Machine Design: cram pack

Formula sheets, the key method steps for every topic and 12 practice problems, with full solutions at the back.

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1Formulas and methods

Gears & gear trains

Meshing gears
n1·N1 = n2·N2
Torque
T2 = T1·(N2/N1)·η
Power
P = T·ω, ω = 2π·n/60
Compound train
total ratio = product of the stage ratios

Torsion of shafts

Shear stress
τ = T·r/J
Solid shaft
J = πd⁴/32
Hollow shaft
J = π(D⁴ − d⁴)/32
Angle of twist
φ = TL/(GJ)
Power
P = T·ω = 2πnT/60

Method

  1. Find the polar moment of area: J = πd⁴/32 for a solid shaft.
  2. Shear stress at the surface: τ = T·r/J, with r the outer radius.
  3. Angle of twist: φ = TL/(GJ) in radians.
  4. If power is given, find the torque first with P = T·ω, ω = 2πn/60.

Mohr’s circle & stress transformation

Centre
C = (σx + σy)/2
Radius
R = √(((σx − σy)/2)² + τxy²)
Principal stresses
σ1,2 = C ± R
Principal direction
tan 2θp = 2τxy/(σx − σy)
Inclined plane
σθ = C + (σx − σy)/2·cos 2θ + τxy·sin 2θ

Method

  1. Calculate the centre of Mohr’s circle: C = (σx + σy)/2.
  2. Calculate the radius: R = √(((σx − σy)/2)² + τxy²).
  3. The principal stresses are C ± R and the largest in-plane shear stress is R.
  4. Angles on the circle are double the angles on the element: tan 2θp = 2τxy/(σx − σy).

Axial stress & strain

Normal stress
σ = F/A
Strain
ε = ΔL/L
Hooke’s law
σ = E·ε
Elongation
ΔL = FL/(EA)
Thermal strain
εT = α·ΔT

Column buckling

Euler load
Pcr = π²EI/(KL)²
Effective length factor
K = 1 pinned–pinned, 0.5 fixed–fixed, 0.7 fixed–pinned, 2 fixed–free
Critical stress
σcr = Pcr/A
Slenderness
λ = KL/r, r = √(I/A)

Mechanical vibrations

Natural frequency
ωn = √(k/m), fn = ωn/(2π)
From static deflection
ωn = √(g/δst)
Critical damping
cc = 2√(km) = 2mωn
Damping ratio
ζ = c/cc
Damped frequency
ωd = ωn√(1 − ζ²)
Logarithmic decrement
δ = (1/n)·ln(x0/xn), ζ = δ/√(4π² + δ²)
Springs in parallel
k = k1 + k2
Springs in series
1/k = 1/k1 + 1/k2

2Practice problems

1.Gears & gear trainsMedium
Nw​ = 72z = 3, 1440 rpm

A worm with 3 start(s) turns at 1440 rpm and drives a worm wheel with 72 teeth. Find the speed nw of the wheel.

z = 3Nw = 72n = 1440 rpm
nw = rpm
2.Gears & gear trainsHard
A = 30B = 60C = 16D = ?

In a compound gear train, gear A (30 teeth) on the input shaft turns at 1440 rpm and drives gear B (60 teeth). Gear C (16 teeth) is fixed to the same shaft as B and drives gear D on the output shaft. The output must turn at 192 rpm. How many teeth ND must gear D have?

nin = 1440 rpmA = 30B = 60C = 16nout = 192 rpm
ND =
3.Torsion of shaftsMedium
T = 100 N·md = 30 mmL = 1.5 mφ = ?

A solid aluminium shaft is fixed at the wall and twisted by a torque T at its free end. Find the angle of twist φ of the free end, in degrees.

T = 100 N·md = 30 mmL = 1.5 mG = 26 GPa
φ = °
4.Torsion of shaftsHard
Td = ?

A solid shaft must transmit 50 kW at 1000 rpm without the shear stress exceeding 75 MPa. Find the smallest diameter d that works.

P = 50 kWN = 1000 rpmτallow = 75 MPa
d = mm
5.Mohr’s circle & stress transformationMedium
σx​ = 80σy​ = 90τxy​ = 50MPa

A point in a loaded part has σₓ = 80 MPa, σᵧ = 90 MPa and τₓᵧ = 50 MPa (tension positive). Find the maximum in-plane shear stress τmax.

σx = 80 MPaσy = 90 MPaτxy = 50 MPa
τmax = MPa
6.Mohr’s circle & stress transformationHard
55°D = 1000 mm, t = 8 mm, p = 0.8 MPap

A thin-walled cylindrical tank of inner diameter 1000 mm and wall thickness 8 mm holds gas at a gauge pressure of 0.8 MPa. It is made from plate welded along a helical seam at 55° to the axis of the cylinder. Find the normal stress σn acting across the weld seam.

D = 1000 mmt = 8 mmp = 0.8 MPaα = 55°
σn = MPa
7.Axial stress & strainMedium
Ø 12 mmSteel0.5 mP = 90 kN

Find the elongation δ of the steel bar under the axial load.

P = 90 kNd = 12 mmL = 0.5 mE = 200 GPa
δ = mm
8.Axial stress & strainHard
Ø 30 mmBrass1.5 mØ 16 mmAluminium1 mP = 120 kN

The stepped bar is fixed at the wall and loaded at its free end. Find the largest normal stress σmax in the bar.

P = 120 kNsegment 1: Ø30 mm, 1.5 m, brass (E = 100 GPa)segment 2: Ø16 mm, 1 m, aluminium (E = 70 GPa)
σmax = MPa
9.Column bucklingMedium
PL = 3 md = 80 mmcross-section

A column of length L made of steel is pinned at both ends. Using Euler’s formula, find its critical buckling load Pcr.

L = 3 mE = 200 GPa (steel)d = 80 mm
Pcr = kN
10.Column bucklingHard
P = 45 kNL = 3 md = ?cross-section

A solid round column of length L made of steel is pinned at both ends. It must carry 45 kN with a factor of safety of 2.5 against buckling. Find the smallest diameter d.

P = 45 kNn = 2.5L = 3 mE = 200 GPa (steel)
d = mm
11.Mechanical vibrationsMedium
tx40 mm1 cycle35.3 mm

In a free-vibration test of a damped mass–spring system, a displacement peak of 40 mm is followed one cycle later by a peak of 35.3 mm. Find the damping ratio ζ.

x0 = 40 mmx1 = 35.3 mmn = 1
ζ =
12.Mechanical vibrationsHard
k1​ = 12k2​ = 40m = 10 kg

A 10 kg mass hangs from two springs connected end to end (in series): the upper spring has k₁ = 12 kN/m and the lower one k₂ = 40 kN/m. Find the equivalent stiffness keq of the spring system in kN/m.

m = 10 kgk1 = 12 kN/mk2 = 40 kN/m
keq = kN/m

3Solutions

1.Gears & gear trains

Answer: nw = 60 rpm

Gear trains: meshing gears have the same speed at the teeth, so n₁·N₁ = n₂·N₂: the gear with fewer teeth turns faster. Gears on one shaft turn at the same speed. Power is passed on (minus losses), so torque goes up when speed goes down: T₂ = T₁·(N₂/N₁)·η, and P = T·ω with ω = 2π·n/60.

Wheel speed

nw = n·z/Nw = 1440·3/72 = 60 rpm

Answer

nw = 60 rpm
2.Gears & gear trains

Answer: ND = 60

Gear trains: meshing gears have the same speed at the teeth, so n₁·N₁ = n₂·N₂: the gear with fewer teeth turns faster. Gears on one shaft turn at the same speed. Power is passed on (minus losses), so torque goes up when speed goes down: T₂ = T₁·(N₂/N₁)·η, and P = T·ω with ω = 2π·n/60.

Intermediate shaft speed

nB = nC = 1440·30/60 = 720 rpm

Teeth on gear D

ND = C·nC/nout = 16·720/192 = 60

Answer

ND = 60
3.Torsion of shafts

Answer: φ = 4.157 °

Torsion of circular shafts: shear stress grows linearly from zero at the centre to τmax = T·r/J at the surface, with J = πd⁴/32 for a solid shaft and J = π(do⁴ − di⁴)/32 for a hollow one. The angle of twist is φ = TL/(GJ) in radians. Power and torque are linked by P = T·ω.

Polar second moment of area

J = π·30⁴/32 = 79522 mm⁴

Angle of twist

φ = TL/(GJ) = 100·1000·1500/(26000·79522) = 0.07255 rad
φ = 0.07255·180/π = 4.157°

Answer

φ = 4.157°
4.Torsion of shafts

Answer: d = 31.89 mm

Torsion of circular shafts: shear stress grows linearly from zero at the centre to τmax = T·r/J at the surface, with J = πd⁴/32 for a solid shaft and J = π(do⁴ − di⁴)/32 for a hollow one. The angle of twist is φ = TL/(GJ) in radians. Power and torque are linked by P = T·ω.

Torque

ω = 2πN/60 = 2π·1000/60 = 104.7 rad/s
T = P/ω = 50000/104.7 = 477.5 N·m

Diameter from the allowable stress

d = ∛(16T/(π·τallow)) = ∛(16·477465/(π·75)) = 31.89 mm

Answer

d = 31.89 mm

In practice you would round up to the next standard size.

5.Mohr’s circle & stress transformation

Answer: τmax = 50.25 MPa

Plane stress transformation: on a plane rotated by θ, σ = (σₓ + σᵧ)/2 + (σₓ − σᵧ)/2·cos 2θ + τₓᵧ·sin 2θ. Mohr’s circle shows all planes at once: its centre is at C = (σₓ + σᵧ)/2 and its radius is R = √(((σₓ − σᵧ)/2)² + τₓᵧ²). The principal stresses are C ± R, and the largest in-plane shear stress is R.

στxyCτmax​

Radius of Mohr’s circle

τmax = R = √(((80 − 90)/2)² + 50²) = 50.25 MPa

Answer

τmax = 50.25 MPa
6.Mohr’s circle & stress transformation

Answer: σn = 33.22 MPa

Plane stress transformation: on a plane rotated by θ, σ = (σₓ + σᵧ)/2 + (σₓ − σᵧ)/2·cos 2θ + τₓᵧ·sin 2θ. Mohr’s circle shows all planes at once: its centre is at C = (σₓ + σᵧ)/2 and its radius is R = √(((σₓ − σᵧ)/2)² + τₓᵧ²). The principal stresses are C ± R, and the largest in-plane shear stress is R. Thin-walled cylinder: hoop stress σh = pr/t and axial stress σa = pr/(2t); these are the principal stresses in the wall.

Wall stresses

r = 1000/2 = 500 mm
σh = pr/t = 0.8·500/8 = 50 MPa
σa = pr/(2t) = 25 MPa

Transform to the seam

Take x along the axis (σa) and y around the hoop (σh). The seam’s normal makes 90° − α with the axis.

σn = 25·sin²55° + 50·cos²55° = 33.22 MPa

Answer

σn = 33.22 MPa
7.Axial stress & strain

Answer: δ = 1.989 mm

Hooke’s law: within the elastic range σ = E·ε. Combining with σ = P/A and ε = δ/L gives δ = PL/(AE).

Stress

A = π·12²/4 = 113.1 mm²
σ = P/A = 90·1000/113.1 = 795.8 MPa

Strain (Hooke’s law)

E for steel = 200 GPa = 200000 MPa.

ε = σ/E = 795.8/200000 = 0.003979 = 3979 µε

Elongation

δ = ε·L = 0.003979·500 mm = 1.989 mm

Answer

δ = 1.989 mm
8.Axial stress & strain

Answer: σmax = 596.8 MPa

Axially loaded members: each prismatic segment obeys δ = PL/(AE). For members in series the elongations add.

Same force in both segments

The free end carries P, so every section of the bar carries the same axial force P. Only the areas and materials change.

A1 = π·30²/4 = 706.9 mm², A2 = π·16²/4 = 201.1 mm²
σ1 = 169.8 MPa
σ2 = 596.8 MPa

Largest stress

The thinner segment has the smaller area, so it carries the larger stress.

σmax = 596.8 MPa

Answer

σmax = 596.8 MPa
9.Column buckling

Answer: Pcr = 441 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.

Smallest second moment of area

A round section has the same I about every axis.

I = πd⁴/64 = π·80⁴/64 = 2.011 × 10⁶ mm⁴

Effective length

KL = 1·3000 = 3000 mm

Critical load

Pcr = π²EI/(KL)² = π²·200000·2.011 × 10⁶/3000² = 440978 N = 441 kN

Answer

Pcr = 441 kN
10.Column buckling

Answer: d = 56.86 mm

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 = 2.5·45000 = 112500 N
KL = 1·3000 = 3000 mm

Solve for the diameter

d = (64·n·P·(KL)²/(π³E))^(1/4) = (64·112500·3000²/(π³·200000))^(1/4) = 56.86 mm

Answer

d = 56.86 mm

Check: the slenderness KL/r is 211.1, so the column is slender and Euler applies.

11.Mechanical vibrations

Answer: ζ = 0.01989

Free vibration of a mass–spring system: the undamped natural frequency is ωn = √(k/m) in rad/s, and fn = ωn/(2π) in Hz. A viscous damper c gives the damping ratio ζ = c/cc, with critical damping cc = 2·√(k·m) = 2·m·ωn. An underdamped system (ζ < 1) oscillates at ωd = ωn·√(1 − ζ²). Springs in parallel add, k = k₁ + k₂; springs in series add as reciprocals, 1/k = 1/k₁ + 1/k₂.

Logarithmic decrement

δ = (1/1)·ln(40/35.3) = 0.125

Damping ratio

ζ = δ/√(4π² + δ²) = 0.125/√(39.48 + 0.01562) = 0.01989

Answer

ζ = 0.01989
12.Mechanical vibrations

Answer: keq = 9.231 kN/m

Free vibration of a mass–spring system: the undamped natural frequency is ωn = √(k/m) in rad/s, and fn = ωn/(2π) in Hz. A viscous damper c gives the damping ratio ζ = c/cc, with critical damping cc = 2·√(k·m) = 2·m·ωn. An underdamped system (ζ < 1) oscillates at ωd = ωn·√(1 − ζ²). Springs in parallel add, k = k₁ + k₂; springs in series add as reciprocals, 1/k = 1/k₁ + 1/k₂.

Equivalent stiffness

Springs in series share the same force and add their deflections, so they combine as reciprocals: 1/k = 1/k1 + 1/k2.

1/keq = 1/12 + 1/40 → keq = 12·40/(12 + 40) = 9.231 kN/m

Answer

keq = 9.231 kN/m

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