Crack tip opening displacement (CTOD) or δ t {\displaystyle \delta _{\text{t}}} is the distance between the opposite faces of a crack tip at the 90° intercept position. The position behind the crack tip at which the distance is measured is arbitrary but commonly used is the point where two 45° lines, starting at the crack tip, intersect the crack faces. The parameter is used in fracture mechanics to characterize the loading on a crack and can be related to other crack tip loading parameters such as the stress intensity factor K {\displaystyle K} and the elastic-plastic J-integral.
For plane stress conditions, the CTOD can be written as:
δ t = ( 8 σ ys a π E ) ln [ sec ( π σ ∞ 2 σ ys ) ] {\displaystyle \delta _{\text{t}}=\left({\frac {8\sigma _{\text{ys}}a}{\pi E}}\right)\ln \left[\sec \left({\frac {\pi \sigma ^{\infty }}{2\sigma _{\text{ys}}}}\right)\right]}
where σ ys {\displaystyle \sigma _{\text{ys}}} is the yield stress, a {\displaystyle a} is the crack length, E {\displaystyle E} is the Young's modulus, and σ ∞ {\displaystyle \sigma ^{\infty }} is the remote applied stress.
Under fatigue loading, the range of movement of the crack tip during a loading cycle Δ δ t {\displaystyle \Delta \delta _{\text{t}}} can be used for determining the rate of fatigue growth using a crack growth equation. The crack extension for a cycle d a / d N {\displaystyle da/dN} , is typically of the order of Δ δ t {\displaystyle \Delta \delta _{\text{t}}} .