| name | stress-intensity-factor |
| description | Stress intensity factor (SIF) — Mode I/II/III K_I/K_II/K_III, Irwin K-G relationship, SIF for common geometries (edge crack, central crack, surface crack, corner crack), stress intensity correction factors (F-functions, finite width correction), superposition principle, mixed-mode SIF (Erdogan-Sih criterion), K_Ic fracture toughness, CTOD, J-integral, linear elastic fracture mechanics (LEFM) validity, weight function method, and ASTM E399/E1820. |
| metadata | {"priority":7,"promptSignals":{"phrases":["stress intensity factor","fracture mechanics","K_I stress intensity","LEFM","fracture toughness","K_Ic"],"minScore":3}} |
Stress Intensity Factor (SIF) — Complete Skill
Linear Elastic Fracture Mechanics (LEFM) Foundation
Stress Field Near Crack Tip
Mode I (opening, tension perpendicular to crack):
σ_ij = (K_I / √(2πr)) × f_ij(θ) + O(r^0) [K_I = stress intensity; r = distance from crack tip; θ = angle from crack plane]
Mode II (in-plane shear):
σ_ij = (K_II / √(2πr)) × g_ij(θ)
Mode III (anti-plane shear/tearing):
τ_ij = (K_III / √(2πr)) × h_ij(θ)
Superposition: for mixed loading, K_I, K_II, K_III each calculated independently and summed for each mode
Physical significance:
K_I quantifies the stress field intensity at the crack tip
Units: MPa√m or ksi√in (1 ksi√in = 1.099 MPa√m)
Fracture occurs when K_I ≥ K_Ic (mode I fracture toughness)
SIF for Common Geometries
Central Through-Crack in Infinite Plate (Griffith)
K_I = σ × √(π × a) [σ = remote applied stress; a = half-crack length]
Basis: Inglis stress concentration + Griffith energy balance
Finite Width Correction
K_I = σ × √(π × a) × F(a/W)
F(a/W) = Feddersen correction:
F(a/W) = √(sec(π × a/W)) = √(sec(π × a/2W)) [depending on convention; a = half crack; W = half width]
Or: F(a/W) = (1 - 0.025(a/W)² + 0.06(a/W)⁴) × √(sec(π × a/(2W))) [more accurate; Feddersen 1966]
Example:
σ = 100 MPa; a = 20 mm = 0.02 m; W = 100 mm (half-width 50 mm → a/W = 0.40)
K_I = 100 × √(π × 0.02) × √(sec(π × 0.02/(2×0.05))) = 100 × 0.2507 × √(sec(0.628)) = 100 × 0.2507 × √(1.236) = 100 × 0.2507 × 1.112 = 27.9 MPa√m
Edge Crack in Semi-Infinite Plate
K_I = 1.12 × σ × √(π × a) [a = crack depth from free surface; 1.12 = free surface correction factor]
More precisely: K_I = F(a/W) × σ × √(π × a)
F(a/W) = 1.12 - 0.231(a/W) + 10.55(a/W)² - 21.72(a/W)³ + 30.39(a/W)⁴ [Tadashi and Mura series]
Surface (Semi-Elliptical) Crack — Raju-Newman
Most common practical crack — on a surface, partially through:
a = crack depth; 2c = crack surface length; t = plate thickness
SIF at deepest point:
K_I = (σ × √(π × a) / Q^0.5) × F_surface [Q = shape factor; F_surface = boundary correction]
Q shape factor:
Q = Φ² - 0.212 × (σ/σ_y)² [Φ = complete elliptic integral; usually Φ² ≈ 1 + 4.593 × (a/c)^1.65]
For a/c = 0.5 (half-circle): Φ² = 2.464; Q = 2.464 - 0.212 × (σ/σ_y)² ≈ 2.464 (for σ/σ_y = 0)
Raju-Newman correction (1984):
F(a/c, a/t, θ, φ) — function of crack shape ratio a/c, depth ratio a/t, location angle φ, and stress
Tables and polynomial expressions in NASA CR-165807 and NASGRO documentation
At surface endpoint (φ = 0):
K_I(surface) = 1.12 × σ × √(π × a / Q) [surface factor 1.12; slightly different from deepest point]
Through-Thickness Crack — Compact Tension (CT)
CT specimen (ASTM E399):
K_I = P/(B×√W) × f(a/W) [P = applied force; B = specimen thickness; W = specimen width]
f(a/W) = (2 + a/W) × (0.886 + 4.64(a/W) - 13.32(a/W)² + 14.72(a/W)³ - 5.60(a/W)⁴) / (1-a/W)^(3/2)
Valid: 0.2 ≤ a/W ≤ 1.0
SENB (Single Edge Notched Bend):
K_I = P × S / (B × W^(3/2)) × f(a/W) [S = span; f(a/W) = ASTM polynomial]
f(a/W) = 3(a/W)^0.5 × [1.99 - (a/W)(1-a/W)(2.15 - 3.93(a/W) + 2.7(a/W)²)] / (2(1+2a/W)(1-a/W)^(3/2))
Pressurized Crack / Thermal Gradient
Internal pressure p in crack faces:
K_I = p × √(π × a) [same form as remote tension; crack opens under pressure]
Additive with remote K_I from far-field stress
Thermal gradient K_I (weight function):
K_I = ∫₀ᵃ σ_T(x) × m(x,a) dx [m(x,a) = weight function for geometry; σ_T(x) = thermal stress distribution]
Superposition Principle
For multiple load cases:
K_I_total = K_I_tension + K_I_bending + K_I_pressure + ... [linear superposition within LEFM]
Example — pressure vessel with surface crack:
Hoop stress σ_θ = p × r/t → K_I_hoop = σ_θ × √(πa) × F_surface
Internal pressure in crack: K_I_pressure = p × √(πa) × F_pressure
K_I_total = K_I_hoop + K_I_pressure
Bending + tension:
K_I = (σ_membrane × F_m + σ_bending × F_b) × √(π × a)
F_m, F_b = different correction factors for membrane vs. bending stress
K-G (SIF — Strain Energy Release Rate) Relationship
Mode I (plane stress):
G_I = K_I² / E [J/m²; G_I = energy release rate per unit crack area advance]
Mode I (plane strain):
G_I = K_I² × (1-ν²) / E
Mixed mode:
G_total = G_I + G_II + G_III [energy release rates from each mode add]
G_total = (K_I² + K_II²) × (1-ν²)/E + K_III² × (1+ν)/E [plane strain]
Fracture criterion:
K_I = K_Ic (Mode I dominant); G = G_c (critical energy release rate) = K_Ic²(1-ν²)/E
Fracture Toughness (K_Ic) — ASTM E399
Test Method
Specimen geometries: CT (compact tension) or SENB; notched and fatigue pre-cracked
Size requirements for valid K_Ic (plane strain):
B ≥ 2.5 × (K_Q/σ_y)² [B = specimen thickness]
a ≥ 2.5 × (K_Q/σ_y)² [crack length]
W - a ≥ 2.5 × (K_Q/σ_y)² [remaining ligament]
If all satisfied: K_Q = K_Ic (valid plane strain fracture toughness)
Typical K_Ic values:
| Material | K_Ic [MPa√m] | Notes |
|---|
| 4340 Steel (σ_y = 1,400 MPa) | 50–70 | High strength; low toughness |
| 4340 Steel (σ_y = 1,100 MPa) | 100–130 | Tempered; better toughness |
| A36 Steel | 150–200 | Structural; high toughness |
| 7075-T6 Al | 24–30 | High strength; low toughness |
| 2024-T3 Al | 44 | Better toughness; aircraft |
| Titanium 6-4 | 55–80 | Good balance |
| INCONEL 718 | 100–110 | Aerospace |
| PMMA (acrylic) | 1–2 | Brittle polymer |
| SiC ceramic | 2–5 | Very brittle |
CTOD and J-Integral (Elastic-Plastic)
When LEFM invalid (plastic zone too large): use CTOD or J-integral (ASTM E1820)
LEFM valid if: plastic zone r_p << crack size
r_p = (1/6π) × (K_I/σ_y)² [Irwin plastic zone radius; plane strain]
Validity: a >> r_p → a > 25 × (K_Ic/σ_y)² [usually satisfied for high-strength materials]
J-integral:
J = -∂U_total/∂A [U_total = total potential energy; A = crack area]
J = K_Ic²/E (plane stress) or K_Ic²(1-ν²)/E (plane strain) — equivalence at limit
CTOD (Crack Tip Opening Displacement):
δ = K_I²/(E × σ_y) × (plane stress) or δ = K_I²/(E × σ_y × (1+ν)) (plane strain)
Or from J: δ = J / (m × σ_y) [m = dimensionless factor ≈ 1.0 (plane stress) to 2.0 (plane strain)]
Mixed-Mode Fracture
Erdogan-Sih (Maximum Tangential Stress) Criterion
Crack propagates in direction of maximum σ_θ:
σ_θ_max at angle θ_c:
θ_c = arctan((K_I - √(K_I² + 8K_II²)) / (4K_II)) [from Erdogan-Sih 1963]
Mixed-mode fracture condition:
K_Ic = cos(θ_c/2) × [K_I × cos²(θ_c/2) - (3/2) × K_II × sin(θ_c)] [interaction locus]
Interaction surface (normalized):
(K_I/K_Ic)² + (K_II/K_IIc)² = 1 [conservative elliptic criterion for mixed mode; K_IIc ≈ 0.6 K_Ic]
Standards and References
| Standard | Scope |
|---|
| ASTM E399 | Test method for linear-elastic plane-strain fracture toughness K_Ic |
| ASTM E1820 | J-integral and CTOD fracture toughness measurement |
| ASTM E647 | Fatigue crack growth rate |
| NASA/NASGRO | Stress intensity factor handbook and crack growth software |
| Stress Intensity Factors Handbook (Murakami) | Comprehensive SIF table for 2D/3D geometries |
| Anderson "Fracture Mechanics" (4th ed.) | Primary textbook |
Output
Provide: geometry description (specimen/component type; crack type: edge/surface/central/corner; dimensions: W [mm], B [mm], a [mm], c [mm] if surface; loading: P [kN] or σ [MPa]), applied SIF formula (source: handbook/ASTM/Raju-Newman; F(a/W) correction factor; finite width/surface correction), K_I calculation (K_I = σ × √(πa) × F [MPa√m]; step-by-step; K_II, K_III if mixed mode), comparison with K_Ic (material K_Ic [MPa√m]; safety factor on K: K_Ic/K_I; margin [%]; fracture risk: low/marginal/critical), LEFM validity (r_p [mm] = (K_I/σ_y)²/(6π); compare with a and B; plane strain condition: B > 2.5(K_Ic/σ_y)² satisfied?), J-integral or CTOD (if plastic zone large: J_applied [kJ/m²]; J_Ic [kJ/m²]; comparison), mixed mode (if K_II present: θ_c [°]; effective K; Erdogan-Sih interaction check), fatigue crack growth (if cyclic: ΔK = K_max - K_min; Paris law da/dN = C × ΔK^m; critical crack size from K_max = K_Ic), and applicable standard (ASTM E399/E1820; Murakami handbook equation reference).