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Faraday’s law Accelerated electron creates time-varying current, time-varying current creates time-varying magnetic field, time-varying magnetic field.

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Presentation on theme: "Faraday’s law Accelerated electron creates time-varying current, time-varying current creates time-varying magnetic field, time-varying magnetic field."— Presentation transcript:

1 Time-varying fields and coupling between E/M fields Maxwell’s equations

2 Faraday’s law Accelerated electron creates time-varying current, time-varying current creates time-varying magnetic field, time-varying magnetic field will create electric field vortex Explanation – sourceless and isolated natural system tend to eliminate any disturbance, with time evolution towards its eigen state: if a time-varying magnetic field is enforced without any other source involved, an electric field vortex will have to be induced, to establish yet another magnetic field with an opposite change towards a cancellation of the total field, hence Faraday’s law holds electromotive force or emf

3 A second way to generate E field
Accelerated charge causes a time-varying charge distribution, leading to a time-varying current; from Ampere’s law, time-varying magnetic field exists; from Faraday’s law, electric vortex exists Therefore, not only electric field can be generated in its divergence form by the static charge distribution, it can also be generated in its curl form by the “temporary” charge distribution The electric field is brought in by both its divergence and curl, following the Helmholtz theorem, the electric field is complete Hence, time-varied magnetic field excites electric field, electric and magnetic fields become coupled; however, such coupling is still unidirectional

4 A map showing all relations
Static charge Moving charge, static charge distribution (constant current) Time-varying charge distribution (time-varying current, temporary charge) Static Electric Field Div. Static Magnetic Curl Time-varying magnetic field electric field Charge conservation law Gauss’s law Ampere’s law Faraday’s law (Derived from Coulomb’s law) (Derived from Biot-Savert’s law)

5 Displacement current Contradiction found between Ampere’s law and the charge conservation law Maxwell mended Ampere’s law, solved the problem Gaussian law is called

6 Mutual coupling between dynamic E/M fields
Significance – similar to a current, a time-varying electric field can generate magnetic field Hence the time-varying rate of the electric displacement vector is equivalent to a current, named as the displacement current; the conventional current caused by the moving charge is then called the conduction current to make a difference Not only time-varying magnetic field, equivalent to temporary charges, can excite electric field, time-varying electric field, equivalent to a “temporary” current (i.e., the displacement current), can also excite magnetic field Finally, electric and magnetic fields are fully coupled through mutual excitation

7 Significance of E/M mutual coupling
Therefore 1. accelerated charge creates time-varying magnetic field in its neighborhood (through the time-varying conduction current and following Ampere’s law); 2. time-varying magnetic field excites electric field in its neighborhood (through Faraday’s law) 3. time-varying electric field excites magnetic field in its neighborhood (through Ampere’s law) Step 2 and 3 form a sustainable loop, and make electric-magnetic fields propagation! Such an electric-magnetic non-local oscillation is named as the electromagnetic wave

8 Maxwell’s equations in vacuum: differential form
Faraday’s law Modified Ampere’s law (by Maxwell), derived from Biot-Savert’s law Gaussian law, derived from Coulomb’s law Gaussian law, derived from Biot-Savert’s law 8 equations with one in redundant, e.g., the 4th equation is embedded in the 1st equation

9 Maxwell’s equations in vacuum: integral form
Faraday’s law Modified Ampere’s law (by Maxwell), derived from Biot-Savert’s law Gaussian law, derived from Coulomb’s law Gaussian law, derived from Biot-Savert’s law The differential form is more general. The integral form is usually ill-posed, can only be used when the system has a high symmetry. Take it as a home work to prove the integral form from the differential form.


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