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Title: Fundamental nuclear symmetries meet classical electrodynamic symmetries at the SNS. Author: Christopher Crawford Last modified by – PowerPoint PPT presentation

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1
5.1 Magnetic Field
  • Christopher Crawford
  • PHY 417
  • 2015-01-16

2
Outline
  • Magnetic field and torque
  • William Gilbert field lines of permanent
    magnets Hans Christian Ørsted magnetic field
    of a current
  • Magnetostatics
  • André-Marie Ampère force on two straight wires
  • Current element continuity equation

3
Static force laws
  • Electrostatics Coulombs law
  • Magnetostatics Biot-Savart law

B.C.s Flux lines bounded by charge Flux lines
continuous Flow sheets continuous
(equipotentials) Flow sheets bounded by current
4
History of magnetism
  • The magnetic force was known in antiquity
  • Magnetism more predominant in nature but more
    difficult to quantify
  • Permanent magnets (magnetization), not electric
    currents
  • No magnetic (point) charge (monopole) gt dipole
    effect (N,S poles)
  • 1-d currents instead of 0-d charges gt cant
    split a wire!
  • Static electricity produced in the lab long
    before steady currents
  • Timeline (from A Ridiculous Brief History of
    Electricity and Magnetism)
  • 600 BC Thales of Miletus discovers lodestones
    attraction to iron
  • 1200 AD Chinese use lodestone compass for
    navigation
  • 1259 AD Petrus Peregrinus (Italy) discovers the
    same thing
  • 1600 AD William Gilbert discovers that the Earth
    is a giant magnet
  • 1742 AD Thomas LeSeur shows inverse cube law for
    magnets
  • 1820 AD Hans Christian Ørsted discovers that
    current twists magnets Andre Marie Ampere shows
    that parallel currents attract/repel
    Jean-Baptiste Biot Felix Savart show inverse
    square law

5
Early magnetism
  • https//www.tcd.ie/Physics/Magnetism/Guide/compass
    .php
  • Wu Ching Tsung Yao (1040)
  • First mention of the magnetic compass
  • Petrus Perigrinus (1269)
  • Epostolia de Magnete rediscovered it
  • William Gilbert (1600)
  • De Magnete the earth is a magnet
  • René Descartes
  • effluvia of "threaded parts

6
Magnetic fields
  • In magnetism it is more natural to start with the
    concept of Magnetic field than the actual force
    law! (dipole)
  • Compass alignswith B-field
  • Iron filings lineup along magneticfield lines
  • Magnetic field lines look like an electric dipole
    (in fact the magnetic dipole was discovered
    first!)

7
Iron Filings
8
Iron Filings
9
Difference between E, B dipoles
  • Same as the differences between Flux and Flow!
  • Charge sources of flux
  • Conservative flow potential
  • Example Amber (electric)
  • Rub to charge
  • 2 charges (/) monopole fluids
  • Exerts force on charges
  • Continuous field lines flux
  • Rotational (source of flow?)
  • Example Lodestone (magnet)
  • Always charged
  • 2 poles (N/S) inseparable dipole
  • Exerts torque on other magnets

10
First connection to currents
  • from Wittaker, A history of the theories of
    Aether and Electricity

11
The current connection
  • There is no magnetic monopole N/S cannot be
    separated
  • The source of all magnetism is electric current
  • A dipole is just a current loop
  • Hans Christian Ørsted
  • Current produces B-field
  • Quantified by Biot Savart

12
Hans Christian Ørsted
  • from Wittaker, A history of the theories of
    Aether and Electricity

13
Electrodynamics
  • André-Marie Ampère showed that parallel currents
    attractand antiparallel currents repel
  • The magnetic force is the basis for
    electromagnetic units

14
Ampères generalization
  • Experimental laws
  • Force formula
  • Problem
  • The force between two current elements does
    NOTpoint along the line from the one to the
    other!

15
Peer criticism
MAXWELL
HEAVISIDE
16
Current elements
  • Analogous to charge elements different
    dimensions
  • Relations between charge / current and different
    dimensions analogy multi-lane highway
    current flux

17
Continuity equation
  • Local conservation of charge
  • Current I is a flux current density J
    flux density
  • 4-vector current
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