Machine Elements · Chapter 10 of 10 · Advanced
Spur and Helical Gears
Gears trade speed for torque at a fixed ratio. The force on a tooth comes from the power and the pitch line, and the Lewis equation treats that tooth as a small cantilever beam.
Readiness check
This closing chapter ties forces to gear geometry. Tick only what you can do closed-notes.
- Relate power, torque, and angular speed.
- Find a pitch-line velocity from diameter and speed.
- Resolve a force into components with an angle.
- Recall bending stress in a cantilever.
- Read a form factor from a table.
The core idea
A gear transmits power as a tangential force at its pitch circle. That force bends the tooth like a tiny cantilever, and the Lewis equation sizes it against bending.
d = mN, V = πdn/60Wt = P/V, Wr = Wt tan φσ = Wt/(b·m·Y)The module m sets the tooth size, and the pitch diameter is d = mN for N teeth. Power flowing through the mesh appears as a tangential force Wt = P/V at the pitch line, plus a radial component Wr = Wt tan φ that pushes the gears apart. That tangential force bends each engaged tooth, and the Lewis equation treats the tooth as a cantilever, giving a bending stress σ = Wt/(b·m·Y) with the form factor Y capturing the tooth shape. A velocity factor then accounts for dynamic load at speed.
The skills, taught in order
Five skills set the gear geometry, the forces at the mesh, the velocity ratio, the Lewis bending stress, and the dynamic correction.
10.1 Gear geometry
The module m (millimetres of pitch diameter per tooth) sets tooth size, so the pitch diameter is d = mN. Standard teeth use a 20° pressure angle and full-depth proportions. Two gears mesh only if they share a module and pressure angle.
10.2 Gear forces
The power transmitted equals the tangential force times the pitch-line velocity, so Wt = P/V = 2T/d. The normal tooth force also has a radial component Wr = Wt tan φ that separates the gears and loads the bearings but transmits no power.
10.3 Velocity ratio
Meshing gears have equal pitch-line velocity, so their speeds are inversely proportional to their tooth counts: n1/n2 = N2/N1. A small pinion driving a large gear trades speed for torque, the reason gearboxes exist.
10.4 Lewis bending stress
Treating the tooth as a cantilever loaded at its tip, the Lewis equation gives σ = Wt/(b·m·Y), with b the face width and Y the Lewis form factor from the tooth count. More teeth give a larger Y and a stronger tooth.
| Number of teeth | Lewis form factor Y |
|---|---|
| 16 | 0.296 |
| 18 | 0.309 |
| 20 | 0.322 |
| 30 | 0.359 |
Lewis form factor for 20° full-depth teeth (Shigley, Table 14-2). Fewer teeth give a weaker, more pointed tooth.
10.5 Velocity factor and AGMA
At speed, meshing errors add a dynamic load, raised by a velocity factor Kv = (6.1 + V)/6.1 for cut teeth. The full AGMA method extends Lewis with factors for load distribution, size, and surface durability (pitting), but the bending core stays the Lewis form.
Engineering connection: the gear forces here set the bending moment on the shaft of Chapter 6 and the radial load on the bearings of Chapter 9, closing the drivetrain.
Worked example 1: forces on a spur gear
A 20-tooth spur pinion of module 4 mm runs at 1200 rev/min and transmits 5 kW. With a 20° pressure angle, find the pitch-line velocity, the tangential force, and the radial force.
- ProblemFind V, Wt, and Wr for the pinion in Figure 1.
- Given / findN = 20, m = 4 mm, n = 1200 rev/min, P = 5 kW, φ = 20°. Find V, Wt, Wr.
- AssumptionsPower transmitted entirely at the pitch line; standard 20° pressure angle.
- ModelPitch diameter d = mN; velocity V = πdn/60; Wt = P/V; Wr = Wt tan φ.
- Equationsd = mN, V = πdn/60Wt = P/V, Wr = Wt tan φ
- Solved = 4 × 20 = 80 mm = 0.080 m. V = π(0.080)(1200)/60 = 5.03 m/s. Wt = 5000/5.03 = 995 N. Wr = 995 × tan 20° = 995 × 0.364 = 362 N.
- CheckBy torque, T = P/ω = 5000/(2π·1200/60) = 39.8 N·m, and Wt = 2T/d = 2(39.8)/0.080 = 995 N, matching. The radial force is about a third of the tangential, as tan 20° gives.
- ConclusionThe tangential force does the work and bends the teeth; the radial force only loads the bearings. Both are needed for the shaft and bearing design.
Worked example 2: Lewis bending stress
The same gear (Wt = 995 N, module 4 mm, 20 teeth so Y = 0.322) has a face width of 40 mm. Find the Lewis bending stress, then apply the velocity factor for V = 5.03 m/s.
- ProblemFind the Lewis bending stress, static and velocity-corrected, for the tooth in Figure 2.
- Given / findWt = 995 N, m = 4 mm, Y = 0.322, b = 40 mm, V = 5.03 m/s. Find σ and the corrected σ.
- AssumptionsTooth as a cantilever loaded at the tip; single tooth carries the full load; cut teeth (Barth velocity factor).
- ModelLewis σ = Wt/(b·m·Y), then multiply by Kv = (6.1 + V)/6.1.
- Equationsσ = Wt/(b·m·Y)Kv = (6.1 + V)/6.1
- Solveσ = 995/(40 × 4 × 0.322) = 995/51.5 = 19.3 MPa. Kv = (6.1 + 5.03)/6.1 = 1.82. Corrected σ = 1.82 × 19.3 = 35.2 MPa.
- CheckThe static stress is modest, but the velocity factor nearly doubles it, showing why speed matters. A steel gear with this stress has a large bending margin; pitting durability would likely govern instead.
- ConclusionLewis sizes the tooth against bending, and the velocity factor brings in dynamic load. The full AGMA method refines this, but the cantilever idea is the core.
Misconceptions and diagnostics
| Mistake | Symptom | Diagnostic question | Correction |
|---|---|---|---|
| Using the radial force for power | Wrong transmitted load | "Which force is tangent to the pitch circle?" | Only Wt transmits power; Wr just loads bearings. |
| Ignoring the velocity factor | Stress under-predicted at speed | "Is the pitch-line velocity high?" | Apply Kv = (6.1 + V)/6.1 for cut teeth. |
| Wrong Y for the tooth count | Stress off for the pinion | "Did I read Y at this number of teeth?" | Use the form factor for the actual tooth count. |
| Checking only bending | Gear pits before it breaks | "Is surface durability checked too?" | Also check contact (pitting) stress in the AGMA method. |
Practice ladder
A gear of module 5 mm has 30 teeth. Find its pitch diameter.
Show answer
d = mN = 5 × 30 = 150 mm. The module times the tooth count is the pitch diameter directly.
The pinion of Worked Example 1 drives a 60-tooth gear. Find the output speed and the velocity ratio.
Show answer
n2 = n1(N1/N2) = 1200(20/60) = 400 rev/min. The ratio is 3:1, trading speed for three times the torque.
A spur gear transmits Wt = 1500 N with module 5 mm, face width 50 mm, and 18 teeth (Y = 0.309). Find the static Lewis stress.
Show answer
σ = Wt/(b·m·Y) = 1500/(50 × 5 × 0.309) = 1500/77.25 = 19.4 MPa.
Find a real geartrain (a drill, a bicycle, a clock). Identify the pinion and gear, estimate the ratio, and explain what it trades and why.
What good work looks like
A tooth-count ratio that matches the speed or torque change, and a clear statement of what the gearset is for: speed reduction, torque multiplication, or direction change.
Working with AI, and proving it yourself
Use AI as an examiner, not a solver
Portfolio task
Analyse a real gear pair: find the module and ratio, compute the tangential and radial forces from the power, and find the Lewis bending stress with the velocity factor.
Retrieval and spaced review
Closed notes. Answer out loud, then reveal.
1. Relate pitch diameter, module, and tooth count.
d = mN, the module times the number of teeth.
2. Write the tangential and radial gear forces.
Wt = P/V = 2T/d, and Wr = Wt tan φ.
3. State the velocity ratio.
n1/n2 = N2/N1: speeds are inverse to tooth counts.
4. Write the Lewis bending stress.
σ = Wt/(b·m·Y), with Y the Lewis form factor.
5. Why apply a velocity factor?
Meshing errors add a dynamic load at speed, raised by Kv = (6.1 + V)/6.1.
Textbook mapping
| Item | Mapping |
|---|---|
| Primary source | Budynas and Nisbett, Shigley's Mechanical Engineering Design, Chapters 13 and 14 (Gears and Spur/Helical Gears) |
| Cross-reference | Norton, Ch. 12 · Manufacturing Processes (gear cutting) |
| Core topics | 10.1 Gear geometry · 10.2 Gear forces · 10.3 Velocity ratio · 10.4 Lewis bending stress · 10.5 Velocity factor and AGMA |
| Engineering connection | Gear forces set the loads on the shaft and bearings, completing the drivetrain. |
| Read next | Return to the Machine Elements hub and integrate the elements. |