Ocean Crustal Magnetization and Magnetic...

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Ocean Crustal Magnetization and Magnetic Anomalies Anomaly and magnetization basics Lavas as largest magnetic source – what controls their magnetization? Do lower crustal layers contribute? Magnetic anomalies and plate reconstructions Skewness poles and anomalous skewness How does crustal accretion affect magnetization source and anomalies? Vector magnetic anomalies Does the ocean crust record intensity variations?

Transcript of Ocean Crustal Magnetization and Magnetic...

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OceanCrustalMagnetizationandMagneticAnomalies

• Anomalyandmagnetizationbasics• Lavasaslargestmagneticsource– whatcontrolstheirmagnetization?

• Dolowercrustallayerscontribute?• Magneticanomaliesandplatereconstructions• Skewness polesandanomalousskewness• Howdoescrustalaccretionaffectmagnetizationsourceandanomalies?

• Vectormagneticanomalies• Doestheoceancrustrecordintensityvariations?

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AnomalyBasics

• Earthfilter:shorterwavelengthsmoreattenuated

• Geomagneticsignalincludesbothdirectionandintensity

• Crustalaccretionprocessesasfilter

Sourcemagnetizationandseasurfaceandnearbottomanomaliesgeneratedatpole(i.e.withremanence andambientfieldbothvertical).55km/m.y.halfspreadingrate.

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• Shape(skewness)ofanomaliesdependsongeometryofspreadinglineation,Mdir,Bdir

• Skewness =phaseshifttomakesimilartopatternatpole

• Anomalousskewness =notpredictedbygeometry

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MagneticMinerals

• Twopropertiesofmagneticmaterials(ferromagnets)– LongrangeorderingbelowCurietemperature

– Magnetichysteresis=magnetizationisafunctionoffieldhistory

• Curietemperatureisafunctionofmineralogy

• Magneticpropertiesastrongfunctionofgrainsize

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Thermoremanent Magnetization

• Magnetizationofoceancrustisprimarilythermalinorigin

• Duringcooling,thermalenergydecreasesandanisotropybarriersincrease

• Smallparticles(<micron)arethemoststable

Tauxe (2010)

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LavasasDominantSource

• Thinextrusivelayerisdominantsource

• AlongaxisprofilefitwithNmagnetizedbathymetry

• Crossaxisprofiletodeterminelayerthickness(~400m)

Talwani etal.(1971)

RidgeparallelprofileoverRcrustshowsnegativecorrelationwithtopography.

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MagneticGrainSize&Remanence

• Coolingatpillow/flowmarginsresultsinlargegradientingrainsize

• Smallestmagneticgrains(nearmargin)havelargestmagnetization

• Compositionoflargetitanomagnetites (TM60)butmorevariablenearmargin

afterKent&Gee(1996);Zhouetal.(2000)

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Remanence andGeochemistry

• Fractionationofmeltinshallowmagmachambers(FeO*increases)

• HigherFeO*shouldresultinmoretitanomagnetiteandhighermagnetization(magnetictelechemistry)

• SignatureofhigherFeatwakesofpropagatingrifts(andnearfracturezones)

Carbotte &Macdonald(1992)

Magnetizationpattern9-10°NonEPR.Maximum~40A/m.

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MagneticTelechemistry

• Magnetizationofaxiallavasdeterminedfromslabsperpendiculartochilledmargin

• Reasonablecorrelation(R=0.81)forFeO*&NRM

• Alongaxismagneticanomalyvariationsgenerallymatchsamplegeochemistry

afterGee&Kent(1997,1998)

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Variationsinmagnetization(calculatedfromanomalydata)arebestmodeledbylavathicknessvariations

Williamsetal.(2008)

Along-AxisMagnetizationVariations

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TemporalChangesinMagnetization

• Anomalyamplitudesandsampleremanence higheratridge

• AttributedtolowToxidationoftitanomagnetite

sampleNRMdatafromIrving(1970) oxidizedTM(fromFuruta,1993)

CrackinginlargetitanomagnetitetypicaloflowToxidation

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SpreadingRateDependence

Gee&Kent(2007)

Largedecreaseinamplitudeanomalyoff-axisconfinedtofullspreadingrateslessthanabout30km/m.y.

CentralAnomalynotsuchapronouncedfeatureatfasterspreadingrates.

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EvidenceforLow-TAlteration

datafromWangetal.(2005,2006),Zhouetal.(2001)

• DirectdeterminationofoxidationstateofTMgrainsbyTEM

• Veryheterogeneousoxidation,withlowvaluesatoldestseafloor

Oxidationparametermeasuredonseafloorlavas.Avalueof1correspondstocompleteoxidationandwouldbeassociatedwitha4xreductioninmagnetization.

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TemporalMagnetizationChanges

Gee&Kent(2007)Age(Ma)

DrillsiteswithlargenhavelowerNRMthanaxialdredgesbutnosystematicchangewithage.

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AlterationandAnomalyAmplitudes

Gee&Kent(2007)

A2xto4xalteration-relatedreductioninmagnetizationiscompatiblewithslowandfastspreadprofiles.Thetimescaleofalterationispoorlydefined.

fullrate80km/m.y. fullrate20km/m.y.

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MagnetizationofSheetedDikes

• Remanence indikes~5xlowerthaninlavas

• UniformlyhighCurietemp.indicatepuremagnetite

Datacompliled fromvarioussources;seeGee&Kent(2007)

NRM,inclinationandCurietemperaturevariationsinHole504B.

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GabbroMagnetization

• Lowercrusthasbeensampledatseveralshallowholesandtwoholespenetrating~1.5km

• Remanence averagesabout1A/m

datacompiledfromvarioussources;seeGee&Kent(2007)

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MagnetizationofDikesandGabbros

Pangetal.(2007)

Lowercrustalrockstypicallyhavenearlypuremagnetite(Curietemperature580C)eitherasaresultofsubdivisionoflargergrainsorastinymagnetitegrainsincludedinsilicateminerals.

Ilmenite lamellaeintitanomagnetite

TwogenerationsofmagnetiteexsolvedfromCPX(fromFeinbergetal.,2004).

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ThreeLayerModel

• Lavashavehighestmagnetization(~5A/m)

• Thickerdikes(2.3A/m)andgabbro(1.2A/m)generatecomparableanomalies

Gee&Kent(2007)

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LavaAccumulationPattern

Macdonaldetal.(1983)

Brunhes/Matuyama boundaryat21°NonEPRillustratinglavaspillover.Brunhes lavasextend250-500mbeyondtheverticallyaveragedreversalboundarydeterminedfromnearbottomdata.

• Transitionzonewidth(4sigma)of1.5to3kmlimitstheultimatetemporalresolution

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MagneticanomaliesfrommodernGPTS

FromGeeandKent,2007,TreatiseonGeophysics,v.5.12

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MarinemagneticanomalyskewnessShape(skewness)afunctionoftheremanentandambientfieldprojectionsandspreadinglineation

θmeas = ʹIr + ʹI f −180ʹIr = tan Ir( ) sin Az−Dec( )

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EffectiveRemanent Inclination

Notethateffectiveinclinationchangesmostrapidlyforspreadingcentersnearthepaleoequator

Variationofeffectiveremanentinclinationasafunctionoflineationandpaleolatitude (fromActonetal.,1996)

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Skewness Lunes ofConfidence

AsingleIr’estimatecouldbeproducedbyafamilyofremanent declination,inclinationpairs

Exampleoflunes ofconfdence fromLateCretaceousanomaliesinthenorthandsouthPacific(thesehavebeenadjustedforanomalousskewnessof14°;Cande,1976)

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AnomalousSkewness

• Anomalousskewness notpredictedbyblockmodelgeometry

• WhartonBasin:differentphaseshiftneededfortwoflanks

Dyment etal.(1994)

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Anomalousskewness estimatesfromIndianOcean(halfdifferenceofconjugateflanks)andanexampleofthesequenceeffect(right).FromDyment etal.(1994)

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Possiblecausesofanomalousskewness

1) outwardtiltofsourceblocks2) slopingboundaryinthelowercrust3) systematicvariationsinfieldintensity

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TiltingofLavas

Tivey etal.(2005)

LavatiltingmodelforODPHole801C.Dipsinferredfromloggingdataareusedtosuggesttiltfromlavaloading.

LavatiltfromloadingplusblockrotationsinferredforSites417/418.

Schouten(2002)

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LavaTiltandSkewness

• Anomalyskewness issensitiveindicatorofsuchtilting(1° tiltcorrespondsto1° differenceinskewness)

• Lavatiltfromloadingresultsinanomalousskewnessoppositetothatobserved

Gee&Kent(2007)

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Nonvertical BoundariesinGabbro

• Slopingisochrons inlowercrustcansignificantlyaffectanomalyshape

• Phaseshiftof~45°,insamesenseasglobalobservationsofanomalousskewness

Gee&Kent(2007)

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RichardGordon’svideopresentationprovidessomeexamplesofapplicationofskewness polestoPacificplatemotion

Best-fittingpaleopoles fromanomaly12r(~32Ma)forthePacificplatefromanomalyskewness (blue)comparedtoestimatesfromsedimentaryfacies,paleomagnetic dataandhotspots

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Exampleofaeromagneticvectordataatlowlatitude

Horner-JohnsonandGordon(2003)

Testsfortwodimensionality

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Notethatmagnitudeofvectoranomaliesisalwaysgreaterthanorequaltototalfieldanomaly.

GeeandCande (2002)

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Vectoranomaliescanallowidentificationofanomaliesingeometrieswithverylowamplitudetotalfieldanomalies

Engelsetal.(2008)

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Vectordataalloworientationofmagneticcontraststobeestimatedfromasingleprofile

Engelsetal.(2008)

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DoesOceanCrustRecordIntensityFluctuations?

• Potentialhigherresolutiontimemarkers

• Consistentpatterninseasurfaceanomalies(anom 5)

• Wavelengthsafunctionofearthfilter

Cande andKent(1992)Bowersetal.(2001)

82mm/yr

31mm/yr

54mm/yr

82mm/yr

54mm/yr

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NearBottomAnomalyData

• Anomaly5profilesacquiredafew100mabovesource

• Nearbottomanomaliesalsolineatedbutmorecomplexpattern

• Unlikelytorepresentreversals

• Globallypresent?

afterBowersetal.(2001)

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AnIndependentRecordofIntensityFluctuationsintheBrunhes

afterGeeetal.(1996)Tauxe andYamazaki(2007)

Sedimentarycoresproviderelativeintensityrecord,thatmatchseasurfaceanomalyprofilesreasonablywell.

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Brunhes NearBottomAnomalies

• Stackof8profilesseparatedbyupto50km

• Topographicvariationscanbeaccountedforwithinversions

• Severalsimilaritieswithsedimentaryrelativeintensityrecords

Geeetal.(2000)

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AnAdditionalCheck

• Candetermineabsoluteintensityofthefieldfromsurface(glass)samples

• Similarpatternwithaxiallowandboundinghighsinmagneticanomaliesandglasspaleointensities

Geeetal.(2000)