Hydraulic Engineering: cram pack

Formula sheets, the key method steps for every topic and 10 practice problems, with full solutions at the back.

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1Formulas and methods

Hydrostatic force

Pressure at depth
p = ρgh
Force on a vertical wall
F = ρg·hc·A
Centre of pressure
yp = yc + Ic/(ycA)
Rectangle
Ic = 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
hf = f·(L/D)·V²/(2g)
Minor losses
hm = ΣK·V²/(2g)
Typical K values
entrance 0.5, exit 1.0, 90° bend ≈ 0.3
Pressure drop
Δp = ρ·g·hf
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
Ph = ρ·g·Q·H = Q·Δp
Shaft power
Pshaft = Ph/ηpump
Electrical power
Pel = Pshaft/ηmotor
Pump head
H = Δz + Δp/(ρ·g) + hL
System losses
hL = (f·L/D + ΣK)·V²/(2g)

Open-channel flow (Manning)

Manning equation
V = (1/n)·R2/3·S1/2
Flow rate
Q = A·V
Hydraulic radius
R = A/P (P = wetted perimeter, free surface excluded)
Rectangle
A = b·y, P = b + 2y
Trapezoid (side slope z:1)
A = (b + z·y)·y, P = b + 2y·√(1 + z²)
Circular pipe, full or half full
R = D/4
Required slope
S = (n·Q/(A·R2/3))²

2Practice problems

1.Hydrostatic forceMedium
gated = 1 mH = 3 m

A vertical rectangular gate 2 m wide sits in the wall of a tank of water, with its top edge 1 m below the surface. Find the resultant hydrostatic force F on the gate.

d = 1 mH = 3 mb = 2 mρ = 1000 kg/m³g = 9.81 m/s²
F = kN
2.Hydrostatic forceHard
gated = 4 mH = 1 m

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

d = 4 mH = 1 mb = 1 mρ = 880 kg/m³g = 9.81 m/s²
F = kN
3.Continuity & BernoulliMedium
v = ?p0​pp0​ − p = 700 Pastagnation point

A pitot-static tube in a wind tunnel reads a difference of 700 Pa between the stagnation pressure and the static pressure. The air density is 1.2 kg/m³. Find the air speed v.

p0 − p = 700 Paρ = 1.2 kg/m³
v = m/s
4.Continuity & BernoulliHard
12d1​ = 100 mm, p1​ = 190 kPad2​ = 25 mm, p2​ = ?Δz = 2 m

Water flows up through a pipe that narrows from 100 mm to 25 mm while rising 2 m. At section 1 the pressure is 190 kPa and the velocity is 0.75 m/s. Ignoring losses, find the pressure p2 at section 2.

d1 = 100 mmd2 = 25 mmp1 = 190 kPav1 = 0.75 m/sΔz = 2 mρ = 1000 kg/m³
p2 = kPa
5.Pipe friction & head lossMedium
Q = 60 L/sD = 250 mmL = 400 mf = 0.028

Water flows at 60 L/s through a pipe 400 m long with an inside diameter of 250 mm. Use the Darcy friction factor f = 0.028 and g = 9.81 m/s². Find the friction head loss hf.

Q = 60 L/sL = 400 mD = 250 mmf = 0.028g = 9.81 m/s²
hf = m
6.Pipe friction & head lossHard
K = 10free outletH = ?L = 150 m, D = 200 mm, f = 0.0223× bend (K = 0.3)

A pipe 150 m long with an inside diameter of 200 mm (Darcy friction factor f = 0.022) runs from an open reservoir and discharges as a free jet into the air. The minor losses are a square-edged entrance (K = 0.5), 3 bends (K = 0.3 each) and a valve (K = 10). Use g = 9.81 m/s². How far H must the reservoir surface be above the pipe outlet for a flow rate of 100 L/s?

Q = 100 L/sL = 150 mD = 200 mmf = 0.022Kentrance = 0.5Kbend = 0.3 (×3)Kvalve = 10
H = m
7.Pumps & pump powerMedium
PQ = 100 L/sH = 52 m

A pump with an efficiency of 65% delivers 100 L/s of water (ρ = 1000 kg/m³) against a head of 52 m. Use g = 9.81 m/s². Find the shaft power Pshaft needed, in kW.

Q = 100 L/sH = 52 mη = 65%g = 9.81 m/s²
Pshaft = kW
8.Pumps & pump powerHard
200 kPa (gauge)PQ = 50 L/sΔz = 5 mL = 300 m, D = 200 mm, f = 0.022, ΣK = 5

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 5 m higher. The pipe is 300 m long with an inside diameter of 200 mm and a Darcy friction factor f = 0.022; the minor-loss coefficients add up to ΣK = 5 (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 = 5 mL = 300 mD = 200 mmf = 0.022ΣK = 5ptank = 200 kPa
H = m
9.Open-channel flow (Manning)Medium
D = 450 mmn = 0.013, S = 0.0005

A concrete storm sewer with an inside diameter of 450 mm flows half full. Manning n = 0.013 and the slope is S = 0.0005. Find the flow rate Q in m³/s.

D = 450 mmn = 0.013S = 0.0005
Q = m³/s
10.Open-channel flow (Manning)Hard
b = 5.5 my = 2.4 mn = 0.015, Q = 46 m³/s

A rectangular brickwork channel 5.5 m wide must carry 46 m³/s in uniform flow at a depth of 2.4 m. Manning n = 0.015. Find the required bed slope S (in m/m).

Q = 46 m³/sb = 5.5 my = 2.4 mn = 0.015
S = m/m

3Solutions

1.Hydrostatic force

Answer: F = 147.2 kN

Hydrostatic force on a plane surface: F = ρ·g·yc·A. It acts at the centre of pressure, ycp = yc + Ic/(ycA), which always lies below the centroid.

Centroid depth and area

yc = d + H/2 = 1 + 3/2 = 2.5 m
A = H·b = 3·2 = 6 m²
gated = 1 mH = 3 mF

Resultant force

F = ρ·g·yc·A = 1000·9.81·2.5·6 = 147.2 kN

Answer

F = 147.2 kN
2.Hydrostatic force

Answer: F = 38.85 kN

Hydrostatic force on a plane surface: F = ρ·g·yc·A. It acts at the centre of pressure, ycp = yc + Ic/(ycA), which always lies below the centroid.

Centroid depth and area

yc = d + H/2 = 4 + 1/2 = 4.5 m
A = H·b = 1·1 = 1 m²
gated = 4 mH = 1 mF

Resultant force

F = ρ·g·yc·A = 880·9.81·4.5·1 = 38.85 kN

Answer

F = 38.85 kN
3.Continuity & Bernoulli

Answer: v = 34.16 m/s

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.

Bernoulli to the stagnation point

The flow comes to rest at the tip, so its kinetic energy shows up as extra pressure.

p0 − p = ½ρv²
v = √(2·700/1.2) = 34.16 m/s

Answer

v = 34.16 m/s
4.Continuity & Bernoulli

Answer: p2 = 98.66 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 = 0.75·(100/25)² = 12 m/s
½ρ(v1² − v2²) = ½·1000·(0.75² − 12²)/1000 = −71.72 kPa
ρgΔz = 1000·9.81·2/1000 = 19.62 kPa
p2 = p1 + ½ρ(v1² − v2²) − ρgΔz = 190 + (−71.72) − 19.62 = 98.66 kPa

Answer

p2 = 98.66 kPa
5.Pipe friction & head loss

Answer: hf = 3.411 m

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 hf = f·(L/D)·V²/(2g). Fittings, valves, the entrance and the exit add minor losses hm = ΣK·V²/(2g). Between two open reservoir surfaces the energy equation gives Δz = hf + hm, with the exit loss K = 1 included.

Mean velocity

A = π·0.25²/4 = 0.04909 m²
V = Q/A = 0.06/0.04909 = 1.222 m/s

Velocity head

V²/(2g) = 1.222²/(2·9.81) = 0.07615 m

Darcy–Weisbach

hf = f·(L/D)·V²/(2g) = 0.028·(400/0.25)·1.222²/(2·9.81) = 3.411 m

Answer

hf = 3.411 m
6.Pipe friction & head loss

Answer: H = 14.92 m

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 hf = f·(L/D)·V²/(2g). Fittings, valves, the entrance and the exit add minor losses hm = ΣK·V²/(2g). Between two open reservoir surfaces the energy equation gives Δz = hf + hm, with the exit loss K = 1 included.

Velocity

V = Q/A = 0.1/0.03142 = 3.183 m/s
V²/(2g) = 0.5164 m

Loss coefficients

f·L/D = 0.022·150/0.2 = 16.5
ΣK = 0.5 + 3·0.3 + 10 = 11.4

Energy equation

The outlet jet still carries its velocity head; it is not a loss but it has to be supplied.

H = (1 + 16.5 + 11.4)·0.5164 = 14.92 m

Answer

H = 14.92 m
7.Pumps & pump power

Answer: Pshaft = 78.48 kW

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

Hydraulic power

Ph = ρ·g·Q·H = 1000·9.81·0.1·52 = 51.01 kW

Shaft power

Pshaft = Ph/η = 51.01/0.65 = 78.48 kW

Answer

Pshaft = 78.48 kW
8.Pumps & pump power

Answer: H = 30.29 m

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

Velocity

V = Q/A = 0.05/0.03142 = 1.592 m/s
V²/(2g) = 0.1291 m

Head losses

hL = (f·L/D + ΣK)·V²/(2g) = (33 + 5)·0.1291 = 4.906 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) + hL = 5 + 20.39 + 4.906 = 30.29 m

Answer

H = 30.29 m
9.Open-channel flow (Manning)

Answer: Q = 0.03188 m³/s

Manning’s equation (SI): for uniform flow in an open channel V = (1/n)·R2/3·S1/2 and Q = A·V, with n the roughness coefficient, S the bed slope (m/m) and R = A/P the hydraulic radius: flow area divided by wetted perimeter. Only the boundary in contact with the water counts in P, not the free surface. Rectangle: A = b·y, P = b + 2y. Trapezoid with side slopes z:1 (horizontal:vertical): A = (b + z·y)·y, P = b + 2y·√(1 + z²). A circular pipe flowing full or half full has R = D/4.

Geometry

A = 0.07952 m², R = D/4 = 0.1125 m

Velocity

V = (1/0.013)·0.11252/3·0.00051/2 = 0.4008 m/s

Flow rate

Q = A·V = 0.07952·0.4008 = 0.03188 m³/s

Answer

Q = 0.03188 m³/s
10.Open-channel flow (Manning)

Answer: S = 0.001963 m/m

Manning’s equation (SI): for uniform flow in an open channel V = (1/n)·R2/3·S1/2 and Q = A·V, with n the roughness coefficient, S the bed slope (m/m) and R = A/P the hydraulic radius: flow area divided by wetted perimeter. Only the boundary in contact with the water counts in P, not the free surface. Rectangle: A = b·y, P = b + 2y. Trapezoid with side slopes z:1 (horizontal:vertical): A = (b + z·y)·y, P = b + 2y·√(1 + z²). A circular pipe flowing full or half full has R = D/4.

Geometry

A = b·y = 5.5·2.4 = 13.2 m²
P = b + 2y = 5.5 + 2·2.4 = 10.3 m
R = A/P = 1.282 m

Solve Manning for S

S1/2 = n·Q/(A·R2/3) = 0.015·46/(13.2·1.18) = 0.0443
S = 0.0443² = 0.001963

Answer

S = 0.001963

That is a fall of 1.963 m per kilometre.

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