In the fig., the pressure at point A is 2900 N/m2. Determine the pressures at points B, C and D. (Take density of air = 1.2 kg/m3)

In the fig., the pressure at point A is 2900 N/m2. Determine the pressures at points B, C and D. (Take density of air = 1.2 kg/m3)

Problem Statement

Given a closed tank, the density of air is \( 1.2 \, \text{kg/m}^3 \), and the density of water is \( 1000 \, \text{kg/m}^3 \). The absolute pressure at point A is \( 2900 \, \text{N/m}^2 \). Determine the absolute pressures at points B, C, and D. Assume the following distances:

  • Distance between A and B: \( 0.2 \, \text{m} \)
  • Distance between A and X: \( 1.3 \, \text{m} \)
  • Distance between X and C: \( 2.3 \, \text{m} \)
  • Distance between A and D: \( 2.0 \, \text{m} \)

Solution

Given:

  • \( \rho = 1000 \, \text{kg/m}^3 \) (density of water)
  • \( \rho_{\text{air}} = 1.2 \, \text{kg/m}^3 \)
  • \( P_A = 2900 \, \text{N/m}^2 \)

Pressure at Point B (\( P_B \)):

Using the hydrostatic pressure equation:

\( P_B = P_A – \rho g h_{\text{between A and B}} \)

Substitute the values:

\( P_B = 2900 – (1000 \times 9.81 \times 0.2) \)

Final Value:

\( P_B = 938 \, \text{N/m}^2 \)

Pressure at Point C (\( P_C \)):

Considering the contributions from water and air columns:

\( P_C = P_A + \rho g h_{\text{between A and X}} – \rho_{\text{air}} g h_{\text{XC}} \)

Substitute the values:

\( P_C = 2900 + (1000 \times 9.81 \times 1.3) – (1.2 \times 9.81 \times 2.3) \)

Final Value:

\( P_C = 15626 \, \text{N/m}^2 \)

Pressure at Point D (\( P_D \)):

Using the hydrostatic pressure equation:

\( P_D = P_A + \rho g h_{\text{between A and D}} \)

Substitute the values:

\( P_D = 2900 + (1000 \times 9.81 \times 2) \)

Final Value:

\( P_D = 22520 \, \text{N/m}^2 \)

Explanation

This problem uses the principles of hydrostatics to determine the pressures at different points:

  1. The pressure at any point in a fluid depends on the density of the fluid, gravitational acceleration, and height difference.
  2. In this case, the pressure contributions are calculated using water’s density for liquid columns and air’s density for gaseous columns.
  3. The small density of air (\( \rho_{\text{air}} \)) compared to water results in a minor pressure contribution from the air column.

Physical Meaning

  1. Density (\( \rho \)): The density of a fluid directly influences its pressure contribution. Water, being denser, has a much greater impact than air.
  2. Hydrostatic Pressure: The difference in pressure between points arises due to height differences and fluid density. This principle applies in both liquid and gas columns.
  3. Negligible Air Pressure: While air’s pressure contribution is small, it is included here for completeness, demonstrating how its effect becomes insignificant in most practical scenarios.

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