Presentation is loading. Please wait.

Presentation is loading. Please wait.

Announcements Reminders: No lectures next week: Feb 15 th and Feb 17 th Quiz II: March 3rd, Ch 25,26, most of 27. {tentative}

Similar presentations


Presentation on theme: "Announcements Reminders: No lectures next week: Feb 15 th and Feb 17 th Quiz II: March 3rd, Ch 25,26, most of 27. {tentative}"— Presentation transcript:

1

2 Announcements Reminders: No lectures next week: Feb 15 th and Feb 17 th Quiz II: March 3rd, Ch 25,26, most of 27. {tentative}

3 Exam Grades Median: 85.5 % {high B+} Mean: 82.8% {low B+} Stdev: 13.2% Questions: email or ask in office hrs

4 Exam Histogram

5 Exam Comments Most Common issues: Field does NOT depend on the magnitude of the test charge, but does on the distance. The force from a field on a charge depends on the sign of the charge. Not all oscillatory motion is simple harmonic motion! On each exam, there should be: Score, Exam Grade Overall Grade The overall grade is what you would have now. If there are two grades this indicates that you are at an interface.

6 Capacitor Two conductors carrying charges of equal magnitude but opposite sign form a capacitor. +Q -Q A parallel plate capacitor is a particularly common type: +Q-Q Capacitors have a voltage across them

7 Capacitor: Field Lines +q -q Perfect parallel plate capacitors have a uniform field. And of course a potential difference

8 Capacitors and Charge Capacitors store charge Capacitance is measure of how well it stores charge Capacitance is a constant for a given capacitor. Farad (F) is C/V, the unit of capacitance Typical capacitances are in  F or pF ranges.

9 Capacitors and Charge Capacitance is a constant for a given capacitor. The voltage (i.e. potential difference) used is this equation is positive. C depends only on the geometry of the capacitor! Note: the material doesn’t matter (except in between the plates} If I change the voltage (for a given geometry), I change the charge. If the charge changes, than the voltage must have changed

10 Finding Capacitance a b +Q+Q-Q-Q So we need to find the field the find the voltage (use Gauss law, withthe sphere as the gaussian surface )

11 Finding Capacitance a b +Q+Q-Q-Q

12 Finding Capacitance: isolated sphere a b +Q+Q-Q-Q a b +Q+Q-Q-Q The isolated sphere is the limit as b-> infinity of the concentric spheres

13 A Parallel Plate Capacitor d area A Dielectric constant 

14 Circuits: First glance wire (conductor) capacitor switch battery +– We will learn how to combine these elements and others as the class progresses. +– This is what is right here!

15 Batteries An ideal battery creates a voltage difference between the two sides +– E A battery can be used to charge a capacitor, and maintain a constant voltage.

16 Combining Capacitors wire (conductor) capacitor switch battery +– In Series: C1C1 C2C2 C3C3 C1C1 C2C2 C3C3 In Parallel: Same Voltages Voltages are the same across each capacitor Charges are the same on each capacitor

17 Each of the Capacitors above has a capacitance of 12  F. What is the combined capacitance of the whole system? A)12  FD) 36  F B)6  FC) 4  F Combining Capacitors

18 For complex problems, capacitors may be combined successively in pairs. 4  F 8  F 6  F 12  F6  F

19 Each of the Capacitors above has a capacitance of 12 pF. What is the combined capacitance of the whole system? A)12 pFC) 8 pF B)4 pFD) 20 pF 12 24 8


Download ppt "Announcements Reminders: No lectures next week: Feb 15 th and Feb 17 th Quiz II: March 3rd, Ch 25,26, most of 27. {tentative}"

Similar presentations


Ads by Google