Mutual Induction and Transformer

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1 P21-Class 21: OutlineHour 1:Expt. 9: Faraday’s LawHour 2:Faraday’s LawTransformersMagnetic Materials2 P21-Last Time:Faraday’s Law3 P21-Faraday’s Law of InductionBdNdtεΦ=−Changing magnetic flux inducesan EMFLenz: Induction opposeschange4 P21-What can change? ()cosdNBAdtθε=−Quantities which can vary with time:•Magnitude of B•Area A enclosed by the loop•Angle θbetween B and loop normal 5 P21-Magnet Falling Through a Ringhttp://ocw.mit.edu/ans7870/8/8.02T/f04/visualizations/faraday/07-FallingMagnetResistive/07-FallMAgRes_f54_320.htmlFalling magnet slows as it approaches a copper ring which has been immersed in liquid nitrogen.6 P21-Example: Magnitude of B Magnet Falling Through a RingFalling magnet approaches a copper ringorCopper Ring approaches Magnet7 P21-Moving Towards DipoleMove ring downAs ring approaches, what happens to flux?It increases8 P21-Moving Over DipoleMove downFluxFlux increases then decreasesNote we have arbitrarily assigned dA up9 P21-Moving Over DipoleCurrentCWCCWMove downCurrent first goes in one direction, then otherIt ALWAYS opposes the changing flux10 P21-Five PRS Questions:Predictions for Experiment 9 Faraday’s Law11 P21-Experiment 9:Faraday’s Law of Induction12 P21-CURRENTFLUXImperfectcurrent 013 P21-Four PRS Questions:Force on A Loop Below Magnet Moving Upward;Moving Rail;Moving Rectangle near Wire;Generator.14 P21-Brakes 15 P21-Magnet Falling Through a RingWhat happened to kinetic energy of magnet?16 P21-Eddy Current Brakinghttp://demoroom.physics.ncsu.edu/html/demos/163.htmlWhat happened to kinetic energy of pendulum?17 P21-Eddy Current Brakinghttp://demoroom.physics.ncsu.edu/multimedia/video/5K20.22.1.MOVWhat happened to kinetic energy of disk?18 P21-Demonstration:Eddy Current Braking 19 P21-Eddy Current BrakingThe magnet induces currents in the metal that dissipate the energy through Joule heating:ω1.Current is induced counter-clockwise (out from center)2.Force is opposing motion (creates slowing torque)XXXX20 P21-Eddy Current BrakingThe magnet induces currents in the metal that dissipate the energy through Joule heating:ω1.Current is induced clockwise (out from center)2.Force is opposing motion (creates slowing torque)3.EMF proportional to ω4..2RFε∝XXXX21 P21-Demonstration:Levitating Magnet Superconductor & Magnethttp://ocw.mit.edu/ans7870/8/8.02T/f04/visualizations/faraday/16-superconductor/16-12_wmv320.html22 P21-PRS Questions:Loop in Uniform Field23 P21-Mutual Inductance24 P21-Mutual Inductance112122 112122NMINMIΦ≡Φ→=21212dIdtMε≡−1221MMM==A current I2in coil 2, induces some magnetic flux Φ12in coil 1. We define the flux in terms of a “mutual inductance” M12:25 P21-Demonstration:Remote Speaker26 P21-TransformerStep-up transformerBssdNdtεΦ=BppdNdtεΦ=ssppNNεε=Ns> Np: step-up transformerNs< Np: step-down transformer27 P21-Demonstrations:One Turn Secondary:NailMany Turn Secondary:Jacob’s Ladder28 P21-Transmission of Electric PowerPower loss can be greatly reduced if transmitted at high voltage29 P21-Example: Transmission linesAn average of 120 kW of electric power is sent from a power plant. The transmission lines have a total resistance of 0.40 Ω. Calculate the power loss if the power is sent at (a) 240 V, and (b) 24,000 V.521.2105002.410PWIAVV×===×(a) 83% loss!!22(500)(0.40)100LPIRAkW==Ω=541.2105.02.410PWIAVV×===×(b)0.0083% loss22(5.0)(0.40)10LPIRAW==Ω=30 P21-Magnetic Materials31 P21-Recall Polar DielectricsDielectric polarization decreasesElectric Field!32 P21-Para/FerromagnetismApplied external field B0tends to alignthe atomic magnetic moments33 P21-Para/FerromagnetismThe aligned moments tend to increasethe B field0mκ=BB􀁇􀁇Eκ=0EE􀁇􀁇Compare to:34 P21-Para/FerromagnetismParamagnet: Turn off B0, everything disordersFerromagnet: Turn off B0, remains (partially) orderedThis is why some items you can pick up with a magnet even though they don’t pick up other items35 P21-Magnetization VectorM=0M>0Useful to define “Magnetization”of material:11NiiVV===∑µMµ􀁇􀁇􀁇00µ=+BBM􀁇􀁇􀁇36 P21-Hysteresisin FerromagnetsThe magnetization Mof a ferromagnetic material depends on the historyof the substanceMagnetization remains even with B0off !!!

Description
"An example of induced e.m.f is that of a falling ring in a magnetic field.The field pattern and the graph between induced current and time is shown.Eddy current and its application to induction braking has been explained.The other topics discussed are mutual induction, transformers power transmission and magnetic materials.


Physics Department Faculty, Lecturers, and Technical Staff, 8.02 Physics II: Electricity and Magnetism, Massachusetts Institute of Technology: MIT OpenCourseWare),http://ocw.mit.edu (Accessed Aug 28th,2011). License: Creative Commons BY-NC-SA: http://ocw.mit.edu/terms/#cc"

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