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​ = 36N2​ = 50

A 7.5 kW motor running at 960 rpm drives a pinion with 36 teeth, which meshes with a gear with 50 teeth. The gear pair has an efficiency of 98%. Find the torque T1 on the motor shaft.

P = 7.5 kWn1 = 960 rpmN1 = 36N2 = 50η = 98%
T1 = N·m
2.Gears & gear trainsHard
A = 12B = 32C = 20D = 36

In a compound gear train, gear A (12 teeth) on the input shaft turning at 1450 rpm drives gear B (32 teeth). Gear C (20 teeth) is fixed to the same shaft as B and drives gear D (36 teeth) on the output shaft. Find the output speed nout.

nin = 1450 rpmA = 12B = 32C = 20D = 36
nout = rpm
3.Torsion of shaftsMedium
do​ = 50, di​ = 35 mmT = 750 N·mL = 1.5 m

A hollow steel shaft (outer diameter 50 mm, inner diameter 35 mm, length 1.5 m) is fixed at one end and twisted by a torque of 750 N·m at the other. Find the angle of twist φ in degrees.

T = 750 N·mdo = 50 mmdi = 35 mmL = 1.5 mG = 80 GPa
φ = °
4.Torsion of shaftsHard
d = 40 mmT0​ = 250 N·mACBa = 2.5 mb = 1 m

A solid aluminium shaft of diameter 40 mm is fixed to rigid walls at both ends A and B. A torque of 250 N·m is applied at C, 2.5 m from A and 1 m from B. Find the maximum shear stress τmax in the shaft.

d = 40 mmT0 = 250 N·ma = 2.5 mb = 1 m
τmax = MPa
5.Mohr’s circle & stress transformationMedium
σx​ = 140σy​ = −80τxy​ = −60MPa

A point has σₓ = 140 MPa, σᵧ = −80 MPa and τₓᵧ = −60 MPa (tension positive). Find the angle θs, between −90° and 90°, from the x-axis to the normal of the plane on which the shear stress has its maximum positive value +R (shear positive in the same sense as τₓᵧ).

σx = 140 MPaσy = −80 MPaτxy = −60 MPa
θs = °
6.Mohr’s circle & stress transformationHard
σx​ = 10σy​ = −60τxy​ = 30MPa

A point in a thin plate is in plane stress: σₓ = 10 MPa, σᵧ = −60 MPa and τₓᵧ = 30 MPa (σz = 0). The material has a yield strength of 460 MPa. Find the factor of safety n against yielding by the Tresca (maximum shear stress) criterion.

σx = 10 MPaσy = −60 MPaτxy = 30 MPaσY = 460 MPa
n =
7.Axial stress & strainMedium
Ø 16 mmBrass1.5 mP = 70 kN

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

P = 70 kNd = 16 mmL = 1.5 mE = 100 GPa
δ = mm
8.Axial stress & strainHard
Ø 40 mmSteel0.5 mØ 12 mmBrass1.5 mP = 95 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 = 95 kNsegment 1: Ø40 mm, 0.5 m, steel (E = 200 GPa)segment 2: Ø12 mm, 1.5 m, brass (E = 100 GPa)
σmax = MPa
9.Column bucklingMedium
PL = 2.5 m20 × 100 mmcross-section

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

L = 2.5 mE = 70 GPa (aluminium)b × h = 20 × 100 mm
Pcr = kN
10.Column bucklingHard
P = 70 kNL = 4 md = ?cross-section

A solid round column of length L made of aluminium is fixed at both ends. It must carry 70 kN with a factor of safety of 2.5 against buckling. Find the smallest diameter d.

P = 70 kNn = 2.5L = 4 mE = 70 GPa (aluminium)
d = mm
11.Mechanical vibrationsMedium
k = 150 kN/mc = 8660 N·s/mm = 500 kg

A 500 kg mass is supported by a spring with a stiffness of 150 kN/m and a viscous damper with a damping coefficient of 8660 N·s/m. Find the damping ratio ζ.

m = 500 kgk = 150 kN/mc = 8660 N·s/m
ζ =
12.Mechanical vibrationsHard
k1​ = 10k2​ = 5m = 5 kg

A 5 kg mass hangs from two springs connected end to end (in series): the upper spring has k₁ = 10 kN/m and the lower one k₂ = 5 kN/m. Find the equivalent stiffness keq of the spring system in kN/m.

m = 5 kgk1 = 10 kN/mk2 = 5 kN/m
keq = kN/m

3Solutions

1.Gears & gear trains

Answer: T1 = 74.6 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·960/60 = 100.5 rad/s
T1 = P/ω₁ = 7500/100.5 = 74.6 N·m

Answer

T1 = 74.6 N·m
2.Gears & gear trains

Answer: nout = 302.1 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 = 1450·12/32 = 543.8 rpm = nC

Second stage

nout = 543.8·20/36 = 302.1 rpm

Answer

nout = 302.1 rpm

total ratio = 4.8 : 1

3.Torsion of shafts

Answer: φ = 1.728 °

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(50⁴ − 35⁴)/32 = 466269 mm⁴

Angle of twist

T = 750 N·m = 750000 N·mm
L = 1.5 m = 1500 mm
G = 80 GPa = 80000 MPa
φ = TL/(GJ) = 750000·1500/(80000·466269) = 0.03016 rad
φ = 0.03016·180/π = 1.728°

Answer

φ = 1.728°
4.Torsion of shafts

Answer: τmax = 14.21 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. 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 = 250
TA·a = TB·b
TA = 250·1/3.5 = 71.43 N·m
TB = 250·2.5/3.5 = 178.6 N·m

Maximum shear stress

The larger of the two torques governs (same diameter).

τmax = 16·178571/(π·40³) = 14.21 MPa

Answer

τmax = 14.21 MPa
5.Mohr’s circle & stress transformation

Answer: θs = −59.31 °

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​

Angle on the circle

On Mohr’s circle the top point (+R) is 90° from the principal point σ₁; on the element that is 45°.

cos 2θs = −60/125.3 = −0.4789, sin 2θs = −110/125.3 = −0.8779
2θs = atan2(−110, −60) = −118.6°

Angle on the element

θs = −59.31°
check: θs − θp = −59.31 − (−14.31) = −45°

Answer

θs = −59.31°

Positive angles are counter-clockwise.

6.Mohr’s circle & stress transformation

Answer: n = 4.989

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. Yield criteria: von Mises predicts yield when σvM = √(σ₁² − σ₁σ₂ + σ₂²) reaches σY; Tresca when the absolute maximum shear stress reaches σY/2.

στxyCσ1​σ2​

Principal stresses

C = −25 MPa, R = 46.1 MPa
σ1 = 21.1 MPa, σ2 = −71.1 MPa, σ3 = 0

Tresca

σmax − σmin = 92.2 MPa
n = 460/92.2 = 4.989

Answer

n = 4.989

n > 1 means the point does not yield; Tresca is slightly more conservative than von Mises.

7.Axial stress & strain

Answer: δ = 5.222 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·16²/4 = 201.1 mm²
σ = P/A = 70·1000/201.1 = 348.2 MPa

Strain (Hooke’s law)

E for brass = 100 GPa = 100000 MPa.

ε = σ/E = 348.2/100000 = 0.003482 = 3482 µε

Elongation

δ = ε·L = 0.003482·1500 mm = 5.222 mm

Answer

δ = 5.222 mm
8.Axial stress & strain

Answer: σmax = 840 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·40²/4 = 1257 mm², A2 = π·12²/4 = 113.1 mm²
σ1 = 75.6 MPa
σ2 = 840 MPa

Largest stress

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

σmax = 840 MPa

Answer

σmax = 840 MPa
9.Column buckling

Answer: Pcr = 29.48 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 rectangle buckles about its weak axis, using the smaller dimension cubed.

Imin = h·b³/12 = 100·20³/12 = 66667 mm⁴

Effective length

KL = 0.5·2500 = 1250 mm

Critical load

Pcr = π²EI/(KL)² = π²·70000·66667/1250² = 29477 N = 29.48 kN

Answer

Pcr = 29.48 kN
10.Column buckling

Answer: d = 67.4 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 = 2.5·70000 = 175000 N
KL = 0.5·4000 = 2000 mm

Solve for the diameter

d = (64·n·P·(KL)²/(π³E))^(1/4) = (64·175000·2000²/(π³·70000))^(1/4) = 67.4 mm

Answer

d = 67.4 mm

Check: the slenderness KL/r is 118.7, so the column is slender and Euler applies.

11.Mechanical vibrations

Answer: ζ = 0.5

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·√(150000·500) = 17321 N·s/m

Damping ratio

ζ = c/cc = 8660/17321 = 0.5

Answer

ζ = 0.5

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

12.Mechanical vibrations

Answer: keq = 3.333 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 = 1/10 + 1/5 → keq = 10·5/(10 + 5) = 3.333 kN/m

Answer

keq = 3.333 kN/m

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