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​N2​ = ?

Two parallel shafts are 150 mm apart. They must be connected by a pair of spur gears with a module of 2.5 mm and a speed reduction of 4 : 1. How many teeth N2 must the gear have?

a = 150 mmm = 2.5 mmi = 4
N2 =
2.Gears & gear trainsHard
A = 40B = 72C = 16D = 36

In a compound gear train, gear A (40 teeth) on the input shaft turning at 960 rpm drives gear B (72 teeth). Gear C (16 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 = 960 rpmA = 40B = 72C = 16D = 36
nout = rpm
3.Torsion of shaftsMedium
do​ = ?T = 1000 N·m

A hollow shaft must carry a torque of 1000 N·m. Its inner diameter is to be 0.6 times its outer diameter, and the shear stress must not exceed 75 MPa. Find the smallest outer diameter do.

T = 1000 N·mdi/do = 0.6τallow = 75 MPa
do = mm
4.Torsion of shaftsHard
d = ?50 kW, 1450 rpm

A solid steel shaft transmits 50 kW at 1450 rpm. The shear stress must not exceed 75 MPa and the twist must not exceed 0.75° per m of length. Find the smallest diameter d that satisfies both limits.

P = 50 kWN = 1450 rpmτallow = 75 MPaθallow = 0.75°/mG = 80 GPa
d = mm
5.Mohr’s circle & stress transformationMedium
σx​ = 140σy​ = 60τxy​ = −20MPa

A point has σₓ = 140 MPa, σᵧ = 60 MPa and τₓᵧ = −20 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 = 60 MPaτxy = −20 MPa
θs = °
6.Mohr’s circle & stress transformationHard
40°D = 400 mm, t = 15 mm, p = 1.5 MPap

A thin-walled cylindrical tank of inner diameter 400 mm and wall thickness 15 mm holds gas at a gauge pressure of 1.5 MPa. It is made from plate welded along a helical seam at 40° to the axis of the cylinder. Find the normal stress σn acting across the weld seam.

D = 400 mmt = 15 mmp = 1.5 MPaα = 40°
σn = MPa
7.Axial stress & strainMedium
P = ?12400 mm300 mmØ25Ø50δ = 0.4 mm

A bar is made of a steel segment (diameter 25 mm, length 400 mm, E = 200 GPa) joined end to end with a segment made of aluminium (diameter 50 mm, length 300 mm, E = 70 GPa). It is fixed at one end and pulled at the other. Find the axial load P that stretches it by 0.4 mm in total.

segment 1: steel, Ø25 mm, 400 mm, E = 200 GPasegment 2: aluminium, Ø50 mm, 300 mm, E = 70 GPaδ = 0.4 mm
P = kN
8.Axial stress & strainHard
Ø 35 mmSteel1 mØ 16 mmSteel2 mP = 70 kN

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

P = 70 kNsegment 1: Ø35 mm, 1 m, steel (E = 200 GPa)segment 2: Ø16 mm, 2 m, steel (E = 200 GPa)
δ = mm
9.Column bucklingMedium
PL = 1 m20 × 40 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 = 1 mE = 70 GPa (aluminium)b × h = 20 × 40 mm
Pcr = kN
10.Column bucklingHard
P = 35 kNL = 6 md = ?cross-section

A solid round column of length L made of aluminium is pinned at both ends. It must carry 35 kN with a factor of safety of 3 against buckling. Find the smallest diameter d.

P = 35 kNn = 3L = 6 mE = 70 GPa (aluminium)
d = mm
11.Mechanical vibrationsMedium
tx40 mm1 cycle21.3 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 21.3 mm. Find the damping ratio ζ.

x0 = 40 mmx1 = 21.3 mmn = 1
ζ =
12.Mechanical vibrationsHard
k1​ = 50k2​ = 15m = 100 kg

A 100 kg mass hangs from two springs side by side (in parallel), with stiffnesses k₁ = 50 kN/m and k₂ = 15 kN/m. The mass stays level. Find the equivalent stiffness keq of the spring system in kN/m.

m = 100 kgk1 = 50 kN/mk2 = 15 kN/m
keq = kN/m

3Solutions

1.Gears & gear trains

Answer: N2 = 96

Gear geometry: the module m sets the tooth size. A gear with N teeth has a pitch diameter d = m·N, two meshing gears have the same module, and their centre distance is a = (d₁ + d₂)/2 = m·(N₁ + N₂)/2. The pitch-line speed is v = π·d·n/60, and the tangential tooth force follows from the torque: Ft = 2T/d.

Total number of teeth

N1 + N2 = 2a/m = 2·150/2.5 = 120

Split by the ratio

N1 = 120/(1 + 4) = 24
N2 = 4·24 = 96

Answer

N2 = 96
2.Gears & gear trains

Answer: nout = 237 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 = 960·40/72 = 533.3 rpm = nC

Second stage

nout = 533.3·16/36 = 237 rpm

Answer

nout = 237 rpm

total ratio = 4.05 : 1

3.Torsion of shafts

Answer: do = 42.73 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.

Outer diameter from the allowable stress

T = 1000 N·m = 1 × 10⁶ N·mm
1 − k⁴ = 1 − 0.6⁴ = 0.8704
do = ∛(16T/(π·τallow·(1 − k⁴))) = ∛(16·1 × 10⁶/(π·75·0.8704)) = 42.73 mm
di = 0.6·42.73 = 25.64 mm

Answer

do = 42.73 mm

A solid shaft would need d = 40.8 mm; the hollow one is a little larger but much lighter.

4.Torsion of shafts

Answer: d = 42.3 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·1450/60 = 151.8 rad/s
T = P/ω = 50000/151.8 = 329.3 N·m

Diameter for strength

T = 329.3 N·m = 329286 N·mm
dτ = ∛(16·329286/(π·75)) = 28.17 mm

Diameter for stiffness

θ = 0.75·π/180/1000 = 1.309 × 10⁻⁵ rad/mm
G = 80 GPa = 80000 MPa
dφ = (32·329286/(π·80000·1.309 × 10⁻⁵))1/4 = 42.3 mm

Governing diameter

Both limits must hold, so the larger diameter governs.

d = max(28.17, 42.3) = 42.3 mm

Answer

d = 42.3 mm

Here stiffness governs.

5.Mohr’s circle & stress transformation

Answer: θs = −58.28 °

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 = −20/44.72 = −0.4472, sin 2θs = −40/44.72 = −0.8944
2θs = atan2(−40, −20) = −116.6°

Angle on the element

θs = −58.28°
check: θs − θp = −58.28 − (−13.28) = −45°

Answer

θs = −58.28°

Positive angles are counter-clockwise.

6.Mohr’s circle & stress transformation

Answer: σn = 15.87 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 = 400/2 = 200 mm
σh = pr/t = 1.5·200/15 = 20 MPa
σa = pr/(2t) = 10 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 = 10·sin²40° + 20·cos²40° = 15.87 MPa

Answer

σn = 15.87 MPa
7.Axial stress & strain

Answer: P = 63.93 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 = 1963 mm²

Flexibilities

L₁/(E₁A₁) = 400/(200000·490.9) = 4.074 × 10⁻⁶ mm/N
L₂/(E₂A₂) = 300/(70000·1963) = 2.183 × 10⁻⁶ mm/N

Load

P = 0.4/6.257 × 10⁻⁶ = 63928 N = 63.93 kN

Answer

P = 63.93 kN
8.Axial stress & strain

Answer: δ = 3.845 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·35²/4 = 962.1 mm², A2 = π·16²/4 = 201.1 mm²
σ1 = 72.76 MPa
σ2 = 348.2 MPa

Add the segment elongations

δ1 = σ1L1/E1 = 72.76·1000/200000 = 0.3638 mm
δ2 = σ2L2/E2 = 348.2·2000/200000 = 3.482 mm
δ = δ1 + δ2 = 3.845 mm

Answer

δ = 3.845 mm
9.Column buckling

Answer: Pcr = 37.6 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 = 40·20³/12 = 26667 mm⁴

Effective length

KL = 0.7·1000 = 700 mm

Critical load

Pcr = π²EI/(KL)² = π²·70000·26667/700² = 37598 N = 37.6 kN

Answer

Pcr = 37.6 kN
10.Column buckling

Answer: d = 102.7 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 = 3·35000 = 105000 N
KL = 1·6000 = 6000 mm

Solve for the diameter

d = (64·n·P·(KL)²/(π³E))^(1/4) = (64·105000·6000²/(π³·70000))^(1/4) = 102.7 mm

Answer

d = 102.7 mm

Check: the slenderness KL/r is 233.6, so the column is slender and Euler applies.

11.Mechanical vibrations

Answer: ζ = 0.09979

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(40/21.3) = 0.6302

Damping ratio

ζ = δ/√(4π² + δ²) = 0.6302/√(39.48 + 0.3971) = 0.09979

Answer

ζ = 0.09979
12.Mechanical vibrations

Answer: keq = 65 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 = 50 + 15 = 65 kN/m

Answer

keq = 65 kN/m

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