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Chapter2Thenatureofsound
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Twofacesofsound
Ifatreefallsihoutaohearit,doesitmakeasound?Thedualmeaningof‘sound’,asphysieion,providesaswer:yesaiohephysidsesofsoundareplex,inthatmanyoftheimpressionssoundmakesoedtoitsphysicalparametersbutothem.So:high-frequendssouched—usually.Andmorepowerfulsoundssouhewhole.Furthermore,manysounds,fromsirenstoskirlsandfromlullabiestolions’roars,makeemotionalimpauswhilythevaguestrelationshipstotheirphysicalparameters.
Thephysicalaspectsofsoueruhaioiswithphysicsthatweshouldbegin.
Pressure>
Soundsareusuallymadebysomethingmovinginahediaphragmofalinandout,thegapbetweenthevocalfandwidening,uitarstringvibratingbadforth.Itisthetransmissioionstmedium(solid,liquid,as),andtheirprogressihthatmedium,thatstitutesound.Ihemotiohemediumitself,suchastheairintheneckofabottlewhenoneblowsacrossit.Non-movingsourcludesuddeenergy,suchasbyexplosionsorsparks,andrapidlyosgheatsources.
&ionisthatofaloudspeaker’sdiaphragm,thecauseisavaryirialwiththesamepatternasthesouhediaphragmwillproduce.Eachtimethediaphragmmovesout,itsqueezestheairmoleculesimmediatelyinfrontofitclether,fionofhighpressure.Thesemoleculespresshbthemcletheriurn,andsoapulseofolecules(ahthemedium,folloressurearea(rarefa),whichisproducedasthediaphragmmovesin>
Thediaphragmtheagain,makingasedpulse.Howoftenthediaphragmmovesinand1sedgivesthefrequencyofthesouz,abbreviatedHz).Thesimplestsounduretoneasmade,forexample,byatuningfork;asnapshotofthevariationihdistansuchaforkwouldbeasinewave,asshowninFigure1.
&aeaks(hs)ofasouhewavelength(λ).Thesoundwilltravelthroughtheairatavelocityv,whichwillbearouresperseperature.Thefrequency(f)isgiveionf=vλ.Aplotofthevariationofpressureovertimeatasiinspaceisalsoasinewave,sowecouldlabeltheabovex-axisofFigure1as‘time’ifwewished.
1.Soundressureplot.
2.Molecularviewofsound>
ImageslikeFigure1aresooiseasytoimagiheyprovidesomekindofapictureofasoundwave,andmanybooksusetheminthisway.Infact,however,thereisnoupanddowioninasouhereisin,say,aheonlymotionisofmoleculesshuttlielyawayfromandtowardsthesource,liketheballsofaon’scradle.Suchwavesarereferredtoaslongitudinal,andifwecouldseeairmoleculestheywouldlooksomethinglikeFigure2.
Ifauoussinatesfromapoispreadsiions,asanexpahedeteareaissmall(likeamiediaphragmoreardrum)aresfromthesource,thecurvatureofthesligible,inwhichcasethesouheformofplanewaves.Evenifthesourceofthesoundhasaparticulardiretoit(likemostloudspeakers),thesoundwillstillspreadspherically,solongasthediaphragmislargerthahofthesound.Fths,thesousiosomeextent,andatsufitlyhighfrequencieswillformabeam(seeChapter6).
gsound
&yofsounddependsoiddensityofthemedium(Chapter1).Inair,souyihinghumidityahiemperature,butonlybecauseofthedensitythatthesefactorsplesaregiveninTable1.
Table1.Souiesimediaands
&hevelocityofsoundinairiemperature,oheairmaresupishotterthaheground,souravelfasterthehighertheyare.Theeffectofthisvelocreaseistobehemdownwardsfromthewarmerair,returhsomedistanceaway,asshowniimessoundsbeheardmreatdistaashortohiseffect.Refraalsoexplainswhyitishardtaihewihegroundslowsthesouly(paredtotheground)buttheairafewmetresupisfaster,sothesoundwavesareslowedalittlemorethere.Thesousfromthelow-veliontothehigher-veloe,andhencecurvesupawayfromthegroundandfromyourears(seeFigure4).
3.Sationwhenairisearthegroundthanhighaboveit.
4.BarbarahearAlan,butnotClive.
ohadiaphragm,opushshtheairthatsurroundsitanyfaster.Mliespressurepulsesthatareclether,whiarriveatapoint—youreardrum,say—morefrequently.Thatistosay,thesoundfrequencywouldrise.Iforiespushingtheairharderbymovingthediaphragmfurtherinandout,theofpression(aion)inthepulsesincreases,leadingtoahighersoundpressure(heardasaloudersound).Ifohediaphragmtomovefasterthayofsoundinthemedium,apulsehasomoveawayfromthediaphragmbeforethepulseforms.Heheypileupintoasiremehigh-pressurepulseknownasashockwave(thecauseofsonisand>
Movingadiaphragmmorerapidlyisnottheonlywaytoihefrequencyofasound:iftheloudspeaker(orothersource)israpidlyapproagyouoryouarerapidlyapproagit,thepressurepulsesarriveatyourearmorefrequently,becauseeachstartsclosertoyouthantheohefrequencyofthesouhesourcehaspassedby,thepulseshityourearwithloervalsiween,becauseeachhasalittlefarthertotravelthantheohefrequencyfalls.Thisisthewell-know,enswheneveroneispassedbyaspeedingmotorbikeorthesirenofthepolicedit(Box2).
&,sous,andaswithrefleirreofthesoundsouredifasurfaceissmoothandhard,soifyouaresomewherebetweensourdsurface,youroximatelythesamesoundfromeachside(butquieterfromthereflectorside).‘Smooth’isarelativetermthough,meaning‘withbumpssmallerthah’.Sindwavesareaboutonemilliontimeslht(paring3kHztoyellow),evenquiteroughsurfaceslikeakegoodairrors.irrorsfocusthesoundsthattheyrefleWorldWarIjustsuirrorswerebuiltalohcoastofEnglandtofocusthesoundplaheearsoflisteningsolders.Wheweentwoormorecurvedreflectors,theresultbeawhisperinggallery,liketheoneinLondon’sSaintPaul’sCathedral.
Box2
Soufromtheiweenaherairaerandair,ordifferentrocklayersih.Howmuchofthesoueddependsonthediffereicesofthetwomedia,andtheimpedaurhedensityofthemediumayofsoundinit.Apedance(Box3)issimilartoelectricalresistaitmeasuresthedificultywithwhidtravelthroughamedium.Itiskeytomasandapplisofsound.Forirubberysurfacewillabsorbsoundaoheat,sirubberhasaremelyhighapedaingsonsubmarinesarebasedonthisfafortunessofrubberisverytemperature-depe,so,whenColdWarsubmarineswereredeployedfromtheNorthAtlantictotheGulffromthelate1980s,thehighereraturesrobbedthemoftheirstealthaoffaflurryofreseardresurfag.
Soundbefocussedbypassingitthroughanacoustiadeofacrylicplastisesworkbecauseawaveisrefraitpassesfromoasitstrikestheiweeaheahroughwhichthewaveisrefradsoioofitsvelothetwomedia(Snell’slaw,Box4).
&whichisusuallyfarmorenoticeableforsoundthanfhtisitsabilitytobendrounddoverreadthroughanopening,aphenomenonknownasdiffraure5).
Box3
Characteristipedanedium:Z0=ρ0v0;densityρ0,velocityofsouistheRayl,andthe0sihesearethevaluesofthemediumwhenitis‘uis,whennosouinit.
Box4
Snell’slaw:sinθ1sinθ2=v1v2;θ(theta)istheahedireofthesoundaaheinterface,vissouy.
5.Difira.
&hewaveleerthebending.Soifahighwallisiweenasoundsourd,say—ahebasssoundsdiffraitstopbatoearthbutthehigh-pitesarelost(Figure6).Thismuffliisausefulcluethathelpsusgaugethedistaniliarsoudoors.
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