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
N1​ = 20N2​ = 30

A 0.75 kW motor running at 2900 rpm drives a pinion with 20 teeth, which meshes with a gear with 30 teeth. The gear pair has an efficiency of 95%. Find the output torque T2 on the gear shaft.

P = 0.75 kWn1 = 2900 rpmN1 = 20N2 = 30η = 95%
T2 = N·m
2.Gears & gear trainsHard
A = 36B = 72C = 18D = ?

In a compound gear train, gear A (36 teeth) on the input shaft turns at 2880 rpm and drives gear B (72 teeth). Gear C (18 teeth) is fixed to the same shaft as B and drives gear D on the output shaft. The output must turn at 720 rpm. How many teeth ND must gear D have?

nin = 2880 rpmA = 36B = 72C = 18nout = 720 rpm
ND =
3.Torsion of shaftsMedium
d = 20 mmT = 50 N·m400 mmφ = 0.91°

In a torsion test, a solid specimen of diameter 20 mm is twisted by a torque of 50 N·m. The two ends of a gauge length of 400 mm rotate 0.91° relative to each other (the material is still elastic). Find the shear modulus G of the material.

T = 50 N·md = 20 mmL = 400 mmφ = 0.91°
G = GPa
4.Torsion of shaftsHard
d = 40 mmT0​ = 200 N·mACBa = 0.8 mb = 2 m

A solid brass shaft of diameter 40 mm is fixed to rigid walls at both ends A and B. A torque of 200 N·m is applied at C, 0.8 m from A and 2 m from B. Find the angle of rotation φC of section C, in degrees.

d = 40 mmT0 = 200 N·ma = 0.8 mb = 2 mG = 39 GPa
φC = °
5.Mohr’s circle & stress transformationMedium
σx​ = 100σy​ = −60τxy​ = 30MPa

A point has σₓ = 100 MPa, σᵧ = −60 MPa and τₓᵧ = 30 MPa (tension positive). The element is rotated 20° clockwise. Find the normal stress σy′ on the faces of the rotated element that are perpendicular to the rotated y′-axis.

σx = 100 MPaσy = −60 MPaτxy = 30 MPaθ = -20°
σy′ = MPa
6.Mohr’s circle & stress transformationHard
σx​τxy​surface of the shaft

A solid shaft of diameter 40 mm carries an axial compressive force of 90 kN together with a torque of 750 N·m. At the surface of the shaft, find the maximum in-plane shear stress τmax.

d = 40 mmF = −90 kNT = 750 N·m
τmax = MPa
7.Axial stress & strainMedium
P = ?12300 mm500 mmØ25Ø30δ = 0.5 mm

A bar is made of a steel segment (diameter 25 mm, length 300 mm, E = 200 GPa) joined end to end with a segment made of brass (diameter 30 mm, length 500 mm, E = 100 GPa). It is fixed at one end and pulled at the other. Find the axial load P that stretches it by 0.5 mm in total.

segment 1: steel, Ø25 mm, 300 mm, E = 200 GPasegment 2: brass, Ø30 mm, 500 mm, E = 100 GPaδ = 0.5 mm
P = kN
8.Axial stress & strainHard
P = ?Ø4070 GPaØ100/70600 mm

A steel rod (diameter 40 mm, E = 200 GPa, allowable stress 150 MPa) sits inside a tube made of aluminium (outer diameter 100 mm, inner diameter 70 mm, E = 70 GPa, allowable stress 70 MPa). They are compressed together between rigid plates. Find the largest load Pmax.

rod: Ø40 mm, E = 200 GPa, σallow = 150 MPatube: Ø100/Ø70 mm, E = 70 GPa, σallow = 70 MPa
Pmax = kN
9.Column bucklingMedium
PL = 1.5 md = 30 mmcross-section

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

L = 1.5 mE = 200 GPa (steel)d = 30 mm
Pcr = kN
10.Column bucklingHard
PL = 1.5 md = 40 mmcross-section

A column of length L made of aluminium is pinned at both ends. Find its slenderness and the critical buckling stress σcr from Euler’s formula.

L = 1.5 mE = 70 GPa (aluminium)d = 40 mm
σcr = MPa
11.Mechanical vibrationsMedium
tx12 mm3 cycles4.7 mm

In a free-vibration test of a damped mass–spring system, a displacement peak of 12 mm is followed 3 cycles later by a peak of 4.7 mm. Find the damping ratio ζ.

x0 = 12 mmx3 = 4.7 mmn = 3
ζ =
12.Mechanical vibrationsHard
k1​ = 15k2​ = 30m = 20 kg

A 20 kg mass hangs from two springs side by side (in parallel), with stiffnesses k₁ = 15 kN/m and k₂ = 30 kN/m. The mass stays level. Ignore damping and the masses of the springs. Find the natural frequency fn of vertical vibration in Hz.

m = 20 kgk1 = 15 kN/mk2 = 30 kN/m
fn = Hz

3Solutions

1.Gears & gear trains

Answer: T2 = 3.519 N·m

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.

Motor torque

ω₁ = 2π·2900/60 = 303.7 rad/s
T1 = P/ω₁ = 750/303.7 = 2.47 N·m

Output torque

T2 = 2.47·30/20·0.95 = 3.519 N·m

Answer

T2 = 3.519 N·m
2.Gears & gear trains

Answer: ND = 36

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 = 2880·36/72 = 1440 rpm

Teeth on gear D

ND = C·nC/nout = 18·1440/720 = 36

Answer

ND = 36
3.Torsion of shafts

Answer: G = 80.17 GPa

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 moment and angle

J = π·20⁴/32 = 15708 mm⁴
φ = 0.91·π/180 = 0.01588 rad

Shear modulus

T = 50 N·m = 50000 N·mm
G = TL/(Jφ) = 50000·400/(15708·0.01588) = 80166 MPa
G = 80.17 GPa

Answer

G = 80.17 GPa

Compare: steel ≈ 80 GPa, brass ≈ 39 GPa, aluminium ≈ 26 GPa.

4.Torsion of shafts

Answer: φC = 0.6681 °

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. When both ends are fixed, statics alone gives only TA + TB = T₀; the second equation is compatibility (equal twist of both parts at the loaded section).

Equilibrium and compatibility

TA + TB = 200
TA·a = TB·b
TA = 200·2/2.8 = 142.9 N·m
TB = 200·0.8/2.8 = 57.14 N·m

Rotation of C

Use segment AC: it is fixed at A and carries TA.

J = π·40⁴/32 = 251327 mm⁴
G = 39 GPa = 39000 MPa
φC = TA·a/(GJ) = 142857·800/(39000·251327) = 0.01166 rad = 0.6681°

Answer

φC = 0.6681°
5.Mohr’s circle & stress transformation

Answer: σy′ = −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.

Transformation equation for the y′ face

σy′ = 20 − 80·0.766 − 30·(−0.6428) = −22 MPa

Check

The sum of the normal stresses does not change with rotation.

σx′ = 62 MPa, σx′ + σy′ = 40 = σx + σy

Answer

σy′ = −22 MPa
6.Mohr’s circle & stress transformation

Answer: τmax = 69.6 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.

Stresses at the surface

σ = F/A = −90000/(π·40²/4) = −90000/1257 = −71.62 MPa
τ = 16T/(πd³) = 16·750000/(π·40³) = 59.68 MPa
στxyCτmax​

Mohr’s circle

C = σ/2 = −35.81 MPa
R = √((−35.81)² + 59.68²) = 69.6 MPa

Answer

τmax = 69.6 MPa
7.Axial stress & strain

Answer: P = 49.36 kN

Two materials: in series (one after the other) every segment carries the same force and the elongations add: δ = P·Σ L/(E·A). In parallel (side by side between rigid plates) both parts shorten by the same amount, so their strains are equal: the stiffer part takes the larger share, Pi = P·EiAi/ΣEA, and σi = Ei·ε. A bar held between two rigid walls with a load at the junction is statically indeterminate: the two segments share the load in proportion to their stiffness k = EA/L.

Areas

A₁ = 490.9 mm², A₂ = 706.9 mm²

Flexibilities

L₁/(E₁A₁) = 300/(200000·490.9) = 3.056 × 10⁻⁶ mm/N
L₂/(E₂A₂) = 500/(100000·706.9) = 7.074 × 10⁻⁶ mm/N

Load

P = 0.5/1.013 × 10⁻⁵ = 49362 N = 49.36 kN

Answer

P = 49.36 kN
8.Axial stress & strain

Answer: Pmax = 398.8 kN

Two materials: in series (one after the other) every segment carries the same force and the elongations add: δ = P·Σ L/(E·A). In parallel (side by side between rigid plates) both parts shorten by the same amount, so their strains are equal: the stiffer part takes the larger share, Pi = P·EiAi/ΣEA, and σi = Ei·ε. A bar held between two rigid walls with a load at the junction is statically indeterminate: the two segments share the load in proportion to their stiffness k = EA/L.

Areas

Ar = π·40²/4 = 1257 mm²
At = π(100² − 70²)/4 = 4006 mm²

Combined axial stiffness

ΣEA = 200·10³·1257 + 70·10³·4006 = 5.317 × 10⁸ N

Governing strain

ε = min(0.00075, 0.001) = 0.00075 (steel)

Largest load

Pmax = 0.00075·5.317 × 10⁸ = 398786 N = 398.8 kN

Answer

Pmax = 398.8 kN
9.Column buckling

Answer: Pcr = 8.721 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·30⁴/64 = 39761 mm⁴

Effective length

KL = 2·1500 = 3000 mm

Critical load

Pcr = π²EI/(KL)² = π²·200000·39761/3000² = 8721 N = 8.721 kN

Answer

Pcr = 8.721 kN
10.Column buckling

Answer: σcr = 30.71 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·40⁴/64 = 125664 mm⁴

Radius of gyration and slenderness

A = 1257 mm²
r = √(I/A) = √(125664/1257) = 10 mm
KL = 1·1500 = 1500 mm
KL/r = 1500/10 = 150

Critical stress

σcr = π²E/(KL/r)² = π²·70000/150² = 30.71 MPa

Answer

σcr = 30.71 MPa
11.Mechanical vibrations

Answer: ζ = 0.04967

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 = (1/3)·ln(12/4.7) = 0.3124

Damping ratio

ζ = δ/√(4π² + δ²) = 0.3124/√(39.48 + 0.09762) = 0.04967

Answer

ζ = 0.04967
12.Mechanical vibrations

Answer: fn = 7.549 Hz

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 side by side share the deflection and add their forces, so their stiffnesses simply add: k = k1 + k2.

keq = 15 + 30 = 45 kN/m

Natural frequency

ωn = √(45000/20) = 47.43 rad/s
fn = 47.43/(2π) = 7.549 Hz

Answer

fn = 7.549 Hz

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