剑桥AS物理课程知识点总结.docx
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剑桥AS物理课程知识点总结.docx
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剑桥AS物理课程知识点总结
I
Displacementisthedistancetravelledinaparticulardirection.
Velocityisdefinedbythewordequation
Thegradientofadisplacement-timegraphisequaltovelocity:
Distanceandspeedarescalarquantities.Ascalarquantityhasonlymagnitude.
Displacementandvelocityarevectorquantities.Avectorquantityhasbothmagnitudeanddirection.
Vectorquantitiesmaybecombinedbyvectoradditiontofindtheirresultant.
II
Accelerationisequaltotherateofchangeofvelocity.
Accelerationisavectorquantity.
Thegradientofavelocity-timegraphisequaltoacceleration:
Theareaunderavelocity-timegraphisequaltodisplacement(ordistancetravelled).
Theequationsofmotion(forconstantaccelerationinastraightline)are:
Vectorssuchasforcescanberesolvedintocomponents.Componentsatrightanglestooneanothercanbetreatedindependentlyofoneanother.Foravelocityvatanangleθtothex-direction,thecomponentsare:
x-direction:
vcosθy-direction:
vsinθ
Forprojectiles,thehorizontalandverticalcomponentsofvelocitycanbetreatedindependently.Intheabsenceofairresistance,thehorizontalcomponentofvelocityisconstantwhiletheverticalcomponentvelocitydownwardsincreasesatarateof9.81ms-2.
III
Anobjectwillremainatrestorinastateofuniformmotionunlessitisactedonbyanexternalforce.ThisisNewton’sfirstlawofmotion.
Forabodyofconstantmass,theaccelerationisdirectlyproportionaltotheresultantforceappliedtoit.ResultantforceF,massmandaccelerationaarerelatedbytheequation:
resultantforce=mass×accelerationorF=ma
ThisisaformofNewton’ssecondlawofmotion.
Whentwobodiesinteract,theforcedtheyexertoneachotherareequalinmagnitudeandoppositeindirection.ThisisNewton’sthirdlawofmotion.
Theaccelerationproducedbyaforceisinthesamedirectionastheforce.Wheretherearetwoormoreforces,wemustdeterminetheresultantforce.
Anewton(N)istheforcerequiredtogiveamassof1kganaccelerationof1ms-2inthedirectionoftheforce.
Thegreaterthemassofanobject,themoreitresistschangesinitsmotion.Massisameasureoftheobject’sinertia.
Theweightofanobjectisaresultofthepullofgravityonit:
weight=mass×accelerationoffreefall(W=mg)
weight=mass×gravitationalfieldstrength
Anobjectfallingfreelyundergravityhasaconstantaccelerationprovidedthegravitationalfieldstrengthisconstant.However,fluidresistance(suchasairresistance)reducesitsacceleration.Terminalvelocityisreachedwhenthefluidresistanceisequaltotheweightoftheobject.
IV
Forcesarevectorquantitiesthatcanbeaddedbymeansofavectortriangle.Theirresultantcanbedeterminedusingtrigonometryorbyscaledrawing.
Vectorssuchasforcescanberesolvedintocomponents.Componentsatrightanglestooneanothercanbetreatedindependentlyofoneanother.ForaforceFatanangleθtothex-direction,thecomponentsare:
x-direction:
Fcosθ
y-direction:
Fsinθ
Themomentofaforce=force×perpendiculardistanceofthepivotfromthelineofactionoftheforce.
Theprincipleofmomentsstatethatforanyobjectthatisinequilibrium,thesumoftheclockwisemomentsaboutanypointprovidedbytheforcesactingontheobjectequalsthesumoftheanticlockwisemomentsaboutthatsamepoint.
Acoupleisapairofequal,parallelbutoppositeforceswhoseeffectistoproduceaturningeffectonabodywithoutgivingitlinearacceleration.
torqueofacouple=oneoftheforces×perpendiculardistancebetweentheforces
Foranobjecttobeinequilibrium,theresultantforceactingontheobjectmustbezeroandtheresultantmomentmustbezero.
V
TheworkdoneWwhenaforceFmovesthroughadisplacementsinthedirectionoftheforce:
W=FsorW=Fscosθ
whereθistheanglebetweentheforceandthedisplacement.
Ajouleisdefinedastheworkdone(orenergytransferred)whenaforceof1Nmovesadistanceof1minthedirectionoftheforce.
TheworkdoneWbyagasatpressurepwhenitexpands:
W=pΔV
whereΔVistheincreaseinitsvolume.
Whenanobjectofmassmrisesthroughaheighth,itsgravitationalpotentialenergyEpincreasesbyanamount:
Ep=mgh
ThekineticenergyEkofabodyofmassmmovingatspeedvis:
Ek=1/2mv2
Theprincipleofconservationofenergystatesthatforaclosedsystem,energycanbetransformedtootherformsbutthetotalamountofenergyremainsconstant.
Theefficiencyofadeviceorsystemisdeterminedusingtheequation:
efficiency=(usefuloutputenergy)/(totalinputenergy)×100%
Poweristherateatwhichworkisdone(orenergyistransferred):
P=W/tandP=Fv
Awattisdefinedasarateoftransferofenergyofonejoulepersecond.
VI
Linearmomentumistheproductofmassandvelocity:
momentum=mass×velocityorp=mv
Theprincipleofconservationofmomentum:
Foraclosedsystem,inanydirectionthetotalmomentumbeforeaninteraction(e.g.collision)isequaltothetotalmomentumaftertheinteraction.
Inallinteractionsorcollisions,momentumandtotalenergyareconserved.
Kineticenergyisconservedinaperfectlyelasticcollision;relativespeedisunchangedinaperfectlyelasticcollision.
Inaninelasticcollision,kineticenergyisnotconserved.Itistransferredintootherformsofenergy(e.g.heatorsound).Mostcollisionsareinelastic.
Newton’sfirstlawofmotion:
Anobjectwillremainatrestorkeeptravelingatconstantvelocityunlessitisactedonbyaresultantforce.
Newton’ssecondlawofmotion:
Theresultantforceactingonabodyisequaltotherateofchangeofitsmomentum:
resultantforce=rateofchangeofmomentumor
Newton’sthirdlawofmotion:
Whentwobodiesinteract,theforcestheyexertoneachotheraeequalandopposite.
TheequationF=maisaspecialcaseofNewton’ssecondlawofmotionwhenmassmremainsconstant.
VII
Densityisdefinedasthemassperunitvolumeofasubstance:
Pressureisdefinedasthenormalforceactingperunitcross-sectionalarea:
Pressureinafluidincreaseswithdepth:
ρ=mgh
Hooke’slawstatethattheextensionofamaterialisdirectlyproportionaltotheappliedforce.Foraspringorawire,F=kx,wherekistheforceconstant.TheforceconstanthasunitsofNm-1.
Stressisdefinedas
Strainisdefinedas
Todescribethebehaviorofamaterialundertensileandcompressiveforces,wehavetodrawagraphofstressagainststrain.ThegradientoftheinitiallinearsectionofthegraphisequaltotheYoungmodulus.TheYoungmodulusisanindicationofthestiffnessofthematerial.
TheYoungmodulusEisgivenby
TheunitoftheYoungmodulusispascal(Pa)orNm-2
Theareaunderaforce-extensiongraphisequaltotheworkdonebytheforce.
ForaspringorawireobeyingHooke’slaw,theelasticpotentialenergyEisgivenby
VIII
Anelectricfieldisafieldofforce,createdbyelectriccharges,andcanberepresentedbyelectricfieldlines.
Thestrengthofthefieldistheforceactingperunitpositivechargeatapointinthefield,
Inauniformfield(e.g.betweentwoparallelchargedplates),theforceonachargeisthesameatallpoints;thestrengthofthefieldisgivenby
.
Anelectricchargemovinginitiallyatright-anglestoauniformelectricfieldfollowsaparabolicpath.
IX
Electriccurrentistherateofflowofcharge.Inametalthisisduetotheflowofelectrons.Inanelectrolyte,theflowofpositiveandnegativeionsproducesthecurrent.
Thedirectionofconventionalcurrentisfrompositivetonegative;thedirectionofelectronflowisfromnegativetopositive.
TheSIunitofchargeiscoulomb(C).Onecoulombisthechargewhichpassesapointwhenacurrentof1Aflowfor1s.
charge=current×time(ΔQ=IΔt)
Theelementarychargee=1.9×1019C.
ThecurrentIinaconductorofcross-sectionalareaAdependsonthemeandriftvelocityvofthechargecarriersandtheirnumberdensityn.
I=nAvq
Thetermpotentialdifference(p.d.)isusedwhenchargesloseenergyinacomponent.Itisdefinedastheenergytransferredperunitcharge.
or
Thetermelectromotiveforce(e.m.f.)isusedwhenchargesgainelectricalenergyfromabatteryorsimilardevice.Itisalsodefinedastheenergytransferredperunitcharge.
or
Avoltisajoulepercoulomb.Thatis,1V=1JC-1.
Poweristherateofenergytransfer.Inelectricalterms,poweristheproductofvoltageandcurrent.Thatis,P=VI.
Resistanceisdefinedastheratioofvoltagetocurrent.Thatis:
Theresistanceofacomponentis1ohmwhenapotentialdifferenceof1voltisproducedperampere.
ForaresistanceR,thepowerdissipatedisgivenby:
P=I2Ror
EnergytransferredinacircuitinatimeΔtisgivenby:
W=IVΔt
X
Kirchhoff’sfirstlawstatesthatthesumofthecurrentsenteringanypointinacircuitisequaltothesumofthecurrentsleavingthatpoint.
Kirchhoff’ssecondlawstatesthatthesumofthee.m.f.saroundanyloopinacircuitisequaltothesumofthep.d.saroundtheloop.
Thecombinedresistanceofresistorsinseriesisgivenbytheformula:
R=R1+R2+…
Thecombinedresistanceofresistorsinparallelisgivenbytheformula:
Ammetershavealowresistanceandareconnectedinseriesinacircuit.
Voltmetershaveahighresistanceandareconnectedinparallelinacircuit.
XI
AconductorobeysOhm’slawifthecurrentinitisdirectlyproportionaltothepotentialdifferenceacrossitsends.
Ohmiccomponentsincludeawireatconstanttemperatureandaresister.
Non-ohmiccomponentsincludeafilamentlambandalight-emittingdiode.
Asemiconductordiodeallowscurrentinonedirectio
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