U.S. Dept. of Commerce / NOAA / OAR / PMEL / Publications


An Example of Fisheries Oceanography: Walleye Pollock in Alaskan Waters

Jim Schumacher

NOAA, Pacific Marine Environmental Laboratory, 7600 Sand Point Way NE, Seattle, WA 98115

Arthur W. Kendall, Jr.

NOAA, Alaska Fisheries Science Center, Seattle, Washington

U.S. National Report to International Union of Geodesy and Geophysics 1991–1994, Rev. Geophys., Suppl., 1153–1163 (1995)
Copyright ©1995 by the American Geophysical Union. Further electronic distribution is not allowed.

Shelikof Strait FOCI

Research Strategy

Prior to FOCI, only very limited knowledge existed of either the physical environment or the life history of pollock in the western Gulf of Alaska. What was known suggested the following hypothesis: optimum survival and subsequent recruitment result when larvae are transported to nursery grounds in coastal regions along the Alaska Peninsula, rather than into the Gulf of Alaska. Further, biophysical processes occurring during transport have significant impact on survival. Initially studies focussed on the life history of pollock and the nature of the regional circulation. As these aspects became known, field operations switched to maintenance time series of selected biological and physical characteristics, studies of biophysical processes, and development of methods to examine preferential survival. Simultaneously, we began implementation of coupled biophysical and correlative models, and development of methods to transfer FOCI results to the assessment and prediction models used to provide biomass scenarios to management.

Pollock Life History

Separation of pollock larvae from those of similar species in field samples was first accomplished in 1981 [Dunn and Matarese, 1987]. At the same time, the strong year-classes in the mid-1970's resulted in a large fishery [Megrey, 1990], and hydroacoustic surveys were conducted to estimate the adult population for input to assessment and prediction models. The surveys showed that large concentrations of pre-spawning walleye pollock migrate from the southwest end of Shelikof Strait (taken to include the sea valley that extends from the Barren Islands southwestward to the slope off Chirikof Island, Figure 1) primarily to the area near Cape Kekurnoi. Spawning takes place mainly in the deep sea valley in early April [Kim and Nunnallee, 1991], at depths between 150-250 m. Each female produces about ½ million free floating planktonic eggs in a series of about 10 batches over a period of a few weeks. The eggs reside mainly below 150 m and hatch in about 2 weeks. The short localized spawning pattern creates a large "patch" of eggs observed in plankton surveys [Kendall and Picquelle, 1990]. Mortality rates of the eggs decrease through the spawning season from 0.4/day to 0.1/day [Kim and Gunderson, 1989].

Figure 1. Upper Panel: The FOCI study area in the western Gulf of Alaska with a schematic showing the location of pollock life history stages. The outlined arrows represent potential transport of larvae off the shelf. Lower Panel: Circulation in the study area as derived from satellite-tracked buoys (51) drogued at 40 m and deployed between 1986 and 1994 (after Schumacher and Kendall [1991]).

The larvae are about 3-4 mm Standard Length (SL) at hatching and are relatively undeveloped, without functioning mouths or eyes. They quickly rise from their deep hatching depth to the upper 50 m of the water column, where they drift in the prevailing currents for the next several weeks (late April through May). They generally remain in identifiable patches, growing about 0.2 mm/day with a daily mortality rate of ~8.7% during this time. Their diet consists mainly of early life stages of copepods [Canino et al., 1991], and the size range of prey increases as the larvae grow. Larger larvae undergo diel migrations (deepest during the day) between 15-50 m. Larvae appear to stay just below the turbulent wind mixed upper layer of the water column [Kendall et al., 1994]. They are visual feeders, eating mostly during the day [Kendall et al., 1987].

By late May considerable year-to-year variation exists in abundance and location of larvae [Kendall and Picquelle, 1990] as well as the zooplankton that produce their prey [Incze and Ainaire, 1994]. Two primary tracks characterize westward larval drift: along the Alaska Peninsula in the relatively slow moving flow (<10 cm s-1) over the shoreward edge of the sea valley, and offshore in the rapidly (>25 cm s-1) moving Alaska Coastal Current [Kim and Kendall, 1989]. By midsummer the larvae have transformed into juveniles, which by late summer are schooled and become concentrated in nearshore areas along the Alaska Peninsula [Hinckley et al., 1991]. After this period, we know little about their life until they enter the fishery and become sexually mature at age ~3 years. The adults live for ~11 years.

We have established the life history pattern between spawning migration and young of the year (Figure 1). Using results from egg and larval surveys, together with estimates of the spawning adult population from hydroacoustic observations and indices of juvenile abundance [Bailey and Spring, 1992], the stages when year-class strength is established have been determined. A low abundance of larvae results in weak recruitment. A large abundance of larvae, however, does not imply strong recruitment. This suggests that processes during the juvenile stage can also be critical [e.g., Bailey et al., 1994b]. Recently, we have focussed more research on understanding young of the year juveniles since interannual variability in their survival also affects year class strength [Bailey and Spring, 1992].

Regional Circulation and Mesoscale Features

Much of the variability in the physical environment in the Gulf of Alaska results from large scale atmospheric phenomena. Global patterns in the upper level atmospheric pressure generate climatic conditions that include an annual cycle in the number of low pressure centers traversing the region [Niebauer, 1988]. The consistent passage of storms along the Aleutian Island chain (the Aleutian Low) dominates wintertime atmospheric circulation. Interaction of frequent storms with the mountainous coastline results in a high precipitation rate (>200 cm yr-1) along the coastal region. The discharge rate of freshwater reflects seasonal variations in air temperature, precipitation, runoff and storage from the previous winter [Royer, 1982].

Along the Alaska Peninsula, along with a deep (>250 m) sea valley, a high, nearly continuous mountain chain exists (Figure 1). The mountains perturb regional winds so that in Shelikof Strait proper down-gradient winds are common [Schumacher et al., 1989], and the winds over coastal waters west of Kodiak Island are altered for ~60 km offshore [Macklin et al., 1993].

The dominant circulation feature is the Alaska Coastal Current (ACC), a distinct flow that only 20 years ago was unknown. FOCI research has elucidated many of the characteristics of the ACC, which extends for >1500 km along the coast of Alaska [Reed and Schumacher, 1981]. This is one of the most vigorous coastal currents in the world with speeds typically between 25 and 100 cm s-1 [Stabeno et al., 1995]. Volume transport results from the addition of freshwater along the entire coastline and is perturbed by the alongshore wind through both confinement of the freshwater and alteration of coastal sea level [Schumacher and Reed, 1980; Royer, 1981; Reed and Schumacher, 1981]. The observed mean transport in Shelikof Strait is ~0.80 × 106 m3 s-1; wind forced pulses exceed 3.0 × 106 m3 s-1 [Schumacher et al., 1989; Stabeno et al., 1995]. Wind-driven fluctuations within the strait proper are greater than those over coastal waters east of Kodiak Island due to the topographic effects on the winds [Stabeno et al., 1995]. Differential Ekman pumping may amplify this mechanism within the strait proper [Reed and Schumacher, 1989a, b]. Estimates of net volume transport computed from water property observations collected between 1985 and 1992 have a mean of 0.66 × 106 m3 s-1 [Reed and Bograd, 1995].

In Shelikof Strait, horizontal density gradients and vertical shear in the mean flow create the baroclinic instability, evident in satellite images [Vastano et al., 1992; Schumacher et al., 1991] and in analysis of current records [Mysak et al., 1981], which dominates flow patterns and generates eddies [Schumacher et al., 1993]. The ACC does not span the sea valley, and estimates of coherence become insignificant for separations >10 km [Reed and Schumacher, 1989b; Bograd et al., 1994]. Estuarine-like flow also exists, with warmer more saline water from the continental slope entering on the southeastern side of the valley [Reed et al., 1987]. The ACC bifurcates east of Sutwik Island; one branch continues along the Alaska Peninsula and the other flows seaward through the sea valley [Schumacher et al., 1989]. Since 1986, 51 satellite tracked buoys (drogued at 40 m) were deployed in the study area during spring near Cape Kekurnoi. To date, 25% of the buoys continued along the Peninsula. The remainder moved seaward past the Semidi Islands, most, however, traveled shoreward (between ~157° and 158°W) and joined the flow along the Peninsula. Only 25% of the buoys left the shelf permanently and became incorporated in the Alaskan Stream [Stabeno and Reed, 1991].

FOCI research has found and elucidated the dominant circulation and mesoscale features: the ACC, eddies generated by baroclinic instability, and an estuarine-like flow of slope waters into the sea valley. These features must be simulated in any numerical model of the region. Further, results show that the timing and location of hatching determines whether larvae enter an eddy, or are transported with either the slow-moving coastal flow or the rapid ACC. Modeling studies [Stabeno et al., 1995] suggest that the location of late larvae varies greatly year to year depending on advection. The phasing between biological and physical processes determines transport of larvae and presumably their eventual recruitment.


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