Question:

For an ideal gas undergoing an isothermal change, there is:

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For an ideal gas: Isothermal = Constant Temperature = Zero Internal Energy Change ($\Delta U = 0$). According to the first law, this simplifies the energy balance to $\Delta Q = \Delta W$, meaning any heat absorbed must be completely converted into work performed by the system.
Updated On: May 20, 2026
  • a decrease in Internal energy of the system and heat released by the system is equal to the work done by the system
  • an increase in Internal energy of the system and heat absorbed by the system is greater than the work done on the system
  • no change in Internal energy of the system and heat released by the system is equal to the work done by the system
  • no change in Internal energy of the system and heat absorbed by the system is equal to the work done by the system
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The Correct Option is D

Solution and Explanation


Concept: The internal energy ($U$) of an ideal gas depends solely on its absolute temperature ($U \propto T$). According to the First Law of Thermodynamics, the total energy balance in a closed system must satisfy the equation: \[ \Delta Q = \Delta U + \Delta W \] where $\Delta Q$ is heat absorbed, $\Delta U$ is internal energy change, and $\Delta W$ is work done by the system.

Step 1:
Analyze the internal energy change ($\Delta U$).
An isothermal process occurs at a constant temperature ($\Delta T = 0$). Because the temperature of the ideal gas remains fixed, its internal energy cannot change: \[ \Delta U = 0 \]

Step 2:
Apply the first law energy balance to determine work and heat tracking.
Substituting $\Delta U = 0$ into the thermodynamic balance equation gives: \[ \Delta Q = 0 + \Delta W \implies \Delta Q = \Delta W \] This shows that any heat energy absorbed by the gas system ($\Delta Q > 0$) is completely transformed into mechanical work performed by the gas on its surroundings ($\Delta W > 0$). This matches statement (D) perfectly.
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