Surfsolver

What actually makes a wave break

Why does a wave break where it does?

6 min read · every figure below is solved, not drawn

A swell can cross six thousand miles of open Pacific without breaking once. It arrives at your beach and falls over inside a couple of hundred metres. Nothing about the wave changed on that last stretch — what changed was the water underneath it.

This is the piece of physics everything else on this site is built on. Once you can see why depth is the trigger, the rest of a forecast stops being a list of numbers and starts being a description of a place.

A wave is energy moving, not water moving

Out in deep water, the water in a wave is not travelling with it. Each parcel of water moves in a circle and returns roughly to where it started, and it is the disturbance — the energy — that moves along. That is why a gull sitting on the surface bobs up and down as a swell passes instead of being carried off toward the beach.

Those circles get smaller with depth. The motion reaches down to about half the wave's own wavelength, and below that the water barely notices there is a wave overhead at all. A fifteen-second swell has a wavelength around 350 metres, so it is still stirring the water 175 metres down. A six-second windswell reaches barely 28 metres.

This is the whole reason depth matters. As long as the seafloor is deeper than that reach, the wave passes over it unaffected. The moment it isn't, the seafloor starts taking energy out of the bottom of the wave, and the wave starts to change shape.

Why shallow water trips it

When the bottom of a wave starts dragging on the seafloor, the wave slows down. The top does not — it is still in open water — so the crest begins to lean forward over its own base. At the same time the wave gets shorter and, to conserve its energy, taller. It stands up.

It falls over when the crest is moving faster than the wave form itself. In practice that happens at a fairly reliable ratio of wave height to water depth: a wave breaks in water roughly three-quarters of its own height. A four-foot wave breaks in about three feet of water. That single rule of thumb explains more about surf than any other sentence in this article.

It also explains why a spot has a personality. The depth contours off your beach are fixed. Feed them a bigger wave and it breaks further out; feed them a longer-period wave and it starts feeling the bottom sooner and spends longer organising itself on the way in. Same ground, different wave, different result — every time, and predictably.

The second and a half after it throws

Most descriptions of breaking stop at 'and then it breaks'. What happens next has been measured in detail, and it is quicker and stranger than people expect.

The lip detaches and becomes a projectile. It falls at about three-quarters of gravity — air drag and surface tension slow it — and lands on the face at roughly one and a half times the speed the crest itself was travelling. Then the wave does the thing that no one draws: instead of fading, the crest jumps. It hops from the original crest to the first splash-up, then to the second, stepping down in height at each jump.

A 6 ft wave at 14 seconds, from the moment the lip lets go

Lip airborne 0.68s — 5% of the period

fullhalf10.00s20.68s31.42s42.29s53.63s68.39s
1
Lip detaches0.00s
The crest throws forward. It has already stopped being a wave and started being a projectile.
2
Lip lands0.68s
Falls at 0.76 g — air drag and surface tension, not free fall — and hits the face at 1.45-1.53x the crest's own speed, angled 22-28° below horizontal.
3
First splash-up1.42s
The jet rebounds off the face it struck. The crest does not decay smoothly — it jumps to the splash and steps DOWN.
4
Second splash-up2.29s
Each rebound is lower than the last. This staircase is the most characteristic thing a breaking wave does, and most renderers smooth it away.
5
Crest height halved3.63s
Roughly 0.8 of a period after impact. Crest-to-trough height is already down to about half of what it was at the moment of breaking.
6
A bore8.39s
5-8 breaker depths from where it broke, it is whitewater: a travelling step, no longer a wave. Height decay from here is the same whether it spilled or plunged.
A six-foot wave at fourteen seconds, in real seconds. The staircase is the measured part: crest-to-trough height falls to 85.5% before the lip even lands, and is halved about 0.8 of a period after impact. The riser positions between those anchors are schematic — nobody has measured them — and the figure draws them dashed for that reason.

Two things in that figure are worth carrying around. The first is how brief the overturn is — a few percent of the period, and it scales with the square root of the wave height rather than with the period at all. A four-metre, sixteen-second wave has its lip in the air for about one second out of sixteen. The second is that getting from there to whitewater takes most of a period: five to eight breaker depths from where it broke, the wave is a bore, a travelling step of foam, and from that point on it decays the same way whether it spilled or pitched.

Spilling, plunging, surging

Waves break in three recognisable ways, and which one you get is not a matter of size. A spilling wave crumbles down its own face and gives you a soft, forgiving shoulder. A plunging wave throws its lip clear of the face and encloses air — the barrel. A surging wave never really breaks at all; it rushes up a steep beach and drains back.

Remarkably, one number predicts which you get. It compares how steep the seafloor is against how steep the wave is, and it is built from three things you already know: the slope of the bottom, the height of the wave, and its period.

spillingplungingsurging0.10.20.41240.290.862.57
Open sand
1:50 bottom · 5 ft · 14 s
ξ = 0.29 — spilling
A gently sloping beach spreads the break out. It crumbles.
Reef point
1:17 bottom · 5 ft · 14 s
ξ = 0.86 — plunging
Three times the slope, same wave. Now it throws a lip.
Steep shore
1:6 bottom · 5 ft · 14 s
ξ = 2.57 — surging
A near-vertical beach face. It surges up the sand instead of breaking.
The Iribarren number, computed from each bottom. Identical wave in all three cases — five feet at fourteen seconds — and only the slope changes. Note that the bar is pale at BOTH ends: lip throw is near zero for spilling waves, peaks in mid-plunging, and disappears again for surging waves that collapse forward before a jet can form.

The non-monotonic part catches people out. It is tempting to read the scale as 'bigger number, hollower wave', and that is wrong past about two: a very steep bottom does not give you a heavier barrel, it gives you a wave that never forms one. The hollowest surf in the world sits in the middle of that range, not at the end of it.

One more caution, because it is the most common overreach with this number: it tells you the type of break, not the shape of the barrel. When researchers went looking for a relationship between the surf-similarity number and barrel proportions at Duck, North Carolina, they found none. Barrel shape tracks the seabed gradient directly.

Reading a break with this

  1. 1Find the depth, not the height — A forecast height tells you how big the wave is offshore. Where it breaks is set by where the water gets to about three-quarters of that height.
  2. 2Look at the slope under the break — Steeper bottom, hollower wave — up to a point. This is why a reef and a beach a mile apart produce completely different waves on identical swell.
  3. 3Remember the tide moves both — Adding water moves the break shoreward onto a different piece of seafloor, which usually has a different slope. Tide changes the type of wave, not only its size.

See it at a real break

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The physics behind these figures, its sources and its limits are written up in the methodology.