Chapter 8 Conservation of Energy 7.3 work done by a varying force 7.4 kinetic Energy and work-...
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Transcript of Chapter 8 Conservation of Energy 7.3 work done by a varying force 7.4 kinetic Energy and work-...
![Page 1: Chapter 8 Conservation of Energy 7.3 work done by a varying force 7.4 kinetic Energy and work- energy principle 8.1 Conservative forces 8.2 Potential Energy.](https://reader036.fdocuments.us/reader036/viewer/2022081418/56649d6e5503460f94a4eb8d/html5/thumbnails/1.jpg)
Chapter 8
Conservation of Energy7.3 work done by a varying force7.4 kinetic Energy and work-energy principle8.1 Conservative forces8.2 Potential Energy
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Work done by a constant force
Units of work: Nm or Joules (J)
F
r
Work is an energy transfer that occurs when a force acts on an object that moves.
•Work is done only when force is exerted over a distance.
(no displacement=no work)
http://i.telegraph.co.uk/telegraph/multimedia/archive/01435/bmw_1435680c.jpg
•Only the part of the force parallel to the displacement does work.
Fcos
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Work can be positive, negative or zero
cosrFWork F
r
Fpush
x
mg
N
Fy
Fx
f
Work done byWorkGravity =
WorkNormal =
WorkFriction =
WorkFPUSH=
0
0
-fxNegative since f is opposite x
Fxcos= FxxPositive since Fx same direction as x
Work done sliding a box across a floor
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7-3 Work Done by a Varying Force
For a force that varies, the work can be approximated by dividing the distance up into small pieces, finding the work done during each, and adding them up.
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7-3 Work Done by a Varying Force
In the limit that the pieces become infinitesimally narrow, the work is the area under the curve:
Or:
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7-3 Work Done by a Varying Force
Work done by a spring force:
You are exerting a force Fp= kx
K is the spring constant or stifness.
The force exerted by a spring is given by: called restoring force
This is called Hooke’s law
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7-3 Work Done by a Varying Force
Plot of F vs. x. Work done is equal to the shaded area.
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7-3 Work Done by a Varying Force
Example 7-5: Work done on a spring.
(a) A person pulls on a spring, stretching it 3.0 cm, which requires a maximum force of 75 N. How much work does the person do? (b) If, instead, the person compresses the spring 3.0 cm, how much work does the person do?
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7-3 Work Done by a Varying Force
Example 7-6: Force as a function of x.
where F0 = 2.0 N, x0 = 0.0070 m, and x is the position of the end of the arm. If the arm moves from x1 = 0.010 m to x2 = 0.050 m, how much work did the motor do?
A robot arm that controls the position of a video camera in an automated surveillance system is manipulated by a motor that exerts a force on the arm. The force is given by
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7-4 Kinetic Energy and the Work-Energy Principle
Energy was traditionally defined as the ability to do work. We now know that not all forces are able to do work; however, we are dealing in these chapters with mechanical energy, which does follow this definition.
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7-4 Kinetic Energy and the Work-Energy Principle
If we write the acceleration in terms of the velocity and the distance, we find that the work done here is
We define the kinetic energy as:
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7-4 Kinetic Energy and the Work-Energy Principle
This means that the work done is equal to the change in the kinetic energy:
•This is the Work-Energy Principle
• If the net work is positive, the kinetic energy increases.
• If the net work is negative, the kinetic energy decreases.
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7-4 Kinetic Energy and the Work-Energy Principle
Because work and kinetic energy can be equated, they must have the same units: kinetic energy is measured in joules. Energy can be considered as the ability to do work:
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7-4 Kinetic Energy and the Work-Energy Principle
Example 7-7: Kinetic energy and work done on a baseball.
A 145-g baseball is thrown so that it acquires a speed of 25 m/s. (a) What is its kinetic energy? (b) What was the net work done on the ball to make it reach this speed, if it started from rest?
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7-4 Kinetic Energy and the Work-Energy Principle
Example 7-8: Work on a car, to increase its kinetic energy.
How much net work is required to accelerate a 1000-kg car from 20 m/s to 30 m/s?
The net work is the increase in kinetic energy, 2.5 x 105 J.
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7-4 Kinetic Energy and the Work-Energy Principle
Example 7-10: A compressed spring.
A horizontal spring has spring constant k = 360 N/m. (a) How much work is required to compress it from its uncompressed length (x = 0) to x = 11.0 cm? (b) If a 1.85-kg block is placed against the spring and the spring is released, what will be the speed of the block when it separates from the spring at x = 0? Ignore friction. (c) Repeat part (b) but assume that the block is moving on a table and that some kind of constant drag force FD = 7.0 N is acting to slow it down, such as friction (or perhaps your finger).
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8-1 Conservative and Nonconservative Forces
A force is conservative if:the work done by the force on an object moving from one point to another depends only on the initial and final positions of the object, and is independent of the particular path taken.Example: gravity.
W=-mg (y2-y1)
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8-1 Conservative and Nonconservative Forces
Another definition of a conservative force:
a force is conservative if the net work done by the force on an object moving around any closed path is zero.
(a) (b)
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8-1 Conservative and Nonconservative Forces
If friction is present, the work done depends not only on the starting and ending points, but also on the path taken. Friction is called a nonconservative force.
W = FPd
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8-1 Conservative and Nonconservative Forces
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8-2 Potential Energy
An object can have potential energy by virtue of its surroundings. Potential energy can only be defined for conservative forces
Familiar examples of potential energy:
• A wound-up spring
• A stretched elastic band
• An object at some height above the ground
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8-2 Potential Energy
In raising a mass m to a height h, the work done by the external force is
We therefore define the gravitational potential energy at a height y above some reference point:
.
.
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8-2 Potential Energy
This potential energy can become kinetic energy if the object is dropped.
Potential energy is a property of a system as a whole, not just of the object (because it depends on external forces).
If Ugrav = mgy, where do we measure y from?
It turns out not to matter, as long as we are consistent about where we choose y = 0. Only changes in potential energy can be measured.
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8-2 Potential EnergyExample 8-1: Potential energy changes for a roller coaster.
A 1000-kg roller-coaster car moves from point 1 to point 2 and then to point 3. (a) What is the gravitational potential energy at points 2 and 3 relative to point 1? That is, take y = 0 at point 1. (b) What is the change in potential energy when the car goes from point 2 to point 3? (c) Repeat parts (a) and (b), but take the reference point (y = 0) to be at point 3.
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8-2 Potential Energy
General definition of gravitational potential energy:
For any conservative force: