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
v0
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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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