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Physics 102: Lecture 09. Currents and Magnetism. Exam 1 Monday night Conflicts, etc.—see course home page Be sure to bring your ID and go to correct room Review Sunday, 3-5 PM, Rm. 141 I will work through HE1 from last semester (fall ‘10)
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Physics 102:Lecture 09 Currents and Magnetism • Exam 1 Monday night • Conflicts, etc.—see course home page • Be sure to bring your ID and go to correct room • Review Sunday, 3-5 PM, Rm. 141 • I will work through HE1 from last semester (fall ‘10) • To be most useful, you should work the exam yourself prior to the review
Summary of Today • Last time: • Magnetic forces on moving charge • magnitude F = qvBsin() • direction: right-hand-rule • Today: • Magnetic forces on currents and current loops • Magnetic fields due to currents • long straight wire • solenoid
B v I = q/t + + + + L = vt Force of B-field on Current • Force on 1 moving charge: • F = q v B sin(q) • Out of the page (RHR) B v q + • Force on many moving charges: • F = q v B sin(q) • = (q/t) (vt) B sin(q) • = I L B sin(q) • Out of the page!
Preflight 9.1 c d B I B L I F=IBLsin b a A rectangular loop of wire is carrying current as shown. There is a uniform magnetic field parallel to the sides a-b and c-d. Here = 0 What is the direction of the force on section a-b of the wire? 60% 25% 15% force is zero out of the page into the page
Preflight 9.2 c d B I b a A rectangular loop of wire is carrying current as shown. There is a uniform magnetic field parallel to the sides a-b and c-d. F What is the direction of the force on section b-c of the wire? 8% 20% 72% force is zero out of the page into the page
Force on loop c d B I B L I F=IBLsin b a A rectangular loop of wire is carrying current as shown. There is a uniform magnetic field parallel to the sides a-b and c-d. Here = 180° Force on section c-d is zero! Same as a-b
ACT: Force on loop (cont’d) c d B I b a A rectangular loop of wire is carrying current as shown. There is a uniform magnetic field parallel to the sides a-b and c-d. F What is the direction of the force on section d-a of the wire? force is zero out of the page into the page
Torque on Current Loop in B field c d B I b a F d c a F b Look from here B F F The loop will spin in place! Preflights 9.3, 9.4: Net force on loop is zero. But the net torque is not!
Torque on Current Loop F d c a F b The loop will spin in place! Recall from Phys 101: F q B B w F L d F a d F Force on sections b-c and a-d: F = IBw B a Torque on loop is t= LF sin(q) = ILwBsin(q) B c c Lw = A ! b F Torque is: b F
ACT: Torque on Current Loop What is the torque on the loop below? • t < IAB • t = IAB • t > IAB x xxxxxxxxxxxxxxx x xxxxxxxxxxxxxxx x xxxxxxxxxxxxxxx x xxxxxxxxxxxxxxx x xxxxxxxxxxxxxxx x xxxxxxxxxxxxxxx x xxxxxxxxxxxxxxx x xxxxxxxxxxxxxxx t = 0
Torque on Current Loop It is useful to define normal vector⊥ to loop F F normal F d f f normal q a normal normal S N B B B f=0 f=0 F f = 180 – q d c F a b F F B Note torque will align normal parallel to B like a magnetic dipole! c If there are N loops: Torque is: Even if loop is not rectangular, as long as it is flat b F
Orbits of electrons “spin” Current loops act like dipoles Electron orbit and “spin” are current loops Why some materials are magnetic Nuclear Magnetic Resonance (NMR) and MRI
B B I I (2) ACT: Torque (1) Compare the torque on loop 1 and 2 which have identical area, and current. Normal vector points out of page for both! f = 90 1) t1 > t2 2) t1 = t2 3) t1 < t2 t = I A B sin(f)
Currents create magnetic fields • Straight wire carrying current I generates a field B at a distance r: Magnitude “Permeability of free space” (similar to e0 for electricity) B • “Right-hand rule 2”: • Thumb of right hand along I • Fingers of right hand along r • Out-of-palm points along B r Direction I(out of page) B field circles wire Note: there are different versions of RHR
F F ACT/Preflight 9.6 A long straight wire is carrying current from left to right. Near the wire is a charge q with velocity v B v q q v • • (b) (a) r r I Compare magnitude of magnetic force on q in (a) vs. (b) 34% 50% 16% a) has the larger force b) has the larger force c) force is the same for (a) and (b) Same Same Same magnitude Different directions q = 90 for (a) and (b)!
ACT: Adding Magnetic Fields Two long wires carry opposite current B x What is the direction of the magnetic field above, and midway between the two wires carrying current – at the point marked “X”? 1) Left 2) Right 3) Up 4) Down 5) Zero
B B F F Example Force between current-carrying wires Currents in same direction Currents opposite direction I towards us I towards us Another I towards us Another I away from us Currents in same direction attract! Currents in opposite direction repel!
+ Comparison:Electric Field vs. Magnetic Field Electric Magnetic Source Charges Moving Charges Acts on Charges Moving Charges Force F = Eq F = q v B sin(q) Direction Parallel E Perpendicular to v,B Field Lines Opposites ChargesAttract Currents Repel
ACT: Force between Wires What is the direction of the force on the top wire, due to the two below? 1) Left 2) Right 3) Up 4) Down 5) Zero
Solenoids • A solenoid consists of N loops of wire Magnitude B is uniform everywhere inside of solenoid: n is the number of turns of wire/meter (n = N/L) N S • Use “Right-hand rule 2” Direction B I B field lines look like bar magnet! Solenoid has N and S poles! I B
ACT: The force between the two solenoids is … (1) Attractive (2) Zero (3) Repulsive Look at field lines, opposites attract. Look at currents, same direction attract.
Summary of Right-Hand Rules Alternate RHR 1 RHR 2 Force on moving q B field from current I Straight wire I Solenoid B r I B I