On Estuarine and in the Middle

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On Estuarine and in the Middle 7 7.1 Introduction On Estuarine and We shall attempt in this chapter to trace the develop- Continental-Shelf ment of ideas about circulation over the continental Circulation shelf in the Middle Atlantic Bight and in the major in the Middle estuaries which drain into the Middle Atlantic Bight. Atlantic Bight The term Middle Atlantic Bight refers to the curved section of the continental shelf off the eastern United States stretching between Cape Hatteras to the south Robert C. Beardsley and Cape Cod and Nantucket Shoals to the northeast. William C. Boicourt The New York Bight is a subsection of the Middle Atlantic Bight and refers to the shelf region stretching between the New Jersey and Long Island coasts. A schematic version of Uchupi's (1965) topographic map is shown in figure 7.1, indicating both the general shape of this shelf region plus the names and locations of the major estuaries and key positions discussed in the text. We have decided to focus this review of estuarine and shelf cirulation on the Middle Atlantic Bight and its estuaries for several reasons. The major Middle At- lantic Bight estuaries have been extensively examined and have provided several important case studies in the development of new ideas about circulation and turbulent-mixing processes in moderately stratified coastal-plain-type estuaries. These estuaries and the adjacent continental shelf border on one of the world's largest urban complexes; a better description and un- derstanding of the circulation and dominant mixing processes occurring in this particular region is clearly needed for a more effective management of the regional estuarine and shelf resources in the face of man's many conflicting uses of the water bodies. Fostered in part by increased environmental concerns, more adequate research funding, and the availability of new instru- mentation and observational techniques, many new circulation and related physical studies have been un- dertaken in the last two decades, and a synthesis of both old and new material into a review of the regional estuarine and shelf circulation seems particularly ap- propriate at this time. While a few scientists have made important contributions in both fields and have thus helped to carry new ideas and techniques from one field into the other, basic research on problems con- ceming estuarine and continental-shelf circulation have evolved more or less independently in time, so that we will present here separate reviews of the his- torical and the modem ideas about estuarine and shelf circulation in the Middle Atlantic Bight. One impor- tant research objective in the 1980s will be to develop a better kinematic and dynamic description of the physical coupling between estuarine and shelf waters. Our present meager knowledge about the different physical processes that connect the shelf and estuary together prevent a more unified discussion. i98 R. C. Beardsley and W. C. Boicourt _ ___·_I_ __·I______ Figure 7.I A topographic map for the Middle Atlantic Bight 200-m isobaths are shown. and a western section of the Gulf of Maine. The 60-, 100-, and 7.2 Estuarine Circulation in the Middle Atlantic 1876), the Strait of Gibraltar in the Mediterranean Sea Bight (Douglas, 1930), and the Strait of Bab el-Mandeb at the mouth of the Red Sea (Buchan, 1897) all reflect the We shall trace here the evolution of estuarine-circula- balance between evaporation, runoff, and precipitation tion ideas. We will use the Middle Atlantic Bight es- in the enclosed seas. On a smaller estuarine scale, the tuaries as a focus because physical studies of these formulation of clear circulation ideas has been hind- water bodies have played a major role not only in the ered by the difficulty of unraveling the different cir- development of the early concepts of the physics of culation components in a variety of estuarine geome- estuaries but also in the recent refinement and refor- tries. In addition to oscillatory tidal currents and mulation of these ideas. Narragansett Bay, the Hudson currents driven by density differences, there has been River, Delaware Bay, and especially the Chesapeake the possibility of "reaction currents" as suggested by Bay system-all have provided case studies from which F. L. Ekman (1876). These were countercurrents and significant advances have been made in our under- undercurrents associated with the entrainment of am- standing of "coastal bodies of water having free con- bient water by the discharge of a river into the sea. nection with the open sea and within which sea water Although the idea of reaction currents seems to have is measurably diluted by fresh water drainage" [Prit- been supported in Helland-Hansen and Nansen's (1909) chard (1967a)]. discussion of the rivers entering the Norwegian Sea and in Buchanan's (1913) description of the flow off the 7.2.1 The Development of Estuarine-Circulation mouth of the Congo River, F. L. Ekman's son, V. W. Concepts Ekman, showed that significant reaction currents were The idea that the introduction of fresh water into the unlikely at the mouths of rivers (Ekman, 1899). The sea can produce an oppositely directed, two-layer cir- terms "reaction current," "induction current" (Cor- culation has existed for a long time. Some early ocean- nish, 1898), "undercurrent" (Dawson; 1897), and "com- ographers understood that the lighter, fresher water pensatory bottom current" (Johnstone, 1923) were spreads away from the source along the surface and the often employed without detailed discussion of the heavier, more saline water moves toward the source physics. In some cases, these terms were used simply underneath. The kinematic details and the dynamics to refer to low-salinity water flowing seaward over of this process have, however, remained elusive until more saline water flowing landward. In other cases, recent years. On a scale as large as the Mediterranean however, the usage harked back to F. L. Ekman's sense Sea, early oceanographers correctly held that the cir- of a countercurrent associated with the river outflow culations were driven by density differences. Two-layer jet. flows observed at the Kattegat in the Baltic (Ekman, I99 Estuarine and Continental-Shelf Circulation - ~~~~_ Reaction currents were invoked to explain the two- role. Wells, Bailey, and Henderson (1929), who titrated layer circulation phenomena found in the early studies the salinity samples for Cowles's surveys, did suggest of the Middle Atlantic Bight estuaries: Although Harris that although the lateral gradient in salinity "had been (1907) correctly described the distribution of pressure ascribed to the fact that the principal rivers enter the surfaces in an estuarine situation, he interpreted Bay on its west side, the rotation of the earth may also Mitchell's (1889) observations on the Hudson River as be a factor." illustrative of F. L. Ekman's countercurrent. Mitchell, Marmer (1925) thought that the greater nontidal sur- in contrast, had interpreted the observed "underrun" face flow and greater ebb duration) along the western of salt water below the outflowing fresher water as a shore of the Hudson River was due to "the effect of the response to a decrease in fresh-water discharge in the deflecting force of the earth's rotation." He noted that, Hudson River. He calculated that "the surface of the at mid-depth, the flood-current velocities were greater river water would have to stand 2-1/2 feet above the on the eastern side of the river, and that the ebb veloc- ocean to prevent the salt water from running in along ities were greater on the western side. Manner in his the bottom; and the sea-water would creep into the Hudson River study, and Zeskind and LeLacheur (1926) basin as soon as the head fell below this." If there were in their study of Delaware Bay, pointed out the de- not mixing between the salt water and the fresh water, crease with depth in ebb-current duration in the estu- Mitchell's analysis would explain the movement of the ary, and ascribed this decrease to the river discharge. density interface between the upper and lower layer Although they noted that the duration of flood may be and the position of the "neutral plane" where "inflow greater than ebb near the bottom of the estuary, neither and outflow balance." Marmer nor Zeskind and LeLacheur conveyed the Although we now know there is significant mixing sense that there is an internal, nontidal circulation between the upper and lower layers in the Hudson, present and that there is net up-estuary motion in the Mitchell's interpretation of his remarkably good cur- lower layer. rent and density observations provided a reasonable Haight's (1938) review of current measurements in explanation for the seasonal variation in salt intrusion. Narragansett Bay contains little discussion of the non- R. P. Cowles (1930) in his monograph on the Bureau of tidal flows. Although the U.S. Coast and Geodetic Sur- Fisheries' studies of the Chesapeake Bay waters noted vey's interest was to define and predict the tidal cur- that such behavior was not adequately explained by rents, Haight may have disregarded reporting the mean reaction currents. He wondered "why the undercurrent flows because the collected measurements were taken (as deduced by salt intrusion) moving in an ingoing by a variety of methods under a variety of conditions, direction is so marked during the winter months, when and because Narragansett Bay displayed such "irregu- the discharge from the rivers is not ordinarily at its larity of currents." Hicks (1959) later noted that Pills- height?" That the surface layers were moving seaward bury's 1889 measurements [summarized by Haight was evident from the U.S. Coast and Geodetic Survey (1938)] did show nontidal flow into the estuary in the data collected by Haight, Finnegan, and Anderson lower layer.
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