Chapter 30. Potential and Field

1. Chapter 30. Potential and Field To understand the production of electricity by solar cells or batteries, we must first address the connection between electric potential and electric field. Chapter Goal: Tounderstand how the electric potential is connected to the electric field.

2. Chapter 30. Potential and Field Topics: • Connecting Potential and Field • Sources of Electric Potential • Finding the Electric Field from the Potential • A Conductor in Electrostatic Equilibrium • Capacitance and Capacitors • The Energy Stored in a Capacitor • Dielectrics

3. Chapter 30. Reading Quizzes

4. What quantity is represented by the symbol ? • Electronic potential • Excitation potential • EMF • Electric stopping power • Exosphericity

5. What quantity is represented by the symbol ? • Electronic potential • Excitation potential • EMF • Electric stopping power • Exosphericity

6. What is the SI unit of capacitance? • Capaciton • Faraday • Hertz • Henry • Exciton

7. What is the SI unit of capacitance? • Capaciton • Faraday • Hertz • Henry • Exciton

8. The electric field • is always perpendicular to an equipotential surface. • is always tangent to an equipotential surface. • always bisects an equipotential surface. • makes an angle to an equipotential surface that depends on the amount of charge.

9. The electric field • is always perpendicular to an equipotential surface. • is always tangent to an equipotential surface. • always bisects an equipotential surface. • makes an angle to an equipotential surface that depends on the amount of charge.

10. This chapter investigated • parallel capacitors • perpendicular capacitors • series capacitors. • Both a and b. • Both a and c.

11. This chapter investigated • parallel capacitors • perpendicular capacitors • series capacitors. • Both a and b. • Both a and c.

12. Chapter 30. Basic Content and Examples

13. Finding the Potential from the Electric Field The potential difference between two points in space is where s is the position along a line from point i to point f. That is, we can find the potential difference between two points if we know the electric field. We can think of an integral as an area under a curve. Thus a graphical interpretation of the equation above is

14. Tactics: Finding the potential from the electric field

15. EXAMPLE 30.2 The potential of a parallel-plate capacitor

16. EXAMPLE 30.2 The potential of a parallel-plate capacitor

17. EXAMPLE 30.2 The potential of a parallel-plate capacitor

18. EXAMPLE 30.2 The potential of a parallel-plate capacitor

19. EXAMPLE 30.2 The potential of a parallel-plate capacitor

22. Batteries and emf The potential difference between the terminals of an ideal battery is In other words, a battery constructed to have an emf of 1.5V creates a 1.5 V potential difference between its positive and negative terminals. The total potential difference of batteries in series is simply the sum of their individual terminal voltages:

23. Finding the Electric Field from the Potential In terms of the potential, the component of the electric field in the s-direction is Now we have reversed Equation 30.3 and have a way to find the electric field from the potential.

24. EXAMPLE 30.4 Finding E from the slope of V QUESTION:

25. EXAMPLE 30.4 Finding E from the slope of V

26. EXAMPLE 30.4 Finding E from the slope of V

27. EXAMPLE 30.4 Finding E from the slope of V

28. EXAMPLE 30.4 Finding E from the slope of V

29. EXAMPLE 30.4 Finding E from the slope of V

31. Kirchhoff’s Loop Law For any path that starts and ends at the same point Stated in words, the sum of all the potential differences encountered while moving around a loop or closed path is zero. This statement is known as Kirchhoff’s loop law.

34. Capacitance and Capacitors The ratio of the charge Q to the potential difference ΔVCis called the capacitance C: Capacitance is a purely geometric property of two electrodes because it depends only on their surface area and spacing. The SI unit of capacitance is the farad: 1 farad = 1 F = 1 C/V. The charge on the capacitor plates is directly proportional to the potential difference between the plates.

35. EXAMPLE 30.6 Charging a capacitor QUESTIONS:

36. EXAMPLE 30.6 Charging a capacitor

37. EXAMPLE 30.6 Charging a capacitor

38. EXAMPLE 30.6 Charging a capacitor

41. Combinations of Capacitors If capacitors C1, C2, C3, … are in parallel, their equivalent capacitance is If capacitors C1, C2, C3, … are in series, their equivalent capacitance is

42. The Energy Stored in a Capacitor • Capacitors are important elements in electric circuits because of their ability to store energy. • The charge on the two plates is ±qand this charge separation establishes a potential difference ΔV = q/Cbetween the two electrodes. • In terms of the capacitor’s potential difference, the potential energy stored in a capacitor is

44. EXAMPLE 30.9 Storing energy in a capacitor QUESTIONS:

45. EXAMPLE 30.9 Storing energy in a capacitor

46. EXAMPLE 30.9 Storing energy in a capacitor

47. The Energy in the Electric Field The energy density of an electric field, such as the one inside a capacitor, is The energy density has units J/m3.

49. Dielectrics • The dielectric constant, like density or specific heat, is a property of a material. • Easily polarized materials have larger dielectric constants than materials not easily polarized. • Vacuum has κ = 1 exactly. • Filling a capacitor with a dielectric increases the capacitance by a factor equal to the dielectric constant.

50. Chapter 30. Summary Slides