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
Tw​ = ?z = 3, 1440 rpm

A 1.1 kW motor at 1440 rpm drives a worm with 3 start(s). The worm wheel has 72 teeth and the drive has an efficiency of 50%. Find the output torque Tw on the wheel shaft.

z = 3Nw = 72n = 1440 rpmP = 1.1 kWη = 50%
Tw = N·m
2.Gears & gear trainsHard
A = 25B = 72C = 12D = 72

In a compound gear train, gear A (25 teeth) on the input shaft turning at 3000 rpm drives gear B (72 teeth). Gear C (12 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 = 3000 rpmA = 25B = 72C = 12D = 72
nout = rpm
3.Torsion of shaftsMedium
T = 500 N·md = 30 mmL = 3 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 = 500 N·md = 30 mmL = 3 mG = 80 GPa
φ = °
4.Torsion of shaftsHard
Td = ?

A solid shaft must transmit 15 kW at 500 rpm without the shear stress exceeding 60 MPa. Find the smallest diameter d that works.

P = 15 kWN = 500 rpmτallow = 60 MPa
d = mm
5.Mohr’s circle & stress transformationMedium
σx​ = −20σy​ = 90τxy​ = 40MPa

A point in a thin plate is in plane stress: σₓ = −20 MPa, σᵧ = 90 MPa and τₓᵧ = 40 MPa, with σz = 0. Find the absolute maximum shear stress τabs at the point (considering all planes in three dimensions).

σx = −20 MPaσy = 90 MPaτxy = 40 MPaσz = 0
τabs = MPa
6.Mohr’s circle & stress transformationHard
σx​τxy​top surface of the shaft

A solid shaft of diameter 30 mm carries a bending moment of 750 N·m together with a torque of 400 N·m. At the top surface, where the bending stress is tensile and largest, find the largest principal stress σ1.

d = 30 mmM = 750 N·mT = 400 N·m
σ1 = MPa
7.Axial stress & strainMedium
Ø 12 mmSteel2 mP = 80 kN

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

P = 80 kNd = 12 mmL = 2 mE = 200 GPa
ε = µε
8.Axial stress & strainHard
Ø 30 mmBrass1 mØ 12 mmBrass0.5 mP = 25 kN

The stepped bar is fixed at the wall and loaded at its free end. Find the total elongation δ.

P = 25 kNsegment 1: Ø30 mm, 1 m, brass (E = 100 GPa)segment 2: Ø12 mm, 0.5 m, brass (E = 100 GPa)
δ = mm
9.Column bucklingMedium
PL = 2 m25 × 60 mmcross-section

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

L = 2 mE = 70 GPa (aluminium)b × h = 25 × 60 mm
Pcr = kN
10.Column bucklingHard
P = 60 kNL = 3 md = ?cross-section

A solid round column of length L made of steel is fixed at both ends. It must carry 60 kN with a factor of safety of 3 against buckling. Find the smallest diameter d.

P = 60 kNn = 3L = 3 mE = 200 GPa (steel)
d = mm
11.Mechanical vibrationsMedium
k = 10 kN/mc = 300 N·s/mm = 100 kg

A 100 kg mass is supported by a spring with a stiffness of 10 kN/m and a viscous damper with a damping coefficient of 300 N·s/m. Find the damping ratio ζ.

m = 100 kgk = 10 kN/mc = 300 N·s/m
ζ =
12.Mechanical vibrationsHard
k1​ = 100k2​ = 25m = 100 kg

A 100 kg mass hangs from two springs side by side (in parallel), with stiffnesses k₁ = 100 kN/m and k₂ = 25 kN/m. The mass stays level. Find the equivalent stiffness keq of the spring system in kN/m.

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

3Solutions

1.Gears & gear trains

Answer: Tw = 87.54 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.

Wheel speed

nw = n·z/Nw = 1440·3/72 = 60 rpm

Output torque

ωw = 2π·60/60 = 6.283 rad/s
Tw = η·P/ωw = 0.5·1100/6.283 = 87.54 N·m

Answer

Tw = 87.54 N·m
2.Gears & gear trains

Answer: nout = 173.6 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 = 3000·25/72 = 1042 rpm = nC

Second stage

nout = 1042·12/72 = 173.6 rpm

Answer

nout = 173.6 rpm

total ratio = 17.28 : 1

3.Torsion of shafts

Answer: φ = 13.51 °

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) = 500·1000·3000/(80000·79522) = 0.2358 rad
φ = 0.2358·180/π = 13.51°

Answer

φ = 13.51°
4.Torsion of shafts

Answer: d = 28.97 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·500/60 = 52.36 rad/s
T = P/ω = 15000/52.36 = 286.5 N·m

Diameter from the allowable stress

d = ∛(16T/(π·τallow)) = ∛(16·286479/(π·60)) = 28.97 mm

Answer

d = 28.97 mm

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

5.Mohr’s circle & stress transformation

Answer: τabs = 68.01 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. In three dimensions the absolute maximum shear stress is (σmax − σmin)/2 over all three principal stresses; in plane stress the third one is zero.

στxyCσ1​σ2​

In-plane principal stresses

C = 35 MPa, R = √((−55)² + 40²) = 68.01 MPa
σ1 = 103 MPa, σ2 = −33.01 MPa, σz = 0

Largest of the three circles

τ = max(|σ1 − σ2|, |σ1|, |σ2|)/2 = max(136, 103, 33.01)/2 = 68.01 MPa

Answer

τabs = 68.01 MPa

Here σ₁ and σ₂ have opposite signs, so the in-plane maximum R is also the absolute maximum.

6.Mohr’s circle & stress transformation

Answer: σ1 = 301.8 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 = 32M/(πd³) = 32·750000/(π·30³) = 282.9 MPa
τ = 16T/(πd³) = 16·400000/(π·30³) = 75.45 MPa
στxyCσ1​σ2​

Mohr’s circle

C = σ/2 = 141.5 MPa
R = √(141.5² + 75.45²) = 160.3 MPa
σ1 = C + R = 301.8 MPa
σ2 = C − R = −18.86 MPa

Answer

σ1 = 301.8 MPa
7.Axial stress & strain

Answer: ε = 3537 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·12²/4 = 113.1 mm²
σ = P/A = 80·1000/113.1 = 707.4 MPa

Strain (Hooke’s law)

E for steel = 200 GPa = 200000 MPa.

ε = σ/E = 707.4/200000 = 0.003537 = 3537 µε

Answer

ε = 3537 µε
8.Axial stress & strain

Answer: δ = 1.459 mm

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·12²/4 = 113.1 mm²
σ1 = 35.37 MPa
σ2 = 221 MPa

Add the segment elongations

δ1 = σ1L1/E1 = 35.37·1000/100000 = 0.3537 mm
δ2 = σ2L2/E2 = 221·500/100000 = 1.105 mm
δ = δ1 + δ2 = 1.459 mm

Answer

δ = 1.459 mm
9.Column buckling

Answer: Pcr = 27.54 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 = 60·25³/12 = 78125 mm⁴

Effective length

KL = 0.7·2000 = 1400 mm

Critical load

Pcr = π²EI/(KL)² = π²·70000·78125/1400² = 27538 N = 27.54 kN

Answer

Pcr = 27.54 kN
10.Column buckling

Answer: d = 45.22 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 = 3·60000 = 180000 N
KL = 0.5·3000 = 1500 mm

Solve for the diameter

d = (64·n·P·(KL)²/(π³E))^(1/4) = (64·180000·1500²/(π³·200000))^(1/4) = 45.22 mm

Answer

d = 45.22 mm

Check: the slenderness KL/r is 132.7, so the column is slender and Euler applies.

11.Mechanical vibrations

Answer: ζ = 0.15

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·√(10000·100) = 2000 N·s/m

Damping ratio

ζ = c/cc = 300/2000 = 0.15

Answer

ζ = 0.15

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

12.Mechanical vibrations

Answer: keq = 125 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 side by side share the deflection and add their forces, so their stiffnesses simply add: k = k1 + k2.

keq = 100 + 25 = 125 kN/m

Answer

keq = 125 kN/m

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