slide1
Download
Skip this Video
Download Presentation
PHY 113 C General Physics I 11 AM – 12:15 P M MWF Olin 101 Plan for Lecture 7: Chapter 7 -- The notion of work and energy Definition of work

Loading in 2 Seconds...

play fullscreen
1 / 40

PHY 113 C General Physics I 11 AM – 12:15 P M MWF Olin 101 Plan for Lecture 7: Chapter 7 -- The notion of work a - PowerPoint PPT Presentation


  • 76 Views
  • Uploaded on

PHY 113 C General Physics I 11 AM – 12:15 P M MWF Olin 101 Plan for Lecture 7: Chapter 7 -- The notion of work and energy Definition of work Examples of work Kinetic energy; Work-kinetic energy theorem Potential energy and work; conservative forces. 7.3,7.15,7.31,7.34.

loader
I am the owner, or an agent authorized to act on behalf of the owner, of the copyrighted work described.
capcha
Download Presentation

PowerPoint Slideshow about ' PHY 113 C General Physics I 11 AM – 12:15 P M MWF Olin 101 Plan for Lecture 7: Chapter 7 -- The notion of work a' - seanna


An Image/Link below is provided (as is) to download presentation

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.


- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -
Presentation Transcript
slide1

PHY 113 C General Physics I

  • 11 AM – 12:15 PM MWF Olin 101
  • Plan for Lecture 7:
  • Chapter 7 -- The notion of work and energy
    • Definition of work
    • Examples of work
    • Kinetic energy; Work-kinetic energy theorem
    • Potential energy and work; conservative forces

PHY 113 C Fall 2013 -- Lecture 7

slide2

7.3,7.15,7.31,7.34

PHY 113 C Fall 2013 -- Lecture 7

slide3

Webassign questions for Assignment 6 -- #1

52. Consider a large truck carrying a heavy load, such as steel beams. … Assume that a 10,000-kg load sits on the flatbed of a 20,000-kg truck initially moving at vi=12 m/s. Assume that the load on the truck bed has a coefficient of static friction of mS=0.5. When the truck is braked at constant force, it comes to rest in a distance d. What is the minimum stopping distance d such that the load remains stationary relative to the truck bed throughout the breaking?

m

a

vi

f

PHY 113 C Fall 2013 -- Lecture 7

slide4

Webassign questions for Assignment 6 -- #1 -- continued

  • iclicker exercise --
  • Do we have enough information to calculate a?
    • Yes
    • No

m

a

vi

f

PHY 113 C Fall 2013 -- Lecture 7

slide5

Webassign questions for Assignment 6 -- #1 -- continued

m

a

vi

f

PHY 113 C Fall 2013 -- Lecture 7

slide6

Webassign questions for Assignment 6 -- #4

A block of mass 3 kg is pushed up against a wall by a force P that makes an angle of q=50o with the horizontal. ms=0.25. Determine the possible values for the magnitude of P that allow the block to remain stationary.

f

N

f

mg

PHY 113 C Fall 2013 -- Lecture 7

slide7

f

N

f

mg

PHY 113 C Fall 2013 -- Lecture 7

slide8

Webassign questions for Assignment 6 -- #6

F

PHY 113 C Fall 2013 -- Lecture 7

slide9

Preparation for the introduction of work:

Digressionon the definition of vector “dot” product

q

PHY 113 C Fall 2013 -- Lecture 7

slide10

Digression: definition of vector “dot” product -- continued

q

PHY 113 C Fall 2013 -- Lecture 7

slide11

Digression: definition of vector “dot” product –

component form

q

Note that the result of a vector dot product is a scalar.

PHY 113 C Fall 2013 -- Lecture 7

slide12

Definition of work:

F

dr

ri

rj

PHY 113 C Fall 2013 -- Lecture 7

slide13

Units of work:

  • work = force · displacement = (N · m) = (joule)
    • Only the component of force in the direction of the displacement contributes to work.
    • Work is a scalar quantity.
    • If the force is not constant, the integral form must be used.
    • Work can be defined for a specific force or for a combination of forces

PHY 113 C Fall 2013 -- Lecture 7

slide14

iclicker question: A ball with a weight of 5 N follows the trajectory shown. What is the work done by gravity from the initial rito final displacement rf?

2.5m

rf

ri

1m

1m

10 m

(A) 0 J (B) 7.5 J (C) 12.5 J (D) 50 J

PHY 113 C Fall 2013 -- Lecture 7

slide15

Gravity does negative work:

Gravity does positive work:

ri

rf

mg

mg

ri

rf

W=-mg(rf-ri)>0

W=-mg(rf-ri)<0

PHY 113 C Fall 2013 -- Lecture 7

slide16

Work done by a variable force:

PHY 113 C Fall 2013 -- Lecture 7

slide17

Example:

PHY 113 C Fall 2013 -- Lecture 7

slide18

Example – spring force: Fx = - kx

PHY 113 C Fall 2013 -- Lecture 7

slide19

Positive work

Negative work

F

x

PHY 113 C Fall 2013 -- Lecture 7

slide20

Detail:

PHY 113 C Fall 2013 -- Lecture 7

slide21

More examples:

Suppose a rope lifts a weight of 1000N by 0.5m at a constant upward velocity of 4.9m/s. How much work is done by the rope?

(A) 500 J (B) 750 J (C) 4900 J (D) None of these

Suppose a rope lifts a weight of 1000N by 0.5m at a constant upward acceleration of 4.9m/s2. How much work is done by the rope?

(A) 500 J (B) 750 J (C) 4900 J (D) None of these

PHY 113 C Fall 2013 -- Lecture 7

slide22

Another example

FP

n

q

fk

mg

xi

xf

Assume FP sinq<<mg

Work of gravity?

0

FPcosq (xf-xi)

Work of FP?

-mkn(xf-xi)=-mk(mg- FP sin q) (xf-xi)

Work of fk?

PHY 113 C Fall 2013 -- Lecture 7

slide23

iclicker exercise:

  • Why should we define work?
    • Because professor like to torture students.
    • Because it is always good to do work
    • Because it will help us understand motion.
    • Because it will help us solve the energy crisis.

 Work-Kinetic energy theorem.

PHY 113 C Fall 2013 -- Lecture 7

slide24

Back to work:

F

dr

ri

rj

PHY 113 C Fall 2013 -- Lecture 7

slide25

Why is work a useful concept?

Consider Newton’s second law:

Ftotal = m a  Ftotal · dr= m a ·dr

Wtotal = ½ m vf2 -½ m vi2

Kinetic energy (joules)

PHY 113 C Fall 2013 -- Lecture 7

slide26

Introduction of the notion of Kinetic energy

Some more details:

Consider Newton’s second law:

Ftotal = m a  Ftotal · dr= m a ·dr

Wtotal = ½ m vf2 -½ m vi2

Kinetic energy (joules)

PHY 113 C Fall 2013 -- Lecture 7

slide27

Kinetic energy: K = ½ m v2

units: (kg) (m/s)2 = (kg m/s2) m

N m = joules

Work – kinetic energy relation:

Wtotal = Kf – Ki

PHY 113 C Fall 2013 -- Lecture 7

slide28

Kinetic Energy-Work theorem

  • iclicker exercise:
    • Does this remind you of something you’ve seen recently?
    • Yes
    • No

PHY 113 C Fall 2013 -- Lecture 7

slide29

Kinetic Energy-Work theorem

PHY 113 C Fall 2013 -- Lecture 7

slide30

Kinetic Energy-Work theorem

Example: A ball of mass 10 kg, initially at rest falls a height of 5m. What is its final velocity?

i

0

h

f

PHY 113 C Fall 2013 -- Lecture 7

slide31

A block, initially at rest at a height h, slides down a frictionless incline. What is its final velocity?

Example

h=0.5m

h

0

PHY 113 C Fall 2013 -- Lecture 7

slide32

Example

    • A block of mass m slides on a horizontal surface with initial velocity vi, coming to rest in a distance d.

vi

vf=0

d

Determine the work done during this process.

Analyze the work in terms of the kinetic friction force.

PHY 113 C Fall 2013 -- Lecture 7

slide33

Example -- continued

f

vi

vf=0

d

PHY 113 C Fall 2013 -- Lecture 7

slide34

Example

A mass m initially at rest and attached to a spring compressed a distance x=-|xi|, slides on a frictionless surface. What is the velocity of the mass when x=0 ?

k

0

PHY 113 C Fall 2013 -- Lecture 7

slide35

Special case of “conservative” forces

conservative  non-dissipative

PHY 113 C Fall 2013 -- Lecture 7

slide36

k

PHY 113 C Fall 2013 -- Lecture 7

slide37

iclicker exercise:

  • Why would you want to write the work as the difference between two “potential” energies?
    • Normal people wouldn’t.
    • It shows a lack of imagination.
    • It shows that the work depends only on the initial and final displacements, not on the details of the path.

PHY 113 C Fall 2013 -- Lecture 7

slide39

Energy diagrams

PHY 113 C Fall 2013 -- Lecture 7

slide40

Example: Model potential energy function U(x) representing the attraction of two atoms

PHY 113 C Fall 2013 -- Lecture 7

ad