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Motors. Physics 102 Professor Lee Carkner Lecture 20. Ring in Solenoid. If the current flows clockwise through the solenoid, the B field inside is straight down To get maximum flux, the ring should face up (same direction as solenoid)
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Motors Physics 102 Professor Lee Carkner Lecture 20
Ring in Solenoid • If the current flows clockwise through the solenoid, the B field inside is straight down • To get maximum flux, the ring should face up (same direction as solenoid) • We need to find the flux through the loop before and after the current is switched off • F = BA cos q = BA • B = m0nI = (4pX10-7)(1000)(10) = 0.0126 T • A = (0.1)(0.1) = 0.01 m2
Current in Ring • F = BA = (0.0126)(0.01) = 1.26 X 10-4 Wb • In 1 second the flux goes to 0 • DF = (1.26 X 10-4) - (0) = 1.26 X 10-4 • Dt = 1 • e = -N(DF/Dt) = (1)(1.26 X 10-4) = 1.26 X 10-4 V • DV = IR or I = e/R = 1.26 X 10-4/10 • I = 1.26 X 10-5 A
Motional emf • If we make the loop larger or smaller, or move it in or out of a field, we will induce a potential • remember emf is a potential difference (or voltage) • How does motion in a field translate to voltage?
The area of the loop increases by LDx in time Dt but Dx = vDt, so DA = LvDt DF/Dt = BDA/Dt = (BLvDt)/Dt e = BLv Motional emf - Derived DA X B field into page v L x Dx in time Dt
Motional emf -- Direction • If the area decreases, the flux decreases and thus the induced B field is in the same direction as the original
Generators • What is the most efficient way to use inductance to produce current? • This changing flux produces an emf in the loop • Turn the loop with an external source of work • A machine that converts work into emf is called a generator
Alternating Current • Which way does the current flow? • As the loop turns the flux points in one direction and then the other • If the loop is turned quickly, the changes in direction can occur rapidly • This is called alternating current
emf From a Generator • Consider a loop of wire rotating in a magnetic field with angular speedw • From Faraday’s Law: e = N(DF/Dt) • The cos q term changes with time and can be related to the angular frequency w (radians/second) • The change of F with time is thus BAw sin wt, so the emf is: e = NBAw sin wt
Sinusoidal Variations emax • As the loop makes one complete rotation (wt goes from 0 to 2p radians) the emf goes from 0, to maximum +, to maximum -, and back to zero again • The current through the loop goes one way and then the other, sometimes is weak and sometimes is strong
Frequency • The number of these cycles made per second is the frequency f = w/2p • 1 turn per second (f=1) means 2p radians per second (w=2p) • NBAw is the maximum emf • sin wt tells us where we are in the cycle between positive and negative maximums
Power Generation • A potential difference causes current to flow • Produced (in general) in two ways: • Chemical reactions separate charges so that one terminal is + and one is - • A changing magnetic field separates charges
Motors • If you run a generator backwards it becomes a motor • Motor converts emf to work • This reduces the emf of the loop and is called back emf • Example: A motor initially has 120 volts, but if the motor produces a back emf of 70 volts, then the total emf is 50 volts
Eddy Currents • As the field through the loop drops, it induces a field in the same direction • If the object is not a loop, circular currents can still be induced which have the same effect • Net effect: • Metal objects moving through a magnetic field will be slowed
Next Time • Read 21.7, 21.9-21.11 • Homework: Ch 21, P 14, 23, 30, 39
What is the direction of current in the loop from the PAL (seen from top down)? • clockwise • counterclockwise • left • right • down
A bar magnet held north pole up is dropped straight down through a face up coil of wire. What is the direction of the current in the coil as the magnet enters and leaves the coil? • clockwise, counterclockwise • counterclockwise, clockwise • clockwise, clockwise • counterclockwise, counterclockwise • no current is induced