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eduKate Learning Manual: Internal Lee Waves | How Deep Currents Crossing Seafloor Mountains Turn Mean Flow Into Ocean Mixing

Wait, What? A deep current flowing over an underwater mountain can make waves inside the ocean even when the tide is not the main driver.

These are internal lee waves. They form when a relatively steady current crosses small-scale rough topography in a stably stratified ocean. The current forces density surfaces up and down over the obstacle. Buoyancy and rotation then turn that displacement into internal-wave motion, allowing energy and momentum to leave the mean current and enter the internal-wave field.

Scientific Job Claimed by This Manual

This manual owns one Ocean World process: quasi-steady near-bottom current → flow crosses rough seafloor topography → density surfaces are displaced → internal lee waves are generated → wave drag removes momentum from the mean current → waves propagate and/or break → deep turbulent mixing can increase. The Internal Tides Learning Manual owns tidal-current conversion over topography. The Internal Waves Learning Manual owns the general wave class. The Diapycnal Mixing Learning Manual owns irreversible cross-density mixing. This article owns mean-current → lee-wave energy conversion and drag.

Primary: Why Does Water Make a Wave After Passing Over a Mountain?

Imagine a river flowing over a bump. The water surface changes shape because the flow has to climb over the obstacle.

In the deep ocean, the important “surface” is often not the air–sea surface but a density layer inside the water. As the current crosses a seamount or ridge, that density layer is pushed upward and downward. Gravity tries to restore it, and the disturbance becomes a wave.

Why Stratification Is Necessary

Internal lee waves need stable stratification. If density changes with depth, a displaced parcel feels a restoring buoyancy force.

Without that restoring force, the current can still feel bottom drag and create turbulence, but it cannot support the same propagating internal-wave response.

Secondary: Mean Current Versus Tide

The distinction from internal tides is essential.

The same ridge can generate both at different times or simultaneously, but the forcing frequency and energy source are different.

Why Small-Scale Roughness Matters

Lee-wave generation depends strongly on the size and slope of seafloor features relative to the current and stratification. Small ridges, abyssal hills and rough continental slopes can be especially effective at disturbing near-bottom density surfaces.

A broad smooth plain produces much less lee-wave conversion than rough topography under the same current.

JC: Intrinsic Frequency and Wave Propagation

For a stationary obstacle and a steady background flow, the lee-wave frequency measured in the moving fluid arises from the current advecting over topographic wavelengths. In simple form, the intrinsic frequency scales like ω ≈ U·k, where U is the background current and k is the horizontal topographic wavenumber.

Only disturbances whose intrinsic frequency lies between the Coriolis and buoyancy frequencies can propagate as freely travelling internal gravity waves. This immediately gives a powerful prediction: not every combination of current speed and topographic scale can radiate a propagating lee wave.

Wave Drag: How the Mean Current Loses Momentum

As the current does work lifting and lowering density surfaces over topography, part of its kinetic energy is converted into internal-wave energy.

The reaction force exerted by the wave field on the mean current is called wave drag. In climate and ocean models, lee-wave drag can be an important route by which large-scale currents transfer momentum toward smaller scales.

Why the Waves Can Break

As internal lee waves propagate upward or encounter changing stratification, their amplitude and shear can increase. If the wave becomes too steep or dynamically unstable, it can break.

Breaking converts organised wave motion into turbulence. That turbulence can then mix heat, salt, oxygen and nutrients across density surfaces.

2026 Evidence From the Antarctic Circumpolar Current

A 2026 Geophysical Research Letters study compared full-depth turbulent kinetic-energy dissipation across the Antarctic Circumpolar Current near 50°E with energy flux estimated for bottom-generated internal waves.

The study found that in much of the observed region, turbulent dissipation was locally consistent with energy input from internal lee waves generated by quasi-steady deep currents crossing small-scale bottom topography. Where larger-scale roughness favoured internal tides, tidal-wave generation instead dominated.

This is an unusually strong receipt because the study measured both the turbulence and the topographic/current conditions required to estimate the lee-wave source. It does not mean every deep-ocean turbulence patch is caused by lee waves.

Why the Antarctic Circumpolar Current Is a Natural Laboratory

The ACC contains strong, deep-reaching currents and crosses some of the roughest large-scale bathymetry on Earth. That combination creates many opportunities for both internal tides and lee waves.

The Antarctic Circumpolar Current Learning Manual owns the circumpolar current system. This manual owns the specific topographic wave-generation process that can extract energy from the deep flow.

Connection to the Bottom Boundary Layer

The Ocean Bottom Boundary Layer Learning Manual owns the persistent frictional and turbulent layer immediately above the seabed.

Lee-wave generation can begin in that same near-bottom region, but the wave can then carry energy away from the seabed before breaking elsewhere. Bottom-boundary turbulence and lee-wave radiation therefore overlap physically without being the same scientific job.

Connection to Internal Tides

The Internal Tides Learning Manual owns barotropic tidal flow converted into internal-wave energy.

Internal lee waves instead tap the kinetic energy of the mean or slowly varying deep current. The same seafloor topography can therefore host two different wave-generation mechanisms, and observations must separate their frequencies and forcing.

Connection to Diapycnal Mixing

The Diapycnal Mixing Learning Manual owns irreversible mixing across density surfaces.

Lee waves are one energy-delivery route that can feed that mixing. The wave is not itself the same thing as the irreversible turbulent end state.

Why Models Need Lee-Wave Parameterisations

Most global climate models cannot resolve every abyssal hill or every metre-scale wave-breaking event. They therefore represent lee-wave drag and associated mixing statistically, using resolved current speed, stratification and subgrid bathymetric roughness.

If the parameterisation is too weak or too strong, the model can place deep mixing and momentum loss in the wrong places, altering simulated overturning circulation.

How Do We Know?

Scientists use lowered acoustic Doppler current profilers, CTDs, microstructure profilers, fast-response thermistors, moorings and multibeam bathymetric mapping.

High-resolution bathymetry provides the roughness spectrum. Near-bottom current measurements provide U. Stratification provides the buoyancy frequency. Turbulence instruments provide the observed dissipation. Together, those measurements allow an energy budget to test whether lee-wave generation can account for the measured mixing.

Observation Versus Attribution

Detecting turbulence near rough topography is not enough to prove lee waves caused it. Internal tides, mean shear, hydraulic jumps and boundary-layer processes can also create turbulence.

Attribution becomes strong when current speed, topographic wavelength, wave frequency, propagation structure and measured dissipation fit the lee-wave energy pathway better than competing mechanisms.

Can You Predict It?

Transfer Test

Two deep-ocean sites have the same stratification and bottom roughness. Site A has a strong persistent current. Site B has little mean flow but large tidal oscillations. Which site is more favourable for internal lee waves, and which for internal tides?

Site A favours internal lee waves; Site B favours internal tides. The distinction comes from the source of the flow over topography.

Model Boundary

The simple picture assumes a steady current crossing idealised roughness. Real currents vary in time, topography is three-dimensional, tides coexist with mean flow, and nonlinear blocking can occur. Energy generation and local dissipation need not balance everywhere because waves can propagate away before breaking.

Useful Misconceptions to Correct

Canonical External Sources

Teaching Method

Begin with the contradiction: “How can a steady current make a wave?” Make students separate the current from the obstacle: the current carries kinetic energy; the topography forces vertical displacement; stratification supplies the restoring force.

For Primary learners, use deep current → underwater hill → density layer lifted → wave forms. For Secondary learners, distinguish steady-current lee waves from tidal internal waves. For JC learners, use ω ≈ U·k, wave drag and an energy budget, then require students to decide whether a turbulence observation is better explained by tides, lee waves or bottom-boundary shear.

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