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How is an aurora so thin yet so tall and wide?

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Presentation on theme: "How is an aurora so thin yet so tall and wide?"— Presentation transcript:

1 How is an aurora so thin yet so tall and wide?
10 電磁 III How is an aurora so thin yet so tall and wide?

2 Sections 磁場 電流與磁場

3 10-1 磁場 The electric field and the magnetic field
Electromagnets and permanent magnets

4 The definition of B

5 The tracks in a bubble chamber
Positron emitted-isotopes (C,N,O) P annihilates with e, emits 2 gamma Glucose usage in brain, schizophrenics(精神分裂症)

6 The SI unit for B 1 tesla = 1T =1 N/A‧m=104 gauss 108 T 1.5 T 10-2 T

7 Magnetic Field Lines Magnetic vs. electric dipoles
A horseshoe and a C-shaped magnets

8 例 1 A 5.3 MeV proton B = 1.2 mT 938 MeV The rest mass energy of an electron is MeV

9 10-1.2 Crossed Fields: Discovery of the Electron
A cathode ray tube Thomson’s procedure: 設定E = 0, B = 0, 並記錄光點位置 開啟電場 開啟磁場,並調至與電場相等 1897 by JJ Thomson at Cambridge

10 Calculation

11 10-1.3 Crossed Fields: The Hall Effect
By the conduction electrons in copper: 1879 by Hall (24) John Hopkins

12 例 2 A cube generator d = 1.5 cm, v = 4.0m/s, B = 0.05T
Electrons shifted to the left, making the left side at lower potential

13 10-1.4 A Circulating Charged Particle
B out of the page

14 頻率與軌跡 The frequency and angular frequency The magnetic bottle machine

15 Helical Paths V∥ and V⊥ The pitch (螺距) of the helical path

16 極光橢圓圈 Pink by N, green by O

17 例 3 The Mass Spectrometer (質譜儀)

18 質譜儀 Isotope Separation Centrifuge and diffusion chamber
x = m, V = V, B = mT Isotope Separation Centrifuge and diffusion chamber

19 10-1.5 Cyclotrons and Synchrotrons
(迴旋加速器與同步加速器) Fermilab: 6.3km ring

20 Synchrotrons The resonance condition: When proton energy > 50Mev:
Out of resonance (relativistic effect) A huge magnet (4×106 m2) is needed for high energy (500Gev) protons The proton sychrotron at Fermilab can produces 1Tev proton

21 10-1.6 Magnetic Force on a Current-Carrying Wire

22 Magnetic Force For a wire segment:

23 例 4 A length of wire with a semicircular arc

24 Calculation

25 線圈

26 10-1.7 Torque on A Current Loop
F2 and F4 cancel F1 and F3 form a force couple

27 例 5 A galvanometer for analog meters

28 10-1.8 The Magnetic Dipole The magnetic dipole moments
The magnetic potential energy

29 磁能

30 10-2 Magnetic Fields due to Currents
Conventional rocket EM Rail Gun

31 10-2.1 Calculating the Magnetic Field due to a current
The law of Biot and Savart

32 Magnetic Field Due to a Current in a Long Straight Wire

33 Integration

34 Magnetic Field Due to a Current in a Circular Arc of Wire

35 例 6 What B does the current produce?

36 10-2.2 Two Parallel Currents

37 例 7 The Field Between Two wires

38 Ampere’s Law Comparing Gauss’ law and Ampere’s law Ampere’s law

39 The Magnetic Field Outside a Long Straight Wire with Current

40 The Magnetic Field Inside a Long Straight Wire with Current

41 例 7 A hollow conducting cylinder

42 10-2.4 Solenoids and Toroids
Magnetic Field of a Solenoid (螺線管) Magnetic Field of a Toroid (螺線環)

43 Magnetic Field of a Solenoid

44 Magnetic Field of a Toroid

45 磁圍阻核融合反應器 Tokamak Fusion Test Reactor

46 10-2.5 A Current Carrying Coil as a Magnetic Dipole
A current loop and a bar magnet

47 Magnetic Field of a Coil

48 敬請期待 電磁 IV


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