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04-BS-7 · December 2014

Question 6 of 13: Stagnation Pressure Limit for a Motorcyclist

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

Notes on this paper

04-BS-7 Mechanics of Fluids — National Examinations, December 2014. Three (3) hours, closed book. Section A: Calculative (9 questions, do 7); Section B: Analytical/Graphical (4 questions, do 3). Ten questions constitute a complete paper (50 marks). Every printed question is solved below, including the two "extra" questions in each Section beyond the minimum required.

Reference texts: White, Fluid Mechanics, 8th ed. (fluid statics & buoyancy Ch.2; Bernoulli/energy & momentum equations Ch.3; pipe friction & the Moody chart Ch.6; drag on immersed bodies Ch.7).

Question 6 — Stagnation Pressure Limit for a Motorcyclist (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
Maximum exhale pressure100 mm water gauge
Density of air (15°C), ρair1.21 kg/m³

Find. The road speed V at which the stagnation pressure at the rider's mouth equals the maximum exhale pressure.

Approach. At a stagnation point the local relative velocity is zero, so by the energy (Bernoulli) equation all of the oncoming air's kinetic energy converts to a local pressure rise (dynamic pressure). Setting this equal to the 100 mm water-gauge exhale limit gives the critical speed.

  1. Convert the exhale limit to a pressure. $$\Delta p = \rho_{water}\, g\, h = 1000\times 9.81\times 0.100 = \boxed{981\text{ Pa}}$$
  2. Equate to the stagnation (dynamic) pressure of the oncoming air and solve for V. $$\tfrac{1}{2}\rho_{air} V^2 = \Delta p \quad\Rightarrow\quad V = \sqrt{\frac{2\Delta p}{\rho_{air}}} = \sqrt{\frac{2(981)}{1.21}} = \boxed{40.3\text{ m/s} = 145\text{ km/h}}$$
QuantityResult
Pressure equivalent, Δp981 Pa
Critical speed, V40.3 m/s (145 km/h)