Fluid Mechanics: cram pack

Formula sheets, the key method steps for every topic and 8 practice problems, with full solutions at the back.

New problems Back to the course

In the print window, choose “Save as PDF” to keep a copy on your device.

1Formulas and methods

Hydrostatic force

Pressure at depth: p = ρgh
Force on a vertical wall: F = ρg·h_c·A
Centre of pressure: y_p = y_c + I_c/(y_cA)
Rectangle: I_c = bH³/12

Continuity & Bernoulli

Continuity: A₁v₁ = A₂v₂
Bernoulli: p₁ + ½ρv₁² + ρgz₁ = p₂ + ½ρv₂² + ρgz₂
Flow rate: Q = A·v
Circle area: A = πd²/4

Pipe friction & head loss

Reynolds number: Re = V·D/ν = ρ·V·D/μ
Flow regime: laminar below Re ≈ 2000, turbulent above Re ≈ 4000
Mean velocity: V = Q/A, A = π·D²/4
Darcy–Weisbach: h_f = f·(L/D)·V²/(2g)
Minor losses: h_m = ΣK·V²/(2g)
Typical K values: entrance 0.5, exit 1.0, 90° bend ≈ 0.3
Pressure drop: Δp = ρ·g·h_f
Two open reservoirs: Δz = (f·L/D + ΣK)·V²/(2g)
Free outlet: H = (1 + f·L/D + ΣK)·V²/(2g)

Pumps & pump power

Hydraulic power: P_h = ρ·g·Q·H = Q·Δp
Shaft power: P_shaft = P_h/η_pump
Electrical power: P_el = P_shaft/η_motor
Pump head: H = Δz + Δp/(ρ·g) + h_L
System losses: h_L = (f·L/D + ΣK)·V²/(2g)

2Practice problems

1.Hydrostatic forceMedium

A vertical rectangular gate 1 m wide sits in the wall of a tank of water, with its top edge 4 m below the surface. Find the resultant hydrostatic force F on the gate.

d = 4 mH = 2 mb = 1 mρ = 1000 kg/m³g = 9.81 m/s²

F = kN

2.Hydrostatic forceHard

A vertical rectangular gate 1.5 m wide sits in the wall of a tank of oil, with its top edge 3 m below the surface. Find the depth y_cp of the centre of pressure below the surface.

d = 3 mH = 1.5 mb = 1.5 mρ = 880 kg/m³g = 9.81 m/s²

y_cp = m

3.Continuity & BernoulliMedium

Water flows through a horizontal pipe that narrows from 75 mm to 40 mm. In the wide section the pressure is 380 kPa and the velocity is 1.25 m/s. Ignoring losses, find the pressure p₂ in the narrow section.

d₁ = 75 mmd₂ = 40 mmp₁ = 380 kPav₁ = 1.25 m/sρ = 1000 kg/m³

p₂ = kPa

4.Continuity & BernoulliHard

Water flows up through a pipe that narrows from 100 mm to 75 mm while rising 3 m. At section 1 the pressure is 340 kPa and the velocity is 0.75 m/s. Ignoring losses, find the pressure p₂ at section 2.

d₁ = 100 mmd₂ = 75 mmp₁ = 340 kPav₁ = 0.75 m/sΔz = 3 mρ = 1000 kg/m³

p₂ = kPa

5.Pipe friction & head lossMedium

Water (ρ = 1000 kg/m³) flows at 2.3 m/s through a horizontal pipe, 300 m long, with an inside diameter of 150 mm. Use the Darcy friction factor f = 0.03 and g = 9.81 m/s². Find the pressure drop Δp over the pipe in kPa.

V = 2.3 m/sL = 300 mD = 150 mmf = 0.03ρ = 1000 kg/m³

Δp = kPa

6.Pipe friction & head lossHard

Two open reservoirs are joined by a pipe 100 m long with an inside diameter of 100 mm and a Darcy friction factor f = 0.015. The minor losses are a square-edged entrance (K = 0.5), 2 bends (K = 0.3 each), a valve (K = 10) and the exit into the lower reservoir (K = 1.0). Use g = 9.81 m/s². What difference in water level Δz between the reservoirs gives a flow rate of 10 L/s?

Q = 10 L/sL = 100 mD = 100 mmf = 0.015K_entrance = 0.5K_bend = 0.3 (×2)K_valve = 10K_exit = 1.0

Δz = m

7.Pumps & pump powerMedium

In a test, a pump delivers 40 L/s of water (ρ = 1000 kg/m³) against a head of 62 m while its shaft takes 34.8 kW. Use g = 9.81 m/s². Find the pump efficiency η in percent.

Q = 40 L/sH = 62 mP_shaft = 34.8 kWg = 9.81 m/s²

η = %

8.Pumps & pump powerHard

A pump moves 50 L/s of water (ρ = 1000 kg/m³) from an open lower reservoir to an upper tank whose water surface is 29 m higher. The pipe is 150 m long with an inside diameter of 150 mm and a Darcy friction factor f = 0.022; the minor-loss coefficients add up to ΣK = 8 (entrance and exit included). Use g = 9.81 m/s². The upper tank is closed and the air above its water is at a gauge pressure of 200 kPa. Find the head H the pump must add.

Q = 50 L/sΔz = 29 mL = 150 mD = 150 mmf = 0.022ΣK = 8p_tank = 200 kPa

H = m

3Solutions

1.Hydrostatic force

Answer: F = 98.1 kN

Hydrostatic force on a plane surface: F = ρ·g·y_c·A. It acts at the centre of pressure, y_cp = y_c + I_c/(y_cA), which always lies below the centroid.

Centroid depth and area

y_c = d + H/2 = 4 + 2/2 = 5 m

A = H·b = 2·1 = 2 m²

Resultant force

F = ρ·g·y_c·A = 1000·9.81·5·2 = 98.1 kN

Answer

F = 98.1 kN

2.Hydrostatic force

Answer: y_cp = 3.8 m

Hydrostatic force on a plane surface: F = ρ·g·y_c·A. It acts at the centre of pressure, y_cp = y_c + I_c/(y_cA), which always lies below the centroid.

Centroid depth and area

y_c = d + H/2 = 3 + 1.5/2 = 3.75 m

A = H·b = 1.5·1.5 = 2.25 m²

Resultant force

F = ρ·g·y_c·A = 880·9.81·3.75·2.25 = 72.84 kN

Centre of pressure

Pressure grows with depth, so the resultant acts below the centroid.

I_c = b·H³/12 = 1.5·1.5³/12 = 0.4219 m⁴

y_cp = y_c + I_c/(y_c·A) = 3.75 + 0.4219/(3.75·2.25) = 3.8 m

Answer

y_cp = 3.8 m

3.Continuity & Bernoulli

Answer: p₂ = 371.1 kPa

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 = 1.25·(75/40)² = 4.395 m/s

½ρ(v₁² − v₂²) = ½·1000·(1.25² − 4.395²)/1000 = −8.875 kPa

p₂ = p₁ + ½ρ(v₁² − v₂²) = 380 + (−8.875) = 371.1 kPa

Answer

p₂ = 371.1 kPa

4.Continuity & Bernoulli

Answer: p₂ = 310 kPa

Continuity and Bernoulli

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

v₂ = v₁·(d₁/d₂)² = 0.75·(100/75)² = 1.333 m/s

½ρ(v₁² − v₂²) = ½·1000·(0.75² − 1.333²)/1000 = −0.6076 kPa

ρgΔz = 1000·9.81·3/1000 = 29.43 kPa

p₂ = p₁ + ½ρ(v₁² − v₂²) − ρgΔz = 340 + (−0.6076) − 29.43 = 310 kPa

Answer

p₂ = 310 kPa

5.Pipe friction & head loss

Answer: Δp = 158.7 kPa

Pipe flow: the Reynolds number Re = V·D/ν = ρ·V·D/μ tells laminar flow (Re below about 2000) from turbulent flow (above about 4000). Friction along a pipe costs the Darcy–Weisbach head loss h_f = f·(L/D)·V²/(2g). Fittings, valves, the entrance and the exit add minor losses h_m = ΣK·V²/(2g). Between two open reservoir surfaces the energy equation gives Δz = h_f + h_m, with the exit loss K = 1 included.

Head loss

h_f = f·(L/D)·V²/(2g) = 0.03·(300/0.15)·2.3²/(2·9.81) = 16.18 m

Pressure drop

The pipe is horizontal and the velocity does not change, so the energy equation reduces to Δp = ρ·g·h_f.

Δp = ρ·g·h_f = 1000·9.81·16.18 = 158700 Pa = 158.7 kPa

Answer

Δp = 158.7 kPa

6.Pipe friction & head loss

Answer: Δz = 2.239 m

Velocity

V = Q/A = 0.01/0.007854 = 1.273 m/s

V²/(2g) = 0.08263 m

Loss coefficients

f·L/D = 0.015·100/0.1 = 15

ΣK = 0.5 + 2·0.3 + 10 + 1.0 = 12.1

Total head loss

h_f = 15·0.08263 = 1.239 m

h_m = 12.1·0.08263 = 0.9998 m

Δz = h_f + h_m = 2.239 m

Answer

Δz = 2.239 m

7.Pumps & pump power

Answer: η = 69.91 %

Pump power: the power given to the water is the hydraulic power P_h = ρ·g·Q·H = Q·Δp. The shaft must deliver more because the pump loses some: P_shaft = P_h/η_pump, and the motor draws P_el = P_shaft/η_motor. The pump head H follows from the energy equation: static lift + pressure head + all friction and minor losses.

Hydraulic power

P_h = ρ·g·Q·H = 1000·9.81·0.04·62 = 24.33 kW

Efficiency

η = P_h/P_shaft = 24.33/34.8 = 69.91%

Answer

η = 69.91%

8.Pumps & pump power

Answer: H = 61.63 m

Velocity

V = Q/A = 0.05/0.01767 = 2.829 m/s

V²/(2g) = 0.408 m

Head losses

h_L = (f·L/D + ΣK)·V²/(2g) = (22 + 8)·0.408 = 12.24 m

Pressure head

p/(ρ·g) = 200000/(1000·9.81) = 20.39 m

Pump head

Both surfaces are practically at rest, so there is no velocity head term.

H = Δz + p/(ρ·g) + h_L = 29 + 20.39 + 12.24 = 61.63 m

Answer

H = 61.63 m

ExamProblems · examproblems.com/courses/fluid-mechanics