Question:

A solid body of constant heat capacity $1 \,J/?C$ is being heated by keeping it in contact with reservoirs in two ways : (i) Sequentially keeping in contact with $2$ reservoirs such that each reservoir supplies same amount of heat. (ii) Sequentially keeping in contact with $8$ reservoirs such that each reservoir supplies same amount of heat. In both the cases body is brought from initial temperature $100^{\circ}C$ to final temperature $200^{\circ}C$. Entropy change of the body in the two cases respectively is :

Updated On: Aug 4, 2024
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  • 2 ln 2, 8 ln 2
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  • ln 2, ln 2
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The Correct Option is D

Solution and Explanation

The entropy change from State $A$ to $B$ is given by
$\Delta S ^{\circ}=\int\limits_{ A }^{ B } \frac{ d Q }{ T } \ldots$ (i)
where $dQ$ is heat supplied in $J$ to the body and temperature is in $K$
$T _{ A }=273+100 \,K =373 \,K$;
$T _{ B }=273+200=473 \,K$
$dQ = C dT$
where $C$ is heat capacity of body and $dT$ is increase in temperature in $C ^{\circ}$
Substituting $T'= T -273$ in equation (i)
where $T'$ is temperature in $C ^{\circ}$ and $T$ is in kelvin.
$dT'= dT$
integration limits: $T _{ A }'=373-273=100 C ^{\circ} $
$; T _{ B }'=473-273=200 \,C ^{\circ}$
$\Delta S^{\circ}=\int\limits_{100}^{200} \frac{C d T'}{T'+273}=\ln \left(\frac{473}{373}\right)$
As the heat transferred is same the entropy change will be same in both the cases
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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.