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 = 4, 2900 rpm

A 0.75 kW motor at 2900 rpm drives a worm with 4 start(s). The worm wheel has 30 teeth and the drive has an efficiency of 60%. Find the output torque Tw on the wheel shaft.

z = 4Nw = 30n = 2900 rpmP = 0.75 kWη = 60%
Tw = N·m
2.Gears & gear trainsHard
A = 16B = 32C = 16D = 20

In a compound gear train, gear A (16 teeth) on the input shaft turning at 2900 rpm drives gear B (32 teeth). Gear C (16 teeth) is fixed to the same shaft as B and drives gear D (20 teeth) on the output shaft. Find the output speed nout.

nin = 2900 rpmA = 16B = 32C = 16D = 20
nout = rpm
3.Torsion of shaftsMedium
d = ?T = 200 N·mL = 2.5 m

A solid steel shaft 2.5 m long carries a torque of 200 N·m. The angle of twist between its ends must not exceed 0.5°. Find the smallest diameter d that meets this limit.

T = 200 N·mL = 2.5 mG = 80 GPaφallow = 0.5°
d = mm
4.Torsion of shaftsHard
Td = ?

A solid shaft must transmit 20 kW at 750 rpm without the shear stress exceeding 75 MPa. Find the smallest diameter d that works.

P = 20 kWN = 750 rpmτallow = 75 MPa
d = mm
5.Mohr’s circle & stress transformationMedium
σx​ = 50σy​ = 0τxy​ = 10MPa

A point in a loaded part has σₓ = 50 MPa, σᵧ = 0 MPa and τₓᵧ = 10 MPa (tension positive). Find the maximum in-plane shear stress τmax.

σx = 50 MPaσy = 0 MPaτxy = 10 MPa
τmax = MPa
6.Mohr’s circle & stress transformationHard
σx​ = −40σy​ = −80τxy​ = 30MPa

A point in a loaded part has σₓ = −40 MPa, σᵧ = −80 MPa and τₓᵧ = 30 MPa (tension positive). Find the normal stress σθ on a plane whose normal is rotated 50° counter-clockwise from the x-axis.

σx = −40 MPaσy = −80 MPaτxy = 30 MPaθ = 50°
σθ = MPa
7.Axial stress & strainMedium
250 kNØ20100 GPaØ100/70300 mmδ = ?

A steel rod (diameter 20 mm, E = 200 GPa) sits inside a tube made of brass (outer diameter 100 mm, inner diameter 70 mm, E = 100 GPa). Both are 300 mm long and are compressed together between rigid plates by 250 kN. Find the shortening δ.

P = 250 kNrod: Ø20 mm, E = 200 GPatube: Ø100/Ø70 mm, E = 100 GPaL = 300 mm
δ = mm
8.Axial stress & strainHard
20 kN12400 mm300 mmØ30Ø30σ2​ = ?

A steel segment (diameter 30 mm, length 400 mm, E = 200 GPa) and a segment made of aluminium (diameter 30 mm, length 300 mm, E = 70 GPa) are joined end to end and fixed between two rigid walls. An axial load of 20 kN acts at the joint, towards segment 2. Find the magnitude of the stress σ2 in segment 2.

segment 1: steel, Ø30 mm, 400 mm, E = 200 GPasegment 2: aluminium, Ø30 mm, 300 mm, E = 70 GPaP = 20 kN
σ2 = MPa
9.Column bucklingMedium
PL = 6 m40 × 80 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 = 6 mE = 70 GPa (aluminium)b × h = 40 × 80 mm
Pcr = kN
10.Column bucklingHard
PL = 2.5 md = 20 mmcross-section

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

L = 2.5 mE = 200 GPa (steel)d = 20 mm
σcr = MPa
11.Mechanical vibrationsMedium
k = 8 kN/mc = 570 N·s/mm = 40 kg

A 40 kg mass is supported by a spring with a stiffness of 8 kN/m and a viscous damper with a damping coefficient of 570 N·s/m. Find the damping ratio ζ.

m = 40 kgk = 8 kN/mc = 570 N·s/m
ζ =
12.Mechanical vibrationsHard
k1​ = 20k2​ = 80m = 5 kg

A 5 kg mass hangs from two springs connected end to end (in series): the upper spring has k₁ = 20 kN/m and the lower one k₂ = 80 kN/m. Ignore damping and the masses of the springs. Find the natural frequency fn of vertical vibration in Hz.

m = 5 kgk1 = 20 kN/mk2 = 80 kN/m
fn = Hz

3Solutions

1.Gears & gear trains

Answer: Tw = 11.11 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 = 2900·4/30 = 386.7 rpm

Output torque

ωw = 2π·386.7/60 = 40.49 rad/s
Tw = η·P/ωw = 0.6·750/40.49 = 11.11 N·m

Answer

Tw = 11.11 N·m
2.Gears & gear trains

Answer: nout = 1160 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 = 2900·16/32 = 1450 rpm = nC

Second stage

nout = 1450·16/20 = 1160 rpm

Answer

nout = 1160 rpm

total ratio = 2.5 : 1

3.Torsion of shafts

Answer: d = 51.97 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.

Required polar moment

T = 200 N·m = 200000 N·mm
L = 2.5 m = 2500 mm
G = 80 GPa = 80000 MPa
φ = 0.5·π/180 = 0.008727 rad
J = TL/(Gφ) = 200000·2500/(80000·0.008727) = 716197 mm⁴

Diameter

d = (32J/π)1/4 = 51.97 mm

Answer

d = 51.97 mm

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

4.Torsion of shafts

Answer: d = 25.86 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·750/60 = 78.54 rad/s
T = P/ω = 20000/78.54 = 254.6 N·m

Diameter from the allowable stress

d = ∛(16T/(π·τallow)) = ∛(16·254648/(π·75)) = 25.86 mm

Answer

d = 25.86 mm

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

5.Mohr’s circle & stress transformation

Answer: τmax = 26.93 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 = √(((50 − 0)/2)² + 10²) = 26.93 MPa

Answer

τmax = 26.93 MPa
6.Mohr’s circle & stress transformation

Answer: σθ = −33.93 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

σθ = −60 + 20·−0.1736 + 30·0.9848 = −33.93 MPa

Answer

σθ = −33.93 MPa
7.Axial stress & strain

Answer: δ = 0.1619 mm

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·20²/4 = 314.2 mm²
At = π(100² − 70²)/4 = 4006 mm²

Combined axial stiffness

ΣEA = 200·10³·314.2 + 100·10³·4006 = 4.634 × 10⁸ N

Shortening

δ = 250000·300/4.634 × 10⁸ = 0.1619 mm

Answer

δ = 0.1619 mm
8.Axial stress & strain

Answer: σ2 = 9.003 MPa

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.

Stiffnesses

k₁ = 200000·706.9/400 = 353429 N/mm
k₂ = 70000·706.9/300 = 164934 N/mm

Share of segment 2

F2 = 20000·164934/518363 = 6364 N

Stress

σ2 = 6364/706.9 = 9.003 MPa (compression)

Answer

σ2 = 9.003 MPa
9.Column buckling

Answer: Pcr = 2.047 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 = 80·40³/12 = 426667 mm⁴

Effective length

KL = 2·6000 = 12000 mm

Critical load

Pcr = π²EI/(KL)² = π²·70000·426667/12000² = 2047 N = 2.047 kN

Answer

Pcr = 2.047 kN
10.Column buckling

Answer: σcr = 7.896 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·20⁴/64 = 7854 mm⁴

Radius of gyration and slenderness

A = 314.2 mm²
r = √(I/A) = √(7854/314.2) = 5 mm
KL = 1·2500 = 2500 mm
KL/r = 2500/5 = 500

Critical stress

σcr = π²E/(KL/r)² = π²·200000/500² = 7.896 MPa

Answer

σcr = 7.896 MPa
11.Mechanical vibrations

Answer: ζ = 0.5038

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·√(8000·40) = 1131 N·s/m

Damping ratio

ζ = c/cc = 570/1131 = 0.5038

Answer

ζ = 0.5038

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

12.Mechanical vibrations

Answer: fn = 9.003 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 in series share the same force and add their deflections, so they combine as reciprocals: 1/k = 1/k1 + 1/k2.

1/keq = 1/20 + 1/80 → keq = 20·80/(20 + 80) = 16 kN/m

Natural frequency

ωn = √(16000/5) = 56.57 rad/s
fn = 56.57/(2π) = 9.003 Hz

Answer

fn = 9.003 Hz

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