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Work and Energy. Work is done when an external force is used to change the energy of the system. Energy is the ability to create change or do work. Energy and work are both measured in Joules (J =Nm). Energy and work are scalar quantities. They only have magnitude, no direction. - PowerPoint PPT Presentation
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Work and Energy
Work is done when an external force is used to change the energy of the system.
Energy is the ability to create change or do work.
• Energy and work are both measured in Joules (J =Nm).
• Energy and work are scalar quantities. They only have magnitude, no direction
There are many different forms of Energy:
Kinetic EnergyThe energy of motion.
Is the object moving?
2
2
1mvK
JNmms
kgm
s
mkg
2
2
)(
Gravitational Potential Energy
The energy due to the height of an object.
Does the object have a height?
mghU g JNmm
s
kgmm
s
mkg
22)()(
Elastic Potential Energy
The energy stored in a stretched or compressed spring.
Is there a loaded spring?
2
2
1kxU s
k = The spring constant (N/m)
x = distance stretched or compressed (m)
JNmmm
N
2
Internal EnergyThe energy transferred to the molecules of
the objects in the due to friction.HEAT
Is there a force of friction acting?
xfE intf = The force of friction.
∆x = The distance traveled.
JNmmN ))((
Chemical Potential Energy
The energy released due to a chemical reaction.
Is there a chemical reaction occurring?
ASK A CHEMISTRY TEACHER
FOR THE FORMULA
?cU
Conservation of Energy
For a closed system the sum of the original energy (Eo) and the work (W) done is equal to the final energy (Ef).
fo EWE
Using Pie Charts to understand Energy transfers
Example 1:
A ball is dropped from rest. (Include air friction)
===
BA DC
v = 0m/s A
C
B
D
Ug
Ug
K
Eint
UgK
Eint Eint
K
h = 0
Example 2:
A pendulum swings from A to E
(Neglect air resistance)
===
BA DC
=
E
E
C
V=0m/s
DB
A
V=0m/s
h =0
Ug Ug K K KUg Ug
Example 3:
A spring launches a block across a horizontal table.
===
BA DC
v=0m/s v=0m/s
vv
Us K
Eint
EintKEint
A B C D
Example 4:
A biker rides up a hill with at a constant speed.
v
v
8m
v
v
===
BA DC
h = 0
K KKKUg Ug
UgUC UCUCUC
A
B
C
D
Let’s do some quantitative problems:
Example 1:
A ball is dropped from a height of 15 meters. What is its velocity just before it hits the ground?
v = 0m/s
v
15m
fEWE 0KU g
2
2
1mvmgh
ghv 2
s
mm
s
mv 3.17)15)(10(2
2 h = 0
Example 2:
A pendulum is released from rest at point A and has a velocity of 6 m/s at point C. Find the initial height (h) from which the pendulum was released. (Neglect air resistance)
C
A
V=0m/s
v = 6m/s
h
fEWE 0KU g
2
2
1mvmgh
g
vh
2
2
m
smsm
h 8.1)10(2
)6(
2
2
Example 3:
A spring is compressed 20cm and launches a 400 gram block across a horizontal table. The block comes to rest after traveling 5 meters. The coefficient of friction is 0.6. What is the spring constant (k)?
v=0m/s v=0m/s
5m
fEWE 0
intEU s
xfkx 22
1
2
2
x
xfk
mgFf
2
2
x
xmgk
m
N600
Example 4:
A 70kg biker has a velocity of 10m/s at the bottom of a 8 meter hill. The biker does 6000J of work in climbing the hill and 2000J is transferred to internal energy as he climbs the hill. What is the final velocity of the biker? v
10m/s
8mfEWE 0
fgo KEUK int6000
20002
16000
2
1 22 mghmvmv
2000)8)(10)(70()70(2
16000)10)(70(
2
1 22 v
7600359500 2 v
s
mv 37.7