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Electromagnetism Ch.7 Methods of Math. Physics, Friday 8 April 2011, EJZ Inductors and inductance Waves and wave equations Electromagnetism & Maxwell’s.

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Presentation on theme: "Electromagnetism Ch.7 Methods of Math. Physics, Friday 8 April 2011, EJZ Inductors and inductance Waves and wave equations Electromagnetism & Maxwell’s."— Presentation transcript:

1 Electromagnetism Ch.7 Methods of Math. Physics, Friday 8 April 2011, EJZ Inductors and inductance Waves and wave equations Electromagnetism & Maxwell’s eqns Derive EM wave equation and speed of light

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4 Faraday’s Law

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9 Break time…

10 Waves

11 Wave equation 1. Differentiate d D/ d t  d 2 D/ d t 2 2. Differentiate d D/ d x  d 2 D/ d x 2 3. Find the speed from

12 Causes and effects of E Gauss: E fields diverge from charges Lorentz force: E fields can move charges F = q E

13 Causes and effects of B Ampere: B fields curl around currents Lorentz force: B fields can bend moving charges F = q v x B = IL x B

14 Changing fields create new fields! Faraday: Changing magnetic flux induces circulating electric field Guess what a changing E field induces?

15 Changing E field creates B field! Current piles charge onto capacitor Magnetic field doesn’t stop Changing electric flux →“displacement current” → magnetic circulation

16 Partial Maxwell’s equations Charge → E fieldCurrent → B field Faraday Changing B → E Ampere Changing E → B

17 Maxwell eqns → electromagnetic waves Consider waves traveling in the x direction with frequency f =   and wavelength =  /k E(x,t)=E 0 sin (kx-  t) and B(x,t)=B 0 sin (kx-  t) Do these solve Faraday and Ampere’s laws?

18 Faraday + Ampere

19 Sub in: E=E 0 sin (kx-  t) and B=B 0 sin (kx-  t)

20 Speed of Maxwellian waves? Faraday:   = k E 0 Ampere:      E 0 =kB 0 Eliminate B 0 /E 0 and solve for v=  /k    x 10 -7 Tm/A   = 8.85 x 10 -12 C 2 N/m 2

21 Maxwell equations → Light E(x,t)=E 0 sin (kx-  t) and B(x,t)=B 0 sin (kx-  t) solve Faraday’s and Ampere’s laws. Electromagnetic waves in vacuum have speed c and energy/volume = 1/2  0 E 2 = B 2 /(2  0 )

22 Full Maxwell equations in integral form

23 Integral to differential form Gauss’ Law: apply Divergence Thm: and the Definition of charge density: to find the Differential form:

24 Integral to differential form Ampere’s Law: apply Curl Thm: and the Definition of current density: to find the Differential form:

25 Integral to differential form Faraday’s Law: apply Curl Thm: to find the Differential form:

26 Finish integral to differential form…

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28 Maxwell eqns in differential form


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