# © 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.

## Presentation on theme: "© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their."— Presentation transcript:

© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their courses and assessing student learning. Dissemination or sale of any part of this work (including on the World Wide Web) will destroy the integrity of the work and is not permitted. The work and materials from it should never be made available to students except by instructors using the accompanying text in their classes. All recipients of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of other instructors who rely on these materials. Lecture PowerPoints Physics for Scientists and Engineers, 3 rd edition Fishbane Gasiorowicz Thornton

Chapter 25 Capacitors and Dielectrics

Main Points of Chapter 25 Definition of capacitance Calculation of capacitance Energy in capacitors and in electric fields Equivalent capacitance for series and parallel connections Dielectrics Microscopic description of dielectrics

25-1 Capacitance Simplest capacitor – two equal and oppositely charged conductors Parallel-plate capacitor:

25-1 Capacitance Coaxial cable: Spherical capacitor:

25-1 Capacitance Conductors of arbitrary shape and size: Isolated conductor: Q: Where’s the other plate? A: At infinity, effectively.

25-1 Capacitance Potential difference between the conductors depends on the charge on them V α Q Definition of capacitance: C = Q/V Depends only on geometry and materials

25-1 Capacitance Capacitance of a parallel-plate capacitor Field is uniform in middle of capacitor Capacitance (ignoring edge effects): (25-4)

25-2 Energy in Capacitors Each bit of charge added increases the electric field; subsequent charges take more work Total work to charge capacitor to Q: (25-7)

25-2 Energy in Capacitors Potential energy of a charged capacitor: (25-8) (25-9) (25-10) All three expressions are equivalent!

25-3 Energy in Electric Fields Using the known electric field inside a parallel-plate capacitor: (25-11) Then dividing by the capacitor’s volume Ad, we find the energy density: (25-12)

This is a general expression for the local energy density in free space, for a constant or variable electric field—not just for a parallel-plate capacitor. 25-3 Energy in Electric Fields (25-12)

25-4 Capacitors in Parallel and in Series Finding the equivalent capacitance: Parallel connection (25-14)

25-4 Capacitors in Parallel and in Series Finding the equivalent capacitance: Series connection (25-14) Just remember—the equivalent capacitance is C eq, not 1/C eq !

25-5 Dielectrics Dielectric = insulator Molecules act as dipoles, permanent or induced This effectively reduces the electric field

25-5 Dielectrics Dielectric also increases capacitance: (25-18) Some dielectric constants:

25-5 Dielectrics If the charge is held constant, insertion of a dielectric causes the voltage to decrease:

25-5 Dielectrics If the voltage is held constant, insertion of a dielectric causes the charge to increase:

25-5 Dielectrics Addition of dielectric to capacitor modifies capacitance equation – use ε instead of ε 0 : (25-23) Dielectric strength – maximum electric field that a material can sustain before breaking down (becoming conductive as electrons are ripped off atoms by intense field)

25-6 The Microscopic Description of Dielectrics For polar molecules (having a permanent dipole moment), an external field tends to rotate them

25-6 The Microscopic Description of Dielectrics For nonpolar molecules, an external field tends to polarize them

25-6 The Microscopic Description of Dielectrics In either case, the induced electric field reduces the overall field:

25-6 The Microscopic Description of Dielectrics Gauss’ Law If the dielectric is uniform (same  throughout): If not: (25-28) (25-29)

Summary of Chapter 25 Capacitor is two equal and oppositely charged conductors Capacitance depends only on geometry and dielectrics Electric fields carry energy Capacitors in parallel add; capacitors in series add reciprocals Dielectrics reduce electric field, increasing capacitance

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