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​ = 40z = 1, 1450 rpm

A worm with 1 start(s) turns at 1450 rpm and drives a worm wheel with 40 teeth. Find the speed nw of the wheel.

z = 1Nw = 40n = 1450 rpm
nw = rpm
2.Gears & gear trainsHard
A = 16B = 60C = 18D = 72

In a compound gear train, gear A (16 teeth) on the input shaft turning at 1500 rpm drives gear B (60 teeth). Gear C (18 teeth) is fixed to the same shaft as B and drives gear D (72 teeth) on the output shaft. Find the output speed nout.

nin = 1500 rpmA = 16B = 60C = 18D = 72
nout = rpm
3.Torsion of shaftsMedium
T = 400 N·md = 30 mmL = 1.5 mφ = ?

A solid steel 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 = 400 N·md = 30 mmL = 1.5 mG = 80 GPa
φ = °
4.Torsion of shaftsHard
Tdo​ = 60 mm, di​ = 45 mm

A hollow shaft transmits 75 kW at 1500 rpm. Find the maximum shear stress τmax in the shaft.

P = 75 kWN = 1500 rpmdo = 60 mmdi = 45 mm
τmax = MPa
5.Mohr’s circle & stress transformationMedium
σx​ = 150σy​ = 0τxy​ = 10MPa

A point in a loaded part has σₓ = 150 MPa, σᵧ = 0 MPa and τₓᵧ = 10 MPa (tension positive). Find the maximum in-plane shear stress τmax.

σx = 150 MPaσy = 0 MPaτxy = 10 MPa
τmax = MPa
6.Mohr’s circle & stress transformationHard
35°D = 800 mm, t = 5 mm, p = 2.5 MPap

A thin-walled cylindrical tank of inner diameter 800 mm and wall thickness 5 mm holds gas at a gauge pressure of 2.5 MPa. It is made from plate welded along a helical seam at 35° to the axis of the cylinder. Find the normal stress σn acting across the weld seam.

D = 800 mmt = 5 mmp = 2.5 MPaα = 35°
σn = MPa
7.Axial stress & strainMedium
Ø 20 mmSteel3 mP = 90 kN

Find the axial strain ε in the steel bar, in microstrain (µε = 10⁻⁶).

P = 90 kNd = 20 mmL = 3 mE = 200 GPa
ε = µε
8.Axial stress & strainHard
Ø 35 mmBrass1.5 mØ 16 mmBrass2 mP = 30 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 = 30 kNsegment 1: Ø35 mm, 1.5 m, brass (E = 100 GPa)segment 2: Ø16 mm, 2 m, brass (E = 100 GPa)
σmax = MPa
9.Column bucklingMedium
PL = 5 md = 50 mmcross-section

A column of length L made of aluminium is fixed at the base and free at the top. Using Euler’s formula, find its critical buckling load Pcr.

L = 5 mE = 70 GPa (aluminium)d = 50 mm
Pcr = kN
10.Column bucklingHard
PL = 1 md = 30 mmcross-section

A column of length L made of aluminium is fixed at the base and free at the top. Find its slenderness and the critical buckling stress σcr from Euler’s formula.

L = 1 mE = 70 GPa (aluminium)d = 30 mm
σcr = MPa
11.Mechanical vibrationsMedium
k = 150 kN/mc = 760 N·s/mm = 150 kg

A 150 kg mass is supported by a spring with a stiffness of 150 kN/m and a viscous damper with a damping coefficient of 760 N·s/m. Find the damping ratio ζ.

m = 150 kgk = 150 kN/mc = 760 N·s/m
ζ =
12.Mechanical vibrationsHard
k1​ = 30k2​ = 25m = 100 kg

A 100 kg mass hangs from two springs connected end to end (in series): the upper spring has k₁ = 30 kN/m and the lower one k₂ = 25 kN/m. Find the equivalent stiffness keq of the spring system in kN/m.

m = 100 kgk1 = 30 kN/mk2 = 25 kN/m
keq = kN/m

3Solutions

1.Gears & gear trains

Answer: nw = 36.25 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 = 1450·1/40 = 36.25 rpm

Answer

nw = 36.25 rpm
2.Gears & gear trains

Answer: nout = 100 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.

First stage

nB = 1500·16/60 = 400 rpm = nC

Second stage

nout = 400·18/72 = 100 rpm

Answer

nout = 100 rpm

total ratio = 15 : 1

3.Torsion of shafts

Answer: φ = 5.404 °

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) = 400·1000·1500/(80000·79522) = 0.09431 rad
φ = 0.09431·180/π = 5.404°

Answer

φ = 5.404°
4.Torsion of shafts

Answer: τmax = 16.47 MPa

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·1500/60 = 157.1 rad/s
T = P/ω = 75000/157.1 = 477.5 N·m

Polar second moment of area

J = π(60⁴ − 45⁴)/32 = 869767 mm⁴

Maximum shear stress

τmax = T·(do/2)/J = 477465·30/869767 = 16.47 MPa

Answer

τmax = 16.47 MPa
5.Mohr’s circle & stress transformation

Answer: τmax = 75.66 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 = √(((150 − 0)/2)² + 10²) = 75.66 MPa

Answer

τmax = 75.66 MPa
6.Mohr’s circle & stress transformation

Answer: σn = 167.1 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 = 800/2 = 400 mm
σh = pr/t = 2.5·400/5 = 200 MPa
σa = pr/(2t) = 100 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 = 100·sin²35° + 200·cos²35° = 167.1 MPa

Answer

σn = 167.1 MPa
7.Axial stress & strain

Answer: ε = 1432 µε

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·20²/4 = 314.2 mm²
σ = P/A = 90·1000/314.2 = 286.5 MPa

Strain (Hooke’s law)

E for steel = 200 GPa = 200000 MPa.

ε = σ/E = 286.5/200000 = 0.001432 = 1432 µε

Answer

ε = 1432 µε
8.Axial stress & strain

Answer: σmax = 149.2 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·35²/4 = 962.1 mm², A2 = π·16²/4 = 201.1 mm²
σ1 = 31.18 MPa
σ2 = 149.2 MPa

Largest stress

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

σmax = 149.2 MPa

Answer

σmax = 149.2 MPa
9.Column buckling

Answer: Pcr = 2.12 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·50⁴/64 = 306796 mm⁴

Effective length

KL = 2·5000 = 10000 mm

Critical load

Pcr = π²EI/(KL)² = π²·70000·306796/10000² = 2120 N = 2.12 kN

Answer

Pcr = 2.12 kN
10.Column buckling

Answer: σcr = 9.715 MPa

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·30⁴/64 = 39761 mm⁴

Radius of gyration and slenderness

A = 706.9 mm²
r = √(I/A) = √(39761/706.9) = 7.5 mm
KL = 2·1000 = 2000 mm
KL/r = 2000/7.5 = 266.7

Critical stress

σcr = π²E/(KL/r)² = π²·70000/266.7² = 9.715 MPa

Answer

σcr = 9.715 MPa
11.Mechanical vibrations

Answer: ζ = 0.08011

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.

Critical damping

cc = 2·√(k·m) = 2·√(150000·150) = 9487 N·s/m

Damping ratio

ζ = c/cc = 760/9487 = 0.08011

Answer

ζ = 0.08011

ζ < 1, so the system is underdamped and oscillates as it decays.

12.Mechanical vibrations

Answer: keq = 13.64 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 = 1/30 + 1/25 → keq = 30·25/(30 + 25) = 13.64 kN/m

Answer

keq = 13.64 kN/m

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