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27 Magnetic Sources charge motion Gauss’s Law (again) Ampere’s Law
materials
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27-1 The Magnetic Field of Moving Point Charges
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Current & Magnetic Field
field circulation
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(RHR) I B
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field-effect ammeter
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RHR Review Magnetic Force: cross-product rule (flat hand or “peanut butter jar”) Magnetic Field: thumb along I, B follows curled fingers
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moving point charge B ~ qvsinq/r2.
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27-2 The Magnetic Field of Currents: The Biot-Savart Law
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Biot-Savart Law integrated field effect of current
all dB same direction at center of hoop
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B on axis of hoop dB not same direction
non-axial component adds vectorially to 0 axial component remains
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section-view of hoop-current
axial B same direction is current in or out of screen at top of hoop?
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electromagnet (solenoid)
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solenoid high# turns/meter N = #turns, L = length (m) Bcenter = moNI/L
n = N/L: Bcenter = monI
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straight current-segment
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Calculate B at Center in terms of L and I.
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B of long straight current
angles are + and – 90 degrees:
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parallel wires same directed I’s attract, opposite directed currents repel.
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Magnetic Force Balance Experiment
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Magnetic Force Balance Experiment
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the ampere current in two long parallel wires that causes a force of 2x10-7 newtons per meter of length of the wires.
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27-3 Gauss’s Law for Magnetism
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Gauss’s Law for B: Absence of Magnetic Charge
Compare to Gauss’s Law for E: Qinside
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E and B Fields: Similarities and Differences
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27-4 Ampere’s Law
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27-5 Magnetism in Matter
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Magnetic Moments of an Un-magnetized Material
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Magnetic Domains in Crystalline Silicone
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Aligned Magnetic Domains Produces “Magnet”
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Magnetic Field due to Naturally Occurring Magnetite
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Magnetic “bits” Recorded on Magnetic Tape… 0, 1, 0
Cross Section of a Recording Head Solenoid
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Magnetic Disk Hard Drive
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Magnetic Disk Hard Drive: 2400x Magnification
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Summary magnetic fields are due to charge motion
biot-savart law determines B. B fields have no point source B integrated along a closed path is proportional to the current enclosed by the path magnetic materials
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general biot-savart
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two hoops
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