The Ocean Basins' Their Structure And Evolution

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THE OCEAN BASINS'THEIR STRUCTURE AND EVOLUTION

THE OCEANOGRAPHYCOURSETEAMAuthorsEvelyn Brown (Waves, Tides, etc.; Ocean Chemistry)Angela Coiling (Ocean Circulation; Seawater (2nd edn); Case Studies)Dave Park (Waves, Tides, etc.)John Phillips (Case Studies)Dave Rothery (Ocean Basins)John Wright (Ocean Basins; Seawater; Ocean Chemistr3,; Case Studies)DesignerJane SheppardGraphic ArtistSue DobsonCartographerRay MunnsEditorGerry BearmanThis Volume forms part of an Open University course. For generalavailability of all the Volumes in the Oceanography Series, please contactyour regular supplier, or in case of difficulty the appropriate ButterworthHeinemann office.Further information on Open University courses may be obtained from:The Admissions Office, The Open University, P.O. Box 48, Walton Hall,Milton Keynes MK7 6AA, UK, or from the Open University website:http://w w w. ope n. ac. ukCover illustration: Satellite image showing distribution of phytoplanktonpigments in the North Atlantic off the US coast in the region of the GulfStream and the Labrador Current. (NASA, and O. Brown andR. Evans, Universit3, of Miami.)

THE OCEAN BASINS'THEIR STRUCTURE AND EVOLUTIONPREPARED BY JOHN WRIGHT AND DAVID A. ROTHERY FOR THE COURSE TEAMSECOND EDITION REVISED FOR THE COURSE TEAM BY DAVID A. ROTHERYU T T E R W O R T HE I N E M A N Nin association withTHE OPEN UNIVERSITY, WALTON HALL,MILTON KEYNES, MK7 6AA, ENGLAND

Butterworth-HeinemannLinacre House, Jordan Hill, Oxford OX2 8DPA division of Reed Educational and Professional Publishing Ltd- Amember of the Reed Elsevier plc groupOXFORD AUCKLAND BOSTONMELBOURNE NEW DELHIJOHANNESBURGCopyright 9 1989, 1998 The Open UniversityFirst edition 1989Second edition 1998. Reprinted (with corrections) 2001, 2003, 2004All rights reserved; no part of this publication may be reproduced, stored in aretrieval system, or transmitted in any form or by any means, electronic,mechanical, photocopying, recording, or otherwise without the prior writtenpermission of the copyright holder except in accordance with the provisions of theCopyright, Designs and Patents Act 1988 or under the terms of a licence permittingrestricted copying issued by the Copyright Licensing Agency, 90 Tottenham CourtRoad, London W IP 0LP. This book may not be lent, resold, hired out or otherwisedisposed of by way of trade in any form of binding or cover other than that inwhich it is published, without the prior consent of the Publishers.British Library Cataloguing in Publication DataA catalogue record for this book is available from the British Library.ISBN 0 7506 3983 0Library of Congress Cataloguing in Publication DataA catalogue record for this book is available from the Library of Congress.Jointly published by the Open University, Walton Hall, Milton KeynesMK7 6AA and Butterworth-Heinemann.Edited, typeset, illustrated and designed by The Open UniversityPrinted in Singapore by Kyodo under the supervision of MRMGraphics Ltd., UKs330vli2.4

ABOUTTHIS VOLUME3ABOUTTHIS SERIES3CHAPTER 1 INTRODUCTION1.11.1.11.1.2MAPPING THE OCEANSNavigationDepth measurement59111.21.2.1MAPPING THE OCEANFLOORSBathymetry from satellites13181.3UNDERWATERGEOLOGY221.4SUMMARY OF CHAPTER125CHAPTER 2 THE SHAPE OF OCEAN BASINSTHE MAIN FEATURESOF ic continental marginsSeismic continental margins and island arcs3031332.32.3.12.3.2OCEANRIDGESRidge topographyAge-depth relationships across ridges353637TRANSFORM FAULTSAND FRACTUREZONES38THE DEEPOCEANFLOORAbyssal plainsSeamountsThe distribution of submarine volcanoesAseismic ridges41414243452.6SATELLITEBATHYMETRY-A CASESTUDY452.7SUMMARY OF CHAPTER2522.12.42.52.5.12.5.22.5.32.5.4CHAPTER 3 THE EVOLUTION OF OCEAN BASINSTHE EVOLUTIONOF OCEANBASINS553.23.2.1THE BIRTH OF AN OCEANThe Red Sea58593.33.3.1THE MAJOROCEANBASINSThe Mediterranean6266SUMMARY OF CHAPTER3673.13.4CHAPTER 4 THE STRUCTURE AND FORMATION OFOCEANIC LITHOSPHERE4.14.1.14.1.24.1.3THE FORMATIONOF OCEANICLITHOSPHEREPillow lavas: the top of the oceanic crustWhy a median valley?Formation of the volcanic layer: two case ATIONOF OCEANICSPREADINGAXESSecond- and third-order segmentation of fast-spreading axesSecond- and third-order segmentation of slow-spreading axesA plausible model for lithospheric growthChanges in spreading patternCrustal abnormalities8384878889894.3SEAMOUNTSAND VOLCANICISLANDS924.4SUMMARY OF CHAPTER494

CHAPTER 5 HYDROTHERMAL CIRCULATION IN OCEANICCRUST5.15.1.1THE NATUREOF HYDROTHERMALCIRCULATIONHeat flow, convection and permeability5.25.2.15.2.25.2.3CHEMICAL CHANGESDURING HYDROTHERMALCIRCULATIONChanges in the rocksChanges in seawaterVariability in hydrothermal systems1001011031055.35.3.15.3.25.3.3BLACKSMOKERS- AN EXERCISEIN PREDICTIONBlack smokers, white smokers and warm-water ventsThe lifetimes of hydrothermal systemsAnatomy of a vent field1061071101115.45.4.15.4.25.4.35.4.45.4.5THE EXTENTOF HYDROTHERMALACTIVITYThe biological significance of hydrothermal vent systemsHydrothermal plumesEvent plumesOff-axis hydrothermal circulationThe extent of hydrothermal metamorphism1121151151171181205.5MASS TRANSFERBY HYDROTHERMALCIRCULATION1205.6SUMMARY OF CHAPTER51229899CHAPTER 6 PALAEOCEANOGRAPHYAND SEA-LEVELCHANGES6.16.1.1THE DISTRIBUTIONOF SEDIMENTSSediments and 56.2.66.2.76.2.86.2.9CHANGESIN SEA-LEVELDifferent time-scales in sea-level changesUsing satellites to monitor sea-level changesThe post-glacial rise in sea-levelMeasuring Quaternary changes in sea-levelThe growth of an ice-sheet: AntarcticaThe salinity crisis in the MediterraneanThe migration of climatic beltsThe effect of plate-tectonic processes on sea-levelMajor transgressions and regressions129130131135136140142146147148SUMMARY OF CHAPTER61496.3CHAPTER 7 THE BROADERPICTURETHE GLOBALCYCLEChanges in components of the cycleSome effects of short-term changesThe steady-state ocean1511541551567.2SOME RATESCOMPARED1577.3SUMMARY OF CHAPTER71587.17.1.17.1.27.1.3APPENDIX THE STRATIGRAPHICCOLUMN160SUGGESTED FURTHER READING161ANSWERS AND COMMENTS TO QUESTIONS162ACKNOWLEDGEMENTS179INDEX181

This is one of a Series of Volumes on Oceanography. It is designed so that itcan be read on its own, like any other textbook, or studied as part of 330Oceanography, a third level course for Open University students. Thescience of oceanography as a whole is multidisciplinary. However, differentaspects fall naturally within the scope of one or other of the major'traditional' disciplines. Thus, you will get the most out of this Volume ifyou have some previous experience of studying geology, geochemistry orgeophysics. Other Volumes in this Series lie more within the fields ofphysics, chemistry and biology (and their associated sub-branches).Chapters l to 4 describe the processes that shape the ocean basins,determine the structure and composition of oceanic crust and control themajor features of continental margins. Today's ocean basins aregeologically ephemeral features, and these Chapters show why. Chapter 5deals with the 'hot springs' of the deep oceans that result from thecirculation of heated seawater through oceanic crust. This phenomenon wasnot even suspected until the mid-1960s and was not confirmed byobservation until some years later. Since then, many people have seen thestriking photographs of 'black smokers' at ocean ridges. Chapter 6summarizes the main patterns of sediment distribution in the ocean basinsand shows how sediments can preserve a record of past climatic and sealevel changes. Finally, Chapter 7 considers the role of the oceans as anintegral part of global chemical cycles.You will find questions designed to help you to develop arguments and/ortest your own understanding as you read, with answers provided at the backof the Volume. Important technical terms are printed in bold type wherethey are first introduced or defined.The Volumes in this Series are all presented in the same style and format,and together provide a comprehensive introduction to marine science.Ocean Basins deals with the structure and formation of oceanic crust,hydrothermal circulation, and factors affecting sea-level. Seawaterconsiders the seawater solution and leads naturally into Ocean Circulation,which is the 'core' of the Series. It provides a largely non-mathematicaltreatment of ocean-atmosphere interaction and the dynamics of winddriven surface current systems, and of density-driven circulation in the deepoceans. Waves, Tides and Shallow-Water Processes introduces the physicalprocesses which control water movement and sediment transport in thenearshore environment (beaches, estuaries, deltas, shelves). OceanChemistry and Deep-Sea Sediments is concerned with biogeochemicalcycling of elements within the seawater solution and with water-sedimentinteraction on the ocean floor. Case Studies in Oceanography and MarineAffairs examines the effect of human intervention in the marineenvironment and introduces the essentials of Law of the Sea. The two casestudies respectively review marine affairs in the Arctic from an historicalstandpoint, and outline the causes and effects of the tropical climaticphenomenon known as E1 Nifio.

Biological Oceanography: An Introduction (by C. M. Lalli and T. R.Parsons) is a companion Volume to the Series, and is also in the same styleand format. It describes and explains interactions between marine plants andanimals in relation to the physical/chemical properties and dynamicbehaviour of the seawater in which they live.

55IMPORTANT: In this Chapter you willfind frequent reference to the divisionsof the geological time-scale. This isshown in the Appendix.The Earth's oldest r o c k s - around 3850 Ma o l d - include both water-lainsediments and evidence of ancient oceanic crust. It follows that oceans havebeen forming since the beginning of the geological record, and probablybefore that. However, the shape of most past ocean basins has to be workedout from observations of remnants preserved in continental areas. That isbecause ocean basins are relatively short-liv d features of this planet: nooceanic crust older than about 180 Ma is known from the present oceans.If we take the life cycle of a large ocean basin to average about 200 Ma, howmany times could such basins have been formed since 3800 Ma ago?The exact answer is 19, but because our figure of 200 Ma is only a crudeguess and we do not know how rates of plate-tectonic processes in the distantgeological past compared with those of the present, it is wiser to give anapproximate figure of 15-20 times. This is probably a minimum, for theEarth's interior was a good deal hotter in the past than it is now, and theturnover of oceanic lithosphere could have been more rapid.That simple calculation was designed only to give you a feeling for the timescale of evolution of individual ocean basins, and it is obviously somewhatartificial. In the past, as one ocean basin expanded, another must havecontracted, just as the Atlantic and Pacific are doing today. Thus, there isalways some overlap in the history of different basins. Continents and oceanbasins are continually changing their shapes and relative positions at ratesthat are geologically very rapid and are not slow even on human time-scales.The speed of sea-floor spreading has been compared with that of growingfingernails. Since the compilation of the first maps to cover any appreciablearea of ocean, around five centuries ago, the Atlantic coasts have drawn apartfrom each other by about 10-20 m. This is a substantial movement, eventhough it represents only 0.0003% of the width of the ocean. Spreading ratesin parts of the Pacific are several times greater than in the Atlantic.An individual ocean basin grows from an initial rift, reaches a maximumsize, then shrinks and ultimately closes completely. Stages in this cycle aresummarized in Table 3.1 (overleaf) and briefly reviewed below.Whether or not the East African rift valleys really are an incipient oceanbasin (Stage 1) and eastern Africa will eventually be split apart is debatable.Nevertheless, such rift valleys must develop along the line of continentalseparation. When separation does occur, sediments from the adjacentcontinents soon begin to build out into the new basin and will become part ofthe eventual continental shelf-slope-rise zone. As the spreading axismigrates away from the marginal areas, the continents become increasinglydistant and so the sediment supply dwindles (Stage 2). The ocean floorbetween the spreading axis and the continent subsides by thermal contractionof the underlying lithosphere (Figure 2.13), abyssal plains form, and thecontinental shelf-slope-rise zone becomes fully developed. The continentalmargins are more or less parallel to the central spreading ridge, as in theAtlantic (Stage 3).

56Table 3.1StageDominant motionsCharacteristic features1 embryonic East Africanrift valleys2 youngRed Sea, Gulfof California3 matureAtlantic Oceancrustal extensionand upliftsubsidence andspreadingspreadingrift valleys4 decliningPacific Oceanspreading andshrinking5 terminalMediterraneanSeaIndus suture inthe Himalayasshrinking andupliftshrinking anduplift6 relict scarFigure 3.1 Palaeogeographicreconstruction,compiled from topographic, palaeoclimatic andpalaeomagnetic data. Panthalassa was the hugeocean that dominated one hemisphere. Pangeawas the supercontinent in the other hemisphere,of which Eurasia and Gondwanaland were twocomponents. (a) Jurassic, about 170 Ma ago.(b) Cretaceous, about 100 Ma ago. (c) Eocene,about 50 Ma ago. The maps show present-daycoastlines for ease of reference. Ancientcoastlines did not coincide with these.Stages in the evolution of ocean basins, with examples.Examplesnarrow seas with parallelcoasts and a central depressionocean basin with activemid-ocean ridgeocean basin with activespreading axes; also numerousisland arcs and adjacenttrenches around marginsyoung mountainsyoung mountainsStage 4 involves the development of one or more destructive plate margins.The reason for the formation of new destructive margins probably lies inchanging circumstances in another part of the globe, such as continentalcollision or the initiation of new continental rifting. If (as seems certain) theEarth is neither expanding nor contracting, the net rates of spreading andsubduction over any great circle on the Earth must be equal, and the patternof plates and plate motion must adjust to keep this so.The Mediterranean is an ocean in the final stages of its life (Stage 5), withthe African Plate being consumed under the European Plate. Unless theworld system of plates changes so as to halt the northward movement ofAfrica relative to Europe, the continental blocks of Europe and Africa willeventually collide, and new mountain ranges will form (Stage 6).

57

583.2THE BIRTH OF AN OCEANFigure 3.2 summarizes the development of a new ocean basin. During crustalextension, the ductile lower part of the crust is stretched, but the brittle upperFigure 3.2 Diagrams illustrating how a new ocean basin may form.(a) The surface of the stretched and rifted region is still above sea-level and may even beuplifted as a result of thermal expansion because of a heat source at the site of the futurespreading axis. Terrigenous sediments (i.e. those derived from erosion on land) occupy the riftvalley.(b) The future continental margins have thinned enough to subside below sea-level and marinesedimentation has begun. Sediments thicken away from the new spreading axis.(c) Separation is complete, a new spreading ridge has developed, and a shelf-slope-rise zone isforming (cf. Figure 2.6).

59part is rifted. Blocks of crust slide down fault planes, and sedimentsaccumulate in the lakes and valleys which occupy the resultingdepressions. When separation occurs, basaltic magma rises to fill the gapbetween the two continental blocks. Because the resulting new oceaniccrust is both thinner and denser than continental crust, it lies below sealevel. The remainder of the lithosphere, below the crust, is composed ofupper mantle material.Initially, the young marine basin is fairly shallow. If repeated influxes ofseawater become wholly or partly evaporated, salt deposits (evaporites)will accumulate. Otherwise, there will be normal marine sedimentation ofmuds, sands and limestones, depending on local conditions. One of theclearest examples of a young ocean basin is the Red Sea.3.2.1THE RED SEAIn the Red Sea, a narrow deep axial zone is flanked on either side by abroad shallow area of shelf sea (Figure 3.3(a)). Evaporites of Miocene age(deposited between about 20 and 5 Ma ago) that are over 4 km thick inplaces underlie the shallower waters of these flanking regions. Theyobscure the nature of the crust beneath, which appears to be thinned andstretched continental crust (Figure 3.3(b)).Figure 3.3 (a) Outline map of the Red Sea,with the axial zone (dark blue) defined by the500-fathom isobath and subdivided into fourmain sections, described in the text (1 fathom 6 feet 1.83 m).(b) Highly schematic cross-section through theRed Sea.The evaporites were deposited at a time when the only marine connectionto the Red Sea was with the Mediterranean by an intermittent, shallow,seaway. Evaporite deposition ended about 5 Ma ago at the end of theMiocene when this seaway was finally broken and a new connection withthe Indian Ocean was opened in the south. Open water conditions wereestablished, in which planktonic organisms flourished, especially in thesouthern Red Sea. High rates of biogenic (biologically derived)sedimentation caused bathymetric features to be smothered, and theybecome much less obvious south of about 16 N.Further north, the post-Miocene biogenic sediments give way to a thinnersequence of terrigenous (land-derived) clays, sands and gravels, producedby erosion of the flanks of the basin. Similar terrigenous sediments can alsobe found interbedded with the Miocene evaporites, especially near themargins.Only in the axial zone, which represents that part of the Red Sea generatedsince the end of evaporite deposition, do we find true oceanic crustproduced by sea-floor spreading. On the basis of seismic and magneticsurveys, submersible observations and side-scan sonar mapping, the axialzone can be subdivided into several regions along its length (Figure 3.3(a))as described below.

60Rift valley regionThe southern part of the axial trough is now known to have a well-developedstraight central rift (similar to that on the Mid-Atlantic Ridge; Figure 2.12),which is offset by 3-10 km about every 30-50 km. These discontinuities maybe either transform faults or some sort of non-transform offset.High-amplitude linear magnetic anomalies occur throughout this region,though they become weak and irregular at the offsets. Measurements of themagnetic anomaly stripes indicate that spreading has proceeded at a rate ofabout 0.8 cm yr - for the past 5 Ma.Multi-deeps regionNorth of about 20 N, the straight axial rift loses its identity and is replacedby a complex series of axial deeps, distributed partly in an en e c h e l o nfashion, perhaps because of offsets by transform faults. The deeps are bestdeveloped between about 20 N and 22 N and they have attractedcommercial interest on account of the metal-rich hot brines and muds whichsome of them contain (Figure 3.4). Individual deeps have a tiff-valley typestructure with strong magnetic anomalies, but between the deeps theanomalies are much weaker and the axial region is sediment-covered.Figure 3.4 Bathymetric details of some major'deeps' in the multi-deeps region of Figure 3.3(a).Hot, metal-rich brines are found in them, andmetalliferous muds are being deposited there.Depths are given in metres.Transitional and northern regionsBeyond about 22 N, the deeps become progressively narrower and lesswell developed, and the associated magnetic anomalies suggest that theoceanic crust in them may be only 2 Ma old or less. North of about 25 N,only isolated deeps are found, the high-amplitude magnetic anomaliescharacteristic of oceanic crust which occur further south have virtuallydisappeared, and the region appears to have a more or less continuoussediment cover.In summary, then, only about 80 km width (2 x 5 x 106 0.8 10.2 m) ofnew ocean floor up to 5 Ma old can be demonstrated to have formed in thesouthern part of the axial zone: further north, ocean floor has formed onlyin the deeps and is 2 Ma old or less.All of this suggests strongly that the axial zone of the Red Sea is anorthward-propagating zone of separation between adjacent plates ofcontinental lithosphere. The fracture began to open properly about 5 Ma agoin the south but has yet to do so in the north. This is consistent with the endof evaporite deposition in the Red Sea about 5 Ma ago, when a link with theIndian Ocean was established via the Gulf of Aden.But what about the crust outside the axial region of the Red Sea? Figure 3.5shows magnetic anomalies in the southern Red Sea. The well-defined axialanomalies that are characteristic of true oceanic crust give way to anirregular and much weaker pattern in the flanking regions. This is consistentwith thinned and stretched continental crust, injected by thin vertical sheetsof basaltic rock (dykes).From a variety of geological evidence, it is clear that this stretching andsubsidence of the continental crust pre-dates the sea-floor spreading in whatbecame the Red Sea. It seems likely that the first stage, about 35 Ma ago,was the propagation of a crack from the Arabian Sea westward through theGulf of Aden. By about 25 Ma ago, east-west extension had begun to befelt across the entire area of the Red Sea (from its junction with the Gulf ofAden northwards as far as the Gulf of Suez), and was manifested by thedevelopment of a rift system within the continental crust. A new fracture

61W1000nT5010050kmI l l I BE !11114.5IIIIIPliocene/Ma0 4.511I1II PleistocenePlioceneFigure 3.5 Magnetic anomalies for the southern Red Sea, showing the contrast between thestrong central pattern over the axial trough and the subdued pattern on either side. For thisprofile, correlation with the magnetic reversal time-scale (black normal polarity; white reverse polarity) gives an average full spreading rate of 1.5 cm yr-1 over the past 4.5 Ma. Themagnetic field is measured in nT (nT nanotesla 10-9T).developed in the north along what is now the Gulf of Aqaba/Dead Sea line,running towards the north-north-east. Transcurrent (lateral) movement alongthis line accompanied further widening of both the Gulf of Aden and the RedSea as Arabia moved away from Africa. Oceanic crust formed in the Gulf ofAden. About this time there was widespread extension-related volcanism inthe western parts of what are now the Yemen, Saudi Arabia, Eritrea, andnorthern Ethiopia.Along the Red Sea rift, the continental crust continued to stretch andsubside, and evaporites were deposited on top of it. About 5 Ma ago thesystem was reactivated when movement was renewed along the Gulf ofAqaba/Dead Sea line. The continental crust was already so fully stretchedthat rather than thinning and stretching even further it was pulled apart, andsea-floor spreading began here for the first time, while continuing in theGulf of Aden.The opening of the Red Sea as a new ocean was clearly a drawn-out andcomplicated affair, and we should bear in mind that the opening stages ofother ocean basins are likely to have been similarly complex. However, wemust now move on to consider larger ocean basins that have reached Stage 3or 4 of Table 3.1, beating in mind that in the early stages of formation, theyprobably resembled the Red Sea.

62Figure 3.6 summarizes the age distribution of oceanic crust beneath theworld's oceans, as determined from magnetic anomaly patterns. The virtuallysymmetrical pattern of ages about the ocean ridges is visible everywhere, andit is clear that (apart from the Caribbean area and in the extreme south-west)the Atlantic has had the least complicated evolution of any of the three mainocean basins. The Pacific and Indian Oceans display more complex histories,partly because of the development of major subduction zones along one ormore boundaries and partly because of adjustments in spreading direction.From Figure 3.6, it is relatively easy to reconstruct stages in disruption of thecontinental jigsaw puzzle that led to the present-day Atlantic. It is simply amatter of moving the continents back along the transform faults to determinethe positions of their margins at any particular time, as represented by the ageof the ocean floor magnetic stripes.The Pacific and Indian Oceans are more difficult to 'close up'. The Pacific isalmost surrounded by subduction zones, so much of the evidence of its olderhistory has disappeared. The widths of the ocean floor age strips increasenorthwards along the line of the East Pacific Rise in a way that is consistentwith increasing spreading rates from south to north. However, the EastPacific Rise runs into the North American continent, beneath which itsnorthern end is being subducted.You have already seen evidence of changes in spreading direction in thenorth-western Pacific (Figure 2.22), and more evidence is to be seen in thepattern of ocean floor ages in Figure 3.6.The East Pacific Rise must have been moving relative to the frame ofreference provided by the Hawaiian and similar chains (the 'hot-spotreference frame'). It is important for you to realize that magnetic anomalies,and the sea-floor age strips which can be mapped using them, record only themotion relative to the spreading axis at which the sea-floor was formed. It isquite possible for the spreading axis itself to be migrating relative to the deepEarth. In fact, it is impossible to have several spreading axes on a sphere andkeep them all stationary, unless the plate motion at each one is individuallyand exactly compensated for by nearby destructive plate margins. Thus, aspreading axis can migrate across an ocean basin, and will be destroyed if itgets carried into a subduction zone. Figure 3.7 (overleaf) shows how theglobal plate boundaries are thought to have evolved over the past 61 Mabased on the types of data you have read about in this and the previousChapter, especially hot-spot traces and magnetic anomaly patterns.

Figure 3.6 The age of the ocean floor, showing strips of floor of different ages derived mainly from measurements of magnetic anomaly stripes. Boundaries are drawn at 2, 4, 9, 20, 35,52, 65, 80, 95, 110, 120, 140 and 160 Ma intervals in a colour scheme that runs from dark grey (youngest) through red, yellow, and green to blue (oldest). Pale brown areas are thecontinental shelves.

64Figure 3.7 Evolutionof plate boundaries overthe past 61 Ma. The arrows show the directionsand relative rates of motion of the plates.The oldest oceanic crust in the Pacific is found in the north-west, but thewestern Pacific as a whole is an area of great complexity. This is because ofthe generation of new oceanic lithosphere at various spreading axes abovesubduction zones, where island arcs are being built and then split apart, andback arc basins are forming, as outlined in Section 2.2.2 and illustrated inFigure 3.8. These events occur independently of sea-floor generation at theEast Pacific Rise.In the Pacific, there is an added complication when it comes toreconstruction of the continental jigsaw puzzle. Palaeomagnetic, geological

65Figure 3.8 A schematic cross-section through atypical western Pacific continental margin. Asmall spreading axis has generated new oceaniccrust behind the island arc. In some places, aneven more complex series of island arcs and backarc basins separates the deep ocean trench fromthe continental margin.and palaeontological evidence have demonstrated that substantial tracts ofwestern North America are 'exotic terranes'. These are blocks of continentalc r u s t - microcontinents - that have been transported by plate movements forgreat distances across the Pacific to become accreted onto North America.The Indian Ocean has several features of interest, too. Its northern boundary isa major complex subduction zone, represented by the Himalayan belt and theJava Trench system. South of India, the spreading direction changed fromnorth-south to north-east-south-west about 50 Ma ago when the presentSouth-east Indian Ridge became established.The aseismic Ninety-east Ridge (Section 2.5.4) must lie on the line of an oldmajor transform fault, for the age of the crust changes in opposite directionson either side of it, as can be seen in Figure 3.6.You can find other examples of changes of spreading rate and direction, anddevelopment of new spreading axes and subduction zones, displayed in Figure3.6. You may also have noticed that many of the ocean floor age strips areoblique to subduction zones, e.g. in the north-east Indian Ocean and parts ofthe western Pacific. Oblique subduction of ocean floor is by no meansexceptional, and it means that continent-continent or continent-island arccollision does not necessarily occur head-on, and so major transcurrentfaulting may result.In the major ocean basins, irrespective of whether they are classified as Stage3 or 4 in Table 3.1, there is no indication that increasing age is correlated withany decline in the intensity of sea-floor spreading activity. The Pacific basin isthe oldest, for instance, but it has the fastest spreading rates. When we cometo Stage 5, we find that even in the latest stages of evolution, there is littlediminution of vigour.

663.3.1THE MEDITERRANEANThe Mediterranean can be classified as an ocean in the final stages of itslife cycle, the only major remnant of the once-extensive Tethys Ocean(Table 3.1, Stage 5; Figure 3.1). The Mediterranean is shrinking as theAfrican Plate continues to thrust its way northwards beneath the Europ

THE OCEANOGRAPHY COURSE TEAM Authors Evelyn Brown (Waves, Tides, etc.; Ocean Chemistry) Angela Coiling (Ocean Circulation; Seawater (2nd edn); Case Studies) Dave Park (Waves, Tides, etc.) John Phillips (Case Studies) Dave Rothery (Ocean Basins) John Wright (Ocean Basins; Seawater; Ocean Chemistr3,; Case Studies) Designer Jane Sheppard Graphic Artist

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