Physics · Engineering Physics · A2 Level

Fracture

Every material eventually breaks in one of two ways: tearing apart slowly after visible warning, or snapping apart suddenly with almost none. Understanding why comes down to a single, sharp idea — stress doesn't spread evenly through a loaded component, it concentrates violently at cracks, notches, and corners, and that's exactly where failure begins and grows.

8 min read

Ductile fracture versus brittle fracture

Fracture is the final separation of a material into pieces under stress. Building directly on the ductile/brittle distinction from earlier in this topic, the way a material fractures — not just whether it does — falls into two broad patterns.

Ductile fracture occurs only after significant plastic deformation and necking, exactly as traced out on the stress-strain graph earlier in this topic. Because the material has already absorbed substantial energy deforming plastically before it finally separates, ductile fracture surfaces are typically rough and fibrous in appearance, and — connecting directly back to the idea of toughness from the "Ductile and Brittle Materials" lesson — propagating a ductile fracture requires considerably more energy than propagating a brittle one, since much of that energy has already gone into plastic deformation throughout the material, not just at the point of final separation.

Brittle fracture, by contrast, occurs with little or no prior plastic deformation. Once initiated, a brittle fracture propagates rapidly through the material — often audibly and visibly suddenly — and typically leaves a relatively flat, smooth, or crystalline-looking fracture surface. Because so little plastic deformation has occurred anywhere in the material, comparatively little energy has been absorbed by the time the material finally separates.

Stress concentration: why cracks grow from their own tip

A crucial and somewhat counter-intuitive fact underlies almost everything about how fracture actually happens: applied stress is not distributed evenly through a loaded component. At any sharp geometric feature — a crack, a notch, a hole, or a sharp internal corner — stress concentrates very sharply in the immediate vicinity of that feature, reaching values far higher than the average stress calculated simply as force divided by the component's overall cross-sectional area.

This stress concentration effect is why a crack, once initiated — for instance, by the fatigue mechanism covered in the previous lesson, or by an existing manufacturing flaw or scratch — tends to keep growing from its own tip, rather than stalling or "healing." The tip of a crack is an extremely sharp geometric feature, and the stress there is dramatically higher than the nominal stress across the rest of the component. That locally intensified stress is what does the work of extending the crack further with each load cycle or each increment of applied stress, which is exactly the crack-growth mechanism described in the fatigue lesson, now explained in terms of its underlying physical cause.

Key ideaWhy sharp features are dangerous
1
Consider a flat plate under uniform tensile stress, with a small circular hole drilled through it.
A simple, standard case for illustrating stress concentration.
2
Far from the hole, stress is uniform and equal to the nominal applied stress, $\sigma_{nominal} = F/A$.
The usual definition of stress applies wherever the material's cross-section is unbroken and uniform.
3
Immediately at the edge of the hole, the local stress can be several times higher than $\sigma_{nominal}$ — this ratio is called the stress concentration factor.
The material near the hole has to carry the same total load over a locally reduced and geometrically disrupted cross-section, concentrating force into a smaller effective area right at the edge.
4
A sharp crack behaves as an extreme, limiting case of this same effect — the sharper the feature, the higher the local stress concentration at its tip.
This is exactly why cracks propagate from their own tip: the local stress there is far higher than anywhere else in the component, even though the average stress across the whole cross-section may be modest.
Insight
A basic principle of good engineering design

Because stress concentrates so sharply at geometric discontinuities, avoiding sharp internal corners — replacing them with smooth, gradual fillets and radii wherever possible — is one of the most basic and effective principles of good engineering design. A sharp internal corner in a shaft, bracket, or panel is a ready-made site for a stress concentration to develop into a fatigue crack, and eventually a fracture, long before the component's average stress would suggest any danger at all.

Closing the topic: from stress to fracture

This lesson completes the arc of this Materials topic, which has built up, lesson by lesson, into a single connected picture of how engineering materials behave and ultimately fail:

Key takeaways — the whole topic, tied together

  • Stress and strain normalise raw force and extension by a specimen's geometry, giving quantities that describe the material itself, independent of sample size or shape.
  • The Young modulus quantifies stiffness in the elastic region — the constant ratio of stress to strain while deformation remains fully recoverable.
  • Elastic vs plastic deformation distinguishes fully recoverable deformation (below the elastic limit) from permanent deformation (above the yield stress).
  • The full stress-strain graph, and the tensile test that produces it, bring together elastic behaviour, yield, strain hardening, ultimate tensile stress, necking, and fracture into one experimentally grounded picture.
  • Ductile vs brittle behaviour describes how much plastic deformation — and therefore how much warning and toughness — a material shows before it finally fails.
  • Fatigue shows that repeated sub-critical loading can cause failure through slow crack growth, even well below a material's static strength.
  • Fracture completes the picture: ductile and brittle failure mechanics, and the stress concentration effect that explains why cracks grow from their own tip and why sharp geometric features are dangerous in engineering design.
  • Together, these nine lessons form the complete toolkit for understanding how and why engineering materials succeed or fail in service — from the first definition of stress right through to the physics of a component's final fracture.