Fluid Mechanics: practice problems and exam questions

Fluid statics and flow: pressure in liquids, forces on submerged surfaces, continuity and Bernoulli’s equation. Exam problems often chain these steps: continuity gives the speed, and Bernoulli then gives the pressure.

Cram pack (PDF)Formula sheets, method steps and practice problems with full solutions, ready to print.

Topics in this course

  1. Hydrostatic forcevertical wall · submerged gate · centre of pressurecalculations
  2. Continuity & Bernoullicontinuity · horizontal reducer · rising pipecalculations
  3. Pipe friction & head lossReynolds number · Darcy–Weisbach head loss · minor losses and total headcalculations
  4. Pumps & pump powerhydraulic power · pump efficiency · system head and powercalculations

Exam tips for Fluid Mechanics

  • Pressure in a liquid at rest depends only on depth: p = ρ·g·h.
  • Apply continuity first: A₁·v₁ = A₂·v₂.
  • Use gauge pressure or absolute pressure, but the same one on both sides of Bernoulli’s equation.

Worked examples

Hydrostatic forceEasy
h = 4 m

Water stands 4 m deep against a vertical wall. Find the height ȳ above the base at which the resultant force acts.

h = 4 mb = 2 mρ = 1000 kg/m³g = 9.81 m/s²

Find ȳ (m)

Show hints
  1. Pressure in a still liquid is p = ρ·g·z.
  2. The pressure diagram on the wall is a triangle. F is its area times the width; it acts through its centroid.
  3. The pressure at the base is 39.24 kPa.
Show the answer and the step-by-step solution

Hydrostatic force: on a plane surface, F = ρ·g·yc·A, where yc is the depth of the centroid. It acts below the centroid, at the centre of pressure.

h = 4 mF

Pressure varies linearly with depth

p = ρ·g·z, from zero at the surface to ρ·g·h at the base, so the load on the wall is a triangle.

pbase = ρgh = 1000·9.81·4 = 39.24 kPa

Line of action

A triangular load acts at its centroid, one third of the height from the base
ȳ = h/3 = 4/3 = 1.333 m above the base

Answer

ȳ = 1.333 m
Continuity & BernoulliMedium
12d1​ = 150 mm, p1​ = 250 kPad2​ = 50 mm, p2​ = ?

Water flows through a horizontal pipe that narrows from 150 mm to 50 mm. In the wide section the pressure is 250 kPa and the velocity is 0.5 m/s. Ignoring losses, find the pressure p2 in the narrow section.

d1 = 150 mmd2 = 50 mmp1 = 250 kPav1 = 0.5 m/sρ = 1000 kg/m³

Find p2 (kPa)

Show hints
  1. First use continuity to find the velocity in the narrow section.
  2. Bernoulli for a horizontal pipe: p₁ + ½ρv₁² = p₂ + ½ρv₂².
  3. v2 = 4.5 m/s.
Show the answer and the step-by-step solution

Continuity and Bernoulli: for an incompressible fluid the flow rate is the same at every section, Q = A₁v₁ = A₂v₂. Along a streamline without losses, p + ½ρv² + ρgz is constant, so where the fluid is faster or higher its pressure is lower.

Continuity and Bernoulli

Work in Pa, then divide by 1000 to get kPa.

v2 = v1·(d1/d2)² = 0.5·(150/50)² = 4.5 m/s
½ρ(v1² − v2²) = ½·1000·(0.5² − 4.5²)/1000 = −10 kPa
p2 = p1 + ½ρ(v1² − v2²) = 250 + (−10) = 240 kPa

Answer

p2 = 240 kPa

How practising works

  • “Practise this course” mixes problems from all its topics, like a real exam.
  • Every problem has new values, so you learn the method instead of an answer.
  • Stuck? Open a small hint first, and the full explanation only when you need it.
  • Mock exams are timed and have no hints, and you get your score and a full review at the end.

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