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
Nw​ = 40z = 4, 1450 rpm

A worm with 4 start(s) turns at 1450 rpm and drives a worm wheel with 40 teeth. Find the speed nw of the wheel.

z = 4Nw = 40n = 1450 rpm
nw = rpm
2.Gears & gear trainsHard
A = 12B = 16C = 18D = 45

In a compound gear train, gear A (12 teeth) on the input shaft turning at 1500 rpm drives gear B (16 teeth). Gear C (18 teeth) is fixed to the same shaft as B and drives gear D (45 teeth) on the output shaft. Find the output speed nout.

nin = 1500 rpmA = 12B = 16C = 18D = 45
nout = rpm
3.Torsion of shaftsMedium
T = 400 N·md = 20 mmL = 0.8 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 = 400 N·md = 20 mmL = 0.8 mG = 80 GPa
φ = °
4.Torsion of shaftsHard
Td = ?

A solid shaft must transmit 20 kW at 300 rpm without the shear stress exceeding 40 MPa. Find the smallest diameter d that works.

P = 20 kWN = 300 rpmτallow = 40 MPa
d = mm
5.Mohr’s circle & stress transformationMedium
σx​ = 120σy​ = −20τxy​ = 40MPa

A point has σₓ = 120 MPa, σᵧ = −20 MPa and τₓᵧ = 40 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 = 120 MPaσy = −20 MPaτxy = 40 MPa
θs = °
6.Mohr’s circle & stress transformationHard
σx​τxy​surface of the shaft

A solid shaft of diameter 50 mm carries an axial tensile force of 180 kN together with a torque of 250 N·m. At the surface of the shaft, find the largest principal stress σ1.

d = 50 mmF = 180 kNT = 250 N·m
σ1 = MPa
7.Axial stress & strainMedium
200 kNØ40120 GPaØ80/60400 mmδ = ?

A steel rod (diameter 40 mm, E = 200 GPa) sits inside a tube made of copper (outer diameter 80 mm, inner diameter 60 mm, E = 120 GPa). Both are 400 mm long and are compressed together between rigid plates by 200 kN. Find the shortening δ.

P = 200 kNrod: Ø40 mm, E = 200 GPatube: Ø80/Ø60 mm, E = 120 GPaL = 400 mm
δ = mm
8.Axial stress & strainHard
Ø 25 mmAluminium2 mØ 20 mmBrass0.5 mP = 50 kN

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

P = 50 kNsegment 1: Ø25 mm, 2 m, aluminium (E = 70 GPa)segment 2: Ø20 mm, 0.5 m, brass (E = 100 GPa)
δ = mm
9.Column bucklingMedium
PL = 6 md = 80 mmcross-section

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

L = 6 mE = 200 GPa (steel)d = 80 mm
Pcr = kN
10.Column bucklingHard
P = 130 kNL = 1.5 md = ?cross-section

A solid round column of length L made of steel is fixed at the base and pinned at the top. It must carry 130 kN with a factor of safety of 2 against buckling. Find the smallest diameter d.

P = 130 kNn = 2L = 1.5 mE = 200 GPa (steel)
d = mm
11.Mechanical vibrationsMedium
k = 100 kN/mζ = 0.7m = 250 kg

A 250 kg mass on a spring with a stiffness of 100 kN/m has a viscous damper giving a damping ratio of 0.7. Find the damped natural frequency fd of its free vibration in Hz.

m = 250 kgk = 100 kN/mζ = 0.7
fd = Hz
12.Mechanical vibrationsHard
k1​ = 30k2​ = 25k3​ = 80m = 25 kg

A 25 kg mass hangs from spring k₃ = 80 kN/m. The top of k₃ is attached to a rigid bar that hangs from two springs side by side, k₁ = 30 kN/m and k₂ = 25 kN/m; the bar stays level. Ignore damping and the masses of the springs and bar. Find the natural frequency fn of vertical vibration in Hz.

m = 25 kgk1 = 30 kN/mk2 = 25 kN/mk3 = 80 kN/m
fn = Hz

3Solutions

1.Gears & gear trains

Answer: nw = 145 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.

Wheel speed

nw = n·z/Nw = 1450·4/40 = 145 rpm

Answer

nw = 145 rpm
2.Gears & gear trains

Answer: nout = 450 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 = 1500·12/16 = 1125 rpm = nC

Second stage

nout = 1125·18/45 = 450 rpm

Answer

nout = 450 rpm

total ratio = 3.333 : 1

3.Torsion of shafts

Answer: φ = 14.59 °

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·20⁴/32 = 15708 mm⁴

Angle of twist

φ = TL/(GJ) = 400·1000·800/(80000·15708) = 0.2546 rad
φ = 0.2546·180/π = 14.59°

Answer

φ = 14.59°
4.Torsion of shafts

Answer: d = 43.28 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·300/60 = 31.42 rad/s
T = P/ω = 20000/31.42 = 636.6 N·m

Diameter from the allowable stress

d = ∛(16T/(π·τallow)) = ∛(16·636620/(π·40)) = 43.28 mm

Answer

d = 43.28 mm

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

5.Mohr’s circle & stress transformation

Answer: θs = −30.13 °

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 = 40/80.62 = 0.4961, sin 2θs = −70/80.62 = −0.8682
2θs = atan2(−70, 40) = −60.26°

Angle on the element

θs = −30.13°
check: θs − θp = −30.13 − 14.87 = −45°

Answer

θs = −30.13°

Positive angles are counter-clockwise.

6.Mohr’s circle & stress transformation

Answer: σ1 = 92.79 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 = 180000/(π·50²/4) = 180000/1963 = 91.67 MPa
τ = 16T/(πd³) = 16·250000/(π·50³) = 10.19 MPa
στxyCσ1​σ2​

Mohr’s circle

C = σ/2 = 45.84 MPa
R = √(45.84² + 10.19²) = 46.95 MPa
σ1 = C + R = 92.79 MPa
σ2 = C − R = −1.118 MPa

Answer

σ1 = 92.79 MPa
7.Axial stress & strain

Answer: δ = 0.1553 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·40²/4 = 1257 mm²
At = π(80² − 60²)/4 = 2199 mm²

Combined axial stiffness

ΣEA = 200·10³·1257 + 120·10³·2199 = 5.152 × 10⁸ N

Shortening

δ = 200000·400/5.152 × 10⁸ = 0.1553 mm

Answer

δ = 0.1553 mm
8.Axial stress & strain

Answer: δ = 3.706 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·25²/4 = 490.9 mm², A2 = π·20²/4 = 314.2 mm²
σ1 = 101.9 MPa
σ2 = 159.2 MPa

Add the segment elongations

δ1 = σ1L1/E1 = 101.9·2000/70000 = 2.91 mm
δ2 = σ2L2/E2 = 159.2·500/100000 = 0.7958 mm
δ = δ1 + δ2 = 3.706 mm

Answer

δ = 3.706 mm
9.Column buckling

Answer: Pcr = 225 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·80⁴/64 = 2.011 × 10⁶ mm⁴

Effective length

KL = 0.7·6000 = 4200 mm

Critical load

Pcr = π²EI/(KL)² = π²·200000·2.011 × 10⁶/4200² = 224989 N = 225 kN

Answer

Pcr = 225 kN
10.Column buckling

Answer: d = 41.47 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 = 2·130000 = 260000 N
KL = 0.7·1500 = 1050 mm

Solve for the diameter

d = (64·n·P·(KL)²/(π³E))^(1/4) = (64·260000·1050²/(π³·200000))^(1/4) = 41.47 mm

Answer

d = 41.47 mm

Check: the slenderness KL/r is 101.3, so the column is slender and Euler applies.

11.Mechanical vibrations

Answer: fd = 2.273 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.

Undamped natural frequency

ωn = √(100000/250) = 20 rad/s
fn = 20/(2π) = 3.183 Hz

Damped natural frequency

fd = fn·√(1 − ζ²) = 3.183·√(1 − 0.7²) = 2.273 Hz

Answer

fd = 2.273 Hz
12.Mechanical vibrations

Answer: fn = 5.747 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

Only k1 and k2 are in parallel. That pair is in series with k3, so combine them as reciprocals.

k12 = 30 + 25 = 55 kN/m
keq = 55·80/(55 + 80) = 32.59 kN/m

Natural frequency

ωn = √(32593/25) = 36.11 rad/s
fn = 36.11/(2π) = 5.747 Hz

Answer

fn = 5.747 Hz

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