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Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

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Page 1: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Chapter 5B - Work and Energy

A PowerPoint Presentation by

Paul E. Tippens, Professor of Physics

Southern Polytechnic State University© 2007

Page 2: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

The Ninja, a roller coaster at Six Flags over Georgia, has a height of 122 ft and a speed of 52 mi/h. The potential energy due to its height changes into kinetic energy of motion.

Page 3: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Objectives: After completing this module, you should be able

to:• Define kinetic energy and potential energy,

along with the appropriate units in each system.

• Describe the relationship between work and kinetic energy, and apply the WORK-ENERGY THEOREM.

• Define and apply the concept of POWER, along with the appropriate units.

Page 4: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

EnergyEnergyEnergyEnergy is anything that can be con-is anything that can be con-verted into work; i.e., anything that verted into work; i.e., anything that can exert a force through a can exert a force through a distancedistance.

Energy is the capability for doing Energy is the capability for doing work.work.

Page 5: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Potential Energy

Potential Energy:Potential Energy: Ability to do work Ability to do work by virtue of position or conditionby virtue of position or condition.

A stretched bowA stretched bowA suspended weightA suspended weight

Page 6: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example Problem: What is the potential energy of a 50-kg person in a

skyscraper if he is 480 m above the street below?

Gravitational Potential Gravitational Potential EnergyEnergy

What is the P.E. of a 50-kg person at a height of 480 m?

U = mgh = (50 kg)(9.8 m/s2)(480 m)

U = 235 kJU = 235 kJ

Page 7: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Kinetic Energy

Kinetic Energy:Kinetic Energy: Ability to do work Ability to do work by virtue of motion. (Mass with by virtue of motion. (Mass with velocity)velocity)A speeding car A speeding car

or a space or a space rocketrocket

Page 8: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Examples of Kinetic Energy

What is the kinetic energy of a 5-g What is the kinetic energy of a 5-g bullet traveling at 200 m/s?bullet traveling at 200 m/s?

What is the kinetic energy of a What is the kinetic energy of a 1000-kg car traveling at 14.1 m/s? 1000-kg car traveling at 14.1 m/s?

5 g5 g

200 200 m/sm/s

K = 100 JK = 100 J

K = 99.4 JK = 99.4 J

2 21 12 2 (0.005 kg)(200 m/s)K mv

2 21 12 2 (1000 kg)(14.1 m/s)K mv

Page 9: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Work and Kinetic EnergyA resultant force changes the velocity A resultant force changes the velocity

of an object and does work on that of an object and does work on that object.object.

m

vo

m

vfx

F F

( ) ;Work Fx ma x 2 2

0

2fv v

ax

2 21 102 2fWork mv mv

Page 10: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

The Work-Energy TheoremWork is Work is equal to the equal to the change inchange in ½mv½mv22

If we define If we define kinetic energykinetic energy as as ½mv½mv22 then we can state a very important then we can state a very important

physical principle:physical principle:

The Work-Energy Theorem:The Work-Energy Theorem: The work The work done by a resultant force is equal to done by a resultant force is equal to the change in kinetic energy that it the change in kinetic energy that it produces.produces.

2 21 102 2fWork mv mv

Page 11: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example 1: A 20-g projectile strikes a mud bank, penetrating a distance of 6 cm before stopping. Find the stopping force F

if the entrance velocity is 80 m/s.x

F = ?F = ?

80 80 m/sm/s

6 cm6 cmWork = ½Work = ½ mvmvff

2 2 - ½- ½ mvmvoo

22

0

F x = - F x = - ½½ mvmvoo22

FF (0.06 m) cos 180 (0.06 m) cos 18000 = - = - ½½ (0.02 kg)(80 (0.02 kg)(80 m/s)m/s)22

FF (0.06 m)(-1) = -64 J (0.06 m)(-1) = -64 J F = 1067 NF = 1067 N

Work to stop bullet = change in K.E. for Work to stop bullet = change in K.E. for bulletbullet

Page 12: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example 2: A bus slams on brakes to avoid an accident. The tread marks of the tires are 80 m long. If k = 0.7, what was

the speed before applying brakes?2525 mm fff = f = k.k.n = n = k k mgmg

Work =Work = F(F(cos cos ) ) xx

Work = - Work = - k k mg mg xx

0K =K = ½½ mvmvff

2 2 - ½- ½ mvmvoo22

-½-½ mvmvoo22 = - = -k k mgmg xx vvoo = = 22kkgxgx

vo = 2(0.7)(9.8 m/s2)(25 m) vo = 59.9 ft/s

vo = 59.9 ft/s

Work = K

K = Work

Page 13: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example 3: A 4-kg block slides from rest at top to bottom of the 300 inclined plane. Find velocity at bottom. (h = 20 m and k =

0.2)

hh3030

00

nnff

mgmg

xx

Plan: Plan: We must calculate We must calculate both the resultant work both the resultant work and the net displacement and the net displacement xx. Then the velocity can . Then the velocity can be found from the fact be found from the fact that that Work = Work = K.K.

Resultant work = (Resultant force down Resultant work = (Resultant force down the plane) the plane) xx (the (the displacement down the displacement down the plane)plane)

Page 14: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example 3 (Cont.): We first find the net displacement x down the plane:

h

300

nf

mg

x

From trig, we know that the Sin From trig, we know that the Sin 303000 = = h/x h/x and:and:

0

20 m40 m

sin 30x 0sin 30

h

x

hx

303000

Page 15: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example 3(Cont.): Next we find the resultant work on 4-kg block. (x = 40 m

and k = 0.2)

WWyy = = (4 kg)(9.8 m/s(4 kg)(9.8 m/s22)(cos 30)(cos 3000) = 33.9 N

hh

303000

nnff

mgmg

x = x = 4040

mm

Draw free-body diagram to find the resultant Draw free-body diagram to find the resultant force:force:

nnff

mgmg303000

x

y

mgmg cos 30 cos 3000 mgmg sin 30 sin 3000

WWxx = = (4 kg)(9.8 m/s(4 kg)(9.8 m/s22)(sin 30)(sin 3000) = 19.6 N

Page 16: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example 3(Cont.): Find the resultant force on 4-kg block. (x = 40 m and k = 0.2)

nnff

mgmg303000

x

y

33.9 N33.9 N19.6 N19.6 N

Resultant force down Resultant force down plane: plane: 19.6 N - 19.6 N - ffRecall that Recall that ffkk = = k k

nnFFyy = 0 or = 0 or nn = 33.9 = 33.9 NN

Resultant Force = 19.6 N – kn ; and k = 0.2Resultant Force = 19.6 N – (0.2)(33.9 N) = 12.8 N

Resultant Force Down Plane = 12.8 N

Page 17: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example 3 (Cont.): The resultant work on 4-kg block. (x = 40 m and FR = 12.8

N)(Work)(Work)RR = = FFRRxx

FFRR

303000

xxNet Work = (12.8 N)(40 m)Net Work = 512 J

Finally, we are able to apply the work-energy theorem to find the final velocity:

2 21 102 2fWork mv mv

0

Page 18: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example 3 (Cont.): A 4-kg block slides from rest at top to bottom of the 300 plane. Find velocity at bottom. (h = 20 m and k

= 0.2)

hh3030

00

nnff

mgmg

xx Resultant Work = Resultant Work = 512 J512 JWork done on block Work done on block

equals the change in K. equals the change in K. E. of block.E. of block.

½½ mvmvff2 2 - ½- ½ mvmvoo

22 = = WorkWork

0 ½½ mvmvff

22 = = 512 J512 J

½½(4 kg)(4 kg)vvff22 = 512 = 512

JJ vf = 16 m/svf = 16 m/s

Page 19: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

PowerPower is defined as the rate at

which work is done: (P = dW/dt )

10 kg

20 mh

m

mg

t

4 s

F

Power of 1 W is work done at rate of 1 J/s

Power of 1 W is work done at rate of 1 J/s

Work F rPower

time t

Work F rPower

time t

2(10kg)(9.8m/s )(20m)

4 s

mgrP

t

490J/s or 490 watts (W)P 490J/s or 490 watts (W)P

Page 20: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Units of Power

1 W = 1 J/s and 1 kW = 1000 W

One watt (W) is work done at the rate of one joule per second.

One ft lb/s is an older (USCS) unit of power.One horsepower is work done at the rate of 550 ft lb/s. ( 1 hp = 550 ft lb/s )

Page 21: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example of Power

Power Consumed: P = 2220 W

Power Consumed: P = 2220 W

What power is consumed in lifting a 70-kg robber 1.6 m in

0.50 s?Fh mghP

t t

2(70 kg)(9.8 m/s )(1.6 m)

0.50 sP

Page 22: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example 4: A 100-kg cheetah moves from rest to 30 m/s in 4 s. What is the power?

Recognize that work is equal Recognize that work is equal to the change in kinetic to the change in kinetic energy:energy: Work

Pt

2 21 102 2fWork mv mv

2 21 12 2 (100 kg)(30 m/s)

4 sfmv

Pt

m = 100 kg

Power Consumed: P = 1.22 kW

Power Consumed: P = 1.22 kW

Page 23: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Power and VelocityRecall that average or constant

velocity is distance covered per unit of time v = x/t.

P = = Fx

t

F x

tIf power varies with time, then calculus is needed to integrate over time. (Optional)

Since P = dW/dt: ( )Work P t dt ( )Work P t dt

P FvP Fv

Page 24: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example 5: What power is required to lift a 900-

kg elevator at a constant speed of 4 m/s?

v = 4 m/s

P = (900 kg)(9.8 m/s2)(4 m/s)

P = F v = mg v

P = 35.3 kW

P = 35.3 kW

Page 25: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Example 6: What work is done by a 4-hp mower in one hour? The

conversion factor is needed: 1 hp = 550 ft lb/s.

Work = 132,000 ft lb

Work = 132,000 ft lb

550ft lb/s4hp 2200ft lb/s

1hp

(2200ft lb/s)(60s)Work

; Work

P Work Ptt

Page 26: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

The Work-Energy Theorem:The Work-Energy Theorem: The work The work done by a resultant force is equal to the done by a resultant force is equal to the change in kinetic energy that it produces.change in kinetic energy that it produces.

The Work-Energy Theorem:The Work-Energy Theorem: The work The work done by a resultant force is equal to the done by a resultant force is equal to the change in kinetic energy that it produces.change in kinetic energy that it produces.

SummaryPotential Energy:Potential Energy: Ability to do Ability to do work by virtue of position or work by virtue of position or conditioncondition.

U mgh

Kinetic Energy:Kinetic Energy: Ability to do work Ability to do work by virtue of motion. (Mass with by virtue of motion. (Mass with velocity)velocity)

212K mv

Work = ½ mvf2 - ½

mvo2

Work = ½ mvf2 - ½

mvo2

Page 27: Chapter 5B - Work and Energy A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007

Summary (Cont.)

Power is defined as the rate at which work is done: (P = dW/dt )

WorkP

t

Work F rPower

time t

Work F rPower

time t

Power of 1 W is work done at rate of 1 J/s

Power of 1 W is work done at rate of 1 J/s

P= F v