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1、大学物理下学期考前复习1 祝 3 班同学逢考必过！第十章恒定磁场一、基本公式1)毕奥-萨伐尔定律304rrlIdBddB=20sinl4rId2)磁场叠加原理LrrlIdBdB3043)磁场中高斯定理0?sdBs(S 是闭合曲面)4)安培环路定律?内LLIl dB0（真空中）)(传导电流?Il dHL（介质中）H?=B?r B?=H?H?=B?=r-真空磁导率（4?10-7N/A2）r 介质磁导率5）安培定律BlIdFd dF=IdlBsinLFdF方向判断：右手四指由 Idl 的方向经小于 角转向 B?的方向，右螺旋前进的方向即为dF?max的方向6）磁通量sdBdsmm?匀强磁场中通过平面
2、：)(nmeSSSB?7）磁矩nmeSSIP若多匝线圈nmeSNSNIP8）磁力矩BPMmM=PmBsin =BISsin9）洛伦兹力公式BVqF带电粒子受电磁力)(EBVqF10）运动电荷产生的磁场304rrVqB二、典型结果1、有限长载流直导线在距其为r 的一点产生的磁场210coscos4rIB2、无限长载流直导线在距其为r 的一点产生的磁场rIB203、半限无长载流直导线在距其一端距离为r 的一点产生的磁场rIB404、载流圆环在环心产生的磁场RIB20|精.|品.|可.|编.|辑.|学.|习.|资.|料.*|*|*|*|欢.|迎.|下.|载.第 1 页，共 6 页大学物理下学期考前复
3、习2 祝 3 班同学逢考必过！5、载流圆弧（已知弧长L 和圆心角）在弧心产生的磁场222200RIRLRIB6、长直密绕螺线管内磁场nIB0第十一章电磁感应电磁场一、基本公式1)电动势定义LildEk2)法拉第电磁感应定律dtdi作用：计算闭合回路上i的大小和方向i方向的判断：首先确定回路绕行方向，如果dBdt 0,?0,则i=-d?dt=-SdBdt0,则表明积分路径是沿着非静电性场强kE的方向进行的，因此B 点电势比A 点电势低。4）感生电动势：产生根源(非静电力)为涡旋电场力或感生电场力公式i?BAldE涡sssddtBddsBdtddtd）（5）自感：自感系数IL，若为长 l,横截面为
4、 S，N匝，介质磁导率为 的螺线管，B=NlI；L=N2V(其中 V 为螺线管体积)感生电动势dtdILL6）互感：互感系数M，互感磁通量212，121互感电动势 21=-d?21dt=-MdI1dt 12=-d?12dt=-MdI2dt7)磁场能量密度2122mw磁场能量VdVdwWmm22一个自感为L,通过电流为I 的线圈，其中所储存的磁能为Wm=12LI2=12n2I2V(其中 V 表示长直螺线管的体积)第十二章机械振动1)谐振动方程：tAxcos谐振子：mk，22020vxA，|精.|品.|可.|编.|辑.|学.|习.|资.|料.*|*|*|*|欢.|迎.|下.|载.第 2 页，共 6
5、 页文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 H
6、K6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6
7、K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 H
8、K6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6
9、K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 H
10、K6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6
11、K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3大学物理下学期考前复习3 祝 3 班同学逢考必过！的求解方法：解析法00anxvarct和旋转矢量法2)同方向同频率简谐振动的合成111costAx222costAx总位移21xxx，合振动tAxcos解析法12212221cos2AAAAA ,22112211coscossinsinAAAAarctg3)振动总能量221KAEEEPK，振动势能)(co
12、skA2121222tKxEP振动动能 Ek=12mv2=13kA2sin2(t+)第十章机械波1)若已知波源O点振动方程 yo=Acos(t+),则该波的波动方程为)x-t2cosy)x-2cosy)x-cosTAvtAvtAy（或（或（2)体积元的能量xtAdVdEdEpk222sin21平均能量密度2221Aw平均能流密度（波动强度）uAwSPI2221u（u为波速）平均能流AVSwP221（V为介质体积，为介质长度，S 为介质侧面积）3）波的干涉条件：振动方向相同，频率相同和位相差恒定?=2干涉加强2-1-2(r2-r1)=2k (k=0、1、2?)A=A1+A2)210(r1212、
13、则波程差若kkr干涉减弱2-1-2(r2-r1)=(2k+1)(k=0、1、2?)A=|A1-A2|)210(12r1212、）（则波程差若kkr4）驻波含义：振幅相同，沿同一直线上相向传播的两列相干波产生的干涉5）以丛波为例，设两列相干波的波动方程为表示它们的频率其中xtAvxtAxtAvxtA2coscosy2coscosy21|精.|品.|可.|编.|辑.|学.|习.|资.|料.*|*|*|*|欢.|迎.|下.|载.第 3 页，共 6 页文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8
14、R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4
15、 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8
16、R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4
17、 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8
18、R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4
19、 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8
20、R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3大学物理下学期考前复习4 祝 3 班同学逢考必过！txAxtAxtAy2cos2cos22cos2cosyy216）相邻波节间各点位相相同，波节两侧点位相相反。相邻波节间距=相邻波腹间距=xk+1-xk=2。驻波无波形传播，无能量传播。7）半波损失发生在光从波疏介质入射到波密介质时发生反射的反射波上。第十三章波动光学基础一、杨氏双缝干涉(分波阵面法干涉)1、Dxdddrtansinr12波程差2、明纹位置：kDxd),2,1,0k(3、暗纹位置：2)12(dDkx),2,1,0(k4、相邻明（暗）纹间距dD
21、x4、若用白光照射，则除了中央明纹（k=0 级）是白色之外，其余明纹为彩色。二、分振幅法干涉1、薄膜干涉（若两束反射光中有一束发生半波损失，则光程差在原来的基础上再加上2；若两束光都有半波损失或都没有，则无需加上2）以下结果发生在入射光垂直入射时)(),2,1,0(212)(),2,1(2sin222122暗纹）（明纹kkkkinnd2、劈尖干涉（出现的是平行直条纹）1）明、暗条纹的条件：)(),2,1,0(2)12()(),2,1(22暗纹明纹kkkknd2）相邻明纹对应劈尖膜的厚度差为n2e1kkkddd）（图中为3）相邻明（暗）纹间距为nnL2sin23、牛顿环（同心环形条纹，明暗环条件
22、同劈尖干涉）1）明环和暗环的半径：)(),2,1,0()(),2,1(2)12(暗环明环knkRrknRkr|精.|品.|可.|编.|辑.|学.|习.|资.|料.*|*|*|*|欢.|迎.|下.|载.第 4 页，共 6 页文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1
23、ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P
24、3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1
25、ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P
26、3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1
27、ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P
28、3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3大学物理下学期考前复习5 祝 3 班同学逢考必过！相邻明环、暗环所对应的膜厚度差为n21kkkddd。三、迈克尔逊干涉仪 1）可移动反射镜
29、移动距离d 与通过某一参考点条纹数目N的关系为2Nd2）在某一光路中插入一折射率n,厚 d 的透明介质薄片时，移动条纹数N与 n、d 的关系为21nNd）（五、夫琅禾费衍射1、明纹条件：),2,1(2)12(sin0kka（中央明纹）2、暗纹条件：),2,1(sinkka3、中央明纹宽度（为1级暗纹间距离）：a2sin2tan20fffl其它暗纹宽度：2sinsintantan111okkkkkklafffffxxl4、半波带数：明纹（又叫极大）为(2k+1);暗纹（又叫极小）为（2k）。六、衍射光栅1、光栅常数d=a(透光宽度)+b（不透光宽度）=单位长度内刻痕（夹缝）数的倒数2、光栅方程)
30、,2,1,0(sin)kkba（明纹（满足光栅方程的明纹称为主极大明纹）k=0、1、2、3称为 0 级、1 级、2 级、3 级明纹3、缺级条件主极大消失、如果、如果、如果（1284449633364222ksinsin)kkabakkabakkabakabakakba七、光的偏振1、马吕斯定律2cos（为入射偏振光的振动方向与偏振片的偏振化方向间的夹角）2、布儒斯特定律120annnit，0i称为布儒斯特角或起偏角。当入射角为布儒斯特角时，反射光为垂直于入射面的线偏振光，并且该线偏振光与折射光线垂直。第十五章量子物理一、光电效应1、光电效应方程Wmhm221（式中表示光子的频率，W表示逸出功）
31、|精.|品.|可.|编.|辑.|学.|习.|资.|料.*|*|*|*|欢.|迎.|下.|载.第 5 页，共 6 页文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编
32、码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S
33、2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编
34、码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S
35、2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编
36、码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S
37、2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3大学物理下学期考前复习6 祝 3 班同学逢考必过！02 U21emm（0U表示遏止电压）0hW（0表示入射光最低频率/红限频率）2、说明了光具有粒子性。3、光的波粒二象性能量：h动量：22chmmc光子动量：hchmcp二、康普顿效应1、散射公式
38、2sin22sin22200ccmh2、说明了光具有粒子性。三、氢原子光谱1、实验规律（表示每一条光谱线的波数，HR（里德伯常数）=1.097*107m-1）氢原子在可见光部分)543(121122、nnRHfn=1 时为赖漫系，fn=2 时为巴耳末系，fn=3 时为帕邢系，fn=4 时为布喇系，fn=5 时为普芳德系132111122fififHnnnnnR、2、轨道半径12rnrn（53.01r*10-10m）(n=1、2、3)氢原子轨道能量121EnEn（eVE6.131）1n称为基态能量；2n称为第一激发态；n=3 称为第二激发态电离能取轨道能量的正值四、实物粒子的波粒二象性1、德布罗
39、意波Ph测不准关系2xPx（一定的数值）2、波函数1）归一化波函数xanaxnsin2)(（ax0）概率密度为2)(xnandxx021)(粒子能量)321(8222、nmahnEn2）标准化条件单值性，有限性，连续性|精.|品.|可.|编.|辑.|学.|习.|资.|料.*|*|*|*|欢.|迎.|下.|载.第 6 页，共 6 页文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4
40、K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4
41、X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4
42、K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4
43、X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4
44、K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3文档编码:CY9P3T1L4K4 HK6K9S2O2N1 ZE8M4X8R6K3