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)
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
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)
Time value of money
Future value
FV = PV·(1 + i)n
Present value
PV = FV/(1 + i)n
Several periods per year
i = r/m, N = m·n
Annuity, present value
PV = PMT·[1 − (1 + i)−n]/i
Annuity, future value
FV = PMT·[(1 + i)n − 1]/i
Method
Draw a timeline with every cash flow and its timing.
Match the rate to the period: a monthly rate for monthly payments.
Use FV = PV·(1 + i)ⁿ for single amounts and the annuity formulas for equal payments.
Check the sign and the order of magnitude of the answer.
NPV & IRR
Net present value
NPV = −C0 + Σ CFt/(1 + r)t
Equal cash flows
NPV = −C0 + CF·[1 − (1 + r)−n]/r
Internal rate of return
the r at which NPV = 0
Decision
accept when NPV > 0 (or IRR > required return)
Method
List all cash flows with their year; the investment at year 0 is negative.
Discount each cash flow: CFt/(1 + r)t.
Add them up to get the NPV. Positive means the project earns more than r.
For the IRR, find the rate that makes NPV zero by trial or interpolation.
Normal distribution
z-score
z = (x − μ)/σ
Below x
P(X < x) = Φ(z)
Above x
P(X > x) = 1 − Φ(z)
Between
Φ(z2) − Φ(z1)
Percentile
x = μ + z·σ
Method
Convert the value to a z-score: z = (x − μ)/σ.
Look up Φ(z), the area to the left of z.
For the area to the right use 1 − Φ(z); for an interval subtract the two left areas.
For a percentile, work backwards: find z for the area, then x = μ + z·σ.
2Practice problems
1.Beam support reactionsMedium
The simply supported beam has a pin at A and a roller at B. Find the vertical support reaction RA.
L = 8 mP1 = 20 kN at 3 mP2 = 45 kN at 7 m
RA = kN
2.Beam support reactionsHard
The simply supported beam has a pin at A and a roller at B. Find the vertical support reaction RB.
L = 8 mP = 60 kN at 7 mw = 12 kN/m from 2 to 3 m
RB = kN
3.Truss: method of jointsMedium
Use the method of joints to find the force FAC in member AC. Give tension as positive and compression as negative.
span = 5 mheight = 3 mB is 3 m from Avertical load = 40 kN
FAC = kN
4.Truss: method of jointsHard
Use the method of joints to find the force FAC in member AC. Give tension as positive and compression as negative.
span = 6 mheight = 4 mB is 5 m from Avertical load = 25 kNhorizontal load = 10 kN ←
FAC = kN
5.Shear force & bending momentMedium
The simply supported beam carries a clockwise couple M0 = 30 kN·m at x = 4 m from A, and no other load. Find the bending moment Mx just to the left of the couple. Use sagging moments positive and upward shear on the left face positive.
L = 10 mM0 = 30 kN·m clockwise, at 4 m
Mx = kN·m
6.Shear force & bending momentHard
The marks A to G split the beam into six equal parts. At which mark is the bending moment largest in size, sagging or hogging? Click it in the diagram.
40 kN @ 6 m55 kN @ 3 m8 kN/m, 0–4 m
1A (x = 0 m)
2B (x = 1 m)
3C (x = 2 m)
4D (x = 3 m)
5E (x = 4 m)
6F (x = 5 m)
7G (x = 6 m)
7.Beam deflectionMedium
A simply supported beam carries a uniformly distributed load w over its whole span. Find the maximum deflection δmax, at midspan.
w = 2 kN/mL = 6 mE = 70 GPa (aluminium)I = 160 × 10⁶ mm⁴
δmax = mm
8.Beam deflectionHard
A simply supported beam carries a point load P at b = 1.5 m from support B. Find the maximum deflection δmax of the beam.
P = 21 kNb = 1.5 mL = 4 mE = 70 GPa (aluminium)I = 57 × 10⁶ mm⁴
δmax = mm
9.Column bucklingMedium
A column of length L made of steel is pinned at both ends. Using Euler’s formula, find its critical buckling load Pcr.
L = 6 mE = 200 GPa (steel)d = 80 mm
Pcr = kN
10.Column bucklingHard
A solid round column of length L made of steel is pinned at both ends. It must carry 60 kN with a factor of safety of 2 against buckling. Find the smallest diameter d.
P = 60 kNn = 2L = 2.5 mE = 200 GPa (steel)
d = mm
11.Centroid & second moment of areaMedium
Find the second moment of area Ix of the T-section about the horizontal axis x through its centroid.
bf = 100 mmtf = 25 mmtw = 16 mmhw = 160 mm
Ix = × 10⁶ mm⁴
12.Centroid & second moment of areaHard
A 120 mm × 240 mm plate has a rectangular cut-out 50 mm wide and 50 mm high, centred on the vertical centre line with its centre 144 mm above the bottom. Find the second moment of area Ix about the horizontal axis through the centroid.
b = 120 mmh = 240 mmcut-out: 50 × 50 mmhole centre: y = 144 mm
Ix = × 10⁶ mm⁴
13.Effective stress in soilMedium
For the soil profile shown, find the total vertical stress σ at point X.
A 4 m thick overconsolidated clay layer has Cc = 0.2, Cr = 0.03 and e₀ = 0.6. At its mid-depth the effective vertical stress is 50 kPa and the preconsolidation pressure is 130 kPa. A new building adds 20 kPa of vertical stress at mid-depth. Find the primary consolidation settlement S in mm.
A clay layer 9.5 m thick has a coefficient of consolidation cv = 1.2 m²/year. It lies on impervious rock, with sand above it, so water drains out only at the top. For 60% average consolidation the time factor is Tv = 0.287. How many years t does the layer take to reach 60% consolidation?
A vertical rectangular gate 2 m wide sits in the wall of a tank of water, with its top edge 3 m below the surface. Find the resultant hydrostatic force F on the gate.
d = 3 mH = 3 mb = 2 mρ = 1000 kg/m³g = 9.81 m/s²
F = kN
18.Hydrostatic forceHard
A vertical rectangular gate 1.5 m wide sits in the wall of a tank of glycerin, with its top edge 2.5 m below the surface. Find the depth ycp of the centre of pressure below the surface.
Water flows at a mean velocity of 1.1 m/s through a pipe 300 m long with an inside diameter of 200 mm. Use the Darcy friction factor f = 0.015 and g = 9.81 m/s². Find the friction head loss hf.
A pipe 400 m long with an inside diameter of 300 mm (Darcy friction factor f = 0.018) 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), 2 bends (K = 0.3 each) and a valve (K = 5). Use g = 9.81 m/s². How far H must the reservoir surface be above the pipe outlet for a flow rate of 75 L/s?
A trapezoidal unfinished concrete channel has a bottom width of 3 m and side slopes of 1.5:1 (horizontal:vertical). Water flows uniformly 1.2 m deep. Manning n = 0.014 and the bed slope is S = 0.003. Find the flow rate Q in m³/s.
b = 3 my = 1.2 mz = 1.5n = 0.014S = 0.003
Q = m³/s
22.Open-channel flow (Manning)Hard
A trapezoidal gravel channel with a bottom width of 2.5 m and side slopes of 1:1 (horizontal:vertical) must carry 25 m³/s in uniform flow at a depth of 2.2 m. Manning n = 0.025. Find the required bed slope S (in m/m).
Q = 25 m³/sb = 2.5 my = 2.2 mz = 1n = 0.025
S = m/m
23.Pumps & pump powerMedium
In a test, a pump delivers 15 L/s of water (ρ = 1000 kg/m³) against a head of 72 m while its shaft takes 12.9 kW. Use g = 9.81 m/s². Find the pump efficiency η in percent.
Q = 15 L/sH = 72 mPshaft = 12.9 kWg = 9.81 m/s²
η = %
24.Pumps & pump powerHard
A pump moves 80 L/s of water (ρ = 1000 kg/m³) from an open lower reservoir to an upper tank whose water surface is 19 m higher. The pipe is 600 m long with an inside diameter of 200 mm and a Darcy friction factor f = 0.018; the minor-loss coefficients add up to ΣK = 6 (entrance and exit included). Use g = 9.81 m/s². Find the head H the pump must add.
You need €10 000 in 2 years. An account pays 3.6% per year, compounded monthly. How much must you deposit today? Find the present value PV.
FV = €10 0003.6% / 12n = 2
PV = €
26.Time value of moneyHard
A loan of €150 000 is repaid with equal monthly payments over 25 years. The interest rate is 4.2% per year, compounded monthly. Find the monthly payment A.
P = €150 0004.2% / 12N = 300
A = €
27.NPV & IRRMedium
An investment of €45 000 gives these cash flows at the end of years 1 to 3: €22 000, €17 000, €11 000. The cost of capital is 7.000000000000001%. Find the net present value NPV.
Project A costs €20 000 and returns €11 000, €8 000, €4 500 at the end of years 1 to 3. Project B costs €22 000 and returns €5 500, €8 500, €12 000. Find the crossover rate r* at which both projects have the same NPV, in percent.
The masses of bags of cement are independent and normal with mean 25 kg and standard deviation 0.5 kg. Find the probability P that the total mass of 12 of them exceeds 303.5 kg. Round z to two decimals.
μ = 25 kgσ = 0.5 kgn = 12> 303.5 kg
P =
30.Normal distributionHard
Hole diameters D are normal with mean 25.04 mm and standard deviation 0.01 mm. Shaft diameters d are independent and normal with mean 25 mm and standard deviation 0.015 mm. A randomly chosen shaft fits when D − d > 0. Find the probability P that it fits. Round z to two decimals.
hole: μ = 25.04 mm, σ = 0.01 mmshaft: μ = 25 mm, σ = 0.015 mm
P =
3Solutions
1.Beam support reactions
Answer: RA = 18.13 kN
Static equilibrium: a body at rest has ΣFx = 0, ΣFy = 0 and ΣM = 0 about any point. Taking moments about one support removes that support’s reaction from the equation.
Free-body diagram
Replace the supports with reaction forces. A roller gives one vertical reaction; with only vertical loads the pin gives one vertical reaction too.
Equilibrium
Moments about A, counter-clockwise positive. Then vertical force balance.
ΣMA = 0: RB·8 = 20·3 + 45·7
RB = 375/8 = 46.88 kN
ΣFy = 0: RA = 65 − 46.88 = 18.13 kN
Answer
RA = 18.13 kN
2.Beam support reactions
Answer: RB = 56.25 kN
Static equilibrium: a body at rest has ΣFx = 0, ΣFy = 0 and ΣM = 0 about any point. Taking moments about one support removes that support’s reaction from the equation.
Free-body diagram
Replace the supports with reaction forces. A roller gives one vertical reaction; with only vertical loads the pin gives one vertical reaction too.
Equilibrium
Moments about A, counter-clockwise positive. Then vertical force balance.
UDL resultant: W = w·ℓ = 12·1 = 12 kN, acting at x̄ = 2.5 m
ΣMA = 0: RB·8 = 60·7 + 12·1·2.5
RB = 450/8 = 56.25 kN
ΣFy = 0: RA = 72 − 56.25 = 15.75 kN
Answer
RB = 56.25 kN
3.Truss: method of joints
Answer: FAC = 16 kN
Method of joints: every pin of a truss is in equilibrium, so ΣFx = 0 and ΣFy = 0 at each joint. Start at a joint with at most two unknown member forces. A negative result means the member is in compression.
Support reactions
Equilibrium of the whole truss. Moments about A, counter-clockwise positive.
ΣMA = 0: Cy·5 = 40·3 → Cy = 24 kN
ΣFy = 0: Ay = 40 − 24 = 16 kN
Joint C
The roller gives only a vertical reaction, so joint C has just two unknown member forces. Assume both in tension.
sin γ = 3/3.606 = 0.8321, cos γ = 2/3.606 = 0.5547
Method of joints: every pin of a truss is in equilibrium, so ΣFx = 0 and ΣFy = 0 at each joint. Start at a joint with at most two unknown member forces. A negative result means the member is in compression.
Support reactions
Equilibrium of the whole truss. Moments about A, counter-clockwise positive.
ΣMA = 0: Cy·6 = 25·5 − 10·4 → Cy = 14.17 kN
ΣFy = 0: Ay = 25 − 14.17 = 10.83 kN
ΣFx = 0: Ax = 10 kN
Joint C
The roller gives only a vertical reaction, so joint C has just two unknown member forces. Assume both in tension.
sin γ = 4/4.123 = 0.9701, cos γ = 1/4.123 = 0.2425
Method of sections: cut the beam where you want the internal forces and keep one side. The shear force V balances the vertical forces on that side, and the bending moment M balances their moments about the cut. An applied couple makes the bending moment diagram jump by the size of the couple.
Support reactions
Moments about A, counter-clockwise positive: RB·L − M0 = 0. Vertical balance: RA + RB = 0.
RB = M0/L = 30/10 = 3 kN (upward)
RA = −RB = −3 kN (downward)
Cut just left of the couple
The left part contains only RA.
Mx = RA·a = −3·4 = −12 kN·m
Answer
Mx = −12 kN·m
6.Shear force & bending moment
Answer: E (x = 4 m)
Largest bending moment: M changes slope wherever the shear force changes, so its peaks sit where the shear force crosses zero: under a point load, inside a distributed load, or over a support of an overhang. At a fixed support of a cantilever the moment is largest at the wall. Compare the size of M at those places, sagging or hogging.
Support reactions
Take moments about one support, then use the vertical force balance.
R1 = 9.75 kN, R2 = 117.3 kN
Bending moment at every mark
Sum the moments of all forces on one side of the cut. Sagging is positive, hogging negative.
MA = 0, MB = 5.75, MC = 3.5, MD = −6.75, ME = −80 kN·m, MF = −40, MG = 0
Answer
Mark E: ME = −80 kN·m
7.Beam deflection
Answer: δmax = 3.013 mm
Beam deflection: deflections come from integrating the curvature M/(EI) twice. Standard cases are tabulated, for example PL³/(3EI) for a cantilever with an end load and 5wL⁴/(384EI) for a simply supported beam under a full uniform load. Deflections from separate loads add (superposition).
Consistent units
Work in N and mm: P in N, w in N/mm (kN/m = N/mm), L in mm, E in N/mm² (GPa × 1000), I in mm⁴.
w = 2 N/mm, L = 6000 mm
EI = 1.12 × 10¹³ N·mm²
Deflection
δmax = 5wL⁴/(384EI) = 5·2·6000⁴/(384·1.12 × 10¹³) = 3.013 mm
Answer
δmax = 3.013 mm
8.Beam deflection
Answer: δmax = 6.455 mm
Beam deflection: deflections come from integrating the curvature M/(EI) twice. Standard cases are tabulated, for example PL³/(3EI) for a cantilever with an end load and 5wL⁴/(384EI) for a simply supported beam under a full uniform load. Deflections from separate loads add (superposition).
Consistent units
Work in N and mm: P in N, w in N/mm (kN/m = N/mm), L in mm, E in N/mm² (GPa × 1000), I in mm⁴.
P = 21000 N, b = 1500 mm, L = 4000 mm
EI = 3.99 × 10¹² N·mm²
Position of the maximum
Setting the slope in the longer segment to zero gives the position.
x = √((L² − b²)/3) = √((4000² − 1500²)/3) = 2141 mm
Maximum deflection
δmax = Pb(L² − b²)3/2/(9√3·EIL) = 6.455 mm
Answer
δmax = 6.455 mm
9.Column buckling
Answer: Pcr = 110.2 kN
Euler buckling: a slender column becomes unstable at Pcr = π²EI/(KL)², where KL is the effective length: K = 1 for pinned–pinned, 2 for fixed–free, 0.7 for fixed–pinned and 0.5 for fixed–fixed. It buckles about the axis with the smallest I. The formula holds for slender columns, whose critical stress stays below the yield stress.
Euler buckling: a slender column becomes unstable at Pcr = π²EI/(KL)², where KL is the effective length: K = 1 for pinned–pinned, 2 for fixed–free, 0.7 for fixed–pinned and 0.5 for fixed–fixed. It buckles about the axis with the smallest I. The formula holds for slender columns, whose critical stress stays below the yield stress.
Required critical load
Pcr = n·P = 2·60000 = 120000 N
KL = 1·2500 = 2500 mm
Solve for the diameter
d = (64·n·P·(KL)²/(π³E))^(1/4) = (64·120000·2500²/(π³·200000))^(1/4) = 52.75 mm
Answer
d = 52.75 mm
Check: the slenderness KL/r is 189.6, so the column is slender and Euler applies.
11.Centroid & second moment of area
Answer: Ix = 16.41 × 10⁶ mm⁴
Composite areas: split the section into rectangles. The centroid is the area-weighted average ȳ = ΣAᵢyᵢ/ΣAᵢ. The second moment of area about the centroidal axis adds each part’s own bh³/12 and its parallel-axis term A·d², where d is the distance from the part’s centroid to the overall centroid. Bending stress is σ = M·y/I.
Split into two rectangles
Measure every y from the bottom edge.
flange: Af = 100·25 = 2500 mm², yf = 160 + 25/2 = 172.5 mm
Sections with holes: treat a hole as a negative area. The centroid is ȳ = (A₁y₁ − A₂y₂)/(A₁ − A₂), with A₁, y₁ for the full plate and A₂, y₂ for the hole. For the second moment of area about the centroidal axis, use the parallel-axis theorem for each part and subtract the hole: I = (Ic1 + A₁d₁²) − (Ic2 + A₂d₂²), where d is the distance from each part's own centroid to the axis through ȳ. A rectangle has Ic = bh³/12 and a circle Ic = πd⁴/64.
Centroid
ȳ = (28800·120 − 2500·144)/(28800 − 2500) = 117.7 mm
Full plate about ȳ
120·240³/12 + 28800·2.281² = 138.4 × 10⁶ mm⁴
Hole about ȳ
50·50³/12 + 2500·26.28² = 2.248 × 10⁶ mm⁴
Subtract
Ix = 136.1 × 10⁶ mm⁴
Answer
Ix = 136.1 × 10⁶ mm⁴
13.Effective stress in soil
Answer: σ = 107 kPa
Effective stress (Terzaghi): the soil skeleton carries σ′ = σ − u. The total stress σ is the weight of everything above the point, Σγ·h, using the dry unit weight above the water table and the saturated unit weight below it. Below the water table the pore water pressure is hydrostatic: u = γw·(depth below the water table).
Total stress
Add the weight of each soil band above X. Above the water table use the dry unit weight, below it the saturated one.
Effective stress (Terzaghi): the soil skeleton carries σ′ = σ − u. The total stress σ is the weight of everything above the point, Σγ·h, using the dry unit weight above the water table and the saturated unit weight below it. Below the water table the pore water pressure is hydrostatic: u = γw·(depth below the water table).
Total stress
Add the weight of each soil band above X. Above the water table use the dry unit weight, below it the saturated one.
σ = γd·1 + γsat,sand·2 + γsat,clay·2
σ = 15·1 + 18.5·2 + 17·2 = 86 kPa
Pore water pressure
Water pressure grows with depth below the water table.
u = γw·(z − zw) = 9.81·4 = 39.24 kPa
Effective stress
σ′ = σ − u = 86 − 39.24 = 46.76 kPa
Answer
σ′ = 46.76 kPa
15.Consolidation settlement
Answer: S = 10.96 mm
Primary consolidation of a clay layer of thickness H, using the effective stress at the middle of the layer: σ′f = σ′0 + Δσ. Normally consolidated clay: S = Cc·H/(1 + e0)·log₁₀(σ′f/σ′0). Overconsolidated clay recompresses along Cr up to the preconsolidation pressure σ′p and follows Cc only beyond it. Time: t = Tv·Hdr²/cv, where the drainage path Hdr is H/2 when water can leave at the top and bottom, and H when only one side drains.
Compare with the preconsolidation pressure
σ′f = 50 + 20 = 70 kPa ≤ 130 kPa
Settlement
The clay stays on its recompression line.
S = Cr·H/(1 + e0)·log₁₀(σ′f/σ′0) = 0.03·4/(1 + 0.6)·log₁₀(70/50) = 10.96 mm
Answer
S = 10.96 mm
16.Consolidation settlement
Answer: t = 21.58 years
Primary consolidation of a clay layer of thickness H, using the effective stress at the middle of the layer: σ′f = σ′0 + Δσ. Normally consolidated clay: S = Cc·H/(1 + e0)·log₁₀(σ′f/σ′0). Overconsolidated clay recompresses along Cr up to the preconsolidation pressure σ′p and follows Cc only beyond it. Time: t = Tv·Hdr²/cv, where the drainage path Hdr is H/2 when water can leave at the top and bottom, and H when only one side drains.
Drainage path
Hdr = H = 9.5 m
Time
t = Tv·Hdr²/cv = 0.287·9.5²/1.2 = 21.58 years
Answer
t = 21.58 years
17.Hydrostatic force
Answer: F = 264.9 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 = 3 + 3/2 = 4.5 m
A = H·b = 3·2 = 6 m²
Resultant force
F = ρ·g·yc·A = 1000·9.81·4.5·6 = 264.9 kN
Answer
F = 264.9 kN
18.Hydrostatic force
Answer: ycp = 3.308 m
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 = 2.5 + 1.5/2 = 3.25 m
A = H·b = 1.5·1.5 = 2.25 m²
Resultant force
F = ρ·g·yc·A = 1260·9.81·3.25·2.25 = 90.39 kN
Centre of pressure
Pressure grows with depth, so the resultant acts below the centroid.
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 head
V²/(2g) = 1.1²/(2·9.81) = 0.06167 m
Darcy–Weisbach
hf = f·(L/D)·V²/(2g) = 0.015·(300/0.2)·1.1²/(2·9.81) = 1.388 m
Answer
hf = 1.388 m
20.Pipe friction & head loss
Answer: H = 1.785 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 = 0.075/0.07069 = 1.061 m/s
V²/(2g) = 0.05738 m
Loss coefficients
f·L/D = 0.018·400/0.3 = 24
ΣK = 0.5 + 2·0.3 + 5 = 6.1
Energy equation
The outlet jet still carries its velocity head; it is not a loss but it has to be supplied.
H = (1 + 24 + 6.1)·0.05738 = 1.785 m
Answer
H = 1.785 m
21.Open-channel flow (Manning)
Answer: Q = 19.2 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 = (b + z·y)·y = (3 + 1.5·1.2)·1.2 = 5.76 m²
P = b + 2y·√(1 + z²) = 3 + 2·1.2·√(1 + 1.5²) = 7.327 m
R = A/P = 0.7862 m
Velocity
V = (1/0.014)·0.78622/3·0.0031/2 = 3.333 m/s
Flow rate
Q = A·V = 5.76·3.333 = 19.2 m³/s
Answer
Q = 19.2 m³/s
22.Open-channel flow (Manning)
Answer: S = 0.002912 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 + z·y)·y = (2.5 + 1·2.2)·2.2 = 10.34 m²
P = b + 2y·√(1 + z²) = 2.5 + 2·2.2·√(1 + 1²) = 8.723 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.
Hydraulic power
Ph = ρ·g·Q·H = 1000·9.81·0.015·72 = 10.59 kW
Efficiency
η = Ph/Pshaft = 10.59/12.9 = 82.13%
Answer
η = 82.13%
24.Pumps & pump power
Answer: H = 38.83 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.
Both surfaces are open and practically at rest, so pressure and velocity terms drop out.
H = Δz + hL = 19 + 19.83 = 38.83 m
Answer
H = 38.83 m
25.Time value of money
Answer: PV = 9306 €
Time value of money: money today is worth more than the same amount later, because it can earn interest. With interest rate i per period, an amount grows as FV = PV·(1 + i)n. A series of equal payments (an annuity) is valued by adding up each payment, which gives the annuity formulas.
Rate and number of periods
i = 0.036000000000000004/12 = 0.003
N = 12·2 = 24
Present value
PV = FV/(1 + i)N = 10 000/1.075 = €9 306.31
Answer
PV = €9 306.31
26.Time value of money
Answer: A = 808.4 €
Time value of money: money today is worth more than the same amount later, because it can earn interest. With interest rate i per period, an amount grows as FV = PV·(1 + i)n. A series of equal payments (an annuity) is valued by adding up each payment, which gives the annuity formulas.
Monthly rate and number of payments
i = 0.042/12 = 0.0035
N = 12·25 = 300
Payment
The present value of N equal payments A is A·(1 − (1 + i)⁻ᴺ)/i. Set it equal to the loan and solve for A.
(1 + i)−N = 0.3506
A = 150 000·0.0035/(1 − 0.3506) = €808.41
Answer
A = €808.41
27.NPV & IRR
Answer: NPV = −611.5 €
Net present value: discount every cash flow back to today with the required rate of return r, then add them up: NPV = Σ CFₜ/(1 + r)ᵗ. A project with NPV > 0 earns more than r and adds value. The internal rate of return (IRR) is the rate at which NPV = 0.
Present value of each cash flow
CF0 = −45 000
CF1/(1 + 0.07)1 = 22 000/1.07 = 20 560.75
CF2/(1 + 0.07)2 = 17 000/1.145 = 14 848.46
CF3/(1 + 0.07)3 = 11 000/1.225 = 8 979.28
Add them up
NPV = €−611.52
Answer
NPV = €−611.52
NPV is negative, so the project earns less than the required return.
28.NPV & IRR
Answer: r* = 2.969 %
Crossover rate: the discount rate at which two projects have the same NPV. It is the IRR of the difference in their cash flows (B − A). Below it the project with the later, larger cash flows has the higher NPV; above it the other one wins.
Difference in cash flows
ΔCF0 = −22 000 − (−20 000) = −2 000
ΔCF1 = 5 500 − 11 000 = −5 500
ΔCF2 = 8 500 − 8 000 = 500
ΔCF3 = 12 000 − 4 500 = 7 500
IRR of the difference
NPVΔ(2%) = 155.85
NPVΔ(3%) = −4.95
r* = 2.969%
Answer
r* = 2.969%
Check: at 2.969% both NPVs are €2 350.15.
29.Normal distribution
Answer: P = 0.02169
Sums and differences of normal variables: if X and Y are independent and normal, X + Y and X − Y are normal too. Means add or subtract: E(X ± Y) = μX ± μY. Variances always add, also for a difference: Var(X ± Y) = σX² + σY², so σ = √(σX² + σY²). Standard deviations never add directly. The total of n independent items with the same distribution has mean n·μ and standard deviation σ·√n. Then standardise as usual: z = (x − mean)/σ and read Φ(z).
Distribution of the total
μT = 300 kg, σT = 0.5·√12 = 1.732 kg
Standardise
z = (303.5 − 300)/1.732 = 2.02
Probability
P = 1 − Φ(2.02) = 0.02169
Answer
P = 0.02169
30.Normal distribution
Answer: P = 0.9868
Sums and differences of normal variables: if X and Y are independent and normal, X + Y and X − Y are normal too. Means add or subtract: E(X ± Y) = μX ± μY. Variances always add, also for a difference: Var(X ± Y) = σX² + σY², so σ = √(σX² + σY²). Standard deviations never add directly. The total of n independent items with the same distribution has mean n·μ and standard deviation σ·√n. Then standardise as usual: z = (x − mean)/σ and read Φ(z).
Distribution of the difference
μ = 25.04 − 25 = 0.04 mm, σ = 0.01803 mm
Standardise
z = (0 − 0.04)/0.01803 = −2.22
Probability
P = 1 − Φ(−2.22) = 0.9868
Answer
P = 0.9868
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