Density, not wind, drives the deep ocean
Thermohaline circulation gets its name from the two properties that set seawater density: temperature (thermo) and salinity (haline). Cold, salty water is denser and sinks; warm, fresh water is buoyant and stays near the surface. The density difference between surface tropical water (~1023 kg/m³) and high-latitude deep water (~1028 kg/m³) is only about 0.5%, yet that tiny contrast is enough to drive a circulation spanning the entire planet. Oceanographers track individual water masses — North Atlantic Deep Water, Antarctic Bottom Water, Mediterranean Outflow Water — by their distinct signature on a temperature-salinity (T-S) diagram, since each forms at a different location with its own characteristic combination of the two.
Where deep water is actually made
New deep water forms at only a handful of places on Earth, where surface water becomes dense enough to convect straight down through the water column. In the Labrador, Irminger and Nordic Seas, winter cooling lowers temperature while brine rejection — the salt expelled into surrounding water as sea ice freezes — raises salinity; together they produce plumes that sink to 2,000-4,000 m and flow south as North Atlantic Deep Water (NADW), the main engine of the Atlantic Meridional Overturning Circulation (AMOC). An even denser water mass, Antarctic Bottom Water, forms on the Weddell and Ross Sea shelves, cold enough (around −1.9°C) and salty enough (~34.7 psu) to sink all the way to the ocean floor and spread beneath NADW in every ocean basin — a journey that takes roughly 400-600 years just to fill the Pacific.
The AMOC: heat transport equivalent to 5 million power plants
The AMOC, the Atlantic branch of the global conveyor, carries roughly 17-19 Sverdrups northward at the surface (1 Sv = 10⁶ m³/s, equivalent to about 100 Amazon rivers) and returns the same volume at depth. That flow carries approximately 1.3 petawatts of heat across 26°N — about 25% of total poleward energy transport at that latitude — which is why London and Calgary, both at 51°N, have January means of roughly +5°C and −8°C respectively. Since 2004, the RAPID-MOCHA mooring array at 26.5°N has measured a mean AMOC strength near 17 Sv with ±3 Sv interannual variability, a notable 30% slowdown in 2009-2010 that preceded a cold European winter, and a long-term weakening trend estimated at about 15% below pre-industrial strength.
ρ(T,S) ≈ ρ₀[1 − α(T−T₀) + β(S−S₀)] α ≈ 2×10⁻⁴ K⁻¹ β ≈ 7.4×10⁻⁴ psu⁻¹ Heat transport: Q = ρ·cp·V̇·ΔT ≈ 1025 kg/m³ × 3850 J/(kg·K) × 17×10⁶ m³/s × 15 K ≈ 1.0 PW
The Stommel bifurcation: two stable states
Accelerating Greenland ice-sheet melt — currently around 280 Gt/yr — and increased Arctic river runoff both add freshwater to the North Atlantic, capping the surface and suppressing the deep convection that drives NADW formation. Henry Stommel showed analytically in 1961 that a simple two-box ocean model has two stable equilibria: a strong "on" circulation and a weak or reversed "off" state, and that the system can flip between them once freshwater forcing crosses a critical threshold. The IPCC's Sixth Assessment Report (2021) judged an abrupt collapse this century "unlikely but not impossible," implying roughly a 5-10% probability under high-emission scenarios — though models disagree by a factor of five on freshwater sensitivity, so whether the AMOC has true bistability or just gradual weakening remains an open question.
What the paleoclimate record shows
Greenland ice cores record 25 Dansgaard-Oeschger events — abrupt warmings of 8-16°C in less than a decade during the last glacial period — each linked to rapid AMOC changes. The best-documented case is the Younger Dryas, roughly 12,900 years ago, a ~1,200-year cold snap triggered by a meltwater pulse from the collapsing Laurentide Ice Sheet. A weaker AMOC also has knock-on effects beyond temperature: it reduces the geostrophic pressure gradient that normally depresses sea level along the US East Coast (a 30% weakening could add 20-30 cm to Boston, New York and Miami) and shifts the Intertropical Convergence Zone southward, intensifying Sahel drought by weakening the West African and Indian monsoons.
Frequently asked questions
What drives thermohaline circulation?
Thermohaline circulation is driven by density differences from temperature (thermo) and salinity (haline). Cold, salty water is denser and sinks; warm, fresh water is buoyant and rises. In the North Atlantic, winter cooling and brine rejection during sea-ice formation both raise the density of surface water enough for it to sink to 2,000-4,000 m depth, forming North Atlantic Deep Water, the main driver of the Atlantic Meridional Overturning Circulation.
Why is Britain warmer than places at the same latitude, like Labrador?
London and Calgary sit at the same latitude, 51°N, yet London's January mean is around +5°C while Calgary's is around −8°C. The AMOC carries roughly 1.3 petawatts of heat northward across 26°N, about 25% of the total poleward energy transport at that latitude, warming the North Atlantic region by 5-10°C above what orbital forcing alone would produce.
Could the AMOC really collapse, and what would that mean?
Henry Stommel showed in 1961 that a simple ocean box model has two stable states, a strong-circulation "on" state and a weak or reversed "off" state, and that the system can flip between them once freshwater input crosses a critical threshold. The IPCC's Sixth Assessment Report judged an abrupt collapse this century unlikely but not impossible, implying roughly a 5-10% probability under high-emission scenarios. Accelerating Greenland ice melt, currently around 280 Gt/yr, is the main freshwater threat being monitored.
Try it live
Everything above runs in your browser — open Thermohaline Circulation — Ocean Conveyor Belt and drag the temperature, sea-ice and freshwater-flux sliders to watch the AMOC gauge weaken in real time. Nothing is installed, nothing is uploaded.
▶ Open Thermohaline Circulation simulation