FEXLA

Stress concentration and the weld toe

How a hole, a notch or a weld toe lifts the stress over a small zone, and why that zone matters for fatigue.

Principle 13 of 20 · 6 min read ·

Surface stress along a plate from a weld toeA section through a plate with an attachment welded on by a fillet weld; a dot marks the weld toe. Above the plate a curve shows the surface stress moving away from the toe: a sharp notch peak at the toe, falling quickly to a gently sloping structural stress. Two readings at 0.4 t and 1.0 t from the toe are joined by a dashed line carried back to the toe, giving the hot-spot value, well below the notch peak. The curve is schematic.Notch peak at the toeHot-spot valuestructural stress0.4t1.0tAttachmentPlate, thickness tSurface stress against distance from the toe (schematic)
Figure 1. Surface stress along a plate from a weld toe.
Contents

A stress concentration is a local rise in stress where the shape of a part changes abruptly, at a hole, a notch or the toe of a weld. It is measured by the stress concentration factor Kt, the peak stress divided by the nominal stress the part would carry without the feature. At a weld toe the rise is sharp and confined to a thin layer, which barely matters for a single load but decides where a crack starts under cycling load.

This article starts with the classic hole in a plate, explains why a ductile part shrugs off a concentration under one load, and then looks at the weld toe: what raises the stress there, how it is read from a model, and why fatigue cracks start there.

Photo: stainless tube TIG fillet-welded onto a larger tube, close-up
Figure 2. Photo: a fillet weld of a small tube onto a larger one. The toe, where the weld meets the parent metal, is where cracks start. (Free-licence photo, see the image credits.)

What a stress concentration factor is

Picture the stress in a plate under tension as lines of force running along it. Where nothing interrupts them they are evenly spaced. A hole or notch forces them to crowd round it, and where they crowd the stress rises. The ratio of the highest stress to the nominal one is the stress concentration factor:

Kt = σ_peak / σ_nominalnominal: the stress the part would carry with the feature taken away

Kt depends on the shape of the feature, not its size. A small hole and a large hole of the same shape give the same factor. Size decides how far the raised stress reaches: about one or two hole radii, beyond which the plate is back to its nominal stress.

The hole in a plate

The classic case is a small round hole of radius a in a wide plate under a remote tension σ. Along the line through the hole's centre, square to the load, elasticity gives the stress along the load direction at a distance r from the centre:

σ(r) = σ·(1 + a²/(2r²) + 3a⁴/(2r⁴))r ≥ a; at the edge r = a this gives 3σ
Stress beside a round hole in a plate under tensionA plot of the stress along the load direction, as a multiple of the remote stress, against distance from the hole's centre in hole radii, from 1 to 5. From the classical solution σ(1 + a²/2r² + 3a⁴/2r⁴) it starts at 3 at the hole's edge, falls to about 1.22 at two radii and 1.07 at three, and approaches 1. A small inset shows the plate, the hole, the horizontal pull and the dashed line through the hole where the stress is read.123123453 × remote at the edgeremote stressStress ÷ remote stressDistance from the hole's centre, r / a
Figure 3. Stress beside a round hole in a plate under tension, from the formula above: three times the remote stress at the edge, nearly back to it within three radii.

Sharper features give higher factors. For an elliptical hole with half-width a across the load and half-height b along it, the edge factor is 1 + 2a/b. A long, thin slot across the load, the shape of a crack, gives a very large value.

Why it rarely matters for a single load

In a ductile metal the peak at a concentration reaches yield long before the part as a whole does. The small zone that yields stops taking extra stress, and further load moves to the elastic metal round it. The part still fails only when the whole section yields, so for one application of load the concentration hardly lowers the strength.

Yielding spreading from a hole in a plate under tensionA plate with a central hole, pulled from left and right. Yielding starts in small zones at the top and bottom of the hole, spreads into larger zones as the load rises, and near collapse forms bands that cross the plate from the hole to its edges.first yieldspreadingnear collapse
Figure 4. Yielding starts at the edge of the hole and spreads; the plate carries load until yielding reaches across it.

That is why design-by-analysis rules treat the concentrated part of a stress as peak stress. It does not enter the strength checks. It is kept for the fatigue check, where it does matter. Brittle materials, and steels at temperatures where they lose toughness, are the exception: there a concentration can start a fracture under one load.

The weld toe

The toe is where the surface of a weld meets the plate. Several things come together there. The surface turns through an angle, often 30° to 60°, with a very small radius. There may be undercut, a small groove left by the welding arc. Welding leaves residual tension near yield in the metal close by. And the toe holds small flaws from the welding process that act as tiny cracks from the start.

Through the wall, the stress at a toe has three layers. The structure's membrane and bending stress is the straight-line part. On top of it the toe's notch adds a sharp rise confined to a thin layer at the surface. That rise is the peak part, and it is what makes the toe the worst spot for fatigue.

Primary and secondary stress: Peak: very local, matters for fatigueA plate with an attachment and fillet welds. Lines of stress crowd together where the welds meet the plate, marked as the weld toes.σ = PD / 2tPressureHoop stress in the wall holds itStrainStressYieldLoad held: strain runs onHot part: free, it would reach hereCool partJoined: the hot part is squeezed,the cool part is stretchedStrainStressYieldStrain set by the fitStress stops at yieldLoadPeak stress at the weld toes
Figure 5. Peak stress: very local, harmless for one load, and the stress that matters for fatigue.

Reading the stress at a toe

A model with a sharp corner at the toe has no finite peak there: the finer the mesh, the higher the reading. So rules that judge welds rarely use the raw peak. They use a structural stress, also called a hot-spot stress, which leaves the notch out. It is either the membrane plus bending stress through the wall at the toe, found by linearisation, or a value extrapolated to the toe from surface points a short way from it. One common surface rule reads the stress at 0.4·t and 1.0·t from the toe:

σ_hs = 1.67·σ(0.4t) − 0.67·σ(1.0t)t the plate thickness; a straight line through the two readings, taken to the toe

Why cracks start at the toe

Under cycling load the toe sees the largest stress range in the joint, in metal already in residual tension, with flaws that are already sharp. A smooth part spends most of its fatigue life starting a crack. A welded toe skips most of that stage, and the crack grows from the toe into the plate from early on. This is why welded joints have their own, lower fatigue curves.

  • Keep welds away from the highest stress where the layout allows, for example off the crotch of a nozzle.
  • Use full-penetration welds where a fillet weld root would be loaded across.
  • Ask for a smooth weld profile; grinding or dressing the toe lowers the notch effect.
  • Check the toe on both faces: the worst one is not always the outside.

Key points

  • Kt is the peak stress over the nominal stress; it depends on the shape of the feature, not its size.
  • A round hole in a wide plate gives Kt = 3, and the rise fades within about three radii.
  • For a single load a ductile part yields locally and the concentration barely lowers its strength.
  • At a weld toe the notch, residual stress and small flaws combine, which is where fatigue cracks start.
  • Weld checks use a structural or hot-spot stress and a weld design curve, not the mesh-dependent peak.

Where this matters in practice

  • Fillet welds of clips, lugs and support brackets to the shell, under cycling loads.
  • Nozzle-to-shell welds, where the toe on the shell side often carries the largest range.
  • Pad edges, where the pad's fillet weld meets the shell at a change of stiffness.
  • Holes and openings in plates and skirts, where the edge stress is a multiple of the nominal stress.

FEXLA checks the local stress where a clip, bracket or support is welded to the shell, and shows each step of the working.

See the clip check

Next principle: Discontinuity stresses at a shell-to-head junction

Educational article. It explains principles and is not design guidance; follow your governing code and edition.