JEE Challenger
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Equilibrium Position of Diathermic Partition in Isolated Gas Cylinder

A thermally insulated cylindrical closed vessel with height 8 m8\text{ m} is held vertically. It is partitioned into two equal sections by a diathermic (perfect thermal conductor) frictionless partition of mass 8.3 kg8.3\text{ kg}. The partition is initially held fixed at a distance of 4 m4\text{ m} from the top, as illustrated in the schematic diagram. Each of the two compartments contains 0.1 mole0.1\text{ mole} of an ideal gas at temperature 300 K300\text{ K}. The partition is released and moves without any leakage of gas between compartments. When equilibrium is attained, the distance of the partition measured from the top (in m\text{m}) will be ______. (Take acceleration due to gravity =10 ms−2= 10\text{ ms}^{-2} and universal gas constant =8.3 J mol−1K−1= 8.3\text{ J mol}^{-1}\text{K}^{-1}).

Question Diagram 1
Official Numerical Answer6

Step-by-Step Solution

To find the distance of the partition from the top at equilibrium, we analyze the forces acting on the diathermic partition when the system reaches mechanical and thermal equilibrium.

1. Given Data

  • Total height of the vessel, H=8 mH = 8\text{ m}
  • Initial position of the partition from the top, x0=4 mx_0 = 4\text{ m}
  • Mass of the partition, m=8.3 kgm = 8.3\text{ kg}
  • Number of moles of gas in each compartment, n=0.1 molen = 0.1\text{ mole}
  • Temperature at equilibrium, T=300 KT = 300\text{ K}
  • Acceleration due to gravity, g=10 ms−2g = 10\text{ ms}^{-2}
  • Universal gas constant, R=8.3 J mol−1K−1R = 8.3\text{ J mol}^{-1}\text{K}^{-1}

2. Equilibrium Equations

Let xx be the distance of the partition from the top in meters at equilibrium, and let AA be the cross-sectional area of the cylinder.

  • Volume of the top compartment: V1=A⋅xV_1 = A \cdot x

  • Volume of the bottom compartment: V2=A⋅(8−x)V_2 = A \cdot (8 - x)

Since the partition is diathermic, thermal equilibrium ensures that both compartments have the same temperature T=300 KT = 300\text{ K}.

Using the ideal gas equation PV=nRTP V = n R T:

  • Pressure in the top compartment (P1P_1): P1=nRTV1=nRTAxP_1 = \frac{n R T}{V_1} = \frac{n R T}{A x}

  • Pressure in the bottom compartment (P2P_2): P2=nRTV2=nRTA(8−x)P_2 = \frac{n R T}{V_2} = \frac{n R T}{A (8 - x)}


3. Mechanical Equilibrium

At equilibrium, the upward force exerted by the bottom gas balances the downward force exerted by the top gas and the weight of the partition: P2A=P1A+mgP_2 A = P_1 A + mg

Dividing both sides by AA: P2−P1=mgAP_2 - P_1 = \frac{mg}{A}

Substitute the expressions for P1P_1 and P2P_2: nRTA(8−x)−nRTAx=mgA\frac{n R T}{A(8 - x)} - \frac{n R T}{A x} = \frac{mg}{A}

Canceling AA from both sides: nRT8−x−nRTx=mg\frac{n R T}{8 - x} - \frac{n R T}{x} = mg

Factoring out nRTn R T: nRT(18−x−1x)=mgn R T \left( \frac{1}{8 - x} - \frac{1}{x} \right) = mg

nRT(x−(8−x)x(8−x))=mgn R T \left( \frac{x - (8 - x)}{x(8 - x)} \right) = mg

nRT(2x−88x−x2)=mgn R T \left( \frac{2x - 8}{8x - x^2} \right) = mg


4. Numerical Calculation

First, evaluate the terms nRTn R T and mgmg: nRT=0.1×8.3×300=249 Jn R T = 0.1 \times 8.3 \times 300 = 249\text{ J} mg=8.3×10=83 Nmg = 8.3 \times 10 = 83\text{ N}

Substitute these values into the equilibrium equation: 249(2x−88x−x2)=83249 \left( \frac{2x - 8}{8x - x^2} \right) = 83

Divide both sides by 8383: 3(2x−88x−x2)=13 \left( \frac{2x - 8}{8x - x^2} \right) = 1

3(2x−8)=8x−x23(2x - 8) = 8x - x^2

6x−24=8x−x26x - 24 = 8x - x^2

Rearranging into standard quadratic form: x2−2x−24=0x^2 - 2x - 24 = 0

Factorizing the quadratic equation: (x−6)(x+4)=0(x - 6)(x + 4) = 0

Since xx represents a physical distance inside the 8 m8\text{ m} cylinder, x>0x > 0: x=6 mx = 6\text{ m}


Final Answer

The distance of the partition measured from the top when equilibrium is attained will be 6.