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# Ch19 Electric Potential Energy and Electric Potential

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### Ch19 Electric Potential Energy and Electric Potential

1. 1. Chapter 19 Electric Potential Energy and Electric Potential
2. 2. AP Learning Objectives ELECTRICITY AND MAGNETISM  Electrostatics • Electric field and electric potential (including point charges) • Students should understand the concept of electric field, so they can: • Define it in terms of the force on a test charge. • Describe and calculate the electric field of a single point charge. • Calculate the magnitude and direction of the electric field produced by two or more point charges. • Calculate the magnitude and direction of the force on a positive or negative charge placed in a specified field. • Interpret an electric field diagram. • Analyze the motion of a particle of specified charge and mass in a uniform electric field.
3. 3. AP Learning Objectives • Students should understand the concept of electric potential, so they can: • Determine the electric potential in the vicinity of one or more point charges. • Calculate the electrical work done on a charge or use conservation of energy to determine the speed of a charge that moves through a specified potential difference. • Determine the direction and approximate magnitude of the electric field at various positions given a sketch of equipotentials. • Calculate the potential difference between two points in a uniform electric field, and state which point is at the higher potential. • Calculate how much work is required to move a test charge from one location to another in the field of fixed point charges. • Calculate the electrostatic potential energy of a system of two or more point charges, and calculate how much work is required to establish the charge system.
4. 4. Table of Contents 1. Potential Energy 2. The Electric Potential Difference 3. The Electric Potential Difference Created by Point Charges 4. Equipotential Surfaces and Their Relation to the electric Field 5. Capacitors and Dielectrics 6. Biomedical Applications of Electric Potential Differences (AP?)
5. 5. Chapter 19: Electric Potential Energy and Electric Potential Section 1: Potential Energy
6. 6.  From Gravity • Energy based on position • Change in position • Change in Energy • Work ( )2 2 1 vmhmg ∆=∆ Potential Energy BAAB mghmghW −=
7. 7. Electrical Potential Energy  Same Effect for Electric Force  Energy present based on position • Change in position • Change in Energy • Remember, unless otherwise stated, test charge is positive FdUE = 2 21 4 1 r qq F o E πε = r r qq U o E       = 2 21 4 1 πε       = r qq U o E 21 4 1 πε
8. 8. 19.1.1. Two electrons are separated by a distance R. If the distance between the charges is increased to 2R, what happens to the total electric potential energy of the system? a) The total electric potential energy of the system would increase to four times its initial value. b) The total electric potential energy of the system would increase to two times its initial value. c) The total electric potential energy of the system would remain the same. d) The total electric potential energy of the system would decrease to one half its initial value. e) The total electric potential energy of the system would decrease to one fourth its initial value.
9. 9. 19.1.2. The electric potential energy for two positive charges of magnitude q and separated by a distance r is EPE1. What will the electric potential energy be if one of the charges is completely removed and replaced by a negative charge of the same magnitude? a) U2 = 2 × U1 b) U2 = U1 c) U2 = −U1 d) U2 = −2 × U1 e) There is no way to determine this without knowing the value of q.
10. 10. Chapter 19: Electric Potential Energy and Electric Potential Section 2: The Electric Potential Difference
11. 11. Electric Potential  Electric Potential is hard to understand, but easy to measure.  The potential energy per unit charge  Related to electric potential energy and the electric field  Commonly called “Voltage”  Measured in volts (1V = 1 J/C)
12. 12. The electric potential at a given point is the electric potential energy of a small test charge divided by the charge itself: SI Unit of Electric Potential: joule/coulomb = volt (V) o AB o A o B AB q W qq VV − =−=− UU o AB o q W q V − = ∆ =∆ U DEFINITION OF ELECTRIC POTENTIAL o E q U V =
13. 13. Example 1 Work, Potential Energy, and Electric Potential The work done by the electric force as the test charge (+2.0x10-6 C) moves from A to B is +5.0x10-5 J. Find the difference in EPE between these points. Determine the potential difference between these points. BAABW UU −= o AB o A o B q W qq V − =−=∆ UU ABW−= C102.0 J100.5 6- 5 × ×− =∆ − V J100.5 5− ×−= (a) (b) V25−=
14. 14. Conceptual Example 2 The Accelerations of Positive and Negative Charges A positive test charge is released from A and accelerates towards B. Upon reaching B, the test charge continues to accelerate toward C. Assuming that only motion along the line is possible, what will a negative test charge do when released from rest at B? Negative charge will accelerate towards A
15. 15. A positive charge accelerates from a region of higher electric potential toward a region of lower electric potential. A negative charge accelerates from a region of lower potential toward a region of higher potential. Explanation
16. 16. We now include electric potential energy as part of the total energy that an object can have: EUkxmghImvE ++++= 2 2 12 2 12 2 1 ω One electron volt is the magnitude of the amount by which the potential energy of an electron changes when the electron moves through a potential difference of one volt. V1060.1eV1 19− ×= Energy Conservation
17. 17. Example 4 The Conservation of Energy A particle has a mass of 1.8x10-5 kg and a charge of +3.0x10-5 C. It is released from point A and accelerates horizontally until it reaches point B. The only force acting on the particle is the electric force, and the electric potential at A is 25V greater than at B. (a) What is the speed of the particle at point B? (b) If the same particle had a negative charge and were released from point B, what would be its speed at A? AABB UmvUmv +=+ 2 2 12 2 1 BAB UUmv −=2 2 1 ( )BAoB VVqmv −=2 2 1 qVU = ( )( ) ( )kg108.1V25C100.32 55 −− ××=Bv ( ) mVVqv BAoB −= 2 sm1.9=Bv Part b) same speed, opposite direction
18. 18. 19.2.1. Which one of the following statements best explains why it is possible to define an electrostatic potential in a region of space that contains an electrostatic field? a) The work required to bring two charges together is independent of the path taken. b) A positive charge will gain kinetic energy as it approaches a negative charge. c) Like charges repel one another and unlike charges attract one another. d) Work must be done to bring two positive charges closer together. e) A negative charge will gain kinetic energy as it moves away from another negative charge.
19. 19. 19.2.2. Four point charges are individually brought from infinity and placed at the corners of a square as shown in the figure. Each charge has the identical value +Q. The length of the diagonal of the square is 2a. What is the electric potential at P, the center of the square? a) b) c) zero volts d) e) a kQ 4 a kQ a kQ2 a kQ4
20. 20. Chapter 19: Electric Potential Energy and Electric Potential Section 3: The Electric Potential Difference Created by Point Charges
21. 21. Difference in Potential  What is the potential difference as a particle moves in an Electric Field • due to the electric force as the point charge moves from A to B  Since the force is a function of distance must use calculus: dr r kqq W B A r r o ∫= 2 ∫= B A r r o r dr kqqW 2
22. 22. B o A o r kqq r kqq −= o AB q W V − =∆ Total Potential of All point charges ∑= i i i r q kV Difference in Potential ∫ −= xx dx 1 2 ∫= B A r r o r dr kqqW 2 WU −=∆ oq U V ∆ =∆ BA r kq r kq −=
23. 23. Example 5 The Potential of a Point Charge Using a zero reference potential at infinity, determine the amount by which a point charge of 4.0x10-8 C alters the electric potential at a spot 1.2m away when the charge is (a) positive and (b) negative. r kq V = (a) (b) V300−=V ( )( ) m2.1 C100.4CmN1099.8 8229 − ×+⋅× =V V300+=V
24. 24. Example 6 The Total Electric Potential At locations A and B, find the total electric potential. ( )( ) ( )( ) m60.0 C100.8CmN1099.8 m20.0 C100.8CmN1099.8 82298229 −− ×−⋅× + ×+⋅× =AV ( )( ) ( )( ) m40.0 C100.8CmN1099.8 m40.0 C100.8CmN1099.8 82298229 −− ×−⋅× + ×+⋅× =BV ∑= i i i r q kV V240+= V0=
25. 25. Conceptual Example 7 Where is the Potential Zero? Two point charges are fixed in place. The positive charge is +2q and the negative charge is –q. On the line that passes through the charges, how many places are there at which the total potential is zero?
26. 26. 19.3.1. Consider the four arrangements of three point charges. Rank the values of the total electric potential at point P in each case in descending order (with the largest first). a) VA > VD > VC > VB b) VC > VB > VD > VA c) VC > VD > VA > VB d) VB > VC > VB > VA e) VD > VB > VA > VC
27. 27. 19.3.2. Two point charges lie along the x axis. One charge, located at the origin, has a magnitude +2q. The other charge of unknown magnitude and sign is located at x = 5 units. If the electric potential at x = 4 units is equal to zero volts, what is the magnitude and sign of the second point charge? a) −q/2 b) −q/4 c) −2q d) +q/2 e) +2q
28. 28. Chapter 19: Electric Potential Energy and Electric Potential Section 4: Equipotential Difference Created by Point Charges
29. 29. r kq V = Equipotential Surfaces  An equipotential surface is a surface on which the electric potential is the same everywhere.  The net electric force does no work on a charge as it moves on an equipotential surface.
30. 30. Electric Field and Equipotential Surfaces  The electric field created by any charge or group of charges is everywhere perpendicular to the associated equipotential surfaces and points in the direction of decreasing potential.
31. 31. Equipotential Surfaces and Their Relation to the Electric Field
32. 32. d V Eavg −= In Parallel Plate Capacitors d
33. 33. Example 9 The Electric Field and Potential Are Related The plates of the capacitor are separated by a distance of 0.032 m, and the potential difference between them is VB-VA=-64V. Between the two equipotential surfaces shown in color, there is a potential difference of -3.0V. Find the spacing between the two colored surfaces. ABd V E −= E V d −= m0.032 V64− = mV100.2 3 ×= mV100.2 V0.3 3 × − −= m105.1 3− ×= dAB
34. 34. 19.4.1. A proton is moved from point B to point A in an electric field as shown. As a result of its movement, its potential increases to V. If three protons are moved from point B to A, how much will the electric potential of the protons increase? a) V/9 b) V/3 c) V d) 3V e) 9V
35. 35. 19.4.2. Which one of the following statements concerning electrostatic situations is false? a) No work is required to move a charge along an equipotential surface. b) If the electric potential with a region of space is zero volts, the electric field within that region must also be zero V/m. c) If a charge is moved along an equipotential surface, there is no component of the force acting along the charges’ path. d) The electric field is always perpendicular to equipotential surfaces. e) The electric field is zero V/m everywhere inside a conductor.
36. 36. 19.4.3. The drawing shows three point charges of equal magnitude, but one is positive (shown in blue) and two are negative (shown in yellow). Some of the equipotential lines surrounding these charges are shown and five are labeled using letters A, B, C, D, and E. At which of the labeled points will an electron have the greatest electric potential energy? a) A b) B c) C d) D e) E
37. 37. 19.4.4. The drawing shows three point charges of equal magnitude, but one is positive (shown in blue) and two are negative (shown in yellow). Some of the equipotential lines surrounding these charges are shown and five are labeled using letters A, B, C, D, and E. What is the direction of the electric field at the location of the letter “D?” a) perpendicular to the equipotential line marked “D” and directed toward the negative charge closest to it b) parallel to the equipotential line marked “D” and directed toward the location of the letter “C” c) perpendicular to the equipotential line marked “D” and directed toward the location of the letter “A” d) toward the negative charge in the lower part of the drawing e) toward the positive charge
38. 38. Chapter 19: Electric Potential Energy and Electric Potential Section 5: Capacitors & Dielectrics
39. 39. Capacitors  A capacitor is a device that can store potential energy  Usually they are build by placing two conductors near each other, without touching  For AP, we will only look at air separating the two plates • We can make capacitors with other insulators separating the two conductors.
40. 40. Capacitors and Dielectrics  A parallel plate capacitor consists of two metal plates, one carrying charge +q and the other carrying charge –q.  It is common to fill the region between the plates with an electrically insulating substance called a dielectric.
41. 41.  The magnitude of the charge in each place of the capacitor is directly proportional to the magnitude of the potential difference between the plates.  The capacitance C is the proportionality constant.  SI Unit of Capacitance: coulomb/volt = farad (F) VQ ∝ THE RELATION BETWEEN CHARGE AND POTENTIAL DIFFERENCE FOR A CAPACITOR V Q C = CVQ =
42. 42. Capacitance  To determine the capacitance, we must look at how easily the charge can flow between the plates  We will assume that air has the same permittivity as a vacuum d A C oε =
43. 43. ENERGY STORAGE IN A CAPACITOR  The energy stored on a capacitor can be expressed in terms of the work done by the battery.  Voltage represents energy per unit charge, • so the work to move a charge element dq from the negative plate to the positive plate is equal to V dq, • where V is the voltage on the capacitor.  The voltage V is proportional to the amount of charge which is already on the capacitor. WdU = dq C q dU = VdqdU =
44. 44. ENERGY STORAGE IN A CAPACITOR  If Q is the amount of charge stored when the whole battery voltage appears across the capacitor, then the stored energy is obtained from the integral:  Since Q=CV, we can rewrite this expression: ∫= Q C dq C q U 0 C Q2 2 1 = 2 2 1 2 1 CVQVUC == ∫= Q dqq C 0 1
45. 45. 19.5.1. An electrical outlet has two vertical slots and a hole into which a three prong plug may be inserted. The maximum potential difference between the two vertical slots is 120 volts. The hole is connected to earth ground. Estimate the maximum electric field that exists between the two vertical slots. a) 240 V/m b) 4800 V/m c) 9200 V/m d) 120 V/m e) 6300 V/m
46. 46. 19.5.2. The plates of an isolated parallel plate capacitor with a capacitance C carry a charge Q. What is the capacitance of the capacitor if the charge is increased to 4Q? a) C/2 b) C/4 c) 4C d) 2C e) C
47. 47. 19.5.3. A parallel plate capacitor with plates of area A and plate separation d is charged so that the potential difference between its plates is V. If the capacitor is then isolated and its plate separation is increased to 2d, what is the potential difference between the plates? a) 4V b) 2V c) V d) 0.5V e) 0.25V
48. 48. 19.5.4. The plates of an isolated parallel plate capacitor with a capacitance C carry a charge Q. The plate separation is d. Initially, the space between the plates contains only air. Then, an isolated metal sheet of thickness 0.5d is inserted between, but not touching, the plates. How does the potential difference between the plates change as a result of inserting the metal sheet? a) The potential difference will decrease. b) The potential difference will not be affected. c) The potential difference will increase. d) The potential difference will be zero volts.
49. 49. 19.5.5. The plates of an isolated parallel plate capacitor with a capacitance C carry a charge Q. The plate separation is d. Initially, the space between the plates contains only air. Then, a Teflon (κ = 2.1) sheet of thickness 0.5d is inserted between, but not touching, the plates. How does the electric field between the plates change as a result of inserting the Teflon sheet? a) The electric field will decrease to approximately one-half its initial value. b) The electric field will not be affected. c) The electric field will increase to approximately twice its initial value. d) The electric field will be zero volts per meter.
50. 50. 19.5.6. The plates of an isolated parallel plate capacitor are separated by a distance d and carry charge of magnitude q. The distance between the plates is then reduced to d/2. How is the energy stored in the capacitor affected by this change? a) The energy increases to twice its initial value. b) The energy increases to four times its initial value. c) The energy is not affected by this change. d) The energy decreases to one fourth of its initial value. e) The energy decreases to one half of its initial value.
51. 51. 19.5.7. A parallel plate capacitor is connected to a battery that maintains a constant potential difference across the plates. Initially, the space between the plates contains only air. Then, a Teflon (κ = 2.1) sheet is inserted between, but not touching, the plates. How does the stored energy of the capacitor change as a result of inserting the Teflon sheet? a) The energy will decrease. b) The energy will not be affected. c) The energy will increase. d) The energy will be zero joules.