# Understanding Force and Energy in Electricity  This chapter covers electrical energy, capacitance, potential energy, conservative force, and dissipative force. Learn why frictional force is dissipative, while Coulomb force is conservative.

• Uploaded on | 1 Views
• katherinepeters

## About Understanding Force and Energy in Electricity

PowerPoint presentation about 'Understanding Force and Energy in Electricity'. This presentation describes the topic on This chapter covers electrical energy, capacitance, potential energy, conservative force, and dissipative force. Learn why frictional force is dissipative, while Coulomb force is conservative.. The key topics included in this slideshow are . Download this presentation absolutely free.

## Presentation Transcript

1. Electrical Energy and Capacitance • Chapter 16

2. Review Review • What is potential energy? – Energy at rest or energy due to position

3. What is a conservative force? – A conservative force is a force that does work in such a way that the work done depends only upon the initial and final positions.

4. Frictional force is dissipative. • The Coulomb force is conservative.

5. What is meant by the conservation of energy? – Energy cannot be created or destroyed, only transformed.

6. Gravitational force is conservative. • Gravitational potential energy depends upon mass, gravity, and position.

7. Introduction Introduction • New concepts – Electric potential energy – Electric potential – Voltage between two points – Electric potential difference – Capacitance

8. Work Done on a Charge • Electrostatic force is conservative – Work may be done by a conservative force

9. The equation for work done on a charge: Since F = qE W = (F) d = (qE) d

10. Electric Potential • Electric potential (V) is a scalar quantity – It is defined as the energy per unit charge (J/C) at a given point – The unit for electric potential is the volt (1 volt = 1 Joule/Coulomb)

11. Potential Difference • Definition of the potential difference (  V) between points A and B   V = V B - V A =  PE/q = -E . d The units are Volts or Joules /Coulomb

12. Useful relationships: 1 V = 1 J/C 1 N/C = 1 V/m

13. Electrical PE and KE • A positive charge gains electrical PE when it moves against the field. • A positive charge gains KE when it moves in the same direction as the field. 166, 16.2

14. A negative charge gains electrical PE when it moves in the same direction as the field. • A negative charge gains KE when it moves against the field. 167

15. Potential Difference And Electric Potential • A 12-volt automobile battery – Maintains a potential difference across its terminals • The positive terminal is at a higher potential. (+ 12 volts) • The negative terminal is at a lower potential (0 volts) and is connected to the car frame. • Charge moves around the circuit. 16.3

16. Zero Potential • A point of zero potential is usually defined by grounding some point in the circuit.

17. A point at infinity may be considered to be at zero potential in relation to a positive charge.

18. Electric Potential at a Point • The electric potential, at a particular location, created by a point charge can be found by using: V = k e (q/r)

19. Electric Potential • The electric potential depends upon only two things:

20. The electric potential depends upon only two things: – Charge – Location

21. The electric potential exists at every point surrounding a given charge. – A second charge is not needed.

22. Electric potential is a scalar quantity. – If there are two or more charges, the potentials add algebraically at a given point. – no vectors to worry about

23. Electric PE • Electric potential energy is the energy that a charge has due to its position in the electric field produced by another charge. It is measured in Joules. 133

24. The electric potential (PE) energy of a pair of charges can be found by using: PE = q 2 V 1 = q 2 (k e q 1 /r) PE = k e (q 1 q 2 /r) 16.7

25. The electric potential energy is positive if the charges are identical and negative if they are different.

26. Equipotentials • No work is required to move a charge between two points that are at the same potential. W = -q(V B – V A )

27. All points on the surface of a charged conductor which is in electrostatic equilibrium are at the same potential.

28. The electric potential is constant everywhere on the surface of a charged conductor in equilibrium.

29. The electric potential is constant everywhere inside a conductor and equal to its value at the surface.

30. The Electron-Volt • The electron-volt is the energy of an electron after it has been accelerated across a potential difference of 1 volt. – It is a very small unit of energy. 1 eV = 1.6 x 10 -19 J

31. Equipotential Surfaces • What is an equipotential surface? – An equipotential surface is one where all points are at the same potential. 169

32. No work is required to move a charge at a constant speed along an equipotential surface. 134

33. The electric field at every point of an equipotential surface is perpendicular to the surface. 16.7

34. Equipotential Lines • Equipotential lines – Two - dimensional views – Equipotential lines are always perpendicular to electric field lines. 16.10, 170, 16.6

35. Applications • Electrostatic precipitator – Power company smokestacks • Electrostatic air cleaners – Furnace filters – Smoke eaters at party halls

36. How does a copy machine work? – Corotron – Selenium drum – Heated pressure rollers 165

37. How does laser printer work? 16.12

38. QUESTIONS 1, 4 – 7, 11 Pg. 564

39. Capacitors • What is a capacitor? – A capacitor is made up of two parallel metal plates with a surface area (A) separated by a dielectric with thickness (d) 171

40. How it works: – Each plate is connected to one side of a battery – Charge flows until the plates have the same potential difference as the battery • One is positive while the other is negative (+ Q and –Q) 68

41. The Definition Of Capacitance • What is capacitance ? – Capacitance is the ratio of the magnitude of the charge on either conducting surface to the potential difference between the two conducting surfaces. C = Q/  V Therefore: Q =  V . C

42. What is the unit of capacitance ? – Farad (F) • Named after Michael Faraday • 1 farad = 1 Coulomb/volt • Microfarads (  F) and picofarads (pF) are more commonly used

43. Capacitance Applications • Tuning stations on radio and television receivers • Storing charge in electronic flash units • Computer keyboards

44. The Parallel Plate Capacitor • Factors affecting capacitance: – Area (A) – Separation (d) – Permittivity of free space (  o ) C =  o A/d (in air) Also: k e = 1/4  o

45. o = 8.85 x 10 -12 C 2 /N . m 2

46. How things work: – Flash attachment

47. How things work: – Computer keyboard 173

48. Circuit Symbols • Symbols for circuit elements – Battery – Capacitor – Resistor – Wires

49. Types of Electrical Circuits • Complete Circuits – Series – Parallel – Combination 7, 16.15

50. Capacitors in Parallel • In Parallel: – The potential differences across each of the capacitors is equal to the battery voltage 16.17

51. In Parallel: – The equivalent capacitance of the circuit is equal to the sum of the individual capacitors C eq = C 1 + C 2 + …

52. In Parallel: – The total charge stored by the capacitors is: Q = Q 1 + Q 2 + …

53. In Parallel: – The equivalent capacitance of a parallel combination is always greater than any of the individual capacitances

54. Capacitors in Series • In Series: – The potential differences across each of the capacitors add up to the battery voltage 16.19

55. In Series: – The equivalent capacitance of the circuit can be found by using: 1/C eq = 1/C 1 +1/C 2 + … There is a Shortcut!

56. The equivalent capacitance of two capacitors in series can be found by using:

57. In Series: – All of the capacitors must have the same charge: Q T = Q 1 = Q 2 = …

58. In Series: – The equivalent capacitance of a series combination is always less than any individual capacitance in the combination 187, 188

59. Combinations Of Capacitors • Some circuits involve combinations of series and parallel capacitors

60. Energy Stored In A Charged Capacitor • A capacitor stores electrical energy in its field – Discharges can be dangerous if high voltages are present.

61. Work is done in charging a capacitor W = 0.5 Q  V 50

62. The energy stored in a capacitor is given by: E = 0.5 C  V 2

63. Electrical breakdown limits the amount of energy that can be stored in a capacitor

64. Medical Applications • Defibrillators – Paddles – Capacitors charge to a high voltage – Charging takes time

65. Capacitors With Dielectrics • A dielectric is an insulating material – Examples of dielectrics • Rubber • Glass • Plastic • Waxed paper

66. Dielectrics can increase capacitance – The dielectric constant (  ) • See Table 16.1 (Pg. 557) – Air has a dielectric constant of 1 C =  o A/d 172, 16.23

67. Types of Capacitors • Tubular • High voltage • Electrolytic (polarized) • Variable

68. Application: DNA And Forensic Science • DNA fragments are separated by mass and by charge

69. QUESTIONS 8, 9, 10, 12 - 14 Pg. 564