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ID:39450421
大小:2.75 MB
页数:384页
时间:2019-07-03
《Understanding Relativity 1996》由会员上传分享,免费在线阅读,更多相关内容在学术论文-天天文库。
1、ThispageintentionallyleftblankThispageintentionallyleftblankThispageintentionallyleftblankThispageintentionallyleftblank20/GalileanRelativitywithm'themassappropriatetoframe5'.Inclassicalmechanics,however,massisconsideredanintrinsicpropertyofabodyandmustbeinvariant.HencewecanputnI'==m.Weshow
2、edearlier(eq.[1.13])thataccelerationisinvariantunderaGalileantransformation:a'==a.Henceequation(1.18)followsfrom(1.17)ifandonlyiftheforceFisalsoinvariant,12thatis,ifF'==F(1.20)Onehastoinvestigatecasebycasewhethertheforcesthatexistinnaturesatisfytheinvariancerequirement(eg.[1.20]).Forexample
3、,thegravitationalattractionbetweentwobodiesisgivenbyNewton'slawofgravity:(1.21)Herem1andm2arethemassesofthebodies,risthedistancebetweenthem,andGisaconstant.Wehavealreadyshownthatdistanceisinvari•antunderaGalileantransformation.Hencethegravitationalforceisin•deedinvariantandthelawofgravityis
4、consistentwiththeprincipleofrelativity.ThemostimportantexampleofaforcelawthatisnotcovariantinGalileanrelativityiselectromagnetism.Thelawsofelectricityandmagne•tismwerecodifiedinthelatenineteenthcenturyinasystemknownasMaxwell'sequations.Ifoneassumesthattheseequationsholdinsomeframe5andmakesa
5、Galileantransformationtoanotherframe5',theequationsin5'donothavethesameform:Maxwell'sequationsarenotcovariantunderaGalileantransformation.ThiswasverytroublingtoEinsteinandmotivatedhisquestforanewtheory.Therewerethreelogicalpossibilities:(i)Therelativityprincipledoesnotapplytoelectromagnetis
6、m;Max•well'sequationsarevalidonlyinonespecialframeofreference.(ii)Therelativityprincipledoesapplytoelectromagnetism,butMax•well'sequationsareonlyapproximatelycorrect;theymustbereplacedbyamoregeneralsetofequationsthatarestrictlycovariant.12.Ifeveryterminarelationisinvariant,asinthepresentexa
7、mple,therelationisobviouslycovariant.Thisisnotanecessarycondition,however.Covariancerequiresonlythatbothsidesoftheequationtransforminthesameway.Suppose,forexample,thatundersomehypotheticaltransformation,a'=2aandF'=2F.Eq.(1.18)wouldbesatisfiedandthelawwou
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