Ch 05 HW
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Date
Apr 3, 2024
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Ch 05 HW
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Ch 05 HW
Due: 11:59pm on Tuesday, March 21, 2023
You will receive no credit for items you complete after the assignment is due. Grading Policy
Boat Statics
A boat owner pulls her boat into the dock shown, where there are six bollards to which to tie the boat.
She has three ropes. She can tie the boat from the boat's center (A) to any of the bollards (B through
G) along the dotted arrows shown.
Suppose the owner has tied three ropes: one rope runs to A from B, another to A from D, and a final
rope from A to F. The ropes are tied such that F
AB
=
F
AD
.
The following notation is used in this problem: When a question refers to, for example, →
F
AB
F_AB_vec
, this quantity is taken to mean the force acting on the boat
due to the rope running to A from B, while F
AB
F_AB
is the magnitude of that force.
Part A
What is the magnitude of the force provided by the third rope, in terms of θ
theta
?
Hint 1. Find the forces in the x
direction
What is the component of →
F
AB
F_AB_vec
in the x
direction (call it simply F
x
F_x
), in terms of F
AB
F_AB
and θ
theta
?
Positive x
is to the right in the diagram.
ANSWER:
Hint 2. Using algebra and trigonometry
Recalling that F
AB
=
F
AD
, you can find the x
component of the net force due to →
F
AB
F_AB_vec
and →
F
AD
F_AD_vec
. How does this relate to the force
provided by the third rope?
ANSWER:
Correct
F
x
=
−
F
AB
cos(
θ
)
F
AB
cos(
θ
)
2
F
AB
cos(
θ
)
2
F
AB
sin(
θ
)
F
AB
sin(
θ
)
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Atwood Machine Special Cases
shows an Atwood machine that consists of two blocks (of masses m
1
and m
2
) tied together with a
massless rope that passes over a fixed, perfect (massless and frictionless) pulley. In this problem
you'll investigate some special cases where physical variables describing the Atwood machine take
on limiting values. Often, examining special cases will simplify a problem, so that the solution may be
found from inspection or from the results of a problem you've already seen.
For all parts of this problem, take upward to be the positive direction and take the gravitational
constant, g
, to be positive.
Part A
Consider the case where m
1
and m
2
are both nonzero, and m
2
>
m
1
. Let T
1
be the magnitude of the tension in the rope connected to the block of mass m
1
,
and let T
2
be the magnitude of the tension in the rope connected to the block of mass m
2
. Which of the following statements is true?
ANSWER:
Correct
Part B
Now, consider the special case where the block of mass m
1
is not present. Find the magnitude, T
, of the tension in the rope. Try to do this without
equations; instead, think about the physical consequences.
Hint 1. How to approach the problem
If the block of mass m
1
is not present, and the rope connecting the two blocks is massless, will the motion of the block of mass m
2
be any different
from free fall?
Hint 2. Which physical law to use
Use Newton's 2nd law on the block of mass m
2
.
ANSWER:
Correct
Part C
T
1
is always equal to T
2
.
T
2
is greater than T
1
by an amount independent of velocity.
T
2
is greater than T
1
but the difference decreases as the blocks increase in velocity.
There is not enough information to determine the relationship between T
1
and T
2
.
T
= 0
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For the same special case (the block of mass m
1
not present), what is the acceleration of the block of mass m
2
?
Express your answer in terms of g
, and remember that an upward acceleration should be positive.
ANSWER:
Correct
Part D
Next, consider the special case where only the block of mass m
1
is present. Find the magnitude, T
, of the tension in the rope.
ANSWER:
Correct
Part E
For the same special case (the block of mass m
2
not present) what is the acceleration of the end of the rope where the block of mass m
2
would have been
attached?
Express your answer in terms of g
, and remember that an upward acceleration should be positive.
ANSWER:
Correct
Part F
Next, consider the special case m
1
=
m
2
=
m
. What is the magnitude of the tension in the rope connecting the two blocks?
Use the variable m
in your answer instead of m
1
or m
2
.
ANSWER:
Correct
Part G
For the same special case (
m
1
=
m
2
=
m
), what is the acceleration of the block of mass m
2
?
ANSWER:
Correct
Part H
Finally, suppose m
1
→ ∞
, while m
2
remains finite. What value does the the magnitude of the tension approach?
a
2
=
-9.80
T
= 0
a
2
=
9.80
T
=
mg
a
2
=
0
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Hint 1. Acceleration of block of mass m
1
As m
1
becomes large, the finite tension T
will have a neglible effect on the acceleration, a
1
. If you ignore T
, you can pretend the rope is gone without
changing your results for a
1
. As m
1
→ ∞
, what value does a
1
approach?
ANSWER:
Hint 2. Acceleration of block of mass m
2
As m
1
→ ∞
, what value will the acceleration of the block of mass m
2
approach?
ANSWER:
Hint 3. Net force on block of mass m
2
What is the magnitude F
net
of the net force on the block of mass m
2
.
Express your answer in terms of T
, m
2
, g
, and any other given quantities. Take the upward direction to be positive.
ANSWER:
ANSWER:
Correct
Imagining what would happen if one or more of the variables approached infinity is often a good way to investigate the behavior of a system.
Two Masses, a Pulley, and an Inclined Plane
Block 1, of mass m
1
m_1
, is connected over an ideal (massless and frictionless) pulley to block 2, of
mass m
2
m_2
, as shown. Assume that the blocks accelerate as shown with an acceleration of
magnitude a
a
and that the coefficient of kinetic friction between block 2 and the plane is μ
mu
.
Part A
Find the ratio of the masses m
1
/
m
2
.
a
1
=
-9.80
a
2
=
9.80
F
net
=
T
−
m
2
g
T
=
2
m
2
g
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Express your answer in terms of some or all of the variables a
a
, μ
mu
, and θ
theta
, as well as the magnitude of the free-fall acceleration g
g
.
Hint 1. Draw a free-body diagram
Which figure depicts the correct free-body diagrams for the blocks in this problem?
Figure a)
Figure b)
Figure c)
ANSWER:
a
b
c
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Hint 2. Apply Newton's 2nd law to block 2 in the direction parallel to the incline
What is Newton's 2nd law for block 2 in the direction parallel to the incline? (Assume the positive direction is going up the incline.)
Express your answer in terms of m
2
m_2
, T
T
, f
f
, and θ
theta
, as well as the magnitude of the free-fall acceleration g
g
.
ANSWER:
Hint 3. Find an expression for the friction force
What is the magnitude f
f
of the friction force acting on block 2?
ANSWER:
Hint 4. Find the normal force
By applying Newton's 2nd law to block 2 in the direction perpendicular to the incline determine the magnitude of the normal force n
n
.
Express your answer in terms of m
2
m_2
and θ
theta
, as well as the magnitude of the free-fall acceleration g
g
.
ANSWER:
Hint 5. Apply Newton's 2nd law to block 1 in the vertical direction
Write an expression for Newton's 2nd law in the vertical direction for block 1. Take the positive direction to point downward.
Express your answer in terms of the variables m
1
m_1
and/or T
T
, as well as the magnitude of the free-fall acceleration g
g
.
ANSWER:
Hint 6. Solve for the unknown tension T
T
Using your result from the previous hint, express T
T
in terms of g
g
, a
a
, and m
1
m_1
.
ANSWER:
Hint 7. Putting it all together
By applying Newton's law to both block 1 and block 2, as you did in Hints 2 and 4, you found two equations where the masses m
1
m_1
, m
2
m_2
, the
tension T
T
, and the acceleration a
a
, all appear, along with g
g
and θ
theta
. (Note that the friction force can be expressed in terms of the normal force,
which, in turn, can be written as m
2
g
cos(
θ
)
, as you found in Hint 3.) Choose one of the two equation and solve for T
T
; substitute this result into the
other equation. You will then have an equation with factors of m
1
m_1
and m
2
m_2
. You can then deduce the ratio.
ANSWER:
m
2
a
=
T
−
f
−
m
2
g
sin(
θ
)
f
=
n
/
μ
f
=
μ
/
n
f
=
μn
→
f
=
μ
→
n
n
n
=
m
2
g
cos(
θ
)
m
1
a
=
m
1
g
−
T
T
T
=
m
1
(
g
−
a
)
m
1
/
m
2
=
a
+ (
μ
cos
θ
+ sin
θ
)
g
g
−
a
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Contact Forces Introduced
Learning Goal:
To introduce contact forces (normal and friction forces) and to understand that, except for friction forces under certain circumstances, these forces must be
determined from: net Force = ma.
Two solid objects cannot occupy the same space at the same time. Indeed, when the objects touch, they exert repulsive normal
forces on each other, as well as
frictional
forces that resist their slipping relative to each other. These contact forces
arise from a complex interplay between the electrostatic forces between the
electrons and ions in the objects and the laws of quantum mechanics. As two surfaces are pushed together these forces increase exponentially over an atomic
distance scale, easily becoming strong enough to distort the bulk material in the objects if they approach too close. In everyday experience, contact forces are
limited by the deformation or acceleration of the objects, rather than by the fundamental interatomic forces. Hence, we can conclude the following:
The magnitude of contact forces is determined by ∑
→
F
=
m
→
a
, that is, by the other forces on, and acceleration of, the contacting bodies. The only exception is
that the frictional forces cannot exceed μn
(although they can be smaller than this or even zero).
Normal and friction forces
Two types of contact forces operate in typical mechanics problems, the normal
and frictional
forces, usually designated by n
n
and f
f
(or F
fric
F_fric
, or something
similar) respectively. These are the components of the overall contact force: n
n
perpendicular to and f
f
parallel to the plane of contact.
Kinetic friction when surfaces slide
When one surface is sliding past the other, experiments show three things about the friction force (denoted f
k
f_k
):
1. The frictional force opposes the relative motion at the point of contact,
2. f
k
f_k
is proportional to the normal force, and
3. the ratio of the magnitude of the frictional force to that of the normal force is fairly constant over a wide range of speeds.
The constant of proportionality is called the coefficient of kinetic friction
, often designated μ
k
mu_k
. As long as the sliding continues, the frictional force is then
f
k
=
μ
k
n
(valid when the surfaces slide by each other).
Static friction when surfaces don't slide
When there is no relative motion of the surfaces, the frictional force can assume any
value from zero up to a maximum μ
s
n
, where μ
s
mu_s
is the coefficient of
static friction
. Invariably, μ
s
mu_s
is larger than μ
k
mu_k
, in agreement with the observation that when a force is large enough that something breaks loose and
starts to slide, it often accelerates.
The frictional force for surfaces with no relative motion is therefore
f
s
≤
μ
s
n
(valid when the contacting surfaces have no relative motion).
The actual magnitude and direction of the static friction force are such that it (together with other forces on the object) causes the object to remain motionless
with respect to the contacting surface as long as the static friction force required does not exceed
μ
s
n
. The equation f
s
=
μ
s
n
is valid only
when the surfaces are on the verge of sliding.
Part A
When two objects slide by one another, which of the following statements about the force of friction between them, is true?
ANSWER:
The frictional force is always equal to μ
k
n
.
The frictional force is always less than μ
k
n
.
The frictional force is determined by other forces on the objects so it can be either equal to or less than μ
k
n
.
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Correct
Part B
When two objects are in contact with no relative motion, which of the following statements about the frictional force between them, is true?
ANSWER:
Correct
For static friction, the actual magnitude and direction of the friction force are such that it, together with any other forces present, will cause the
object to have the observed acceleration. The magnitude of the force cannot exceed μ
s
n
. If the magnitude of static friction needed to keep
acceleration equal to zero exceeds μ
s
n
, then the object will slide subject to the resistance of kinetic friction. Do not
automatically assume that
f
s
=
μ
s
n
unless you are considering a situation in which the magnitude of the static friction force is as large as possible (i.e., when determining at
what point an object will just begin to slip). Whether the actual magnitude of the friction force is 0, less than μ
s
n
, or equal to μ
s
n
depends on the
magnitude of the other forces (if any) as well as the acceleration of the object through ∑
→
F
=
m
→
a
.
Part C
When a board with a box on it is slowly tilted to larger and larger angle, common experience shows that the box will at some point "break loose" and start
to accelerate down the board.
The box begins to slide once the component of gravity acting parallel to the board F
g
F_g
just begins to exceeds the maximum force of static friction. Which
of the following is the most general explanation for why the box accelerates down the board?
ANSWER:
Correct
At the point when the box finally does "break loose," you know that the component of the box's weight that is parallel to the board just exceeds
μ
s
n
(i.e., this component of gravitational force on the box has just reached a magnitude such that the force of static friction, which has a maximum
value of μ
s
n
, can no longer oppose it.) For the box to then accelerate, there must be a net force on the box along the board. Thus, the
component of the box's weight parallel to the board must be greater than the force of kinetic friction. Therefore the force of kinetic friction μ
k
n
must be less than the force of static friction μ
s
n
which implies μ
k
<
μ
s
, as expected.
Part D
Consider a problem in which a car of mass M
M
is on a road tilted at an angle θ
theta
. The normal force
Select the best answer.
ANSWER:
The frictional force is always equal to μ
s
n
.
The frictional force is always less than μ
s
n
.
The frictional force is determined by other forces on the objects so it can be either equal to or less than μ
s
n
.
The force of kinetic friction is smaller than that of maximum static friction, but F
g
F_g
remains the same.
Once the box is moving, F
g
F_g
is smaller than the force of maximum static friction but larger than the force of kinetic friction.
Once the box is moving, F
g
F_g
is larger than the force of maximum static friction.
When the box is stationary, F
g
F_g
equals the force of static friction, but once the box starts moving, the sliding reduces the normal force, which
in turn reduces the friction.
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Correct
The key point is that contact forces must be determined from Newton's equation. In the problem described above, there is not enough information
given to determine the normal force (e.g., the acceleration is unknown). Each of the answer options is valid under some conditions (
θ
= 0
, the car
is sliding down an icy incline, or the car is going around a banked turn), but in fact none is likely to be correct if there are other forces on the car
or if the car is accelerating. Do not memorize values for the normal force valid in different problems--you must determine →
n
n_vec
from ∑
→
F
=
m
→
a
.
Centripetal Acceleration Explained
Learning Goal:
To understand that centripetal acceleration is the acceleration that causes motion in a circle.
Acceleration is the time derivative of velocity. Because velocity is a vector, it can change in two ways: the length (magnitude) can change and/or the direction
can change. The latter type of change has a special name, the centripetal acceleration
. In this problem we consider a mass moving in a circle of radius R
with
angular velocity ω
,
→
r
(
t
) =
R
cos(
ωt
)
ˆ
i
+ sin(
ωt
)
ˆ
j
=
R
cos(
ωt
)
ˆ
i
+
R
sin(
ωt
)
ˆ
j
.
The main point of the problem is to compute the acceleration using geometric arguments.
Part A
What is the velocity of the mass at a time t
? You can work this out geometrically with the help of the hints, or by differentiating the expression for →
r
(
t
)
given
in the introduction.
Express this velocity in terms of R
R
, ω
omega
, t
t
, and the unit vectors ˆ
i
i_unit
and ˆ
j
j_unit
.
n
=
Mg
n
=
Mg
cos(
θ
)
n
=
Mg
cos (
θ
)
is found using ∑
→
F
=
M
→
a
[
]
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Hint 1. Direction of the velocity
What is the angle between →
r
(
t
= 0)
and →
r
(
t
)
? As shown in the figure, this angle is directly related to the direction of the velocity vector. Keep in mind
that when t
= 0
, →
r
(
t
= 0) =
R
ˆ
i
.
Express your result in terms of quantities given in the problem introduction.
ANSWER:
Hint 2. Speed
What is v
(
t
)
, the speed (magnitude of velocity) of the mass at time t
?
Express v
(
t
)v(t)
in terms of ω
omega
and R
R
.
ANSWER:
ANSWER:
Correct
Assume that the mass has been moving along its circular path for some time. You start timing its motion with a stopwatch when it crosses the positive x
axis, an
instant that corresponds to t
= 0
. [Notice that when t
= 0
, →
r
(
t
= 0) =
R
ˆ
i
.] For the remainder of this problem, assume that the time t
is measured from the moment
you start timing the motion. Then the time −
t
refers to the moment a time t
before you start your stopwatch.
Part B
What is the velocity of the mass at a time −
t
?
Express this velocity in terms of R
R
, ω
omega
, t
t
, and the unit vectors ˆ
i
i_unit
and ˆ
j
j_unit
.
ANSWER:
Correct
Part C
What is the average acceleration of the mass during the time interval from −
t
to t
?
Express this acceleration in terms of R
R
, ω
omega
, t
t
, and the unit vectors ˆ
i
i_unit
and ˆ
j
j_unit
.
Hint 1. Average acceleration
θ
=
ωt
v
(
t
)
=
ωR
→
v
(
t
)
=
−
Rω
sin(
ωt
)
ˆ
i
+
Rω
cos(
ωt
)
ˆ
j
→
v
( −
t
)
=
Rω
sin(
ωt
)
ˆ
i
+
Rω
cos(
ωt
)
ˆ
j
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The definition of average acceleration over the interval from t
1
to t
2
is →
a
avg
[
t
1
,
t
2
] =
→
v
(
t
2
) −
→
v
(
t
1
)
t
2
−
t
1
.
ANSWER:
Correct
Part D
What is the magnitude of this acceleration in the limit of small t
? In this limit, the average acceleration becomes the instantaneous acceleration.
Express your answer in terms of R
R
and ω
omega
.
Hint 1. Expansion of sin(
x
)
For small times t
(or more precisely when ωt
1
), what is the first term in the Taylor series expansion for sin(
ωt
)
?
Express your answer in terms of ω
omega
and t
t
.
Hint 1. Taylor series expansion
The Taylor series expansion of sin(
x
)
is
sin
x
=
x
−
x
3
3 !
+
x
5
5 !
−
x
7
7 !
+ …
.
ANSWER:
ANSWER:
Correct
Part E
Consider the following statements:
a. The centripetal acceleration might better be expressed as −
ω
2
→
r
(
t
)
because it is a vector.
b. The magnitude of the centripetal acceleration is v
2
radial
/
R
.
c. The magnitude of the centripetal acceleration is v
2
tangential
/
R
.
d. A particle that is going along a path with local
radius of curvature R
at speed s
experiences a centripetal acceleration −
s
2
/
R
.
e. If you are in a car turning left, the force you feel pushing you to the right is the force that causes the centripetal acceleration.
In these statements v
radial
refers to the component of the velocity of an object in the direction toward or away from the origin of the coordinate system or the
rotation axis. Conversely, v
tangential
refers to the component of the velocity perpendicular to v
radial
.
Identify the statement or statements that are false
.
ANSWER:
→
a
avg
[ −
t
,
t
]
=
−
Rω
sin (
ωt
)
ˆ
i
t
sin(
ωt
)
=
ωt
a
centripetal
=
Rω
2
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Correct
That's right; the true statements are therefore:
a. The centripetal acceleration might better be expressed as −
ω
2
→
r
(
t
)
because it is a vector.
c. The magnitude of the centripetal acceleration is v
2
tangential
/
R
.
d. A particle that is going along a path with local
radius of curvature R
at speed s
experiences an acceleration −
s
2
/
R
.
There is so much confusion about centrifugal force that you should probably ban this term from your vocabulary and thought processes. If you
are in a car turning left, your centripetal acceleration is to the left (i.e., inward) and some real force must be applied to you to give you this
acceleration--typically this would be provided by friction with the seat. The force you "feel" pushing you to the right is not a real force but rather a
"fictitious force" that is present if you are in an accelerating coordinate system (in this case the car). It is best to stick to inertial (i.e.,
nonaccelerating) coordinate systems when doing kinematics and dynamics (i.e., →
F
=
m
→
a
calculations).
Video Tutor: Ball Leaves Circular Track
First, launch the video below. You will be asked to use your knowledge of physics to predict the outcome of an experiment. Then, close the video window and
answer the questions at right. You can watch the video again at any point.
Part A
Consider the video demonstration that you just watched. Which of the following changes would make it more likely for the ball to hit both the white can and
the green can?
Hint 1. How to approach the problem
To answer this question, you first have to decide whether changing the ball’s mass or its speed can change the path it follows after it leaves the
track.
Newton’s second law says that a net
force acting on the ball will change the ball’s motion—that is, its speed and/or direction. Newton’s first law says
that, in the absence of a net force, the ball’s motion won’t change.
After the ball leaves the track, does a net force act on it? Draw a free-body diagram for the ball if you’re not sure.
To hit the green can, the ball must continue following a curved path. What would be needed to make that happen?
a only
b only
c only
d only
e only
b and e
c and e
d and e
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ANSWER:
Correct
By Newton’s first law, after it has left the circular track, the ball will travel in a straight line until it is subject to a nonzero net force. Thus, the ball
can only hit the white can, because that is the only can in the ball’s straight-line path.
± Banked Frictionless Curve, and Flat Curve with Friction
A car of mass M
M
= 1500 kg
traveling at 45.0 km/hour
enters a banked turn covered with ice. The road is banked at an angle θ
, and there is no friction between
the road and the car's tires as shown in . Use g
g
= 9.80 m/s
2
throughout this problem.
Part A
What is the radius r
r
of the turn if θ
theta
= 20.0 (assuming the car continues in uniform circular motion around the turn)?
Express your answer in meters.
Hint 1. How to approach the problem
You need to apply Newton's 2nd law to the car. Because you do not want the car to slip as it goes around the curve, the car needs to have a net
acceleration of magnitude v
2
/
r
pointing radially inward (toward the center of the curve).
Hint 2. Identify the free-body diagram and coordinate system
Which of the following diagrams represents the forces acting on the car and the most appropriate choice of coordinate axes?
Use a ball that is lighter than the original ball, but still heavier than an empty can.
Use a ball that is heavier than the original ball.
Roll the ball faster.
Roll the ball slower.
None of the above
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ANSWER:
Hint 3. Calculate the normal force
Find n
n
, the magnitude of the normal force between the car and the road. Take the positive x
axis to point horizontally toward the center of the curve
and the positive y
axis to point vertically upward.
Express your answer in newtons.
Hint 1. Consider the net force
The only forces acting on the car are the normal force and gravity. There must be a net acceleration in the horizontal direction, but because
the car does not slip, the net acceleration in the vertical
direction must be zero. Use this fact to find n
n
.
Hint 2. Apply Newton's 2nd law to the car in the y
direction
Which equation accurately describes the equation for the net force acting on the car in the y
direction?
ANSWER:
ANSWER:
Hint 4. Determine the acceleration in the horizontal plane
Take the y
axis to be vertical and let the x
axis point horizontally toward the center of the curve. By applying ∑
F
x
=
Ma
x
in the horizontal direction,
determine a
a
, the magnitude of the acceleration, using your result for the normal force.
Express your answer in meters per second squared.
Hint 1. Apply Newton's 2nd law to the car in the x
direction
Which equation accurately describes the equation for the net force acting on the car in the x
direction?
Figure A
Figure B
Figure C
∑
F
y
=
n
cos
θ
+
Mg
∑
F
y
=
n
sin
θ
+
Mg
∑
F
y
=
n
cos
θ
−
Mg
∑
F
y
=
n
sin
θ
−
Mg
n
=
1.56×10
4
N
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ANSWER:
ANSWER:
ANSWER:
Correct
Part B
Now, suppose that the curve is level (
θ
= 0
) and that the ice has melted, so that there is a coefficient of static friction μ
mu
between the road and the car's
tires as shown in . What is μ
min
mu_min
, the minimum value of the coefficient of static friction
between the tires and the road required to prevent the car from slipping? Assume that the car's
speed is still 45.0 km/hour
and that the radius of the curve is 43.8 m
.
Express your answer numerically.
Hint 1. How to approach the problem
You need to apply Newton's 2nd law to the car. Because you do not want the car to slip as it goes around the curve, the car needs to have a net
acceleration of magnitude v
2
/
r
pointing radially inward (toward the center of the curve).
Hint 2. Identify the correct free-body diagram
∑
F
x
=
n
cos
θ
∑
F
x
=
n
sin
θ
∑
F
x
=
n
cos
θ
+
Mv
2
r
∑
F
x
=
n
cos
θ
−
Mv
2
r
a
= 3.57
m/s
2
r
= 43.8
m
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Which of the following diagrams represents the forces acting on the car as it goes around the curve? F
fr
F_fr
represents the friction force.
ANSWER:
Hint 3. Calculate the net force
What is the net force F
net
F_net
that acts on the car?
Express your answer in newtons.
Hint 1. How to determine the net force
Newton's 2nd law tells you that
∑
→
F
=
m
→
a
.
Because you do not want the car to slip as it goes around the curve, the car needs to have a net acceleration of magnitude v
2
/
r
pointing
radially inward (toward the center of the curve).
ANSWER:
Hint 4. Calculate the friction force
If the coefficient of friction were equal to μ
min
mu_min
, what would be F
fr
F_fr
, the magnitude of the force provided by friction? Let m
m
be the mass of
the car and g
g
be the acceleration due to gravity.
Hint 1. Equation for the force of friction
The force of friction is given by
F
fr
=
μn
.
Hint 2. Find the normal force
What is the normal force n
n
acting on the car?
Enter your answer in newtons.
Hint 1. Acceleration in the y
direction
Because the car is neither sinking into the road nor levitating, you can conclude that a
y
= 0
.
Figure A
Figure B
Figure C
Figure D
F
net
=
5350
N
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ANSWER:
ANSWER:
ANSWER:
Correct
Hanging Chandelier
A chandelier with mass m
m
is attached to the ceiling of a large concert hall by two cables. Because
the ceiling is covered with intricate architectural decorations (not indicated in the figure, which uses a
humbler depiction), the workers who hung the chandelier couldn't attach the cables to the ceiling
directly above the chandelier. Instead, they attached the cables to the ceiling near the walls. Cable 1
has tension T
1
T_1
and makes an angle of θ
1
theta_1
with the ceiling. Cable 2 has tension T
2
T_2
and
makes an angle of θ
2
theta_2
with the ceiling.
Part A
Find an expression for T
1
T_1
, the tension in cable 1, that does not depend on T
2
T_2
.
Express your answer in terms of some or all of the variables m
m
, θ
1
theta_1
, and θ
2
theta_2
, as well as the magnitude of the acceleration due to
gravity g
g
. You must use parentheses around θ
1
theta_1
and θ
2
theta_2
, when they are used as arguments to any trigonometric functions in your
answer.
Hint 1. Find the sum of forces in the x
direction
The chandelier is static; hence the vector forces on it sum to zero. Type in the sum of the x
components of the forces acting on the chandelier, using
the coordinate system shown.
Express your answer in terms of some or all of the variables m
m
, T
1
T_1
, T
2
T_2
, θ
1
theta_1
, and θ
2
theta_2
. You must use parentheses around
θ
1
theta_1
and θ
2
theta_2
, when they are used as arguments to any trigonometric functions in your answer.
n
n
=
1.47×10
4
N
F
fr
=
μ
min
Mg
F
fr
=
μ
min
Mg
μ
min
=
0.364
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ANSWER:
Hint 2. Find the sum of forces in the y
direction
Now type the corresponding equation relating the y
components of the forces acting on the chandelier, again using the coordinate system shown.
Express your answer in terms of some or all of the variables m
m
, T
1
T_1
, T
2
T_2
, θ
1
theta_1
, and θ
2
theta_2
, as well as the magnitude of the
acceleration due to gravity g
g
. You must use parentheses around θ
1
theta_1
and θ
2
theta_2
, when they are used as arguments to any
trigonometric functions in your answer.
ANSWER:
Hint 3. Putting it all together
There are two unknowns in this problem, T
1
T_1
and T
2
T_2
. Each of the previous two hints leads you to an equation involving these two unknowns.
Eliminate T
2
T_2
from this pair of equations and solve for T
1
T_1
.
ANSWER:
Correct
Exercise 5.18 - Enhanced - with Feedback
A transport plane takes off from a level landing field with two gliders in tow, one behind the other. The mass of each glider is 700 kg
, and the total resistance (air
drag plus friction with the runway) on each may be assumed constant and equal to 2500 N
. The tension in the towrope between the transport plane and the first
glider is not to exceed 12000 N
.
Part A
If a speed of 40 m/s
is required for takeoff, what minimum length of runway is needed?
Express your answer in meters to two significant figures.
ANSWER:
∑
F
x
= 0
=
T
2
cos
θ
2
−
T
1
cos
θ
1
(
)
(
)
∑
F
y
= 0
=
T
1
sin
θ
1
+
T
2
sin
θ
2
−
mg
(
)
(
)
T
1
=
mg
sin
θ
1
+ cos
θ
1
tan
θ
2
(
)
(
)
(
)
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Correct
Part B
What is the tension in the towrope between the two gliders while they are accelerating for the takeoff?
Express your answer in newtons.
ANSWER:
Correct
PSS 5.2 Newton’s Second Law: Dynamics of Particles
Learning Goal:
To practice Problem-Solving Strategy 5.2 Newton’s Second Law: Dynamics of Particles.
You want to move a heavy box with mass 30.0 kg
across a carpeted floor. You pull hard on one of the edges of the box at an angle 30
above the horizontal
with a force of magnitude 240 N
, causing the box to move horizontally. The force of friction between the moving box and the floor has magnitude 41.5 N
. What
is the box's acceleration just after it begins to move?
Problem-Solving Strategy: Newton’s second law—Dynamics of particles
IDENTIFY the relevant concepts:
Identify the target variable—usually an acceleration or a force. If the target variable is velocity, time, or distance, you will use Newton's second law to find the
acceleration and then use kinematics to find the target variable.
SET UP the problem using the following steps:
1. Draw a simple sketch of the situation. Identify one or more moving bodies to which you’ll apply Newton’s second law.
2. For each body you identified, draw a free-body diagram that shows all the forces acting on the body.
3. Label each force with an algebraic symbol for the force’s magnitude
.
4. Choose your x
and y
coordinate axes for each body, and show them in that body's free-body diagram.
5. If more than one body is involved, there may be relationships among their motions; for example, they may be connected by a rope. Express any
such relationships as equations relating the accelerations of the various bodies.
EXECUTE the solution as follows:
1. For each object, determine the components of the forces along each of the object’s coordinate axes.
2. For each object, write a separate equation for each component of Newton’s second law, Σ
F
x
=
ma
x
and Σ
F
y
=
ma
y
.
3. Make a list of all the known and unknown quantities. In your list, identify the target variable or variables.
4. Check that you have as many equations as there are unknowns. If you have too few equations, go back to Step 5 of “Set up the problem".
5. Do the easy part—the math! Solve the equations to find the target variable(s).
EVALUATE your answer:
Does your answer have the correct units? Does it have the correct algebraic sign? When possible, consider particular values or extreme cases of quantities
and compare the results with your intuitive expectations. Ask, “Does this result make sense?”
IDENTIFY the relevant concepts
The target variable in this problem is the acceleration of the box. Since you know the magnitudes and directions of all of the forces, you can use Newton's
second law to find the acceleration.
SET UP the problem using the following steps
Part A
The figure shows the situation described. Which of the following describes the best coordinate system? You should generally align the positive x
axis with
the direction in which your object of interest is accelerating.
160
m
6000
N
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ANSWER:
Correct
Part B
Draw a free-body diagram for the box in accordance with the coordinate system decided in Part A. The box may be treated as a point particle. The black
dot in the figure represents the box.
Draw the vectors starting at the black dot. The location and orientation of the vectors will be graded. The length of the vectors will not be
graded.
ANSWER:
Positive x
axis to the left, positive y
axis upward
Positive x
axis to the left, positive y
axis downward
Positive x
axis to the right, positive y
axis upward
Positive x
axis to the right, positive y
axis downward
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Correct
EXECUTE the solution as follows
Part C
Find both the x
and y
components of the acceleration of the box.
Enter the x
and y
components of the acceleration in meters per second squared, separated by commas.
Hint 1. Find the x component of the pulling force
The pulling force →
F
p
F_p_vec
points in a direction 30
above the positive x
axis. Use this to determine the value of F
px
F_px
, the x
component of the
pulling force.
Express your answer in newtons.
ANSWER:
Hint 2. Find the y
component of the pulling force
The pulling force →
F
p
F_p_vec
points in a direction 30
above the positive x
axis. Use this to determine the value of F
py
F_py
, the y
component of the
pulling force.
Express your answer in newtons.
ANSWER:
No elements selected
F
px
F_px
=
208
N
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Hint 3. Find the magnitude of the weight
You know that the mass of the box is 30.0 kg
and that g
g
= 9.80 m/s
2
. Use this information to calculate the magnitude w
w
of the weight of the box.
Express your answer in newtons.
ANSWER:
Hint 4. Set up Newton's second law for the x
direction
Newton's second law states that Σ
F
x
=
ma
x
. Write an expression for Σ
F
x
in terms of the forces acting on the box. Use f
f
, n
n
, and w
w
for the
magnitudes of the friction force, the normal force, and the weight, respectively. Use F
px
F_px
and F
py
F_py
for the magnitudes of the x
and the y
components of the pulling force, respectively.
Express your answer in terms of some or all of the variables F
px
F_px
, F
py
F_py
, f
f
, n
n
, and w
w
.
ANSWER:
Hint 5. Newton's second law in the y
direction
You are told that the box moves horizontally, which means that the acceleration in the y
direction must be zero. Therefore, from Newton's second
law in the y
direction, you see that the net force in the y
direction must also be zero.
As long as the upward component F
py
F_py
of the pulling force has a smaller magnitude than the weight (which is true in this case), the normal force
will take a value that leads to a net force of zero in the y
direction.
The preceding paragraphs explain why both sides of Σ
F
y
=
ma
y
are zero.
ANSWER:
Correct
EVALUATE your answer
Part D
A normal walking speed is around 2.0 m/s
. How much time t
t
does it take the box to reach this speed if it has the acceleration 5.54 m/s
2
that you
calculated above?
Express your answer in seconds to two significant figures.
ANSWER:
Correct
This time should match roughly to your experience with pulling boxes or furniture around. If you found a time longer than 10 s
, you should be
skeptical of your work, since it would generally not take you so long to get a box up to a normal walking pace. Note that once you get up to a
normal walking pace, you generally reduce the force you exert so that it is just enough to balance the force of friction. In this way, the box will
continue to move with you at a comfortable pace.
Board Pulled Out from under a Box
F
py
F_py
= 120
N
w
w
= 294
N
Σ
F
x
=
F
px
−
f
=
ma
x
a
x
a_x
,
a
y
a_y
=
5.54,0
m/s
2
, m/s
2
t
t
= 0.36
s
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A small box of mass m
1
m_1
is sitting on a board of mass m
2
m_2
and length L
L
. The board rests on a
frictionless horizontal surface. The coefficient of static friction between the board and the box is
μ
s
mu_s
. The coefficient of kinetic friction between the board and the box is, as usual, less than μ
s
mu_s
.
Throughout the problem, use g
g
for the magnitude of the free-fall acceleration. In the hints, use f
for
the magnitude of the friction force between the board and the box.
Part A
Find F
min
F_min
, the constant force with the least magnitude that must be applied to the board in order to pull the board out from under the the box (which
will then fall off of the opposite end of the board).
Express your answer in terms of some or all of the variables μ
s
mu_s
, m
1
m_1
, m
2
m_2
, g
g
, and L
L
. Do not
include f
in your answer.
Hint 1. Condition for the board sliding out from under the box
The board will slide out from under the box if the magnitude of the board's acceleration exceeds the magnitude of the maximum acceleration that
friction can give to the box.
Hint 2. Find the acceleration of the box in terms of f
Assume that the coefficient of static friction between the board and the box is not known at this point. What is the magnitude of the acceleration of
the box in terms of the friction force f
?
Express your answer in terms of f
and m
1
m_1
.
ANSWER:
Hint 3. Find the largest acceleration of the box
Now take the coefficient of static friction between the board and the box to be μ
s
mu_s
. What is the largest possible magnitude of the acceleration of
the box?
Express your answer in terms of some or all of the variables μ
s
mu_s
, g
g
, and m
1
m_1
.
Hint 1. Maximum force on the box
Friction is the only horizontal force on the box. What is the largest possible value for f
f
?
ANSWER:
Hint 4. Find the sum of horizontal forces on the board
Write down the sum of all the horizontal forces acting on the board. Take the positive x
direction to be to the right.
Give your answer in terms of F
F
, f
, and any constants necessary.
Hint 1. Friction and Newton's 3rd law
Remember, by Newton's 3rd law, if there is a force of magnitude f
f
acting on the box due to the board, there is a force of equal magnitude
and opposite direction acting on the board due to the box.
a
box
a_box
=
f
m
1
a
box
a_box
=
μ
s
g
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ANSWER:
Hint 5. Find the acceleration of the board for large f
In Hint 4 you found the net horizontal force on the board. Now, find the acceleration of the board when the force of static friction reaches its
maximum possible value.
Express your answer in terms of F
F
, μ
s
mu_s
, m
1
m_1
, m
2
m_2
, and g
g
.
ANSWER:
Hint 6. Putting it all together
Reread Hint 1. In Hint 3, you found the largest possible acceleration of the box, a
box
a_box
. In Hint 5, you found the acceleration of the board,
a
board
a_board
. What is the minimum value of the constant force, F
min
F_min
, so that a
board
>
a
box
?
ANSWER:
Correct
Exercise 5.34 - Enhanced - with Feedback
Consider the system shown in the figure . Block A
weighs 44.3 N
and block B
weighs 30.2 N
. Once
block B
is set into downward motion, it descends at a constant speed.
Part A
Calculate the coefficient of kinetic friction between block A
and the tabletop.
ANSWER:
Correct
∑
F
x
=
F
−
f
a
board
a_board
=
F
−
μ
s
m
1
g
m
2
|
|
|
|
F
min
F_min
=
m
1
+
m
2
μ
s
g
(
)
μ
= 0.682
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Part B
A cat, also of weight 44.3 N
, falls asleep on top of block A
. If block B
is now set into downward motion, what is its acceleration magnitude?
Express your answer in meters per second squared.
ANSWER:
Correct
Part C
A cat, also of weight 44.3 N
, falls asleep on top of block A
. If block B
is now set into downward motion, what is its acceleration direction?
ANSWER:
Correct
Exercise 5.54 - Enhanced - with Feedback
The Cosmoclock 21 Ferris wheel in Yokohama City, Japan, has a diameter of 100 m
. Its name comes from its 60 arms, each of which can function as a second
hand (so that it makes one revolution every 60.0 s
).
Part A
Find the speed of the passengers when the Ferris wheel is rotating at this rate.
Express your answer in meters per second.
ANSWER:
Correct
Part B
A passenger weighs 902 N
at the weight-guessing booth on the ground. What is his apparent weight at the lowest point on the Ferris wheel?
Express your answer in newtons.
ANSWER:
Correct
Part C
What is his apparent weight at the highest point on the Ferris wheel?
Express your answer in newtons.
ANSWER:
a
= 2.49
m/s
2
upwards
downwards
v
= 5.2
m/s
w
lowest
=
950
N
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Correct
Part D
What would be the time for one revolution if the passenger's apparent weight at the highest point were zero?
Express your answer in seconds.
ANSWER:
Correct
Part E
What then would be the passenger's apparent weight at the lowest point?
Express your answer in newtons.
ANSWER:
Correct
Normal Force and Centripetal Force Ranking Task
A roller-coaster track has six semicircular "dips" with different radii of curvature. The same roller-coaster cart rides through each dip at a different speed.
Part A
For the different values given for the radius of curvature R
R
and speed v
v
, rank the magnitude of the force of the roller-coaster track on the cart at the
bottom of each dip.
Rank from largest to smallest. To rank items as equivalent, overlap them.
Hint 1. Newton’s 2nd law
Newton’s 2nd law is valid for any motion, whether the motion is along a straight line or a circular path. The net force acting on the cart must be equal
to the product of its mass and acceleration,
w
highest
= 850
N
t
= 14
s
w
lowest
= 1800
N
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∑
→
F
=
m
→
a
,
and since the cart is moving along a circular path, its acceleration (toward the center of the circular path) is given by
a
=
v
2
R
.
Hint 2. Determine the net force on the cart
Defining up as the positive direction, which of the following expressions describes the net force acting on the cart in the vertical direction while it's at
the bottom of the dip? The variables F
gravity
F_gravity
and F
track
F_track
are the magnitudes of the forces.
ANSWER:
ANSWER:
Correct
Problem 5.84 - Enhanced - with Feedback
Part A
If the coefficient of static friction between a table and a uniform massive rope is μ
s
, what fraction of the rope can hang over the edge of the table without the
rope sliding?
Express your answer in terms of μ
s
mu_s
.
∑
F
=
F
gravity
+
F
track
∑
F
=
F
gravity
−
F
track
∑
F
= −
F
track
−
F
gravity
∑
F
=
F
track
−
F
gravity
Reset
Help
The correct ranking cannot be determined.
R
= 30 m
v
= 16 m/s
R
= 15 m
v
= 8 m/s
R
= 15 m
v
= 12 m/s
R
= 30 m
v
= 4 m/s
R
= 60 m
v
= 16 m/s
R
= 45 m
v
= 4 m/s
smallest
largest
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ANSWER:
Correct
Problem 5.110 - Enhanced - with Feedback
A road heading due east passes over a small hill. You drive a car of mass m
at constant speed v
over the top of the hill, where the shape of the roadway is well
approximated as an arc of a circle with radius R
. Sensors have been placed on the road surface there to measure the downward force that cars exert on the
surface at various speeds. The table gives values of this force versus speed for your car is shown in the table below. Treat the car as a particle.
Speed (
m/s
)
6.00
8.00
10.0
12.0
14.0
16.0
Force (
N
)
8100
7690
7050
6100
5200
4200
Part A
Select a way to represent the data as a straight line. You might need to raise the speed, the force, or both to some power.
ANSWER:
Correct
Part B
Select the correct graph with the equation for the straight line that is the best fit to the data points described in the previous part.
ANSWER:
r
=
μ
s
1 +
μ
s
n
vs. v
2
n
2
vs. v
n
vs. v
n
2
vs. v
2
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.
.
.
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Correct
Part C
Use the graph to calculate m
.
Express your answer with the appropriate units.
ANSWER:
Correct
Part D
Use the graph to calculate R
.
Express your answer with the appropriate units.
ANSWER:
Correct
Part E
What maximum speed can the car have at the top of the hill and still not lose contact with the road?
Express your answer with the appropriate units.
ANSWER:
Correct
Key Example Variation Problem 5.5
Be sure to review Example 5.5 (Section 5.1) before attempting these problems. In all problems, ignore air resistance.
VP 5.5.1
Part A
In a modified version of the cart and bucket in , the angle of the slope is α
alpha_1
= 36.9 and the bucket weighs 295 N
. The cart moves up the incline and
the bucket moves downward, both at constant speed. The cable has negligible mass, and there is no friction. What is the weight of the cart?
Express your answer with the appropriate units.
.
m
= 897 kg
R
= 49.6 m
v
= 22.0 m
s
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ANSWER:
Correct
Part B
What is the tension in the cable?
Express your answer with the appropriate units.
ANSWER:
Correct
VP 5.5.2
Part C
You change the angle of the slope in a to 26.0 and use a different cart and a different bucket.
You observe that the cart and bucket remain at rest when released and that the tension in the
cable of negligible mass is 155 N
. There is no friction.What is the weight of the cart?
Express your answer with the appropriate units.
ANSWER:
Correct
Part D
What is the combined
weight of the cart and bucket?
w
cart 1
=
491 N
T
1
= 295 N
w
cart 2
=
354 N
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Express your answer with the appropriate units.
ANSWER:
Correct
VP 5.5.3
Part E
You construct a version of the cart and bucket in , but with a slope whose angle can be adjusted.
You use a cart of mass 185 kg
and a bucket of mass 59.0 kg
. The cable has negligible mass,
and there is no friction. What must be the angle of the slope so that the cart moves downhill at a
constant speed and the bucket moves upward at the same constant speed?
Express your answer in degrees.
ANSWER:
Correct
Part F
With this choice of angle, what will be the tension in the cable?
Express your answer with the appropriate units.
ANSWER:
Correct
VP 5.5.4
Part G
In the situation shown in , let α
be the angle of the slope and suppose there is
friction between the cart and the track. You find that if the cart and bucket
each have the same weight w
, they remain at rest when released. In this case, what is the magnitude of the friction force on the cart?
Express your answer in terms of α
alpha
and w
w
.
w
combined
=
509 N
θ
3
= 18.6
T
3
=
578 N
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ANSWER:
Correct
Part H
Is the friction force less than, greater than, or equal to w
?
ANSWER:
Correct
Key Example Variation Problem 5.15
Be sure to review Examples 5.13, 5.14, and 5.15 (Section5.3) before attempting these problems.
VP 5.15.1
Part A
You pull on a crate using a rope as in , except the rope is at an angle of 20.0 above the
horizontal. The weight of the crate is 325 N
, and the coefficient of kinetic friction between the
crate and the floor is 0.250. What must be the tension in the rope to make the crate move at a
constant velocity?
Express your answer with the appropriate units.
ANSWER:
f
=
w
(1 − sin
α
)
f
=
w
f
>
w
f
<
w
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Correct
Part B
What is the normal force that the floor exerts on the crate?
Express your answer with the appropriate units.
ANSWER:
Correct
VP5.15.2
Part C
You pull on a large box using a rope as in , except the rope is at an angle of 15.0
below
the
horizontal. The weight of the box is 325 N
, and the coefficient of kinetic friction between the box
and the floor is 0.250. What must be the tension in the rope to make the box move at a constant
velocity?
Express your answer with the appropriate units.
ANSWER:
Correct
Part D
What is the normal force that the floor exerts on the box?
Express your answer with the appropriate units.
ANSWER:
Correct
VP 5.15.3
Part E
You are using a lightweight rope to pull a sled along level ground. The sled weighs 435 N
, the coefficient of kinetic friction between the sled and the ground
is 0.200, the rope is at an angle of 12
above the horizontal, and you pull on the rope with a force of 125 N
. Find the normal force that the ground exerts on
the sled.
T
1
= 79.3 N
n
1
=
298 N
T
2
=
90.2 N
n
2
=
348 N
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Express your answer with the appropriate units.
ANSWER:
Correct
Part F
Find the acceleration of the sled. Is the sled speeding up or slowing down?
Express your answer with the appropriate units. Enter positive value if the sled is speeding up and negative value if the sled is slowing down.
ANSWER:
Correct
VP 5.15.4
Part G
A large box of mass m
sits on a horizontal floor. You attach a lightweight rope to this box, hold the rope at an angle θ
above the horizontal, and pull. You find
that the minimum tension you can apply to the rope in order to make the box start moving is T
min
. Find the coefficient of static friction between the floor and
the box.
Express your answer in terms of the variables m
m
, θ
theta
, T
min
T_min
, and acceleration due to gravity g
g
.
ANSWER:
Correct
Key Example Variation Problem 5.22
Be sure to review Examples 5.20, 5.21, and 5.22 (Section 5.4) before attempting these problems.
VP 5.22.1
Part A
You make a conical pendulum using a string of length 0.900 m
and a bob of mass 0.450 kg
. When the bob is moving in a circle at a constant speed, the
string is at an angle of 30.0 from the vertical. What is the radius of the circle around which the bob moves?
Express your answer with the appropriate units.
n
= 409 N
a
= 0.91 m
s
2
μ
s
=
T
min
cos
θ
mg
−
T
min
sin
θ
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ANSWER:
Correct
Part B
How much time does it take the bob to complete one circle?
Express your answer with the appropriate units.
ANSWER:
Correct
Part C
What is the tension in the string?
Express your answer with the appropriate units.
ANSWER:
Correct
VP 5.22.2
Part D
A competition cyclist rides at a constant 12.5 m/s
around a curve that is banked at 38.0 . The cyclist and her bicycle have a combined mass of 69.0 kg
.
What must be the radius of her turn if there is to be no friction force pushing her either up or down the banked curve?
Express your answer with the appropriate units.
ANSWER:
Correct
Part E
R
= 0.450 m
t
= 1.77 s
T
= 5.09 N
R
= 20.4 m
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What is the magnitude of her acceleration?
Express your answer with the appropriate units.
ANSWER:
Correct
Part F
What is the magnitude of the normal force that the surface of the banked curve exerts on the bicycle?
Express your answer with the appropriate units.
ANSWER:
Correct
VP 5.22.3
Part G
An aerobatic airplane flying at a constant 60.0 m/s
makes a horizontal turn of radius 275 m
. The pilot has mass 80.0 kg
. What is the bank angle of the
airplane?
Express your answer in degrees.
ANSWER:
Correct
Part H
What is the pilot's apparent weight during the turn?
Express your answer with the appropriate units.
ANSWER:
Correct
Part I
How many times greater than his actual weight is this?
ANSWER:
Correct
VP 5.22.4
a
rad
=
7.66 m
s
2
n
= 858 N
β
b
=
53.2
n
= 1310 N
n
/
w
= 1.67
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Part J
A sports car moves around a banked curve at just the right constant speed v
so that no friction is needed to make the turn. During the turn, the driver
(mass m
) feels as though she weighs x
times her actual weight. Find the magnitude of the net
force on the driver during the turn in terms of m
, g
, and x
.
Express your answer in terms of the variables m
m
, x
x
, and acceleration due to gravity g
g
.
ANSWER:
Correct
Part K
Find the radius of the turn.
Express your answer in terms of the variables v
v
, x
x
, and acceleration due to gravity g
g
.
ANSWER:
Correct
Exercise 5.15 - Enhanced - with Solution
A load of bricks with mass m
1
m_1
= 15.0 kg
hangs from one end of a rope that passes over a small, frictionless pulley. A counterweight of mass
m
2
m_2
= 31.0 kg
is suspended from the other end of the rope, as shown in . The system is released
from rest.
For related problem-solving tips and strategies, you may want to view a Video Tutor Solution of Two
bodies with the same magnitude of acceleration
.
Part A
Draw a free-body diagram for the load of bricks.
Draw the vectors starting at the black dot. The location, orientation, and relative length of the vectors will be graded. The exact length of the
vectors will not be graded.
ANSWER:
F
net
=
mg
√
x
2
− 1
r
=
v
2
g
√
x
2
− 1
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Correct
Part B
Draw a free-body diagram for the counterweight.
Draw the vectors starting at the black dot. The location, orientation, and relative length of the vectors will be graded. The exact length of the
vectors will not be graded.
ANSWER:
No elements selected
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Correct
Part C
What is the magnitude of the upward acceleration of the load of bricks?
Express your answer with the appropriate units.
ANSWER:
Correct
Part D
What is the tension in the rope while the load is moving?
Express your answer with the appropriate units.
ANSWER:
Correct
Part E
No elements selected
a
= 3.41 m
s
2
T
= 198 N
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How does the tension compare to the weight of the load of bricks? To the weight of the counterweight?
Drag the terms on the left to the appropriate blanks on the right to complete the sentence.
ANSWER:
Correct
Exercise 5.46 - Enhanced - with Feedback
A small car with mass 0.640 kg
travels at constant speed on the inside of a track that is a vertical circle with radius 5.00 m
.
Part A
If the normal force exerted by the track on the car when it is at the top of the track (point B
) is 6.00 N
, what is the normal force on the car when it is at the
bottom of the track (point A
)?
Express your answer with the appropriate units.
ANSWER:
Correct
Exercise 5.39 - Enhanced - with Solution
As shown in , block A
(mass 2.22 kg
) rests on a tabletop. It is connected by a horizontal cord passing over a light, frictionless pulley to a hanging block B
(mass
1.28 kg
). The coefficient of kinetic friction between block A
and the tabletop is 0.448. The blocks are released then from rest.
For related problemsolving tips and strategies, you may want to view a Video Tutor Solution of Friction in horizontal motion
.
Reset
Help
smaller than
greater than
The tension in the rope is greater than
the
weight of the load of bricks and smaller than
the weight of the counterweigh.
F
= 18.5 N
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Part A
Draw the free-body diagram for block A
.
Draw the force vectors with their tails at the center of the block A. The location and orientation of your vectors will be graded. The exact length
of your vectors will not be graded but the relative length of one to the other will be graded.
ANSWER:
No elements selected
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Correct
IDENTIFY: Apply Σ
→
F
=
m
→
a
to each block. The target variables are the tension T
in the cord and the acceleration a
of the blocks. Then a
can be
used in a constant acceleration equation to find the speed of each block. The magnitude of the acceleration is the same for both blocks.
SET UP: The system is sketched in the figure below.
For each block take a positive coordinate direction to be the direction of the block’s acceleration.
block on the table: The free-body is sketched in the figure below
EXECUTE:
Σ
F
y
=
ma
y
n
−
m
A
g
= 0
n
=
m
A
g
f
k
=
μ
k
n
=
μ
k
m
A
g
Σ
F
x
=
ma
x
T
−
f
k
=
m
A
a
T
−
μ
k
m
A
g
=
m
A
a
Part B
Draw the free-body diagram for block B
.
Draw the force vectors with their tails at the center of the block B. The location and orientation of your vectors will be graded. The exact length
of your vectors will not be graded but the relative length of one to the other will be graded.
ANSWER:
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SET UP: hanging block: The free-body is sketched in the figure below.
EXECUTE:
Σ
F
y
=
ma
y
m
B
g
−
T
=
m
B
a
T
=
m
B
g
−
m
B
a
Use the second equation in the first
m
B
g
−
m
B
a
−
μ
k
m
A
g
=
m
A
a
(
m
A
+
m
B
)
a
= (
m
B
−
μ
k
m
A
)
g
a
=
(
m
B
−
μ
k
m
A
)
g
m
A
+
m
B
=
( 1.28 kg − ( 0.448 ) ( 2.22 kg ) ) ( 9.80 m / s
2
)
2.22 kg + 1.28 kg
= 0.7992 m/s
2
Part C
No elements selected
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Find the speed of each block after moving 2.30 cm
.
Express your answer in meters per second.
ANSWER:
Correct
SET UP: Now use the constant acceleration equations to find the final speed. Note that the blocks have the same speeds. x
−
x
0
= 0.0230 m
,
a
x
= 0.7992 m/s
2
, v
0
x
= 0
, v
x
= ?
v
2
x
=
v
2
0
x
+ 2
a
x
(
x
−
x
0
)
EXECUTE: v
x
=
2
a
x
(
x
−
x
0
) =
√
2(0.7992 m/s
2
)(0.0230 m) = 0.192 m/s = 19.2 cm/s
.
Part D
Find the tension in the cord.
Express your answer in newtons.
ANSWER:
Correct
T
=
m
B
g
−
m
B
a
=
m
B
(
g
−
a
) = 1.28 kg(9.80 m/s
2
− 0.7992 m/s
2
) = 11.5 N
Or, to check, T
−
μ
k
m
A
g
=
m
A
a
.
T
=
m
A
(
a
+
μ
k
g
) = 2.22 kg(0.7992 m/s
2
+ (0.448)(9.80 m/s
2
)) = 11.5 N
, which checks.
EVALUATE: The force T
exerted by the cord has the same value for each block. T
<
m
B
g
since the hanging block accelerates downward. Also,
f
k
=
μ
k
m
A
g
= 9.75 N
. T
>
f
k
and the block on the table accelerates in the direction of T
.
Exercise 5.56
A 51.0 kg
stunt pilot who has been diving her airplane vertically pulls out of the dive by changing her course to a circle in a vertical plane.
Part A
If the plane's speed at the lowest point of the circle is 95.0 m/s
, what is the minimum radius of the circle so that the acceleration at this point will not exceed
4.00
g
?
Express your answer with the appropriate units.
ANSWER:
Correct
Part B
What is the apparent weight of the pilot at the lowest point of the pullout?
Express your answer with the appropriate inits.
ANSWER:
v
= 0.19
m/s
√
T
= 12
N
R
= 230 m
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Problem 5.60 - Enhanced - with Hints
An adventurous archaeologist crosses between two rock cliffs by slowly going hand-over-hand along a rope stretched between the cliffs. He stops to rest at the
middle of the rope . The rope will break if the tension in it exceeds 2.60×10
4
N
, and our hero's mass
is 85.4 kg
.
You may want to review (Page) .
For help with math skills, you may want to review:
Vector Components
For general problem-solving tips and strategies for this topic, you may want to view a Video Tutor
Solution of Two dimensional equilibrium
.
Part A
If the angle between the rope and the horizontal is θ
theta
= 10.5 , find the tension in the rope.
Express your answer in newtons.
Hint 1. How to approach the problem
Start by drawing a diagram with the forces acting on the person, as he rests at the middle of the rope. Create an xy
coordinate system that best
matches the forces and angles on the diagram.
Consider that the suspended person is in equilibrium in both the x
and y
directions and that a tension is exerted by each half of the rope on either
side of the person.
Use this information, and apply Newton's 1st law in both the x
and y
directions separately. Then, solve for the tension in the rope.
ANSWER:
Correct
Part B
What is the smallest value the angle θ
can have if the rope is not to break?
Express your answer in degrees.
Hint 1. How to approach the problem
From Part A, you obtained an expression for the tension in the rope for a given angle θ
. Use this expression in conjunction with the value given for
the maximum tension the rope can bear to solve for the angle at this limit.
ANSWER:
n
= 2500 N
2300
N
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Problem 5.73
An 3.00 kg
box sits on a ramp that is inclined at 33.0
above the horizontal. The coefficient of kinetic friction between the box and the surface of the ramp is
μ
k
= 0.300. A constant horizontal
force F
F
= 26.0 N
is applied to the box , and the box moves down
the ramp.
Part A
If the box is initially at rest, what is its speed 2.00 s
after the force is applied?
Express your answer with the appropriate units.
ANSWER:
Correct
Bridging Problem: In a Rotating Cone
A small block with mass m
is placed inside an inverted cone that is rotating about a vertical axis such that the time for one revolution of the cone is T
. The walls
of the cone make an angle β
with the horizontal. The coefficient of static friction between the block
and the cone is μ
s
. If the block is to remain at a constant height h
above the apex of the cone, what
are (a) the maximum value of T
and (b) the minimum value of T
? (That is, find expressions for T
max
and T
min
in terms of β
and h
.)
0.922
v
= 23.1 m
s
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IDENTIFY and SET UP
Part A
Although we want the block not to slide up or down on the inside of the cone, this is not
an equilibrium problem. The block rotates with the cone and is in
uniform circular motion, so it has an acceleration directed toward the center of its circular path.
Identify the forces on the block.
Select all that apply.
ANSWER:
Correct
Part B
What is the direction of the friction force when the cone is rotating as slowly as possible, so T
has its maximum value T
max
?
ANSWER:
Correct
Part C
What is the direction of the friction force when the cone is rotating as rapidly as possible, so T
has its minimum value T
min
?
ANSWER:
Correct
Part D
the normal force
the weight of the block
the tension force
the friction force
the weight of the cone
down along the direction of cone's inner surface
clockwise
counterclockwise
up along the direction of cone's inner surface
horizontally towards the rotational axis at the cone's center
down along the direction of cone's inner surface
counterclockwise
up along the direction of cone's inner surface
horizontally towards the rotational axis at the cone's center
clockwise
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When T
=
T
max
and T
=
T
min
does the static friction force have its maximum magnitude? Why or why not?
ANSWER:
Correct
The normal force is in direct proportion to the static friction force. Thus, at the minimum period T
of rotation the normal force has its maximum and
so does the static friction force.
Part E
Draw a free-body diagram for the block when the cone is rotating with T
=
T
max
.
Draw the force vectors starting at the black dot. The location and orientation of the vectors will be graded. The length of the vectors will not be
graded.
Hint 1. The normal force
Recall that the normal force is always perpendicular to the surface.
ANSWER:
When T
=
T
min
, the radial acceleration is maximal, so the normal force exerted on the block, and hence, the static friction force has its
maximum magnitude. When T
=
T
max
, the static friction force has its minimum.
The static friction force has its maximum magnitude in both cases, when T
=
T
max
and T
=
T
min
. The only difference is in the direction of the
friction force.
The static friction force has its minimum magnitude in both cases, when T
=
T
max
and T
=
T
min
. The only difference is in the direction of the
friction force.
When T
=
T
max
, the radial acceleration is maximal, so the normal force exerted on the block, and hence, the static friction force has its
maximum magnitude. When T
=
T
min
, the static friction force has its minimum.
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Part F
Draw a free-body diagram for the block when the cone is rotating with T
=
T
min
.
Draw the force vectors starting at the black dot. The location and orientation of the vectors will be graded. The length of the vectors will not be
graded.
ANSWER:
No elements selected
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Correct
Part G
What is the radius of the circular path that the block follows?
Express your answer in terms of variables β
beta
and h
h
.
ANSWER:
Correct
Part H
Choose the unknown quantities, and decide which of these are the target variables.
ANSWER:
No elements selected
R
=
h
tan
β
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EXECUTE
Part I
In case of the rotation with a period T
=
T
max
and with a period T
=
T
min
, write the acceleration of the block.
Express your answer in terms of the variables T
T
, β
beta
, and h
h
.
ANSWER:
Correct
Part J
Find T
max
and T
min
.
Express your answer in terms of the variables μ
s
mu_s
, β
beta
, h
h
, and constants g
g
, π
pi
separated by a comma.
Hint 1. Newton's second law
Choose coordinate axes, and remember that it’s usually easiest to choose one of the axes to be in the direction of the acceleration. Write Newton's
second law in component form.
Hint 2. Static friction
Recall that the relationship for when maximum static friction acts is f
s
=
μ
s
n
.
Hint 3. Simplification
It will be enough to solve T
max
or T
min
-- the other one can be obtained with the change of a sign before μ
s
.
ANSWER:
Correct
EVALUATE
Part K
What do your expressions for T
max
and T
min
become if μ
s
= 0?
Express your answer in terms of the variables β
beta
, h
h
, and constants g
g
, π
pi
separated by a comma.
f
s
, n
, β
, R
, T
; the target variables are T
and n
.
f
s
, n
, R
, T
; the target variable is T
.
f
s
, n
, w
, R
, T
; the target variable is T
.
f
s
, n
, w
, β
, R
, T
; the target variable are T
and R
.
a
=
4
π
2
h
T
2
tan (
β
)
T
max
, T
min
=
4
π
2
h
cos (
β
) +
μ
s
sin (
β
)
g
tan (
β
)
sin (
β
) −
μ
s
cos (
β
)
,
4
π
2
h
cos (
β
) −
μ
s
sin (
β
)
g
tan (
β
)
sin (
β
) +
μ
s
cos (
β
)
√
(
)
(
)
√
(
)
(
)
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ANSWER:
Correct
Substituting the earlier relationships v
=
2
πR
T
and h
=
R
tan
β
, this result can be rewritten as tan
β
=
v
2
gR
, which is the same result as Example 5.22 for
a car rounding a banked curve with no friction.
For the steps and strategies involved in solving this problem, you may view the Video Tutor Solution
.
Score Summary:
Your score on this assignment is 30.4%.
You received 7.91 out of a possible total of 26 points.
T
max
, T
min
=
4
π
2
h
g
tan (
β
)
2
,
4
π
2
h
g
tan (
β
)
2
√
√
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