Determine the total pressure and centre of pressure on an isosceles triangular plate of base 5 m and altitude 5 m when the plate is immersed vertically in an oil of sp. gr. 0.8. The base of the plate is 1 m below the free surface of the oil.

Isosceles Triangle Pressure Problem

Problem Statement

Determine the total pressure and centre of pressure on an isosceles triangular plate of base 5 m and altitude 5 m when the plate is immersed vertically in an oil of sp. gr. 0.8. The base of the plate is 1 m below the free surface of the oil.

Given Data

  • Base of plate, \( b = 5 \, \text{m} \)
  • Altitude of plate, \( d = 5 \, \text{m} \)
  • Specific Gravity of oil, \( S.G. = 0.8 \)
  • Density of oil, \( \rho = 0.8 \times 1000 = 800 \, \text{kg/m}^3 \)
  • Depth of base below free surface = 1 m

Solution

(i) Total Pressure (Force, \(F\))

First, we calculate the area of the plate and the depth of its centroid (\(\bar{h}\)).

$$ A = \frac{1}{2} \times b \times d = \frac{1}{2} \times 5 \times 5 = 12.5 \, \text{m}^2 $$

The centroid of a triangle is \(d/3\) from its base. Since the plate is inverted, the centroid is below the base.

$$ \bar{h} = (\text{Depth of base}) + \frac{d}{3} $$ $$ \bar{h} = 1 + \frac{5}{3} = \frac{8}{3} \approx 2.667 \, \text{m} $$

Now, we can calculate the total force.

$$ F = \rho g A \bar{h} $$ $$ F = 800 \times 9.81 \times 12.5 \times \frac{8}{3} $$ $$ F = 261600 \, \text{N} $$

(ii) Position of Centre of Pressure (\(h^*\))

The depth of the centre of pressure is found using the parallel axis theorem.

$$ h^* = \frac{I_G}{A\bar{h}} + \bar{h} $$

First, we need the moment of inertia about the centroid (\(I_G\)) for a triangle.

$$ I_G = \frac{bd^3}{36} = \frac{5 \times (5)^3}{36} = \frac{625}{36} \approx 17.361 \, \text{m}^4 $$

Now, we substitute all values into the formula for \(h^*\).

$$ h^* = \frac{17.361}{12.5 \times (8/3)} + \frac{8}{3} $$ $$ h^* = \frac{17.361}{33.333} + 2.667 $$ $$ h^* \approx 0.5208 + 2.667 \approx 3.188 \, \text{m} $$
Final Results:

Total Pressure (Force): \( F = 261.6 \, \text{kN} \).

Depth of Centre of Pressure: \( h^* \approx 3.188 \, \text{m} \) below the free surface.

Explanation of Concepts

Centroid of an Inverted Triangle: The problem describes an inverted triangle where the base is closer to the surface than the apex. The centroid is the geometric center, which for a triangle is one-third of the altitude from the base. We add this distance to the depth of the base to find the centroid's total depth from the free surface.

Centre of Pressure: The total hydrostatic force, or "total pressure," acts at the centre of pressure, not the centroid. Because pressure increases with depth, this point is always vertically below the centroid for a submerged plane. The distance between them depends on the object's shape (through its moment of inertia, \(I_G\)) and its depth.

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