JEE Challenger
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Temperature of Rising Gas Bubble in Liquid Column

Comprehension Passage

Paragraph for Question Nos. 38 to 40

A small spherical monoatomic ideal gas bubble (γ=53)\left(\gamma = \frac{5}{3}\right) is trapped inside a liquid of density ρl\rho_l (see figure). Assume that the bubble does not exchange any heat with the liquid. The bubble contains nn moles of gas. The temperature of the gas when the bubble is at the bottom is T0T_0, the height of the liquid is HH and the atmospheric pressure is P0P_0 (Neglect surface tension).

Passage Diagram 0

When the gas bubble is at a height yy from the bottom, its temperature is

Options

A

T0(P0+ρlgHP0+ρlgy)2/5T_0 \left(\frac{P_0 + \rho_l g H}{P_0 + \rho_l g y}\right)^{2/5}

B

T0(P0+ρlg(H−y)P0+ρlgH)2/5T_0 \left(\frac{P_0 + \rho_l g (H - y)}{P_0 + \rho_l g H}\right)^{2/5}

Correct
C

T0(P0+ρlgHP0+ρlgy)3/5T_0 \left(\frac{P_0 + \rho_l g H}{P_0 + \rho_l g y}\right)^{3/5}

D

T0(P0+ρlg(H−y)P0+ρlgH)3/5T_0 \left(\frac{P_0 + \rho_l g (H - y)}{P_0 + \rho_l g H}\right)^{3/5}

Step-by-Step Solution

To find the temperature of the gas bubble as a function of height yy from the bottom of the container, we analyze the thermodynamics of the process:

  1. Pressure of the Bubble:
    Neglecting surface tension, the pressure inside the bubble is equal to the hydrostatic pressure of the liquid at that depth plus the atmospheric pressure P0P_0.

    • At the bottom of the liquid column (depth =H= H), the pressure is:
      Pbottom=P0+ρlgHP_{\text{bottom}} = P_0 + \rho_l g H
      The temperature of the gas at this position is given as T0T_0.
    • At a height yy from the bottom, the depth of the bubble below the free liquid surface is (H−y)(H - y). Hence, the pressure inside the bubble is:
      P(y)=P0+ρlg(H−y)P(y) = P_0 + \rho_l g (H - y)
  2. Thermodynamic Process:
    Since the bubble does not exchange any heat with the surrounding liquid, the expansion of the gas as it rises is an adiabatic process.

    For an adiabatic process involving an ideal gas:
    P1−γTγ=constant  ⟹  T∝Pγ−1γP^{1-\gamma} T^\gamma = \text{constant} \implies T \propto P^{\frac{\gamma - 1}{\gamma}}

  3. Calculation of Temperature:
    For a monoatomic ideal gas, the adiabatic index is γ=53\gamma = \frac{5}{3}.
    The exponent is:
    γ−1γ=53−153=2/35/3=25\frac{\gamma - 1}{\gamma} = \frac{\frac{5}{3} - 1}{\frac{5}{3}} = \frac{2/3}{5/3} = \frac{2}{5}

    Applying the relation between the initial state (at the bottom) and the state at height yy:
    T(y)T0=(P(y)Pbottom)γ−1γ\frac{T(y)}{T_0} = \left(\frac{P(y)}{P_{\text{bottom}}}\right)^{\frac{\gamma - 1}{\gamma}}

    Substituting the pressures:
    T(y)=T0(P0+ρlg(H−y)P0+ρlgH)2/5T(y) = T_0 \left(\frac{P_0 + \rho_l g (H - y)}{P_0 + \rho_l g H}\right)^{2/5}

Therefore, the correct option is B.