Question:

For irreversible expansion of an ideal gas under isothermal condition, the correct option is

Updated On: Nov 13, 2025
  • ∆U≠0, ∆Stotal=0

  • ∆U=0, ∆Stotal=0

  • ∆U≠0, ∆Stotal≠0

  • ∆U=0, ∆Stotal≠0

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The Correct Option is D

Solution and Explanation

To solve the question about the irreversible expansion of an ideal gas under isothermal conditions, let's consider the thermodynamic principles involved.

Concept Explanation: 

  • Isothermal Process: In an isothermal process, the temperature (T) of the system remains constant. For an ideal gas, the internal energy (U) depends only on temperature. Therefore, if the temperature doesn't change, the internal energy remains constant, i.e., \(\Delta U = 0\).
  • Irreversible Process: In an irreversible process, the system is not in equilibrium, and entropy is produced. This means that the total change in entropy of the universe (\( \Delta S_{\text{total}} \)) is greater than zero for irreversible processes.

Analysis of Options:

  1. \(\Delta U \neq 0, \Delta S_{\text{total}} = 0\): This is incorrect because for an isothermal process involving an ideal gas, \(\Delta U = 0\). Also, \(\Delta S_{\text{total}} = 0\) cannot be correct for an irreversible process.
  2. \(\Delta U = 0, \Delta S_{\text{total}} = 0\): This is incorrect. While \(\Delta U = 0\) is correct for an isothermal process, \(\Delta S_{\text{total}} = 0\) is true only for reversible processes, not irreversible ones.
  3. \(\Delta U \neq 0, \Delta S_{\text{total}} \neq 0\): This is incorrect because for an isothermal process of an ideal gas, \(\Delta U\) should be zero.
  4. \(\Delta U = 0, \Delta S_{\text{total}} \neq 0\): This is the correct option. In an isothermal, irreversible expansion of an ideal gas, \(\Delta U = 0\) because the temperature is constant, and \(\Delta S_{\text{total}} \neq 0\) because entropy increases in an irreversible process.

Conclusion: Therefore, the correct answer is \(\Delta U = 0, \Delta S_{\text{total}} \neq 0\), which is option D.

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Concepts Used:

Behaviour of Real Gases

Real gases are gases that do not follow the ideal gas law, which assumes that gas particles have negligible volume and no intermolecular forces. In reality, gas particles do have volume and interact with each other, leading to deviations from ideal gas behavior.

The behavior of real gases can be described using various gas laws, such as the van der Waals equation and the virial equation. These equations take into account the effects of gas particle size and intermolecular forces on gas behavior.

One important property of real gases is compressibility. Real gases are more compressible than ideal gases, meaning that they can be compressed to a smaller volume at the same pressure. This is due to the fact that gas particles occupy a finite amount of space and are subject to intermolecular forces that can cause them to come closer together.

Also Read: Derivation from Ideal Gas Behavior

Another property of real gases is that their behavior is strongly affected by temperature and pressure. At high pressures and low temperatures, real gases tend to deviate more from ideal gas behavior. This is because the intermolecular forces become stronger and the gas particles are closer together.

Real gases also exhibit a phenomenon called condensation, where gas particles condense into a liquid or solid state when cooled or compressed sufficiently. This is due to the fact that the intermolecular forces become strong enough to overcome the kinetic energy of the gas particles, causing them to condense into a denser state.

Overall, the behavior of real gases is complex and influenced by various factors such as temperature, pressure, and intermolecular forces. Understanding the behavior of real gases is important in many scientific and industrial applications, such as in chemical reactions, power generation, and refrigeration.