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Physics 212 Lecture 15

Physics 212 Lecture 15. Ampere’s Law. Music. Who is the Artist? Oscar Peterson Kenny Barron Dave Brubeck Thelonius Monk Marcus Roberts. A classic for a classic day. Physics 212 Lecture 17. “ Pretty neat stuff. I like how similar this is to Gauss’s law. ”

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Physics 212 Lecture 15

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  1. Physics 212 Lecture 15 Ampere’s Law

  2. Music • Who is the Artist? • Oscar Peterson • Kenny Barron • Dave Brubeck • Thelonius Monk • Marcus Roberts A classic for a classic day Physics 212 Lecture 17

  3. “Pretty neat stuff. I like how similar this is to Gauss’s law.” “Need more explanation on the magnetic field directions. ” Easier method to calculate magnetic fields Your Comments “You should probably look at getting some of the images up and running properly, its hard to deduce anything unless I try to imagine what youre asking about, which in any case i would be right all the time.” “I find this kind of confusing. Also most of the checkpoint pictures didn’t work for me, so I can’t go back and study from them. It makes it more confusing when I can’t see the pictures to answer questions..” Sorry! We’ll go through the checkpoints (with pictures) Spend some time building the integrals “Integrals are my greatest enemy ” “Daaag man, my boy Gauss be gettin’ his style cramped by dat Ampere clown.” Hour Exam II – THURSDAY Mar. 29 05

  4. LHS: RHS: General Case Infinite current-carrying wire :05

  5. Practice on Enclosed Currents Checkpoint 1c Checkpoint 1a Checkpoint 1b Ienclosed = 0 Ienclosed = 0 Ienclosed = I Ienclosed = 0 Ienclosed = I Ienclosed = I For which loop is B·dl the greatest? A. Case 1 B. Case 2 C. Same For which loop is B·dl the greatest? A. Case 1 B. Case 2 C. Same For which loop is B·dl the greatest? A. Case 1 B. Case 2 C. Same :08

  6. An infinitely long hollow conducting tube carries current I in the direction shown. Cylindrical Symmetry X X X X Enclosed Current = 0 Checkpoint 2a Check cancellations What is the direction of the magnetic field inside the tube? A. clockwise B. counterclockwise C.radially inward to the center D.radially outward from the center E. the magnetic field is zero “If you point your thumb in the direction of I, your fingers curl CW.” “Force is tangent to the cylinder so according to the RHR the magnetic field must be radailly towards the middle ” “The enclosed current is zero, and if you take a non-zero closed path, then we zeo that the field MUST be zero in order for amperes law to hold true” :22

  7. Ampere’s Law(+ integrals + magnetic field directions) I intoscreen :12

  8. dl B dl B B dl Ampere’s Law :14

  9. B dl B dl B dl Ampere’s Law :16

  10. B dl B dl dl B Ampere’s Law :16

  11. Which of the following current distributions would give rise to the B.dL distribution at the right? A C B :18

  12. :19

  13. :19

  14. :19

  15. Match the other two: B A :21

  16. A current carrying wire is wrapped around a cardboard tube as shown below. Checkpoint 2b In which direction does the magnetic field point inside the tube? A. Left B. Right C. Up D. Down E. Out of screen Use the right hand rule and curl your fingers along the direction of the current. :22

  17. Simulation :23

  18. Solenoid n = # turns/length Several loops packed tightly together form a uniform magnetic field inside, and nearly zero magnetic field outside. 1 2 3 4 From this simulation, we can assume a constant field inside the solenoid and zero field outside the solenoid, and apply Ampere’s law to find the magnitude of the constant field inside the solenoid !! :28

  19. Similar to the Current Sheet • Total integral around the loop

  20. Example Problem y For circular path concentric w/ shell An infinitely long cylindrical shell with inner radiusaand outer radiusbcarries a uniformly distributed currentIout of the screen. Sketch |B| as a function of r. I a x • Conceptual Analysis • Complete cylindrical symmetry (can only depend on r) can use Ampere’s law to calculate B • B field can only be clockwise, counterclockwise or zero! b • Strategic Analysis • Calculate B for the three regions separately: • 1) r < a • 2) a < r < b • 3) r > b :31

  21. Example Problem y so 0 I r a b x What does |B| look like for r < a ? (A) (B)(C) :33

  22. Example Problem y I I r a b x What does |B| look like for r > b ? (A) (B)(C) :35

  23. Example Problem y LHS: RHS: What does |B| look like for r > b ? dl I r B a b x (A) (B)(C) :36

  24. Example Problem y j = I / area I What is the current density j (Amp/m2) in the conductor? a b x (A) (B)(C) :40

  25. Example Problem y I r a b x What does |B| look like for a < r < b ? (A) (B)(C) :43

  26. Example Problem y Starts at 0 and increases almost linearly What does |B| look like for a < r < b ? I r a b x (A) (B)(C) :45

  27. Example Problem y An infinitely long cylindrical shell with inner radiusaand outer radiusbcarries a uniformly distributed currentIout of the screen. Sketch |B| as a function of r. I a x b :48

  28. Example Problem y An infinitely long cylindrical shell with inner radiusaand outer radiusbcarries a uniformly distributed currentIout of the screen. Sketch |B| as a function of r. I a x How big is B at r = b? b Suppose I = 10 A, b = 1 mm :48

  29. Follow-Up y X Add an infinite wire along the z axis carrying current I0. What must be true about I0 such that there is some value of r, a < r < b, such that B(r) = 0 ? I a I0 x A) |I0| > |I| AND I0 into screen b B) |I0| > |I| AND I0 out of screen C) |I0| < |I| AND I0 into screen D) |I0| < |I| AND I0 out of screen E) There is no current I0 that can produce B = 0 there B will be zero if total current enclosed = 0 :48

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