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Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17: Electric Forces and Fields.

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1 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17: Electric Forces and Fields

2 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Electric Forces and Fields Chapter 17 Section 1 Electric Charge Section 2 Electric Force Section 3 The Electric Field Table of Contents

3 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 1 Electric Charge Properties of Electric Charge There are two kinds of electric charge. –like charges repel –unlike charges attract Electric charge is conserved. –Positively charged particles are called protons. –Uncharged particles are called neutrons. –Negatively charged particles are called electrons.

4 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 1 Electric Charge Properties of Electric Charge, continued Electric charge is quantized. That is, when an object is charged, its charge is always a multiple of a fundamental unit of charge (e) Charge is measured in coulombs (C). The fundamental unit of charge, e, is the magnitude of the charge of a single electron or proton. e = x 10 –19 C

5 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 1 Electric Charge Electric Charge (q) Summary (**Know This) Electric charge(q) is the physical property of matter that causes it to experience a force when close to other electrically charged matter.physical propertymatterforce Two types, Positive and Negative Like charges repel, unlike ones attract. Positive charge comes from having more protons than electrons; Negative charge comes from having more electrons than protons. Charge is quantized. That is, when an object is charged, its charge is always a multiple of a fundamental unit of charge. The fundamental unit of charge, e, is the magnitude of the charge of a single electron or proton e = x 10 –19 C A proton has a charge of +e, while an electron has a charge of -e. Unit: CoulombSymbol is q Equation: q=F/E F=Electric Force (N) E=Electric Field Strength(N/C)

6 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 1 Electric Charge Electric Charge (q) Summary (**Know This) Electric field (E ) - Defined as the electric force per unit charge. –The direction of the field is taken to be the direction of the force it would exert on a positive test charge. UNIT: N/C –Equation: E=F/q –The electric field is radially outward from a positive charge and radially in toward a negative point charge.

7 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 1 Electric Charge Electric Charge (q) Summary (**Know This) Electric Force (F ) - The electric force acting on a point charge q 1 as a result of the presence of a second point charge q 2 is given by Coulomb's Law. Unit: Newtons(N) Equation: Coulombs Law: A point charge is a hypothetical charge located at a single point in space.

8 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 1 Electric Charge Materials are divided into three categories, depending on how easily they will allow charge (e.g. electrons) to flow along them. These are: –conductor is a material in which electrons can move freely. e.g. metals –insulator is a material in which electrons cannot move freely. e.g. wood/plastic –Semi-conductor - not as conductive as metals but considerably more conductive than insulators. i.e. Silicon. Used in electronics to control current flow.

9 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 1 Electric Charge Transfer of Electric Charge -3 ways Friction – Used for charging Insulators by rubbing one material with another which allows electrons to transfer. e.g. silk rubs glass leaves glass positive. electrons go from glass to silk. e.g. fur rubs a PVC rod and leaves the rod negative. Electrons go from fur to PVC.

10 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 1 Electric Charge Conduction or contact - useful for charging Insulators or conductors. –A charged object touches the other object resulting in: Some charge will be transferred between the first object and the second object. The second object will be charged with the same sign as the first object.

11 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 1 Electric Charge Induction- Also useful for charging metals and other conductors. –A charged object is used, but this time it is only brought close to the conductor, and does not touch it. –If the conductor is connected to ground electrons will either flow on to it or away from it. –When the ground connection is removed, the conductor will have a charge opposite in sign to that of the charged object.

12 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 1 Electric Charge Transfer of Electric Charge, continued A surface charge can be induced on insulators by polarization. With polarization, the charges within individual molecules are realigned such that the molecule has a slight charge separation.

13 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Coulombs Law Two charges near one another exert a force on one another called the electric force. Coulombs law states that the electric force is propor- tional to the magnitude of each charge and inversely proportional to the square of the distance between them. Section 2 Electric Force

14 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Coulombs Law, continued The resultant force on a charge is the vector sum of the individual forces on that charge. Adding forces this way is an example of the principle of superposition. When a body is in equilibrium, the net external force acting on that body is zero. Section 2 Electric Force

15 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Sample Problem The Superposition Principle Consider three point charges at the corners of a triangle, as shown at right, where q 1 = –9 C, q 2 = – –9 C, and q 3 = –9 C. Find the magnitude and direction of the resultant force on q 3. Section 2 Electric Force

16 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 2 Electric Force Sample Problem, continued The Superposition Principle 1. Define the problem, and identify the known variables. Given: q 1 = –9 Cr 2,1 = 3.00 m q 2 = – –9 Cr 3,2 = 4.00 m q 3 = –9 Cr 3,1 = 5.00 m = 37.0º Unknown:F 3,tot = ? Diagram:

17 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 2 Electric Force Sample Problem, continued The Superposition Principle Tip: According to the superposition principle, the resultant force on the charge q 3 is the vector sum of the forces exerted by q 1 and q 2 on q 3. First, find the force exerted on q 3 by each, and then add these two forces together vectorially to get the resultant force on q Determine the direction of the forces by analyzing the charges. The force F 3,1 is repulsive because q 1 and q 3 have the same sign. The force F 3,2 is attractive because q 2 and q 3 have opposite signs.

18 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 2 Electric Force Sample Problem, continued The Superposition Principle 3. Calculate the magnitudes of the forces with Coulombs law.

19 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 2 Electric Force Sample Problem, continued The Superposition Principle 4. Find the x and y components of each force. At this point, the direction each component must be taken into account. F 3,1 : F x = (F 3,1 )(cos 37.0º) = ( –8 N)(cos 37.0º) F x = –9 N F y = (F 3,1 )(sin 37.0º) = ( –8 N)(sin 37.0º) F y = –9 N F 3,2 :F x = –F 3,2 = – –9 N F y = 0 N

20 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 2 Electric Force Sample Problem, continued The Superposition Principle 5. Calculate the magnitude of the total force acting in both directions. F x,tot = –9 N – –9 N = –9 N F y,tot = –9 N + 0 N = –9 N

21 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 2 Electric Force Sample Problem, continued The Superposition Principle 6. Use the Pythagorean theorem to find the magni- tude of the resultant force.

22 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 2 Electric Force Sample Problem, continued The Superposition Principle 7. Use a suitable trigonometric function to find the direction of the resultant force. In this case, you can use the inverse tangent function:

23 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Coulombs Law, continued The Coulomb force is a field force. A field force is a force that is exerted by one object on another even though there is no physical contact between the two objects. Chapter 17 Section 2 Electric Force

24 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 3 The Electric Field Electric Field Strength An electric field is a region where an electric force on a test charge can be detected. The SI units of the electric field, E, are newtons per coulomb (N/C). The direction of the electric field vector, E, is in the direction of the electric force that would be exerted on a small positive test charge.

25 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 3 The Electric Field Electric Field Strength, continued Electric field strength depends on charge and distance. An electric field exists in the region around a charged object. Electric Field Strength Due to a Point Charge

26 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 3 The Electric Field Sample Problem Electric Field Strength A charge q 1 = µC is at the origin, and a charge q 2 = –5.00 µC is on the x- axis m from the origin, as shown at right. Find the electric field strength at point P,which is on the y-axis m from the origin.

27 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Sample Problem, continued Electric Field Strength 1. Define the problem, and identify the known variables. Given: q 1 = µC = –6 Cr 1 = m q 2 = –5.00 µC = – –6 Cr 2 = m = 53.1º Unknown: E at P (y = m) Tip: Apply the principle of superposition. You must first calculate the electric field produced by each charge individually at point P and then add these fields together as vectors. Section 3 The Electric Field

28 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Sample Problem, continued Electric Field Strength 2. Calculate the electric field strength produced by each charge. Because we are finding the magnitude of the electric field, we can neglect the sign of each charge. Section 3 The Electric Field

29 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Sample Problem, continued Electric Field Strength 3. Analyze the signs of the charges. The field vector E 1 at P due to q 1 is directed vertically upward, as shown in the figure, because q 1 is positive. Likewise, the field vector E 2 at P due to q 2 is directed toward q 2 because q 2 is negative. Section 3 The Electric Field

30 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Sample Problem, continued Electric Field Strength 4. Find the x and y components of each electric field vector. For E 1 : E x,1 = 0 N/C E y,1 = N/C For E 2 : E x,2 = ( N/C)(cos 53.1º) = N/C E y,1 = ( N/C)(sin 53.1º)= – N/C Section 3 The Electric Field

31 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Sample Problem, continued Electric Field Strength 5. Calculate the total electric field strength in both directions. E x,tot = E x,1 + E x,2 = 0 N/C N/C = N/C E y,tot = E y,1 + E y,2 = N/C – N/C = N/C Section 3 The Electric Field

32 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Sample Problem, continued Electric Field Strength 6. Use the Pythagorean theorem to find the magnitude of the resultant electric field strength vector. Section 3 The Electric Field

33 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Sample Problem, continued Electric Field Strength 7. Use a suitable trigonometric function to find the direction of the resultant electric field strength vector. In this case, you can use the inverse tangent function: Section 3 The Electric Field

34 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Sample Problem, continued Electric Field Strength 8. Evaluate your answer. The electric field at point P is pointing away from the charge q 1, as expected, because q 1 is a positive charge and is larger than the negative charge q 2. Section 3 The Electric Field

35 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 3 The Electric Field Electric Field Lines The number of electric field lines is proportional to the electric field strength. Electric field lines are tangent to the electric field vector at any point.

36 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 3 The Electric Field Conductors in Electrostatic Equilibrium The electric field is zero everywhere inside the conductor. Any excess charge on an isolated conductor resides entirely on the conductors outer surface. The electric field just outside a charged conductor is perpendicular to the conductors surface. On an irregularly shaped conductor, charge tends to accumulate where the radius of curvature of the surface is smallest, that is, at sharp points.

37 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice 1. In which way is the electric force similar to the gravitational force? A. Electric force is proportional to the mass of the object. B. Electric force is similar in strength to gravitational force. C. Electric force is both attractive and repulsive. D. Electric force decreases in strength as the distance between the charges increases. Standardized Test Prep Chapter 17

38 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 1. In which way is the electric force similar to the gravitational force? A. Electric force is proportional to the mass of the object. B. Electric force is similar in strength to gravitational force. C. Electric force is both attractive and repulsive. D. Electric force decreases in strength as the distance between the charges increases. Standardized Test Prep Chapter 17

39 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 2. What must the charges be for A and B in the figure so that they produce the electric field lines shown? F. A and B must both be positive. G. A and B must both be negative. H. A must be negative, and B must be positive. J. A must be positive, and B must be negative. Standardized Test Prep Chapter 17

40 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 2. What must the charges be for A and B in the figure so that they produce the electric field lines shown? F. A and B must both be positive. G. A and B must both be negative. H. A must be negative, and B must be positive. J. A must be positive, and B must be negative. Standardized Test Prep Chapter 17

41 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 3. Which activity does not produce the same results as the other three? A. sliding over a plastic-covered automobile seat B. walking across a woolen carpet C. scraping food from a metal bowl with a metal spoon D. brushing dry hair with a plastic comb Standardized Test Prep Chapter 17

42 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 3. Which activity does not produce the same results as the other three? A. sliding over a plastic-covered automobile seat B. walking across a woolen carpet C. scraping food from a metal bowl with a metal spoon D. brushing dry hair with a plastic comb Standardized Test Prep Chapter 17

43 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 4. By how much does the electric force between two charges change when the distance between them is doubled? Standardized Test Prep Chapter 17

44 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 4. By how much does the electric force between two charges change when the distance between them is doubled? Standardized Test Prep Chapter 17

45 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued Use the passage below to answer questions 5–6. A negatively charged object is brought close to the surface of a conductor, whose opposite side is then grounded. 5. What is this process of charging called? A. charging by contact B. charging by induction C. charging by conduction D. charging by polarization Standardized Test Prep Chapter 17

46 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued Use the passage below to answer questions 5–6. A negatively charged object is brought close to the surface of a conductor, whose opposite side is then grounded. 5. What is this process of charging called? A. charging by contact B. charging by induction C. charging by conduction D. charging by polarization Standardized Test Prep Chapter 17

47 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued Use the passage below to answer questions 5–6. A negatively charged object is brought close to the surface of a conductor, whose opposite side is then grounded. 6. What kind of charge is left on the conductors surface? F. neutral G. negative H. positive J. both positive and negative Standardized Test Prep Chapter 17

48 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued Use the passage below to answer questions 5–6. A negatively charged object is brought close to the surface of a conductor, whose opposite side is then grounded. 6. What kind of charge is left on the conductors surface? F. neutral G. negative H. positive J. both positive and negative Standardized Test Prep Chapter 17

49 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 7. What is the electric field strength 2.0 m from the center of the conducting sphere? A. 0 N/C B N/C C N/C D N/C Standardized Test Prep Chapter 17 Use the graph below to answer questions 7–10. The graph shows the electric field strength at different distances from the center of the charged conducting sphere of a Van de Graaff generator.

50 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 7. What is the electric field strength 2.0 m from the center of the conducting sphere? A. 0 N/C B N/C C N/C D N/C Standardized Test Prep Chapter 17 Use the graph below to answer questions 7–10. The graph shows the electric field strength at different distances from the center of the charged conducting sphere of a Van de Graaff generator.

51 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 8. What is the strength of the electric field at the surface of the conducting sphere? F. 0 N/C G N/C H N/C J N/C Standardized Test Prep Chapter 17 Use the graph below to answer questions 7–10. The graph shows the electric field strength at different distances from the center of the charged conducting sphere of a Van de Graaff generator.

52 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 8. What is the strength of the electric field at the surface of the conducting sphere? F. 0 N/C G N/C H N/C J N/C Standardized Test Prep Chapter 17 Use the graph below to answer questions 7–10. The graph shows the electric field strength at different distances from the center of the charged conducting sphere of a Van de Graaff generator.

53 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 9. What is the strength of the electric field inside the conducting sphere? A. 0 N/C B N/C C N/C D N/C Standardized Test Prep Chapter 17 Use the graph below to answer questions 7–10. The graph shows the electric field strength at different distances from the center of the charged conducting sphere of a Van de Graaff generator.

54 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 9. What is the strength of the electric field inside the conducting sphere? A. 0 N/C B N/C C N/C D N/C Standardized Test Prep Chapter 17 Use the graph below to answer questions 7–10. The graph shows the electric field strength at different distances from the center of the charged conducting sphere of a Van de Graaff generator.

55 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 10. What is the radius of the conducting sphere? F. 0.5 m G. 1.0 m H. 1.5 m J. 2.0 m Standardized Test Prep Chapter 17 Use the graph below to answer questions 7–10. The graph shows the electric field strength at different distances from the center of the charged conducting sphere of a Van de Graaff generator.

56 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Multiple Choice, continued 10. What is the radius of the conducting sphere? F. 0.5 m G. 1.0 m H. 1.5 m J. 2.0 m Standardized Test Prep Chapter 17 Use the graph below to answer questions 7–10. The graph shows the electric field strength at different distances from the center of the charged conducting sphere of a Van de Graaff generator.

57 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Short Response 11. Three identical charges (q = +5.0 mC) are along a circle with a radius of 2.0 m at angles of 30°, 150°, and 270°, as shown in the figure.What is the resultant electric field at the center? Standardized Test Prep Chapter 17

58 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Short Response, continued 11. Three identical charges (q = +5.0 mC) are along a circle with a radius of 2.0 m at angles of 30°, 150°, and 270°, as shown in the figure.What is the resultant electric field at the center? Answer: 0.0 N/C Standardized Test Prep Chapter 17

59 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Short Response, continued 12. If a suspended object is attracted to another object that is charged, can you conclude that the suspended object is charged? Briefly explain your answer.

60 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Short Response, continued 12. If a suspended object is attracted to another object that is charged, can you conclude that the suspended object is charged? Briefly explain your answer. Answer: not necessarily; The suspended object might have a charge induced on it, but its overall charge could be neutral.

61 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Short Response, continued 13. One gram of hydrogen contains atoms, each with one electron and one proton. Suppose that 1.00 g of hydrogen is separated into protons and electrons, that the protons are placed at Earths north pole, and that the electrons are placed at Earths south pole. Assuming the radius of Earth to be m, what is the magnitude of the resulting compressional force on Earth?

62 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Short Response, continued 13. One gram of hydrogen contains atoms, each with one electron and one proton. Suppose that 1.00 g of hydrogen is separated into protons and electrons, that the protons are placed at Earths north pole, and that the electrons are placed at Earths south pole. Assuming the radius of Earth to be m, what is the magnitude of the resulting compressional force on Earth? Answer: N

63 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Short Response, continued 14. Air becomes a conductor when the electric field strength exceeds N/C. Determine the maximum amount of charge that can be carried by a metal sphere 2.0 m in radius.

64 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Short Response, continued 14. Air becomes a conductor when the electric field strength exceeds N/C. Determine the maximum amount of charge that can be carried by a metal sphere 2.0 m in radius. Answer: –3 C

65 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Extended Response Use the information below to answer questions 15–18. A proton, which has a mass of –27 kg, accelerates from rest in a uniform electric field of 640 N/C. At some time later, its speed is m/s. 15. What is the magnitude of the acceleration of the proton?

66 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Extended Response, continued Use the information below to answer questions 15–18. A proton, which has a mass of –27 kg, accelerates from rest in a uniform electric field of 640 N/C. At some time later, its speed is m/s. 15. What is the magnitude of the acceleration of the proton? Answer: m/s 2

67 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Extended Response, continued Use the information below to answer questions 15–18. A proton, which has a mass of –27 kg, accelerates from rest in a uniform electric field of 640 N/C. At some time later, its speed is m/s. 17. How long does it take the proton to reach this speed?

68 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Extended Response, continued Use the information below to answer questions 15–18. A proton, which has a mass of –27 kg, accelerates from rest in a uniform electric field of 640 N/C. At some time later, its speed is m/s. 17. How long does it take the proton to reach this speed? Answer: –5 s

69 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Extended Response, continued Use the information below to answer questions 15–18. A proton, which has a mass of –27 kg, accelerates from rest in a uniform electric field of 640 N/C. At some time later, its speed is m/s. 17. How far has it moved in this time interval?

70 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Extended Response, continued Use the information below to answer questions 15–18. A proton, which has a mass of –27 kg, accelerates from rest in a uniform electric field of 640 N/C. At some time later, its speed is m/s. 17. How far has it moved in this time interval? Answer: 12 m

71 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Extended Response, continued Use the information below to answer questions 15–18. A proton, which has a mass of –27 kg, accelerates from rest in a uniform electric field of 640 N/C. At some time later, its speed is m/s. 18. What is its kinetic energy at the later time?

72 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Extended Response, continued Use the information below to answer questions 15–18. A proton, which has a mass of –27 kg, accelerates from rest in a uniform electric field of 640 N/C. At some time later, its speed is m/s. 18. What is its kinetic energy at the later time? Answer: –15 J

73 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Extended Response, continued 19. A student standing on a piece of insulating material places her hand on a Van de Graaff generator. She then turns on the generator. Shortly thereafter, her hairs stand on end. Explain how charge is or is not transferred in this situation, why the student is not shocked, and what causes her hairs to stand up after the generator is started.

74 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Standardized Test Prep Chapter 17 Extended Response, continued 19. (See previous slide for question.) Answer: The charge on the sphere of the Van de Graaff generator is transferred to the student by means of conduction. This charge remains on the student because she is insulated from the ground. As there is no path between the student and the generator and the student and the ground by which charge can escape, the student is not shocked. The accumulation of charges of the same sign on the strands of the students hair causes the strands to repel each other and so stand on end.

75 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 1 Electric Charge Charging By Induction

76 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 1 Electric Charge Transfer of Electric Charge

77 Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Chapter 17 Section 3 The Electric Field Electric Field Lines


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