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My question here is regarding fracture of materials. I have problems in understanding some concepts. Now, for static loading, there is a property called KIC (fracture toughness). By equating our stress from the static load to this KIC, we get the maximum length of the crack which does not propagate. Above this length for this static loading, crack start propagating.
q1) What happens if our K becomes larger than K_IC? Does it rupture or the crack starts propagating?
Now, linking this to fatigue loading. In Paris relation, da/dN = C Δ Km. This is applicable for region II in the crack growth. As seen from the attached figure, region II it has two asymptotes along its sides. Stage I is the ΔKth. Here this threshold intensity factor is the point at which if we pass this threshold, the crack starts propagating.
q2) Can we link this figure to what is happening in the static failure. In other words, can we use a critical crack length which is common between them?
It would be better if I have a discussion group chat or something since this might save a lot of time and clear any confusion.
Thanks in advance
q1) What happens if our K becomes larger than K_IC? Does it rupture or the crack starts propagating?
Now, linking this to fatigue loading. In Paris relation, da/dN = C Δ Km. This is applicable for region II in the crack growth. As seen from the attached figure, region II it has two asymptotes along its sides. Stage I is the ΔKth. Here this threshold intensity factor is the point at which if we pass this threshold, the crack starts propagating.
q2) Can we link this figure to what is happening in the static failure. In other words, can we use a critical crack length which is common between them?
It would be better if I have a discussion group chat or something since this might save a lot of time and clear any confusion.
Thanks in advance