Physics 131: Lecture 14 Notes
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Transcript Physics 131: Lecture 14 Notes
Physics 151: Lecture 12
Today’s Topics:
Review Springs
Review Work - Energy Theorem.
Problems we can do with that.
Physics 151: Lecture 13, Pg 1
See text: 7-1
Definition of Work:
Work (W) of a constant force F acting through a displacement r is:
.
W = F r = F r cos = Fr r
Definition of Kinetic Energy :
The kinetic energy of an object of mass (m) moving at speed (v) is:
K = 1/2 m v2
Work Kinetic-Energy Theorem:
Wnet K
K 2 K1
1
1
2
2
mv 2 mv1
2
2
Physics 151: Lecture 13, Pg 2
Question
Planets go around the sun in elliptical orbits. The highly
exaggerated diagram below shows a portion of such an orbit and
the force on the planet at one position along that orbit. The planet
is moving to the right. FT and FR are the components of the force
parallel (tangential) and perpendicular (radial) to the orbit. The
work they do is WT and WR at the position shown
a. WT slows the planet down; WR speeds it up.
b. WT slows the planet down; WR does no work on it.
c. WT speeds the planet up; WR does no work on it.
d. WT speeds the planet up; WR slows it down.
e. WT does no work on it; WR speeds the planet up.
Physics 151: Lecture 13, Pg 3
Act 1
When a crate of mass m is dragged a distance d along a
surface with coefficient of kinetic friction , then dragged back
along the same path to its original position, the work done by
friction is :
(a) 0
(b) -ukmgd
(c) +ukmgd
(d) -2ukmgd
(e) +2ukmgd
Act 2
When a ball rises vertically to a height h and returns to its
original point of projection, the work done by the gravitational
force is :
(a) 0
(b) -mgh
(c) +mgh
(d) -2mgh
(e) +2mgh
Physics 151: Lecture 13, Pg 4
Work Done Against Gravity
Consider lifting a box onto the tail gate of a truck.
m
h
The work required for this task is,
W = F.d
=(mg)(h) (1)
W = mgh
Physics 151: Lecture 13, Pg 5
Work Done Against Gravity
Now use a ramp to help you with the task.
Is less work needed to get the box into the truck?
(It’s “easier” to lift the box)
h
Physics 151: Lecture 13, Pg 6
Work Done Against Gravity
N
F
mgsin
h
mg
mgcos
To push the box with constant speed, F = mgsin
The length of the ramp is h/sin
So the work done is,
W = Fd
= (mgsin)(h/sin)
W = mgh
Same as before !
Physics 151: Lecture 13, Pg 7
Lecture 13 - ACT 3
Work of Springs
I have a spring with k = 20 N/m. Its compressed
30 cm by a 200 gram mass. How much work is
done by the spring in this process ?
A) 0.6 J
B) 6 J
C) 0.9 J
D) –0.9 J
Physics 151: Lecture 13, Pg 8
Act 4
Two clowns are launched from the same spring-loaded
circus cannon with the spring compressed the same
distance each time. Clown A has a 40-kg mass; clown B a
60-kg mass. The relation between their speeds at the
instant of launch is:
a) vA = 3/2 vB
b) vA = (3/2 )1/2 vB
c) vA = vB
d) vB = (3/2 )1/2 vA
e) vB = 3/2 vA
Physics 151: Lecture 13, Pg 9
Example Problem
At the train station, you notice a large horizontal spring at the end of the
track where the train comes in. This is a safety device to stop the train so
that it will not go plowing through the station if the engineer misjudges the
stopping distance. While waiting, you wonder what would be the fastest
train that the spring could stop by being fully compressed, 3.0 ft (~ 1m). To
keep the passengers as safe as possible when the spring stops the train,
you assume that the maximum stopping acceleration of the train, caused
by the spring, is g/2. You make a guess that a train might have a mass of
0.5 million kilograms. For the purpose of getting your answer, you assume
that all frictional forces are negligible.
You find the maximum speed the train can have is:
(A) < 5 mph
(B) between 5mph and 10mph
(C ) > 10 mph
( Note: 1 m/s ~ 2 mph )
Physics 151: Lecture 13, Pg 10
Lecture 13, ACT 5
Work & Energy
Two blocks having mass m1 and m2 where m1 > m2. They are
sliding on a frictionless floor and have the same kinetic energy
when they encounter a long rough stretch (i.e. m > 0) which
slows them down to a stop.
Which one will go farther before stopping ?
(a) m1 (b) m2
(c) they will go the same distance
m1
m2
Physics 151: Lecture 13, Pg 11
Lecture 13, ACT 6
Work & Energy
You like to drive home fast, slam on your brakes at the bottom
of the driveway, and screech to a stop laying rubber all the
way. It’s particularly fun when your mother is in the car with
you. You practice this trick driving at 20 mph and with some
groceries in your car with the same mass as your mama. You
find that you only travel half way up the driveway. Thus when
your mom joins you in the car, you try it driving twice as fast.
How far will you go this time ?
(a) The same distance. Not so exciting.
(b) 2 times as far (only 7/10 of the way up the driveway)
(c) twice as far, right to the door. Whoopee!
(d) four times as far. Crashes into house. Sorry Ma.
Physics 151: Lecture 13, Pg 12
Another Example
A 3.0-kg block is dragged over a rough horizontal
surface by a constant force of 16 N acting at an
angle of 37° above the horizontal as shown. The
speed of the block increases from 4.0 m/s to 6.0
m/s in a displacement of 5.0 m. What work was
done by the friction force during this displacement?
a.
b.
c.
d.
e.
–34 J
–64 J
–30 J
–94 J
+64 J
Physics 151: Lecture 13, Pg 13
Another Example
1. You have been hired to design a spring based toy pistol. The
design criterion states that you have to be able to shoot an
extremely aerodynamic bullet of mass 50 grams a distance of 20
meters. Unfortunately, there are not that many choices you can
make, because the company insists on you using the left-over
plastic gun-bodies from a previous, failed product. You do
however have to design an appropriate spring. The gun body has
a barrel of length 10 cm on the outside and 8 cm on the inside.
The entire plastic body has a mass of 150g. You figure that the
spring can fill the entire barrel, and can probably have a maximum
compression to about half of its original length.
What is the design of your spring ?
(k=? )
k = 6.2 kN/m
Physics 151: Lecture 13, Pg 14
Recap of today’s lecture
Work/Energy Theorem
W = K
Kinetic Energy
K = 1/2 mv2
Physics 151: Lecture 13, Pg 15