1. Chapter 6
Work and Energy

2. Units of Chapter 6 Work Done by a Constant Force
Kinetic Energy, and the Work-Energy Principle
Potential Energy
Conservative and Nonconservative Forces
Mechanical Energy and Its Conservation
Key Ideas
Work
Energy
Power

3. Work Work is defined to be: _______________________
The force must be in the direction of motion
Force x Distance

4. Work Units Work = Force x distance Work Force distance
Other units - BTU, calorie

5. 6-1 Work Done by a Constant Force
The work done by a constant force is defined as the distance moved multiplied by the component of the force in the direction of displacement:
(6-1)

6. 6-1 Work Done by a Constant Force
Solving work problems:
Draw a free-body diagram.
Choose a coordinate system.
Apply Newton’s laws to determine any unknown forces.
Find the work done by a specific force.
To find the net work, either
find the net force and then find the work it does, or
find the work done by each force and add.

7. Forces that do work This force _____________ F=20N D=2 m F=35N D=2 m
Bottom force does not do work
F=35N
D=2 m
This force _______ ________

8. Negative work F=35N Ff=10N D=6 m How much work is done on the box?
Bottom force does not do work
D=6 m
How much work is done on the box?

9. 6-1 Work Done by a Constant Force
Work done by forces that oppose the direction of motion, such as friction, will be negative.
Centripetal forces do no work, as they are always perpendicular to the direction of motion.

10. 6-2 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. As the pieces become very narrow, the work done is the area under the force vs. distance curve.

11. Energy Energy is the stored ability to do work (for mechanical types.
Mechanical types we will study
___________
____________
Other types of energy:
Heat, chemical, electrical, spring

12. Kinetic Energy Kinetic Energy eq: __________________ Derivation:
Units are ________________
W=Fd, f=ma so W = mad v^2=2ad a=v^2/2d
W=mv2/2d or 1/2 mv2 more specifically W = 1/2mv2 - 1/mv2

13. Kinetic Energy Kinetic energy =
How much energy does a 1000Kg car have at 20 m/s?
How much work was done on the car to get it going that fast?
1/2 mv^2

14. 6-3 Kinetic Energy, and the Work-Energy Principle
This means that the work done is equal to the change in the kinetic energy:
(6-4)
If the net work is positive, the kinetic energy increases.
If the net work is negative, the kinetic energy decreases.

15. 6-3 Kinetic Energy, and the Work-Energy Principle
The 3000kg bus accelerates from 20m/s to 44 m/s. How much work is done?
If it took 200m, what force is required?
Could be done by F=ma v2=2ad

16. Kinetic Energy and Work
The 3000kg bus decelerates from 30 m/s to 5 m/s in 400m. How much work is done?
What force is required to stop the bus?
Could be done by F=ma v2=2ad

17. Kinetic Energy and Work
A 1000 kg car has tires with a µ = .5. How far is the stopping distance from 33 m/s?
b) How will it change at twice the distance?
Also see p examples
1/2mv2 = Fd = µFn x d =
109 meters

18. 6-3 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 approach makes some problems solvable. Ex: roller coasters, variable forces.

19. 6-4 Potential Energy
In raising a mass m to a height h, the work done by the external force is
W=Fd
= Weight x height
=(mg) x height
gravitational potential energy:
PE = mg∆h
(6-6)

20. Potential Energy Potential energy =____________
* only depends on difference in height
h=4m
h=4m
20kg
20kg

21. 6-4 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 , 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.

22. Energy Conservation
Conservation of Energy - ___________________________________________________________________
So energy can be changed from PE to KE and back again
Energy is transferred from one form to another not created or destroyed.

23. 6-7 Problem Solving Using Conservation of Mechanical Energy
In the image on the left, the total mechanical energy is:
The energy buckets (right) show how the energy moves from all potential to all kinetic.

24. Energy Conservation Problems
Energy Before = Energy After
mgh + 1/2 mv2 = mgh + 1/2 mv2
(you could also add 1/2kx2 and any other energy forms)
A projectile is fired straight upward at a velocity of 12 m/s from a height of 25meters. What is the velocity when it is 13 meters off the ground?
W = f*d 100 x 10 x3 = 3000J for both

25. The pendulum
Show PE KE trade off

26. Pendulum A 5kg mass is hung on a string. It is lifted 2 meters.
Where is it going the fastest?
How fast is it going at that point?
How high does it go?
How fast is it going when it is 1 meter up?

27. 6-7 Problem Solving Using Conservation of Mechanical Energy
If there is no friction, the speed of a roller coaster will depend only on its height compared to its starting height.

28. Power #1
A 100kg boy walks up a 3 meter tall flight of stairs in 10 seconds. How much work is done? #2
A 100kg boy walks up a 3 meter tall flight of stairs in 3 seconds. How much work is done?
W = f*d 100 x 10 x3 = 3000J for both
Which is more difficult? How do you measure it?

29. Power Power is the rate at which work is done Power = Units: Power
P=work/time
Power
Work
time

30. Power How much power is used in each case? #1
A 100kg boy walks up a 3 meter tall flight of stairs in 10 seconds. How much work is done? #2
A 100kg boy walks up a 3 meter tall flight of stairs in 3 seconds. How much work is done?
W = f*d 100 x 10 x3 = 3000J for both
3000/10 = 300 Watts 3000/3 = 1000 watts
(900 Watts output for a healthy person, trained cyclist 2000 W peak)
How much power is used in each case?

31. 6-10 Power Power is the rate at which work is done –
(6-17)
In the SI system, the units of power are watts:
The difference between walking and running up these stairs is power – the change in gravitational potential energy is the same.

32. 6-10 Power
Power is also needed for acceleration and for moving against the force of gravity.
The average power can be written in terms of the force and the average velocity:
Watts=

33. 6-4 Potential Energy
Potential energy can also be stored in a spring when it is compressed; the figure below shows potential energy yielding kinetic energy.

34. 6-4 Potential Energy
The force required to compress or stretch a spring is:
where k is called the spring constant, and needs to be measured for each spring.
(6-8)
Units? k = Newtons/meter

35. 6-4 Potential Energy
The force increases as the spring is stretched or compressed further. We find that the potential energy of the compressed or stretched spring, measured from its equilibrium position, can be written:
(6-9)

36. Optional after this slide

37. 6-5 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.

38. 6-5 Conservative and Nonconservative Forces
Potential energy can only be defined for conservative forces.

39. 6-5 Conservative and Nonconservative Forces
Therefore, we distinguish between the work done by conservative forces and the work done by nonconservative forces.
We find that the work done by nonconservative forces is equal to the total change in kinetic and potential energies:
(6-10)

40. 6-6 Mechanical Energy and Its Conservation
If there are no nonconservative forces, the sum of the changes in the kinetic energy and in the potential energy is zero – the kinetic and potential energy changes are equal but opposite in sign.
This allows us to define the total mechanical energy:
And its conservation:
(6-12b)

41. 6-7 Problem Solving Using Conservation of Mechanical Energy
For an elastic force, conservation of energy tells us:
(6-14)

42. 6-8 Other Forms of Energy; Energy Transformations and the Conservation of Energy
Some other forms of energy:
Electric energy, nuclear energy, thermal energy, chemical energy.
Work is done when energy is transferred from one object to another.
Accounting for all forms of energy, we find that the total energy neither increases nor decreases. Energy as a whole is conserved.

43. 6-9 Energy Conservation with Dissipative Processes; Solving Problems
If there is a nonconservative force such as friction, where do the kinetic and potential energies go?
They become heat; the actual temperature rise of the materials involved can be calculated.

44. 6-9 Energy Conservation with Dissipative Processes; Solving Problems
Problem Solving:
Draw a picture.
Determine the system for which energy will be conserved.
Figure out what you are looking for, and decide on the initial and final positions.
Choose a logical reference frame.
Apply conservation of energy.
Solve.

45. Summary of Chapter 6 Work: Kinetic energy is energy of motion:
Potential energy is energy associated with forces that depend on the position or configuration of objects.
The net work done on an object equals the change in its kinetic energy.
If only conservative forces are acting, mechanical energy is conserved.
Power is the rate at which work is done.