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Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley Work and energy changes - Figures 18.3 Work is done on the charge by the field.
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Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Goals for Chapter 18 • To calculate electrical potential energy.
• To define potential.
• To study equipotential surfaces
• To review Millikan’s oil drop experiment.
• To examine capacitors.
• To determine electrical field energy
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Electrical and gravitational forces - Figures 18.1-18.2• The forces are similar and conservative.
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Work and energy changes - Figures 18.3• Work is done on the charge by the field.
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Parallel plates and energy conservation – Example 18.2• See the worked example on page 588 and Figure 18.8.
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Potential of point and plate charges – Examples 18.3,4• Refer to figures 18.9 and 18.10 with worked examples on pages 589-91.
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
The equipotential map around charges – Figure 18.11
•Around an charge or arrangement of charges regions of equal potential may be drawn as equal-potential lines.
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Equipotential lines may not cross – Figure 18.12
• Considering conduction and geometry one may prove why the lines do not cross.
• Refer to page 592 in your text.
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Robert Millikan and electronic charge – Figure 18.16
He suspended charged oil drops of various masses between the parallel plates of a capacitor. His determination found many different multiple of *the same number*. The number was the charge of a single electron, 1.60217653(14)x10-19C.
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Energetics of a single electron – Figure 18.17
One electron suspended in a 1V field allows the definition of an energy equivalence.
1eV = 1.602x10-19J
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
The capacitor – Figure 18.18
Devices may be constructed which separate two conductors of various sizes with materials of various conductance.
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
The symbol and units of capacitance – Figure 18.19
• Refer to pages 596 – 598 in your text.
• Define the Farad and follow worked examples 18.6 and 18.7.
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Capacitors are often joined – Figures 18.21
• Like resistors, capacitors may be combined sequentially (in series).
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Capacitors are often joined II – Figures 18.22
• Like resistors, capacitors may be combined in simultaneous fashion (in parallel).
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Capacitors store energy – Example 18.9
• This is the whine you can hear while an electronic flash charges.
•Refer to the worked example on pages 602-603.
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
What is between the conductors? – Figures 18.26,27• As we stated on an earlier slide, the amount of charge that may be stored in a capacitor depends in part on the “filler”.
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Capacitors with different dialectrics – Figure 18.28
• Select the dialelectric from table 18.1.
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley
Calculation with a specific dialectric – Example 18.10
Refer to the worked problem on page 605 and figure 18.29.