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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?
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Sections 磁場 電流與磁場
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10-1 磁場 The electric field and the magnetic field
Electromagnets and permanent magnets
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The definition of B
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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)
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The SI unit for B 1 tesla = 1T =1 N/A‧m=104 gauss 108 T 1.5 T 10-2 T
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Magnetic Field Lines Magnetic vs. electric dipoles
A horseshoe and a C-shaped magnets
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例 1 A 5.3 MeV proton B = 1.2 mT 938 MeV The rest mass energy of an electron is MeV
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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
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Calculation
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10-1.3 Crossed Fields: The Hall Effect
By the conduction electrons in copper: 1879 by Hall (24) John Hopkins
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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
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10-1.4 A Circulating Charged Particle
B out of the page
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頻率與軌跡 The frequency and angular frequency The magnetic bottle machine
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Helical Paths V∥ and V⊥ The pitch (螺距) of the helical path
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極光橢圓圈 Pink by N, green by O
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例 3 The Mass Spectrometer (質譜儀)
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質譜儀 Isotope Separation Centrifuge and diffusion chamber
x = m, V = V, B = mT Isotope Separation Centrifuge and diffusion chamber
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10-1.5 Cyclotrons and Synchrotrons
(迴旋加速器與同步加速器) Fermilab: 6.3km ring
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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
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10-1.6 Magnetic Force on a Current-Carrying Wire
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Magnetic Force For a wire segment:
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例 4 A length of wire with a semicircular arc
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Calculation
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線圈
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10-1.7 Torque on A Current Loop
F2 and F4 cancel F1 and F3 form a force couple
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例 5 A galvanometer for analog meters
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10-1.8 The Magnetic Dipole The magnetic dipole moments
The magnetic potential energy
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磁能
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10-2 Magnetic Fields due to Currents
Conventional rocket EM Rail Gun
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10-2.1 Calculating the Magnetic Field due to a current
The law of Biot and Savart
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Magnetic Field Due to a Current in a Long Straight Wire
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Integration
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Magnetic Field Due to a Current in a Circular Arc of Wire
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例 6 What B does the current produce?
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10-2.2 Two Parallel Currents
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例 7 The Field Between Two wires
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Ampere’s Law Comparing Gauss’ law and Ampere’s law Ampere’s law
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The Magnetic Field Outside a Long Straight Wire with Current
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The Magnetic Field Inside a Long Straight Wire with Current
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例 7 A hollow conducting cylinder
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10-2.4 Solenoids and Toroids
Magnetic Field of a Solenoid (螺線管) Magnetic Field of a Toroid (螺線環)
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Magnetic Field of a Solenoid
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Magnetic Field of a Toroid
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磁圍阻核融合反應器 Tokamak Fusion Test Reactor
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10-2.5 A Current Carrying Coil as a Magnetic Dipole
A current loop and a bar magnet
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Magnetic Field of a Coil
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敬請期待 電磁 IV
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