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1、大学物理下册复习热学复习一、理想气体的状态方程及其变形(1)RTPV;(2)222111TVPTVP;(3)nKTP(4)molMRTPVNn称为分子数密度,摩尔数表达式:molmolVVNNMM0二、理想气体的压强公式和温度公式:22313231vnvnmPt,KTvmt23212三、理想气体的能量(注意掌握各种理想气体的自由度)1一个分子的能量平均平动动能:KTt23;平均转动动能:KTrr2平均总动能:KTrtKTik2)(22理想气体内能:TCPViRTiEmV,22单位体积的内能PiVE2)/(;单位质量的内能molMiRTME2)/(四、三种速率及其应用(特别注意最可几速率的应用)
2、最可几速率:molPMRTmkTv22平均速率:molMRTmkTv88方均根速率:PMRTmkTvmol3332五、速率分布函数NdvdNvf)(及其应用(归一化条件:1)(0dvvf)意义:表示在速率v附近,单位速率区间内的分子数占总分子数的百分比。dvvv区间的分子数占总分子数的百分比:dvvfNdN)(dvvv区间的分子数:dvvNfdN)(21vv有限区间的分子数:21)(vvdvvNfdNN利用速率分布函数求平均值:2121)()(vvvvdvvfdvvvfv,2121)()(22vvvvdvvfdvvfvv六、热力学第一定律(有限过程:AEQ,微小过程:AddEQd)1理想气体的
3、内能增量、功、热量(1)体积功:微小过程PdVAd,有限过程PdVA(适用于准静态过程)注意:在 PV 状态图中,有时可以用求面积法来求功。(2)内能增量:微小过程RdTidE2,有限过程TCTRiEmV,2(3)热量:TCQC 为摩尔热容量等压过程:等压摩尔热容量mPC,,TCQmPP,等容过程:等容摩尔热容量mVC,,TCQmVV,理想气体:RCCmVmP,,RiCmV2,,RiCmP22,,比热比:iiCCmVmP2,注意三个物理量正负的规定:系统吸热 Q 为正值,放热Q 为负值;系统对外作功 A 为正值,外界对系统作功A 为负值;系统内能增加E 为正值,系统内能减小E 为负值。2热力学
4、第一定律在四个等值过程中的应用(求 Q、A、E)(1)等容过程0dV,0ATCTRiEQVV2(2)等压过程0dPTRVPAP,VPiTCTRiEV22,TCQPP(3)等温过程0dT0E,2112lnlnPPRTVVRTQATT(4)绝热过程0Q,TCEV,TCEAV绝热过程方程:1CPV;21CTV;31CTP(C1、C2、C3都为常数)七、循环过程1 热机效率:吸放吸QQQA|1,致冷机致冷系数:吸放吸吸QQQAQ|2卡诺循环:由两个等温过程和两个绝热过程所构成的循环。卡诺热机效率:121TT卡,卡诺致冷机致冷系数:212TTT卡八:克劳修斯熵公式的应用、熵增加原理。静电场复习文档编码:
5、CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I
6、7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8
7、HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10
8、V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6
9、 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1
10、W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L
11、7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7一、真空中的库仑定律rrqqrrqqF?414122103210注意点电荷的概念(只有电量而无几何形状和大小的带电体)及其应用二、电场强度1电场强度定义0qFE(点电荷的场强:r
12、?rq41rrq41qFE20300)2电场强度的计算(1)利用场强迭加原理点电荷系的场强:i2iii0n21rr?q41EEEE连续带电体的场强:r?rdq41EdE20(注意dq的选取)(2)利用高斯定理求场强(掌握电通量的概念)真空0内iiSeqSdE,电介质:内iiSqSdD(其中EEDr0)利用高斯定理求解主要有三种情况:无限长带电直线(圆柱或圆柱体);无限大平面;球面(球体、球层)几种特殊带电体的场强:无限长直带电体:aE02无限大平面:02E三、电势和电势差1电势:零势点a0paaldEqEU电势差:ba0ab0pbpabaabldEqAqEEUUU电场强度与电势的关系:zUEy
13、UExUEUEzyxgrad重点掌握已知U(x,y,z)求电场强度,注意公式中的负号!2电势的求解:(1)利用电势的定义式)(ppldEU求解。(2)利用电势迭加原理求解。文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码
14、:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1
15、I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8
16、 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V1
17、0V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L
18、6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H
19、1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7
20、L7点电荷系:i0iir4qUU;连续带电体:r4dqU0。特别:均匀带电球面或金属带电球体:)(4)(400RrrqURrRqU球面内是等势体.求电场中任一点的电势可以用电势叠加的方法,也可以用先求电场强度分布,再从定义来分段积分.求解电荷非对称分布电场中的电势时,一定用叠加原理,即rqU04d.有导体存在时,必须先求感应电荷的分布再求电势分布;求感应电荷时必须以对称中心的电势为参考点。四、电荷在电场中的受力点电荷:EqF0;连续带电体:dqEFdF五、静电场的功、电势能1电场力的功:)(0)()(0)()(bababaabUUql dEql dFA2电势能:零势点a0paldEqE,电势能
21、差:bapbpal dEqEE0六、静电场中的导体(关键是掌握电荷在导体表面的分布)1 根据导体的静电平衡条件(内部场强处处为零),分析电荷在导体表面的分布,并进一步求电势等。特别要注意导体接地的情况。要先分清是导体还是电介质,如是导体必须判断是否带电或接地等(1).导体:在电场中的导体一定处于静电平衡状态(静电场)整个导体为等势体电荷分布在导体表面上导体内部无电荷导体表面,导体内部场强为零内表面表面内.30.20.10qEEE计算有导体存在时的电场强度UE,分布时文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10
22、V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6
23、 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1
24、W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L
25、7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:
26、CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I
27、7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8
28、HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7qSDSd.3.2.1高 斯 定 理接 地 时)电 荷 守 恒 定 律(导 体 不利 用 上 述 条 件;.注意导体表面的电荷重新分布,导体接地时是U=0,两导体相连时是U1=U2.注意导体附近有点电荷存在时,求感应电荷的方法是以对称中心的电势为参考,叠加各部分电势,通过电势关系求出感应电荷。(2
29、).电介质:在电场中电介质处于极化状态,对各向同性的均匀电介质而言,有:EDPEPrr00(cos)1(电介质表面)适用于介质内部各点电介质中的高斯定理包围的自由电荷)(dqSDS,灵活使用补偿或叠加原理。2电容的定义ABUqC及其求解,注意电容器串联和并联的特点。.平行板电容器中dr、的变化,外力所做的功为:前后外WWA,应分电源断开与不断开两种情况来讨论。(3).电容器电容的定义及计算步骤:(重点掌握各种电容器内部的电场强度分布)先假设两极板分别带QQ、求出两板间的电场强度分布求出两板间的电势差UUQC,常见电容器的电容:rabbaabRRRRCRRlCdSC04ln2其中球形电容器柱形电
30、容器平行板电容器七、静电场中的电介质1在各向同性电介质中,电位移矢量EEDr0(注意,0r的区别与联系:0r)文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1
31、W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L
32、7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:
33、CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I
34、7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8
35、HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10
36、V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L72介质中的高斯定理:isqsdD(重点掌握平行板电容器的特
37、点,如:dSCD,,电容器一直通电或通电后断开的情况下插入介质有关物理量的变化)八、电场的能量1电容器能量:2221212ababCUQUCQW2电场的能量能量密度:221Ee,(真空:2021Ee)定域空间 V 体积内的电场能量:dVEdWW221电场问题的求解步骤:先确定电荷Q 的分布用高斯定理求DEEDr求出0cos212dd2d4d,d21222PnPPCUCQWrSrrlrrVVwWEDwUUeVeee极化强度或用等效法板:柱:球:能量为电场能量密度及电势差电势稳恒磁场复习一、磁感应强度1电流元lId的概念2磁感应强度的计算(1)利用场强迭加原理计算电流元:304 rrlIdBd,任
38、意载流导线:304 rrlIdBdB.磁场叠加原理:)(sind4d02rrlIByyxxBBBBBd,dd再分析对称性叠加时先分解成分量,的方向注意文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E
39、8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V
40、10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7
41、L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9
42、H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q
43、7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编
44、码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7(2)利用运动电荷
45、的磁场公式304 rrvqB计算(3)利用安培环路定理计算真空LIl dB0,磁介质0LIldH(其中BBHr0)掌握几种特殊电流的磁场:(1)一段载流导体的磁场:)cos(cos4210aIB(注意:1,2,a的含义)无限长aIB20;当场点在载流导体的延长线上时0B;(2)圆电流轴线上场点的磁场:2322202xRIRB,圆心处:RIB20(3)长直螺线管:nIB0密绕螺绕环:rNIB20.掌握面电流的分割法(特别电流线密度的定义)LIj总.会用已知结果(特别是直线与圆组合)的叠加(几种电流在同一点P 的磁场叠加)PPPBBB21.运动电荷产生的磁场:运动轨迹闭合时,用等效电流法2,ddn
46、nqnInqI为转速,或,也可直接用运动电荷产生磁场公式叠加,3d4drrvqB二、掌握磁通量SdBd的求解三、磁力及其应用1洛仑兹力:Bvqf(F 方向与 q 正负有关)主要用于判断霍尔效应的有关问题(先用左手定则判断载流子的受力方向);在洛仑兹力作用下,带电粒子的运动情况(洛仑兹力提供向心力)。2安培力电流元:BlIdFd,载流导线:)(BlIdFdF方向可用左手定则判断叠加时先分解在合成yyxxFFFFFFddd文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:
47、CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I
48、7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8
49、HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10
50、V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6 ZC9H1W10Q7L7文档编码:CQ4A1I7N9E8 HP5V10V2Z7L6