Question:

As shown schematically in the figure, two vessels contain water solutions (at temperature $T$ ) of potassium permanganate $\left( KMnO _{4}\right)$ of different concentrations $n _{1}$ and $n _{2}\left( n _{1} > n _{2}\right)$ molecules per unit volume with $\Delta n =\left( n _{1}- n _{2}\right) < < n _{1}$. When they are connected by a tube of small length $\ell$ and cross-sectional area $S , KMnO _{4}$ starts to diffuse from the left to the right vessel through the tube. Consider the collection of molecules to behave as dilute ideal gases and the difference in their partial pressure in the two vessels causing the diffusion. The speed $v$ of the molecules is limited by the viscous force $-\beta v$ on each molecule, where $\beta$ is a constant. Neglecting all terms of the order $(\Delta n )^{2}$, which of the following is/are correct? ( $k_{B}$ is the Boltzmann constant)
two vessels contain water solutions (at temperature T )

Updated On: Jul 13, 2024
  • the force causing the molecules to move across the tube is βˆ†π‘›π‘˜π΅π‘‡π‘†

  • force balance implies 𝑛1𝛽𝑣𝑙 = βˆ†π‘›π‘˜π΅π‘‡

  • total number of molecules going across the tube per $\sec$ is $\left(\frac{\Delta n}{l}\right)\left(\frac{k_{B} t}{\beta}\right) S$
  • rate of molecules getting transferred through the tube does not change with time
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The Correct Option is A, B, C

Solution and Explanation

The Correct Options are : A, B, C : 
the force causing the molecules to move across the tube is βˆ†π‘›π‘˜π΅π‘‡π‘†
force balance implies 𝑛1𝛽𝑣𝑙 = βˆ†π‘›π‘˜π΅π‘‡
total number of molecules going across the tube per $\sec$ is $\left(\frac{\Delta n}{l}\right)\left(\frac{k_{B} t}{\beta}\right) S$
 

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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.