1. Lecture 41: WED 02 DEC Final Exam Review I Physics 2113 Jonathan Dowling

2. The Grading Midterms - 100 points each Final Exam - 200 points Homework - 75 points In Class PP- 25 points TOTAL: 600 points Numerical Grade: Total Points / 6

3. A+: 98-100 A: 92-97 A-: 89-91 B+: 86-88 B: 78-85 B-: 75-77 C+: 72-74 C: 63-71 C-: 60-62 D+: 57-59 D: 53-56 D-: 50-52 F: <50

4. Final Exam 3:00PM – 5:00PM MON 07DEC PHYS 2113-1 (Moreno) is scheduled to take their exam in Lockett 9 PHYS 2113-2 (Gaarde) is scheduled to take their exam in Lockett 10 PHYS 2113-3 (Dowling) is scheduled to take their exam in Lockett 6 PHYS 2113-4 (O'Connell) is scheduled to take their exam in Lockett 15 PHYS 2113-5 and 6 (Abdelwahab) is scheduled to take their exam in Lockett 2 PHYS 2113-7 (Hansen) Last name starts with A - K: take their exam in Lockett 10, last name starts with L - Z: take their exam in Lockett 2

5. Final Exam 100 PTS: CH 13, 21–30 / HW01-11 This part will be 11 multiple choice questions one from each chapter. 100 PTS: CH 31–33 / HW12-14 This part will be three multiple choice questions and three word problems, one each from each chapter.

6. What do you need to make on the final to get an A, B, C, etc.? A: 90–100 B: 75–89 C: 60–74 D: 50–59 F: <50 Solve this simple equation for x: Where mt1=exam1, mt2=exam2, mt3=exam3, hw=total points on your hws01–14 (out of 472), icppc=checks, icppx=X’s, icpp=number of times you were called on, max is the binary maximum function, and y is your desired cutoff number, y = 90, 75, 60, or 50. Then x is the score out of 200 you need on the final to make that cutoff grade y. This assumes no curve.

7. Example: John D’oh wants to know what he needs to make on the final in order to get an A- = 89 in this class. It is very likely impossible for John to get an A- as he’d need better than a perfect score on the final. How good does he need to do to avoid a C+ = 74? John is extremely unlikely to get an A, and is unlikely to get a C, so the most probable outcome is that John will get a B in this class.

10. LC Circuits

11. The magnetic field on the coil starts to deflux, which will start to recharge the capacitor. Finally, we reach the same state we started with (with opposite polarity) and the cycle restarts. PHYS2113 An Electromagnetic LC Oscillator Capacitor discharges completely, yet current keeps going. Energy is all in the B-field of the inductor all fluxed up. Capacitor initially charged. Initially, current is zero, energy is all stored in the E-field of the capacitor. A current gets going, energy gets split between the capacitor and the inductor.

13. Electric Oscillators: the Math Energy as Function of Time Voltage as Function of Time Amplitude = ?

14. Example In an LC circuit, L = 40 mH; C = 4  F At t = 0, the current is a maximum; When will the capacitor be fully charged for the first time?  = 2500 rad/s T = period of one complete cycle T =  = 2.5 ms Capacitor will be charged after T=1/4 cycle i.e at t = T/4 = 0.6 ms

15. Example In the circuit shown, the switch is in position “a” for a long time. It is then thrown to position “b.” Calculate the amplitude  q 0 of the resulting oscillating current. Switch in position “a”: q=CV = (1  F)(10 V) = 10  C Switch in position “b”: maximum charge on C = q 0 = 10  C So, amplitude of oscillating current = 0.316 A b a E =10 V 1 mH 1  F

16. Damped LCR Oscillator Ideal LC circuit without resistance: oscillations go on forever;  = (LC) –1/2 Real circuit has resistance, dissipates energy: oscillations die out, or are “damped” Math is complicated! Important points: –Frequency of oscillator shifts away from  = (LC) -1/2 –Peak CHARGE decays with time constant = –  QLCR =2L/R –For small damping, peak ENERGY decays with time constant –  ULCR = L/R C R L 048121620 0.0 0.2 0.4 0.6 0.8 1.0 E time (s) U

18. t(s) Q(t)

19. (31-27)

20. Example, Transformer:

23. Maxwell II: Gauss’ law for B-Fields: Maxwell II: Gauss’ law for B-Fields: field lines are closed or, there are no magnetic monopoles S SS S SS

25. B ! E i B i B Displacement “Current” Maxwell proposed it based on symmetry and math — no experiment! Changing E-field Gives Rise to B-Field!

26. 32.3: Induced Magnetic Fields: Here B is the magnetic field induced along a closed loop by the changing electric flux  E in the region encircled by that loop. Fig. 32-5 (a) A circular parallel-plate capacitor, shown in side view, is being charged by a constant current i. (b) A view from within the capacitor, looking toward the plate at the right in (a).The electric field is uniform, is directed into the page (toward the plate), and grows in magnitude as the charge on the capacitor increases. The magnetic field induced by this changing electric field is shown at four points on a circle with a radius r less than the plate radius R.

28. 32.5: Maxwell’s Equations: