1. Physics II PHY 202/222 Magnetism
452 South Anderson Road
Rock Hill, SC 29730

2. Magnetism– Test 5 SP: 3 Beiser Chapters 27 MC: odd, SP: 5 – 17 odd
Browne Chapter for PHY 222 Students
26: 1,5,9
27: 2,
28: 7
29: 1, 2

3. Chapter 27 – Magnetism
Beiser p.319

4. Magnets
When we think of magnets we either consider permanent magnets or magnetic effects of moving charge. Since permanent magnets come from moving charge, we consider moving charge first.
Beiser p.319

5. Magnetic Fields Unit of magnetic field is the Tesla where
1 T = 1 N/Am = 1 Weber/m2 = 10,000 Gauss
The field around a strong permanent magnet is 0.1 T. An MRI is from 0.2 to 1.5 T. A junkyard electromagnet for lifting cars is 1 T.
Beiser p.319

6. Magnetic Field of a Straight Current
Every current in a wire generates a magnetic field.
Point the thumb of your right hand in the direction of the current, and your curled fingers will point in the direction of the field.
The magnitude at a distance s from the wire is given by the formula:
Beiser p.320

7. Magnetic Field of a Loop
A current in a loop of wire generates a magnetic field.
Point the fingers of your right hand in the direction of the current, and your thumb will point in the direction of the field inside the coil.
The magnitude of the field inside the loop is given by the formula:
Beiser p.321

8. Earth Magnetism
The Earth has a magnetic field due to currents of molten material in the core.
The magnitude is around
3 x T
Beiser p.322

9. Magnetic Force on a Moving Charge
A charge Q moving in a magnetic field B with velocity v will experience force F.
In the picture, the charge is moving to the right in a magnetic field into the screen. The magnitude of the force is given by
The force will be upwards as follows:
Put the thumb of your right hand in the direction of v. Put your fingers in the direction of B. Curl fingers up. Force will be in direction of fingers for a positve charge, and opposite for a negative charge. v
Magnetic field into screen F B +Q
Beiser p.323

10. Magnetic Force on a Currentv
Magnetic field into screen F B
Wire +Q I
L – Length of wire in magnetic field
F = I L B
The force will be upwards as follows:
Put the thumb of your right hand in the direction of I. Put your fingers in the direction of B. Curl fingers up. Force will be in direction of fingers.
Beiser p.323

11. Force Between two CurrentsL s
If currents are in opposite directions, the force is repulsive; same attractive.
Beiser p.324

12. Ferromagnetism
Beiser p.327

13. 27.6

14. 27.10

15. 27.12

16. 27.14

17. 27.16

18. Chapter 28 – Electromagnetic Induction
Beiser p.335

19. Electromagnetic Induction
A current is produced if:
If a conductor is moved in a magnetic field
If a magnet is moved near a wire, especially a coil of wire
A magnetic field changes near a conductor/coil.
For a straight conductor moving perpendicular to a magnetic field.
Beiser p.335

20. Faraday’s Law For a magnet moving in a coil:
Lenz’s Law: an induced current is always in the direction so that it’s own magnetic field opposes the effect that created it.
Hence the negative sign above.
Beiser p.335,6

21. Transformers N1 N2
Beiser p.337

22. Self Induction
A change in current in a conductor causes a change in magnetic field.
A change in magnetic field causes an self-induced emf.
Where L is the inductance of the circuit component.
For a solenoid:
Beiser p.339

23. Inductors in Combination

24. Energy of an Inductor
Beiser p.341

25. Time Constants and Current
When a switch in an inductive circuit is closed, the current builds up to it’s full value according to the formula:
Where the time constant, T = L / R.
Beiser p.341-3

26. 28.4

27. 28.6

28. 28.8

29. 28.10

30. 28.12

31. 28.14

32. 28.16

33. 28.18

34. 28.20

35. Chapter 29 – Alternating Current Circuits
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36. Alternating Current V = constant V = Vmax sin ωt I= Imax sin ωt
AC Alternating Current
V = Vmax sin ωt
I= Imax sin ωt
DC Direct Current
V = constant
Beiser p.350

37. Generators Split ring commutator Slip rings
Generator: Move the coil, electricity out. Motor: Electricity in, motion out.

38. Effective Values
Since the average AC voltage V = Vmax sin ωt is zero, we need a way to be able to calculate its capacity to do work. So we use the “effective value” or root-mean-square (rms) value.
Beiser p.350

39. Phase Angle
ELI – ICE
In an AC circuit with only an inductor (L) the voltage (E) leads the (I) current by 900.
In an AC circuit with only an capacitor (C) the current (I) leads the voltage (E) by 900.
In AC circuits with both inductors and capacitors you would have to find the phase angle as shown in the book.
Beiser p.353

40. Maxwell’s Equations
Gauss’s Law for electricity: Electric fields come from charges
Gauss’s Law for Magnetism: There are no magnetic charges/monopoles. Any “ball” has the same B out as in: sum =0
Faraday’s Law: Change in magnetic field makes electricity.
Ampere’s Law: Change in electric field makes magnetism.
ΔE → ΔB → ΔE → … propagates through space as light or other EM waves. WOW!
Browne p.343