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Chapter 20-21-23 Review. The behavior of bar magnets.

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Presentation on theme: "Chapter 20-21-23 Review. The behavior of bar magnets."— Presentation transcript:

1 Chapter Review

2 The behavior of bar magnets

3 Our Earth itself has a magnetic field

4 Charges moving with respect to a field

5

6

7 The Right Hand Rule Using the right hand rule, one may determine the direction of the field produced by a moving positive charge.

8 Magnetism and circular motion F = |q|vB If the motion is Circular F = mv 2 /R R = mv/ |q|B ω = v/R = |q|B/m

9 Force on a conductor with current F = ILB

10 Applications of force on a conductor

11 Magnetic field of long straight conductor

12 Magnetic field of a long, straight wire: B = μ 0 I/(2πr) r is the distance from the wire μ 0 is called the permeability of vacuum μ 0 = 4π x T.m/A

13 Fields in two conductors side-by-side

14

15 2 wires with currents flowing in the same direction attract each other 2 wires with currents flowing in opposite directions repel each other F = μ 0 L(I 1 I 2 )/(2πr) Force per unit length F/L = μ0 (I1 I2)/(2πr)

16 Currents in a loop Magnetic field at the center of a circular loop B = μ o I /(2R) For N loops: B = μ o NI /(2R)

17 Electromagnetic Induction

18 Does the field induce a current or not?

19 Magnetic flux at various orientations

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22 FRADAY’s LAW When the magnetic flux Φ B changes in time, there is a an induced emf directly proportional to the time rate of change of the magnetic flux : ɛ = |Δ Φ B /Δt | If we have a coil with N identical turns, then ɛ = N |Δ Φ B /Δt |

23 V ab = vBL a b

24 Lenz’s Law

25

26 Transformers

27 TRANSFORMERS V 2 / V 1 = N 2 / N 1 If energy completely transformed V 1 I 1 = V 2 I 2

28 Energy associated with an induced current. energy is stored in an electronic device.

29 The R-L circuit

30 Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley The L-C circuit

31 In the case of an inductor with a capacitor, the energy is transferred from the electric field (capacitor) to magnetic field (inductor) and vice versa. The total energy is however conserved: The back and forth of the energy constitutes an oscillatory behavior with a frequency ω:

32 A metal loop moves at constant velocity toward a long wire carrying a steady current, as shown in the figure. The current induced in the loop is directed A) Clockwise B) counterclockwise C) zero

33 A metal loop moves at constant velocity toward a long wire carrying a steady current, as shown in the figure. The current induced in the loop is directed A) Clockwise B) counterclockwise C) zero B out of page increasing ΔΦ out of page B i into page

34 The slide wire of the variable resistor in the figure is moved steadily to the right, increasing the resistance in the circuit. While this is being done, the current induced in the small circuit A is directed : A) clockwise B) counterclockwise C) zero

35 I=V/R I decreases when R increases B due to I decreases as I decreases B out of page and decreases hence ΔΦ into page B i out of page I


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