magnetism and levitation - university of oklahoma physics &...
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Magnetism and Levitation
Brent HobbsDan Stark
Timothy Wofford
Junior Lab IWednesday, December 11, 2002
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Types of Magnetism
FerromagnetismAntiferromagnetismFerrimagnetismParamagnetismSuperparamagnetismDiamagnetism
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FerromagnetismRefrigerator MagnetUnpaired electronSpin coupling causes large parallel dipole domains to formDomains are randomly oriented until aligned by an external fieldBecomes a paramagnet above the Curie Temperature (Phase Change)
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Hysteresis LoopsCurrent magnetic statedependent on historyFound with ferro, ferri, and superpara magnetismsSaturation points at tipsRemanence is the field left over when external B-field is removed
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ParamagnetismUnpaired ElectronSpin coupling smallThermal energy tends to destroy any net effect of couplingExhibits other behavior below Curie Temp.Extra electron acts as dipole and aligns itself with the field. >0
Works like paramegnetism, but has decay time to return to random polarizationYields a hysteresis loop that decays to a curve over time.
Superparamagnetism
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AntiferromagnetismUnpaired electronAntiparallel dipolescancelSpin coupling causes large antiparallel dipole domains to formNet magnetization is due to spin cantingProduces very weak effects
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FerrimagnetismUnpaired electronAntiparallel dipolescancel partially Spin coupling causes large (anti)parallel dipole domains to formDue to crystal structure, dipoles are larger in one direction than the other, netting a field
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DiamagnetismNo unpaired electronMagnetic moment due to orbitalangular momentumInduced Magnetic moments antiparallel to applied field (Lenz’s law)Superconductors are perfect diamagnetsEverything is diamagneticNegative allows stable equilibrium points => levitation
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Solutions to Laplace Equation only have saddles
Laplace’s Equation applies to energy of Static mass distributions Static charge distributions Static magnetic dipole distributions
Equillibrium at energy minimum Energy only has saddles
THUSStatic distributions of mass, charge, and magnetic dipoles cannot be held in equillibrium by other static distributions of mass, charge, and magnetic dipoles
Earnshaw’s Theorem
When Engineers Attack
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Levitation possible when constrainedEquilibrium is not stable
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Energy of magnetic and gravitational field in a material
Equillibrium Conditions
So if is negative….diamagnetic materialscan levitate!
V is Volume is magnetic susceptibility
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Basics of Superconductors Form Cooper Pairs – Pairs of Electrons around Fermi Level Energy separation between Cooper Pairs and single
electrons Cooper Pairs form Bose-Einstein Condensate (pairs occupy
the same space (coherence length) -> many pair interaction) Not enough thermal energy to scatter or destroy pair -> no
resistance Type I -> Destroyed above Critical Field Type II -> Destroyed gradually from lower Critical Field to
upper
Internal Feedback
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Basics of Superconductors (cont.)A superconductor repels all magnetic fields (the Meissner Effect) →Perfect Diamagnet
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Ideal Conductor ≠ Superconductor
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Superconducting Levitation Changing magnetic field
induces a current Current induces magnetic field
(Remember Meissner Effect!) Perfectly cancels gravity Stable Equilibrium
Superconducting Effects!!!
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Magnetic Pinning Outside B-field introduced above
TC → permeates impurities Stays pinned within impurities
(vortices) as T lowers < TC B-field cannot separate from
Superconductor B-field can be broken
Superconducting Effects!!!
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Referenceshttp://hyperphysics.phy-astr.gsu.edu/hbase/solids/chrlen.html#c4http://edu.ioffe.ru/lib/galperin/09ch.pdfJaejun Yu. http://phya.snu.ac.kr/~ssphy2002_1/pdf/ssp2-lecture-3-2002.pdf. Seoul National University.http://hyperphysics.phy-astr.gsu.edu/hbase/solids/magpr.htmlhttp://web.mit.edu/8.13/www/JLExperiments/expt39/node6.htmlhttp://www.fys.uio.no/faststoff/ltl/levitation/