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 128: Practice Problems

Exercise 17
Solution 1
Solution 2
Step 1
1 of 7
force = mass x acceleration
but there is a resistance opposing the force so the law is going to be
Step 2
2 of 7
force – resistance = mass x acceleration
and since the problem describes motion as (constant speed) so that means that the acceleration = zero
Step 3
3 of 7
force – resistance = zero
by adding +resistance to both sides
Step 4
4 of 7
force = resistance
substitute force with 36N
and acceleration with $mu_k$ $times$ 52
Step 5
5 of 7
36 = $52 times mu_k$
Step 6
6 of 7
$$
mu_k = dfrac{36}{52}
$$
Result
7 of 7
$mu_k$ = 0.69
Step 1
1 of 2
In this task we will calculate the friction factor for the given data.

Known:

$$
begin{align*}
F_g&=52 mathrm{N} \
F_p&=36 mathrm{N} tag{force exerted on sled by girl} \
end{align*}
$$

Unknown:

$$
begin{align*}
{mu } &=? \
\
F_f&={mu}cdot F_N tag{$F_N$ normal force} \
mu&=dfrac{F_f}{F_N} \
\
F_f&=F_p \
F_N&=F_g \
\
mu&=dfrac{F_p}{F_g} \
&=dfrac{36 mathrm{N} } {52 mathrm{N}} \
&=boxed{0.692}
end{align*}
$$

Notice that $mu$ is ratio and that it has no unit of measurement.

Result
2 of 2
$$
mu=0.692
$$
Exercise 18
Step 1
1 of 6
weight = mass x acceleration due to gravity
105 x 9.8 = 1029 N
the mass is given in KG but we work in Newton
so to convert it we multiply the mass with 9.8
Step 2
2 of 6
acceleration = zero
when it says (constant speed,uniform velocity,maximum velocity) that means that the acceleration = zero
a.k.a left = right
up = down
Step 3
3 of 6
force = resistance
substitute force with 102 N and resistance with 1029 x $mu_s$
Step 4
4 of 6
$$
102 = 1029 times mu_s
$$
Step 5
5 of 6
$$
mu_s = dfrac{102}{1029}
$$
Result
6 of 6
$mu_s$ = 0.099
Exercise 19
Step 1
1 of 4
In this problem we are calculating the force needed tu push a box.

Known:

$$
begin{align*}
F_g&=134 mathrm{N} \
mu&=0.55
end{align*}
$$

Unknown:

$$
begin{align*}
F_p&=?
end{align*}
$$

Step 2
2 of 4
Force needed to push a box is equal to the force of friction because that is the force that keeps the box at rest.

$$
begin{align*}
F_p&=F_f \
F_g&=F_N
end{align*}
$$

Step 3
3 of 4
Calculating the force needed.

$$
begin{align*}
F_p&=mucdot F_g \
&=0.55cdot 134 mathrm{N} \
&=boxed{73.98 mathrm{N}}
end{align*}
$$

Result
4 of 4
$$
F_p=73.94 mathrm{N}
$$
Exercise 20
Step 1
1 of 5
We are tasked to find the force $F_f$ required to pull the sled at a constant speed across the snow.
Step 2
2 of 5
Let us review the given values. We have the coefficient of kinetic friction $mu_k$, the weight $W_{person}$ of the person on the sled, and the weight $W_{sled}$ of the sled.

$$
begin{align*}
mu_k &= 0.12\
W_{person} &= 650 ,mathrm{N}\
W_{sled} &= 52 , mathrm{N}
end{align*}
$$

Step 3
3 of 5
begin{align}
intertext{Given the formula}
F_f &= mu_kF_N
intertext{such that}
F_N &= W_{person} + W_{sled}
end{align}

where $F_f$ is the force needed to needed to move the sled, $F_N$ is the normal force for the system, and $mu_k$ is the coefficient of kinetic friction acting against the system.

Step 4
4 of 5
We can now solve for the force by plugging in the given values.

$$
begin{align*}
F_f &= mu_kF_N\
&= mu_k(W_{person} + W_{sled})\
&= (0.12)(650.,mathrm{N} + 52.0,mathrm{N})\
&= boxed{84.0 ,mathrm{N}}
end{align*}
$$

Result
5 of 5
$$
F_f = 84.0 ,mathrm{N}
$$
Exercise 21
Solution 1
Solution 2
Step 1
1 of 2
By applying oil, the coefficient of friction $mu$ is reduced and thus the friction force is reduced so that the required force is also lower.

$$
begin{align*}
F_f&=5.8 mathrm{N} tag{Force when oil is not applied.} \
mu_{d}&=0.58 \
mu_{wo}&=0.06\
F’_f&=?tag{Force after oil application.}\
\
F_f&=mucdot F_N \
F_N&=dfrac{F_f}{mu_{d}} \
&=dfrac{5.8 mathrm{N}}{0.58} \
&=10 mathrm{N} \
\
F’_f&=mu_{wo}cdot F_N \
&=0.06cdot 10 mathrm{N} \
&=0.6 mathrm{N}
end{align*}
$$

Result
2 of 2
$$
F’_f=0.6 mathrm {N}
$$
Step 1
1 of 3
In the book we are given the coefficients of friction on a table. Steel on steel (dry) is .58 for kinetic, therefore we can assume that the rest of our (m)(g) is equal to 10 because of the 5.8N we start with.
Step 2
2 of 3
Using the same table we can see Steel on Steel (with oil) as a .06 so we multiply it by 10 to get 0.6N
Result
3 of 3
0.6N
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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