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04-BS-7 · December 2016

Question 10 of 13: Velocity and Flow-Rate Response of a Wide River in Flood

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

Notes on this paper

04-BS-7 Mechanics of Fluids — December 2016 (National Examinations, three hours, closed book). Section A (Calculative) offers 9 questions and instructs "do seven"; Section B (Graphical and Analytical) offers 4 questions and instructs "do three." Every question is answered below (13 of 13), so students can use the full paper as a study resource. Constants used throughout (from the paper's own Constants page): g = 9.81 m/s², patm = 100 kPa, ρwater = 1000 kg/m³, ρconcrete = 2400 kg/m³, ρair = 1.19 kg/m³ (20°C) / 1.21 kg/m³ (15°C), μwater = 1.0×10⁻³ N·s/m², μair = 1.8×10⁻⁵ N·s/m², Rair = 287 J/kg·K.

Reference texts: F. M. White, Fluid Mechanics, 8th ed. (McGraw-Hill) — fluid statics and buoyancy/stability (Ch. 2), Bernoulli and control-volume momentum (Ch. 3), potential (inviscid) flow past a cylinder (Ch. 8), pipe friction and the Moody/Colebrook relation (Ch. 6), open-channel flow (Ch. 10), drag on immersed bodies and Stokes' law (Ch. 7); B. R. Munson et al., Fundamentals of Fluid Mechanics — actuator-disk propeller theory and variable-area tank draining.

Question 10: Velocity and Flow-Rate Response of a Wide River in Flood (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.

For a wide, shallow channel of fixed width, the wetted perimeter is dominated by the bottom (the two side walls contribute negligibly as the width-to-depth ratio is large), so the hydraulic radius Rh=A/P ≈ y (the flow depth itself). Combined with the Manning/Chezy uniform-flow relation V ∝ Rh2/3 (slope and roughness unchanged), this lets both ratios be found from the single depth ratio alone.

  1. (a) Velocity ratio. With Rh≈y and V ∝ Rh2/3: $$\frac{V_{flood}}{V_{normal}} = \left(\frac{y_{flood}}{y_{normal}}\right)^{2/3} = 2^{2/3} = \boxed{1.587}$$ The flood velocity is therefore greater than the normal velocity — but (since the exponent 2/3 < 1) less than double it.
  2. (b) Flow-rate ratio. Flow rate Q=VA=V(y·width), and since the width is fixed: $$\frac{Q_{flood}}{Q_{normal}} = \frac{V_{flood}}{V_{normal}}\times\frac{y_{flood}}{y_{normal}} = 2^{2/3}\times 2 = 2^{5/3} = \boxed{3.17}$$ The flood flow rate is therefore greater than two times the normal flow rate.
  3. (c) Justification. Both results follow from the Manning-type relation V=(1/n)Rh2/3S1/2: doubling the depth doubles the driving cross-section directly (the "A" in Q=VA") AND increases the hydraulic radius (hence velocity, via reduced relative wall friction) by a further factor of 22/3, so the two effects compound and Q rises faster than linearly with depth.
QuantityResult
Vflood/Vnormal1.587 (greater than normal, less than double)
Qflood/Qnormal3.17 (greater than two times)