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EnergyEnergy is anything that can be con-verted into work; i.e., anything that can exert a force through a distance.
Energy is the ability to do work.
Kinetic EnergyKinetic Energy: Ability to do work by virtue of motion. (Mass with velocity)A speeding car
or a space rocket
Types of Mechanical Energy
• KE = ½ mass x velocity2
• KE = ½ mv2
Examples of Kinetic Energy
2 21 12 2 (1000 kg)(14.1 m/s)K mv
2 21 12 2 (0.005 kg)(200 m/s)K mv
What is the kinetic energy of a 5-g bullet traveling at 200 m/s?
5 g
200 m/s KE = 100 JKE = 100 J
How fast must a 700 kg car drive in order to have 78,750 J of kinetic
energy?𝐾=
12𝑚𝑣2
78,750 𝐽=12(700𝑘𝑔)𝑣2
𝒗=𝟏𝟓𝒎𝒔
Potential EnergyPotential Energy: Ability to do work by virtue of position or condition.
A stretched bowA suspended weight
Types of Mechanical Energy
Gravitational Potential Energy
• PEg = weight x height• PEg = [mass X gravitational acceleration] X
height
• PEg = mgh
Elastic Potential Energy
What is the potential energy of a 50 kg person in a skyscraper if he is 480 m above the street below?
A typical 747 airplane flying at an altitude of 11 km has 2.7x1010 Joules of gravitational potential energy. What is the mass of this airplane?
Examples of Potential Energy
PE = mgh = (50 kg)(9.8 m/s2)(480 m)
PE = 235,200 JPE = 235,200 J
PE = mgh2.7x1010 J = (m)(9.8 m/s2)(11,000 m)m = 250,464 kg
Heat Energy• Energy from the internal
motion of particles of matter The hotter something is,
the faster its molecules are moving around and/or vibrating, i.e. the more energy the molecules have.
Nuclear Energy• Energy from the
nucleus of the atom– Fusion is when
two atoms combine• The Sun
– Fission is when the atom splits• Nuclear power
plant
Mass-Energy Equivalence: E=mc2
16
Conservation of Energy
Students will:
a) Identify situations on which conservation of mechanical energy is valid.
b) Recognize the forms that conserved energy can take.
c) Solve problems using conservation of mechanical energy.
17
Mechanical Energy
• Mechanical Energy is the sum of kinetic energy and all forms of potential energy in a system.
• In the absence of “nonconservative” resistive forces like friction and drag, mechanical energy is conserved.
• When we say that something is conserved, we mean that it remains constant.
18
THE PRINCIPLE OF CONSERVATION OF MECHANICAL ENERGY
The Total Mechanical Energy (TME) of an object remains constant as the object moves, in the absence of friction.
finalinitial TMETME
ffii PEKEPEKE
constantTME
19
Con
serv
atio
n of
Ene
rgy
All Potential Energy, no Kinetic Energy
1/2 Potential Energy, 1/2 Kinetic Energy
1/4 Potential Energy, 3/4 Kinetic Energy
No Potential Energy, all Kinetic Energy
3/4 Potential Energy, 1/4 Kinetic Energy
20
If friction and wind resistance are ignored, a bobsled run illustrates how kinetic energy can be converted to potential energy, while the total mechanical energy remains constant.
22
fffinal mghmvTME 221
Example 1: A person on top of a building throws a 4 kg ball upward with an initial velocity of 17 m/s from a height of 30 meters. If the ball rises and then falls all the way to the ground, what is its velocity just before it hits the ground?
17 m/s
30 m
continued on next slide
m = 4 kg vi = 17 m/s vf = ?
g = 9.8 m/s hi = 30 m hf = 0 m
iiinitial mghmvTME 221
23
ffii mghmvmghmv 2212
21
)30)(8.9)(4()17)(4( 22
21 mkgkg
sm
sm
)0)(8.9)(4()4( 22
21 mkgvkg
sm
f
JJ 1176578 Jvkg f 0)4( 221
J1754 221 )4( fvkg
2
2
877sm 2
fvsm6.29 fv
Example 1 continued:
24
Example 2: A 10 kg stone is dropped from a height of 6 meters above the ground. Find the Potential Energy, Kinetic Energy, and velocity of the stone when it is at a height of 2 meters.
6 m
At 6 m:
TME = PEi + KEi= mghi + ½ mvi2
= (10 kg)(9.8 m/s)(6 m) + ½ (10 kg)(0 m/s)2
= 588 J + 0 J
= 588 J
2 m
At 2 m:
TME = PEf + KEf = mghf + ½ mvf2
= (10 kg)(9.8 m/s)(2 m) + ½ (10 kg)(vf)2
= 196 J + ½ (10 kg)(vf)2
Therefore: 588 J = 196 J + ½ (10 kg)(vf)2
588 J – 196 J = ½ (10 kg)(vf)2
392 J = ½ (10 kg)(vf)2
solve for vf = 8.9 m/s
25
Example 3: A Daredevil MotorcyclistA motorcyclist (300 kg including the bike) is trying to leap across the canyon by driving horizontally off a cliff with an initial speed of 38.0 m/s. Ignoring air resistance, find the speed with which the cycle strikes the ground on the other side.
38.0 m/s
70 m70 m70 m
55 m
vf = ?
26
ffii mghmvmghmv 2212
21
)70)(8.9)(300()38)(300( 22
21 mkgkg
sm
sm
)55)(8.9)(300()300( 22
21 mkgvkg
sm
f
JJ 800,205600,216 Jvkg f 700,161)300( 221
J700,260 221 )300( fvkg
2
2
1738sm 2
fvsm7.41 fv
Example 3 continued
27
•Example 4:Starting from rest, a child on a sled zooms down a frictionless slope from an initial height of 8.00 m. What is his speed at the bottom of the slope? Assume he and the sled have a total mass of 40.0 kg.
??
:
0
0
0.40
00.8
:
f
f
sm
i
i
v
Unknown
mh
v
kgm
mhh
Given8.00 m
ffii
sm
ff
fff
sm
ii
sm
ii
PEKEPEKE
JmkgmghPE
vkgmvKE
JmkgmghPE
JkgmvKE
0081.90.40
)0.40(
313900.881.90.40
000.40
2
2
2212
21
2
212
21
continued on next slide
28
fsm
fsm
fsm
f
f
f
v
v
v
vkg
J
vkgJ
vkgJJ
5.12
157
157
20
3139
203139
00.4031390
2
2
2
2 2
2
2
221
•Example 4 - continued
ffii PEKEPEKE
answer
Example 5: Unknown MassA skier starts from rest and slides down the frictionless slope as shown. What is the skier’s speed at the bottom?
H=40 m
L=250 m
start
finish
continued on next slide
m = unknown vi = 0 m/s vf = ?
g = 9.8 m/s hi = 40 m hf = 0 m
30
Example 5: Unknown Mass - continued
ffii PEKEPEKE
ffii mghmvmghmv 2212
21
You can divide the mass out of the above equation.
ffii mghmvmghmv 2212
21
)40)(8.9()0( 22
21 m
sm
sm )0)(8.9( 2
221 mv
sm
f
2
2392s
m 221
fv
sm28 fv