LSU PHYS 2102 - Magnetic Fields Due to Currents

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Lecture 16:Lecture 16: TUE 16 MAR 10TUE 16 MAR 10Magnetic Fields Due to Currents: Magnetic Fields Due to Currents: Biot-Savart Biot-Savart LawLawPhysics 2102Jonathan DowlingJean-BaptisteBiot (1774-1862)Felix Savart (1791–1841)What Are We Going to Learn?What Are We Going to Learn?A Road MapA Road Map• Electric charge Electric force on other electric charges Electric field, and electric potential• Moving electric charges : current• Electronic circuit components: batteries, resistors, capacitors• Electric currents  Magnetic field Magnetic force on moving charges• Time-varying magnetic field  Electric Field• More circuit components: inductors.• Electromagnetic waves  light waves• Geometrical Optics (light rays).• Physical optics (light waves)Electric Current:Electric Current:A Source of Magnetic FieldA Source of Magnetic FieldIBWire withcurrentINTO pageB• Observation: an electriccurrent creates amagnetic field• Simple experiment: holda current-carrying wirenear a compass needle!BHans Christian Oersted was a professor ofscience at Copenhagen University. In 1820he arranged in his home a sciencedemonstration to friends and students. Heplanned to demonstrate the heating of awire by an electric current, and also tocarry out demonstrations of magnetism, forwhich he provided a compass needlemounted on a wooden stand.While performing his electricdemonstration, Oersted noted to hissurprise that every time the electriccurrent was switched on, the compassneedle moved. He kept quiet and finishedthe demonstrations, but in the months thatfollowed worked hard trying to make senseout of the new phenomenon.New Right Hand Rule!New Right Hand Rule!• Point your thumb along the direction ofthe current in a straight wire• The magnetic field created by thecurrent consists of circular loops directedalong your curled fingers.• The magnetic field gets weaker withdistance: For long wire it’s a 1/R Law!• You can apply this to ANY straight wire(even a small differential element!)• What if you have a curved wire? Breakinto small elements.iBDirection of B!iSuperpositionSuperposition• Magnetic fields (like electricfields) can be “superimposed”-- just do a vector sum of Bfrom different sources• The figure shows four wireslocated at the 4 corners ofa square. They carry equalcurrents in directionsindicated• What is the direction of Bat the center of the square?BI-OUTI-OUTI-INI-INWhen we computed the electric field due to charges we usedCoulomb’s law. If one had a large irregular object, one broke itinto infinitesimal pieces and computed,rrdqEdˆ4120!"=!Which we write as,If you wish to compute the magnetic field due to acurrent in a wire, you use the law of Biot and Savart.CoulombCoulomb’’s Law For E-Fieldss Law For E-FieldsThe The Biot-Savart Biot-Savart LawLawFor B-FieldsFor B-Fields• Quantitative rule for computingthe magnetic field from anyelectric current• Choose a differential elementof wire of length dL andcarrying a current i• The field dB from this elementat a point located by thevector r is given by the Biot-Savart Law304 rrLidBd!!!!="µµ0 =4πx10–7 T•m/A(permeability constant)Jean-Baptiste Biot (1774-1862)Felix Savart (1791-1841)Ld!r!idBd!E =14!"0dqr2ˆrLd!r!idB d!B =µ04!id!L "ˆrr2Biot-Savart Law for B-FieldsCoulomb Law for E-FieldsBiot-Savart Requires ARight-Hand RuleBoth Are 1/r2 Laws!The has no units.ˆr ˆr =!r!r=!rrBiot-Savart Biot-Savart LawLaw• An infinitely long straight wirecarries a current i.• Determine the magnetic fieldgenerated at a point located ata perpendicular distance R fromthe wire.• Choose an element ds as shown• Biot-Savart Law: dB pointsINTO the page• Integrate over all suchelements304 rrsidBd!!!!="µ30)sin(4 rridsdB!"µ=!""#=30)sin(4 rrdsiB$%µ( )!""#+=2/32204RsRdsi$µ( )!"+=02/32202RsRdsi#µ( )!""#$%%&'+=02/122202RsRsiR(µRi!µ20=rR /sin =!2/122)( Rsr +=!""#=30)sin(4 rrdsiB$%µField of a Straight WireField of a Straight Wire304 rrsidBd!!!!="µ30)sin(4 rridsdB!"µ=Is the B-Field From a Power Line Dangerous?Is the B-Field From a Power Line Dangerous?A power linecarries a currentof 500 A.What is themagnetic field in ahouse located100!m away fromthe power line?RiB!µ20= =(4!"10#7T $ m / A)(500A)2!(100m)= 1 µTRecall that the earth’s magneticfield is ~10–4T = 100 µTProbably not dangerous!Biot-Savart Biot-Savart LawLaw• A circular arc of wire of radiusR carries a current i.• What is the magnetic field atthe center of the loop?304 rrdsiBd!!!="µ203044 RiRdRidsRdB!"µ"µ==0 04 4iidBR Rµ µ!" "#= =$Direction of B?? Not anotherright hand rule?!TWO right hand rules!:If your thumb points along theCURRENT, your fingers will pointin the same direction as theFIELD.If you curl our fingers arounddirection of CURRENT, yourthumb points along FIELD!iaIB!µ2101=Magnetic field due to wire 1 where the wire 2 is,1221BILF =aI2I1LaIIL!µ2210=Force on wire 2 due to this field,FForces Between WiresForces Between WireseHarmony’s Rule for Currents: Same Currents – Attract!Opposite Currents – Repel!SummarySummary• Magnetic fields exert forces on moving charges:• The force is perpendicular to the field and the velocity.• A current loop is a magnetic dipole moment.• Uniform magnetic fields exert torques on dipole moments.• Electric currents produce magnetic fields:•To compute magnetic fields produced by currents, use Biot-Savart’s law for each element of current, and then integrate.• Straight currents produce circular magnetic field lines, withamplitude B=µ0i/2πr (use right hand rule for direction).• Circular currents produce a magnetic field at the center (givenby another right hand rule) equal to B=µ0iΦ/4πr• Wires currying currents produce forces on each other: eHarmony’sRule: parallel currents attract, anti-parallel currents


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LSU PHYS 2102 - Magnetic Fields Due to Currents

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