Question:

A given quantity of gas is taken from A to C in two ways; a) directly from A\(\rightarrow\)C along a straight line and b) in two steps, from A\(\rightarrow\)B and then from B\(\rightarrow\)C.Work done and heat absorbed along the direct path A\(\rightarrow\)C are 200J and 280J respectively. If the work done along A\(\rightarrow\)B\(\rightarrow\)C is 80J, then heat absorbed along the path is,
A given quantity of gas is taken from A to C

Updated On: Mar 13, 2025
  • 80J
  • 0
  • 160J
  • 120J
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The Correct Option is C

Approach Solution - 1

While moving along path AC, the change in internal energy (dU) is determined by the difference between heat (dQ) added to the system and work (dW) done by the system. In this case, dU=dQdW=300−200=100J. This illustrates that internal energy is a point function, which means it remains consistent across all paths.

Along path ABC, the heat (dQ) is the sum of the change in internal energy (dU) and the work (dW) done on the system. 

The correct option is(C) 160J

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Approach Solution -2

To determine the heat absorbed along the path A → B → C, let's break down the solution step by step:
 Given Data:
1. Work done along the direct path A → C (\(W_{AC}\)) = 200 J
2. Heat absorbed along the direct path A → C (\(Q_{AC}\)) = 280 J
3. Work done along the path A → B → C (\(W_{ABC}\)) = 80 J
Using the first law of thermodynamics for the direct path A → C:
\[ \Delta U = Q_{AC} - W_{AC} \]
Substituting the given values:
\[ \Delta U = 280 \, \text{J} - 200 \, \text{J} = 80 \, \text{J} \]
This change in internal energy (\(\Delta U\)) is the same for both paths A → C and A → B → C since internal energy is a state function and depends only on the initial and final states, not on the path taken.
Calculating Heat Absorbed Along Path A → B → C:
Using the first law of thermodynamics again for the path A → B → C:
\[ \Delta U = Q_{ABC} - W_{ABC} \]
We know \(\Delta U\) (from the direct path A → C) and \(W_{ABC}\):
\[ 80 \, \text{J} = Q_{ABC} - 80 \, \text{J} \]
Solving for \(Q_{ABC}\):
\[ Q_{ABC} = 80 \, \text{J} + 80 \, \text{J} = 160 \, \text{J} \]
Conclusion:
The heat absorbed along the path A → B → C is 160 J.
Therefore, the correct option is (C) 160 J.
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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.