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Q10.22(b):

A manometer reads the pressure of a gas in an enclosure as shown in Fig. 10.25 (a) When a pump removes some of the gas, the manometer reads as in Fig. 10.25 (b) The liquid used in the manometers is mercury and the atmospheric pressure is 76 cm of mercury. (b) How would the levels change in case (b) if 13.6 cm of water (immiscible with mercury) are poured into the right limb of the manometer ? (Ignore the small change in the volume of the gas).

A manometer reads the pressure of a gas in an enclosure as shown in fig.  10.25 (a) when a pump removes some of the gascomma the manometer reads as  in fig. 10.25 (

Solution :

Step 1: Establishing Initial Parameters and Hydrostatic Equilibrium

From the problem statement and Figure 10.25 (b), let the initial pressure of the gas in the enclosure be $P_g$. In the right limb, the column of mercury is exposed to the atmosphere ($P_{atm} = 76 \text{ cm of Hg}$). In the left limb, the mercury column is connected to the gas enclosure. Let $h$ be the height difference between the mercury levels in the two limbs. According to the law of hydrostatics [Per the Law of Communicating Vessels], the pressure at a horizontal level in a continuous static fluid is equal.

The equilibrium condition for the manometer in state (b) is given by:

$P_g + h_{left} \cdot \rho_{Hg} \cdot g = P_{atm} + h_{right} \cdot \rho_{Hg} \cdot g$

$P_g = P_{atm} - h \cdot \rho_{Hg} \cdot g$ (where $h$ is the difference in mercury levels).

Step 2: Analysis of Adding Immiscible Water

We add $h_w = 13.6 \text{ cm}$ of water to the right limb. Since water is immiscible with mercury and $\rho_w < \rho_{Hg}$, the water floats on top of the mercury in the right limb. This increases the total pressure on the mercury surface in the right limb. The density of water is $\rho_w = 1 \text{ g/cm}^3$ and the density of mercury is $\rho_{Hg} = 13.6 \text{ g/cm}^3$.

The equivalent pressure head of water in terms of mercury is calculated as:

$h_{eq} = h_w \times \frac{\rho_w}{\rho_{Hg}}$

$h_{eq} = 13.6 \text{ cm} \times \frac{1 \text{ g/cm}^3}{13.6 \text{ g/cm}^3} = 1 \text{ cm of Hg}$

Step 3: Calculating the Shift in Mercury Levels

Let the new difference in mercury levels be $h'$. The new pressure equilibrium equation at the common interface level in the left limb becomes:

$P_g + h_1 \rho_{Hg} g = P_{atm} + h_2 \rho_{Hg} g + h_w \rho_w g$

Because the gas volume is assumed constant and the tube cross-section is uniform, if the mercury level in the right limb drops by $x$, the level in the left limb rises by $x$. The new difference $h'$ relates to the previous difference $h$ as $h' = h + 2x$. However, the hydrostatic balance dictates that the added 1 cm of mercury pressure equivalent must be distributed across the two columns.

Gas Water Hg

When 13.6 cm of water is added, it exerts a pressure equivalent to 1 cm of Hg. This pressure pushes the mercury in the right limb down. Consequently, the mercury level in the left limb rises. By the principle of displacement in U-tubes:

  • Pressure increment on right side = $1 \text{ cm Hg}$.
  • Since the pressure must balance, the mercury column height difference $h'$ must adjust to compensate for the additional $1 \text{ cm}$ of head.
  • The mercury level in the right limb will descend by $0.5 \text{ cm}$, and the mercury level in the left limb will rise by $0.5 \text{ cm}$.

Summary of Level Changes

Limb Direction of Change Magnitude
Right Limb (Water side) Downward $0.5 \text{ cm}$
Left Limb (Gas side) Upward $0.5 \text{ cm}$

Final Solution: Upon pouring 13.6 cm of water into the right limb, the mercury level in the right limb will fall by 0.5 cm, and the mercury level in the left limb will rise by 0.5 cm, resulting in a net increase of 1 cm in the mercury level difference between the two limbs.


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