Short commentary on marine productivity at Arctic shelf breaks: upwelling, advection and vertical mixing

In their seminal 2003 paper mentioned above, Carmack and Chapman applied a numerical model to study shelf–basin exchange on the Beaufort Sea shelf and argued that decreased ice concentrations will enhance upwelling in the area. The argument goes like this: when a thick ice cover lies like a lid on the ocean, it absorbs most of the wind stress instead of transferring it to the underlying ocean. When the ice edge recedes far enough north that the shelf break is exposed, however, the winds can move around the surface waters more easily. Sustained easterlies, for example, will lead to a northward Ekman transport, and where the shelf is shallow enough that it affects surface currents (see Figs. 2 and 3), deeper waters are drawn up to balance the off-shelf transport.

Figure 2Depth of the Arctic shelf break extracted from the IBCAO V3 bathymetry of the Arctic Ocean (Jakobsson et al., 2012), excluding only the Saint Anna Trough and the Chukchi Borderland. Most visible are the continental shelf off Alaska and the westernmost part of the Canadian shelf, where Carmack and Chapman (2003) conducted their study and upwelling has been frequently documented, and north of the Laptev Sea. In most other areas of the Arctic Ocean, the shelf break is several hundred metres deep and therefore out of reach to interact significantly with Ekman-driven surface ocean dynamics. For a detailed explanation of the algorithm and the computer code used to extract shelf break depths, see the Supplement.

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Figure 3Schematic of the mechanism behind wind-driven shelf break upwelling. When wind blows along the shelf break, it generates an Ekman current (horizontal arrows) off-shelf. (a) When the shelf is shallow enough, the current over the shelf is slowed down, leading to a horizontal divergence and thus pressure gradient that is filled by drawing up deeper waters. (b) When the shelf is deeper, there is no horizontal divergence. Other mechanisms, such as dynamic uplift, are independent from wind and not discussed here, but see e.g. the book by Kämpf and Chapman (2016).

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This argument was reinforced by a number of studies conducted in the Pacific Arctic (Arrigo et al., 2014; Lin et al., 2016; Schulze and Pickart, 2012; Spall et al., 2014; Williams et al., 2006), which directly extended earlier direct observations of shelf break upwelling dating back to at least the 1980s (Aagaard et al., 1981). A detailed study (Spall et al., 2014) on the dynamic response during one particularly impressive example of shelf break upwelling in the Chukchi Sea (Arrigo et al., 2014) demonstrated potentially large contributions to primary productivity in that area.

The idea has since caught on to explain or project marine productivity also in other regions of the Arctic Ocean, for example at the Barents Sea shelf break. There it has appeared both in numerous personal communications among the community working with the physical and ecological environment of the Barents Sea and a number of published articles (Falk-Petersen et al., 2014; Haug et al., 2017; Hunt et al., 2016; Tetzlaff et al., 2014; Våge et al., 2016; Wassmann et al., 2015). Thus it might appear as if shelf break upwelling is currently being cemented as a universal paradigm to conceptualize the “new” Arctic Ocean where global climate change is taking us. We will argue that some of the regional differences cannot be ignored when discussing what governs productivity in the various shelf regions.

Upwelling comes in many different forms: the well-known upwelling that feeds so many productive coastal areas of the world is created by winds blowing along-shore, driving an offshore surface current that “pulls up” nutrient rich waters. (This will in practice most often be the Ekman transport; however, shelf break upwelling would function in much the same way at the Equator where there is no Coriolis force, even though upwelling-favourable winds would then blow directly off-shelf instead of along-shelf.) The divergence sets up a horizontal gradient in sea surface height that balances the Coriolis force, meaning that deeper waters are drawn towards the surface and/or onto the shelf (Kämpf and Chapman, 2016).

Alternatively, storms can lift deeper waters up to the shelf break, making them spill over and mix with shelf waters. Canyons and troughs that cut into a continental shelf may aid by steering the flow there through its topography. All of these phenomena can act together to bring new nutrients into shelf waters.

But besides upwelling, other factors are at play. Two important ones are vertical mixing and advection with large-scale ocean currents, and both of them can become entangled with upwelling in that they can lead to similar effects in the regional oceanography and be hard to tell apart by the most basic means of hydrography, which are vertical profiles of temperature and salinity. Because different areas within the Arctic Ocean are subject to very different forcing, large gradients in physical properties exist between e.g. the Bering Strait, Fram Strait and the Siberian Shelf. Naturally, this means that the drivers of marine productivity will also vary strongly between these areas.

There is an ample storage of fresh water in the Arctic Ocean because of the large rivers draining Siberia and North America, but also because the inflow of Pacific Water through the Bering Strait is much fresher than its Atlantic counterpart (Aagaard and Carmack, 1989). But the fresh water is not evenly distributed: most of it is found in the Beaufort Gyre located around the Canadian Basin (Morison et al., 2012; Proshutinsky et al., 2015). When light water (at low temperatures, this means fresher) sits on top of heavy water, mixing will not be as efficient (Osborn, 1980), which means that the most important factor for vertical mixing is vertical stability (since overall, there is a given amount of energy available to stir the ocean, e.g. from tides, wind and so on.) In the Beaufort Gyre, all the fresh water and the resulting strong stratification severely restrict the upward supply of fresh nutrients, making it one of the most nutrient-depleted regions of the world ocean (Codispoti et al., 2013; Gruber and Sarmiento, 1997; Tremblay et al., 2015).

In contrast, the Atlantic inflow along the shelf break north of Svalbard is much denser than the surface waters of the central Arctic Ocean, but nevertheless extends up to the surface (Rudels, 2016). Seeing this situation in the contour plot of a hydrographic transect (see Fig. 4b) may at first look like a classical upwelling scenario: surely there must have been upwelling to get the heavy waters up there in the first place? The answer is not necessarily – what we are seeing is Arctic and Atlantic water masses meeting, and the narrow but strong gradient is maintained by a continuous inflow of more Atlantic Water. In the absence of detailed (hydrographic) time series, it is impossible to say anything conclusive about the state of upwelling from Fig. 4b alone.

Figure 4Representative illustration of the hydrographic regime in the Atlantic inflow area along the northern Barents Sea shelf break. (a) Inflowing warm and salty Atlantic Water maintains high surface salinity on and around the shelf, enabling convection when the surface waters are cooled in winter. The colour scale shows salinity, and the black contour lines show the 0 and 3 ^∘C isotherms (average of 2015–2018 monthly January mean at 10 m of depth from the operational ocean reanalysis Mercator, downloaded from http://marine.copernicus.eu (last access: 7 March 2018); the version of Mercator used for this plot is a global ocean forecasting model on a 1/12^∘ × 1/12^∘ grid and showed good agreement with winter data for this area in a study by Koenig et al., 2017). The cyan line indicates the location of the transect displayed in panel (b). (b) Seawater absolute salinity S_A and conservative temperature in a typical wintertime transect across the shelf slope north of Svalbard; sampled in January 2014. Data from approximately 81.5^∘ N, 17.5^∘ E; RV Helmer Hanssen, Carbon Bridge project (Randelhoff and Sundfjord, 2017); see panel (b) for location. Salinity is plotted on the colour scale, and temperature is marked (in ^∘C) on the black isolines inside the plot. The surface water is markedly heavier above the upper shelf slope than over the deep basin. Black triangles mark hydrographic stations. The black patch marks the along-transect bathymetry extracted from the IBCAO V3 bathymetry (Jakobsson et al., 2012). During the sampling of this transect, winds were moderate southerlies to south–south-easterlies, so mean Ekman transport in the surface was mainly directed along-shelf to the east.

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We thus need to distinguish between basin-scale and regional hydrography; that is, between strong haline stratification in the Arctic Ocean in general and weak thermal stratification in the Atlantic inflow (Carmack, 2007). The salient point is this: as the Atlantic Water is cooled on its way north, it loses stability, potentially leading to wintertime convection (Ivanov et al., 2016) and efficient vertical mixing. The result is that the surface layer nutrient reservoirs are replenished long before the end of winter (Randelhoff et al., 2015); increased wintertime upwelling will not bring more nutrients to the surface. Essentially, the upwelling water mass would have the same salinity and nutrient characteristics as the one that is already present in the surface; upwelling does not add nutrients when there is no vertical gradient in nutrient concentrations. In contrast, the Beaufort Sea is strongly stratified throughout the year; if winter upwelling is to increase there because of reduced sea ice, this can be an important factor contributing to the pre-bloom nutrient pool.

In contrast to storms, which can lift deeper waters independently from any sort of topographic constraint (i.e. Ekman pumping), coastal and shelf break upwelling driven by specific wind directions need the presence of a coastline or a sufficiently shallow shelf. This is because they require a horizontal divergence in the off-shelf transport of surface waters. This divergence can only be potent enough when the shelf itself is shallow enough to actually constrict the surface flow over the shelf (Fig. 3). Whereas large swaths of the continental shelves of the Arctic Ocean are very shallow (in parts less than 50 m), the Northern Barents Sea shelf break is relatively deep at around 150–250 m (see Fig. 2). Because surface and bottom boundary layers will not overlap in this case (Price and Sundermeyer, 1999), shelf break upwelling as an effect of along-shore winds is presumably negligible. Also note that Ekman layer depth decreases with increasing latitude and decreasing wind strength (Wang and Huang, 2004) and that during the stratified summer period, the Ekman layer will at any rate be restricted to at most the surface mixed layer (see e.g. Price et al., 1987).

In general, the regions that (only based on the depth of the shelf break) stand out as most prone to wind-driven shelf break upwelling are the aforementioned continental shelves of Alaska, the westernmost part of northern Canada and possibly the Laptev Sea, although the shelf is rather wide here, potentially diminishing the effect of easterlies somewhat. In regions where the shelf is narrow, the presence of the coastline can aid in the upwelling of deeper waters. Seeing that the Chukchi and Siberian shelves are rather wide, potential upwelling will likely be relatively weak across large swaths of the Arctic shelf regions.

We have seen how the pre-bloom surface nutrient inventory at the northern Barents Sea shelf break can be replenished just by the inflowing Atlantic Water, without recourse to wintertime upwelling. In summer, however, nutrients are depleted in surface waters such that even sporadic upwelling could inject nutrients that could be utilized immediately and funnelled into the food web (Kämpf and Chapman, 2016).

Here, another difference between the Atlantic and Pacific inflow areas comes into play, namely dominant wind patterns: the Beaufort Sea shelf is dominated by the Beaufort High–Aleutian Low system, meaning predominantly easterlies at the Canadian shelf break (Serreze and Barrett, 2011). The atmospheric circulation in the Atlantic sector is more dynamic in summer, with less of a preference for a specific upwelling-favourable wind direction (see e.g. Fig. 5). This comes on top of a general pattern in which wind speeds north of Svalbard are lower in summer than in winter. Fig. 5 illustrates how only roughly 2 % of all summer days through the last 30 years can be considered upwelling-favourable using a very generous criterion for what constitutes “upwelling-favourable”, and even this is assuming that the local topography would allow for this kind of upwelling. (Again, note the difference to the Beaufort shelf where winds are very upwelling-favourable also in June; see Lin et al., 2016.) There might still be storms that make deeper waters spill onto the shelf by Ekman pumping alone, but these also have a tendency to occur more frequently in the winter season (Lind and Ingvaldsen, 2012).

Figure 5Days of “potentially upwelling-favourable” winds north of Svalbard 1987–2017, assuming that the local bathymetry facilitates such upwelling, based on ERA-Interim data (Dee et al., 2011) for the region 79–81^∘ N, 5–30^∘ E. A daily wind speed was considered “potentially upwelling-favourable” if its (approximately easterly) along-shelf component exceeded 3 m s⁻¹ for at least 3 consecutive days. (3 m s⁻¹ is a rather low wind speed, well below the “optimal environmental window” of 5–6 m s⁻¹ for upwelling suggested by Cury and Roy (1989) and makes for a generous criterion in this regard. Likewise, Kämpf and Chapman (2016) give a timescale of around 5 days from the onset until the complete development of coastal upwelling. Effectively, both criteria should err on the upwelling-favourable side.) From the beginning of May through August each year, ∼ 2 % of all days were “potentially upwelling-favourable”.

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As has been shown above, wind statistics as well as general physical considerations and geographical features – the northern Barents Sea shelf being too deep for surface and bottom Ekman layers to overlap and produce shelf break upwelling – imply that upwelling should not be expected to feature very prominently on the Barents side of the Arctic. This is not to say that upwelling events cannot ever happen (and indeed, in a system as complex as the Earth, it would be surprising if it never happened), but no known physical mechanism would suggest a magnitude, frequency or importance similar to what has been found in the Pacific sector. To illustrate our point, we refer to recent analysis by A. Renner and collaborators. They have analysed the first year-long time series from a moored CTD array over the shelf slope north of the Barents Sea (A-TWAIN project at 30^∘ E). By applying methods that have successfully detected the frequent occurrence of upwelling over the Beaufort Sea slope (Lin et al., 2016), they could not identify signatures of upwelling in the density field in response to possibly favourable along-slope winds (Angelika H. H. Renner, personal communication, 2017, and Renner et al., 2018).

Shelf break upwelling is often thought of as becoming more prominent in the Arctic as the ice recedes poleward with ongoing climate change, exposing the shelf break more and more (see references given in the previous section “Upwelling in the Arctic”). But it should be kept in mind that the mere earlier presence of an ice cover would not have prohibited wind-driven upwelling (or Ekman pumping) and could even have enhanced it in some circumstances. For instance, Martin et al. (2014) showed how a loose ice cover (80–90 % ice concentration) can yield an optimum transfer of wind energy into the upper ocean when internal ice stresses are negligible because sea ice has a rougher surface than open water and can therefore be moved around more easily by the winds. This is consistent with the observation of Schulze and Pickart (2012) that the upwelling response at the Beaufort Sea shelf off Alaska was strongest when there was partial ice cover. Once again, there are differences between the historically thick, multi-year ice cover of the Pacific Arctic (Maslanik et al., 2007) and the more dynamic first- and second-year ice cover north of Svalbard (Renner et al., 2013). In the latter area, it is not a new feature that the ice cover is quite dynamic and rough, which possibly leads to an efficient transfer of wind energy as was demonstrated in the previously mentioned paper by Martin et al. (2014). It is therefore not a given that reduced ice cover north of Svalbard will automatically make surface currents more responsive than they were in the past, especially under the responsive summer pack ice when upwelling has the chance to substantially alter the marine ecosystem through sporadic nutrient input.

In fact, there are pathways entirely unrelated to upwelling through which climate change is probably impacting and enhancing marine productivity. Indeed, the regional loss of sea ice has been attributed to the inflow of warmer Atlantic Water (Onarheim et al., 2014). As the Atlantic Water travels further and further east along the shelf break before it is sufficiently cooled and its core is subsequently subducted under the Arctic water masses, it pushes back the ice edge and erodes stratification (Polyakov et al., 2017) – meaning it provides access to nutrients and light at the same time! This will enhance regionally averaged primary production by itself, without the need to invoke shelf break upwelling.

In addition to heat, salt and nutrients, the Atlantic (like the Pacific) water also carries large amounts of zooplankton. This makes the inflow areas perfect feeding grounds for larger fish and mammals, adding to local primary production. For instance, there is an excess of organic carbon production NW of Spitsbergen in May and June (Maria Vernet, personal communication, 2017), in agreement with modelling results (Wassmann et al., 2015). As sea ice recedes northward and eastward, it might extend this region of net heterotrophy (carbon consumption). However, results from a coupled ocean and ecosystem model indicate that by the end of the 21st century, zooplankton advection along the shelf break will dwindle, and marine life in the area might rely much more on local production (Wassmann et al., 2015). Such processes would contrast a projected pan-Arctic strengthening of upper ocean stratification that might lead to a smaller plankton size spectrum, fuelling a food web that recycles more than providing food for higher trophic levels (Li et al., 2009, 2013).

The data shown in Fig. 4b are available at https://doi.org/10.21334/npolar.2017.f40317d5 (2017; see the references). The algorithm used to generate Fig. 2 is published in detail in the Supplement.

The supplement related to this article is available online at: https://doi.org/10.5194/os-14-293-2018-supplement.

The authors declare that they have no conflict of interest.