Upload
gil-best
View
61
Download
2
Embed Size (px)
DESCRIPTION
Chapter 7 Work and Kinetic Energy. Reading and Review. Force and Work. a) one force b) two forces c) three forces d) four forces e) no forces are doing work. A box is being pulled up a rough incline by a rope connected to a pulley. How many forces are doing work on the box?. - PowerPoint PPT Presentation
Citation preview
Copyright © 2010 Pearson Education, Inc.
Chapter 7
Work and Kinetic Energy
Copyright © 2010 Pearson Education, Inc.
Reading and Review
Copyright © 2010 Pearson Education, Inc.
Force and Work
a) one force
b) two forces
c) three forces
d) four forces
e) no forces are doing work
A box is being pulled up a rough
incline by a rope connected to a
pulley. How many forces are
doing work on the box?
Copyright © 2010 Pearson Education, Inc.
Force and Work
N
f
T
mg
displacementAny force not perpendicular
to the motion will do work:
N does no work
T does positive work
f does negative work
mg does negative work
a) one force
b) two forces
c) three forces
d) four forces
e) no forces are doing work
A box is being pulled up a rough
incline by a rope connected to a
pulley. How many forces are
doing work on the box?
Copyright © 2010 Pearson Education, Inc.
Free Fall I
a) quarter as much
b) half as much
c) the same
d) twice as much
e) four times as much
Two stones, one twice the
mass of the other, are dropped
from a cliff. Just before hitting
the ground, what is the kinetic
energy of the heavy stone
compared to the light one?
Copyright © 2010 Pearson Education, Inc.
Consider the work done by gravity to make the stone
fall distance d:
KE = Wnet = F d cos
KE = mg d
Thus, the stone with the greater mass has the greater
KE, which is twice as big for the heavy stone.
Free Fall I
a) quarter as much
b) half as much
c) the same
d) twice as much
e) four times as much
Two stones, one twice the
mass of the other, are dropped
from a cliff. Just before hitting
the ground, what is the kinetic
energy of the heavy stone
compared to the light one?
Follow-up: How do the initial values of gravitational PE compare?
Copyright © 2010 Pearson Education, Inc.
In the previous question, just
before hitting the ground, what is
the final speed of the heavy stone
compared to the light one?
a) quarter as much
b) half as much
c) the same
d) twice as much
e) four times as much
Free Fall II
Copyright © 2010 Pearson Education, Inc.
In the previous question, just
before hitting the ground, what is
the final speed of the heavy stone
compared to the light one?
a) quarter as much
b) half as much
c) the same
d) twice as much
e) four times as much
All freely falling objects fall at the same rate, which is g.
Because the acceleration is the same for both, and the
distance is the same, then the final speeds will be the same for
both stones.
Free Fall II
Copyright © 2010 Pearson Education, Inc.
Work Done by a Variable Force
The force needed to stretch a spring an amount x is F = kx.
Therefore, the work done in stretching the spring is
Copyright © 2010 Pearson Education, Inc.
Application: work by a spring
Hooke’s Law: F = - kx k = (3kg)(9.8 m/s2) / (3.9 cm)k = 760 N/m
Loaded spring: W = kx2/2 = (760 N/m) (0.04m)2/ 2
W = 0.61 J
How fast?: v = d/t = (0.020 m) (0.020 s) = 1 m/s
KE = mv2/2 = (1kg)(1m/s)2 / 2KE = 0.55 J
Kinetic Energy:
Copyright © 2010 Pearson Education, Inc.
Power
Power is a measure of the rate at which work is done:
SI unit: J/s = watt, W
1 horsepower = 1 hp = 746 W
ave
WP
t
Copyright © 2010 Pearson Education, Inc.
Power
Copyright © 2010 Pearson Education, Inc.
Power
If an object is moving at a constant speed in the face of friction, gravity, air resistance, and so forth, the power exerted by the driving force can be written:
Question: what is the total work per unit time done on the object?
F x xP F Fv
t t
Copyright © 2010 Pearson Education, Inc.
a) energy
b) power
c) current
d) voltage
e) none of the above
Electric Bill
When you pay the electric
company by the kilowatt-hour,
what are you actually paying for?
Copyright © 2010 Pearson Education, Inc.
We have defined: Power = energy /
time
So we see that: Energy = power ×
time
This means that the unit of power ×
time (watt-hour) is a unit of energy !!
Electric Bill
When you pay the electric
company by the kilowatt-hour,
what are you actually paying for?
a) energy
b) power
c) current
d) voltage
e) none of the above
Copyright © 2010 Pearson Education, Inc.
A block rests on a horizontal frictionless surface. A string is attached to the block, and is pulled with a force of 45.0 N at an angle above the horizontal, as shown in the figure. After the block is pulled through a distance of 1.50 m, its speed is 2.60 m/s, and 50.0 J of work has been done on it. (a) What is the angle (b) What is the mass of the block?
Copyright © 2010 Pearson Education, Inc.
Copyright © 2010 Pearson Education, Inc.
The pulley system shown is used to lift a 52 kg crate. Note that one chain connects the upper pulley to the ceiling and a second chain connects the lower pulley to the crate. Assuming the masses of the chains, pulleys, and ropes are negligible, determine (a) the force F required to lift the crate with constant speed, and(b) the tension in two chains
Copyright © 2010 Pearson Education, Inc.
(a) the force F required to lift the crate with constant speed, and(b) the tension in two chains
(a) constant velocity, a=0, so net force =0.
2T - (52kg)(9.8m/s2) = 0
T = 250 NF = -250 Ny
(b) upper pulley doesn’t move:Tch - 2Trope = 0 Tch = 500 N
lower pulley has constant accelerationTch -2Trope =0 Tch = 500 N
Mechanical Advantage!
Copyright © 2010 Pearson Education, Inc.
(a) how much power is applied to the box by the chain?(b) how much power is applied on the rope by the applied force?
What about work?
Trope = 250 NTchain = 500 NF = -250 Ny
(a) P = Fv = 500 N * vbox
(b)P = Fv = 250 N * vhand
hand moves twice as fast
hand moves twice as far
Copyright © 2010 Pearson Education, Inc.
Chapter 8
Potential Energy and Conservation of Energy
Copyright © 2010 Pearson Education, Inc.
Units of Chapter 8
• Conservative and Nonconservative Forces
• Potential Energy and the Work Done by Conservative Forces
• Conservation of Mechanical Energy
• Work Done by Nonconservative Forces
• Potential Energy Curves and Equipotentials
Copyright © 2010 Pearson Education, Inc.
8-1 Conservative and Nonconservative Forces
Conservative force: the work it does is stored in the form of energy that can be released at a later time
Example of a conservative force: gravity
Example of a nonconservative force: friction
Also: the work done by a conservative force moving an object around a closed path is zero; this is not true for a nonconservative force
Copyright © 2010 Pearson Education, Inc.
8-1 Conservative and Nonconservative Forces
Work done by gravity on a closed path is zero:
Copyright © 2010 Pearson Education, Inc.
8-1 Conservative and Nonconservative Forces
Work done by friction on a closed path is not zero:
Copyright © 2010 Pearson Education, Inc.
8-1 Conservative and Nonconservative Forces
The work done by a conservative force is zero on any closed path:
Copyright © 2010 Pearson Education, Inc.
8-2 The Work Done by Conservative Forces
If we pick up a ball and put it on the shelf, we have done work on the ball. We can get that energy back if the ball falls back off the shelf; in the meantime, we say the energy is stored as potential energy.
(8-1)
Copyright © 2010 Pearson Education, Inc.
8-2 The Work Done by Conservative Forces
Gravitational potential energy:
Copyright © 2010 Pearson Education, Inc.
Is it possible for the
gravitational potential
energy of an object to
be negative?
a) yes
b) no
Sign of the Energy II
Copyright © 2010 Pearson Education, Inc.
Is it possible for the
gravitational potential
energy of an object to
be negative?
a) yes
b) no
Gravitational PE is mgh, where height h is measured relative to
some arbitrary reference level where PE = 0. For example, a
book on a table has positive PE if the zero reference level is
chosen to be the floor. However, if the ceiling is the zero level,
then the book has negative PE on the table. Only differences (or
changes) in PE have any physical meaning.
Sign of the Energy II
Copyright © 2010 Pearson Education, Inc.
You and your friend both solve a problem involving a skier going down a slope, starting from rest. The two of you have chosen different levels for y = 0 in this problem. Which of the following quantities will you and your friend agree on?
a) only B
b) only C
c) A, B, and C
d) only A and C
e) only B and C
Question 8.2 KE and PE
A) skier’s PE B) skier’s change in PE C) skier’s final KE
Copyright © 2010 Pearson Education, Inc.
You and your friend both solve a problem involving a skier going down a slope, starting from rest. The two of you have chosen different levels for y = 0 in this problem. Which of the following quantities will you and your friend agree on?
a) only B
b) only C
c) A, B, and C
d) only A and C
e) only B and C
The gravitational PE depends upon the reference level, but
the difference PE does not! The work done by gravity
must be the same in the two solutions, so PE and KE
should be the same.
Question 8.2 KE and PE
A) skier’s PE B) skier’s change in PE C) skier’s final KE
Follow-up: Does anything change physically by the choice of y = 0?
Copyright © 2010 Pearson Education, Inc.
8-2 The Work Done by Conservative Forces
Springs: (8-4)
Copyright © 2010 Pearson Education, Inc.
8-3 Conservation of Mechanical Energy
Definition of mechanical energy:
(8-6)
Using this definition and considering only conservative forces, we find:
Or equivalently:
Copyright © 2010 Pearson Education, Inc.
8-3 Conservation of Mechanical Energy
Energy conservation can make kinematics problems much easier to solve:
Copyright © 2010 Pearson Education, Inc.
Example: A mass m slides down a 2 m long smooth ramp which makes an angle of 30o with the top of a table which is 1 m above the floor. The end of the ramp is at the edge of the table. At what horizontal distance from the edge of the table does the mass hit the floor?
Copyright © 2010 Pearson Education, Inc.
You and your friend both solve a problem involving a skier going down a slope, starting from rest. The two of you have chosen different levels for y = 0 in this problem. Which of the following quantities will you and your friend agree on?
a) only B
b) only C
c) A, B, and C
d) only A and C
e) only B and C
KE and PE
A) skier’s PE B) skier’s change in PE C) skier’s final KE
Copyright © 2010 Pearson Education, Inc.
You and your friend both solve a problem involving a skier going down a slope, starting from rest. The two of you have chosen different levels for y = 0 in this problem. Which of the following quantities will you and your friend agree on?
a) only B
b) only C
c) A, B, and C
d) only A and C
e) only B and C
The gravitational PE depends upon the reference level, but
the difference PE does not! The work done by gravity
must be the same in the two solutions, so PE and KE
should be the same.
KE and PE
A) skier’s PE B) skier’s change in PE C) skier’s final KE
Follow-up: Does anything change physically by the choice of y = 0?
Copyright © 2010 Pearson Education, Inc.
Example: Two water slides are shaped differently, but start at the same height h and are of equal length. Two rides, Paul and Kathy, start from rest at the same time on different slides.a)Which is travelling faster at the bottom?b)Which makes it to the bottom first?
Copyright © 2010 Pearson Education, Inc.
8-4 Work Done by Nonconservative Forces
In the presence of nonconservative forces, the total mechanical energy is not conserved:
Solving,
(8-9)
Copyright © 2010 Pearson Education, Inc.
8-4 Work Done by Nonconservative Forces
In this example, the nonconservative force is water resistance:
Copyright © 2010 Pearson Education, Inc.
8-5 Potential Energy Curves and Equipotentials
The curve of a hill or a roller coaster is itself essentially a plot of the gravitational potential energy:
Copyright © 2010 Pearson Education, Inc.
8-5 Potential Energy Curves and Equipotentials
The potential energy curve for a spring:
Copyright © 2010 Pearson Education, Inc.
8-5 Potential Energy Curves and Equipotentials
Contour maps are also a form of potential energy curve:
Copyright © 2010 Pearson Education, Inc.
Summary of Chapter 8
• Conservative forces conserve mechanical energy
• Nonconservative forces convert mechanical energy into other forms
• Conservative force does zero work on any closed path
• Work done by a conservative force is independent of path
• Conservative forces: gravity, spring
Copyright © 2010 Pearson Education, Inc.
Summary of Chapter 8
• Work done by nonconservative force on closed path is not zero, and depends on the path
• Nonconservative forces: friction, air resistance, tension
• Energy in the form of potential energy can be converted to kinetic or other forms
• Work done by a conservative force is the negative of the change in the potential energy
• Gravity: U = mgy
• Spring: U = ½ kx2
Copyright © 2010 Pearson Education, Inc.
Summary of Chapter 8
• Mechanical energy is the sum of the kinetic and potential energies; it is conserved only in systems with purely conservative forces
• Nonconservative forces change a system’s mechanical energy
• Work done by nonconservative forces equals change in a system’s mechanical energy
• Potential energy curve: U vs. position