1. Magnetism Magnetism: Permanent and Temporary
See FSU’s site for much more information!! 1

2. Magnetic Topics
Magnetism, B
Electromagnetic Induction

3. Assignments
Read and write reflections on Ch 36&37 in Conceptual Physics
Complete Summaries for 36&37

4. General Properties of Magnets
Like magnetic poles repel; unlike magnetic poles attract
Magnetic field lines are directed from north to south
Magnetic field lines always form close loops
A magnetic field exists around any wire that carries current

5. Gen’l Properties cont. Spinning electrons are small magnets.
A current-carrying wire experiences a force when the wire is perpendicular to a magnetic field. A coil of wire that carries a current has a magnetic field about a permanent magnet

6. Magnetic Facts
The source of all magnetism is moving electric charges. Surrounding every moving electron is both an electric field and a magnetic field. Even in a broken magnet, there is N and S. A small compass in a magnetic field will line up parallel with the magnetic field lines. Magnetic domains are regions of aligned atoms. Magnets can attract unmagnetized objects by temporarily producing magnetism in the object. Magnetic fields are always produced by current carrying wires.

7. The magnetic pole in the N Hemisphere is in Canada
The magnetic pole in the N Hemisphere is in Canada. The Earth’s magnetic field is probably due to convection currents in Earth’s molten interior. Magnetic deflection is the discrepancy between magnetic and true norths. The greatest force on an electron moving in a magnetic field is when the angle of motion is 90o. Cosmic rays are most intense at Earth’s poles producing aurorae. Earth’s geographic South pole is nearest its N pole. Electric fields can increase a moving electron’s speed.

8. A magnetic force field can accelerate an electron by changing its direction, not its speed.
If a current carrying wire in magnetic field is caused to move down, current flowing in the opposite direction will cause the wire to move up.

9. Forces Caused by Magnetic Fields
When a current-carrying wire is placed in a magnetic field, a force acts on the wire that is perpendicular to both the field and the wire. Meters operate on this principle.
Magnetic field strength is measured in tesla, T (one newton per ampere per meter).
b is the symbol for magnetic field

10. Forces cont.
An electric motor consists of a coil of wire (armature) placed in a magnetic field. When current flows in the coil, the coil rotates as a result of the force on the wire in the magnetic field.

11. Forces cont.
The force a magnetic field exerts on a charged particle depends on the velocity and charge of the particle and the strength of the magnetic field. The direction of the force is perpendicular to both the field and particle’s velocity.

12. Key Equations
F = BIL  Force on a current carrying wire in a magnetic field. Force = magnetic field strength x current x length of wire. Newton = tesla x amp x meter
F = BqV  Force of a magnetic field on a single charged particle. Force = magnetic field strength x charge x velocity of the charge. Newton = tesla x coulomb x m/s

13. E = - N DF / D t
Ampere’s Rule for parallel, straight conductors: F = 2k l I1 I2 / d
Transformer Equations
Pp = Ps  VpIp = VsIs
Is = Vp = Np
Ip Vs Ns
Induction
M = -Es / D Ip/ D t
L = -E / D I / D t

15. The small picture – how magnetism occurs
Domain theory – when enough atoms of a substance line up in the same direction
Strong magnets – iron and steel
Very strong – Alnico alloy
Weak – aluminum, platinum
Natural – magnetite or lodestodes formed when rock was molten

16. Magnetic field lines
Magnetic flux, (F) – number of field lines passing through a surface
Unit: weber = 1 nm/amp
Magnetic flux density, B = F /A
Unit: wb/m2 = nm/a m2 = n/am
1 wb/m2 = 1 Tesla
Earth, 10–4 T Humans, 10–11 T

17. Hand Rule #1- B field direction around a current carrying wire
Point thumb in direction of current in the wire
Fingers of your hand circle the wire and show the direction of the magnetic field
Knuckles, N
Finger tips, S

19. Hand Rule #2 – Determine the polarity of an electromagnet
Wrap the fingers of your right hand around the loops in the direction of the current
Extended thumb points toward the N pole of the electromagnet

20. Solenoid – conducting linear coil which acts like a bar magnet
Increase B, magnetic flux density by
Increasing the current
Adding loops of wire
Inserting an iron core into solenoid – now it is an electromagnet

21. Hand rule #3 – shows force acting on wire in B field
Lay right hand flat, palm up
Extend thumb 90 degrees to rest of fingers
Fingers point in direction of B field
Thumb points in direction of current, I
Imaginary vector coming up perpendicular out of the palm points in the direction of force acting on current carrying wire.

22. Fingers point in direction of b field
Thumb - direction of current flow
Imaginary vector coming from palm is direction that conductor is forced out of the field

24. Sample Problems
A straight wire that carries a 5.0 amp current is in a uniform magnetic field oriented at right angles to the wire. When 0.10 m of the wire is in the field, the force on the wire is 0.20 n. What is the strength of the magnetic field, B?

25. Solution Known: Unknown: I = 5.0 amp B =? L = 0.10m F = 0.20 N
F=BIL  B = F/IL
= 0.20N/5.0 amp(0.10m)
= 0.40 T

26. Sample Problem
A beam of electrons travels at 3.0 x 106 m/s through a uniform magnetic field of 4.0 x 10–1 T at right angles to the field. How strong is the force that acts on each electron?
Known Unknown
V = 3.0 x 106 m/s F =?
B = 4.0 x 10–1 T
Q = x 10–19 c

27. Solution F = BqV = 4.0 x 10–1 T (-1.6 x 10–19c)(3.0 x 106 m/s)
= -1.9 x 10–13 Tcm/s
= -1.9 x n

28. Moving Charges in a Magnetic Field
Right-Hand Rule for Moving Charges      

29. Sources http://www.walter-fendt.de/ph11e/electricmotor.htm
Other physics information:
Great diagrams of magnetic rules:

30. Electromagnetic Induction (EMI)
Relative motion between a conductor and a magnetic produces both current and a magnetic field
Electric current can be induced in a wire by moving a magnet up and down near the wire
More loops in a coil of wire (solenoid) increases the voltage produced
Placing an iron rod in a current-carrying wire, yields a greater magnetic field

31. A generator changes mechanical energy to electrical energy
A generator changes mechanical energy to electrical energy. A motor does opposite
An e-m wave contains perpendicular electric and magnetic fields
E-M waves travel at the speed of light

32. Michael Faraday and Joseph Henry around the same time…
Discovered that when there is relative motion between a magnetic field and a complete circuit (and the conductor cuts across the magnetic field), that electricity will flow!!! An induced EMF causes electricity to flow.

33. If current flows, there must be an EMF – this is EM induction
Faraday’s Law of Induction:
E = - N DF / D t
E, emf, volts
-N, # of turns of wire (- means the current opposes the change that induced it)
DF, change in flux in weber, wb
t, change in time, sec
This essentially says that the induced voltage in a coil is proportional to the product of the number of loops and the rate at which the magnetic field changes within those loops.

34. Sample Problem
If a coil of 200 turns is moved perpendicularly in a magnetic field at a constant rate, find the induced emf. The flux linkage change ( DF / D t)
is 4.00 x wb in sec.

35. Imagine what thousands of turns would produce!
If a coil of 200 turns is moved perpendicularly in a magnetic field at a constant rate, find the induced emf. The flux linkage change ( DF / D t)
is 4.00 x wb in sec.
E = - N DF
D t
E = (-200)(4.00 x 10 –6 wb)
1.00 x 10 –2 s
E = x 10 –2 v
Imagine what thousands of turns would produce!

36. Electric Generators
Convert mechanical energy into electrical energy by rotating a looped conductor (armature) in a magnetic field
Alternating-Current electricity produced is conducted by slip rings and brushes to be used *
Direct current can be produced by using split rings *

37. A = 2.0 m2 N = 35 B = .55 T Dt = 0.85 s E = -N D F / D t = - NBA / D t
A coil with a wire is wound around a 2.0 m2 hollow tube 35 times. A uniform magnetic field is applied perpendicular to the plane of the coil. If the field changes uniformly from 0.00 T to 0.55 T in 0.85 s, what is the induced emf in the coil?
A = 2.0 m2 N = 35
B = .55 T Dt = 0.85 s
E = -N D F / D t = - NBA / D t
E = 35 (0.55 T) (2 m 2)
0.85s
E = 45.3 v

38. Generator Output
Rectifier changes AC to DC
Inverter changes DC to AC

39. Lenz’s Law -
The direction of an induced current is such that the magnetic field resulting from the induced current opposes the change in he field that caused the induced current.
When the N pole of a magnet is moved toward the left end of a coil, that end of the coil must become a N, causing induced current flow in opposition.

40. Inductance
The property of an electric circuit by which a varying current induces a back emf in that circuit or a neighboring circuit.
Mutual Inductance, M
Self Inductance, L

41. Mutual Inductance, M
Effect that occurs in a transformer when a varying magnetic field created in the primary coil is carried through the iron core to the secondary coil, where the varying field induces a varying emf.
M = -Es / D Ip/ D t

42. M = Es D Ip/ D t
Shows the ratio of induced emf in one circuit to the rate of change of current in the other circuit.
M, inductance, Henry
Es, average induced emf across secondary
D Ip/ D t, time rate of change in current in primary coil
- sign, induced v opposes D I (Lenz’s law)

43. M = - Es So, Es = -M DIp DIp/D t D t Es = -1.25 h (10.0 a) 0.0250 s
Two coils have a mutual inductance of 1.25 henrys. Find the average emf induced in the secondary if the current in the primary builds up to 10.0 amp in sec after the switch is closed.
M = - Es So, Es = -M DIp
DIp/D t D t
Es = h (10.0 a) s
Es = v or 5.00 x 102 v

44. Self Inductance
Ratio of induced emf across a coil to the rate of change of current in the coil
L = -E / D I / D t
L, henry
I, current, amp
t, time, sec

45. Transformer
Two separate coils of wire placed near one another that are used to increase or decrease AC voltages with little loss of energy.
It contains a Primary coil and a Secondary coil
When the primary is connected to AC voltage, the changing current creates a varying magnetic field that is carried through the core to the secondary coil.

46. Transformer, cont.
In the secondary coil, the varying field induces a varying emf. This is called mutual inductance
Secondary voltage = secondary #turns
Primary voltage primary # turns
Power = Voltage x Current

47. Transformers lose no power
Pp = Ps  Vp Ip = Vs Is
Transformer Equation:
Is = Vp = Np
Ip Vs Ns

48. Transformer Problem A. Vs = NsVp/Np = 3000(90.0V) / 200 = 1.35 kV
A step-up transformer has a primary coil consisting of 200 turns and a secondary coil that has 3000 turns. The primary coil is supplied with an effective AC voltage of 90.0v. A) What is the Vs? B) If Is = 2.00a, find Ip. C) What is the power in the primary circuit?
A. Vs = NsVp/Np = 3000(90.0V) / 200 = 1.35 kV
B. Pp = Ps, VpIp = VsIs  Ip = VsIs/Vp =
Ip =1350v(2.00a) / 90.0v = 30.0a
C. Pp = Vp Ip = 90.0v(30.0a) = 2.70 kW