Windenergie 3 - Fatigue

13 May 2026, Po Wen Cheng

Questions at the beginning

Basics of Fatigue

Converting real analogue signal into usable stress cycles for linear damage accumulation

If you are below a certain stress intensity, there is no crack growth. Above, the crack will grow linearly
(See Paris-Erdogan Crack Growth Law on Slide 9)

$$ \int_{a_i}^{a_f}\frac{da}{\left( F(a) \cdot \sqrt{a} \right)^m} = C \cdot \Delta \sigma ^m \cdot \pi^{\frac{m}{2}} \cdot N $$

$N$ is the number of cycles for the crack to grow from an initial size $a_i$ to a final size $a_f$

Stress Ratio R

Experimental S-N Curve

Linear Damage Accumulation Hypothesis

$$ D = \sum _i \frac{n_i(\Delta \sigma _i)}{N_i(\Delta \sigma _i)} $$