Physics: Principles and Problems
Physics: Principles and Problems
9th Edition
Elliott, Haase, Harper, Herzog, Margaret Zorn, Nelson, Schuler, Zitzewitz
ISBN: 9780078458132
Table of contents
Textbook solutions

All Solutions

Page 565: Practice Problems

Exercise 1
Solution 1
Solution 2
Step 1
1 of 4
A force from an electric field exerts on a positive test charge, we have to calculate what is the magnitude of electric field at the location of the charge. It is given that charge is $5cdot10^{-6}$ C and force is equal to $2cdot10^{-4}$ N.
Step 2
2 of 4
To calculate electric field we can use its definition:
$$E=frac{F}{q}$$
Step 3
3 of 4
When we put numbers in we get:
$$E=frac{2cdot10^{-4}}{5cdot10^{-6}}$$
$$boxed{E=40,,rm N/C}$$
Result
4 of 4
$$E=40,,rm N/C$$
Step 1
1 of 2
We are told that the force $F$ exerted on a positive test charge $q = 5 cdot 10^{-6} ~mathrm{C}$ is $F = 2 cdot 10^{-4} ~mathrm{N}$. To find the magnitude of the electric field, let’s remind ourselves that force $F$ acting on a charge $q$ in the electric field $E$ is equal to:

$$
F = q E
$$

Let’s express electric field $E$ from the equation above and solve for it:

$$
begin{align*}
E &= dfrac{F}{q} \
E &= dfrac{ 2 cdot 10^{-4} ~mathrm{N} }{ 5 cdot 10^{-6} ~mathrm{C}}
end{align*}
$$

$$
boxed{E = 40 ~mathrm{dfrac{N}{C}}}
$$

Result
2 of 2
$$
E = 40 ~mathrm{dfrac{N}{C}}
$$
Exercise 2
Solution 1
Solution 2
Step 1
1 of 4
In this problem we have negative charge in electric field. It is given that force on the charge by electric field is $2cdot10^{-8}$ N, and we have to calculate what is the magnitude of the electric field and direction at that location.
Step 2
2 of 4
To find magnitude of the electric field we can use its definition:
$$E=frac{F}{q}$$
When you put the numbers in you have to put negative sign for charge because it is negative.
Step 3
3 of 4
When we put numbers in we get:
$$E=frac{0.06}{-2cdot10^{-8}}$$
$$boxed{E=-3cdot10^{6},,rm N/C}$$
Minus sign means that direction of the field is opposite to the force, because we chose to put direction of the force as positive, hence direction is to the left.
Result
4 of 4
$E=3cdot10^{6},,rm N/C$, direction is to the left.
Step 1
1 of 2
We are told that the force $F$ exerted on a negative charge $q = -2 cdot 10^{-8} ~mathrm{C}$ is $F = 0.06 ~mathrm{N}$.
Note that in problem text it’s stated that charge is negative, but we’re told that charge is $2 cdot 10^{-8} ~mathrm{C}$, from which we concluded that charge is
$q = -2 cdot 10^{-8} ~mathrm{C}$, as stated above.
To find the magnitude of the electric field, let’s remind ourselves that force $F$ acting on a charge $q$ in the electric field $E$ is equal to:

$$
F = q E
$$

Notice that since charge $q$ is negative, electric field $E$ must also be negative since we’re given force $F$ and, as we can see, force $F$ is positive. Knowing that electric field $E$ is negative, we conclude that source of the electric field is negatively charged. Let’s express electric field $E$ from the equation above and solve for it:

$$
begin{align*}
E &= dfrac{F}{q} \
E &= dfrac{ 0.06 ~mathrm{N} }{ -2 cdot 10^{-8} ~mathrm{C}}
end{align*}
$$

$$
boxed{ E = – 3 cdot 10^6 ~mathrm{dfrac{N}{C}} }
$$

We are told that direction of the force is to the right and we concluded that this force is repulsive. In order for this force to be repulsive, electric field must be negative, which means that source of the electric field is negatively charged. Direction of the electric field coming from a negatively charged source is always pointing inward to the source, from which we conclude that direction of the electric field is to the left.

Result
2 of 2
$$
E = – 3 cdot 10^6 ~mathrm{dfrac{N}{C}}
$$

$$
text{Direction of electric field is to the left}
$$

Exercise 3
Solution 1
Solution 2
Step 1
1 of 4
In this problem we have charge in electric field and we have to calculate force on the charge. It is given that charge is $3cdot10^{-7}$ C and magnitude of electric field is 27 N/C.
Step 2
2 of 4
We can calculate force form definition of the electric field:
$$E=frac{F}{q}rightarrow F=Eq$$
Step 3
3 of 4
When we put numbers in we get:
$$F=3cdot10^{-7}cdot27$$
$$boxed{F=8.1cdot10^{-6},,rm N}$$
Result
4 of 4
$$F=8.1cdot10^{-6},,rm N$$
Step 1
1 of 2
We are told that charge $q = 3 cdot 10^{-7} ~mathrm{C}$ is located in an electric field with magnitude $E = 27 ~mathrm{dfrac{N}{C}}$. To find the magnitude of the force $F$ with which electric field acts on charge $q$, let’s remind ourselves that force $F$ acting on a charge $q$ in the electric field $E$ is equal to:

$$
F = q E
$$

Let’s express electric field $E$ from the equation above and solve for it:

$$
begin{align*}
F &= q E \
F &= 3 cdot 10^{-7} ~mathrm{C} cdot 27 ~mathrm{dfrac{N}{C}}
end{align*}
$$

$$
boxed{ F = 8.1 cdot 10^{-6} ~mathrm{N} }
$$

Result
2 of 2
$$
F = 8.1 cdot 10^{-6} ~mathrm{N}
$$
Exercise 4
Solution 1
Solution 2
Step 1
1 of 4
In this problem we have ball in electric field and we have to calculate charge that most be placed on the ball so that its force suspend the force of gravity. It is given that ball weight $2.1cdot 10^{-3}$ N and magnitude of the electric field is $6.5cdot10^{4}$ N/C and it is in downward direction.
Step 2
2 of 4
We can use definition of electric field:
$$E=frac{F}{q}rightarrow q=frac{F}{E}$$
Force that we put in the equation is equal in magnitude but in opposite in direction to he force of the gravity:
$$F=-F_g$$
$$q=frac{-F_g}{E}$$
Step 3
3 of 4
When we put numbers in we get:
$$q=frac{-2.1cdot10^{-3}}{6.5cdot10^{4}}$$
$$boxed{q=-3.23cdot10^{-8},,rm C}$$
Result
4 of 4
$$q=-3.23cdot10^{-8},,rm C$$
Step 1
1 of 2
Weight of the pith ball is $F_g = 2.1 cdot 10^{-3} ~mathrm{N}$ and it, of course, points downward. Pith ball is placed in a downward electric field with magnitude
$E = 6.5 cdot 10^4 ~mathrm{dfrac{N}{C}}$. If we want to suspend the electric force $F_e$ against force of gravity $F_g$, we need to charge the pith ball in such a way that electric force points upward. Since electric field points downward and we know that force $F$ acting on charge $q$ in an electric field $E$ is equal to:

$$
F_e = q E
$$

we conclude that we need to charge the pith ball negatively, so that electric field and electric force are in the opposite direction.
To calculate charge $q$, we’ll express it from the equation above:

$$
begin{align*}
F_e &= q E \
q &= dfrac{F_e}{E} \
&text{Notice that $F_e = – F_g$} \
q &= dfrac{ – F_g }{E} \
q &= dfrac{ – 2.1 cdot 10^{-3} ~mathrm{N}}{ 6.5 cdot 10^4 ~mathrm{dfrac{N}{C}} }
end{align*}
$$

$$
boxed{ q = -3.23 cdot 10^{-8} ~mathrm{C} }
$$

Result
2 of 2
$$
q = – 3.23 cdot 10^{-8} ~mathrm{C}
$$
Exercise 5
Solution 1
Solution 2
Step 1
1 of 4
In this problem you are probing the electric field with two charges. In part textbf{a} it is asked would you measure the same forces at the same place with the two charges and in part textbf{b} would you find the same magnitude of the field? It is given that first test charge is $1cdot10^{-6}$ C and second is $2cdot 10^{-6}$ C.
Step 2
2 of 4
a)

You would not measure the same force for the same place with the two test charges. Because force is given with equation:
$$F=Eq$$
we can see that with different charge you get different force.

Step 3
3 of 4
b)

Yes you would find the same magnitude of the field. Because field magnitude depends only on the position and we did not change the position.

Result
4 of 4
a) No
b) Yes
Step 1
1 of 2
a)

No. The electric force is proportional to the magnitude of the charge.

b)

Yes. The field strength is independent of the magnitude of the charge.

Result
2 of 2
a) No.

b) Yes.

Exercise 6
Solution 1
Solution 2
Step 1
1 of 4
In this problem we have to calculate magnitude of the field. It is given that position is 1.2 m and charge is $4.2cdot10^{-6}$ C.
Step 2
2 of 4
We can use this equation to calculate field

$$E=kfrac{q}{r^2}$$
where $k$ is Coulomb constant.

Step 3
3 of 4
When we put numbers in we get:
$$E=frac{9cdot10^{9}cdot4.2cdot10^{-6}}{1.2^2}$$
$$boxed{E=26250,,rm N/C}$$
Result
4 of 4
$$E=26250,,rm N/C$$
Step 1
1 of 2
We know that magnitude of the electric field $E$ coming from a charge $q$ at a distance $r$ from the source of the electric field is given as:

$$
E = dfrac{kq}{r^2}
$$

where $k = 9 cdot 10^9 ~mathrm{dfrac{N m^2}{C^2}}$ is Coulomb constant.

To calculate the magnitude of the electric field coming from charge
$q = 4.2 cdot 10^{-6} ~mathrm{C}$ at a distance $r = 1.2 ~mathrm{m}$ from it, we will plug in the given data into the equation above:

$$
begin{align*}
E &= dfrac{kq}{r^2} \
E &= dfrac{ 9 cdot 10^9 ~mathrm{dfrac{N m^2}{C^2}} cdot4.2 cdot 10^{-6} ~mathrm{C} }{ (1.2 ~mathrm{m})^2 }
end{align*}
$$

$$
boxed{E = 26250 ~mathrm{dfrac{N}{C}}}
$$

Result
2 of 2
$$
E = 26250 ~mathrm{dfrac{N}{C}}
$$
Exercise 7
Solution 1
Solution 2
Step 1
1 of 4
In this problem we have to calculate magnitude of the electric field where distance is twice as far from the previous problem. In previous problem is given that distance is 1.2 m and charge is $4.2cdot10^{-6},,rm C$.
Step 2
2 of 4
We can use this equation to calculate electric field:
$$E=kfrac{q}{r^2}$$
where $k$ is Coulomb constant.
Step 3
3 of 4
When we put numbers in we get that:
$$E=frac{9cdot10^9cdot4.2cdot10^{-6}}{2.4^2}$$
$$boxed{E=6562.5,,rm N/C}$$
Result
4 of 4
$$E=6562.5,,rm N/C$$
Step 1
1 of 2
We know that magnitude of the electric field $E$ coming from a charge $q$ at a distance $r$ from the source of the electric field is given as:

$$
E = dfrac{kq}{r^2}
$$

where $k = 9 cdot 10^9 ~mathrm{dfrac{N m^2}{C^2}}$ is Coulomb constant.

To calculate the magnitude of the electric field coming from charge
$q = 4.2 cdot 10^{-6} ~mathrm{C}$ at a distance $r = 2 cdot 1.2 ~mathrm{m} = 2.4 ~mathrm{m}$ from it, we will plug in the given data into the equation above:

$$
begin{align*}
E &= dfrac{kq}{r^2} \
E &= dfrac{ 9 cdot 10^9 ~mathrm{dfrac{N m^2}{C^2}} cdot4.2 cdot 10^{-6} ~mathrm{C} }{ (2.4 ~mathrm{m})^2 }
end{align*}
$$

$$
boxed{E = 6562.5 ~mathrm{dfrac{N}{C}}}
$$

Note that since magnitude of the electric field is inversely proportional to the square of the distance $r$ to the source charge $q$, we expected that magnitude of the electric field will be reduced by a factor of 4 if distance from the source charge was doubled, which is precisely what we calculated.

Result
2 of 2
$$
E = 6562.5 ~mathrm{dfrac{N}{C}}
$$
Exercise 8
Solution 1
Solution 2
Step 1
1 of 4
In this problem we have to calculate electric field. It is given that position is 1.6 m east and charge is $7.2cdot10^{-6},,rm$ C.
Step 2
2 of 4
We can calculate electric field with equation:
$$E=kfrac{q}{r^2}$$
where $k$ is Coulomb constant.
Step 3
3 of 4
When we put numbers in we get:
$$E=frac{9cdot10^9cdot7.2cdot10^{-6}}{1.6^2}$$
$$boxed{25312.5,,rm N/C}$$
Result
4 of 4
$$E=25312.5,,rm N/C$$
Step 1
1 of 2
We know that magnitude of the electric field $E$ coming from a charge $q$ at a distance $r$ from the source of the electric field is given as:

$$
E = dfrac{kq}{r^2}
$$

where $k = 9 cdot 10^9 ~mathrm{dfrac{N m^2}{C^2}}$ is Coulomb constant.

To calculate the magnitude of the electric field coming from charge
$q = 7.2 cdot 10^{-6} ~mathrm{C}$ at a distance $r = 1.6 ~mathrm{m}$ from it, we will plug in the given data into the equation above:

$$
begin{align*}
E &= dfrac{kq}{r^2} \
E &= dfrac{ 9 cdot 10^9 ~mathrm{dfrac{N m^2}{C^2}} cdot 7.2 cdot 10^{-6} ~mathrm{C} }{ (1.6 ~mathrm{m})^2 }
end{align*}
$$

$$
boxed{E = 25312.5 ~mathrm{dfrac{N}{C}}}
$$

Note that magnitude of the electric field doesn’t depend on the direction to in which we measure electric field, which means that when we’re told to calculate the electric field at a point east of the source of the electric field, it gives us an information about direction of the electric field, but not its magnitude. In this case, since source charge is positive, electric field points to the east.

Result
2 of 2
$$
E = 25312.5 ~mathrm{dfrac{N}{C}}
$$

$$
text{Electric field points to the east.}
$$

Exercise 9
Solution 1
Solution 2
Step 1
1 of 4
In this problem we have to calculate the charge in the sphere that is placed in electric field. It is given that distance is 0.25 m and magnitude of the electric field 450 N/C toward the sphere.
Step 2
2 of 4
We can use equation for electric field:
$$E=kfrac{q}{r^2}rightarrow q=frac{Er^2}{k}$$
where $k$ is Coulomb constant. And because electric field is toward the sphere it means that it has negative sign.
Step 3
3 of 4
When we put numbers in we get:
$$q=frac{-450cdot0.25^2}{9cdot10^{9}}$$
$$boxed{q=-3.125cdot10^{-9},,rm C}$$
Result
4 of 4
$$q=-3.125cdot10^{-9},,rm C$$
Step 1
1 of 2
We know that magnitude of the electric field $E$ coming from a charge $q$ at a distance $r$ from the source of the electric field is given as:

$$
E = dfrac{kq}{r^2}
$$

where $k = 9 cdot 10^9 ~mathrm{dfrac{N m^2}{C^2}}$ is Coulomb constant.

To calculate charge on the sphere for which magnitude of the electric field is $E = 450 ~mathrm{dfrac{N}{C}}$ at a distance $r = 0.25 ~mathrm{m}$ from it, we’ll plug in the given data into the equation above and express charge $q$ from it:

$$
begin{align*}
E &= dfrac{kq}{r^2} \
&tag{multiply by $r^2$} \
Er^2 &= kq\
&tag{divide by $q$}\
q &= dfrac{E r^2}{k} \
q &= dfrac{ 450 ~mathrm{dfrac{N}{C}} cdot (0.25 ~mathrm{m})^2 }{ 9 cdot 10^9 ~mathrm{dfrac{N m^2}{C^2}} } \
q &= 3.125 cdot 10^{-9 } ~mathrm{C}
end{align*}
$$

We’ve calculated the magnitude of the charge on the sphere, but notice that we’re told that electric field points to the sphere, which means that sphere is negatively charged. We thus conclude that charge on the sphere is:

$$
boxed{ q = – 3.125 cdot 10^{-9 } ~mathrm{C} }
$$

Result
2 of 2
$$
q = – 3.125 cdot 10^{-9 } ~mathrm{C}
$$
Exercise 10
Solution 1
Solution 2
Step 1
1 of 4
We have to calculate the distance from point charge to the test charge to measure a field of 360 N/C. It is also given that that point charge is $2.4cdot10^{-6}$ C.
Step 2
2 of 4
We can use equation for electric field:
$$E=kfrac{q}{r^2}rightarrow r=sqrt{frac{kq}{E}}$$
where $k$ is Coulomb constant.
Step 3
3 of 4
When we out numbers in we get:
$$r=sqrt{frac{9cdot10^{9}cdot2.4cdot10^{-6}}{360}}$$
$$boxed{r=7.75,,rm m}$$
Result
4 of 4
$$r=7.75,,rm m$$
Step 1
1 of 2
We know that magnitude of the electric field $E$ coming from a charge $q$ at a distance $r$ from the source of the electric field is given as:

$$
E = dfrac{kq}{r^2}
$$

where $k = 9 cdot 10^9 ~mathrm{dfrac{N m^2}{C^2}}$ is Coulomb constant.

To calculate distance $r$ where test charge must be placed in order for magnitude of the electric field, coming from charge $q = 2.4 cdot 10^{-6} ~mathrm{C}$ to be $E = 360 ~mathrm{dfrac{N}{C}}$, we’ll use the equation above and express distance $r$ from it:

$$
begin{align*}
E &= dfrac{kq}{r^2} \
&tag{multiply by $r^2$} \
Er^2 &= kq\
&tag{divide by $E$}\
r^2 &= dfrac{kq}{E} \
tag{ find square root of the equation }\
r &= sqrt{ dfrac{kq}{E} } \
r &= sqrt{ dfrac{ 9 cdot 10^9 ~mathrm{dfrac{N m^2}{C^2}} cdot 2.4 cdot 10^{-6} ~mathrm{C} }{ 360 ~mathrm{dfrac{N}{C}} } } \
r &= sqrt{60 ~mathrm{m^2}}
end{align*}
$$

$$
boxed{ r = 7.746 ~mathrm{m} }
$$

Result
2 of 2
$$
r = 7.746 ~mathrm{m}
$$
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Chapter 1: A Physics Toolkit
Section 1.1: Mathematics and Physics
Section 1.2: Measurement
Section 1.3: Graphing Data
Page 24: Assessment
Page 29: Standardized Test Practice
Chapter 3: Accelerated Motion
Section 3.1: Acceleration
Section 3.2: Motion with Constant Acceleration
Section 3.3: Free Fall
Page 80: Assessment
Page 85: Standardized Test Practice
Chapter 4: Forces in One Dimension
Section 4.1: Force and Motion
Section 4.2: Using Newton’s Laws
Section 4.3: Interaction Forces
Page 112: Assessment
Page 117: Standardized Test Practice
Chapter 5: Forces in Two Dimensions
Section 5.1: Vectors
Section 5.2: Friction
Section 5.3: Force and Motion in Two Dimensions
Page 140: Assessment
Page 145: Standardized Test Practice
Chapter 6: Motion in Two Dimensions
Section 6.1: Projectile Motion
Section 6.2: Circular Motion
Section 6.3: Relative Velocity
Page 164: Assessment
Page 169: Standardized Test Practice
Chapter 7: Gravitation
Section 7.1: Planetary Motion and Gravitation
Section 7.2: Using the Law of Universal Gravitation
Page 190: Assessment
Page 195: Standardized Test Practice
Chapter 8: Rotational Motion
Section 8.1: Describing Rotational Motion
Section 8.2: Rotational Dynamics
Section 8.3: Equilibrium
Page 222: Assessment
Page 227: Standardized Test Practice
Chapter 9: Momentum and Its Conservation
Chapter 10: Energy, Work, and Simple Machines
Section 10.1: Energy and Work
Section 10.2: Machines
Page 278: Assessment
Page 283: Standardized Test Practice
Chapter 11: Energy and Its Conservation
Section 11.1: The Many Forms of Energy
Section 11.2: Conservation of Energy
Page 306: Assessment
Page 311: Standardized Test Practice
Chapter 13: State of Matter
Section 13.1: Properties of Fluids
Section 13.2: Forces Within Liquids
Section 13.3: Fluids at Rest and in Motion
Section 13.4: Solids
Page 368: Assessment
Page 373: Standardized Test Practice
Chapter 14: Vibrations and Waves
Section 14.1: Periodic Motion
Section 14.2: Wave Properties
Section 14.3: Wave Behavior
Page 396: Assessment
Page 401: Section Review
Chapter 15: Sound
Section 15.1: Properties of Detection of Sound
Section 15.2: The Physics of Music
Page 424: Assessment
Page 429: Standardized Test Practice
Chapter 17: Reflections and Mirrors
Section 17.1: Reflection from Plane Mirrors
Section 17.2: Curved Mirrors
Page 478: Assessment
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Chapter 18: Refraction and lenses
Section 18.1: Refraction of Light
Section 18.2: Convex and Concave Lenses
Section 18.3: Applications of Lenses
Page 508: Assessment
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Chapter 21: Electric Fields
Section 21.1: Creating and Measuring Electric Fields
Section 21.2: Applications of Electric Fields
Page 584: Assessment
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Chapter 22: Current Electricity
Section 22.1: Current and Circuits
Section 22.2: Using Electric Energy
Page 610: Assessment
Page 615: Standardized Test Practice
Chapter 23: Series and Parallel Circuits
Section 23.1: Simple Circuits
Section 23.2: Applications of Circuits
Page 636: Assessment
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Chapter 24: Magnetic Fields
Section 24.1: Magnets: Permanent and Temporary
Section 24.2: Forces Caused by Magnetic Fields
Page 664: Assessment
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Chapter 25: Electromagnetic Induction
Section 25.1: Electric Current from Changing Magnetic Fields
Section 25.2: Changing Magnetic Fields Induce EMF
Page 690: Assessment
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Chapter 30: Nuclear Physics
Section 30.1: The Nucleus
Section 30.2: Nuclear Decay and Reactions
Section 30.3: The Building Blocks of Matter
Page 828: Assessment
Page 831: Standardized Test Practice