Fatigue Fundamentals
Stress-Life (S-N) Approach
Basquin's Equation (High-Cycle Fatigue):
\[
S_f = a N_f^b
\]
- Sf = fatigue strength (stress amplitude) at Nf cycles (psi or MPa)
- a = fatigue strength coefficient (psi or MPa)
- Nf = number of cycles to failure (cycles)
- b = fatigue strength exponent (dimensionless, typically -0.05 to -0.12)
Alternative Log-Log Form:
\[
\log S_f = \log a + b \log N_f
\]
Endurance Limit Estimation (Steel):
\[
S_e' = 0.5 S_{ut} \quad \text{(for } S_{ut} \leq 200 \text{ ksi or 1400 MPa)}
\]
\[
S_e' = 100 \text{ ksi or } 700 \text{ MPa} \quad \text{(for } S_{ut} > 200 \text{ ksi or 1400 MPa)}
\]
- Se' = uncorrected endurance limit (rotary-beam specimen) (psi or MPa)
- Sut = ultimate tensile strength (psi or MPa)
- Note: Most non-ferrous metals do not have a true endurance limit
Corrected Endurance Limit:
\[
S_e = k_a k_b k_c k_d k_e k_f S_e'
\]
- Se = corrected endurance limit (psi or MPa)
- ka = surface condition modification factor
- kb = size modification factor
- kc = load modification factor
- kd = temperature modification factor
- ke = reliability modification factor
- kf = miscellaneous effects modification factor
Modification Factors
Surface Condition Factor:
\[
k_a = a S_{ut}^b
\]
- For ground surface: a = 1.34 (1.58 SI), b = -0.085
- For machined or cold-drawn: a = 2.70 (4.51 SI), b = -0.265
- For hot-rolled: a = 14.4 (57.7 SI), b = -0.718
- For as-forged: a = 39.9 (272 SI), b = -0.995
- Sut in ksi (MPa for SI coefficients)
Size Modification Factor (Bending/Torsion):
\[
k_b = \begin{cases}
1.0 & \text{for } d \leq 0.3 \text{ in (7.6 mm)} \\
0.879 d^{-0.107} & \text{for } 0.3 < d="" \leq="" 10="" \text{="" in="" (2.79="" ≤="" d="" ≤="" 254="" mm)}="" \\="" 0.91="" d^{-0.157}="" &="" \text{for="" }="" d=""> 10 \text{ in (d > 254 mm)}
\end{cases}
\]
- d = effective diameter (in or mm)
- For non-circular sections, use equivalent diameter: \(d = 0.808(hb)^{0.5}\) where h = height, b = width
Size Modification Factor (Axial Loading):
\[
k_b = 1.0
\]
Load Modification Factor:
\[
k_c = \begin{cases}
1.0 & \text{bending} \\
0.85 & \text{axial} \\
0.59 & \text{torsion (shear)}
\end{cases}
\]
Temperature Modification Factor:
\[
k_d = \begin{cases}
1.0 & \text{for } T \leq 450°\text{F (840 K)} \\
\text{use material-specific data} & \text{for } T > 450°\text{F (840 K)}
\end{cases}
\]
Reliability Modification Factor:
- 50% reliability: ke = 1.000
- 90% reliability: ke = 0.897
- 95% reliability: ke = 0.868
- 99% reliability: ke = 0.814
- 99.9% reliability: ke = 0.753
- 99.99% reliability: ke = 0.702
Stress Concentration Effects
Fatigue Stress Concentration Factor:
\[
K_f = 1 + q(K_t - 1)
\]
- Kf = fatigue stress concentration factor (dimensionless)
- Kt = theoretical (geometric) stress concentration factor (dimensionless)
- q = notch sensitivity (0 ≤ q ≤ 1, dimensionless)
Notch Sensitivity (Neuber's Equation):
\[
q = \frac{1}{1 + \frac{a}{\sqrt{r}}}
\]
- a = Neuber constant (material dependent) (in or mm)
- r = notch radius (in or mm)
- For steels: a ≈ 0.01 to 0.10 in (0.25 to 2.5 mm), depends on Sut
Fatigue Notch Factor for Shear:
\[
K_{fs} = 1 + q_s(K_{ts} - 1)
\]
- Kfs = fatigue stress concentration factor for shear (dimensionless)
- Kts = theoretical stress concentration factor for shear (dimensionless)
- qs = notch sensitivity for shear (dimensionless)
Fluctuating Stresses
Stress Components
Mean Stress:
\[
\sigma_m = \frac{\sigma_{max} + \sigma_{min}}{2}
\]
- σm = mean stress (psi or MPa)
- σmax = maximum stress in cycle (psi or MPa)
- σmin = minimum stress in cycle (psi or MPa)
Alternating (Amplitude) Stress:
\[
\sigma_a = \frac{\sigma_{max} - \sigma_{min}}{2}
\]
- σa = alternating stress amplitude (psi or MPa)
Stress Range:
\[
\Delta \sigma = \sigma_{max} - \sigma_{min} = 2\sigma_a
\]
- Δσ = stress range (psi or MPa)
Stress Ratio:
\[
R = \frac{\sigma_{min}}{\sigma_{max}}
\]
- R = stress ratio (dimensionless)
- R = -1 for fully reversed loading
- R = 0 for zero-to-tension loading
- R = 1 for static loading
Amplitude Ratio:
\[
A = \frac{\sigma_a}{\sigma_m}
\]
- A = amplitude ratio (dimensionless)
Mean Stress Correction Theories
Soderberg Criterion (Conservative):
\[
\frac{\sigma_a}{S_e} + \frac{\sigma_m}{S_y} = \frac{1}{n}
\]
- n = factor of safety (dimensionless)
- Sy = yield strength (psi or MPa)
- Most conservative; uses yield strength
Modified Goodman Criterion:
\[
\frac{\sigma_a}{S_e} + \frac{\sigma_m}{S_{ut}} = \frac{1}{n}
\]
- Sut = ultimate tensile strength (psi or MPa)
- Most commonly used in practice
- Moderately conservative
Gerber Criterion (Parabolic):
\[
\frac{\sigma_a}{S_e} + \left(\frac{\sigma_m}{S_{ut}}\right)^2 = \frac{1}{n}
\]
- Better fits test data for ductile materials
- Less conservative than Goodman
ASME Elliptic Criterion:
\[
\left(\frac{\sigma_a}{S_e}\right)^2 + \left(\frac{\sigma_m}{S_y}\right)^2 = \frac{1}{n^2}
\]
- Moderately conservative
- Prevents yielding on first cycle
Yielding Check (First Cycle):
\[
\sigma_{max} = \sigma_a + \sigma_m \leq \frac{S_y}{n}
\]
Combined Stress Fluctuating Loading
Equivalent Alternating Stress (von Mises Combined):
\[
\sigma_{a,eq} = \sqrt{\sigma_a^2 + 3\tau_a^2}
\]
- σa,eq = equivalent alternating stress (psi or MPa)
- σa = alternating normal stress (psi or MPa)
- τa = alternating shear stress (psi or MPa)
Equivalent Mean Stress (von Mises Combined):
\[
\sigma_{m,eq} = \sqrt{\sigma_m^2 + 3\tau_m^2}
\]
- σm,eq = equivalent mean stress (psi or MPa)
- σm = mean normal stress (psi or MPa)
- τm = mean shear stress (psi or MPa)
Modified Goodman for Combined Stresses:
\[
\frac{\sigma_{a,eq}}{S_e} + \frac{\sigma_{m,eq}}{S_{ut}} = \frac{1}{n}
\]
Strain-Life (ε-N) Approach
Coffin-Manson Relationship
Total Strain Amplitude:
\[
\frac{\Delta \varepsilon}{2} = \frac{\Delta \varepsilon_e}{2} + \frac{\Delta \varepsilon_p}{2}
\]
- Δε/2 = total strain amplitude (in/in or mm/mm)
- Δεe/2 = elastic strain amplitude (in/in or mm/mm)
- Δεp/2 = plastic strain amplitude (in/in or mm/mm)
Strain-Life Equation:
\[
\frac{\Delta \varepsilon}{2} = \frac{\sigma_f'}{E}(2N_f)^b + \varepsilon_f'(2N_f)^c
\]
- σf' = fatigue strength coefficient (psi or MPa)
- E = modulus of elasticity (psi or MPa)
- Nf = cycles to failure (cycles)
- b = fatigue strength exponent (typically -0.05 to -0.12, dimensionless)
- εf' = fatigue ductility coefficient (in/in or mm/mm)
- c = fatigue ductility exponent (typically -0.5 to -0.7, dimensionless)
Elastic Strain Amplitude:
\[
\frac{\Delta \varepsilon_e}{2} = \frac{\sigma_f'}{E}(2N_f)^b
\]
Plastic Strain Amplitude:
\[
\frac{\Delta \varepsilon_p}{2} = \varepsilon_f'(2N_f)^c
\]
Transition Life (Elastic equals Plastic):
\[
2N_t = \left(\frac{\varepsilon_f' E}{\sigma_f'}\right)^{\frac{1}{b-c}}
\]
- Nt = transition life where elastic and plastic strains are equal (cycles)
Cyclic Stress-Strain Behavior
Ramberg-Osgood Cyclic Stress-Strain Curve:
\[
\frac{\Delta \varepsilon}{2} = \frac{\Delta \sigma}{2E} + \left(\frac{\Delta \sigma}{2K'}\right)^{\frac{1}{n'}}
\]
- Δσ/2 = stress amplitude (psi or MPa)
- K' = cyclic strength coefficient (psi or MPa)
- n' = cyclic strain hardening exponent (dimensionless)
Cyclic Strength Coefficient Estimation:
\[
K' \approx \frac{\sigma_f'}{\left(\varepsilon_f'\right)^{n'}}
\]
Cyclic Strain Hardening Exponent Estimation:
\[
n' \approx \frac{b}{c}
\]
Cumulative Damage
Palmgren-Miner Linear Damage Rule
Miner's Rule:
\[
D = \sum_{i=1}^k \frac{n_i}{N_i} \leq 1.0
\]
- D = total damage fraction (dimensionless)
- ni = number of cycles applied at stress level i (cycles)
- Ni = number of cycles to failure at stress level i (cycles)
- k = number of different stress levels
- Failure predicted when D ≥ 1.0
- Conservative approach often uses D ≥ 0.7 to 1.0 for failure
Remaining Life:
\[
n_{remaining} = N_i\left(1 - \sum_{j=1}^{i-1} \frac{n_j}{N_j}\right)
\]
Static Failure Theories
Ductile Materials
Maximum Shear Stress Theory (Tresca):
\[
\tau_{max} = \frac{\sigma_1 - \sigma_3}{2} \leq \frac{S_y}{n}
\]
- τmax = maximum shear stress (psi or MPa)
- σ1 = maximum principal stress (psi or MPa)
- σ3 = minimum principal stress (psi or MPa)
- Sy = yield strength (psi or MPa)
- n = factor of safety (dimensionless)
Simplified for Uniaxial Tension:
\[
\frac{S_y}{2} \leq \frac{S_y}{n}
\]
Distortion Energy Theory (von Mises):
\[
\sigma' = \sqrt{\sigma_1^2 - \sigma_1\sigma_2 + \sigma_2^2} \leq \frac{S_y}{n}
\]
- σ' = von Mises equivalent stress (psi or MPa)
- σ1, σ2 = principal stresses (psi or MPa)
- Most accurate for ductile materials
von Mises for 3D Stress State:
\[
\sigma' = \sqrt{\frac{(\sigma_1 - \sigma_2)^2 + (\sigma_2 - \sigma_3)^2 + (\sigma_3 - \sigma_1)^2}{2}} \leq \frac{S_y}{n}
\]
von Mises in Terms of Stress Components:
\[
\sigma' = \sqrt{\sigma_x^2 - \sigma_x\sigma_y + \sigma_y^2 + 3\tau_{xy}^2} \leq \frac{S_y}{n}
\]
- σx, σy = normal stresses in x and y directions (psi or MPa)
- τxy = shear stress (psi or MPa)
- For plane stress (σz = 0)
von Mises for General 3D State:
\[
\sigma' = \sqrt{\frac{1}{2}\left[(\sigma_x - \sigma_y)^2 + (\sigma_y - \sigma_z)^2 + (\sigma_z - \sigma_x)^2 + 6(\tau_{xy}^2 + \tau_{yz}^2 + \tau_{zx}^2)\right]}
\]
Brittle Materials
Maximum Normal Stress Theory (Rankine):
\[
\sigma_1 \leq \frac{S_{ut}}{n} \quad \text{(tension)}
\]
\[
|\sigma_3| \leq \frac{S_{uc}}{n} \quad \text{(compression)}
\]
- Sut = ultimate tensile strength (psi or MPa)
- Suc = ultimate compressive strength (psi or MPa)
- Used for brittle materials
Coulomb-Mohr Theory:
\[
\frac{\sigma_1}{S_{ut}} - \frac{\sigma_3}{S_{uc}} \leq \frac{1}{n}
\]
- Accounts for different tensile and compressive strengths
- For σ1 ≥ 0 ≥ σ3
Modified Mohr Theory:
- If σ1 ≥ σ2 ≥ 0: \(\sigma_1 \leq \frac{S_{ut}}{n}\)
- If σ1 ≥ 0 ≥ σ2: \(\frac{\sigma_1}{S_{ut}} - \frac{\sigma_2}{S_{uc}} \leq \frac{1}{n}\)
- If 0 ≥ σ1 ≥ σ2: \(|\sigma_2| \leq \frac{S_{uc}}{n}\)
Fracture Mechanics
Stress Intensity Factor
Mode I Stress Intensity Factor:
\[
K_I = \beta \sigma \sqrt{\pi a}
\]
- KI = stress intensity factor for Mode I (opening) (psi√in or MPa√m)
- β = geometry correction factor (dimensionless)
- σ = applied stress (psi or MPa)
- a = crack length (in or m)
For Center Crack in Infinite Plate:
\[
K_I = \sigma \sqrt{\pi a}
\]
- β = 1.0 for center crack
- a = half crack length
For Edge Crack:
\[
K_I = 1.12 \sigma \sqrt{\pi a}
\]
- β = 1.12 for edge crack
- a = full crack length
Fracture Toughness Criterion:
\[
K_I \leq K_{Ic}
\]
- KIc = plane strain fracture toughness (psi√in or MPa√m)
- Critical material property
Critical Crack Length:
\[
a_c = \frac{1}{\pi}\left(\frac{K_{Ic}}{\beta \sigma}\right)^2
\]
- ac = critical crack length for fracture (in or m)
Paris Law (Fatigue Crack Growth)
Paris Equation:
\[
\frac{da}{dN} = C(\Delta K)^m
\]
- da/dN = crack growth rate per cycle (in/cycle or m/cycle)
- C = material constant (depends on units)
- ΔK = stress intensity factor range (psi√in or MPa√m)
- m = material constant (typically 2 to 4, dimensionless)
Stress Intensity Factor Range:
\[
\Delta K = K_{max} - K_{min} = \beta \Delta \sigma \sqrt{\pi a}
\]
- Δσ = stress range (psi or MPa)
Cycles to Failure (Integration of Paris Law):
\[
N_f = \int_{a_i}^{a_f} \frac{da}{C(\Delta K)^m}
\]
- ai = initial crack length (in or m)
- af = final (critical) crack length (in or m)
For Constant β and Δσ:
\[
N_f = \frac{1}{C(\beta \Delta \sigma \sqrt{\pi})^m} \int_{a_i}^{a_f} a^{-m/2} da
\]
Simplified Result (m ≠ 2):
\[
N_f = \frac{2}{C(\beta \Delta \sigma \sqrt{\pi})^m (2-m)} \left[a_i^{1-m/2} - a_f^{1-m/2}\right]
\]
Impact and Dynamic Loading
Impact Factor
Suddenly Applied Load:
\[
\sigma_{dynamic} = 2\sigma_{static}
\]
- Impact factor = 2 for suddenly applied load
Axial Impact:
\[
\sigma_{max} = \frac{P}{A}\left(1 + \sqrt{1 + \frac{2hAE}{PL}}\right)
\]
- σmax = maximum stress (psi or MPa)
- P = weight of falling object (lb or N)
- A = cross-sectional area (in² or m²)
- h = drop height (in or m)
- E = modulus of elasticity (psi or MPa)
- L = length of member (in or m)
Bending Impact:
\[
\sigma_{max} = \frac{Mc}{I}\left(1 + \sqrt{1 + \frac{2hEI}{McL}}\right)
\]
- M = static moment from weight (lb·in or N·m)
- c = distance from neutral axis to extreme fiber (in or m)
- I = moment of inertia (in⁴ or m⁴)
Safety Factors and Design Criteria
Factor of Safety Definitions
Factor of Safety Based on Yield:
\[
n = \frac{S_y}{\sigma_{applied}}
\]
Factor of Safety Based on Ultimate Strength:
\[
n = \frac{S_{ut}}{\sigma_{applied}}
\]
Factor of Safety for Fatigue:
\[
n = \frac{S_e}{\sigma_a} \quad \text{(fully reversed)}
\]
Factor of Safety with Mean Stress (Goodman):
\[
\frac{1}{n} = \frac{\sigma_a}{S_e} + \frac{\sigma_m}{S_{ut}}
\]
Design Stress Limits
Allowable Stress:
\[
\sigma_{allow} = \frac{S}{n}
\]
- σallow = allowable stress (psi or MPa)
- S = strength parameter (Sy or Sut) (psi or MPa)
Required Area:
\[
A_{req} = \frac{P}{\sigma_{allow}}
\]
Multiaxial Fatigue
Critical Plane Approaches
Findley Criterion:
\[
\frac{\tau_a + k\sigma_{n,max}}{f} \leq 1
\]
- τa = shear stress amplitude on critical plane (psi or MPa)
- σn,max = maximum normal stress on critical plane (psi or MPa)
- k = material constant (dimensionless)
- f = fatigue limit in pure torsion (psi or MPa)
Smith-Watson-Topper (SWT) Parameter:
\[
SWT = \sigma_{max} \varepsilon_a E
\]
- σmax = maximum normal stress (psi or MPa)
- εa = strain amplitude (in/in or mm/mm)
- Used for mean stress effects in crack initiation
Fatigue under Torsion
Endurance Limit in Torsion:
\[
S_{se} = 0.577 S_e
\]
- Sse = endurance limit in pure shear (psi or MPa)
- Based on von Mises criterion
Alternative Estimation:
\[
S_{se} = 0.67 S_{ut}
\]
Creep and High-Temperature Failure
Larson-Miller Parameter
Larson-Miller Parameter:
\[
LMP = T(C + \log t_r)
\]
- LMP = Larson-Miller parameter
- T = absolute temperature (°R or K)
- C = material constant (typically 20 for metals)
- tr = rupture time (hours)
Time to Rupture:
\[
t_r = 10^{(LMP/T - C)}
\]
Variable Amplitude Loading
Rainflow Counting Method
- Used to convert complex loading histories into equivalent constant amplitude cycles
- Extracts closed stress-strain hysteresis loops
- Each cycle characterized by mean stress and alternating stress
- Results used with Miner's rule for damage calculation
Equivalent Stress Methods
Root-Mean-Square (RMS) Stress:
\[
\sigma_{rms} = \sqrt{\frac{1}{n}\sum_{i=1}^n \sigma_i^2}
\]
- σrms = root-mean-square stress (psi or MPa)
- n = number of stress values
Equivalent Constant Amplitude:
\[
\sigma_{eq} = \left(\sum_{i=1}^k n_i \sigma_i^m\right)^{1/m}
\]
- σeq = equivalent stress amplitude (psi or MPa)
- m = inverse slope of S-N curve (typically 3 to 5)