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1 《电磁波基础及应用》沈建其讲义 Chapter 2. Maxwell equations 1) Displacement current 2) Maxwell equations 3) Boundary conditions of time-dependent electromagnetic field.

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Presentation on theme: "1 《电磁波基础及应用》沈建其讲义 Chapter 2. Maxwell equations 1) Displacement current 2) Maxwell equations 3) Boundary conditions of time-dependent electromagnetic field."— Presentation transcript:

1 1 《电磁波基础及应用》沈建其讲义 Chapter 2. Maxwell equations 1) Displacement current 2) Maxwell equations 3) Boundary conditions of time-dependent electromagnetic field 4) Poynting’s Theorem and Poynting’s Vector 5) The generalized definition of conductors and insulators 6) The Lorentz potential

2 2 ( 1 ) Gauss’ law in electrostatic field ( 2 ) The loop theorem of the electrostatic field 1. Basic principles of time-dependent electric and magnetic fields Conservative field ( 保守场 ) Active field 1) Displacement current

3 3 H 是涡旋场, 因为 它的旋度不为零 Passive field In the above four equations, D, E, B, H are the fields produced by rest charges or steady current. q is the sum of charges enclosed by Gauss’ surface, and I is algebraic sum of conduction current through the closed loop. ( 3 ) Gauss’ law for magnetic field ( 4 ) The loop theorem of the magnetostatic field

4 4 The relationship between the circulation ( 环量 ) of rotational field and the varying magnetic field is: The equation indicates that the varying magnetic field can produce a rotional electric field. Then a new question could be asked: can the varying electric field produce a magnetic field? ( 5 ) Faraday’s law of electromagnetic induction

5 5 2. Displacement current Assume that the capacitor is charged. The charges on plates A and B is +q and –q, respectively. The charge densities are +  and - , respectively. So, one can readily obtain

6 6 Due to the current continuity equation On the polar plate S 2 surface where J D is a displacement current density

7 7 Now Ampere’s law can be rewritten as: The differential form of Ampere’s law can be expressed as andin the loop C obey the right-hand screw rule

8 8 3. The relationship between the displacement current and the conduction current (I.e., the connection and difference between… ) (1) They can both produce the magnetic field with the same strength, provided that the displacement current and the conduction current have the same current density. 位移电流与传导电流在产生磁效应上是等价的. (2)They are produced in different ways (They originate from different sources): specifically, the conduction current is caused by the motion of the free charges, while the physical essence of the displacement current is the varying electric field. (3)They will exhibit different effects when passing through the metal conductor: the conduction current can produce the Joule heat while the displacement current cannot.

9 9 Example: the conductivity of sea water is 4S/m and its relative dielectric constant is 81, determine the ratio of the displacement current to the conduction current at 1MHz frequency. We assume that the electric field is of the sinusoidal form, The density of the displacement current is The amplitude is given by The density of the conduction current is with the amplitude So,

10 10 1. Maxwell equation set in integral and differential forms 2) Maxwell equations (1)The characteristic of electric field ( 电场特性 ) Gauss’ law The dielectric flux through a closed surface equals the total charges Q inside the closed surface. Integral form The source of a electric field is the free charge Differential form

11 11 (2) The characteristic of magnetic field Continuity of magnetic flux Magnetic field is passive field. There is no free magnetic charge in nature.

12 12 (3) The relationship between the varying electric field and the magnetic field General Ampere law The integral of magnetic field strength H along closed loop C equals the sum of conduction current and displacement current The vorticity source of a magnetic field is the conduction current and displacement current.

13 13 (4) The relationship between the varying magnetic field and the electric field Faraday’s law of electromagnetic induction Time-dependent magnetic flux can produce electromotive force, the vorticity of an electric field is the time-dependent magnetic field

14 14 Maxwell equation set ( 需熟记 Maxwell 方程组,并明确各个方程的物理含义 ) Maxwell equation set ( 需熟记 Maxwell 方程组,并明确各个方程的物理含义 ) Integral form Differential form

15 15 2. Constitutive equation 材料的本构关系(方程)

16 16 3. The relationship between electric field and magnetic field chargecurrent Magnetic field Electric field motion varying Agitation (电流能激发 磁场) Agitation (电荷能激发 电场) varying

17 17 3) Boundary conditions of time-dependent electromagnetic field ( 电磁场边界条件, 具体讨论可见谢处方、饶克谨《电磁场与电磁波》 pp ) 1. Boundary condition of magnetic field strength H  1,  1  2,  2 h Rectangle loop in the interface J ST is the component of J vertical to  l. When h  0, the second term in the right equation is 0. Then we have When J S = 0 or tangential: 切向的 normal: 法向的

18 18 2. Boundary condition of electric field strength E When h  0, the right term in the above equation is 0 or  1,  1  2,  2 h Rectangle loop in the interface tangential: 切向的 normal: 法向的

19 19 3. Boundary condition of magnetic field strength B or The normal component of the magnetic flux density B in the interface is continuous 4. Boundary condition of dielectric flux density D When  S = 0 or

20 20 5. Summary of the boundary conditions or

21 21 or Interface of two passive media 无源,交界面上的边界条件

22 22 Ideal medium 1 and ideal conductor 2 理想介质1与理想导体2 or

23 23 4) Poynting’s Theorem and Poynting’s Vector Poynting’s theorem is the mathematical expression for the law of conservation of energy of the electromagnetic fields. Poynting’s vector describes the flow of electromagnetic energy. Poynting 定律是电磁能量的守恒定律,其中 Poynting 矢量的物理意义是:电 磁能流密度。

24 24 1. Poynting’s theorem Combine the above equations From Maxwell equation set, we have If we assume that the medium is linear, we can obtain

25 25 For linear media E i is impressed electric field, J  E i is the power of impressing (external) sources per unit volume. 外电源也产生了一个电场 If we substitute the above expression into the equation we have

26 26 Let us multiply this equation by a volume element d and integrate over an arbitrary volume of the field, we have The power of all the sources inside v Transformed inside v into heat (焦耳热) change rate of the energy localized in the electric and magnetic field inside v Power transferred through S to a region outside S How the power is classified

27 27 2. Poynting’s vector W/m 2 Energy flow density (能流密度)

28 28 Example: in passive free space, the time-dependent electromagnetic field is Determine: (1) magnetic field strength; ( 2 ) instantaneous Poynting’s vector ;( 3 ) average Poynting’s vector (1)

29 29 (2) (3)

30 30 5) The generalized definition of conductors and insulators ( 导体与绝缘体的推广定义 ) For linear media and time-harmonic (时谐) fields

31 31 Therefore 6) The Lorentz potential M agnetic vector potential and electric field strength in terms of retarded potentials ( 延迟势 ) magnetic vector potential ( Wb /m ) Scalar potential (V) Electric field strength in terms of retarded potential

32 32 If We get Helmholtz theorem

33 33 Lorentz condition: D’ Alembert’s equation ( 达兰伯方程 ) For sinusoidal electromagnetic field Lorentz condition:

34 34 说明:为什么要引入一个 Lorentz 条件? 在经典电动力学中,我们可以用E,B,H,D来描述电磁场.与之 等价的方案是,可以用上面提到的四维电磁势来代替E,B,H, D.但是我们发现,同一个电场E与磁场B可以对应无穷多套电磁 势.也就是说,对于描述电磁场,电磁势是 “ 超定的 ” ,不是 “ 欠定 的 ” .为了把电磁势定下来,我们需要额外的约束.这个约束条件就 是 Lorentz 条件.当然,约束条件是可以随意选的.我们不一定必须 选 Lorentz 条件.有时我们可以选择库仑规范. 无论选择什么约束条件,都是等价的.选择什么约束条件,主要看问 题方便而定.如为了照顾到狭义相对论不变性,我们就使用 Lorentz 条件.

35 35 Lorentz potential and gauge transformation ( 规范变换 ) can be written as This implies that the term in ( ) can be written as the gradient of a scalar potential V, i.e., At this stage it is convenient to consider only the vacuum case. Then the Maxwell equation 1) Vector and scalar potential

36 36 can be expressed in terms of the potentials as We have now reduced the set of four Maxwell equations to two equations. But they are still coupled. The uncoupling can be achieved by using the arbitrariness in the definition of the potentials.

37 37 2) Gauge Transformations, Lorentz Gauge, Coulomb Gauge We choose The transformations

38 38 * Lorentz Gauge Also,

39 39 These two equations are equivalent to 4 Maxwell equations. Under the Lorentz condition: In other words, as long as satisfies the above equation, the Lorentz condition preserves under the gauge transformation. ** Coulomb Gauge The solution is

40 40 The scalar potential is just the instantaneous Coulomb potential due to the charge density. This is the origin of the name “ Coulomb gauge ”. The vector potential satisfies The term involving the scalar potential V can, in principle, be calculated from the previous integral.

41 41 With the help of the continuity equation The Coulomb gauge is often used when no sources are present. Then V=0

42 42 谈谈电荷守恒和能量守恒 (A) 电荷守恒( charge conservation ) 什么是电荷守恒? 电荷守恒的数学表达式是什么? 答:古典的 “ 电荷守恒 ” 定律,是指电荷不能凭空创生,也不能凭空消失。 自从量子电动力学 (quantum electrodynamics) 诞生( 1940 年代)以来, 电荷可以创生,也可以湮灭,如一个高能光子( gamma 射线光子) 可以变成正负电子对,正电子(带正电)与普通电子(带负电)相遇 可以变成光子。 正电子质量与普通电子一样,只是带正电。反质子(带负电)与正 电子可以构成反氢原子,即反物质。反物质世界好比正物质世界的 “ 镜像世界 ” (如反物质世界的左、右定义与我们正物质世界的左、右 定义相反)。来自反物质世界的友好人士与你握手,你俩瞬间变为光 子和各种射线, 真正的 “ 灰飞烟灭 ” 。所以要谨慎交友。

43 43

44 44 (B) 能量守恒 (energy conservation)

45 45 动量守恒与 Lorentz 力公式的推导 值得一提的是, Poynting 定律(电磁学能量守恒定 律)是一个功率方程(其微分形式为功率密度方 程)。能量在时间上的变化率即为功率;能量在空 间上的变化率即为力。除了上述功率方程,由 Maxwell 方程组亦可以得到力方程,即含有 Lorentz 力公式的电磁学动量守恒定律。 由于其比较复杂,一般电动力学和电磁波理论教材都 不讲。在文件夹 “ 供学有余力或课时有多时讲授 ” 内 有一个 “Lorentz 力公式的推导.pdf”( 文题是:由 Maxwell 方程推导 Lorentz 力公式 ) 可供参考。


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