Prelude to an Exam Allegro con brio Next Friday – EXAMINATION #2 New WebAssign on Board on Magnetism TWO Old WebAssigns due this week • No Extensions Please take a look at the short memo on vector multiplication that was put on the website earlier … we will no start to use this material. Magnetism 1 Magnetism A Whole New Topic October 18, 2005 Magnetism 2 DEMO Magnetism 3 Lodestone (Mineral) • Lodestones attracted iron filings. • Lodestones seemed to attract each other. • Used as a compass. – One end always pointed north. • Lodestone is a natural magnet. Magnetism 4 Magnetism • Refrigerators are attracted to magnets! Magnetism 5 Applications • Motors • Navigation – Compass • Magnetic Tapes – Music, Data • Television – Beam deflection Coil • Magnetic Resonance Imaging • High Energy Physics Research Magnetism 6 Magnets S N Shaded End is NORTH Pole Shaded End of a compass points to the NORTH. Magnetism • Like Poles Repel • Opposite Poles Attract • Magnetic Poles are only found in pairs. – No magnetic monopoles have ever been observed. 7 Observations • Bring a magnet to an electrically charged object and nothing happens. No forces. • Bring a magnet near some metals (Co, Fe, Ni …) and it will be attracted to the magnet. – The metal will be attracted to both the N and S poles independently. – Some metals are not attracted at all. – Wood is NOT attracted to a magnet. – Neither is water. • A magnet will force a compass needle to align with it. (No big Surprise.) Magnetism 8 Magnets Cutting a bar magnet in half produces TWO bar magnets, each with N and S poles. Magnetism 9 Consider a Permanent Magnet B N Magnetism S 10 Introduce Another Permanent Magnet B N N S pivot S The bar magnet (a magnetic dipole) wants to align with the B-field. Magnetism 11 Field of a Permanent Magnet B N N S S The south pole of the small bar magnet is attracted towards the north pole of the big magnet. Also, the small bar magnet (a magnetic dipole) wants to align with the B-field. The field attracts and exerts a torque on the small magnet. Magnetism 12 Field of a Permanent Magnet B N N S S The bar magnet (a magnetic dipole) wants to align with the B-field. Magnetism 13 The Magnetic Field • Similar to Electric Field … exists in space. – Has Magnitude AND Direction. • The “stronger” this field, the greater is the ability of the field to interact with a magnet. Magnetism 14 Convention For Magnetic Fields X Field INTO Paper Magnetism B Field OUT of Paper 15 Experiments with Magnets Show • Current carrying wire produces a circular magnetic field around it. • Force on Compass Needle (or magnet) increases with current. Magnetism 16 Current Carrying Wire Current into the page. B Right hand RuleThumb in direction of the current Fingers curl in the direction of B Magnetism 17 Current Carrying Wire • B field is created at ALL POINTS in space surrounding the wire. • The B field had magnitude and direction. • Force on a magnet increases with the current. • Force is found to vary as ~(1/d) from the wire. Magnetism 18 Compass and B Field • Observations – North Pole of magnets tend to move toward the direction of B while S pole goes the other way. – Field exerts a TORQUE on a compass needle. – Compass needle is a magnetic dipole. – North Pole of compass points toward the NORTH. Magnetism 19 Planet Earth Magnetism 20 Inside it all. 8000 Miles Magnetism 21 On the surface it looks like this.. Magnetism 22 Inside: Warmer than Floriduh Magnetism 23 Much Warmer than Floriduh Magnetism 24 Finally Magnetism 25 In Between The molten iron core exists in a magnetic field that had been created from other sources (sun…). The fluid is rotating in this field. This motion causes a current in the molten metal. The current causes a magnetic field. The process is self-sustaining. The driving force is the heat (energy) that is generated in the core of the planet. Magnetism 26 After molten lava emerges from a volcano, it solidifies to a rock. In most cases it is a black rock known as basalt, which is faintly magnetic, like iron emerging from a melt. Its magnetization is in the direction of the local magnetic force at the time when it cools down. Instruments can measure the magnetization of basalt. Therefore, if a volcano has produced many lava flows over a past period, scientists can analyze the magnetizations of the various flows and from them get an idea on how the direction of the local Earth's field varied in the past. Surprisingly, this procedure suggested that times existed when the magnetization had the opposite direction from today's. All sorts of explanation were proposed, but in the end the only one which passed all tests was that in the distant past, indeed, the magnetic polarity of the Earth was sometimes reversed. Magnetism 27 Ancient Navigation Magnetism 28 This planet is really screwed up! NORTH POLE Magnetism SOUTH POLE 29 Repeat Navigation DIRECTION N S If N direction is pointed to by the NORTH pole of the Compass Needle, then the pole at the NORTH of our planet must be a SOUTH MAGNETIC POLE! Compass Direction Navigation DIRECTION S N And it REVERSES from time to time. Magnetism 30 Magnetism 31 Rowland’s Experiment Field is created by any moving charge. Rotating INSULATING Disk which is CHARGED + or – on exterior. ++ Magnetism + + ++ xxx xxx B xxx Increases with charge on the disk. Increases with angular velocity of the disk. Electrical curent is a moving charge. 32 A Look at the Physics B q v q B There is NO force on a charge placed into a magnetic field if the charge is NOT moving. There is no force if the charge moves parallel to the field. • If the charge is moving, there is a force on the charge, perpendicular to both v and B. F=qvxB Magnetism 33 WHAT THE HECK IS THAT??? • A WHAT PRODUCT? • A CROSS PRODUCT – Like an angry one?? • Alas, yes …. • F=qv X B Magnetism 34 The Lorentz Force This can be summarized as: F qv B F or: F qvBsin v B mq is the angle between B and V Magnetism 35 Note B is sort of the Force per unit (charge-velocity) Whatever that is!! Magnetism 36 Practice B and v are parallel. Crossproduct is zero. So is the force. Which way is the Force??? Magnetism 37 Units F Bqv Sin(θ ) Units : F N N B qv Cm / s Amp m Magnetism 1 tesla 1 T 1 N/(A - m) 38 teslas are At the Surface of the Earth 3 x 10-5 T Typical Refrigerator Magnet 5 x 10-3 T Laboratory Magnet 0.1 T Large Superconducting Magnet 10 T Magnetism 39 The Magnetic Force is Different From the Electric Force. Whereas the electric force acts in the same direction as the field: The magnetic force acts in a direction orthogonal to the field: F qE F qv B (Use “Right-Hand” Rule to determine direction of F) And --the charge must be moving !! Magnetism 40 So… A moving charge can create a magnetic field. A moving charge is acted upon by a magnetic field. In Magnetism, things move. In the Electric Field, forces and the field can be created by stationary charges. Magnetism 41 Trajectory of Charged Particles in a Magnetic Field (B field points into plane of paper.) + +B + v+ + + + + + + + + F + + + + F + + + + + + + + + + + + + + + + + + + B + + + + + Magnetism v 42 Trajectory of Charged Particles in a Magnetic Field (B field points into plane of paper.) + +B + v+ + + + + + + + + F + + + + F + + + + + + + + + + + + + + + + + + + B + + + + + Magnetism v Magnetic Force is a centripetal force 43 Review of Rotational Motion = s / r s = r ds/dt = d/dt r v = r s r = angle, = angular speed, = angular acceleration at ar at = r tangential acceleration ar = v2 / r radial acceleration The radial acceleration changes the direction of motion, while the tangential acceleration changes the speed. Uniform Circular Motion ar = constant v and ar constant but direction changes Magnetism v ar = v2/r = 2 r KE = ½ mv2 = ½ mw2r2 F = mar = mv2/r = m2r 44 Magnetism 45 Radius of a Charged Particle Orbit in a Magnetic Field +B + + v+ + + + + + + + + + r + + + + + + F + Magnetism Centripetal Force = Magnetic Force mv 2 qvB r mv r qB Note: as Fv , the magnetic 46 force does no work! Cyclotron Frequency +B + + v+ + + + + + + + + + r + + + + + + F + Magnetism The time taken to complete one orbit is: 2r v 2 mv v qB T 1 qB f T 2 m qB c 2f m 47 More Circular Type Motion in a Magnetic Field Magnetism 48 Mass Spectrometer Smaller Mass Magnetism 49 Magnetism 50 An Example A beam of electrons whose kinetic energy is K emerges from a thin-foil “window” at the end of an accelerator tube. There is a metal plate a distance d from this window and perpendicular to the direction of the emerging beam. Show that we can prevent the beam from hitting the plate if we apply a uniform magnetic field B such that 2mK B 2 2 ed Magnetism 51 Problem Continued From Before r mv r qB 1 2 2K K mv so v 2 m m 2K 2mK r d 2 2 eB m e B Solve for B : Magnetism 2mK B e2d 2 52 Let’s Look at the effect of crossed E and B Fields: x x x B E x x x v q , m Magnetism • 53 What is the relation between the intensities of the electric and magnetic fields for the particle to move in a straight line ?. x x x B E x x x v q• m FE = q E and FB = q v B If FE = FB the particle will move following a straight line trajectory qE=qvB v=E/B FB FE • Magnetism 54 What does this mean?? v=E/B Magnetism This equation only contains the E and B fields in it. Mass is missing! Charge is missing! This configuration is a velocity filter! 55 “Real” Mass Spectrometer Create ions from injected species. This will contain various masses, charges and velocities. These are usually accelerated to a certain ENERGY (KeV) by an applied electric field. The crossed field will only allow a selected velocity to go forward into the MS. From before: R=mv/Bq Magnetism 56 Components of MS: Accelerate the ions through a known potential difference . 1 2 mv qVapplied 2 So q 1 2 1 v m 2 Vapplied The velocity can be selected via an E x B field and the MS will separate by: mv R Bq Magnetism Unknown is mass to charge ratio which can be sorted from the spectrum 57 Magnetism 58 PHYSICS NEWS • Exam will be available Friday or Monday (depending on grader). • QUIZ on Friday – Magnetism through today’s work. • Exam #3 is 4 weeks from today! • FINAL EXAM 1.5 weeks after that. • ADVICE: Start to study old material NOW! Magnetism 59 Magnetism 60 REMEMBER The Lorentz Force This can be summarized as: F qv B F or: F qvBsin v B mq is the angle between B and V Magnetism 61 VECTOR CALCULATIONS i a b ax bx Magnetism j ay by k az bz 62 Wires • A wire with a current contains moving charges. • A magnetic field will apply a force to those moving charges. • This results in a force on the wire itself. – The electron’s sort of PUSH on the side of the wire. F Remember: Electrons go the “other way”. Magnetism 63 The Wire in More Detail Assume all electrons are moving with the same velocity vd. q it i L vd F qvd B i L vd B iLB vd vector : F iL B L in the direction of the motion of POSITIVE charge (i). B out of plane of the paper Magnetism 64 Magnetic Levitation Magnetic Force mg Where does B point???? Into the paper. Current = i iLB mg mg B iL m/l is a constant for the wire. Magnetism 65 MagLev Magnetism 66 Magnetic Repulsion Magnetism 67 Detail Magnetism 68 Moving Right Along …. Magnetism 69 Acceleration Magnetism 70 Don’t Buy A Ticket Quite Yet.. This is still experimental. Much development still required. Some of these attempts have been abandoned because of the high cost of building a MagLev train. Probably 10-20 years out. Or More. Magnetism 71 Current Loop What is force on the ends?? Loop will tend to rotate due to the torque the field applies to the loop. Magnetism 72 The Loop OBSERVATION Force on Side 2 is out of the paper and that on the opposite side is into the paper. No net force tending to rotate the loop due to either of these forces. The net force on the loop is also zero, pivot Magnetism 73 An Application The Galvanometer Magnetism 74 The other sides t1=F1 (b/2)Sin() =(B i a) x (b/2)Sin() total torque on the loop is: 2t1 Total torque: t=(iaB) bSin() =iABSin() (A=Area) Magnetism 75 A Coil For a COIL of N turns, the net torque on the coil is therefore : τ NiABSin(θ ) Normal to the coil RIGHT HAND RULE TO FIND NORMAL TO THE COIL: “Point or curl you’re the fingers of your right hand in the direction of the current and your thumb will point in the direction of the normal to the coil. Magnetism 76 Dipole Moment Definition Define the magnetic dipole moment of the coil m as: m=NiA Magnetism We can convert this to a vector with A as defined as being normal to the area as in the previous slide. 77 Current Loop t iAB sin Consider a coil with N turns of wire. Define Magnetic Moment μ NiA and t μB Magnetism 78 Verify the Direction τ μB m Magnetism B 79 A length L of wire carries a current i. Show that if the wire is formed into a circular coil, then the maximum torque in a given magnetic field is developed when the coil has one turn only, and that maximum torque has the magnitude … well, let’s see. Circumference = L/N Magnetism L 2r N L r 2N 80 Problem continued… t NiAB since sin( m , B) is maximum when the angle is 90o A r 2 L t NiB 2N 2 2 L N L2 iB t iB ....... (BiA) 2 4 N 2N Maximum when N 1 and Magnetism iBL2 t 4 81 So Far Moving Charges experience forces due to magnetic field. We showed in the demo that a compass placed near a current carrying wire was affected. The current carrying wire therefore creates a magnetic field. Current is affected by a B field and at the same time creates a B field of its own! Magnetism 82 Try to remember… 1 rdq r dq dE 2 3 40 r r 40 r 1 r UNIT VECTOR r Magnetism 83 The “Coulomb’s Law of Magnetism A Vector Equation … duck Magnetism 84 For the Magnetic Field, current “elements” create the field. This is the Law of Biot-Savart In a similar fashion to E field : m 0 ids runit m 0 ids r B 2 4 r 4 r 3 permeabili ty m 0 4 10 7 Tm / A 1.26 10 7 Tm BY DEFINITION Magnetism 85 Magnetic Field of a Straight Wire • We intimated via magnets that the Magnetic field associated with a straight wire seemed to vary with 1/d. • We can now PROVE this! Magnetism 86 From the Past Using Magnets Magnetism 87 Right-hand rule: Grasp the element in your right hand with your extended thumb pointing in the direction of the current. Your fingers will then naturally curl around in the direction of the magnetic field lines due to that element. Magnetism 88 Let’s Calculate the FIELD Note: For ALL current elements ds X r is into the page Magnetism 89 The Details m 0 ids sin( ) dB 4 r2 Negative portion of the wire contribute s an equal amount so we integrate from 0 to and DOUBLE it. m 0i sin( )ds B 2 0 r2 Magnetism 90 Moving right along r s R 2 2 sin sin( ) R s2 R2 So m 0i m 0i Rds B 3 / 2 2 0 s 2 R 2 2R Magnetism 1/d 91 A bit more complicated A finite wire Magnetism 92 P1 NOTE : sin( ) sin( ) ds r ds r sin( ) r ds R sin( ) r m 0i ds sin( ) dB 2 4 r r s R Magnetism 2 2 1/ 2 93 More P1 L/2 m 0i ds B 3/ 2 2 2 4 L / 2 s R and m 0i L B 2R L2 4 R 2 when L , Magnetism m 0i B 2R 94 P2 m 0iR ds B 4 L s 2 R 2 3 / 2 0 or m 0i L B 4R s 2 R 2 Magnetism 95 APPLICATION: Find the magnetic field B at point P in for i = 10 A and a = 8.0 cm. Magnetism 96 Circular Arc of Wire Magnetism 97 More arc… ds ds Rd m 0 ids m 0 iRd dB 2 4 R 4 R 2 m 0 iRd m 0i B dB d 2 4 R 4R 0 0 m 0 i B at point C 4R Magnetism 98 Howya Do Dat?? ds r 0 No Field at C Magnetism 99 Force Between Two Current Carrying Straight Parallel Conductors Wire “a” creates a field at wire “b” Magnetism Current in wire “b” sees a force because it is moving in the magnetic field of “a”. 100 The Calculation The FIELD at wire " b" due to wire " a" is what we just calculated : m 0ia Bat "b" 2d Fon "b" ib L B Since L and B are at right angles... m 0 Lia ib F 2d Magnetism 101 Definition of the Ampere The force acting between currents in parallel wires is the basis for the definition of the ampere, which is one of the seven SI base units. The definition, adopted in 1946, is this: The ampere is that constant current which, if maintained in two straight, parallel conductors of infinite length, of negligible circular cross section, and placed 1 m apart in vacuum, would produce on each of these conductors a force of magnitude 2 x 10-7 newton per meter of length. Magnetism 102 TRANSITION AMPERE Magnetism 103 Welcome to Andre’ Marie Ampere’s Law Normally written as a “circulation” vector equation. We will look at another form, but first… Magnetism 104 Remember GAUSS’S LAW?? E d A Surface Integral Magnetism qenclosed 0 105 Gauss’s Law • Made calculations easier than integration over a charge distribution. • Applied to situations of HIGH SYMMETRY. • Gaussian SURFACE had to be defined which was consistent with the geometry. • AMPERE’S Law is the Gauss’ Law of Magnetism! (Sorry) Magnetism 106 The next few slides have been lifted from Seb Oliver on the internet Whoever he is! Magnetism 107 Biot-Savart • The “Coulombs Law of Magnetism” m 0 ids rˆ dB 2 4 r Magnetism 108 Invisible Summary • Biot-Savart Law m 0 ids rˆ dB 2 4 r m0 I – (Field produced by wires) B 2R – Centre of a wire loop radius R m NI B 0 – Centre of a tight Wire Coil with N turns 2R – Distance a from long straight wire • Force between two wires • Definition of Ampere Magnetism m0 I B 2a F m 0 I1 I 2 l 2a 109 Magnetic Field from a long wire Using Biot-Savart Law r I Take a short vector on a circle, ds B ds Magnetism B ds B ds cos 0 cos 1 Thus the dot product of B & the short vector ds is: m0 I B 2r B ds B ds m0 I B ds ds 2r 110 Sum . B ds around a circular path m0 I B ds ds 2r r I B Sum this around the whole ring ds Circumference of circle Magnetism B ds ds 2r m0 I ds 2r m0 I ds 2r m0 I B ds 2r m 0 Ι 2r 111 Consider a different path B ds 0 i Magnetism • Field goes as 1/r • Path goes as r. • Integral independent of r 112 SO, AMPERE’S LAW by SUPERPOSITION: We will do a LINE INTEGRATION Around a closed path or LOOP. Magnetism 113 Ampere’s Law B d s m i 0 enclosed USE THE RIGHT HAND RULE IN THESE CALCULATIONS Magnetism 114 The Right Hand Rule Magnetism 115 Another Right Hand Rule Magnetism 116 COMPARE B d s m i 0 enclosed Line Integral E d A Surface Integral Magnetism qenclosed 0 117 Simple Example Magnetism 118 Field Around a Long Straight Wire B d s m i 0 enclosed B 2r m 0i m 0i B 2r Magnetism 119 Field INSIDE a Wire Carrying UNIFORM Current Magnetism 120 The Calculation B ds B ds 2rB m i 0 enclosed ienclosed r 2 i 2 R and m 0i B r 2 2R Magnetism 121 B m 0i 2R R Magnetism r 122 Procedure • Apply Ampere’s law only to highly symmetrical situations. • Superposition works. – Two wires can be treated separately and the results added (VECTORIALLY!) • The individual parts of the calculation can be handled (usually) without the use of vector calculations because of the symmetry. • THIS IS SORT OF LIKE GAUSS’s LAW WITH AN ATTITUDE! Magnetism 123 The figure below shows a cross section of an infinite conducting sheet carrying a current per unit x-length of l; the current emerges perpendicularly out of the page. (a) Use the Biot–Savart law and symmetry to show that for all points P above the sheet, and all points P´ below it, the magnetic field B is parallel to the sheet and directed as shown. (b) Use Ampere's law to find B at all points P and P´. Magnetism 124 FIRST PART Vertical Components Cancel Magnetism 125 Apply Ampere to Circuit L B Infinite Extent B current per unit length Current inside the loop is therefore : i L Magnetism 126 The “Math” B Infinite Extent B B ds m i 0 enclosed BL BL m 0L B Magnetism m 0 2 127 A Physical Solenoid Magnetism 128 Inside the Solenoid For an “INFINITE” (long) solenoid the previous problem and SUPERPOSITION suggests that the field OUTSIDE this solenoid is ZERO! Magnetism 129 More on Long Solenoid Field is ZERO! Field looks UNIFORM Field is ZERO Magnetism 130 The real thing….. Finite Length Weak Field Stronger - Leakage Magnetism 131 Another Way Ampere : B ds m i 0 enclosed 0h Bh m 0 nih B m 0 ni Magnetism 132 Application • Creation of Uniform Magnetic Field Region • Minimal field outside – except at the ends! Magnetism 133 Two Coils Magnetism 134 “Real” Helmholtz Coils Used for experiments. Can be aligned to cancel out the Earth’s magnetic field for critical measurements. Magnetism 135 The Toroid Slightly less dense than inner portion Magnetism 136 The Toroid Ampere again. We need only worry about the INNER coil contained in the path of integratio n : B ds B 2r m Ni (N total # turns) 0 so m 0 Ni B 2r Magnetism 137