| name | tribology |
| description | Tribology — lubrication regimes (Stribeck curve), hydrodynamic bearing theory (Reynolds equation), EHD lubrication, film thickness, wear models (Archard), friction, lubricant viscosity selection. |
| metadata | {"priority":7,"promptSignals":{"phrases":["tribology","lubrication","friction","wear","Stribeck","hydrodynamic bearing","EHD","lubricant","viscosity","bearing film"],"minScore":4}} |
Tribology — Complete Skill
Lubrication Regimes (Stribeck Curve)
Plot: friction coefficient μ vs. Hersey number (ηN/P = viscosity × speed / load)
Boundary Lubrication (low ηN/P)
Surfaces in contact; asperity contact dominates
μ = 0.05-0.15 (with boundary additives), 0.3-0.5 (dry)
Wear rate high; controlled by surface chemistry (EP/AW additives)
Mixed Lubrication
Partial fluid film + asperity contact
μ = 0.01-0.1
Transition region; running-in phase of new machinery
Hydrodynamic (HD) Lubrication (high ηN/P)
Full fluid film separates surfaces; no solid contact
μ = 0.001-0.005 (viscous drag only)
Film thickness >> surface roughness (h_min/R_q > 3: λ ratio = film parameter)
Governed by Reynolds equation
Elastohydrodynamic (EHD) Lubrication
HD film with elastic deformation of surfaces + pressure-viscosity effect
Occurs in: rolling element bearings, gears (Hertz contact + thin film)
Film thickness much thinner than HD (μm scale)
Lambda (Λ) Ratio (Film Parameter)
Λ = h_min / √(R_q1² + R_q2²)
Λ > 3: full film (EHD regime), negligible wear
1 < Λ < 3: mixed lubrication, some asperity contact
Λ < 1: boundary lubrication, significant wear
R_q = RMS roughness of each surface [μm]
Reynolds Equation (Hydrodynamic Theory)
∂/∂x(h³/η × ∂p/∂x) + ∂/∂z(h³/η × ∂p/∂z) = 6U × ∂h/∂x + 12 × ∂h/∂t
Where:
h(x) = film thickness [m]
η = dynamic viscosity [Pa·s]
p = pressure [Pa]
U = entraining velocity = (U₁ + U₂)/2
Simplified (1D, Rigid Surfaces)
For inclined slider: p(x) from ∂/∂x(h³∂p/∂x) = 6ηU × ∂h/∂x
Sommerfeld solution for journal bearings (full 360° film)
Journal Bearing Theory
Sommerfeld Number (S)
S = (r/c)² × η × N / P
r = journal radius, c = radial clearance, N = speed [rev/s], P = load/projected area
Short bearing approximation (L/D < 0.5):
ε = eccentricity ratio = e/c (e = journal offset from center)
From load → S → ε (eccentricity curve)
Minimum film thickness:
h_min = c(1 - ε)
Design requirement: h_min > 5 × R_q_surface (λ > 5 for safe operation)
Typical values:
Clearance ratio c/r: 0.001-0.003 (1-3‰ of radius)
Sommerfeld number for full film: S > 0.1
Petroff's equation (lightly loaded, concentric):
μ = 2π²η × r/c × N/P (friction coefficient)
Friction power: P_fric = μ × W × r × ω
Oil film temperature rise:
ΔT ≈ P_fric / (ṁ_oil × c_p_oil) [≤ 20-30°C rise acceptable]
EHD Film Thickness (Rolling Contacts)
Dowson-Higginson Formula (Line Contact — Gears, Cylindrical Bearings)
h_min = 2.65 × α^0.54 × (η₀U)^0.7 × R'^0.43 / (E'^0.03 × W'^0.13)
Dimensionless groups:
U = η₀U_s/(E'R') [speed parameter]
W = F/(E'R'L) [load parameter]
G = αE' [material parameter]
α = pressure-viscosity coefficient [Pa⁻¹], η₀ = viscosity at ambient [Pa·s]
Elliptic contact (ball bearings — Hamrock-Dowson):
h_min = 3.63 U^0.68 G^0.49 W^(-0.073) (1 - e^(-0.68k)) × R_x
k = ellipticity ratio = a/b (long/short axis of contact ellipse)
Typical EHD film thickness: 0.1-2 μm (gears), 0.05-1 μm (ball bearings)
Viscosity and Lubricants
Dynamic vs. Kinematic Viscosity
η [Pa·s = mPa·s = cP] = dynamic (absolute)
ν [m²/s = mm²/s = cSt] = kinematic = η/ρ
Conversion: ν [cSt] = η [cP] / ρ [g/cm³]
Viscosity-temperature (Walther equation):
log log(ν + 0.7) = A - B × log(T) [ASTM D341, T in Rankine or Kelvin]
Viscosity Index (VI): higher VI → less viscosity change with temperature
VI > 100: multigrade oil; VI < 0: highly temperature-sensitive
ISO Viscosity Grades (ISO VG — at 40°C)
VG 10, 15, 22, 32, 46, 68, 100, 150, 220, 320, 460, 680...
±10% tolerance around grade center
AGMA Gear Oil Grades
AGMA 1 ≈ ISO VG 46; AGMA 2 ≈ VG 68; AGMA 4 ≈ VG 150; AGMA 6 ≈ VG 320; AGMA 8 ≈ VG 460
R&O (rust & oxidation inhibited): plain gearboxes
EP (extreme pressure): bevel, worm, hypoid, high-load
SAE Engine Oil Grades
Monograde: SAE 30, 40, 50 (kinematic at 100°C)
Multigrade: SAE 5W-30 (5W = cold, 30 = hot) — W = winter
SAE 5W-30: η cold = 3,500 mPa·s at -25°C; ν = 9.3-12.5 cSt at 100°C
Pressure-Viscosity Effect
η = η₀ × exp(α × P)
α ≈ 10-30 GPa⁻¹ for mineral oils
At 1 GPa contact pressure: η/η₀ = e^(20×10⁻⁹ × 10⁹) = e^20 = 5×10⁸ ← huge increase!
This is why EHD works — viscosity soars under Hertzian contact pressure
Wear Models
Archard Wear Law
Q = k × P × L / H
Q = wear volume [m³]
k = dimensionless wear coefficient (10⁻⁸ to 10⁻³, material/lubricant dependent)
P = normal load [N], L = sliding distance [m], H = hardness [Pa]
Wear rate: dV/ds = k × P/H
Specific wear rate k_s = k/H [m²/N] = archard coefficient / hardness
Typical k values:
Steel on steel (dry): k = 10⁻² to 10⁻³
Steel on steel (lubricated): k = 10⁻⁵ to 10⁻⁷
PTFE on steel: k = 10⁻⁸ to 10⁻⁶
DLC on steel (dry): k = 10⁻⁹
Wear Regimes
Mild wear: oxide/protective layer intact; k ≈ 10⁻⁶
Severe wear: metallic contact, delamination; k ≈ 10⁻³
Transition: depends on PV value (pressure × velocity)
PV limit: max pressure × velocity before transition to severe wear
PTFE: PV_max ≈ 0.03 MPa·m/s (dry); nylon: 0.07; bronze: 0.5; steel (oil): 3.0
Friction Coefficient Reference Table
| Pair | Dry | Lubricated |
|---|
| Steel - Steel | 0.5-0.8 | 0.05-0.15 |
| Steel - Cast Iron | 0.3-0.5 | 0.05-0.10 |
| Steel - Bronze | 0.15-0.3 | 0.05-0.10 |
| Steel - PTFE | 0.04-0.20 | 0.04-0.10 |
| Steel - Rubber | 0.5-1.5 | 0.2-0.5 |
| Bronze - Bronze | 0.2-0.3 | 0.04-0.08 |
| DLC - Steel | 0.05-0.15 | 0.01-0.05 |
Output
Provide: lubrication regime (HD/EHD/mixed/boundary), Λ ratio, minimum film thickness h_min [μm], Sommerfeld number S, friction coefficient μ, wear rate Q [mm³/hr], lubricant viscosity grade (ISO VG), oil film temperature rise ΔT [°C].