A 5.0 kg block initially at rest is pulled to the right along a horizontal surface by a constant horizontal force of 21 N. () A block puled to the right on a rough surface bya constant hertental force () The appled force is at an angle to the herental (For the following, when entering a mathematical expression, do not substitute numerical values; use variables only.) (a) Find the speed of the block after it has moved 2.5 mif the surfaces in contact have a coeficient of kinetic friction of 0.16. SOLUTION Conceptualize This example is similar to the example "A Block Pulled on a Frictioniless Surface" in Chapter 7, but modified so that the surface is no longer frictioniess. The rough surface applies a friction force on the block opposite to the applied force. As a result, we expect the speed to be er han Categorize The block is pulled by a force and the surface is rough, so the block and the surface are modeled as nonoiated Analyze Figure (a) ilustrates this situation. Neither the normai force nor the gravitational force does work on the system because their points of application are displaced horizontally. that found in "A Block Pulled on a Frictionless Surface. system with a nonconservative force. Find the work done on the system by the applied force (Use the following as necessary: Fand ar.): Apply the particle in equilibrium model to the block in the vertical direction (Use the following as necessary: F, Ar, m, and 9.): Find the magnitude of the friction force (in N): Substitute the energies into the equation shown and solve for the final speed of the block (Use the following as necessary: F, Ax and f,): Far - AK + sE-(mv? - 0) •ar
A 5.0 kg block initially at rest is pulled to the right along a horizontal surface by a constant horizontal force of 21 N. () A block puled to the right on a rough surface bya constant hertental force () The appled force is at an angle to the herental (For the following, when entering a mathematical expression, do not substitute numerical values; use variables only.) (a) Find the speed of the block after it has moved 2.5 mif the surfaces in contact have a coeficient of kinetic friction of 0.16. SOLUTION Conceptualize This example is similar to the example "A Block Pulled on a Frictioniless Surface" in Chapter 7, but modified so that the surface is no longer frictioniess. The rough surface applies a friction force on the block opposite to the applied force. As a result, we expect the speed to be er han Categorize The block is pulled by a force and the surface is rough, so the block and the surface are modeled as nonoiated Analyze Figure (a) ilustrates this situation. Neither the normai force nor the gravitational force does work on the system because their points of application are displaced horizontally. that found in "A Block Pulled on a Frictionless Surface. system with a nonconservative force. Find the work done on the system by the applied force (Use the following as necessary: Fand ar.): Apply the particle in equilibrium model to the block in the vertical direction (Use the following as necessary: F, Ar, m, and 9.): Find the magnitude of the friction force (in N): Substitute the energies into the equation shown and solve for the final speed of the block (Use the following as necessary: F, Ax and f,): Far - AK + sE-(mv? - 0) •ar
College Physics
11th Edition
ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Units, Trigonometry. And Vectors
Section: Chapter Questions
Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...
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![A Block Pulled on a Rough Surface
A 5.0 kg block initially at rest is pulled to the right along a horizontal surface by a constant horizontal force of 21 N.
(a) A block pulled to the right on a rough surface
(b) The applied force is at an angle e to the
by a constant horizontal force.
horizontal.
mg
mg
(For the following, when entering
mathematical expression, do not substitute numerical values; use variables only.)
(a) Find the speed of the block after it has moved 2.5 m if the surfaces in contact have a coefficient of kinetic friction of 0.16.
SOLUTION
Conceptualize
This example is similar to the example "A Block Pulled on a Frictionless Surface" in Chapter 7, but modified so that the surface is no longer frictionless.
The rough surface applies
friction force on the block opposite to the applied force. As a result, we expect the speed to be [higher than
that found in "A Block Pulled on a Frictionless Surface."
Categorize The block is pulled by a force and the
rough, so the block
d the surfac
are modeled as a nonis
ated V
system with a nonconservative force.
Analyze Figure (a) illustrates this situation. Neither the normal force nor the gravitational force does work on the system because their points of application are displaced horizontally.
Find the work done on the system by the applied force (Use the following as necessary: F and Ax.):
= W =
other forces
Apply the particle in equilibrium model to the block in the vertical direction (Use the following as necessary: F, Ax, m, and g.):
>'F, = 0 -n - mg = 0 →n =
Find the magnitude
the friction force (in N):
f, = Hn = Hmg =
N
Substitute the energies into the equation shown and solve for the final speed of the block (Use the following as necessary: F, Ax and f,.):
FAx = AK + AE =Gmv? - 0) + fAx
int
-Ax +
2
V,=
Substitute numerical values (Enter your answer in m/s.):
m/s
Finalize As expected, this value is -Select---
that found in the case of the block sliding on a frictionless surface. The difference in kinetic energies between the block sliding on a frictionless surface and the block in this example
equal to the increase in internal energy of the block-surface system in this example.
(b) Suppose the force F is applied at an angle 0 as shown in figure (b). At what angle should the force be applied to achieve the largest possible speed after the block has moved 2.5 m to the right?
SOLUTION
Conceptualize You might guess that 0 = 0 would give the largest speed because the force would have the largest component possible in the direction parallel to the surface. Think about Fapplied at an arbitrary nonzero angle, however. Although the horizontal component of the force would be reduced, the vertical component of the force would --Select--
speed could be maximized by pulling at an angle other than 0 = 0.
Categorize As in part (a), we model the block and the surface as a nonisolated system with a
-Select---
force acting.
Analyze Find the work done by the applied force, noting that d = Ax because the path followed by the block is a straight line (Use the following as necessary: F, Ax, and 0.):
(1) Sw
other forces W= Fd cos(0) =
Apply the particle in equilibrium model to the block in the vertical direction:](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F60608e4a-7bcf-415e-bb82-3a29182c9aeb%2Fa455b82a-c61f-4343-8eef-83657f0d003f%2F7g7exu_processed.png&w=3840&q=75)
Transcribed Image Text:A Block Pulled on a Rough Surface
A 5.0 kg block initially at rest is pulled to the right along a horizontal surface by a constant horizontal force of 21 N.
(a) A block pulled to the right on a rough surface
(b) The applied force is at an angle e to the
by a constant horizontal force.
horizontal.
mg
mg
(For the following, when entering
mathematical expression, do not substitute numerical values; use variables only.)
(a) Find the speed of the block after it has moved 2.5 m if the surfaces in contact have a coefficient of kinetic friction of 0.16.
SOLUTION
Conceptualize
This example is similar to the example "A Block Pulled on a Frictionless Surface" in Chapter 7, but modified so that the surface is no longer frictionless.
The rough surface applies
friction force on the block opposite to the applied force. As a result, we expect the speed to be [higher than
that found in "A Block Pulled on a Frictionless Surface."
Categorize The block is pulled by a force and the
rough, so the block
d the surfac
are modeled as a nonis
ated V
system with a nonconservative force.
Analyze Figure (a) illustrates this situation. Neither the normal force nor the gravitational force does work on the system because their points of application are displaced horizontally.
Find the work done on the system by the applied force (Use the following as necessary: F and Ax.):
= W =
other forces
Apply the particle in equilibrium model to the block in the vertical direction (Use the following as necessary: F, Ax, m, and g.):
>'F, = 0 -n - mg = 0 →n =
Find the magnitude
the friction force (in N):
f, = Hn = Hmg =
N
Substitute the energies into the equation shown and solve for the final speed of the block (Use the following as necessary: F, Ax and f,.):
FAx = AK + AE =Gmv? - 0) + fAx
int
-Ax +
2
V,=
Substitute numerical values (Enter your answer in m/s.):
m/s
Finalize As expected, this value is -Select---
that found in the case of the block sliding on a frictionless surface. The difference in kinetic energies between the block sliding on a frictionless surface and the block in this example
equal to the increase in internal energy of the block-surface system in this example.
(b) Suppose the force F is applied at an angle 0 as shown in figure (b). At what angle should the force be applied to achieve the largest possible speed after the block has moved 2.5 m to the right?
SOLUTION
Conceptualize You might guess that 0 = 0 would give the largest speed because the force would have the largest component possible in the direction parallel to the surface. Think about Fapplied at an arbitrary nonzero angle, however. Although the horizontal component of the force would be reduced, the vertical component of the force would --Select--
speed could be maximized by pulling at an angle other than 0 = 0.
Categorize As in part (a), we model the block and the surface as a nonisolated system with a
-Select---
force acting.
Analyze Find the work done by the applied force, noting that d = Ax because the path followed by the block is a straight line (Use the following as necessary: F, Ax, and 0.):
(1) Sw
other forces W= Fd cos(0) =
Apply the particle in equilibrium model to the block in the vertical direction:
![Apply the particle in equilibrium model to the block in the vertical direction:
= n + F sin(0) - mg = 0
Solve for n (Use the following as necessary: F, Ax, 0, m and g.):
(2)
n =
Use
= W = AK + AE,, to find the final kinetic energy for this situation:
other forces
int
W = AK + AE = (K,- 0) + f Ax - K,- W.-Ax
int
Substitute the results in Equations (1) and (2):
K = FAx cos(0) - H,nAx = FAx cos(0) - u, (mg - F sin(0))Ax
Maximizing the speed is equivalent to maximizing the final kinetic energy. Consequently, differentiate K with respect to 0 and set the result equal to zero (Use the following as necessary: Ax, 0, and g.):
dk,
= -FAx sin(0) - H(0 - F cos(0))Ax = 0
d0
-sin(0) + H, cos(0) = 0
Evaluate 0 (in degrees) for u, = 0.16:
0 = tan-(H,) = tan-(0.16) =|
Finalize Notice that the angle at which the speed of the block is a maximum
indeed not 0 = 0. When the angle exceeds 9.09°, the horizontal component of the applied force is too small to be compensated by the reduced friction force and the speed of the block begins to
Select-
from its maximum value.
EXERCISE
A 17.5 kg block is dragged over
rough, horizontal surface by a 75 N force acting at 21° above the horizontal. The block
displaced 5.7 m, and the coefficient of kinetic friction is 0.200. (Enter your answers in J.)
Hint
(a) Find the work done on the block by the 75 N force.
(b) Find the work done on the block by the normal force.
(c) Find the work done on the block by the gravitational force.
(d) What is the increase in internal energy of the block-surface system due to friction?
(e) Find the total change in the block's kinetic energy.
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Transcribed Image Text:Apply the particle in equilibrium model to the block in the vertical direction:
= n + F sin(0) - mg = 0
Solve for n (Use the following as necessary: F, Ax, 0, m and g.):
(2)
n =
Use
= W = AK + AE,, to find the final kinetic energy for this situation:
other forces
int
W = AK + AE = (K,- 0) + f Ax - K,- W.-Ax
int
Substitute the results in Equations (1) and (2):
K = FAx cos(0) - H,nAx = FAx cos(0) - u, (mg - F sin(0))Ax
Maximizing the speed is equivalent to maximizing the final kinetic energy. Consequently, differentiate K with respect to 0 and set the result equal to zero (Use the following as necessary: Ax, 0, and g.):
dk,
= -FAx sin(0) - H(0 - F cos(0))Ax = 0
d0
-sin(0) + H, cos(0) = 0
Evaluate 0 (in degrees) for u, = 0.16:
0 = tan-(H,) = tan-(0.16) =|
Finalize Notice that the angle at which the speed of the block is a maximum
indeed not 0 = 0. When the angle exceeds 9.09°, the horizontal component of the applied force is too small to be compensated by the reduced friction force and the speed of the block begins to
Select-
from its maximum value.
EXERCISE
A 17.5 kg block is dragged over
rough, horizontal surface by a 75 N force acting at 21° above the horizontal. The block
displaced 5.7 m, and the coefficient of kinetic friction is 0.200. (Enter your answers in J.)
Hint
(a) Find the work done on the block by the 75 N force.
(b) Find the work done on the block by the normal force.
(c) Find the work done on the block by the gravitational force.
(d) What is the increase in internal energy of the block-surface system due to friction?
(e) Find the total change in the block's kinetic energy.
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