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WORK AND ENERGY Scalars are back

Work and Energy

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Work and Energy. Scalars are back. Review. Equations for Motion Along One Dimension. Review. Motion Equations for Constant Acceleration. 1. 2. 3. 4. Review. 3 Laws of Motion If in Equilibrium If not in equilibrium Change in Motion is Due to Force - PowerPoint PPT Presentation

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Page 1: Work and Energy

WORK AND ENERGYScalars are back

Page 2: Work and Energy

REVIEW Equations for Motion Along One Dimension

dtdx

txv

txv

t

ave

0lim

dtdv

tva

tva

t

ave

0lim

Page 3: Work and Energy

REVIEW Motion Equations for Constant Acceleration

•1.

•2.

•3.

•4.

atvv 0

221

00 attvxx

20vvvave

xavv 220

2

Page 4: Work and Energy

REVIEW 3 Laws of Motion If in Equilibrium

If not in equilibrium Change in Motion is Due to Force

Force causes a change in acceleration

0F

maF

Page 5: Work and Energy

SPRINGS AND OTHER PROBLEMS Force exerted by a

spring is dependent on amount of deformity of the spring

Amount of force applied changes continuously over time

What is the velocity of an object launched from the spring?

Page 6: Work and Energy

WORK Work done on an

object by all forces is equal to the change in kinetic energy of the object.

This definition is valid even if the force is not constant

Page 7: Work and Energy

WORK – CONSTANT FORCE When a force, F, is

doing work on an object, the object will move and be displaced.

The work done, by the force, F, is defined as

Where d is the objects displacement

FdW

Page 8: Work and Energy

WORK – CONSTANT FORCE We are only

interested in the component of the force that is parallel to the direction of motion dFW ||

Page 9: Work and Energy

WORK – CONSTANT FORCE We are only

interested in the component of the force that is parallel to the direction of motion

or

cosFdW

dFW

Page 10: Work and Energy

JOULE

Work done by 1N of force to move an object 1 meter in the same direction

cosFdW

JJouleWmNWmNW

111

11

Page 11: Work and Energy

JAMES PRESCOTT JOULE December 24, 1818-

October 11, 1889 The mechanical

equivalent of heat 838 ft.lbf of work to

raise temperature of 1 lb of water by 1 degree farenheit

Led to the theory of conservation of energy

Helped Lord Kelvin develop the absolute scale of temperature

Page 12: Work and Energy

WORK – ZERO, NEGATIVE, POSITIVE When defining work

done, its always important to specify which force is acting on what object Work done by man Work done by

gravity Work done by

barbell

Page 13: Work and Energy

TOTAL WORK Compute work done

by forces individually

Then just add to get total work done on the object

Note: work is scalar

...21 WWWWtot

Page 14: Work and Energy

EXAMPLE Farmer hitches a tractor

with firewood and pulls it a distance 20m on level ground. Total weight of the sled and wood is 14700N and the tractor pulls with a constant force of 5000N at an angle 36.9o above the horizontal. There is a 3500N friction force opposing the motion. Find the work done by each of the forces and the total work done by all forces.

Page 15: Work and Energy

EXAMPLE

JW

W

dFWJW

WW

dFW

friction

friction

frictionfriction

tractor

tractor

tractor

Tractortractor

70000

)180cos()20)(3500(

cos8000079968

)9.36cos()20)(5000(cos

Page 16: Work and Energy

WORK DONE BY NON-CONSTANT FORCE Requires the use of integrals

Page 17: Work and Energy

ENERGY Energy is a hard to

define concept Simplified definition The ability of a

physical system to do work on another physical system

Many types of energy- these are much easier to define

Page 18: Work and Energy

KINETIC ENERGY Energy of motion When work is done

to an object the object moves

It also affects an objects speed W>0 – object speeds

up W<0 – object slows

down W=0 – no effect

Page 19: Work and Energy

KINETIC ENERGY

Newton’s 2nd LawFdW

madW

Page 20: Work and Energy

KINETIC ENERGY

20

2

20

2

20

2

20

2

20

2

20

2

21

21

2

2

2

2

2

mvmvW

vvmW

ddvvmW

dvva

advv

advv

madW

Page 21: Work and Energy

KINETIC ENERGY

Work done is the change in kinetic energy of an object

This is translational kinetic energy

20

2

21

21 mvmvW

2

21 mvK

Page 22: Work and Energy

WORK – ENERGY THEOREM Assuming mass is

constant

Unit of work is Joules Unit of energy is also

Joules

Note: Energy is also scalar

KW

mvW

2

21

Page 23: Work and Energy

EXAMPLE Farmer hitches a tractor

with firewood and pulls it a distance 20m on level ground. Total weight of the sled and wood is 14700N and the tractor pulls with a constant force of 5000N at an angle 36.9o above the horizontal. There is a 3500N friction force opposing the motion. Suppose it’s initial speed is 2.0 m/s, what is its final speed after travelling 20m.

Page 24: Work and Energy

EXAMPLE

sm

total

total

total

vv

v

v

vvmW

KEWJW

41633.4

2333.13

)2)(1500(2110000

)(21

10000

22

22

20

2

Page 25: Work and Energy

EXAMPLE A 15kg block is

placed on a 40o incline and allowed to slide for 5m. What is it’s final speed? kg15

Page 26: Work and Energy

POTENTIAL ENERGY Energy due to a

body’s configuration or surroundings.

Many different types Springs Electrical Gravitational

Page 27: Work and Energy

GRAVITATIONAL POTENTIAL An object held in the

air has the “potential” to do work once released.

Assume object at some height

After travelling some distance y

00 v

gyv

ygv

advv

2

))((2

2

2

2

20

2

Page 28: Work and Energy

GRAVITATIONAL POTENTIAL An object held in the

air has the “potential” to do work once released.

KE after travelling some distance y

mgyK

mgymvK

gyv

221

212

2

2

Page 29: Work and Energy

GRAVITATIONAL POTENTIAL An object held in the

air has the “potential” to do work once released.

Amount of potential work

mgyKWmgyK

K

00

Page 30: Work and Energy

GRAVITATIONAL POTENTIAL An object held in the

air has the “potential” to do work once released.

Note: choose your origin and be consistent

mgyUPEgrav

Page 31: Work and Energy

EXAMPLE- GIANCOLI 6-28 By how much does the gravitational potential

energy of a 64-kg pole vaulter change if his center of mass rises 4.0m?

Page 32: Work and Energy

EXAMPLE- GIANCOLI 6-28 By how much does the gravitational potential

energy of a 64-kg pole vaulter change if his center of mass rises 4.0m?

JUJU

mgUmgUmgyU

25002500

)4)(8.9)(64()4(0)0(0

Page 33: Work and Energy

WORK DONE EXAMPLE What is work done

to lift a block by 5 m?

If a 40o was used?kg15

Page 34: Work and Energy

CONSERVATIVE AND NON-CONSERVATIVE FORCE Conservative Force Work Done is

independent of the path taken Gravity Elastic Electric

You can “store” energy in these types of systems by doing work on the system

Non Conservative Force

Work done depends on the path taken Friction Air resistance Tension Push-Pull from a

person Cannot define

potential energy for these types of forces

Page 35: Work and Energy

CONSERVATION OF MECHANICAL ENERGY If only gravity is

acting on the object

Valid for all conservative forces

If only conservative forces are acting, the total mechanical energy of a system neither increase nor decrease in any process. It stays constant- it is conserved.00

00 )(UKUKUUKK

UK

UWWKW

grav

Page 36: Work and Energy

CONSERVATION OF MECHANICAL ENERGY If a non-

conservative force is acting on the object

Most common non-conservative energy is friction

NC

NC

NC

grav

NCgrav

NCgrav

WUKUKUKWUWK

UW

KWWW

WWW

00

fdWNC

Page 37: Work and Energy

EXAMPLE – FROM OUR 2ND LECTURE A motorcycle stuntman rides over a cliff. Just

at the cliff edge his velocity is completely horizontal with magnitude 9.0 m/s. Find the motorcycles speed after 0.50s.

Page 38: Work and Energy

LIST THE GIVEN Origin is cliff edge a=-g=-9.80m/s2

At time t=0s

At time t=0.50s

0v

v00 x 00 y

?d?v

smv 0.90

Page 39: Work and Energy

SPLIT INTO COMPONENTS

0v

v

yDxD

DDD

y

x

yx

yx vvv

sm

xv 0.90

00 yv

Page 40: Work and Energy

CALCULATE COMPONENTS INDEPENDENTLY

0v

vxv

yv

sm

xx vv 0.90

sm

y

y

yy

v

gtv

gtvv

9.4

)5.0)(8.9(0

Page 41: Work and Energy

CALCULATE VELOCITY

0v

vxv

yv

sm

xv 0.9s

myv 9.4

sm

sm

yx

xvv

vvv

100.125.10)9.4()0.9( 22

22

Page 42: Work and Energy

NOT NEEDED

29o below the horizontal

0v

v

xv

yv

sm

xv 0.9s

myv 9.4

smxv 100.1

544.099.4tan

x

y

vv

2956.28

smxv 100.1

Page 43: Work and Energy

ALTERNATE SOLUTION

0v

vxv

yv

0

0.9

0

202

10

0

00

UmvK

vUKUK

sm

Page 44: Work and Energy

ALTERNATE SOLUTION

0v

vxv

yv

mygty

gttvyy y

225.1)5.0)(8.9( 2

212

21

221

00

0

0.9

0

202

10

0

00

UmvK

vUKUK

sm

Page 45: Work and Energy

ALTERNATE SOLUTION

0v

vxv

yv

247.101.105

)225.1)(8.9(29

0

0

2

22

20

2

202

1221

00

0

202

10

00

vv

v

gyvv

mgymvmv

UUKKmgyU

UmvK

UKUK

Page 46: Work and Energy

PROBLEM – YOUNG AND FREEDMAN 7.14 A small rock with mass 0.12 kg is fastened to

a massless string with length 0.80 m to form a pendulum. The pendulum is swung so that it makes a maximum angle of 45o with the vertical. (a) What is the speed of the rock when it passes the vertical position? (b) What is the tension in the string when it makes an angle 45o with the vertical? (c) What is the tension in the string when it passes through the vertical?

Page 47: Work and Energy

PROBLEM – SERWAY 7.33 A crate of mass 10.0 kg is pulled up a rough

incline with an initial speed of 1.50 m/s. The pulling force is 100N parallel to the incline, which makes an angle of 20o with the horizontal. The coefficient of kinetic friction is 0.400, and the crate is pulled 5.00m. (a) How much work is done by the gravitational force on the crate? (b) Determine the increase in internal energy of the crate-incline system due to friction. (c) How much work is done by the 100N force on the crate? (d) What is the change in kinetic energy of the crate? (e) What is the speed of the crate after being pulled 5m?

Page 48: Work and Energy

OTHER TYPES OF POTENTIAL ENERGY Elastic Potential For Ideal Springs If a spring is to be

stretched a certain distance x

Where k is the spring constant (the spring’s stiffness)

It’s me again

kxF

Page 49: Work and Energy

POTENTIAL ENERGY OF SPRINGS Restoring Force

Hooke’s Law – valid for small x

kxFs

Page 50: Work and Energy

POTENTIAL ENERGY OF SPRINGS Work done ON the spring

(from equilibrium)

NO Force is not constant We can still use average

force Luckily F varies linearly

with x

))(( xkxWFdWkxF

Page 51: Work and Energy

POTENTIAL ENERGY OF SPRINGS Work done ON the spring

(from equilibrium)

Where U is the elastic potential

221

221

21

021

0

))((

)(

0)0(

kxU

kxW

xkxWdFW

FFFkxFkF

ave

ave

Page 52: Work and Energy

CONSERVATION OF MECHANICAL ENERGY EXPANDED Conservative

With Non conservative

springgravspringgrav UUKUUK 000

NCspringgravspringgrav WUUKUUK 000

Page 53: Work and Energy

YOUNG AND FREEDMAN 7.20 A 1.20kg piece of

cheese was placed on a vertical spring of negligible mass and force constant k=1800 N/m that is compressed 15.0 cm. When the spring is released how high does the cheese rise from its original position?

Page 54: Work and Energy

POWER Rate at which work

is done

SI unit is called the Watt = 1J/s

Horsepower = 550ftlb/s = 746W

TimeWorkPAve

Page 55: Work and Energy

POWER Rate at which work

is done

Efficiency

TimeWorkPAve

aveAve FvtFdP

in

out

PPe

Page 56: Work and Energy

EXAMPLE GIANCOLI 6-58 How long will it take a 1750W motor to lift a

315 kg piano to a sixth story window 16.0m above?

Page 57: Work and Energy

EXAMPLE GIANCOLI 6-58 How long will it take a 1750W motor to lift a

315 kg piano to a sixth story window 16.0m above?

sPWt

JFdWTimeWorkPAve

2.28

4939216)8.9(315

1750

Page 58: Work and Energy

PROBLEM SERWAY 7.40 A 650 kg elevator starts from rest. It moves

upward for 3s with constant acceleration until it reaches its cruising speed of 1.75m/s. (a) What is the average power of the elevator motor during this period? (b) How does this compare when the elevator moves at cruising speed?

Page 59: Work and Energy

YOUNG AND FREEDMAN – 7.42 A 2.00 kg block is pushed against a spring

with negligible mass and force constant k= 400 N/m, compressing it 0.220m. When the block is released, it moves along a frictionless, horizontal surface and then up a frictionless incline with slope 37.0o. (a) what is the speed of the block on the horizontal surface after leaving the spring? (b) How far up the slope does the block travel before starting to slide back down?

Page 60: Work and Energy

GIANCOLI 6-56 A 280 g wood block is firmly attached to the

end of a horizontal spring. The block can slide along the table with a coefficient of friction of 0.30. A force of 22 N compresses the string 18 cm. if the spring is released, how far from the equilibrium position will it stretch at its first maximum extension.

Page 61: Work and Energy

GROUP WORK A 1500 kg rocket is to be launched with an

initial upward speed of 50.0 m/s. In order to assist the engines, the engineers will start it from rest on a ramp that rises 53o above the horizontal. The engines provide a constant forward thrust of 2000N and the coefficient of kinetic friction with the ramp is 0.05. At what height should the rocket start?