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04-BS-7 · Undated paper

Question 3 of 13: Counterweight Mass for a Hinged Dam Gate

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

04-BS-7 Mechanics of Fluids — undated sitting, identified as May 2019 (National Examinations, three hours, closed book). Section A (Calculative) offers 9 questions and instructs “do seven”; Section B (Analytical) offers 4 questions and instructs “do three.” A complete paper is any 10 of the 13, each worth 5 marks. Every question is answered below (13 of 13) so the set can be used as a full study resource. Constants used throughout (from the paper's own Constants page, p.12): g = 9.81 m/s², patm = 100 kPa, ρwater = 1000 kg/m³, SGbenzene = 0.90, SGmercury = 13.56, SGcarbon tetrachloride = 1.59, ρair = 1.19 kg/m³ (20°C), μwater = 1.0×10⁻³ N·s/m², μair = 1.8×10⁻⁵ N·s/m².

Reference texts: F. M. White, Fluid Mechanics, 8th ed. (McGraw-Hill) — fluid statics and manometry (Ch. 2), hydrostatic forces on plane surfaces (Ch. 2), the Bernoulli/continuity pair and orifice flow (Ch. 3), the linear-momentum equation for moving vanes (Ch. 3), pipe friction and the Moody/Colebrook relation (Ch. 6), boundary layers and drag (Ch. 7), capillary rise (Ch. 1), high-lift devices and aircraft wing aerodynamics (J. D. Anderson, Fundamentals of Aerodynamics, Ch. 4–5).

Question 3: Counterweight Mass for a Hinged Dam Gate (5 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given.

QuantityValue
Gate width, b1.5 m
Gate height, h2.0 m
Depth to top of gate3.0 m
Hinge locationtop of gate
Counterweight arm length1.2 m (horizontal, from hinge)

Find. The mass of the counterweight at which the gate is on the verge of opening.

water surface 3.0 m hinge gate, 2.0 m 1.2 m (arm) F (hydrostatic)
Gate hinged at the top; water pressure resultant F acts below the hinge, the counterweight arm extends 1.2 m to the side above it.

Approach. Compute the hydrostatic resultant force and its centre of pressure on the gate, then take moments about the top hinge: the counterweight's moment (weight × 1.2 m arm) must equal the water force's moment (F × distance from hinge down to the centre of pressure) at the threshold of opening.

  1. Resultant hydrostatic force on the gate. Depth to centroid, yc = 3.0 + 2.0/2 = 4.0 m; area A = 1.5(2.0) = 3.0 m²: $$ F = \rho g y_c A = (1000)(9.81)(4.0)(3.0) = 117\,720\ \text{N} $$
  2. Depth to the centre of pressure. Using I_c = bh^3/12 = 1.5(2.0)^3/12 = 1.0 m⁴: $$ y_p = y_c + \frac{I_c}{y_c A} = 4.0 + \frac{1.0}{(4.0)(3.0)} = 4.0833\ \text{m} $$
  3. Lever arm from the hinge (top of gate, depth 3.0 m) to the centre of pressure. $$ d = y_p - 3.0 = 1.0833\ \text{m} $$
  4. Moment balance about the hinge. Setting the weight's moment equal to the water force's moment at the threshold of opening: $$ mg(1.2) = F\,d \quad\Rightarrow\quad m = \frac{Fd}{g(1.2)} = \frac{(117\,720)(1.0833)}{(9.81)(1.2)} $$ $$ \boxed{m \approx 10\,833\ \text{kg} \approx 10.8\ \text{tonnes}} $$
QuantityResult
Hydrostatic force on gate117.7 kN
Depth to centre of pressure4.083 m
Required counterweight mass≈ 10 833 kg
Check: the large counterweight mass follows directly from the given geometry — the water force (117.7 kN, about 12 tonnes-force) acts on a moment arm from the hinge (1.08 m) that is comparable to the counterweight arm (1.2 m), so a large mass is genuinely required; this is not an arithmetic error.