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Back to the Moon with Nuclear Rockets

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Shearing suloy on <strong>the</strong> boundary of <strong>the</strong> sou<strong>the</strong>rly flowing curren<strong>to</strong>f Mozambique Channel, from <strong>the</strong> Shuttle Discovery,Aug. 16, 1985, at 190 nautical miles.where I feared for <strong>the</strong> planks," as stated in more than one of<strong>the</strong> log books in Maury's hands.If <strong>the</strong> chaotic "siomes" in <strong>the</strong> open ocean extend <strong>to</strong> depthsof 200 meters, <strong>with</strong> <strong>the</strong> degree of turbulence measured byScully-Power from <strong>the</strong> Kimbla, <strong>the</strong>y possibly represent acousticdiscontinuities as substantial as those in meso-scale eddies.Any knowledge of <strong>the</strong>ir generation, distribution, and life his<strong>to</strong>riesis clearly more than academic.Actually, little more is unders<strong>to</strong>od about <strong>the</strong> nature ofchaotic wave-lines than was known in <strong>the</strong> early 1 980s, o<strong>the</strong>rthan <strong>the</strong>ir distribution. Russian oceanographers have done <strong>the</strong>most work on this strange state of <strong>the</strong> sea, giving it <strong>the</strong> name of"suloy." The fullest description of suloys was made by <strong>the</strong> lateDr. Konstantin Fedorov in his 1983 book on The Physical Natureand Structure of Oceanic Fronts. In it, Fedorov documents<strong>the</strong> regions of <strong>the</strong> oceans in which suloys are most often encountered,and <strong>the</strong> variety of ocean conditions under whichsuloys may occur, such as tides, a convergence of currents, a<strong>to</strong>ceanic fronts, or a<strong>to</strong>p internal waves. "Wherever," he notes,"<strong>the</strong> dynamics of <strong>the</strong> near-surface ocean cause a convergence,<strong>the</strong>re is a suloy."Tidal suloys are readily explained, because <strong>the</strong>y occur whenstrong tidal currents enter <strong>the</strong> shallow water of narrow straits.A line of precipi<strong>to</strong>us waves, a suloy, is formed at <strong>the</strong> front of<strong>the</strong> tidal surge as it meets, and converges <strong>with</strong>, <strong>the</strong> surfacewind waves. The precipi<strong>to</strong>us chaotic waves in suloys mayattain heights of 5 m (see pho<strong>to</strong>, p. 41). West of San Francisco'sGolden Gate, waves in <strong>the</strong> Point Bonita suloy can becomeso intense that even moderate-size ships have requiredmore than one attempt <strong>to</strong> sail through <strong>the</strong> roaring wave line.Suloys arise also where <strong>the</strong> strong discharge from majorrivers converge on waters of <strong>the</strong> coastal ocean. Such featureshave been observed on several occasions by astronauts inContinued from page 39lands are bright and sharp. In <strong>the</strong> next instant, <strong>the</strong>y recognizewhitecaps and foam streaks on <strong>the</strong> sea.Visual observations and pho<strong>to</strong>graphy of whitecaps areclearly not suitable <strong>to</strong> learn <strong>the</strong> extent <strong>to</strong> which <strong>the</strong>ycover <strong>the</strong> world's sea surface at any given time. Yet, thatknowledge is key <strong>to</strong> <strong>the</strong> determination of wind speedsand directions from Earth-orbiting, satellite-bornemicrowave scatterometers. Whitecaps and foam greatlyinfluence <strong>the</strong> microwave emissivity of <strong>the</strong> ocean. Themagnitude and variability of this emissivity change is notyet resolved."We continue <strong>to</strong> observe 'corduroy' and 'herringbone'seas in every part of <strong>the</strong> ocean where <strong>the</strong> Sun's glitter givesus a good look at <strong>the</strong> surface," reported Skylab astronauts,Cols. Gerald Carr and William Pogue, and Dr. Edward Gibson,in January 1974, indicating <strong>the</strong>ir ease in observing majorocean swell patterns. The "corduroy" seas are <strong>the</strong> resul<strong>to</strong>f parallel swell, while <strong>the</strong> "herringbone" seas are <strong>the</strong> resul<strong>to</strong>f swell crossing each o<strong>the</strong>r at oblique angles.Ocean Swell. When wind waves leave <strong>the</strong> area of generation,<strong>the</strong> sea ceases <strong>to</strong> be random and <strong>the</strong> dominant waveperiod and direction of propagation take over. The sharppeaks of wind-waves flatten, <strong>the</strong> height decreases, and aregular pattern of parallel crests appears as <strong>the</strong> waves aretransformed in<strong>to</strong> swell. As <strong>the</strong> swell travel onward—throughthousands of kilometers of ocean if no land intervenes—<strong>the</strong>longest lengths and greatest periods, predominate. Crestlengths may grow <strong>to</strong> thousands of meters and become extraordinarilyparallel <strong>to</strong> each o<strong>the</strong>r. These are <strong>the</strong> corduroyseas visible from space in <strong>the</strong> great expanses of <strong>the</strong> oceans(see pho<strong>to</strong>, p. 43, bot<strong>to</strong>m left).Swell from more than one s<strong>to</strong>rm-generating region, ororiginating simultaneously from s<strong>to</strong>rmy oceans in <strong>the</strong> Nor<strong>the</strong>rnand Sou<strong>the</strong>rn hemispheres, may eventually intersecteach o<strong>the</strong>r. In such parts of <strong>the</strong> ocean, commonly near <strong>the</strong>Equa<strong>to</strong>r, <strong>the</strong> intersecting swell form <strong>the</strong> "herringbone seas"that were observed first by <strong>the</strong> Skylab-4 crew, but subsequentlyon innumerable occasions by astronauts aboard <strong>the</strong>Space Shuttle (see pho<strong>to</strong>, p. 43, <strong>to</strong>p right).Breakers, Surf, and Refraction. When a wave approaches<strong>the</strong> shore, its crest moves faster than <strong>the</strong> trough, responding<strong>to</strong> <strong>the</strong> friction exerted by <strong>the</strong> sea floor. At <strong>the</strong> moment when<strong>the</strong> velocity of water particles in <strong>the</strong> crest exceeds <strong>the</strong> forwardspeed of <strong>the</strong> wave form, <strong>the</strong> wave "breaks." The cres<strong>to</strong>vertakes <strong>the</strong> trough at this stage, <strong>the</strong> leading slope of <strong>the</strong>wave becomes steeper than <strong>the</strong> trailing side, and <strong>the</strong> <strong>to</strong>p of<strong>the</strong> wave cascades down <strong>the</strong> steep slope, forming <strong>the</strong> "surfzone."Waves tend <strong>to</strong> form "plunging breakers" where bot<strong>to</strong>mslopes <strong>to</strong> <strong>the</strong> beach are relatively steep. These are <strong>the</strong> spectacular"curling" breakers, in which <strong>the</strong> crests literally collapseon<strong>to</strong> <strong>the</strong> steep, forward slope of <strong>the</strong> breaking wave.Where better <strong>to</strong> see <strong>the</strong>se crashing giants than at SunsetBeach on <strong>the</strong> north shore of Oahu in winter? They are <strong>the</strong>professional surfers' joy; <strong>the</strong> amateurs' continuous "hangten" disasters (see pho<strong>to</strong>, p. 43, bot<strong>to</strong>m right).Continued on page 4542 Summer 1 999 21st CENTURY

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