Chapter 2 Meteorology and · PDF fileChapter 2 Meteorology and Oceanography ... Wind is one of...
Transcript of Chapter 2 Meteorology and · PDF fileChapter 2 Meteorology and Oceanography ... Wind is one of...
PART II ACTIONS AND MATERIAL STRENGTH REQUIREMENTS, CHAPTER 2 METROLOGY AND OCEANOGRAPHY
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Chapter 2 Meteorology and Oceanography
1 Meteorology and Oceanography Items to be Considered for Performance Verification1.1 GeneralThefollowingmeteorologyandoceanographyitems,shallbeconsideredwithregardtotheperformanceverificationofportfacilities.
Atmosphericpressureanditsdistributionarefactorsthatgeneratewinds.
Windsgeneratewavesandstormsurge,andaffectthewindpressurethatactsuponportfacilitiesandmooredvessels,andbecomeafactortointerferewithcargohandlingandotherportoperations.See2 Windsfordetails.
The tidal level affects soil pressure andwater pressure,which act onport facilities, andbecomes a factor tointerferewithcargohandlingandotherportoperations.Also,ithasaneffectonwavesinareasofshallowwater.See3 Tidal levelfordetails.
Wavesexertwaveforceonportfacilities,andbecomeafactortointerferewiththefunctioningofportfacilities.Theyalsoactonmooredvessels,causingthemtomoveandinterferewithcargohandlingandotherportoperations.Theyalsocanraisethemeanwaterlevel,whichhaseffectssimilartothetidallevelasmentionedabove.See4 Wavesfordetails.
Tsunamiexertswaveforceandfluidforceonportfacilities,andbecomesafactortointerferewiththefunctioningofportfacilities.Italsoactsonmooredships,causingthemtomove.See5 Tsunamisfordetails.
Watercurrentsaffectsedimentsontheseabottomandbecomeafactortointerferewiththefunctioningofportfacilities.See6 Water Currents etc.fordetails.
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2 WindsPublic NoticeWinds
Article 6Characteristicsofwindsshallbesetbythemethodsprovidedinthesubsequentitemscorrespondingtothesingleactionorcombinationoftwoormoreactionstobeconsideredintheperformancecriteriaandtheperformanceverification:(1) Oceansurfacewinds tobeused in theestimationofwavesandstormsurge shallbeappropriately
definedintermsofwindvelocity,winddirectionandothersbasedonthelong-termwindobservationorweatherhindcasting.
(2) Windstobeusedinthecalculationofwindpressuresshallbeappropriatelydefinedintermsofthewindvelocityanddirectioncorrespondingtothereturnperiodthroughthestatisticalanalysisofthelong-termdataofobservedorhindcastedwindsorothermethods.
(3) Windstobeusedinthecalculationofwindenergyshallbeappropriatelydefinedintermsofthejointfrequencydistributionofwindvelocityanddirectionforacertaindurationoftime,basedonthelong-termdataofobservedorhindcastedwinds.
[Commentary]
1) WindstobeusedintheEstimationofWavesandStormSurge:Windstobeusedintheestimationofwavesandstormsurgeshallbeobservedorhindcastedvaluesfor30yearsormoreasastandard.
2) WindstobeusedintheCalculationofWindPressure:Windstobeusedinthecalculationofwindpressureshallbeobservedorhindcastedvaluesfor30yearsormoreasastandard.
[Technical Note]
2.1 General
(1)Windisoneofthemostdistinctivemeteorologicalphenomena,namely,thephenomenonthattheairmovesduetoatmosphericpressuredifferencesandheat.Theconditionsunderwhichwindsblowovertheoceanareusuallyverydifferentthanforthoseoverland.Windvelocitiesovertheoceanaremuchhigherthanthoseoverlandneartheshore.1)Forperformanceverificationofportfacilities,theeffectsofwindsmustbeappropriatelyevaluated.
(2)GradientWinds
Thevelocityofthegradientwindcanbeexpressedasafunctionofpressuregradient,radiusofcurvatureofbarometicisolines,latitude,andairdensityasinequation(2.1.1).
(2.1.1)
where Vg :velocityofgradientwind(m/s);inthecaseofananticyclone,equation(2.1.1)givesanegative
valueandsotheabsolutevalueshouldbetaken. p/r :pressuregradient(takentobepositiveforacyclone,negativeforananticyclone)(kg/m2/s2) r :radiusofcurvatureofbarometicisolines(m) :angularvelocityofEarth'srotation(1/s) =7.2710-5/s :latitude() a :densityofair(kg/m3)
Beforeperformingthecalculation,measurementunitsshouldfirstbeconvertedintotheMKSunitslistedabove.Notethat1oflatitudecorrespondstoadistanceofapproximately1.11105m,andanairpressureof1.0hPais100kg/m/s2.
PART II ACTIONS AND MATERIAL STRENGTH REQUIREMENTS, CHAPTER 2 METROLOGY AND OCEANOGRAPHY
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Agradientwindforwhichthebarometicisolinesarestraightlines(i.e.,theirradiusofcurvatureinequation(2.1.1)isinfinite)iscalledthegeostrophicwind.Inthiscase,thewindvelocityisasequation (2.1.2).
(2.1.2)
Theactualseasurfacewindvelocityisgenerallylowerthanthevalueobtainedfromthegradientwindequation.Moreover, although the direction of a gradientwind is parallel to the barometic isolines in theory, the seasurfacewindblowsatacertainangletothebarometicisolinesinrealityasillustratedinFig. 2.1.2.Inthenorthernhemisphere,thewindsaroundacycloneblowinacounterclockwisedirectionandinwards,whereasthewindsaroundananticycloneblowinaclockwisedirectionandoutwards.Itisknownthattherelationshipbetweenthevelocityofgradientwindsandthatoftheactualseasurfacewindvarieswiththelatitude.ThisrelationshipundertheaverageconditionsissummarizedasinTable 2.1.1.3)
Low
High
(a) Cyclone (b) Anticyclone
Fig. 2.1.2 Wind Direction for a Cyclone (Low) and an Anticyclone (High)
Table 2.1.1 Relationship between Sea Surface Wind Speed and Gradient Wind SpeedLatitude() 10 20 30 40 50
Angle() 24 20 18 17 15
VelocityratioVs /Vg 0.51 0.60 0.64 0.67 0.70
(3)TyphoonWindsIncalculationsconcerningthegenerationofstormsurgeorwavesduetoatyphoon,itiscommontoassumethattheairpressuredistributionfollowseitherFujitasequation (2.1.3)4)or Myers equation (2.1.4) 4);theconstantsinthechosenequationaredeterminedbasedonactualairpressuremeasurementsintheregionoftyphoons.
Fujitasformula
(2.1.3)
Myersformula
(2.1.4)
where p :airpressureatadistancer fromthecenteroftyphoon(hPa) r :distancefromthecenteroftyphoon(km) pc :airpressureatthecenteroftyphoon(hPa) r0 :estimateddistancefromthecenteroftyphoontothepointwherethewindvelocityismaximum
(km) p :airpressuredropatthecenteroftyphoon(hPa) p=p-pc p :airpressureatr =(hPa); p=pc+p
Thesizeofatyphoonvarieswithtime,andso r0andp mustbedeterminedasthefunctionsoftime
(4)MeteorologicalGPVOrganizations such as the Japan Meteorological Agency, the European Center for Medium-Range Weather
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Forecasts(ECMWF),andAmericasNationalCenterforEnvironmentalProtection(NCEP),calculatethevaluesofitemssuchasairpressure,windvelocity,winddirection,andwatervaporflux,basedoncalculationmodelsformeteorologicalvaluesthatuseathree-dimensionalcalculationgrid,andthevaluesatthegridpoints(GPV:gridpointvalues)aresaved.TheseGPVsmaybeusedinsteadofwindhindcastingsbasedonequation (2.1.1) throughequation (2.1.4). However,whenagridwithlargespacingisusedformeteorologicalcalculationstheatmosphericpressureandwindsmaynotbesatisfactorilyreproducedatplaceswheremeteorologicalconditionschangedrasticallywithposition,suchasnear thecentersof typhoons. Therefore,whenGPVsareused, it ispreferabletouseobservationalvaluestoverifytheprecision.
(5)WindEnergyIfwindsareconsideredasthemovementoftheairthenthewindenergythatcrossesaunitcross-sectionalareainunittimeisgivenbyequation(2.1.5).1) Winds forestimating thewindenergyshallbeappropriatelyspecifiedwith jointstatisticdistributions forvelocity and direction for a fixed time (usually, one year), based on long-term (usually, three years ormore)observedorhindcasteddata.
(2.1.5)
where P :windforceenergyperunitcross-sectionalarea(W/m2) a :airdensity(kg/m3) V :windvelocity(m/s)
Inotherwords,thewindforceenergyisproportionaltothecubeofthewindvelocity,soasmalldifferenceinwindvelocitycanmeanabigdifferenceinenergy(powergeneration).Therefore,duringperformanceverificationoffacilitiesthatusewindforceenergy,itisimportanttoaccuratelyunderstandhowtheconditionschangewithregardtotimeandspace. Inthecoastalzonethewindconditionsvariesdrasticallybetweenlandandsea.Also,windvelocityshowsgreatvariationonlandduetoaltitude,butovertheseathechangesinwindvelocitywithaltitudearegradual,soitispossibletoobtainhighlystabilizedwindsthatareappropriateforpowergenerationatrelativelylowaltitudes.Forexample,theresultsofmeasurementsinthevicinityoftheKansaiInternationalAirport,showthatthewindenergyoverthecourseofayearatameasurementtower(MTstation)placedataheightof15metersovertheoceanwereroughlythesameasatalandstation(Cstation)withanaltitudeof100meters,andaboutfivetimesgreaterthanatalandstationwithanaltitudeof10meters.5)
2.2 Characteristic Values of Wind Velocity
(1)DeterminationofWindCharacteristicsTheelementsofwindsaredirectionandvelocity,wherethewinddirectionisexpressedasoneofsixteendirectionsand thewindvelocity is themeanvelocityover10minutes. Thevelocityofwinds thatactsdirectlyonportfacilitiesandmooredshipsisspecifiedingeneralasavelocityforacertainperiodofoccurrence,asestimatedfromtheprobabilityofoccurrencedistributionofwindvelocitybasedonlong-termmeasuredvaluesover30yearsormore.Usingtheannualmaximum10-minutemeanwindvelocitiesoverabout35years,basedonMeasurementTechnicalDataSheet#34oftheJapanMeteorologicalAgency,7)andassumingadoubleexponentialdistribution,theexpectedwindvelocitiesover5,10,20,50,100,and200yearshavebeencalculatedat141meteorologicalstations. Forperformanceverificationoffacilities, thesedatacanbeusedasreferencevalues,however if thelocationofstudyhasdifferenttopographicalconditionsfromtheclosestofthesemeteorologicalstationsthenitisnecessarytotakemeasurementsforatleastoneyeartodeterminetheeffectofthetopography.8)
(2)Thewindvelocitiesobtainedatthemeteorologicalstationsarethevaluesatabout10metersabovetheground.Therefore,whenusingthemeasuredvaluestoestimatethewindsovertheocean,iftheheightofthetargetfacilityisverydifferentfromtheheightmentionedabove,thencorrectionoftheheightshallbeperformedforthewindvelocity.Theverticaldistributionofwindvelocityisusuallyshownonalogarithmicscale,howeverforsimpli