1. Sources of the Magnetic Field March 22, 2006

2. 1013-MarBREAK 1120-MarMagnetic FieldSources of B 1227-MarAmpere’s LawFaraday's LawFaraday’s Law 133-AprInductance EXAM #3 1410-AprInductance - FinishAC Circuits 1517-AprAC CircuitsEM FIELDSLight Topics 1624-AprLight TopicsNo Class FINAL EXAM 171-MayNo Class Schedule

3. Watsgoinondisweek? Today we start looking at how currents create magnetic fields. Today we start looking at how currents create magnetic fields. Quiz on Friday Quiz on Friday –Magnetism Chapter –NOT today’s material Next Exam is on April 7 th. Next Exam is on April 7 th. New WebAssign on Sources will be posted shortly. New WebAssign on Sources will be posted shortly.

4. Last time - Current Loop

5. A length L of wire carries a current i. Show that if the wire is formed into a circular coil, then the maximum torque in a given magnetic field is developed when the coil has one turn only, and that maximum torque has the magnitude … well, let’s see. Circumference = L/N

6. Problem continued…

7. NEW TOPIC: SOURCES OF THE MAGNETIC FIELD Chapter 30

8. Remember the wire?

9. Try to remember…

10. The “Coulomb’s Law” of Magnetism A Vector Equation … duck

11. For the Magnetic Field, current “elements” create the field. This is the Law of Biot-Savart

12. Magnetic Field of a Straight Wire We intimated via magnets that the Magnetic field associated with a straight wire seemed to vary with 1/d. We can now PROVE this!

13. From the Past Using Magnets

14. Right-hand rule: Grasp the element in your right hand with your extended thumb pointing in the direction of the current. Your fingers will then naturally curl around in the direction of the magnetic field lines due to that element.

15. Let’s Calculate the FIELD Note: For ALL current elements in the wire: d s X r is into the page

16. The Details

17. Moving right along 1/d

18. A bit more complicated A finite wire

19. P1P1 r   ds

20. More P 1

21. P2

22. APPLICATION: Find the magnetic field B at point P

23. Center of a Circular Arc of a Wire carrying current

24. More arc… ds

25. The overall field from a circular current loop Sorta looks like a magnet!

26. Iron

27. Howya Do Dat?? No Field at C

28. Force Between Two Current Carrying Straight Parallel Conductors Wire “a” creates a field at wire “b” Current in wire “b” sees a force because it is moving in the magnetic field of “a”.

29. The Calculation

30. Definition of the Ampere The force acting between currents in parallel wires is the basis for the definition of the ampere, which is one of the seven SI base units. The definition, adopted in 1946, is this: The ampere is that constant current which, if maintained in two straight, parallel conductors of infinite length, of negligible circular cross section, and placed 1 m apart in vacuum, would produce on each of these conductors a force of magnitude 2 x 10-7 newton per meter of length.

31. Ampere’s Law The return of Gauss

32. Remember GAUSS’S LAW?? Surface Integral

33. Gauss’s Law Made calculations easier than integration over a charge distribution. Applied to situations of HIGH SYMMETRY. Gaussian SURFACE had to be defined which was consistent with the geometry. AMPERE’S Law is the Gauss’ Law of Magnetism! (Sorry)

34. The next few slides have been lifted from Seb Oliver on the internet Whoever he is!

35. Biot-Savart The “Coulombs Law of Magnetism”

36. Invisible Summary Biot-Savart Law (Field produced by wires) Centre of a wire loop radius R Centre of a tight Wire Coil with N turns Distance a from long straight wire Force between two wires Definition of Ampere

37. Magnetic Field from a long wire I B r ds Using Biot-Savart Law Take a short vector on a circle, ds Thus the dot product of B & the short vector ds is:

38. Sum B. ds around a circular path I B r ds Sum this around the whole ring Circumference of circle

39. Consider a different path Field goes as 1/r Path goes as r. Integral independent of r i

40. SO, AMPERE’S LAW by SUPERPOSITION: We will do a LINE INTEGRATION Around a closed path or LOOP.

41. Ampere’s Law USE THE RIGHT HAND RULE IN THESE CALCULATIONS

42. The Right Hand Rule.. AGAIN

43. Another Right Hand Rule

44. COMPARE Line Integral Surface Integral

45. Simple Example

46. Field Around a Long Straight Wire

47. Field INSIDE a Wire Carrying UNIFORM Current

48. The Calculation

49. R r B

50. Procedure Apply Ampere’s law only to highly symmetrical situations. Superposition works. Two wires can be treated separately and the results added (VECTORIALLY!) The individual parts of the calculation can be handled (usually) without the use of vector calculations because of the symmetry. THIS IS SORT OF LIKE GAUSS’s LAW WITH AN ATTITUDE!

51. The figure below shows a cross section of an infinite conducting sheet carrying a current per unit x-length of l; the current emerges perpendicularly out of the page. (a) Use the Biot–Savart law and symmetry to show that for all points P above the sheet, and all points P´ below it, the magnetic field B is parallel to the sheet and directed as shown. (b) Use Ampere's law to find B at all points P and P´.

52. FIRST PART Vertical Components Cancel

53. Apply Ampere to Circuit Infinite Extent B B L

54. The “Math” Infinite Extent B B B  ds=0

55. A Physical Solenoid

56. Inside the Solenoid For an “INFINITE” (long) solenoid the previous problem and SUPERPOSITION suggests that the field OUTSIDE this solenoid is ZERO!

57. More on Long Solenoid Field is ZERO! Field is ZERO Field looks UNIFORM

58. The real thing….. Weak Field Stronger - Leakage Fairly Uniform field Finite Length

59. Another Way

60. Application Creation of Uniform Magnetic Field Region Minimal field outside except at the ends!

61. Two Coils

62. “Real” Helmholtz Coils Used for experiments. Can be aligned to cancel out the Earth’s magnetic field for critical measurements.

63. The Toroid Slightly less dense than inner portion

64. The Toroid