Unformatted text preview: Inductance
Faraday's Law: Faraday' Big Picture
B = E d =  d dt ( B dA) =  ddt Electrostatics Circuits Magnetics Chapter 27: Magnetic Force on Charges and currents Chapter 28: Sources of Magnetic Field Chapter 29: Electromagnetic Induction Chapter 30: Self Inductance and Inductors Lenz's Law: Lenz' Motional emf: emf: Induced magnetic field will oppose the change in the system. Lenz's Law Faraday's Law Faraday' Lenz' =
Binduced
Wednesday, 28 March 2007 d B =B v dt I= R = B v R
1 Optics
Wednesday, 28 March 2007 2 B2 Mutual Inductance
Coil 1: N1 turns, radius R1 Coil 2: N2 turns, radius R2 R1 << R2 What is the flux of 2 through 1? B2 Mutual Inductance
Coil 1: N1 turns, radius R1 Coil 2: N2 turns, radius R2 R1 << R2 What is the flux of 2 through 1? Through 1 turn of Coil 1:
A1 2 B1 = B2 dA1 = B2 dA1 = B2 dA1 = B2 A1 = B2 (R1 ) Through 1 turn of Coil 1: B1 = N 2 Through N1 turn of Coil 1:
2 1 o I2
2 B2 dA1 A1 B2 constant A1 = N1 N 2 o I 2
2 (d 2 R2 2 B2 = N 2 o I 2
2 (d 2 R2 2 2 + R2 ) 3/ 2 B1 = N 2 o I2
2 (d 2 R2 2 2 + R2 ) 3/ 2 (R )
3 (d +R R
2 2 3/ 2 2 2 2 ) (R )
2 1 +R Mutual Inductance: M = N1
Wednesday, 28 March 2007 Wednesday, 28 March 2007 B1 oR R = N1 N 2 I2 2 d 2 + R2 ( 2 3/ 2 2 2 2 1 2 2 3/ 2 ) (R )
2 1 ) 4 1 B2 Mutual Inductance
Coil 1: N1 turns, radius R1 Coil 2: N2 turns, radius R2 R1 << R2 What is the flux of 2 through 1? Mutual Inductance II
Solenoid 1: N1 turns, radius R1 Solenoid 2: N2 turns, radius R2 21 = B2 dA1
= B2 dA1 = N1 B2 A2 N2
2 = N1 B2 R2 B2 dA1 12 = B1 dA2 = B1 dA2 = N 2 B1 A2 N 2 = N 2 1 o I1 R2 = MI1 M = o N1 N 2 Mutual Inductance: M = N1 B1 = N 2 B2 I2 I1
Units: H(Henries) = B2 0 outside of R2 Tm 2 Vs J = = A A A2 ( ) o I 2 (R22 ) ( ) d B = N dt
Wednesday, 28 March 2007 dI Mutual = M 2 Induced emf: 1 emf: dt dI 2 = M 1 dt
5 = N1 = MI 2 (R )
2 2
6 Wednesday, 28 March 2007 Question
The mutual inductance M = N1 A. Current in Coil 1 B1 = N 2 B2 depends on: depends I2 I1 Tesla Coil
Consider the following circuit: Vac Vsolenoid 1 = 0 Vsolenoid 1 = Vac = = d turn 1 Vac = dt N1 Vac A1 d turn 2 = N1 A2 dt d total 1 d turn 1 = N1 dt dt A1 turn 2 A2 d turn 1 A1 d turn 2 = dt A2 dt B. Magnetic flux in Coil 2 C. N1 D. N2 E. C & D turn 1 = d turn 2 Vac A2 = dt N1 A1 N1 = 10 N 2 = 10,000
Vac 15,000 V
8 total 2
Wednesday, 28 March 2007 7 AN d turn 2 = Vac 2 2 = N2 A1 N1 dt Wednesday, 28 March 2007 2 Tesla Coil in Reverse  Transformer
When electricity moves from a power plant it is put into a very high voltage to be able to travel long distances (~155,000 V to ~765,000 V). ~765,000 For us to use it, the electricity is "steppeddown" to a lower level using a stepped down" transformer (maintaining the same frequency). This lower voltage electricity is put into the local electric wires at a substation. Once smaller substation. transformers take that voltage down to usually 7,200, the power leaves this substation. A transformer on top of a utility pole, or one connected to underground underground wires, transforms the 7,200 volts into 220240 volts. This is then sent into 220your home over three wires. The three wires go through the electric electric meter, which measures how much electricity you use. One of the three three wires is the ground, and the other two are the positives. Some of the electrical appliances in your home use the 220240 volts. 220These are things like a water heater, stove and oven, or air conditioner. conditioner. They have very special connections and plugs. Other devices, like your like TV or computer only use onehalf of the electricity  110120 volts. one110Wednesday, 28 March 2007 9 B Can Crusher C C = 147 F = 3500 V 1 U = CV 2 = 900 J 2 Must be a net force! B d B Lenz's Law: Lenz' dt Oppose the change in
flux! Change the area! I induced F is inward everywhere!
Wednesday, 28 March 2007 10 Self Inductance
A current loop can create a flux through itself! Consider a solenoid: Energy in Inductors
N I
dI dt dI = 0 Multiply through by I dt dI Power Equation! I  I 2 R  LI =0 dt 1 dU L dU = Pdt = LIdI U L = LI 2 PL = 2 dt
Apply Kirchhoff's Rule: Kirchhoff' B = o nI = o
N I (R N ) =
2  IR  L = B dA = BA = o
L= o N 2R 2 I = LI PL = LI o N R
2 2 = o n2 A is the self inductance of the solenoid. What if the current changes? = dI d B d =  (LI ) =  L dt dt dt
11 L = on2 A B2 B2 A 1 1 2 = U = LI 2 = o n A 2 o n2 2o 2 2
Solenoids: B = o nI Compare to the energy density of Efield, found Efrom capacitors: Inductors oppose change in the current through them!
Wednesday, 28 March 2007 uB = B2 U = vol 2 o Wednesday, 28 March 2007 Energy is stored in the magnetic field through the inductor! 1 uB = o E 2 2
12 3 Energizing an RL Circuit
At t = 0: 0: I=0 At t : I = /R For 0 < t < , apply Kirchhoff's Rule: Kirchhoff' DeEnergizing an RL Circuit DedI dt  IR  L dI =0 dt  IR = L
I= (  IR )dt = LdI
R  I dt = LdI R Rdt dI = L ( R  I ) eL = R t ( R
R t L RI) R 1 e R  t L For 0 < t < , apply Kirchhoff's Rule: Kirchhoff' dI = 0 VR2 = 0 dt I R1 = IL = R1 R1 At t = 0 (when switch is opened): Change is bad! I L = opened): R1
I R1 Switch has been closed "a long time" time" IL VL = 0, b c ( ( R  I )e = R
R  t L R  I ) = ( R )e
R  t L I = I f 1 e L = R  t L L dI  IR2 = 0 dt dI = IR2 dt dI is negative dt dI R =  2 dt I L ln R R t = ln ( R  I ) L
Wednesday, 28 March 2007 I R = 2t Io L I = Ioe  t =  IR = e 1 I = I oe  R2 t L L R2
14 13 Wednesday, 28 March 2007 Good for surge protectors! R4
I1 R1 RLC Circuits
I2
I3 R3 Material for Exam 3
IC = 0 IR2 = 0 L1
C I1 L2
R2 Immediately after closing the switch ... At t = 0: 0: IL1 = 0 IL2 = 0 Chapter 27: All Chapter 28: Sections 2 through 7 28.8: 3 slides from lecture Not 28.1 = (R1+ R3+ R4)
At t : IL1 = 0 because the capacitor is charged! IC = 0 IL2 = 0 IR2 = 0 Chapter 29: Sections 1 through 6 Not 29.7, 29.8 I1 = I 2 + I 3 I 2 + I 3 = I1
Wednesday, 28 March 2007  I1R4 +  I1R1  I 3 R3 = 0  I1R4 +  I1R1  I 2 R2 = 0
15 Chapter 30: Sections 1 through 4 Not 30.5, 30.6 Wednesday, 28 March 2007 16 4 ...
View
Full Document
 Fall '07
 JapGuy
 Inductance, Magnetic Field, Inductor, Faraday's law of induction, DT DT DT, B Lenz

Click to edit the document details