cold, oxygen-rich water, displacing the bottom water in its path. The displaced
bottom water is forced to move upwards slowly, setting up an oceanic circulation
(Figs 6.27 & 6.28).
The deep mixing at high latitudes only occurs in two locations: in the North
Atlantic and around Antarctica. Deep mixing does not occur in the North Pacific,
mainly because a physical sill, related to the Aleutian Arc, prevents water
exchange between the Arctic and the Pacific (Fig. 6.28). This asymmetry in deep
mixing drives a global ocean circulation, in which surface water sinks in the North
Atlantic, returns to the surface in the Antarctic and then sinks again and enters
the Pacific and Indian Oceans (Fig. 6.27). The deep flow tends to concentrate at
the western edge of ocean basins, but allows a slow diffusion of water through-
out the ocean interiors. This slow, deep-water flow is compensated by a poleward
return flow in surface waters (Fig. 6.29). A ‘parcel’ of seawater takes hundreds of
years to complete this global ocean journey, during the course of which the deep
water continually acquires the decay products of sinking organic matter from
surface seawater. Waters in the North Pacific have more time to acquire these
decay products because they are the ‘oldest’, in the sense of time elapsed since
they were last at the surface and had their nutrients removed by biological
processes. As a result the deep waters of the Pacific Ocean have higher macronu-
trient concentrations than those in the Atlantic Ocean (Fig. 6.20). The waters of
the North Pacific also have the lowest dissolved oxygen concentrations and high
230 Chapter Six
Americas
Atlantic
Pacific
Americas
Antarctica
Indian
Africa
Europe–Asia
Source
Recooling
Fig. 6.27Idealized map of oceanic deep-water flow (solid lines) and surface-water flow
(dashed lines). Open circles represent areas of water sinking and dark circles areas of
upwelling. After Broecker and Peng (1982).