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Review basic knowledge points of engineering electromagnetic field
2022-07-28 03:16:00 【Kyle942】
Chapter one Vector analysis and field theory 1 Source point refers to . 2 Field point refers to . 3 The distance vector is , The unit vector representing its direction is expressed by Express . 4 The isosurface equation of scalar field is expressed as , The vector line equation can be expressed in coordinate form , It can also be expressed in vector form . 5 Gradient is a tool for studying scalar fields , Modular representation of gradient , The direction of the gradient indicates . 6 The relationship between directional derivative and gradient is .

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Chapter two electrostatic field
1 Point charge q The formula for calculating the electric field intensity generated in space is .
2 Point charge q The calculation formula of the potential generated in space is .

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6 A conductor in static equilibrium , The direction of the electric field intensity on the surface of the conductor follows .
7 A conductor in static equilibrium , The electric field intensity inside the conductor is equal to .
8 A conductor in static equilibrium , The relationship between internal potential and external potential is .
9 A conductor in static equilibrium , Its internal charge volume density is .
10 A conductor in static equilibrium , The charge is distributed on the surface of the conductor .

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17 Volume density of polarized charge in medium

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20 Potential shift vector D, Electric field intensity vector E The relationship between is .
21 Dielectric strength refers to .
22 In electrostatic field , The curl of the electric field intensity is equal to .
23 In electrostatic field , The divergence of the electric displacement vector is equal to .
24 In electrostatic field , The line integral of the electric field intensity along any closed path is equal to .
25 In electrostatic field , The flux of the electric displacement vector on any closed surface is equal to .
26 In electrostatic field , The interface condition of electric field strength is .
27 In electrostatic field , The interface condition of the electric displacement vector is .
28 In electrostatic field , The Poisson equation satisfied by the potential is .
29 In electrostatic field , The interface condition satisfied by the potential is .
30 In electrostatic field , The normal derivative of potential at the interface of two media satisfies .
31 In electrostatic field , The tangential derivative of the potential at the interface between the two media satisfies .
32 In electrostatic field , The normal derivative of potential on the interface of conductor and medium satisfies .
33 In electrostatic field , The tangential derivative of potential at the interface of conductor and medium satisfies .
34 The first kind of boundary condition in electrostatic field boundary value problem is .
35 The second kind of boundary condition in electrostatic field boundary value problem is .
36 The third kind of boundary condition in electrostatic field boundary value problem is .
37 Elementary charge dq The formula for calculating the electric field intensity generated in space is .
38 Elementary charge dq The calculation formula of the potential generated in space is .
39 The differential form of the basic equation of electrostatic field is .
40 The boundary value problem of electrostatic field refers to .
The third chapter Constant electric field
1 The unit of Bulk current density is .
2 The unit of surface current density is .
3 The relationship between bulk current density and charge velocity is .
4 The relationship between surface current density and charge velocity is .
5 The relationship between current density and electric field intensity is .
6 The definition of external electric field is .
7 The definition of power electromotive force is .
8 The mathematical expression of the integral form of the current continuity equation is .
9 The mathematical expression of the differential form of the current continuity equation is .
10 The mathematical expression of the integral form of the current continuity equation in a constant electric field is .
11 The mathematical expression of the differential form of the current continuity equation in a constant electric field is .
12 The basic equation of constant electric field is .
13 The auxiliary equation of constant electric field is .
14 The differential form of Ohm's law is .
15 The relationship between electric field intensity and potential of constant electric field is .
16 The equation satisfied by the constant electric field potential outside the power supply is .
17 On the interface of two conductive media in a constant electric field , The interface condition of current density is .
18 In a constant electric field, when the conductivity of the conductive medium is known , On the interface , The interface condition satisfied by the normal derivative of potential is .
Chapter four Constant magnetic field
1 Volume current element 、 Area current element and line current element are respectively expressed as 、 、 .

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10 The Coulomb specification is expressed as .
11 Surfaces S The magnetic flux on the surface is Flux of , Expressed as .
12 The formula for calculating magnetic flux with vector magnetic potential is .
13 The continuous differential of magnetic flux is expressed as .
14 The magnetic induction line equation is expressed in the form of coordinates , Expressed as a vector, the form is .
15 In a parallel plane field , Magnetic induction line is .
16 The curl of magnetic induction intensity is equal to .
17 The radius is R There is current in the straight wire of I, The current is evenly distributed , The magnetic induction intensity inside the conductor is , The external magnetic induction intensity is .
18 There is current distribution on the infinite plane , Current area density K Is a constant vector , The magnetic induction intensity on both sides of the plane is .
19 A magnetic dipole is a small enclosed current carrying circuit , Set the loop area as S, The loop current is I, Then the magnetic dipole moment of the magnetic dipole m= .
20 Magnetization M The physical meaning of is .
21 Bulk density of magnetizing current JM= .
22 Area density of magnetizing current KM= .
23 Magnetic field intensity H, Magnetic induction intensity B, Magnetization M The relationship between .
24 For linear 、 Isotropic medium , Magnetic field intensity H And magnetic induction B The relationship between .
25 The differential form of the basic equation of the constant magnetic field is .
26 The auxiliary equation of the constant magnetic field is .
27 The interface condition of magnetic induction intensity is .
28 The interface condition of magnetic field strength is .
29 When there is no free current on the interface , The interface condition of magnetic field strength is .
30 The curl of the magnetic field intensity is equal to .
31 The line integral of the magnetic field intensity along any closed loop is equal to that around the loop .
32 The Poisson equation of vector magnetic potential is .
The fifth chapter Time varying electromagnetic field
1 The essence of Faraday's law of electromagnetic induction is the generation of a changing magnetic field .
2 Transformer electromotive force refers to .
3 Electromotive force of generator refers to .
4 The electric field generated by the changing magnetic field is called the induced electric field , The curl of the induced electric field is equal to .
5 Displacement current density is defined as JD= .
6 There are three forms of current , Respectively , , , The corresponding current density forms are , , .
7 The essence of the displacement current hypothesis is the generation of a changing electric field .
8 The differential form of the law of total current is .
9 Write the integral form of Maxwell's equations and its auxiliary equations .
10 Write the differential form of Maxwell's equations and its auxiliary equations .
11 The refraction law of electric field intensity on the interface of two media is .
12 The refraction law of the magnetic field intensity on the interface between two media is .
13 Write the differential form of Maxwell's equations in vector form and its auxiliary equations .
Chapter six Mirror method
1 The theoretical basis for implementing the mirror image method is .
2 In the process of implementing the image method , What cannot be changed is , ,
, What can be changed is , .
3 Write down the steps to implement the mirror method .
4 Above an infinite conductor h There is a little charge at q, Then the electric field intensity at any point in the upper half space is .
5 Above an infinite conductor h There is a little charge at q, The distribution law of electric field intensity on the surface of conductor is .
6 Above an infinite conductor h There is a little charge at q, The distribution law of the area density of the induced charge on the surface of the conductor is .
7 The boundary potential of the rectangular region is 0, The distance from a point charge to the two boundaries is a,b, Take the rectangular region as the region for solving the electric field , Write the mirror charge .
8 The radius of grounding conductor ball is R, Ball outer distance ball center d There is a little charge at q, Take the outside of the conductor sphere as the solution space , Then mirror charge q’= , Distance from the ball center .
9 The radius of grounding conductor ball is R, Ball outer distance ball center d There is a little charge at q, Then the electric field intensity outside the conductor is .
10 The radius of grounding conductor ball is R, Ball outer distance ball center d There is a little charge at q, Then the upper distance of the conductor sphere q The electric field intensity at the nearest point is , distance q The electric field intensity at the farthest point is .
11 The radius of grounding conductor ball is R, Ball outer distance ball center d There is a little charge at q, Then the induced charge surface density on the conductor sphere is .
12 The radius of ungrounded conductor ball is R, Ball outer distance ball center d There is a little charge at q, Then the conductor spherical potential is .
13 From the infinite dielectric interface h Place a little charge at q, The point charge is in the first medium , The dielectric constants of the two media are

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, Take the first medium as the solution region , Then the mirror charge is , Position in , The electric field intensity at any point in the upper half space is .
14 From the infinite dielectric interface h Place a little charge at q, The point charge is in the first medium , The dielectric constants of the two media are

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, Take the second medium as the solution region , Then the mirror charge is , Position in , The electric field intensity at any point in the lower half space is .
Chapter viii. Energy and force of electromagnetic field
1 It is known that n The charge of each conductor is

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, Potential

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, The electric field energy of the electrostatic system is .
2 The potential shift vector of the known electric field D And electric field strength E, Then the volume density of the electric field energy distribution is .

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6 The magnetic induction intensity of a known magnetic field B And magnetic field strength H, Then the volume density of the magnetic field energy distribution is .
7 Poyinting vector Sp= , Physical meaning .
8 When the potential remains constant , About generalized coordinates g Generalized electric field force fg= , When the power remains unchanged , About generalized coordinates g Generalized electric field force fg= .
9 When the current is constant , About generalized coordinates g Generalized magnetic force fg= , When the flux linkage does not change , About generalized coordinates g Generalized magnetic force fg= .
10 When the generalized coordinates are angles , The generalized force calculated by the virtual displacement method is .
Chapter nine Plane electromagnetic wave
1 The uniform plane electromagnetic wave in infinite ideal medium is TEM wave , The direction of the electric field 、 The relationship between the direction of magnetic field and the direction of wave propagation is .
2 The ratio of electric field strength to magnetic field strength of uniform plane electromagnetic wave in ideal medium is .

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5 The wave impedance of vacuum medium is .
6 It is proved that the electric field energy density of plane electromagnetic wave in ideal medium is equal to the magnetic field energy density .
7 The phase relationship between the electric field intensity and the magnetic field intensity of plane electromagnetic waves in an ideal medium is .
8 The frequency is f, The speed of propagation is v The plane electromagnetic wave propagates in the ideal medium , The phase constant is , Its physical meaning is .

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16 Penetration depth is defined as , The relationship with attenuation constant is .
17 The relationship between attenuation constant and phase constant in a good conductor is .
18 The penetration depth of electromagnetic wave in a good conductor is

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, therefore , For high-frequency electromagnetic waves , Electromagnetic fields can only exist in the , This phenomenon is called .
Chapter ten Calculation principle of circuit parameters

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