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Magnetic Fields in Matter Chapter 6. 2  Magnetization.

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Presentation on theme: "Magnetic Fields in Matter Chapter 6. 2  Magnetization."— Presentation transcript:

1 Magnetic Fields in Matter Chapter 6

2 2  Magnetization

3 3

4 4 Torques and Forces on Magnetic Dipoles rotation

5 5  Magnetization random paramagnetism Diamagnetism External B field Ferromagnetism

6 6  Magnetization Force on magnetic dipole Case of uniform field (B=constant): 0

7 7  Magnetization x y Case of nonuniform field (B ≠ constant): I B Fringing field

8 8  Magnetization I y z x

9 9 I y z x

10 10  Magnetization Electric dipole - + Magnetic dipole S N Gilbert model I Ampere model

11 11  Magnetization Effect of magnetic field on atomic orbits

12 12  Magnetization only electric force add magnetic field

13 13  Magnetization when B is turn on,the electron speeds up.

14 14  Magnetization

15 15  Bound Currents

16 16  Bound Currents

17 17  Bound Currents 0

18 18  Bound Currents --Using Biot-Savart law

19 19  Bound Currents Exp 1: Find the magnetic field at the center of a uniformly magnetized sphere.

20 20  Bound Currents Exp 1:

21 21  Bound Currents Exp 1: R θ

22 22  Bound Currents Exp 1: b

23 23  Bound Currents Find the magnetic field of point P. Find the magnetic field of point P.

24 24  Bound Currents    u R

25 25  Physical Interpretation of Bound Currents When the magnetization is uniform:

26 26 When the magnetization is nonuniform:  Physical Interpretation of Bound Currents

27 27  The Auxiliary Field H

28 28  The Auxiliary Field H Exp 2: A long copper rod of radius R carries a uniformly distributed (free) current I. Find H inside and outside the rod. current I. Find H inside and outside the rod.  The Auxiliary Field H

29 29 Exp 2:  The Auxiliary Field H

30 30  A Deceptive Parallel Ampere law in vacuum : Ampere law in magnetic materials : Whereas,the divergence of is not, in general, zero.

31 31  Boundary condition a

32 32  Boundary condition

33 33  Linear and Nonlinear Media 磁化率

34 34  Linear and Nonlinear Media 磁導率

35 35 For linear isotropic homogeneous media ElectricMagnetic  Linear and Nonlinear Media

36 36  Linear and Nonlinear Media Exp 3: An infinite solenoid (n turns per unit length, current I) is filled with linear material of susceptibility χ m. Find the magnetic field inside the solenoid. material of susceptibility χ m. Find the magnetic field inside the solenoid.

37 37  Ferromagnetism Ferromagnetic Materials : Fe, Co, Ni, Gd, Dy domain The domains range from about 10 -12 to 10 -8 m 3 in volume and contain 10 17 to 10 21 atoms. domain wall

38 38  Ferromagnetism Ferromagnetic domains. (photo courtesy of R. W. DeBlois)

39 39  Ferromagnetism Hysteresis loop saturation remanence coercive c a g b d f e

40 40 Hysteresis loop hard soft  Ferromagnetism

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56 56  In diamagnetic materials (bismuth 鉍 ): spin moments tend to be dominant and produce f ields that oppose the external field. Thus, the internal magnetic field is reduced slightly c ompared to the external field.  If diople moments dominate slightly, then the internal field is increase slightly over the external field and the material is paramagnetic (tungsten 鎢 ).  Large diople moments are produced in certain regions or domains for the ferromagnetic materials (iron). A random domain alignment exists for virgin ferromagnetic material. W hen an external field is applied and then removed, a net alignment occurs given permane nt magnetization and hysteresis effect. Alloys of some of the ferromagnetic materials are also ferromagnetic (alnico 磁性合金 )  In ferrimagnetic materials, adjacent atoms develop unequal, but oppositely directed mo ments, allowing a rather larger response to external fields. From the point of view of eng ineering applications, the ferrites are very important ferrimagnetic materials. Ferries poss ess a very high resistance, and hence give very little eddy current loss at higher frequenci es when used as transformer cores.  The magnetic tape used for audio and video recording is a superparamagnetic material and is composed of an array of small ferromagnetic particles.

57 57  The Auxiliary Field H


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