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Physics for Scientists and Engineers with Modern Physics

Raymond A. Serway, John W. Jewett, Jr.

Chapter 15

Oscillatory Motion - all with Video Answers

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Chapter Questions

02:13

Problem 1

A $0.60-\mathrm{kg}$ block attached to a spring with force constant $130 \mathrm{~N} / \mathrm{m}$ is free to move on a frictionless, horizontal surface as in Figure $15.1 .$ The block is released from rest when the spring is stretched $0.13 \mathrm{~m}$. At the instant the block is released, find (a) the force on the block and (b) its acceleration.

Lisa Tarman
Lisa Tarman
Numerade Educator
04:23

Problem 2

A piston in a gasoline engine is in simple harmonic motion. The engine is running at the rate of 3600 rev/min. Taking the extremes of its position relative to its center point as $\pm 5.00 \mathrm{~cm},$ find the magnitudes of the (a) maximum velocity and (b) maximum acceleration of the piston.

Mukesh Devi
Mukesh Devi
Numerade Educator
02:18

Problem 3

The position of a particle is given by the expression $x=4.00 \cos (3.00 \pi t+\pi),$ where $x$ is in meters and $t$ is in seconds. Determine (a) the frequency and (b) period of the motion, (c) the amplitude of the motion, (d) the phase constant, and (e) the position of the particle at $t=0.250 \mathrm{~s}$

Matt Braby
Matt Braby
Numerade Educator
00:57

Problem 4

A 7.00 -kg object is hung from the bottom end of a vertical spring fastened to an overhead beam. The object is set into vertical oscillations having a period of $2.60 \mathrm{~s}$. Find the force constant of the spring.

Matt Braby
Matt Braby
Numerade Educator
07:17

Problem 5

A particle moves along the $x$ axis. It is initially at the position $0.270 \mathrm{~m},$ moving with velocity $0.140 \mathrm{~m} / \mathrm{s}$ and acceleration $-0.320 \mathrm{~m} / \mathrm{s}^{2}$. Suppose it moves as a particle under constant acceleration for 4.50 s. Find (a) its position and (b) its velocity at the end of this time interval. Next, assume it moves as a particle in simple harmonic motion for $4.50 \mathrm{~s}$ and $x=0$ is its equilibrium position. Find (c) its position and (d) its velocity at the end of this time interval.

Matt Braby
Matt Braby
Numerade Educator
06:16

Problem 6

A ball dropped from a height of $4.00 \mathrm{~m}$ makes an elastic collision with the ground. Assuming no decrease in mechanical energy due to air resistance, (a) show that the ensuing motion is periodic and (b) determine the period of the motion. (c) Is the motion simple harmonic? Explain.

Jacob Schulze
Jacob Schulze
Numerade Educator
06:27

Problem 7

A particle moving along the $x$ axis in simple harmonic motion starts from its equilibrium position, the origin, at $t=0$ and moves to the right. The amplitude of its motion is $2.00 \mathrm{~cm},$ and the frequency is $1.50 \mathrm{~Hz}$. (a) Find an expression for the position of the particle as a function of time. Determine (b) the maximum speed of the particle and (c) the earliest time $(t>0)$ at which the particle has this speed. Find (d) the maximum positive acceleration of the particle and (e) the earliest time $(t>0)$ at which the particle has this acceleration. (f) Find the total distance traveled by the particle between $t=0$ and $t=1.00 \mathrm{~s}$

Sheh Lit Chang
Sheh Lit Chang
University of Washington
11:46

Problem 8

The initial position, velocity, and acceleration of an object moving in simple harmonic motion are $x_{i}, v_{i},$ and $a_{i} ;$ the angular frequency of oscillation is $\omega .$ (a) Show that the position and velocity of the object for all time can be written as
$$
\begin{array}{l}
x(t)=x_{i} \cos \omega t+\left(\frac{v_{i}}{\omega}\right) \sin \omega t \\
v(t)=-x_{i} \omega \sin \omega t+v_{i} \cos \omega t
\end{array}
$$
(b) Using $A$ to represent the amplitude of the motion, show that
$$
v^{2}-a x=v_{i}^{2}-a_{i} x_{i}=\omega^{2} A^{2}
$$

Ren Jie Tuieng
Ren Jie Tuieng
Numerade Educator
02:43

Problem 9

You attach an object to the bottom end of a hanging vertical spring. It hangs at rest after extending the spring $18.3 \mathrm{~cm}$. You then set the object vibrating. (a) Do you have enough information to find its period?
(b) Explain your answer and state whatever you can about its period.

Keshav Singh
Keshav Singh
Numerade Educator
01:35

Problem 10

To test the resiliency of its bumper during low-speed collisions, a 1000 -kg automobile is driven into a brick wall. The car's bumper behaves like a spring with a force constant $5.00 \times 10^{6} \mathrm{~N} / \mathrm{m}$ and compresses $3.16 \mathrm{~cm}$ as the car is brought to rest. What was the speed of the car before impact, assuming no mechanical energy is transformed or transferred away during impact with the wall?

Matt Braby
Matt Braby
Numerade Educator
02:32

Problem 11

A particle executes simple harmonic motion with an amplitude of $3.00 \mathrm{~cm} .$ At what position does its speed equal half of its maximum speed?

Deepak Kohli
Deepak Kohli
Numerade Educator
02:50

Problem 12

The amplitude of a system moving in simple harmonic motion is doubled. Determine the change in (a) the total energy, (b) the maximum speed, (c) the maximum acceleration, and (d) the period.

Deepak Kohli
Deepak Kohli
Numerade Educator
View

Problem 13

A simple harmonic oscillator of amplitude $A$ has a total energy $E .$ Determine (a) the kinetic energy and
(b) the potential energy when the position is one-third the amplitude. (c) For what values of the position does the kinetic energy equal one-half the potential energy?
(d) Are there any values of the position where the kinetic energy is greater than the maximum potential energy? Explain.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
06:23

Problem 14

A 65.0 -kg bungee jumper steps off a bridge with a light bungee cord tied to her body and to the bridge. The unstretched length of the cord is $11.0 \mathrm{~m}$. The jumper reaches the bottom of her motion $36.0 \mathrm{~m}$ below the bridge before bouncing back. We wish to find the time interval between her leaving the bridge and her arriving at the bottom of her motion. Her overall motion can be separated into an 11.0 -m free fall and a 25.0 -m section of simple harmonic oscillation.
(a) For the free-fall part, what is the appropriate analysis model to describe her motion? (b) For what time interval is she in free fall? (c) For the simple harmonic oscillation part of the plunge, is the system of the bungee jumper, the spring, and the Earth isolated or nonisolated? (d) From your response in part (c) find the spring constant of the bungee cord. (e) What is the location of the equilibrium point where the spring force balances the gravitational force exerted on the jumper?
(f) What is the angular frequency of the oscillation? (g) What time interval is required for the cord to stretch by $25.0 \mathrm{~m} ?$
(h) What is the total time interval for the entire 36.0 -m drop?

Deepak Kohli
Deepak Kohli
Numerade Educator
06:06

Problem 15

A $0.250-\mathrm{kg}$ block resting on a frictionless, horizontal surface is attached to a spring whose force constant is $83.8 \mathrm{~N} / \mathrm{m}$ as in Figure $\mathrm{P} 15.15 .$ A horizontal force $\overrightarrow{\mathbf{F}}$ causes the spring to stretch a distance of $5.46 \mathrm{~cm}$ from its equilibrium position. (a) Find the magnitude of $\overrightarrow{\mathbf{F}}$.
(b) What is the total energy stored in the system when the spring is stretched? (c) Find the magnitude of the acceleration of the block just after the applied force is removed. (d) Find the speed of the block when it first reaches the equilibrium position. (e) If the surface is not frictionless but the block still reaches the equilibrium position, would your answer to part (d) be larger or smaller? (f) What other information would you need to know to find the actual answer to part (d) in this case? (g) What is the largest value of the coefficient of friction that would allow the block to reach the
equilibrium position?

Jacob Schulze
Jacob Schulze
Numerade Educator
06:32

Problem 16

While driving behind a car traveling at $3.00 \mathrm{~m} / \mathrm{s},$ you notice that one of the car's tires has a small hemispherical bump on its rim as shown in Figure $\mathrm{P} 15.16$.
(a) Explain why the bump, from your viewpoint behind the car, executes simple harmonic motion. (b) If the radii of the car's tires are $0.300 \mathrm{~m}$, what is the bump's period of oscillation? (c) What If? You hang a spring with spring constant $k=100 \mathrm{~N} / \mathrm{m}$ from the rear view mirror of your car. What is the mass that needs to be hung from this spring to produce simple harmonic motion with the same period as the bump on the tire? (d) What would be the maximum speed of the hanging mass in your car if you initially pulled the mass down $8.00 \mathrm{~cm}$ beyond equilibrium before releasing it?

Jacob Schulze
Jacob Schulze
Numerade Educator
01:16

Problem 17

A simple pendulum makes 120 complete oscillations in $3.00 \mathrm{~min}$ at a location where $g=9.80 \mathrm{~m} / \mathrm{s}^{2}$. Find (a) the period of the pendulum and (b) its length.

Matt Braby
Matt Braby
Numerade Educator
01:28

Problem 18

A particle of mass $m$ slides without friction inside a hemispherical bowl of radius $R$. Show that if the particle starts from rest with a small displacement from equilibrium, it moves in simple harmonic motion with an angular frequency equal to that of a simple pendulum of length $R$. That is, $\omega=\sqrt{g / R}$

Deepak Kohli
Deepak Kohli
Numerade Educator
01:49

Problem 19

A physical pendulum in the form of a planar object moves in simple harmonic motion with a frequency of $0.450 \mathrm{~Hz}$. The pendulum has a mass of $2.20 \mathrm{~kg}$, and the pivot is located $0.350 \mathrm{~m}$ from the center of mass. Determine the moment of inertia of the pendulum about the pivot point.

Matt Braby
Matt Braby
Numerade Educator
02:10

Problem 20

A physical pendulum in the form of a planar object moves in simple harmonic motion with a frequency $f$. The pendulum has a mass $m,$ and the pivot is located a distance $d$ from the center of mass. Determine the moment of inertia of the pendulum about the pivot point.

Keshav Singh
Keshav Singh
Numerade Educator
13:42

Problem 21

A simple pendulum has a mass of $0.250 \mathrm{~kg}$ and a length of $1.00 \mathrm{~m} .$ It is displaced through an angle of $15.0^{\circ}$ and then released. Using the analysis model of a particle in simple harmonic motion, what are (a) the maximum speed of the bob, (b) its maximum angular acceleration, and (c) the maximum restoring force on the bob? (d) What If? Solve parts (a) through (c) again by using analysis models introduced in earlier chapters. (e) Compare the answers.

Ren Jie Tuieng
Ren Jie Tuieng
Numerade Educator
07:59

Problem 22

Consider the physical pendulum of Figure 15.16 . (a) Represent its moment of inertia about an axis passing through its center of mass and parallel to the axis passing through its pivot point as $I_{\mathrm{CM}}$. Show that its period is
$$
T=2 \pi \sqrt{\frac{I_{C M}+m d^{2}}{m g d}}
$$
where $d$ is the distance between the pivot point and the center of mass. (b) Show that the period has a minimum value when $d$ satisfies $m d^{2}=I_{C M}$

Jacob Schulze
Jacob Schulze
Numerade Educator
02:45

Problem 23

A watch balance wheel (Fig. P15.23) has a period of oscillation of $0.250 \mathrm{~s}$ The wheel is constructed so that its mass of $20.0 \mathrm{~g}$ is concentrated around a rim of radius $0.500 \mathrm{~cm}$.
What are (a) the wheel's moment of inertia and (b) the torsion constant of the attached spring?

Jacob Schulze
Jacob Schulze
Numerade Educator
01:49

Problem 24

Show that the time rate of change of mechanical energy for a damped, undriven oscillator is given by $d E / d t=-b v^{2}$ and hence is always negative. To do so, differentiate the expression for the mechanical energy of an oscillator, $E=\frac{1}{2} m v^{2}+\frac{1}{2} k x^{2},$ and use Equation $15.31 .$

Ajay Singhal
Ajay Singhal
Numerade Educator
11:34

Problem 25

Show that Equation 15.32 is a solution of Equation 15.31 provided that $b^{2}<4 m k$

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
01:48

Problem 26

As you enter a fine restaurant, you realize that you have accidentally brought a small electronic timer from home instead of your cell phone. In frustration, you drop the timer into a side pocket of your suit coat, not realizing that the timer is operating. The arm of your chair presses the light cloth of your coat against your body at one spot. Fabric with a length $L$ hangs freely below that spot, with the timer at the bottom. At one point during your dinner, the timer goes off and a buzzer and a vibrator turn on and off with a frequency of $1.50 \mathrm{~Hz}$. It makes the hanging part of your coat swing back and forth with remarkably large amplitude, drawing everyone's attention. Find the value of $L$.

Deepak Kohli
Deepak Kohli
Numerade Educator
03:14

Problem 27

A $2.00-\mathrm{kg}$ object attached to a spring moves without friction $(b=0)$ and is driven by an external force given by the expression $F=3.00 \sin (2 \pi t),$ where $F$ is in newtons and $t$ is in seconds. The force constant of the spring is $20.0 \mathrm{~N} / \mathrm{m}$. Find (a) the resonance angular frequency of the system, (b) the angular frequency of the driven system, and (c) the amplitude of the motion.

Deepak Kohli
Deepak Kohli
Numerade Educator
05:27

Problem 28

Considering an undamped, forced oscillator $(b=0),$ show that Equation 15.35 is a solution of Equation 15.34 , with an amplitude given by Equation 15.36 .

Luis Rios
Luis Rios
Numerade Educator
05:31

Problem 29

You have scored a part time job at a company that makes small probes to be released from satellites to study the very thin atmosphere at the location of satellite orbits. In order to keep the probes in a proper orientation in space, they will be spun about their axis before being released. It is important to know the moment of inertia of the odd-shaped probe. Your boss asks you to measure its moment of inertia. You set up a system such as that in Figure 15.18 , modifying it by adding a very light frame (Fig. $\mathrm{P} 15.29$ ) into which you can place objects, centering them on the disk. The frame is attached at the edges of the disk. The support wire is rigidly connected to the top of the frame so that it does not interfere with the objects you wish to place on the disk. The disk is of mass $M=5.25 \mathrm{~kg}$ and has a radius of $R=25.8 \mathrm{~cm}$ You rotate the empty disk from its equilibrium position and let it operate as a torsional pendulum. You carefully measure its period of oscillation to be $T_{\text {empty }}=10.8$ s. You then place the probe on the disk and adjust its position until the disk hangs exactly horizontal, so you know that the center of mass of the probe is directly over the center of the disk. You rotate the loaded disk from its equilibrium position and let it operate as a torsional pendulum. (a) You carefully measure its period of oscillation to be $T_{\text {loaded }}=18.7 \mathrm{~s},$ and from this result you determine the moment of inertia of the probe about its center of mass. (b) When you present your results to your supervisor, she asks you about the moment of inertia of the frame you built. You go back to your desk and think about it. When you consider that the frame has some moment of inertia, is the value calculated in part (a) too high or too low?

Jacob Schulze
Jacob Schulze
Numerade Educator
11:26

Problem 30

You take on a research assistantship with a molecular physicist. She is studying the vibrations of diatomic molecules. In these vibrations, the two atoms in the molecule move back and forth along the line connecting them (see Figure $20.5 \mathrm{c}$ ). As an introduction to her research, she asks you to familiarize yourself with the Lennard-Jones potential (see Example 7.9 ), which describes the potential energy function for a diatomic molecule. She asks you to determine the effective spring constant, in terms of the parameters $\sigma$ and $\epsilon,$ for the bond holding the atoms together in the molecule for small vibrations around the equilibrium separation $r_{\mathrm{cq}} .$ After being stumped for a while, you ask her for a hint. She responds, "Example 7.9 provides the derivative of the potential energy function. Compare that to Equation 7.29 to find the force between the atoms. You want to show that $F$ is of the form $-k x$, and find $k .$ Let the separation distance $r=r_{\mathrm{eq}}+x,$ where $x$ is small and take advantage of the series approximations in Appendix Section B.5." Wow, that's several hints! You sit down and get to work.

Jacob Schulze
Jacob Schulze
Numerade Educator
02:39

Problem 31

An object of mass $m$ moves in simple harmonic motion with amplitude $12.0 \mathrm{~cm}$ on a light spring. Its maximum acceleration is $108 \mathrm{~cm} / \mathrm{s}^{2}$. Regard $m$ as a variable. (a) Find the period $T$ of the object. (b) Find its frequency $f$. (c) Find the maximum speed $v_{\max }$ of the object. (d) Find the total energy $E$ of the object-spring system. (e) Find the force constant $k$ of the spring. (f) Describe the pattern of dependence of each of the quantities $T, f, v_{\max }, E,$ and $k$ on $m$.

Matt Braby
Matt Braby
Numerade Educator
06:11

Problem 32

Review. This problem extends the reasoning of Problem 41 in Chapter $9 .$ Two gliders are set in motion on an air track. Glider 1 has mass $m_{1}=0.240 \mathrm{~kg}$ and moves to the right with speed $0.740 \mathrm{~m} / \mathrm{s}$. It will have a rear-end collision with glider $2,$ of mass $m_{2}=0.360 \mathrm{~kg},$ which initially moves to the right with speed $0.120 \mathrm{~m} / \mathrm{s}$. A light spring of force constant $45.0 \mathrm{~N} / \mathrm{m}$ is attached to the back end of glider 2 as shown in Figure $\mathrm{P} 9.41 .$ When glider 1 touches the spring, superglue instantly and permanently makes it stick to its end of the spring. (a) Find the common speed the two gliders have when the spring is at maximum compression. (b) Find the maximum spring compression distance. The motion after the gliders become attached consists of a combination of
(1) the constant-velocity motion of the center of mass of the two-glider system found in part (a) and (2) simple harmonic motion of the gliders relative to the center of mass.
(c) Find the energy of the center-of-mass motion.
(d) Find the energy of the oscillation.

Jacob Schulze
Jacob Schulze
Numerade Educator
03:18

Problem 33

An object attached to a spring vibrates with simple harmonic motion as described by Figure $\mathrm{P} 15.33 .$ For this motion, find (a) the amplitude, (b) the period, (c) the angular frequency, (d) the maximum speed, (e) the maximum acceleration, and (f) an equation for its position $x$ as a function of time.

Keshav Singh
Keshav Singh
Numerade Educator
05:11

Problem 34

A rock rests on a concrete sidewalk. An earthquake strikes, making the ground move vertically in simple harmonic motion with a constant frequency of $2.40 \mathrm{~Hz}$ and with gradually increasing amplitude. (a) With what amplitude does the ground vibrate when the rock begins to lose contact with the sidewalk? Another rock is sitting on the concrete bottom of a swimming pool full of water. The earthquake produces only vertical motion, so the water does not slosh from side to side. (b) Present a convincing argument that when the ground vibrates with the amplitude found in part
(a), the submerged rock also barely loses contact with the floor of the swimming pool.

Jacob Schulze
Jacob Schulze
Numerade Educator
02:36

Problem 35

A pendulum of length $L$ and mass $M$ has a spring of force constant $k$ connected to it at a distance $h$ below its point of suspension (Fig. $\mathrm{P} 15.35$ ). Find the frequency of vibration of the system for small values of the amplitude (small $\theta$ ). Assume the vertical suspension rod of length $L$ is rigid, but ignore its
mass.

James Kiss
James Kiss
Numerade Educator
09:42

Problem 36

To account for the walking speed of a bipedal or quadrupedal animal, model a leg that is not contacting the ground as a uniform rod of length $\ell$, swinging as a physical pendulum through one-half of a cycle, in resonance. Let $\theta_{\max }$ represent its amplitude. (a) Show that the animal's speed is given by the expression $v=\frac{\sqrt{6 g \ell} \sin \theta_{\max }}{\pi}$ if $\theta_{\max }$ is sufficiently small that the motion is nearly simple harmonic. An empirical relationship that is based on the same model and applies over a wider range of angles is $$
v=\frac{\sqrt{6 g \ell \cos \left(\theta_{\max } / 2\right)} \sin \theta_{\max }}{\pi}
$$
(b) Evaluate the walking speed of a human with leg length $0.850 \mathrm{~m}$ and leg-swing amplitude $28.0^{\circ} .$ (c) What leg length would give twice the speed for the same angular amplitude?

Ren Jie Tuieng
Ren Jie Tuieng
Numerade Educator
07:20

Problem 37

Review. A particle of mass $4.00 \mathrm{~kg}$ is attached to a spring with a force constant of $100 \mathrm{~N} / \mathrm{m}$. It is oscillating on a frictionless, horizontal surface with an amplitude of $2.00 \mathrm{~m} . \mathrm{A}$ $6.00-\mathrm{kg}$ object is dropped vertically on top of the $4.00-\mathrm{kg}$ object as it passes through its equilibrium point. The two objects stick together. (a) What is the new amplitude of the vibrating system after the collision?
(b) By what factor has the period of the system changed?
(c) By how much does the energy of the system change as a result of the collision?
(d) Account for the change in energy.

Jacob Schulze
Jacob Schulze
Numerade Educator
06:27

Problem 38

People who ride motorcycles and bicycles learn to look out for bumps in the road and especially for washboarding, a condition in which many equally spaced ridges are worn into the road. What is so bad about washboarding? A motorcycle has several springs and shock absorbers in its suspension, but you can model it as a single spring supporting a block. You can estimate the force constant by thinking about how far the spring compresses when a heavy rider sits on the seat. A motorcyclist traveling at highway speed must be particularly careful of washboard bumps that are a certain distance apart. What is the order of magnitude of their separation distance?

Jacob Schulze
Jacob Schulze
Numerade Educator
03:28

Problem 39

A ball of mass $m$ is connected to two rubber bands of length $L$, each under tension $T$ as shown in Figure $\mathrm{P} 15.39 .$ The ball is displaced by a small distance $y$ perpendicular to the length of the rubber bands. Assuming the tension does not change, show that (a) the restoring force is $-(2 T / L) y$ and (b) the system exhibits simple harmonic motion with an angular frequency $\omega=\sqrt{2 T / m L}$

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
02:14

Problem 40

Consider the damped oscillator illustrated in Figure $15.19 .$ The mass of the object is 375 g, the spring constant is $100 \mathrm{~N} / \mathrm{m},$ and $b=0.100 \mathrm{~N} \cdot \mathrm{s} / \mathrm{m} .$ (a) Over what time interval does the amplitude drop to half its initial value? (b) What If? Over what time interval does the mechanical energy drop to half its initial value? (c) Show that, in general, the fractional rate at which the amplitude decreases in a damped harmonic oscillator is one-half the fractional rate at which the mechanical energy decreases.

Prashant Bana
Prashant Bana
Numerade Educator
01:42

Problem 41

Review. A lobsterman's buoy is a solid wooden cylinder of radius $r$ and mass $M .$ It is weighted at one end so that it floats upright in calm seawater, having density $\rho$. A passing shark tugs on the slack rope mooring the buoy to a lobster trap, pulling the buoy down a distance $x$ from its equilibrium position and releasing it. (a) Show that the buoy will execute simple harmonic motion if the resistive effects of the water are ignored.
(b) Determine the period of the oscillations.

Penny Riley
Penny Riley
Numerade Educator
14:39

Problem 42

Your thumb squeaks on a plate you have just washed. Your sneakers squeak on the gym floor. Car tires squeal when you start or stop abruptly. You can make a goblet sing by wiping your moistened finger around its rim. When chalk squeaks on a blackboard, you can see that it makes a row of regularly spaced dashes. As these examples suggest, vibration commonly results when friction acts on a moving elastic object. The oscillation is not simple harmonic motion, but is called stick-and-slip. This problem models stick-andslip motion. A block of mass $m$ is attached to a fixed support by a horizontal spring with force constant $k$ and negligible mass (Fig. $\mathrm{P} 15.42$ ). Hooke's law describes the spring both in extension and in compression. The block sits on a long horizontal board, with which it has coefficient of static friction $\mu_{s}$ and a smaller coefficient of kinetic friction $\mu_{k}$. The board moves to the right at constant speed $v .$ Assume the block spends most of its time sticking to the board and moving to the right with it, so the speed $v$ is small in comparison to the average speed the block has as it slips back toward the left.
(a) Show that the maximum extension of the spring from its unstressed position is very nearly given by $\mu_{s} m g / k$. (b) Show that the block oscillates around an equilibrium position at which the spring is stretched by $\mu_{k} m g / k$. (c) Graph the block's position versus time. (d) Show that the amplitude of the block's motion is $A=\frac{\left(\mu_{s}-\mu_{k}\right) m g}{k}$ (e) Show that the period of the block's motion is
$$
T=\frac{2\left(\mu_{s}-\mu_{k}\right) m g}{v k}+\pi \sqrt{\frac{m}{k}}
$$
It is the excess of static over kinetic friction that is important for the vibration. "The squeaky wheel gets the grease" because even a viscous fluid cannot exert a force of static friction.

Jacob Schulze
Jacob Schulze
Numerade Educator
01:01

Problem 43

Your father is preparing the backyard for the installation of new sod. He has finished cleaning the ground of roots and rocks, has raked it to the correct contours, and now must pull a heavy roller, shown in Figure $\mathrm{P} 15.43 \mathrm{a}$, over the ground several times to flatten and compact the dirt. He is tired after all of his work and asks you to do the rolling for him. He tells you that each section of the yard must be rolled over ten times with the roller. You are tired from your physics studying, but decide you can use your understanding of physics to make the job easier. You attach the roller to a spring as shown in Figure $\mathrm{P} 15.43 \mathrm{~b},$ with the other end attached to a post pounded into the ground. You then just pull the roller out once and let it oscillate over each part of the yard for ten rolls while you sit back and relax. Before beginning, you wonder how much time you will have to relax at each location before you have to move the post and roller to a new location. The mass of the roller is $M=$ $400 \mathrm{~kg},$ and the spring constant is $k=3500 \mathrm{~N} / \mathrm{m} .$ The flat, smooth ground supplies enough friction that the roller rolls instead of sliding, but the rolling friction is negligible.

Dominador Tan
Dominador Tan
Numerade Educator
05:52

Problem 44

Why is the following situation impossible? Your job involves building very small damped oscillators. One of your designs involves a spring-object oscillator with a spring of force constant $k=10.0 \mathrm{~N} / \mathrm{m}$ and an object of mass $m=1.00 \mathrm{~g}$. Your design objective is that the oscillator undergo many oscillations as its amplitude falls to $25.0 \%$ of its initial value in a certain time interval. Measurements on your latest design show that the amplitude falls to the $25.0 \%$ value in $23.1 \mathrm{~ms}$ This time interval is too long for what is needed in your project. To shorten the time interval, you double the damping constant $b$ for the oscillator. This doubling allows you to reach your design objective.

Ren Jie Tuieng
Ren Jie Tuieng
Numerade Educator
09:13

Problem 45

block of mass $m$ is connected to two springs of force contants $k_{1}$ and $k_{2}$ in two ways as shown in Figure $\mathrm{P} 15.45$. In both cases, the block moves on a frictionless table after it is disblaced from equilibrium and released. Show that in the two ases the block exhibits simple harmonic motion with periods
(a) $T=2 \pi \sqrt{\frac{m\left(k_{1}+k_{2}\right)}{k_{1} k_{2}}}$ and
(b) $T=2 \pi \sqrt{\frac{m}{k_{1}+k_{2}}}$

Jacob Schulze
Jacob Schulze
Numerade Educator
08:16

Problem 46

A light balloon filled with helium of density $0.179 \mathrm{~kg} / \mathrm{m}^{3}$ is tied to a light string of length $L=3.00 \mathrm{~m}$ The string is tied to the ground forming an "inverted" simple pendulum (Fig. $\mathrm{P} 15.46 \mathrm{a}) .$ If the balloon is displaced slightly from equilibrium as in Figure $\mathrm{P} 15.46 \mathrm{~b}$ and released, (a) show that the motion is simple harmonic and (b) determine the period of the motion. Take the density of air to be $1.20 \mathrm{~kg} / \mathrm{m}^{3} .$ Hint: Use an analogy with the $\operatorname{sim}$ ple pendulum and see Chapter 14. Assume the air applies a buoyant force on the balloon but does not otherwise affect its motion.

Jacob Schulze
Jacob Schulze
Numerade Educator
07:38

Problem 47

A particle with a mass of $0.500 \mathrm{~kg}$ is attached to a horizontal spring with a force constant of $50.0 \mathrm{~N} / \mathrm{m}$. At the moment $t=0,$ the particle has its maximum speed of $20.0 \mathrm{~m} / \mathrm{s}$ and is moving to the left. (a) Determine the particle's equation of motion, specifying its position as a function of time. (b) Where in the motion is the potential energy three times the kinetic energy? (c) Find the minimum time interval required for the particle to move from $x=0$ to $x=$ $1.00 \mathrm{~m} .$ (d) Find the length of a simple pendulum with the same period.

Susan Hallstrom
Susan Hallstrom
Numerade Educator
12:21

Problem 48

A smaller disk of radius $r$ and mass $m$ is attached rigidly to the face of a second larger disk of radius $R$ and mass $M$ as shown in Figure $\mathrm{P} 15.48$. The center of the small disk is located at the edge of the large disk. The large disk is mounted at its center on a frictionless axle. The assembly is rotated through a small angle $\theta$ from its equilibrium position and released. (a) Show that the speed of the center of the small disk as it passes through the equilibrium position is
$$
v=2\left[\frac{\operatorname{Rg}(1-\cos \theta)}{(M / m)+(r / R)^{2}+2}\right]^{1 / 2}
$$
(b) Show that the period of the motion is
$$
T=2 \pi\left[\frac{(M+2 m) R^{2}+m r^{2}}{2 m g R}\right]^{1 / 2}
$$

Ren Jie Tuieng
Ren Jie Tuieng
Numerade Educator
10:30

Problem 49

A system consists of a spring with force constant $k=1250 \mathrm{~N} / \mathrm{m},$ length $L=1.50 \mathrm{~m},$ and an object of mass $m=5.00 \mathrm{~kg}$ attached to the end (Fig. $\mathrm{P} 15.49$ ). The object is placed at the level of the point of attachment with the spring unstretched, at position $y_{i}=L,$ and then it is released so that it swings like a pendulum. (a) Find the $y$ position of the object at the lowest point. (b) Will the pendulum's period be greater or less than the period of a simple pendulum with the same mass $m$ and length $L$ ? Explain.

Jacob Schulze
Jacob Schulze
Numerade Educator
08:55

Problem 50

Why is the following situation impossible? You are in the high-speed package delivery business. Your competitor in the next building gains the right-of-way to build an evacuated tunnel just above the ground all the way around the Earth. By firing packages into this tunnel at just the right speed, your competitor is able to send the packages into orbit around the Earth in this tunnel so that they arrive on the exact opposite side of the Earth in a very short time interval. You come up with a competing idea. Figuring that the distance through the Earth is shorter than the distance around the Earth, you obtain permits to build an evacuated tunnel through the center of the Earth (Fig. $\mathrm{P} 15.50$ ). By simply dropping packages into this tunnel, they fall downward and arrive at the other end of your tunnel, which is in a building right next to the other end of your competitor's tunnel. Because your packages arrive on the other side of the Earth in a shorter time interval, you win the competition and your business flourishes. Note: An object at a distance $r$ from the center of the Earth is pulled toward the center of the Earth only by the mass within the sphere of radius $r$ (the reddish region in Fig. $\mathrm{P} 15.50$ ). Assume the Earth has uniform density.

Ren Jie Tuieng
Ren Jie Tuieng
Numerade Educator
09:32

Problem 51

A light, cubical container of volume $a^{3}$ is initially filled with a liquid of mass density $\rho$ as shown in Figure P15.51a. The cube is initially supported by a light string to form a simple pendulum of length $L_{i}$ measured from the center of mass of the filled container, where $L_{i}>>$ a. The liquid is allowed to flow from the bottom of the container at a constant rate $(d M / d t)$. At any time $t,$ the level of the liquid in the container is $h$ and the length of the pendulum is $L$ (measured relative to the instantaneous center of mass) as shown in Figure $\mathrm{P} 15.51 \mathrm{~b}$.
(a) Find the period of the pendulum as a function of time.
(b) What is the period of the pendulum after the liquid completely runs out of the container?

Jacob Schulze
Jacob Schulze
Numerade Educator