Morphology and Structure of Maury Channel, Northeast Atlantic Ocean
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NORMAN Z. CHERKIS ] HENRY S. FLEMING I Naval Research Laboratory, Washington, D.C. 20375 ROBERT H. FEDEN Morphology and Structure of Maury Channel, Northeast Atlantic Ocean ABSTRACT Maury Channel is a 3,500-km-long, ero- sional/depositional feature. Originating on the southern slope of the Faeroe-Iceland Ridge at about 64° N., 13° W., the channel follows the deepest axis of Rockall Basin until about 53° N., where it begins a meandering course through several northeast Atlantic fracture zones. The channel finally empties into the northern Iberian Basin. Turbidity currents and overflow boulses of Norwegian Sea deep water are thought to be responsible for the formation of the channel. Strong bottom cur- rents are responsible for keeping the channel "open" south of 53° N. Seismic reflection pro- files reveal a characteristic "signature," indi- cating deposition of dense turbidite material wherever the channel is encountered. INTRODUCTION Maury Channel (Ballard and others, 1971), also called Viking Channel (Cherkis and others, 1971), is a long, narrow erosional/depositional feature that undulates along the floor of the Figure 1. Locations of Maury Channel and other northeast Atlantic Ocean for a distance of known and implied channels in the northeast Atlantic Ocean. Heavy E.-W. lines indicate positions of the about 3,500 km. As early as 1953, Ewing and double axis of the Gibbs fracture zone and the axis of others suspected the existence of this channel, a second, unnamed fracture zone at 50°30' N. or "mid-ocean canyon." However, confirma- tion of Maury Channel's existence was not before beginning its meandering course through published until Johnson and Schneider (1969) the complex topography associated with sev- displayed a portion of the channel as it passes eral of the northern Atlantic fracture zones. adjacent to the base of Rockall Rise to the The channel finally debouches into the north- east. Although no mention of the channel was ern Iberian Basin. Johnson and others (1971) made in that paper, the contour chart clearly suggest that the channel empties into the displays the feature. Porcupine Abyssal Plain at 49° N„ 20° W. From its origin on the southern slope of the Molnia and Ruddiman (1971) suggest that the Faeroe-Iceland Ridge at about 64° N., 13° W., channel, while traveling eastward at 48° N., the channel traverses southward along the debouches into the Biscay Abyssal Plain. The deepest axis of Rockall Basin between Rockall authors suggest that Maury Channel does Rise and Reykjanes Ridge (Fig. 1). It then neither. Recent bathymétrie and seismic re- hugs the base of the west side of Rockall Rise, flection studies have clearly shown that the Geological Society of America Bulletin, v. 84, p. 1601-1606, 3 figs., May 1973 1601 Downloaded from http://pubs.geoscienceworld.org/gsa/gsabulletin/article-pdf/84/5/1601/3443289/i0016-7606-84-5-1601.pdf by guest on 26 September 2021 1602 CHERKIS AND OTHERS bathymetric expression and dense acoustic per sec. These waters debouch into Rockall signature of the channel continues to appear Basin along with the other overflow water as the channel undulates southward of 48° N. and are additionally joined with discharge- (Figs. 2 and 3 A and B). laden melt and glacial runoff from Iceland. Current velocities of 8 to 25 cm per sec are ORIGINS strong enough to limit deposition of sediments Turbidity currents are generally believed to in all size ranges smaller than coarse gravel be primary processes in the formation of deep- (Jones and others, 1970), and deep-water sea channels world-wide (Dietz, 1953; Ewing masses flowing at ths rate of 100 cm per sec and others, 1953; Menard, 1955; Shepard and are capable of generating turbidity current Dill, 1966; Heezen and others, 1969). It is, flows. Bottom photographs should confirm the therefore, reasonable to assume that the forma- flow ay showing a current-scoured bottom tion of Maury Channel was at least partially along the overflow areas. dependent upon turbidity currents, possibly The fact that turbidity flow is at least a occurring at the same time as the late Pleisto- partial agent in the formation of Maury Chan- cene flooding that produced turbidity currents nel is borne out by observed sediments in the resulting in the formation of Cascadia Channel northern part of the channel where black vol- (Griggs and others, 1970; Griggs and Kulm, canic sands and gravels exist (Ballard and 1970) in the northeast Pacific Ocean. During others, 1971). Rounded, possibly ice-rafted the Pleistocene, sea level decreased as much as pebbles (Molnia and Ruddiman, 1971) have 60 fathoms (110 m) (Moore, 1958). During also been recovered in the northern part of those periods, glacial recessions produced tre- the channel. In all probability, a complex mendous volumes of heavily discharge-laden combination of periodic turbidity-current melt that helped to cut the numerous near- flows and regular bcttom-current movements shore submarine canyons at the seaward '.Termi- are responsible for both the formation and nations of the straths on the southeast coast present-day conditions of Maury Channel. of Iceland. Another agent possibly resulting in the generation of these formational turbidity STRUCTURE currents is slumping along the insular slope of Maury Channel lies upon Paleocene crust Iceland caused by sedimentary overburden at or near its source area (Molnia and Ruddi- and the numerous seismic events in the area. man, 1971). The ages of the northern channel Still another means for generation of turbidity sediments are believed to be 12 to 13 m.y. old, currents is through density changes in deep contingent upon the premise that their source water. Dietz (1953) explains that "a very area is Iceland. The segment north of the Gibbs slight increase of salinity or a decrease of fracture zone lies geographically near the temperature of a water mass with respect to deepest axis of Rockall Basin. From 60° N. to the surrounding water will cause it to under- 56° N., the axis is at the base of Rockall Rise- flow the surrounding water if the mass of water Hatton Bank (Scrutton and Roberts, 1971). with increased density is large." In the area The rise is heavily incised, indicating that a near the head of Maury Channel, cold dense good deal of detritus is moving downslope and Norwegian Sea deep water overflows the hence toward the channel. Along this portion, Iceland-Scotland Ridge system. Between Rock- coriolis force (Menard, 1955; Dietz, 1958) is all Rise and Reykjanes Ridge, the deep cur- nullified by the adjacent topographic barrier. rents have been measured at 8 to 25 cm per sec (Steele and others, 1962). The deep water is The channel follows the basic trend of the also sent into Rockall Basin after overflowing Mid-Atlantic Ridge to the west. Lateral ridge the Faeroe-Shetland Sill. This water is di- offsets such as the Gibbs fracture zone (Fleming verted westward into Faeroe Bank Channel and others, 1969, 1970) are transform faults (also called Southwestern Faeroe Channel; between the ridge crests (Wilson, 1965; Menard Harvey, 1965) by the Wyville-Thcmson and Atwater, 1969), and these features extend Ridge. The latter effectively blocks deep-water beyond the offset ridge crests as troughlike movement because of its 600-m sill depth features. The sharp, easterly bends in Maury (Ellett and Martin, 1970). Crease (1965) re- Channel occur at precisely the points where ports that current velocities through the the channel intersects the northern trough Faeroe Bank are are on the order of 100 cm wall of each individual fracture zone. At these junctures, the channel follows the fracture Downloaded from http://pubs.geoscienceworld.org/gsa/gsabulletin/article-pdf/84/5/1601/3443289/i0016-7606-84-5-1601.pdf by guest on 26 September 2021 MAURY CHANNEL, ATLANTIC OCEAN 15° 3000 J Figure 2. Locations of bathymetric profiles across Maury Channel. Arrows over profiles indicate channel axis. zone troughs for as many as 140 n mi (260 km) double fracture zone), the fracture runs from before encountering a gap or gaps breaching about 48° W. (Olivet and others, 1970a, the fracture zone southern trough wall and re- 1970b) across the offset Mid-Atlantic Ridge turning to the predominantly southern flow. (which it creates), and continues eastward to In the case of the Gibbs fracture zone (a east of 20° W. long. (Naval Research Labora- Downloaded from http://pubs.geoscienceworld.org/gsa/gsabulletin/article-pdf/84/5/1601/3443289/i0016-7606-84-5-1601.pdf by guest on 26 September 2021 1604 CHERK::S AND OTHERS tory, 1971, unpub. data). Maury Channel 30° '5° 0° intersects the Gibbs fracture zone north all of the northern trough at 26°30' W. The chan- nel then turns south until it breaches the north wall of the southern trough. The zigzag process repeats itself, but this time for only 20 n mi (37 km). Farther south, at 50°30' N„ the easterly bend occurs along another fracture zone (NRL, 1969, unpub. data). The channel flows along this fracture zone trough for about 140 n mi (260 km) before encountering a breach in the southern wall, whereupon the channel returns to a southerly flow. These processes are repeated several times between the latitudes of 48° N. and 55° N. The bends are always to the east rather than flowing west along the fracture zone troughs. The theory that coriolis force controls fluid movement in the oceans is supported by these observations, although the force appears to be truncated upon encountering each fracture zone. North of the fracture zone province, the Norwegian Sea deep water comes off the bot- tom and laminates and disperses (D. Fenner and P. Bucca, 1972, oral commun.), and a great Figure 3A.