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1、均勻帶電球體表面電場強(qiáng)度的計(jì)算論文I摘要因此均勻帶電球體表面電場強(qiáng)度使用高斯定理不能獲得因?yàn)楦咚苟ɡ硎且粋€(gè)幾何表面表面電荷也利用幾何模型當(dāng)高斯分割和表面電荷表面電荷不能被視為一個(gè)幾何面與普通物理的電磁學(xué)教材在討論均勻表面電荷產(chǎn)生的電場強(qiáng)度分布不計(jì)算表面電場。本文介紹了疊加原理點(diǎn)電荷球形均勻一個(gè)任意點(diǎn)的磁場強(qiáng)度值表面磁場強(qiáng)度為球形面很近球形點(diǎn)電場強(qiáng)度平均值并從外地疊加原理的兩種方法求出了均勻帶電球面電場強(qiáng)度值。關(guān)鍵詞帶點(diǎn)球面電場強(qiáng)度疊加原理電荷面密度高斯定理突變IIAbstractpickduetouniformchargedspheresurfaceelectricfield
2、intensityusingGausstheoremcannotbeobtainedbecauseGaussstheoremisageometricsurfacesurfacechargeisalsousingthegeometricmodelwhenGausssegmentationandsurfacechargesurfacechargecannotberegardedasageometricsurfaceandgeneralphysicselectromagneticsteachingmaterialsinthediscussionofuniformchargedsur
3、faceelectricfieldintensityproducedbydistributionarenotcalculatedsphericalelectricfieldintensityof.Thispaperintroducestheprincipleofsuperpositionofpointchargeandsphericaluniformwithanarbitrarypointofthefieldstrengthvaluethesurfacefieldstrengthforsphericalsidesverynearsphericalpointfieldstren
4、gthaveragevalueandfromthefieldsuperpositionprinciplebytwokindsofmethodtoseekouttheuniformlychargedsphericalsurfaceelectricfieldstrengthvalue.Keywords:withsphericalelectricfieldintensitysuperpositionprinciplesurfacechargedensityGausstheoremmutationIII目錄摘要.....................................
5、.......................................................................................................................IAbstract........................................................................................................................................................II引言.......
6、.......................................................................................................................................................11.電場強(qiáng)度與電場的疊加原理的概念......................................................................................................11.1電場強(qiáng)度............
7、.........................................................................................................................11.2電場疊加原理...........................................................................................................................
