W05D1 Conductors and Insulators Capacitance & Capacitors Energy Stored in Capacitors

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1 W05D1 Conductors and Insulators Capacitance & Capacitors Energy Stored in Capacitors W05D1 Reading Assignment Course Notes: Sections 3.3, 4.5,

2 Outline Conductors and Insulators Conductors as Shields Capacitance & Capacitors Energy Stored in Capacitors 2

3 Conductors and Insulators Conductor: Charges are free to move Electrons weakly bound to atoms Example: metals Insulator: Charges are NOT free to move Electrons strongly bound to atoms Examples: plastic, paper, wood 3

4 Charge Distribution and Conductors The Charged Metal Slab Applet: Non-zero charge placed in metal slab Charges move to surface (move as far apart as possible) Electric field perpendicular to surface, zero inside slab 4

5 Induced Charge Distribution in External Electric Field Charging by Induction, Exterior of a Neutral Metallic Box Induced charges move to surface Electric field perpendicular to surface, zero inside slab 5

6 Conductors in Equilibrium Conductor Placed in External Electric Field 1) E = 0 inside 2) E perpendicular to surface 3) Induced surface charge distribution 6

7 Hollow Conductors: Applet Charge placed OUTSIDE induces charge separation ON OUTSIDE. Electric field is zero inside. 7

8 Electric Field on Surface of Conductor 1) E perpendicular to surface 2) Excess charge on surface Apply Gauss s Law E surface A =! A " 0 # E surface =! " 0 8

9 Conductors are Equipotential Surfaces 1) Conductors are equipotential objects 2) E perpendicular to surface 9

10 Group Problem: Metal Spheres Connected by a Wire Two conducting spheres 1 and 2 with radii r 1 and r 2 are connected by a thin wire. What is the ratio of the charges q 1 /q 2 on the surfaces of the spheres? You may assume that the spheres are very far apart so that the charge distributions on the spheres are uniform. 10

11 Concept Question: Point Charge in Conductor A point charge +q is placed inside a hollow cavity of a conductor that carries a net charge +Q. What is the total charge on the outer surface of the conductor? 1. Q. 2. Q + q. 3. q. 4. Q - q. 5. Zero. 11

12 Hollow Conductors: Applet Charge placed INSIDE induces balancing charge ON INSIDE. Electric field outside is field of point charge. 12

13 Capacitors and Capacitance Our first of 3 standard electronics devices (Capacitors, Resistors & Inductors) 13

14 Capacitors: Store Electric Charge Capacitor: Two isolated conductors Equal and opposite charges ±Q Potential difference between them.!v C = Q!V Units: Coulombs/Volt or Farads C is Always Positive 14

15 Parallel Plate Capacitor; Applet Oppositely charged plates: Charges move to inner surfaces Electric field perpendicular to surface, zero inside plates 15

16 Calculating E (Gauss s Law) S! E! d A! "" = q in ( ) =! A Gauss E A Gauss σ Q E = = ε 0 Aε # 0 " 0 0 Note: We only consider a single sheet! Doesn t the other sheet matter? 16

17 Superposition Principle Between the plates:! E =! E + +! E! =! " 2# 0 ĵ! " 2# 0 ĵ =! " # 0 ĵ Above the plates:! E =! E + +! E! = + " 2# 0 ĵ! " 2# 0 ĵ =! 0 Below plates:! E =! E + +! E! =! " 2# 0 ĵ + " 2# 0 ĵ =! 0 17

18 Parallel Plate Capacitor!V = " E#! $ d S! = Ed = Q d C = Q A%!V = " A 0 d 0 top bottom C depends only on geometric factors A and d 18

19 Group Problem: Spherical Shells A spherical conductor of radius a carries a charge +Q. A second thin conducting spherical shell of radius b carries a charge Q. Calculate the capacitance. 19

20 Concept Question: Isolated Spherical Conductor What is the capacitance of an isolated spherical conductor of radius a? 1. Capacitance is not well defined. 4!" 0 a 2. Capacitance is. 3. Capacitance is infinite. 4. Capacitance is zero. 20

21 Demonstration: Capacitance of Van der Graaf Generator C = 4!" 0 a!v = k e Q a E = k e Q a 2!V = Ea 21

22 Capacitance of Earth For an isolated spherical conductor of radius a: C = 4πε 0a ε 0 = F m a = m C = F = 0.7mF A Farad is REALLY BIG! We usually use pf (10-12 ) or nf (10-9 ) 22

23 Energy To Charge Capacitor 1. Capacitor starts uncharged. 2. Carry +dq from bottom to top. Now top has charge q = +dq, bottom -dq 3. Repeat 4. Finish when top has charge q = +Q, bottom -Q 23

24 Stored Energy in Charging Capacitor At some point top plate has +q, bottom has q Potential difference is V = q / C Change in stored energy done lifting another dq is du = dq V 24

25 Stored Energy in Charging Capacitor So change in stored energy to move dq is: du = dqv = dq q C = 1 C q dq Total energy to charge to Q U = Q! du = 1! C q dq = 1 C 0 Q

26 Energy Stored in Capacitor Since C = Q!V U = Q 2 = 1 Q ΔV = 1 C ΔV 2 2C 2 2 Where is the energy stored??? 26

27 Energy Stored in Capacitor Energy stored in the E field! Parallel-plate capacitor: C =! o A d and V = Ed U = 1 2 CV 2 = 1 2! o A d ( Ed ) 2 =! E 2 o 2 " ( Ad) = u " (volume) E Energy density [J/m 3 ] u E =! o E

28 Demonstration: Changing Distance Between Circular Capacitor Plates E4 28

29 Concept Question: Changing Dimensions A parallel-plate capacitor is charged until the plates have equal and opposite charges ±Q, separated by a distance d, and then disconnected from the charging source (battery). The plates are pulled apart to a distance D > d. What happens to the magnitude of the potential difference V and charge Q? 1. V, Q increases. 2. V increases, Q is the same. 3. V increases, Q decreases. 4. V is the same, Q increases. 5. V is the same, Q is the same. 6. V is the same, Q decreases. 7. V decreases, Q increases. 8. V decreases, Q is the same. 9. V decreases, Q decreases. 29

30 Concept Question: Changing Dimensions A parallel-plate capacitor is charged until the plates have equal and opposite charges ±Q, separated by a distance d. While still connected to the charging source, the plates are pulled apart to a distance D > d. What happens to the magnitude of the potential difference V and charge Q? 1. V, Q increases. 2. V increases, Q is the same. 3. V increases, Q decreases. 4. V is the same, Q increases. 5. V is the same, Q is the same. 6. V is the same, Q decreases. 7. V decreases, Q increases. 8. V decreases, Q is the same. 9. V decreases, Q decreases. 30

31 Concept Question: Changing Dimensions A parallel-plate capacitor, disconnected from a battery, has plates with equal and opposite charges, separated by a distance d. Suppose the plates are pulled apart until separated by a distance D > d. How does the final electrostatic energy stored in the capacitor compare to the initial energy? 1. The final stored energy is smaller 2. The final stored energy is larger 3. Stored energy does not change. 31

32 Demonstration: Charging Up a Capacitor A 100 microfarad oil-filled capacitor is charged to 4 KV and discharged through a wire Stored Energy: U = 1 2 CV 2 = 1 2 (1!10"4 F)(4!10 3 V) 2 = 800 J 32