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今(Jin)日(Ri)分(Fen)享(Xiang)（十(Shi)六(Liu)）如(Ru)何(He)学(Xue)好(Hao)大(Da)学(Xue)物(Wu)理(Li)（5）电(Dian)学(Xue)总(Zong)结(Jie)2022-09-05 18:38·LearningYard学(Xue)苑(Yuan)今(Jin)日(Ri)分(Fen)享(Xiang)（十(Shi)六(Liu)）如(Ru)何(He)学(Xue)好(Hao)大(Da)学(Xue)物(Wu)理(Li)（5）电(Dian)学(Xue)总(Zong)结(Jie).mp33:09来(Lai)自(Zi)LearningYard学(Xue)苑(Yuan)分(Fen)享(Xiang)兴(Xing)趣(Qu)，传(Chuan)播(Bo)快(Kuai)乐(Le)，增(Zeng)长(Chang)见(Jian)闻(Wen)，留(Liu)下(Xia)美(Mei)好(Hao)！亲(Qin)爱(Ai)的(De)您(Nin)，这(Zhe)里(Li)是(Shi)LearningYard学(Xue)苑(Yuan)。今(Jin)天(Tian)小(Xiao)编(Bian)为(Wei)大(Da)家(Jia)带(Dai)来(Lai)今(Jin)日(Ri)分(Fen)享(Xiang)（十(Shi)六(Liu)），欢(Huan)迎(Ying)您(Nin)的(De)访(Fang)问(Wen)！Share interests, spread happiness, increase knowledge,and leave a good legacy!Dear you, this is The LearningYard Academy.Today Xiaobian brings you today's sharing (eleven), welcome your visit!静(Jing)电(Dian)场(Chang)电(Dian)荷(He)的(De)量(Liang)子(Zi)化(Hua)：任(Ren)何(He)带(Dai)电(Dian)体(Ti)所(Suo)带(Dai)电(Dian)量(Liang)是(Shi)最(Zui)小(Xiao)电(Dian)量(Liang)单(Dan)元(Yuan)的(De)整(Zheng)数(Shu)倍(Bei)q=±ne，(n=1、2、3......)Quantization of charge: The amount of electricity carried by any charged body is an integer multiple of the minimum charge unit q= ±ne, (n = 1, 2, 3......)电(Dian)荷(He)守(Shou)恒(Heng)定(Ding)律(Lv)：在(Zai)与(Yu)外(Wai)界(Jie)没(Mei)有(You)电(Dian)荷(He)交(Jiao)换(Huan)的(De)系(Xi)统(Tong)内(Nei)，无(Wu)论(Lun)进(Jin)行(Xing)怎(Zen)样(Yang)的(De)过(Guo)程(Cheng)，系(Xi)统(Tong)内(Nei)正(Zheng)负(Fu)电(Dian)荷(He)量(Liang)的(De)代(Dai)数(Shu)和(He)保(Bao)持(Chi)不(Bu)变(Bian)Law of Conservation of Charge: In a system without charge exchange with the outside world, the algebraic sum of the positive and negative charge amounts in the system remains constant regardless of the process库(Ku)仑(Lun)定(Ding)律(Lv)：只(Zhi)适(Shi)用(Yong)于(Yu)真(Zhen)空(Kong)中(Zhong)的(De)点(Dian)电(Dian)荷(He)Coulomb's law: Applies only to point charges in a vacuum电(Dian)场(Chang)基(Ji)本(Ben)性(Xing)质(Zhi)：1、电(Dian)场(Chang)对(Dui)放(Fang)入(Ru)电(Dian)场(Chang)中(Zhong)的(De)任(Ren)何(He)电(Dian)荷(He)都(Du)有(You)作(Zuo)用(Yong)力(Li)2、电(Dian)场(Chang)力(Li)对(Dui)电(Dian)场(Chang)中(Zhong)移(Yi)动(Dong)的(De)电(Dian)荷(He)做(Zuo)功(Gong)Basic properties of electric fields:1. The electric field has a force on any charge put into the electric field2. The electric field force works on the electric charge moving in the electric field电(Dian)场(Chang)强(Qiang)度(Du)：描(Miao)述(Shu)电(Dian)场(Chang)的(De)强(Qiang)弱(Ruo)和(He)方(Fang)向(Xiang)。把(Ba)一(Yi)个(Ge)试(Shi)探(Tan)电(Dian)荷(He)放(Fang)入(Ru)电(Dian)场(Chang)，判(Pan)断(Duan)电(Dian)荷(He)所(Suo)受(Shou)的(De)电(Dian)场(Chang)力(Li)，电(Dian)场(Chang)力(Li)与(Yu)电(Dian)荷(He)电(Dian)量(Liang)的(De)比(Bi)值(Zhi)。大(Da)小(Xiao)等(Deng)于(Yu)单(Dan)位(Wei)电(Dian)荷(He)在(Zai)该(Gai)点(Dian)的(De)受(Shou)力(Li)大(Da)小(Xiao)，方(Fang)向(Xiang)为(Wei)正(Zheng)电(Dian)荷(He)在(Zai)该(Gai)点(Dian)受(Shou)力(Li)的(De)方(Fang)向(Xiang)E=F/qElectric Field Strength: Describes the strength and direction of the electric field. Put a tentative charge into the electric field and determine the electric field force to which the charge is subjected, and the ratio of the electric field force to the charge charge. The size is equal to the magnitude of the force per unit charge at that point, and the direction is the direction in which the positive charge is forced at that pointE=F/q场(Chang)强(Qiang)叠(Die)加(Jia)原(Yuan)理(Li)（Principle of field strength superposition）：电(Dian)场(Chang)强(Qiang)度(Du)通(Tong)量(Liang)（Electric field strength flux）：高(Gao)斯(Si)定(Ding)理(Li)：可(Ke)计(Ji)算(Suan)具(Ju)有(You)对(Dui)称(Cheng)性(Xing)的(De)电(Dian)场(Chang)的(De)电(Dian)场(Chang)强(Qiang)度(Du)Gauss's theorem: The electric field intensity of an electric field with symmetry can be calculated电(Dian)势(Shi)能(Neng)：反(Fan)应(Ying)的(De)是(Shi)一(Yi)个(Ge)电(Dian)荷(He)与(Yu)电(Dian)场(Chang)共(Gong)同(Tong)组(Zu)成(Cheng)的(De)系(Xi)统(Tong)的(De)性(Xing)质(Zhi)W=∫qEdlElectric Potential Energy: It reflects the properties of a system of charge and electric fieldW=∫qEdl电(Dian)势(Shi)：反(Fan)映(Ying)电(Dian)场(Chang)本(Ben)身(Shen)的(De)性(Xing)质(Zhi)，与(Yu)电(Dian)荷(He)无(Wu)关(Guan)，所(Suo)以(Yi)表(Biao)达(Da)式(Shi)里(Li)无(Wu)q.V=∫EdlPotential: Reflects the properties of the electric field itself and has nothing to do with the charge, so there is no q in the expression.V=∫Edl静(Jing)电(Dian)场(Chang)中(Zhong)的(De)导(Dao)体(Ti)和(He)电(Dian)解(Jie)质(Zhi)自(Zi)由(You)电(Dian)子(Zi)：导(Dao)体(Ti)内(Nei)可(Ke)自(Zi)由(You)移(Yi)动(Dong)的(De)电(Dian)子(Zi)Free electrons: Freely movable electrons in the conductor静(Jing)电(Dian)平(Ping)衡(Heng)：导(Dao)体(Ti)上(Shang)没(Mei)有(You)电(Dian)荷(He)作(Zuo)宏(Hong)观(Guan)定(Ding)向(Xiang)运(Yun)动(Dong)的(De)状(Zhuang)态(Tai)Electrostatic equilibrium: there is no charge on the conductor for macroscopic directional motion静(Jing)电(Dian)平(Ping)衡(Heng)条(Tiao)件(Jian)：导(Dao)体(Ti)内(Nei)场(Chang)强(Qiang)处(Chu)处(Chu)为(Wei)0Electrostatic equilibrium conditions: the conductor's internal field strength is 0 everywhere电(Dian)介(Jie)质(Zhi)的(De)极(Ji)化(Hua)：外(Wai)电(Dian)场(Chang)作(Zuo)用(Yong)下(Xia)，电(Dian)介(Jie)质(Zhi)显(Xian)示(Shi)电(Dian)性(Xing)的(De)现(Xian)象(Xiang)。一(Yi)般(Ban)情(Qing)形(Xing)下(Xia)，未(Wei)经(Jing)电(Dian)场(Chang)作(Zuo)用(Yong)的(De)电(Dian)介(Jie)质(Zhi)内(Nei)部(Bu)的(De)正(Zheng)负(Fu)束(Shu)缚(Fu)电(Dian)荷(He)平(Ping)均(Jun)说(Shuo)来(Lai)处(Chu)处(Chu)抵(Di)消(Xiao)，宏(Hong)观(Guan)上(Shang)并(Bing)不(Bu)显(Xian)示(Shi)电(Dian)性(Xing)。Polarization of the dielectric: Under the action of the external electric field, the dielectric shows the phenomenon of electrical properties. In general, the positive and negative bound charges inside the dielectric without the action of the electric field are offset on average, and the macroscopic level does not show electrical properties.极(Ji)化(Hua)：在(Zai)外(Wai)电(Dian)场(Chang)的(De)作(Zuo)用(Yong)下(Xia)，束(Shu)缚(Fu)电(Dian)荷(He)的(De)局(Ju)部(Bu)移(Yi)动(Dong)导(Dao)致(Zhi)宏(Hong)观(Guan)上(Shang)显(Xian)示(Shi)出(Chu)电(Dian)性(Xing)，在(Zai)电(Dian)介(Jie)质(Zhi)的(De)表(Biao)面(Mian)和(He)内(Nei)部(Bu)不(Bu)均(Jun)匀(Yun)的(De)地(Di)方(Fang)出(Chu)现(Xian)电(Dian)荷(He)，出(Chu)现(Xian)的(De)电(Dian)荷(He)称(Cheng)为(Wei)极(Ji)化(Hua)电(Dian)荷(He)。充(Chong)满(Man)电(Dian)介(Jie)质(Zhi)的(De)电(Dian)容(Rong)器(Qi)比(Bi)真(Zhen)空(Kong)电(Dian)容(Rong)器(Qi)的(De)电(Dian)容(Rong)大(Da)就(Jiu)是(Shi)由(You)于(Yu)电(Dian)介(Jie)质(Zhi)的(De)极(Ji)化(Hua)作(Zuo)用(Yong)。Polarization: Under the action of the external electric field, the local movement of the bound charge causes the macroscopic display of electricity, and the charge appears on the surface and internal unevenness of the dielectric, and the charge that appears is called the polarized charge. The larger capacitance of a dielectric-filled capacitor than a vacuum capacitor is due to the polarization of the dielectric.电(Dian)位(Wei)移(Yi)矢(Shi)量(Liang)：是(Shi)一(Yi)个(Ge)用(Yong)以(Yi)描(Miao)述(Shu)电(Dian)场(Chang)的(De)辅(Fu)助(Zhu)物(Wu)理(Li)量(Liang)，用(Yong)符(Fu)号(Hao)D表(Biao)示(Shi)。Electric displacement vector: is an auxiliary physical quantity used to describe the electric field, denoted by the symbol D.定(Ding)义(Yi)式(Shi)为(Wei)：D=ε0E+PThe definition is: D=ε0E+P电(Dian)容(Rong)器(Qi)的(De)电(Dian)容(Rong)：C=Q/UThe capacitance of the capacitor: C=Q/U电(Dian)场(Chang)的(De)能(Neng)量(Liang)：是(Shi)电(Dian)场(Chang)所(Suo)具(Ju)有(You)的(De)能(Neng)量(Liang)，等(Deng)于(Yu)电(Dian)场(Chang)能(Neng)量(Liang)密(Mi)度(Du)对(Dui)电(Dian)场(Chang)所(Suo)处(Chu)空(Kong)间(Jian)的(De)积(Ji)分(Fen)。The energy of the electric field: it is the energy of the electric field, which is equal to the integral of the energy density of the electric field to the space at the electric field.今(Jin)天(Tian)的(De)分(Fen)享(Xiang)就(Jiu)到(Dao)这(Zhe)里(Li)了(Liao)。如(Ru)果(Guo)您(Nin)对(Dui)今(Jin)天(Tian)的(De)文(Wen)章(Zhang)有(You)什(Shi)么(Me)独(Du)特(Te)的(De)想(Xiang)法(Fa)，欢(Huan)迎(Ying)评(Ping)论(Lun)留(Liu)言(Yan)，让(Rang)我(Wo)们(Men)相(Xiang)约(Yue)明(Ming)天(Tian)，祝(Zhu)您(Nin)今(Jin)天(Tian)过(Guo)得(De)开(Kai)心(Xin)快(Kuai)乐(Le)！That's it for today's sharing.If you have any unique ideas for today's article, please leave a comment, let us meet tomorrow,I wish you a happy day!
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总(窜辞苍驳)之(窜丑颈)，无(奥耻)论(尝耻苍)是(厂丑颈)在(窜补颈)宁(狈颈苍驳)静(闯颈苍驳)的(顿别)城(颁丑别苍驳)市(厂丑颈)道(顿补辞)路(尝耻)，还(贬耻补苍)是(厂丑颈)在(窜补颈)宽(碍耻补苍)广(骋耻补苍驳)的(顿别)高(骋补辞)速(厂耻)公(骋辞苍驳)路(尝耻)上(厂丑补苍驳)，正(窜丑别苍驳)确(蚕耻别)选(齿耻补苍)择(窜别)和(贬别)使(厂丑颈)用(驰辞苍驳)挡(顿补苍驳)位(奥别颈)，都(顿耻)是(厂丑颈)确(蚕耻别)保(叠补辞)行(齿颈苍驳)车(颁丑别)安(础苍)全(蚕耻补苍)、提(罢颈)高(骋补辞)驾(闯颈补)驶(厂丑颈)体(罢颈)验(驰补苍)的(顿别)重(窜丑辞苍驳)要(驰补辞)环(贬耻补苍)节(闯颈别)。希(齿颈)望(奥补苍驳)每(惭别颈)一(驰颈)位(奥别颈)车(颁丑别)主(窜丑耻)都(顿耻)能(狈别苍驳)够(骋辞耻)根(骋别苍)据(闯耻)自(窜颈)己(闯颈)的(顿别)实(厂丑颈)际(闯颈)驾(闯颈补)驶(厂丑颈)需(齿耻)要(驰补辞)，灵(尝颈苍驳)活(贬耻辞)地(顿颈)掌(窜丑补苍驳)握(奥辞)和(贬别)运(驰耻苍)用(驰辞苍驳)顿挡(顿补苍驳)和(贬别)厂挡(顿补苍驳)，让(搁补苍驳)驾(闯颈补)驶(厂丑颈)变(叠颈补苍)得(顿别)更(骋别苍驳)加(闯颈补)得(顿别)心(齿颈苍)应(驰颈苍驳)手(厂丑辞耻)。记(闯颈)住(窜丑耻)，无(奥耻)论(尝耻苍)选(齿耻补苍)择(窜别)哪(狈补)个(骋别)挡(顿补苍驳)位(奥别颈)，都(顿耻)应(驰颈苍驳)以(驰颈)安(础苍)全(蚕耻补苍)为(奥别颈)先(齿颈补苍)，确(蚕耻别)保(叠补辞)每(惭别颈)次(颁颈)行(齿颈苍驳)车(颁丑别)都(顿耻)是(厂丑颈)平(笔颈苍驳)稳(奥别苍)且(蚕颈别)高(骋补辞)效(齿颈补辞)的(顿别)。
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