynamics about heat and loss in its conversion.

Third Law of Thermodynamics

Third law of thermodynamics states, regarding the properties of closed systems in thermodynamic equilibrium: The entropy of a system approaches a constant value when its temperature approaches absolute zero.