chapter 7 conservation of energy. recap – work & energy the total work done on a particle is...

33
Chapter 7 Conservation of Energy

Upload: natalie-sellinger

Post on 28-Mar-2015

220 views

Category:

Documents


1 download

TRANSCRIPT

Page 1: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Chapter 7Conservation of Energy

Page 2: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Recap – Work & Energy

2 21 12 2f iW mv mv

The total work done on a particle is equal to the change in its kinetic energy

Page 3: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Potential Energy

The total work done on an object equals the change in its kinetic energy

But the total work done on a system of objects may or may not change its total kinetic energy. The energy may be stored as potential energy.

Page 4: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Potential Energy – A Spring

Both forces do work on the spring. Butthe kinetic energy of the spring is unchanged. The energy is stored as

potential energy

Page 5: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Conservative Forces

If the ski lift takes youup a displacement h, thework done on you, bygravity, is –mgh.

But when you ski downhill the work done by gravity is +mgh, independent of the path you take

Page 6: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Conservative Forces

The work done ona particle bya conservative force is independent of the path takenbetween any two points

Page 7: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Potential-Energy Function

2

12 1

s

sU U U F ds

If a force is conservative, then we candefine a potential-energy function as thenegative of the work done on the particle

Page 8: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Potential-Energy Function

0

0

0

0

0

( ˆˆ ˆ) ( )

( )

ˆ

s

s

s

s

y

y

i

U U U F ds

mg dx dy dz

mg dy

m

k

g y y

j j

potential-energy function associatedwith gravity (taking +y to be up)

0 0( )U U mg y y

The valueof U0 = U(y0)can be set to any convenientvalue

Page 9: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Potential-Energy Function of a Spring

210 2U U kx By convention,

one choosesU0 =U(0) = 0

Page 10: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Force & Potential-Energy Function

dUF

dx

In 1-D, given the potential energy function associated with a force one can compute the latter using:

Example:

212

dUU kx F kx

dx

Page 11: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

7-1Conservation of Energy

Page 12: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Conservation of Energy

inE 0sysE

Energy can be neither created nor destroyed

outE

0sysE Closed System

Open System

Page 13: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Conservation of Mechanical Energy

constantmechE K U

If the forces acting are conservativethen the mechanical energy is conserved

Page 14: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Example 7-3 (1)

How high does the block go?

Initial mechanical energy of system

212iE kx

Final mechanical energy of system

fE mgh

Page 15: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Example 7-3 (2)

Forces are conservative, therefore,mechanical energy is conserved

212 kx mgh

Height reached2

2

kxh

mg

Page 16: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Example 7-4 (1)

How far does the mass drop?

2 21 12 2i i i iE mgy ky mv

Final mech. energy2 21 1

2 2f f ff mgy ky vE m

Initial mech. energy

Page 17: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Example 7-4 (2)

2 21 12 2

2 21 12 2

( ) ( ) (0

(0)

)

(0) (0)mg m

mg d d m

Final mech. energy = Initial mech. energy

2 21 12

2 2

2

2 21 1f f f

i i imgy ky mv

mgy ky mv

Page 18: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Example 7-4 (3)

2mgd

k

Solve for d

12( ) 0kd mg d

2mg

Since d ≠ 0

Page 19: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Example 7-4 (4)

gravE mgd

Note21

2springE kd

2mg

is equal to loss in gravitational potentialenergy

Page 20: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Conservation of Energy & Kinetic Friction

Non-conservative forces, such as kinetic friction, cause mechanical energy to be transformed into other forms of energy, such as thermal energy.

Page 21: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Work-Energy Theorem

Work done, on a system, by external forces is equal to the change in energyof the system

ext sysW EThe energy in a system can be distributed in many different ways

Page 22: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Example 7-11 (1)

ext sysW E

Find speed of blocks after spring isreleased. Consider spring & blocks as system. Write down initial energy.Write down final energy.Subtract initialfrom final

ext sysW E

Page 23: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Example 7-11 (2)

212i iE kx

Initial Energy

ext sysW E

Take potentialenergy of system to be zero initially

Kinetic energy of system is zeroinitially

Page 24: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Example 7-11 (3)

21

2112 2 1

212 20

othermf s m

k

E

m

E

m v m g

E E

gv

E

ms s

Final Energy

ext sysW E

Kinetic and potential energies of system have changed

Page 25: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Example 7-11 (4)

ext f iW E E Subtract initial energy from final energy

ext sysW E

But since noexternal forcesact, Wext = 0, soEf = Ei

Page 26: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Example 7-11 (5)

22 1

1 2

2 2i kkx m g s m g sv

m m

And the answer is…

ext sysW ETry to derivethis.

Page 27: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

E = mc2

In a brief paper in 1905Albert Einstein wrotedown the most famousequation in science

E = mc2

Page 28: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Sun’s Power Output

Power1 Watt = 1 Joule/second100 Watt light bulb = 100 Joules/second

Sun’s power output3.826 x 103.826 x 102626 Watts Watts

Page 29: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Sun’s Power Output

Mass to Energy Kg/s = 3.826 x 10 3.826 x 102626 Watts Watts / (3 x 108 m/s)2

The Sun destroys mass at~ 4 billion kg / s

Page 30: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Problems

To go…

Page 31: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Ch. 7, Problem 19

Page 32: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Ch. 7, Problem 29

Page 33: Chapter 7 Conservation of Energy. Recap – Work & Energy The total work done on a particle is equal to the change in its kinetic energy

Ch. 7, Problem 74