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

Section 14.1: Periodic Motion

Exercise 1
Solution 1
Solution 2
Step 1
1 of 2
Information given in the text are:

$x = 0.25, mathrm{m}$

$k = 95, mathrm{N/m}$

Force, which we have to determine, is given by:

$$
F = kx
$$

When we put known values into the previous equation we get:

$$
F = 95, mathrm{N/m} cdot 0.25, mathrm{m}
$$

Finally, the force is:

$$
boxed{F = 24, mathrm{N}}
$$

Result
2 of 2
$$
F = 24, mathrm{N}
$$
Step 1
1 of 3
$mathbf{Known:}$

In this question, we have to calculate the Force needed to stretch a spring. We know that the spring constant is 95 $dfrac{text{N}}{text{m}}$ and the length of the spring is 0.25 m.

Therefore, the formula to calculate the force needed to stretch the spring is as follow.

$mathbf{F = kx}$

where;

F = Force ,

k = spring constant and

x = length

Step 2
2 of 3
$mathbf{Formula:}$

1) Using the formula stated in cell 1.

$mathbf{F = kx}$

2) Substituting the vales in the formula:

F = (95) (0.25)

$$
boxed{ F = 24 text{N}}
$$

Result
3 of 3
$$
boxed{ F = 24 text{N}}
$$
Exercise 2
Step 1
1 of 2
Information given in the text are:

$k = 56, mathrm{N/m}$

$F = 18, mathrm{N}$

Force is given by:

$$
F = kx
$$

We can express $x$ from the precious equation:

$$
x = dfrac{F}{k}
$$

When we put known values into the previous equation we get:

$$
F = dfrac{18, mathrm{N}}{56, mathrm{N/m}}
$$

Finally:

$$
boxed{x = 0.32, mathrm{m}}
$$

Result
2 of 2
$$
x = 0.32, mathrm{m}
$$
Exercise 3
Step 1
1 of 2
Information given in the text are:

$x= 12, mathrm{cm} = 0.12, mathrm{m}$

$F = 24, mathrm{N}$

Force is given by the following equation:

$$
F = kx
$$

$k$ , expressed form the previous equation, is:

$$
k = dfrac{F}{x}
$$

When we put known values into the previous equation we get:

$$
k = dfrac{24, mathrm{N}}{0.12, mathrm{m}}
$$

Therefore, the spring constant will be:

$$
boxed{k = 200, mathrm{N/m}}
$$

Result
2 of 2
$$
k = 200, mathrm{N/m}
$$
Exercise 4
Step 1
1 of 2
We should use $P E_{sp} = dfrac{1}{2} k x^{2}$ equation ;

So

$P E_{sp} = dfrac{1}{2} k x^{2} = dfrac{1}{2} (144 N/m) (0.165m)^{2} = 1.96 J$

Result
2 of 2
$textit$$text{color{#c34632} 1.96J $$}$
Exercise 5
Step 1
1 of 2
$$
text{color{#4257b2}PE = $dfrac{1}{2}kx^2$}
$$

Substitute : PE = 48, $k=256$ and solve for $x$

$$
48 = dfrac{1}{2}(256)x^2
$$

$$
48 = 128x^2
$$

Divide both sides by $128$ and take square root

$$
sqrt{dfrac{48}{128}} = x
$$

$$
x=sqrt{dfrac{48}{128}} approx 0.61text{ m}=61text{ cm}
$$

Result
2 of 2
$$
text{color{#4257b2}61text{ cm}}
$$
Exercise 6
Solution 1
Solution 2
Step 1
1 of 2
$$
color{#4257b2}T = 2pisqrt{dfrac{L}{g}}
$$

Substitute $L = 1$ m and $g = 9.8$ m/s$^2$

$$
T = 2pisqrt{dfrac{1}{9.8}}approx2
$$

Result
2 of 2
$$
text{color{#4257b2}2 seconds}
$$
Step 1
1 of 4
**Given information**

– Pendulum length: $l=1mathrm{~m}$

**Objective**
– Find the period $T$.

Step 2
2 of 4
**Approach**

In order to find the period $T$, we need to relate it to the known information (length $l$ and acceleration due to gravity on Earth $a=g=9.81mathrm{~dfrac{m}{s^2}}$). To do this, we can use the formula:

$$begin{align}
T=2cdot picdotsqrt{dfrac{l}{g}}
end{align}$$

Using formula $(1)$, we can now simply calculate.

Step 3
3 of 4
Calculation:

$$begin{aligned}
T&=2cdot picdotsqrt{dfrac{l}{g}}
\&=2cdot picdotsqrt{dfrac{1}{9.81}}
\&=boxed{2mathrm{~sec}}
end{aligned}$$

Result
4 of 4
$T=2mathrm{~sec}$
Exercise 7
Solution 1
Solution 2
Step 1
1 of 2
$$
color{#4257b2}T = 2pisqrt{dfrac{l}{g}}
$$

Substitute : $T = 2$ sec, $g = 1.6$ m/s$^2$ and solve for $l$

$$
2 = 2pisqrt{dfrac{l}{1.6}}
$$

Divide both sides by $2pi$

$$
dfrac{1}{pi} =sqrt{dfrac{l}{1.6}}
$$

Square both sides

$$
dfrac{1}{pi^2} =dfrac{l}{1.6}
$$

Multiply both sides by 1.6

$$
dfrac{1.6}{pi^2} =l
$$

$$
l = dfrac{1.6}{pi^2} approx 0.16text{ m} = 16text{ cm}
$$

Result
2 of 2
$$
text{color{#4257b2}16text{ cm}}
$$
Step 1
1 of 5
**Given information**

– Acceleration due to gravity: $g_{moon}=1.6mathrm{~dfrac{m}{s^2}}$
– Period: $T=2mathrm{~sec}$

**Objective**

– Find the length $L$.

Step 2
2 of 5
**Approach**

In order to find length of pendulum $L$, we need to relate it to the given information ($g_{moon}$ and $T$). To do this, we can use the formula for period of the pendulum:

$$begin{align}
T=2cdot picdotsqrt{dfrac{L}{g}}
end{align}$$

Where $g$ is the acceleration due to gravity. We can now express the length $L$ from equation $(1)$ and calculate the result.

Step 3
3 of 5
In order to express the length $L$ from the equation $(1)$, we can first square both sides of the equation:

$$begin{aligned}
T&=2cdot picdotsqrt{dfrac{L}{g}}
\T^2&=4cdot pi^2cdot dfrac{L}{g}
end{aligned}$$

Now we can express $L$:
$$begin{align}
T^2&=4cdot pi^2cdot dfrac{L}{g}rightarrow L=dfrac{T^2cdot g}{4cdot pi^2}
end{align}$$

Step 4
4 of 5
Using the equation $(2)$, and using $g=g_{moon}$, we can now simply calculate:

$$begin{aligned}
L&=dfrac{T^2cdot g_{moon}}{4cdot pi^2}
\&=dfrac{2^2cdot 1.6}{4cdot pi^2}
\&=boxed{0.16mathrm{~m}}
end{aligned}$$

Result
5 of 5
$L=0.16mathrm{~m}$
Exercise 8
Solution 1
Solution 2
Step 1
1 of 3
$$
color{#4257b2}T = 2pisqrt{dfrac{l}{g}}
$$

Substitute : $T = 1.8$ sec, $l = 0.75$ m and solve for $g$

$$
1.8 = 2pisqrt{dfrac{0.75}{g}}
$$

Divide both sides by $2pi$

$$
dfrac{1.8}{2pi} = sqrt{dfrac{0.75}{g}}
$$

Square both sides

$$
left( dfrac{1.8}{2pi}right)^2 = dfrac{0.75}{g}
$$

Take reciprocal of both sides

$$
left( dfrac{2pi}{1.8}right)^2 = dfrac{g}{0.75}
$$

Step 2
2 of 3
Multiply both sides by 0.75

$$
0.75cdot left( dfrac{2pi}{1.8}right)^2 =g
$$

$$
g = 0.75cdot left( dfrac{2pi}{1.8}right)^2 approx 9.1text{ m/s}^2
$$

Result
3 of 3
$$
text{color{#4257b2}$9.1text{ m/s}^2$}
$$
Step 1
1 of 5
**Given information**

– Pendulum length: $L=0.75mathrm{~m}$
– Period: $T=1.8mathrm{~sec}$

**Objective**

– Find the acceleration due to gravity $g$.

Step 2
2 of 5
**Approach**

In order to find the acceleration due to gravity $g$, we need to relate it to the given information (Length $L$ and period $T$). To do this we can use the formula:

$$begin{align}
T=2cdot picdotsqrt{dfrac{L}{g}}
end{align}$$

In this formula, we know all the parameters except acceleration $g$, which we are looking for. So, we can just express $g$ from formula $(1)$, and calculate the result.

Step 3
3 of 5
To express $g$ from equation $(1)$, we can first square both sides of the equation:

$$begin{align}
T^2=4cdotpi^2cdot{dfrac{L}{g}}
end{align}$$

Now we simply express the acceleration due to gravity $g$ from $(2)$:
$$begin{align}
g={dfrac{4cdotpi^2cdot L}{T^2}}
end{align}$$

Finally, using equation $(3)$, we can calculate acceleration due to gravity $g$.

Step 4
4 of 5
Calculation:

$$begin{aligned}
g&={dfrac{4cdotpi^2cdot L}{T^2}}
\&={dfrac{4cdotpi^2cdot 0.75}{1.8^2}}
\&=boxed{9.14mathrm{~dfrac{m}{s^2}}}
end{aligned}$$

Result
5 of 5
$g=9.14mathrm{~dfrac{m}{s^2}}$
Exercise 9
Step 1
1 of 2
In order to determine which of the two springs has a greater constant we should hang same weight to both of them and the spring that stretches more will have smaller spring constant and vice versa.
Result
2 of 2
By attaching same weight to both of the strings.
Exercise 10
Step 1
1 of 2
We can conclude from the graph if the rubber band obeys Hooke’s law by checking if the graph shows straight or curved line, if the line is straight it obeys it.
Result
2 of 2
If the line on the graph is straight, rubber band obeys Hooke’s law.
Exercise 11
Step 1
1 of 5
$$
text{color{#4257b2}Remember that : $$T = 2pisqrt{dfrac{l}{g}}$$}
$$
Step 2
2 of 5
$$
dfrac{T_{new}}{T_{old}} = dfrac{cancel{2pi}sqrt{dfrac{l_{new}}{g}}}{cancel{2pi}sqrt{dfrac{l_{old}}{g}}}
$$

$$
dfrac{T_{new}}{T_{old}} = dfrac{sqrt{dfrac{l_{new}}{g}}}{sqrt{dfrac{l_{old}}{g}}}
$$

$$
dfrac{T_{new}}{T_{old}} = sqrt{dfrac{l_{new}}{g}}timessqrt{dfrac{g}{l_{old}}}
$$

$$
dfrac{T_{new}}{T_{old}} = sqrt{dfrac{l_{new}}{l_{old}}}
$$

Square both sides

$$
left( dfrac{T_{new}}{T_{old}}right)^2 =dfrac{l_{new}}{l_{old}}
$$

$$
text{color{#c34632}$$l_{new } = l_{old}times left( dfrac{T_{new}}{T_{old}}right)^2$$}
$$

Step 3
3 of 5
When the period becomes double, we have $dfrac{T_{new}}{T_{old}} = 2$

$$
l_{new} = l_{old}times (2)^2
$$

$$
l_{new} = 4cdot l_{old}
$$

$$
text{color{#4257b2}For period to become 2 times, the length must become 4 times }
$$

Step 4
4 of 5
When the period becomes half, we have $dfrac{T_{new}}{T_{old}} = dfrac{1}{2}$

$$
l_{new} = l_{old}times (1/2)^2
$$

$$
l_{new} =dfrac{l_{old}}{4}
$$

$$
text{color{#4257b2}For period to become half, the length must become one fourth}
$$

Result
5 of 5
$$
text{color{#4257b2}For period to become 2 times, the length must become 4 times

$ $

color{#4257b2}For period to become half, the length must become one fourth}
$$

Exercise 12
Solution 1
Solution 2
Step 1
1 of 1
$T = 2pi sqrt{dfrac{I}{g}}$ . So ; $dfrac{T_{2}}{T_{1}} = sqrt{dfrac{I_{2}}{I_{1}}}$

To double the period ;

$dfrac{T_{2}}{T_{1}} = sqrt{dfrac{I_{2}}{I_{1}}} = 2$ . So;$dfrac{I_{2}}{I_{1}} = 4$

The length must be quadrupled.

To halve the period:

$dfrac{T_{2}}{T_{1}} = sqrt{dfrac{I_{2}}{I_{1}}} = dfrac{1}{2}.$ So ; $dfrac{I_{2}}{I_{1}} = dfrac{1}{4}$

The length is reduced to one-fourth its
original length.

Step 1
1 of 6
**Given information**

– First length of displacement: $l_1=0.40mathrm{~m}$
– Second length of displacement: $l_2=0.20mathrm{~m}$

**Objective**

– Find the change in potential energy.

Step 2
2 of 6
**Approach**

To find the change in potential energy, we can first consider the formula for the potential energy of the spring $P$ due to displacement (stretch) of length $x$:

$$begin{align}
P=dfrac{1}{2}cdot kcdot x^2
end{align}$$
Where $k$ is the spring constant (different constant for different strings/materials).

Step 3
3 of 6
We can now write formula $(1)$ for given displacements $l_1$ and $l_2$, to get the potential energy of the spring for both cases $P_1$ and $P_2$:

$$begin{align}
P_1=dfrac{1}{2}cdot kcdot l_1^2
end{align}$$

$$begin{align}
P_2=dfrac{1}{2}cdot kcdot l_2^2
end{align}$$

The constant $k$ is the property of the spring, and since it is the same spring for both cases, it stays the same constant for $l_1$ and $l_2$.

Step 4
4 of 6
To find how did the potential energy change $varDelta P$, we can simply divide equation $(2)$ by equation $(3)$:

$$begin{align}
dfrac{P_1}{P_2}&=dfrac{dfrac{1}{cancel 2}cdot cancel kcdot l_1^2} nonumber{dfrac{1}{cancel2}cdot cancel kcdot l_2^2}
\&=dfrac{l_1^2}{l_2^2}
end{align}$$

Using this result, we can simply calculate the proportion $dfrac{P_1}{P_2}$.

Step 5
5 of 6
Calculation:
$$begin{aligned}
dfrac{P_1}{P_2}&=dfrac{l_1^2}{l_2^2}
\&=dfrac{0.4^2}{0.2^2}
\&=4
end{aligned}$$

So, from this result, we see that $boxed{P_2=dfrac{ P_1}{4}}$, meaning that the potential energy stored at $0.2mathrm{~m}$ displacement is $4$ times smaller then energy stored at the $0,4mathrm{~m}$ displacement.

Step 6
6 of 6
$P_2=dfrac{ P_1}{4}$
Exercise 13
Solution 1
Solution 2
Step 1
1 of 1
Car will start shaking strongly when Tire’s rotation frequency = Resonant frequency of the car
Step 1
1 of 1
Car will shake strongly when resonant frequency of the car is equal to the rotation frequency of the tire.
Exercise 14
Step 1
1 of 1
Uniform circular motion and simple harmonic motion are both periodic motions, but they are different because uniform circular motion is motion in two dimensions and simple harmonic motion is motion in one dimension.
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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
Page 483: Standardized Test Practice
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
Page 513: Standardized Test Practice
Chapter 21: Electric Fields
Section 21.1: Creating and Measuring Electric Fields
Section 21.2: Applications of Electric Fields
Page 584: Assessment
Page 589: Standardized Test Practice
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
Page 641: Standardized Test Practice
Chapter 24: Magnetic Fields
Section 24.1: Magnets: Permanent and Temporary
Section 24.2: Forces Caused by Magnetic Fields
Page 664: Assessment
Page 669: Standardized Test Practice
Chapter 25: Electromagnetic Induction
Section 25.1: Electric Current from Changing Magnetic Fields
Section 25.2: Changing Magnetic Fields Induce EMF
Page 690: Assessment
Page 695: Standardized Test Practice
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