3.2 Spur, Helical, Bevel & Worm Gears and Epicyclic Gear Trains

Key Takeaways

  • Involute gear geometry is governed by Diametral Pitch P=N/dP = N/d (teeth/in) or Module m=d/Nm = d/N (mm/tooth), with circular pitch p=π/P=πmp = \pi/P = \pi m and base pitch pb=pcos⁡ϕp_b = p \cos\phi.

  • To eliminate interference and root undercutting during hobbing of standard 20∘20^\circ full-depth spur gears, the minimum pinion tooth count is Nmin⁡=2ksin⁡2(20∘)=18N_{\min} = \frac{2k}{\sin^2(20^\circ)} = 18 teeth (1212 teeth for 25∘25^\circ).

  • Gear tooth forces decompose into transmitted tangential force Wt=2T/dW_t = 2T/d, radial separating force Wr=Wttan⁡ϕtW_r = W_t \tan\phi_t, and axial thrust force Wa=Wttan⁡ψW_a = W_t \tan\psi (for helical gears) or Wa=Wttan⁡ϕsin⁡γW_a = W_t \tan\phi \sin\gamma (for bevel gears).

  • AGMA rating decouples gear failure into root bending fatigue (σb∝Wt\sigma_b \propto W_t) and surface Hertzian contact pitting (σc∝Wt\sigma_c \propto \sqrt{W_t}); doubling torque doubles bending stress (2.0×2.0\times) but increases contact stress by only 2≈1.414×\sqrt{2} \approx 1.414\times.

  • Epicyclic (planetary) gear train velocity ratios are resolved using the Willis relative formula nL−nCnF−nC=etrain\frac{n_L - n_C}{n_F - n_C} = e_{\text{train}} with carrier speed nCn_C, sun, planet, and ring gears satisfying NR=NS+2NPN_R = N_S + 2 N_P.

Last updated: August 2026

Spur, Helical, Bevel & Worm Gears and Epicyclic Gear Trains

Gears are toothed cylindrical or conical mechanical elements designed to transmit positive, non-slip angular velocity and mechanical torque between rotating shafts. On the NCEES PE Mechanical exam, gear problems evaluate five fundamental competencies: involute tooth geometry and conjugate action, kinematic interference and undercutting limits, static and dynamic 3D tooth force resolution, AGMA fatigue ratings (tooth root bending vs. surface pitting), and compound/planetary gear train kinematics.

+---------------------------------------------------------------------------------------------------+
|                                GEAR CLASSIFICATION & CHARACTERISTICS                              |
|                                                                                                   |
|   SPUR GEARS:             HELICAL GEARS:           BEVEL GEARS:             WORM GEARSETS:        |
|   - Parallel shafts       - Parallel / Crossed     - Intersecting shafts    - Non-intersecting    |
|   - Straight axial teeth  - Inclined helix angle   - Conical pitch surface  - 90 deg shaft angle  |
|   - Zero axial thrust     - High contact ratio     - Combined thrust/radial - High ratio (10-100) |
|   - Low cost / standard   - Quiet & smooth mesh    - Shaft angle (Sigma=90) - Self-locking action |
+---------------------------------------------------------------------------------------------------+

1. Fundamentals of Involute Gear Tooth Geometry

Modern gears utilize the involute of a circle tooth profile because it satisfies the Fundamental Law of Gearing: the common normal to the tooth profiles at all points of contact must pass through a fixed pitch point (PP), ensuring a strictly constant angular velocity ratio (mV=ωin/ωout=constm_V = \omega_{\text{in}}/\omega_{\text{out}} = \text{const}) regardless of center distance variation.

+---------------------------------------------------------------------------------------------------+
|                             INVOLUTE SPUR GEAR TOOTH NOMENCLATURE                                 |
|                                                                                                   |
|                                    Addendum Circle (d_a = d + 2a)                                 |
|                            ---------------------------------------------                          |
|                            ^                                                                      |
|                  Addendum  | a = 1/P = 1.0 m                                                      |
|                            v       Pitch Circle (d = N/P = m*N)                                   |
|   =========================+============================================                          |
|                            ^                                                                      |
|                  Dedendum  | b = 1.25/P = 1.25 m                                                  |
|                            v       Base Circle (d_b = d * cos(phi))                               |
|                            ---------------------------------------------                          |
|                                    Dedendum / Root Circle (d_r = d - 2b)                          |
|                            ---------------------------------------------                          |
|                                                                                                   |
|   Circular Pitch: p = pi*d / N = pi/P = pi*m    |    Base Pitch: p_b = p * cos(phi)               |
|   Whole Depth: h_t = a + b = 2.25/P             |    Clearance: c = b - a = 0.25/P                |
+---------------------------------------------------------------------------------------------------+

Essential Geometric Equations

ParameterUS Customary FormulaSI Metric FormulaDefinition & Significance
Diametral Pitch (PP)P=NdP = \frac{N}{d}P=25.4mP = \frac{25.4}{m}Teeth per inch of pitch diameter
Module (mm)m=25.4Pm = \frac{25.4}{P}m=dNm = \frac{d}{N}Millimeters of pitch diameter per tooth
Pitch Diameter (dd)d=NPd = \frac{N}{P}d=mNd = m NOperating reference diameter
Circular Pitch (pp)p=πdN=πPp = \frac{\pi d}{N} = \frac{\pi}{P}p=πmp = \pi mArc length between adjacent tooth centers (p⋅P=πp \cdot P = \pi)
Base Circle (dbd_b)db=dcos⁡ϕd_b = d \cos\phidb=dcos⁡ϕd_b = d \cos\phiDiameter where involute generation begins
Base Pitch (pbp_b)pb=pcos⁡ϕp_b = p \cos\phipb=pcos⁡ϕp_b = p \cos\phiDistance between teeth along the line of action
Addendum (aa)a=1.0Pa = \frac{1.0}{P}a=1.0ma = 1.0 mRadial height above pitch circle (full depth)
Dedendum (bb)b=1.25Pb = \frac{1.25}{P}b=1.25mb = 1.25 mRadial depth below pitch circle
Center Distance (CC)C=NP+NG2PC = \frac{N_P + N_G}{2 P}C=m(NP+NG)2C = \frac{m(N_P + N_G)}{2}Nominal shaft centerline spacing

Interference, Undercutting & Minimum Pinion Teeth

When generating teeth with a rack cutter or hob, if the addendum of the generating rack extends inside the tangency point of the base circle, the cutter cuts away ("undercuts") the flank of the tooth, severely weakening the root fillet. To prevent undercutting in standard full-depth spur gears:

Nmin⁡=2ksin⁡2ϕN_{\min} = \frac{2 k}{\sin^2\phi}

Where k=1.0k = 1.0 for standard full-depth teeth and k=0.8k = 0.8 for stub teeth:

  • For ϕ=20∘\phi = 20^\circ full-depth (k=1k=1): Nmin⁡=2(1)sin⁡2(20∘)=20.11698=17.1  ⟹  18 teethN_{\min} = \frac{2(1)}{\sin^2(20^\circ)} = \frac{2}{0.11698} = 17.1 \implies \mathbf{18\text{ teeth}}.
  • For ϕ=25∘\phi = 25^\circ full-depth (k=1k=1): Nmin⁡=2(1)sin⁡2(25∘)=20.17861=11.2  ⟹  12 teethN_{\min} = \frac{2(1)}{\sin^2(25^\circ)} = \frac{2}{0.17861} = 11.2 \implies \mathbf{12\text{ teeth}}.
  • For ϕ=14.5∘\phi = 14.5^\circ full-depth (k=1k=1, obsolete): Nmin⁡=2(1)sin⁡2(14.5∘)=31.9  ⟹  32 teethN_{\min} = \frac{2(1)}{\sin^2(14.5^\circ)} = 31.9 \implies \mathbf{32\text{ teeth}}.

2. Pitch Line Velocity and 3D Tooth Force Resolution

Power is transmitted at the pitch circle at linear pitch line velocity VV:

V=πdPNP12(ft/min in US Customary, with dP in inches, NP in rpm)V = \frac{\pi d_P N_P}{12} \quad (\text{ft/min in US Customary, with } d_P \text{ in inches, } N_P \text{ in rpm}) V=πdPNP60×1000(m/s in SI, with dP in mm, NP in rpm)V = \frac{\pi d_P N_P}{60 \times 1000} \quad (\text{m/s in SI, with } d_P \text{ in mm, } N_P \text{ in rpm})
+---------------------------------------------------------------------------------------------------+
|                                 GEAR TOOTH FORCE VECTORS                                          |
|                                                                                                   |
|   SPUR GEAR TOOTH FORCES:                           HELICAL GEAR TOOTH FORCES:                    |
|                                                                                                   |
|                 W (Total Normal Load)                             W_a (Axial Thrust = W_t*tan(psi)|
|                      /|                                              <------                      |
|                     / |                                                   | \                     |
|                    /  | W_r = W_t * tan(phi)                              |  \                    |
|                   /   |                                    W_r = W_t*tan(phi_t) \                 |
|                  /phi |                                                   |    \ W (Total Normal) |
|                 +-----+                                                   | phi_t\                |
|                   W_t (Tangential Load)                                   +-------+               |
|                                                                               W_t                 |
+---------------------------------------------------------------------------------------------------+

1. Spur Gear Force Resolution

  • Tangential Force (WtW_t): Transmits power and driving torque TT. Wt=33000PhpV=2TdP(US: Wt in lbf)∣Wt=1000PkWV=2TdP(SI: Wt in N)W_t = \frac{33000 P_{\text{hp}}}{V} = \frac{2 T}{d_P} \quad (\text{US: } W_t \text{ in lbf}) \quad \Big| \quad W_t = \frac{1000 P_{\text{kW}}}{V} = \frac{2 T}{d_P} \quad (\text{SI: } W_t \text{ in N})
  • Radial Separating Force (WrW_r): Pushes gear shafts apart, loading support bearings. Wr=Wttan⁡ϕW_r = W_t \tan\phi
  • Total Normal Force (WW): Acts perpendicular to the tooth involute along the line of action. W=Wtcos⁡ϕ=Wt2+Wr2W = \frac{W_t}{\cos\phi} = \sqrt{W_t^2 + W_r^2}

2. Helical Gear Force Resolution

Helical teeth are cut at helix angle ψ\psi. Transverse pressure angle ϕt\phi_t and normal pressure angle ϕn\phi_n are related by:

tan⁡ϕt=tan⁡ϕncos⁡ψ\tan\phi_t = \frac{\tan\phi_n}{\cos\psi} Normal Pitch: Pn=Ptcos⁡ψ,pn=ptcos⁡ψ\text{Normal Pitch: } P_n = \frac{P_t}{\cos\psi}, \quad p_n = p_t \cos\psi
  • Tangential Load: Wt=2TdPW_t = \frac{2 T}{d_P}
  • Axial (Thrust) Load: Wa=Wttan⁡ψW_a = W_t \tan\psi (requires thrust bearings or herringbone double-helical teeth to cancel)
  • Radial Separating Load: Wr=Wttan⁡ϕt=Wttan⁡ϕncos⁡ψW_r = W_t \tan\phi_t = W_t \frac{\tan\phi_n}{\cos\psi}
  • Total Resultant Normal Load: W=Wtcos⁡ϕncos⁡ψ=Wt2+Wr2+Wa2W = \frac{W_t}{\cos\phi_n \cos\psi} = \sqrt{W_t^2 + W_r^2 + W_a^2}

3. Straight Bevel Gear Force Resolution

Bevel gears operate on intersecting shafts (typically at shaft angle Σ=90∘\Sigma = 90^\circ). Pitch cone angles satisfy tan⁡γ=NPNG\tan\gamma = \frac{N_P}{N_G} (pinion) and tan⁡Γ=NGNP\tan\Gamma = \frac{N_G}{N_P} (gear).

  • Tangential Force: Wt=2TdavgW_t = \frac{2 T}{d_{\text{avg}}} (acting at midpoint of tooth face)
  • Radial Separating Force (Pinion): WrP=Wttan⁡ϕcos⁡γW_{rP} = W_t \tan\phi \cos\gamma
  • Axial Thrust Force (Pinion): WaP=Wttan⁡ϕsin⁡γW_{aP} = W_t \tan\phi \sin\gamma
  • (Note: For 90∘90^\circ shaft angle, WaP=WrGW_{aP} = W_{rG} and WrP=WaGW_{rP} = W_{aG})

4. Worm Gearset Forces & Efficiency

A worm gearset transmits power between non-intersecting, perpendicular shafts. Ratio mG=NGNWm_G = \frac{N_G}{N_W} (where NWN_W is number of worm starts: 1, 2, 3, or 4). Lead angle λ\lambda satisfies tan⁡λ=LπdW=NWpxπdW\tan\lambda = \frac{L}{\pi d_W} = \frac{N_W p_x}{\pi d_W}.

  • Equilibrium Relations: Wt,W=Wa,GW_{t,W} = W_{a,G}, Wa,W=Wt,GW_{a,W} = W_{t,G}, and Wr,W=Wr,GW_{r,W} = W_{r,G}.
  • Mesh Efficiency with Friction μ\mu: η=cos⁡ϕn−μtan⁡λcos⁡ϕn+μcot⁡λ\eta = \frac{\cos\phi_n - \mu \tan\lambda}{\cos\phi_n + \mu \cot\lambda}
  • Self-Locking Condition: The gearset cannot be backdriven by the gear when tan⁡λ≤μ\tan\lambda \le \mu (typically λ<5∘\lambda < 5^\circ).

3. AGMA Tooth Root Bending Fatigue Rating

Gear teeth act as short cantilever beams. The AGMA bending stress equation modifies the classic Lewis formula with empirical dynamic and geometry correction factors:

σb=WtKoKvKsPFKmKBJ≤StYNSFYθYZ(US Customary)\sigma_b = W_t K_o K_v K_s \frac{P}{F} \frac{K_m K_B}{J} \le \frac{S_t Y_N}{S_F Y_\theta Y_Z} \quad (\text{US Customary}) σb=WtbmKAKvKsKH1YJ≤σFPYNSFYθYZ(SI Metric)\sigma_b = \frac{W_t}{b m} K_A K_v K_s K_H \frac{1}{Y_J} \le \frac{\sigma_{FP} Y_N}{S_F Y_\theta Y_Z} \quad (\text{SI Metric})

Where:

  • Wt=Transmitted tangential load (lbf or N)W_t = \text{Transmitted tangential load (lbf or N)}
  • P=Diametral pitch (in−1)P = \text{Diametral pitch (}\text{in}^{-1}\text{)}, m=Module (mm)m = \text{Module (mm)}
  • F=b=Face width (in or mm)F = b = \text{Face width (in or mm)} (Standard range: 9P≤F≤14P\frac{9}{P} \le F \le \frac{14}{P})
  • J=YJ=AGMA Bending Geometry Factor (incorporates Lewis form factor Y and root stress concentration Kf)J = Y_J = \text{AGMA Bending Geometry Factor (incorporates Lewis form factor } Y \text{ and root stress concentration } K_f\text{)}
  • Ko=KA=Overload / Application factor (1.0 uniform, 1.50 moderate shock, 2.0+ heavy shock)K_o = K_A = \text{Overload / Application factor (1.0 uniform, 1.50 moderate shock, 2.0+ heavy shock)}
  • Kv=Dynamic factor (accounts for tooth pitch errors and pitch-line velocity vibration)K_v = \text{Dynamic factor (accounts for tooth pitch errors and pitch-line velocity vibration)}
  • Ks=Size factor (1.0 for standard pitches)K_s = \text{Size factor (1.0 for standard pitches)}
  • Km=KH=Load distribution factor (accounts for shaft deflection and face crowning)K_m = K_H = \text{Load distribution factor (accounts for shaft deflection and face crowning)}
  • KB=Rim thickness factor (1.0 for solid gear webs)K_B = \text{Rim thickness factor (1.0 for solid gear webs)}
  • St=σFP=AGMA allowable bending fatigue strengthS_t = \sigma_{FP} = \text{AGMA allowable bending fatigue strength}
  • SF=Design safety factor against tooth bending breakageS_F = \text{Design safety factor against tooth bending breakage}

4. AGMA Surface Pitting Fatigue / Contact Stress

Surface fatigue failure (macropitting) occurs when cyclic Hertzian contact stresses exceed the surface endurance limit of the tooth material:

σc=CpWtKoKvKsKmCfdPFI≤ScZNCHSHYθYZ\sigma_c = C_p \sqrt{W_t K_o K_v K_s \frac{K_m C_f}{d_P F I}} \le \frac{S_c Z_N C_H}{S_H Y_\theta Y_Z}

Where:

  • Cp=Elastic Coefficient=1π(1−νP2EP+1−νG2EG)C_p = \text{Elastic Coefficient} = \sqrt{\frac{1}{\pi \left( \frac{1 - \nu_P^2}{E_P} + \frac{1 - \nu_G^2}{E_G} \right)}} (Cp≈2300psiC_p \approx 2300\sqrt{\text{psi}} or 191MPa191\sqrt{\text{MPa}} for steel-on-steel)
  • I=Surface Geometry Factor=sin⁡ϕcos⁡ϕ2mNmGmG+1I = \text{Surface Geometry Factor} = \frac{\sin\phi \cos\phi}{2 m_N} \frac{m_G}{m_G + 1} (for external spur gears)
  • dP=Pinion pitch diameterd_P = \text{Pinion pitch diameter}, F=Face widthF = \text{Face width}
  • Cf=Surface condition factor (1.0)C_f = \text{Surface condition factor (1.0)}
  • Sc=AGMA allowable contact fatigue strengthS_c = \text{AGMA allowable contact fatigue strength}
  • SH=Design safety factor against surface pittingS_H = \text{Design safety factor against surface pitting}

Note

Bending vs. Contact Stress Scaling: Bending stress scales linearly with load (σb∝Wt\sigma_b \propto W_t), whereas contact stress scales with the square root of load (σc∝Wt\sigma_c \propto \sqrt{W_t}). Doubling transmitted torque doubles root bending stress (+100%+100\%), but increases contact stress by only 41.4%41.4\% (2=1.414\sqrt{2} = 1.414). Surface pitting resistance almost universally governs steel gear sizing.


5. Gear Train Kinematics & Planetary Gear Trains

+---------------------------------------------------------------------------------------------------+
|                                 GEAR TRAIN CONFIGURATIONS                                         |
|                                                                                                   |
|   SIMPLE TRAIN:                COMPOUND TRAIN:              PLANETARY (EPICYCLIC) TRAIN:          |
|   - One gear per shaft         - Multiple gears per shaft   - Sun (S), Planets (P), Ring (R)      |
|   - Idlers change direction    - Velocity ratio multiplied  - Carrier / Arm (C) rotates           |
|   - e = (-1)^k * (N_in/N_out)  - e = (Prod N_in)/(Prod N_out)- Willis: (n_L - n_C)/(n_F - n_C) = e |
+---------------------------------------------------------------------------------------------------+

1. Simple and Compound Gear Trains

  • Simple Train: Idler gears between input and output reverse the direction of rotation but have zero effect on overall velocity ratio (e=(−1)kNinNoute = (-1)^k \frac{N_{\text{in}}}{N_{\text{out}}}, where kk is number of external meshes).
  • Compound Train: Multiple gears keyed to intermediate shafts multiply reductions: e=ωoutputωinput=∏Teeth on Driving Gears∏Teeth on Driven Gearse = \frac{\omega_{\text{output}}}{\omega_{\text{input}}} = \frac{\prod \text{Teeth on Driving Gears}}{\prod \text{Teeth on Driven Gears}}

2. Planetary (Epicyclic) Gear Trains

Planetary gearsets provide high reduction ratios in compact, coaxial packages. A standard planetary set comprises a central Sun gear (SS), multiple Planet gears (PP), an internal toothed Ring gear (RR), and a rotating Carrier/Arm (CC).

+---------------------------------------------------------------------------------------------------+
|                             PLANETARY GEARSET COAXIAL GEOMETRY                                    |
|                                                                                                   |
|                                    +-----------------------+                                      |
|                                  /       RING GEAR (R)       \                                    |
|                                /       +---------------+       \                                  |
|                               |       /  PLANET (P)     \       |  Geometric Pitch Rule:          |
|                               |      |   (d_P, N_P)      |      |  d_R = d_S + 2*d_P              |
|                               |       \                 /       |                                 |
|                               |        +---------------+        |  Tooth Count Rule:              |
|                               |       /    SUN (S)      \       |  N_R = N_S + 2*N_P              |
|                               |      |   (d_S, N_S)      |      |                                 |
|                               |       \                 /       |  (For module m = const)         |
|                                \       +---------------+       /                                  |
|                                  \                           /                                    |
|                                    +-----------------------+                                      |
+---------------------------------------------------------------------------------------------------+

The Willis Relative Velocity Equation

Fix the carrier in thought to determine the basic train value etraine_{\text{train}} from first gear (FF) to last gear (LL):

nL−nCnF−nC=etrain\frac{n_L - n_C}{n_F - n_C} = e_{\text{train}}

Where nFn_F, nLn_L, and nCn_C are rotational speeds of First gear, Last gear, and Carrier. With Sun as first gear and Ring as last gear: etrain=−NSNRe_{\text{train}} = -\frac{N_S}{N_R}.

Standard Planetary Operational Modes

Fixed ElementInput ElementOutput ElementOverall Speed Ratio (nin/noutn_{\text{in}} / n_{\text{out}})Direction
Ring Gear (nR=0n_R = 0)Sun Gear (SS)Carrier (CC)1+NRNS1 + \frac{N_R}{N_S}Same as Input (Reduction)
Sun Gear (nS=0n_S = 0)Ring Gear (RR)Carrier (CC)1+NSNR=NR+NSNR1 + \frac{N_S}{N_R} = \frac{N_R + N_S}{N_R}Same as Input (Reduction)
Carrier (nC=0n_C = 0)Sun Gear (SS)Ring Gear (RR)−NRNS-\frac{N_R}{N_S}Opposite (Reverse Drive)

6. Step-by-Step Worked Problem: Helical Gear Forces & Planetary Ratio

Problem Statement

  1. A 20∘20^\circ normal pressure angle (ϕn=20∘\phi_n = 20^\circ) helical pinion with NP=24N_P = 24 teeth, transverse diametral pitch Pt=6 in−1P_t = 6\text{ in}^{-1}, and right-hand helix angle ψ=30∘\psi = 30^\circ transmits 30 hp30\text{ hp} at 1800 rpm1800\text{ rpm} to a driven gear. Determine pitch diameter dPd_P, pitch line velocity VV, tangential force WtW_t, radial force WrW_r, and axial thrust force WaW_a.
  2. A planetary gearset has a Sun gear with NS=20N_S = 20 teeth and a Ring gear with NR=80N_R = 80 teeth. If the Ring gear is fixed (nR=0n_R = 0) and the Sun rotates clockwise at 1500 rpm1500\text{ rpm}, compute the Carrier output speed nCn_C and the number of teeth on each Planet gear NPN_P.

Step-by-Step Solution

Part 1: Helical Gear Force Calculation

  • Pitch diameter: dP=NPPt=246=4.0 inchesd_P = \frac{N_P}{P_t} = \frac{24}{6} = 4.0\text{ inches}.
  • Pitch line velocity: V=πdPNP12=π(4.0)(1800)12=1884.96 ft/minV = \frac{\pi d_P N_P}{12} = \frac{\pi (4.0)(1800)}{12} = 1884.96\text{ ft/min}.
  • Transmitted tangential force: Wt=33000PhpV=33000×301884.96=525.2 lbfW_t = \frac{33000 P_{\text{hp}}}{V} = \frac{33000 \times 30}{1884.96} = 525.2\text{ lbf}.
  • Axial thrust force: Wa=Wttan⁡ψ=525.2×tan⁡(30∘)=525.2×0.57735=303.2 lbfW_a = W_t \tan\psi = 525.2 \times \tan(30^\circ) = 525.2 \times 0.57735 = 303.2\text{ lbf}.
  • Transverse pressure angle: tan⁡ϕt=tan⁡ϕncos⁡ψ=tan⁡(20∘)cos⁡(30∘)=0.363970.86603=0.42027  ⟹  ϕt=22.80∘\tan\phi_t = \frac{\tan\phi_n}{\cos\psi} = \frac{\tan(20^\circ)}{\cos(30^\circ)} = \frac{0.36397}{0.86603} = 0.42027 \implies \phi_t = 22.80^\circ.
  • Radial separating force: Wr=Wttan⁡ϕt=525.2×0.42027=220.7 lbfW_r = W_t \tan\phi_t = 525.2 \times 0.42027 = 220.7\text{ lbf}.
  • Total resultant load: W=Wt2+Wr2+Wa2=525.22+220.72+303.22=645.4 lbfW = \sqrt{W_t^2 + W_r^2 + W_a^2} = \sqrt{525.2^2 + 220.7^2 + 303.2^2} = 645.4\text{ lbf}.

Part 2: Planetary Kinematics

  • Planet tooth count: NR=NS+2NP  ⟹  80=20+2NP  ⟹  2NP=60  ⟹  NP=30 teethN_R = N_S + 2 N_P \implies 80 = 20 + 2 N_P \implies 2 N_P = 60 \implies \mathbf{N_P = 30\text{ teeth}}.
  • Carrier speed using Willis formula (Sun = First, Ring = Last, etrain=−NSNR=−2080=−0.25e_{\text{train}} = -\frac{N_S}{N_R} = -\frac{20}{80} = -0.25): nR−nCnS−nC=−0.25  ⟹  0−nC1500−nC=−0.25\frac{n_R - n_C}{n_S - n_C} = -0.25 \implies \frac{0 - n_C}{1500 - n_C} = -0.25 −nC=−0.25(1500−nC)=−375+0.25nC  ⟹  1.25nC=375-n_C = -0.25(1500 - n_C) = -375 + 0.25 n_C \implies 1.25 n_C = 375 nC=3751.25=+300 rpm (Clockwise)n_C = \frac{375}{1.25} = \mathbf{+300\text{ rpm (Clockwise)}} (Ratio is 1+NRNS=1+8020=5:11 + \frac{N_R}{N_S} = 1 + \frac{80}{20} = 5:1 reduction).

7. Exam Tips & Common Traps

Tip

Planetary Gear Shortcut: When the Ring gear is stationary (nR=0n_R = 0), the ratio from Sun to Carrier is always 1+(NR/NS)1 + (N_R / N_S). You can solve speed in 5 seconds without writing out the full Willis formula.

Warning

Common Traps to Avoid:

  • Normal vs Transverse Pitch: For helical gears, normal pitch PnP_n is greater than transverse pitch PtP_t (Pn=Pt/cos⁡ψP_n = P_t / \cos\psi). Pitch diameter is computed using transverse pitch (d=N/Ptd = N/P_t).
  • Worm Gear Efficiency Sign: Make sure to distinguish between driving through the worm vs backdriving through the gear. Worms with lead angle λ<tan⁡−1(μ)\lambda < \tan^{-1}(\mu) cannot be backdriven.
Test Your Knowledge

What is the theoretical minimum number of teeth required on a standard full-depth spur pinion with a 20-degree pressure angle to completely prevent tooth undercutting during manufacture with a standard rack hob?

A

12 teeth

B

14 teeth

C

17 teeth

D

18 teeth

Test Your Knowledge

If transmitted torque across a pair of commercial spur gears is doubled (2.0x), how do the tooth root bending stress (sigma_b) and surface Hertzian contact stress (sigma_c) change, assuming geometry and speed remain constant?

A

Bending stress increases by 2.0x, and contact stress increases by 2.0x.

B

Bending stress increases by 2.0x, and contact stress increases by 1.414x (sqrt(2)).

C

Bending stress increases by 1.414x, and contact stress increases by 2.0x.

D

Bending stress increases by 4.0x, and contact stress increases by 2.0x.

Test Your Knowledge

A planetary gearset has a stationary Ring gear with N_R = 72 teeth and a Sun gear with N_S = 24 teeth. If the Sun gear rotates at 1200 rpm clockwise, what is the rotational speed and direction of the output carrier?

A

300 rpm clockwise

B

400 rpm clockwise

C

240 rpm clockwise

D

400 rpm counterclockwise

Test Your Knowledge

A worm gearset has a double-threaded worm (N_W = 2) rotating at 1750 rpm driving a 60-tooth worm wheel (N_G = 60). What is the output speed of the worm wheel and the velocity ratio?

A

29.17 rpm with ratio 60:1

B

58.33 rpm with ratio 30:1

C

87.50 rpm with ratio 20:1

D

116.67 rpm with ratio 15:1

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