HP_16_win Electric Forces and Fields

Download Report

Transcript HP_16_win Electric Forces and Fields

How to Use This Presentation
• To View the presentation as a slideshow with effects
select “View” on the menu bar and click on “Slide Show.”
• To advance through the presentation, click the right-arrow
key or the space bar.
• From the resources slide, click on any resource to see a
presentation for that resource.
• From the Chapter menu screen click on any lesson to go
directly to that lesson’s presentation.
• You may exit the slide show at any time by pressing
the Esc key.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter Presentation
Transparencies
Visual Concepts
Sample Problems
Standardized Test Prep
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Electric Forces and Fields
Table of Contents
Section 1 Electric Charge
Section 2 Electric Force
Section 3 The Electric Field
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 1 Electric Charge
Objectives
• Understand the basic properties of electric charge.
• Differentiate between conductors and insulators.
• Distinguish between charging by contact, charging
by induction, and charging by polarization.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 1 Electric Charge
Electric Charge
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
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.
• 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 = 1.602 176 x 10–19 C
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 1 Electric Charge
The Milikan Experiment
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 1 Electric Charge
Milikan’s Oil Drop Experiment
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 1 Electric Charge
Transfer of Electric Charge
• An electrical conductor is a material in which
charges can move freely.
• An electrical insulator is a material in which charges
cannot move freely.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 1 Electric Charge
Transfer of Electric Charge, continued
• Insulators and conductors can be charged by contact.
• Conductors can be charged by induction.
• Induction is a process of charging a conductor by
bringing it near another charged object and
grounding the conductor.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 1 Electric Charge
Charging by Induction
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 2 Electric Force
Objectives
• Calculate electric force using Coulomb’s law.
• Compare electric force with gravitational force.
• Apply the superposition principle to find the resultant
force on a charge and to find the position at which the
net force on a charge is zero.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Section 2 Electric Force
Chapter 16
Coulomb’s Law
• Two charges near one another exert a force on one
another called the electric force.
• Coulomb’s law states that the electric force is proportional to the magnitude of each charge and inversely
proportional to the square of the distance between
them.
qq 
Felectric  kC  1 2 2 
 r 
electric force = Coulomb constant 
 charge 1 charge 2 
2
distance


Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 2 Electric Force
Coulomb’s 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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 2 Electric Force
Superposition Principle
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 2 Electric Force
Sample Problem
The Superposition Principle
Consider three point
charges at the corners of a
triangle, as shown at right,
where q1 = 6.00  10–9 C,
q2 = –2.00  10–9 C, and
q3 = 5.00  10–9 C. Find
the magnitude and
direction of the resultant
force on q3.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 2 Electric Force
Sample Problem, continued
The Superposition Principle
1. Define the problem, and identify the known
variables.
Given:
q1 = +6.00  10–9 C
r2,1 = 3.00 m
q2 = –2.00  10–9 C
r3,2 = 4.00 m
q3 = +5.00  10–9 C
r3,1 = 5.00 m
q = 37.0º
Unknown: F3,tot = ? Diagram:
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 2 Electric Force
Sample Problem, continued
The Superposition Principle
Tip: According to the superposition principle, the resultant
force on the charge q3 is the vector sum of the forces
exerted by q1 and q2 on q3. First, find the force exerted on
q3 by each, and then add these two forces together
vectorially to get the resultant force on q3.
2. Determine the direction of the forces by analyzing
the charges.
The force F3,1 is repulsive because q1 and q3 have
the same sign.
The force F3,2 is attractive because q2 and q3 have
opposite signs.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 2 Electric Force
Sample Problem, continued
The Superposition Principle
3. Calculate the magnitudes of the forces with
Coulomb’s law.


2  5.00  10 –9 C 6.00  10 –9 C


q3q1
N

m
9
F3,1  kC
  8.99  10
 
2
2
2
(r 3,1)
C
 5.00 m 


 


F3,1  1.08  10 –8 N
F3,2


2  5.00  10 –9 C 2.00  10 –9 C

q3 q 2
9 Nm 
 kC
  8.99  10
 
2
2
2
(r 3,2)
C 
4.00m




F3,1  5.62  10 –9 N
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
 


Chapter 16
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.
F3,1: Fx = (F3,1)(cos 37.0º) = (1.08  10–8 N)(cos 37.0º)
Fx = 8.63  10–9 N
Fy = (F3,1)(sin 37.0º) = (1.08  10–8 N)(sin 37.0º)
Fy = 6.50  10–9 N
F3,2: Fx = –F3,2 = –5.62  10–9 N
Fy = 0 N
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 2 Electric Force
Sample Problem, continued
The Superposition Principle
5. Calculate the magnitude of the total force acting
in both directions.
Fx,tot = 8.63  10–9 N – 5.62  10–9 N = 3.01  10–9 N
Fy,tot = 6.50  10–9 N + 0 N = 6.50  10–9 N
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 2 Electric Force
Sample Problem, continued
The Superposition Principle
6. Use the Pythagorean theorem to find the magnitude of the resultant force.
F3,tot  (Fx ,tot )2  (Fy ,tot )2  (3.01 109 N)2  (6.50  109 N)2
F3,tot  7.16  10 –9 N
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
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:
tan  
Fy ,tot
Fx ,tot
6.50  10 –9 N

3.01 10 –9 N
  65.2º
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 2 Electric Force
Coulomb’s 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 menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
Objectives
• Calculate electric field strength.
• Draw and interpret electric field lines.
• Identify the four properties associated with a
conductor in electrostatic equilibrium.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
Electric Fields and Test Charges
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
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
E  kC
q
r2
electric field strength = Coulomb constant 
charge producing the field
Chapter menu
 distance 
2
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
Calculating Net Electric Field
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
Sample Problem
Electric Field Strength
A charge q1 = +7.00 µC is
at the origin, and a charge
q2 = –5.00 µC is on the xaxis 0.300 m from the
origin, as shown at right.
Find the electric field
strength at point P,which is
on the y-axis 0.400 m from
the origin.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
Sample Problem, continued
Electric Field Strength
1. Define the problem, and identify the known
variables.
Given:
q1 = +7.00 µC = 7.00  10–6 C
r1 = 0.400 m
q2 = –5.00 µC = –5.00  10–6 C
r2 = 0.500 m
q = 53.1º
Unknown:
E at P (y = 0.400 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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
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.
–6
q1
9
2
2  7.00  10 C 
5
E1  kC 2  8.99  10 N  m /C 

3.93

10
N/C
2 
r1
 (0.400 m) 
–6
q2
9
2
2  5.00  10 C 
5
E2  kC 2  8.99  10 N  m /C 

1.80

10
N/C
2 
r2
 (0.500 m) 




Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
Sample Problem, continued
Electric Field Strength
3. Analyze the signs of the
charges.
The field vector E1 at P due
to q1 is directed vertically
upward, as shown in the
figure, because q1 is
positive. Likewise, the field
vector E2 at P due to q2 is
directed toward q2 because
q2 is negative.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
Sample Problem, continued
Electric Field Strength
4. Find the x and y components of each electric field
vector.
For E1: Ex,1 = 0 N/C
Ey,1 = 3.93  105 N/C
For E2: Ex,2= (1.80  105 N/C)(cos 53.1º) = 1.08  105 N/C
Ey,1= (1.80  105 N/C)(sin 53.1º)= –1.44  105 N/C
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
Sample Problem, continued
Electric Field Strength
5. Calculate the total electric field strength in both
directions.
Ex,tot = Ex,1 + Ex,2 = 0 N/C + 1.08  105 N/C
= 1.08  105 N/C
Ey,tot = Ey,1 + Ey,2 = 3.93  105 N/C – 1.44  105 N/C
= 2.49  105 N/C
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Section 3 The Electric Field
Chapter 16
Sample Problem, continued
Electric Field Strength
6. Use the Pythagorean theorem to find the
magnitude of the resultant electric field strength
vector.
Etot 
E   E 
Etot 
1.08  10 N/C    2.49  10 N/C 
2
x ,tot
2
y ,tot
5
2
5
2
Etot  2.71 105 N/C
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
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:
tan  
E y ,tot
E x ,tot
2.49  105 N/C

1.08  105 N/C
  66.0
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
Sample Problem, continued
Electric Field Strength
8. Evaluate your answer.
The electric field at point P is pointing away from the
charge q1, as expected, because q1 is a positive
charge and is larger than the negative charge q2.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
Rules for Drawing Electric Field Lines
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
Rules for Sketching Fields Created by Several
Charges
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
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 conductor’s outer surface.
• The electric field just outside a charged conductor is
perpendicular to the conductor’s 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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Multiple Choice, continued
4. By how much does the electric force between two
charges change when the distance between them is
doubled?
F. 4
G. 2
1
H.
2
1
J.
4
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Multiple Choice, continued
4. By how much does the electric force between two
charges change when the distance between them is
doubled?
F. 4
G. 2
1
H.
2
1
J.
4
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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 conductor’s
surface?
F. neutral
G. negative
H. positive
J. both positive and negative
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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 conductor’s
surface?
F. neutral
G. negative
H. positive
J. both positive and negative
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Multiple Choice, continued
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.
7. What is the electric field
strength 2.0 m from the
center of the conducting
sphere?
A. 0 N/C
B. 5.0  102 N/C
C. 5.0  103 N/C
D. 7.2  103 N/C
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Multiple Choice, continued
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.
7. What is the electric field
strength 2.0 m from the
center of the conducting
sphere?
A. 0 N/C
B. 5.0  102 N/C
C. 5.0  103 N/C
D. 7.2  103 N/C
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Multiple Choice, continued
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.
8. What is the strength of
the electric field at the
surface of the
conducting sphere?
F. 0 N/C
G. 1.5  102 N/C
H. 2.0  102 N/C
J. 7.2  103 N/C
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Multiple Choice, continued
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.
8. What is the strength of
the electric field at the
surface of the
conducting sphere?
F. 0 N/C
G. 1.5  102 N/C
H. 2.0  102 N/C
J. 7.2  103 N/C
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Multiple Choice, continued
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.
9. What is the strength of
the electric field inside
the conducting sphere?
A. 0 N/C
B. 1.5  102 N/C
C. 2.0  102 N/C
D. 7.2  103 N/C
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Multiple Choice, continued
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.
9. What is the strength of
the electric field inside
the conducting sphere?
A. 0 N/C
B. 1.5  102 N/C
C. 2.0  102 N/C
D. 7.2  103 N/C
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Multiple Choice, continued
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.
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
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Multiple Choice, continued
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.
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
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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?
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Short Response, continued
13. One gram of hydrogen contains 6.02  1023 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 Earth’s north
pole, and that the electrons are placed at Earth’s
south pole. Assuming the radius of Earth to be 6.38 
106 m, what is the magnitude of the resulting
compressional force on Earth?
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Short Response, continued
13. One gram of hydrogen contains 6.02  1023 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 Earth’s north
pole, and that the electrons are placed at Earth’s
south pole. Assuming the radius of Earth to be 6.38 
106 m, what is the magnitude of the resulting
compressional force on Earth?
Answer: 5.12  105 N
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Short Response, continued
14. Air becomes a conductor when the electric field
strength exceeds 3.0  106 N/C. Determine the
maximum amount of charge that can be carried by a
metal sphere 2.0 m in radius.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Short Response, continued
14. Air becomes a conductor when the electric field
strength exceeds 3.0  106 N/C. Determine the
maximum amount of charge that can be carried by a
metal sphere 2.0 m in radius.
Answer: 1.3  10–3 C
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Extended Response
Use the information
below to answer
questions 15–18.
A proton, which has a
mass of 1.673  10–27 kg,
accelerates from rest in a
uniform electric field of
640 N/C. At some time
later, its speed is 1.2  106
m/s.
15. What is the magnitude
of the acceleration of
the proton?
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Extended Response, continued
Use the information
below to answer
questions 15–18.
A proton, which has a
mass of 1.673  10–27 kg,
accelerates from rest in a
uniform electric field of
640 N/C. At some time
later, its speed is 1.2  106
m/s.
15. What is the magnitude
of the acceleration of
the proton?
Answer: 6.1  1010 m/s2
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Extended Response, continued
Use the information
below to answer
questions 15–18.
A proton, which has a
mass of 1.673  10–27 kg,
accelerates from rest in a
uniform electric field of
640 N/C. At some time
later, its speed is 1.2  106
m/s.
16. How long does it take
the proton to reach this
speed?
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Extended Response, continued
Use the information
below to answer
questions 15–18.
A proton, which has a
mass of 1.673  10–27 kg,
accelerates from rest in a
uniform electric field of
640 N/C. At some time
later, its speed is 1.2  106
m/s.
16. How long does it take
the proton to reach this
speed?
Answer: 2.0  10–5 s
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Extended Response, continued
Use the information
below to answer
questions 15–18.
A proton, which has a
mass of 1.673  10–27 kg,
accelerates from rest in a
uniform electric field of
640 N/C. At some time
later, its speed is 1.2  106
m/s.
17. How far has it moved
in this time interval?
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Extended Response, continued
Use the information
below to answer
questions 15–18.
A proton, which has a
mass of 1.673  10–27 kg,
accelerates from rest in a
uniform electric field of
640 N/C. At some time
later, its speed is 1.2  106
m/s.
17. How far has it moved
in this time interval?
Answer: 12 m
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Extended Response, continued
Use the information
below to answer
questions 15–18.
A proton, which has a
mass of 1.673  10–27 kg,
accelerates from rest in a
uniform electric field of
640 N/C. At some time
later, its speed is 1.2  106
m/s.
18. What is its kinetic
energy at the later
time?
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
Extended Response, continued
Use the information
below to answer
questions 15–18.
A proton, which has a
mass of 1.673  10–27 kg,
accelerates from rest in a
uniform electric field of
640 N/C. At some time
later, its speed is 1.2  106
m/s.
18. What is its kinetic
energy at the later
time?
Answer: 1.2  10–15 J
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Standardized Test Prep
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 student’s hair causes the strands to
repel each other and so stand on end.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 1 Electric Charge
Charging By Induction
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 1 Electric Charge
Transfer of Electric Charge
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 16
Section 3 The Electric Field
Electric Field Lines
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.