Transcript Chapter 6

Fundamentals of Physics
Chapter 7 Kinetic Energy & Work
1. Energy
2. Work
3. Work & Kinetic Energy
4. Work Done by a Gravitational Force
5. Work Done by a Spring Force
6. Work Done by a General Variable Force
7. Power
Review & Summary
Questions
Exercises & Problems
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Energy & Work
Energy comes in many forms:
• Thermal, Chemical, Atomic, Nuclear Energies
•
Energy is conserved.
• A new tool to solve problems.
•
Descriptions of Energy:
• Potential Energy (Chapter 7)
• Kinetic Energy - motion of a massive object
Kinetic Energy 
Units :
2009
1
2
m v2
kg m 2
1 Joule  1
s2
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WOW!
August 10, 1972, a large meteorite skipped across the atmosphere.
m  4 106 kg
v  15 m s
KE 
1
2
m v 2  0  5 1014 J
KE  0.1 MT  8 WWII atomic bombs
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“Work”
•
Work (W) is energy transferred to or from an object by means of a force acting
on the object.
– Energy transferred to the object is positive work.
– Stepping on the gas causes positive work to be done on a car.
– Energy transferred from the object is negative work.
– Stepping on the brakes causes negative work to be done on a
moving car.
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Work & Kinetic Energy
Consider a force acting on an object constrained to move in the x-direction:
v 2  v02  2 ax d
Frictionless Wire
v 2  v02  2 a x d
1
2
m v 2  12 m v02  m ax d
1
2
m v 2  12 m v02  Fx d
The force causes a change in kinetic energy; the force does work:
"Work "  Fx d  F cos  d
Units: 1 Joule = 1 kg (m / s)2 = (1 kg m / s2) m = 1 N m
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A force acting on a particle moving along a curve:
F does no work.
Work  FS s
F does not change the velocity.
cos   cos 900  0
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Work  F cos  s

Work  F  s
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“Work”
 
W  F  d  F cos  d
 Work (W) is energy transferred to or from an object by means of a force
acting on the object.
– A force does positive work when it has a vector component in the same
direction as the displacement.
– A force does negative work when it has a vector component in the
opposite direction as the displacement.
– A force does zero work when it is perpendicular to the displacement.
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Work – Kinetic Energy Theorem
W  FS ds
W 
aS 

s2
s1
FS ds 

s2
s1
m aS ds
dv
dv ds
dv

v
dt
ds dt
ds
chain rule for derivatives
v
dv
ds

m
s1 ds
v0 v dv
2
W  12 m v 2  12 m v0
W  K f  Ki
W 
s2
mv
W  K
Net Work Done
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= Change in Kinetic Energy
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Scalar (Dot) Product of Two Vectors
 
a  b  a b cos 
Commutative Law:
 
 
a b  b  a
 
a  b  ax bx  a y by  az bz
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Example

Work  F  s
W  Fx x  Fy y
W  3N 2m   4 N  5m 
W   14 Nm
Tipler p 157
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Example:
vf = ?
s  57 m
v0  3.6 m s
m  58 kg
f K  70 N

Work  Fnet s

Fnet  m g sin 250  f K
m g sin 25
0

 fK s 
1
2
m v f  12 m v0
2
2
v f  19 m s
Cutnell p 160
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Work done by the forces on the box?

N

F
F  210 N
  200
mg
d  3m
 
WF  F  d
WF  F d cos  (210 N )(3 m) cos(200 )  600 J
WN
 
 N d
WN  N d cos(900 )  0  Wg
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Object sliding on a frictionless floor
Work = ?
v0  0
F1  3.00 N
F2  4.00 N
F3  10.0 N
Fnet x   F1  F2 sin 500  F3 cos 350
Fnet y   F2 cos 500  F3 sin 350
Fnet 2  Fnet x 2  FnetY 2
Since v0  0, d is parallel to Fnet :
W  Fnet d
W  15.3 J
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Work Done by the Gravitational Force
Going down:
 
W  F d
W  m g d cos 00
W  m g d
The work done by the gravity
force increased the kinetic
energy of the object.
Going up:
 
W  F d
W  m g d cos1800
W  m g d
The work done by the gravity force
reduced the kinetic energy of the object.
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Work Done Lifting & Lowering an Object
To raise an object to a new location, an applied force, F, must act to overcome the gravity
force, Fg.
Consider a case where an object is at rest before and after the move.
Work- Energy Theorem:
Kf - Ki = Wa + Wg
But Kf = Ki = 0:
0 = Wa + Wg
Wa = - Wg
The work done by the applied force is the
negative of the work done by the
gravitational force.
Raising
Wa  m g d
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Lowering
Wa   m g d
The work done by the lifter.
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Pull with constant force F.

F
 
F F


F  ma
2 F  mg  ma  0
F 
1
2
mg

F
Is less energy expended or less work done when
using a pulley (or other such device)?
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Pull with constant force F.

F
 
F F


F  ma
2 F  mg  ma  0
F 
1
2
mg
d
2d
W  ( F )(2d )
W  mgd
W  (2 F )(d )
W  mgd
Same amount of work!
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An object accelerated downwards
a = g/4
drops d
Work by cord ?
Work by gravity?
Final velocity
v0  0


F  ma
 g
T  mg  M a  M   
 4
T  34 M g
T
WT    34 M g  d
Wg   M g d

aa

d
Wnet   14 M g d
Mg
Work Energy Theorem:
K  K 0  Wnet
1
2
M v2  0 
1
4
v  
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M gd
1
2
gd
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Work Done by a Spring Force
Relaxed
Hooke’s Law:


F  k d
where k = spring constant (N/m)
Stretching
The force varies linearly with displacement.
Compressing
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Work Done by a Spring Force


F  k d
Hooke’s Law:
Relaxed
Work done by the spring force:
WS 

xf
xi
F ( x ) dx
WS   k 
xf
xi
Stretching
WS 
1
2
x dx   1 2 k x 2
k xi2 
WS   12 k x 2
1
2
xf
xi
k x 2f
( xi  0)
Wa  WS
Compressing
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A block is dropped on a relaxed spring
Wg  m g d
m = 250 g
k = 2.5 N/cm
d = 12 cm
Wg ? W s?
v?
WS   1 2 k d 2
Wnet  Wg  WS
Wnet  K f  K i
mgd 
1
2
k d2  0 
1
2
mv 2
v
d
v0
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v 
k 2
  d  2gd
 m
v  35
. ms
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Work – Kinetic Energy Theorem with a Variable Force
WS 

xf
F ( x ) dx  m
xi

xf
a x dx
xi
dv
dx
a x dx 
dx 
dv  v dv
dt
dt
W  m

xf
xi
v dv 
1
vf
2
mv 2 v
i
W  KE f  KEi
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Problem
A 10 kg brick moves with the following variable acceleration; how much work is done on the
brick in the first 8 seconds.
a  x
20 m s2

 2.5 s 2
8m
a  2.5 x
WS 
W 
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
F ( x ) dx  2.5 m 
xf
xi
2 .5
xf
xi
8
2
m x2 0 
2 .5
2
x dx
(10)(8) 2  800 J
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Power
Power = time rate at which Work is done due to a Force.
P 
SI Units:
dW
dt
1 Watt = 1 Joule / s = 1 N m / s
English Units: horsepower
1 hp = 550 ft lbs / s = 746 Watts
For a constant force:


 
 
d F d
P 
 F v
dt
Work = Power x Time
1 kW hr = 3.6 x 106 J
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