Physics 106 - How Things Work - Spring, 1998
Problem Set 1 - Answers
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Due Monday, February 2, 1998, in class
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Please answer each problem as concisely as possible
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You may discuss the problems with one another but you must write them
up separately and in your own words.
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There are 5 problems containing a total of 24 parts. Each part will be
worth 4 points.
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You will receive an additional 4 points for writing your name legibly on
the problem set before turning it in.
Problem 1: Chapter 1, Case 1a-e (Pg. 72)
You’re riding on a playground swing. You’re traveling back and forth
once every few seconds.
a. At what point(s) in your motion is your velocity zero?
Answer: At the end or peak of each swing.
Why: As the you approaches the end of a swing, you are accelerating
directly backward and you slow to a complete stop. You continue to accelerate
in that same direction and thus reverse your direction of travel.
b. At what point(s) in your motion is your gravitational potential
energy at its maximum?
Answer: At the end or peak of each swing.
Why: At the end of a swing, you are as high up as you ever get.
Since gravitational potential energy is proportional to altitude, this
highest point is also the point at which your gravitational potential energy
is at its maximum.
c. At what point(s) in your motion is your kinetic energy at its
maximum?
Answer: At the bottom or middle of each swing (when you a directly
below the support for the ropes).
Why: When you are at the bottom of a swing, you are as low down
as you ever get. Since your gravitational potential energy is then at its
minimum, your kinetic energy must be at its maximum. Equivalently, your
speed is greatest at the bottom of the swing because you have been accelerating
partially forward up to that point. Since kinetic energy is proportional
to speed squared, your kinetic energy is also maximum. Once you pass the
bottom of the swing, you begin to accelerate partially backward and lose
both speed and kinetic energy.
d. As you reach the bottom of a swing, when the swing’s ropes are
exactly vertical, are you accelerating?
Answer: Yes.
Why: At the bottom of the swing, your speed is not changing
but your direction of travel is. You are accelerating upward. To see that
this is the case, note that your direction of travel is tipping more and
more upward throughout your swing, meaning that the direction of your velocity
goes from significantly downward near the start of the swing to significantly
upward near the end of the swing. For your velocity to tip upward in this
manner, you must be accelerating partially upward. At the bottom of the
swing, you are accelerating directly upward!
e. At the moment described in d, is the force that the ropes exert
on you more, less, or equal to your weight?
Answer: More than your weight.
Why: Since you are accelerating upward at the bottom of the
swing, the net force on you must be upward. This can only occur if the
ropes are pulling upward on you with a force that is larger in magnitude
than your weight. That way, you are pulled upward harder than you are pulled
downward and you accelerate upward. That's how your velocity tips more
and more upward so that you follow an upward circular arc rather than falling
or heading in a straight line.
Problem 2: Chapter 1, Case 17a-e (Pg. 75)
You’re seated in a crowded bus that has stopped at a bus stop. Two people
board the bus, one wearing rubber-soled shoes and one wearing inline skates
(roller skates — i.e., no friction). They both have to stand in the middle
of the aisle and neither one holds onto anything.
a. The bus driver is new and the bus lurches forward from the
bus stop. Which way does the person wearing inline skates move in relationship
to the bus?
Answer: The skater moves backward relative to the bus (but stays
in one place relative to the bus stop).
Why: As the bus accelerates away from the bus stop, the ground
pushes it forward. To remain with the bus, the skater also needs a forward
force but the skates prevent the
bus from exerting such a forward force on the skater. The wheels of
the skates just spin. So instead of accelerating forward, the skater remains
in place in front of the bus
stop and the bus drives out from under the skater. To the passengers
on the bus, the skater rolls backward through the isle and hits the back
of the bus.
b. The bus is accelerating forward as it pulls away from the bus
stop. Why doesn’t the person wearing inline skates accelerate with the
bus?
Answer: The bus can't exert the forward force on the skater
that the skater needs to accelerate forward with the bus.
Why: The skate wheels turn as the bus accelerates forward, so
that the skater doesn't experience the forward frictional force that a
person in normal shoes would need to
accelerate with the bus.
c. The person wearing rubber-soled shoes remains in place as the
bus starts moving. What provides the force that causes that person to accelerate
with the bus?
Answer: (Static) friction.
Why: Static friction between the bus floor and the person's
rubber-soled shoes pushes the person forward and the bus floor backward.
As a result, the person accelerates with
the bus and the bus accelerates somewhat more slowly than it would
have had the person not been in the bus.
d. Once the bus has reached a constant velocity (it’s traveling
along a straight road at a steady pace), the person wearing inline skates
is able to stand comfortably in the aisle without rolling anywhere. What
is the net force on the person wearing skates?
Answer: Zero.
Why: Since the bus and the skater are both moving at constant
velocity, neither one is accelerating. The skater (like the bus) is experiencing
zero net force.
e. The driver accidentally runs into a curb and the bus stops so
abruptly that everything slides forward, including the person wearing rubber-soled
shoes. In stopping quickly, the bus experiences an enormous backward acceleration.
Why doesn’t the person wearing rubber-soled shoes accelerate backward with
the bus?
Answer: The force of static friction can't provide enough backward
force to slow the person with the bus.
Why: When the bus stops gradually, static friction between the
shoes and the bus floor exert enough backward force on the person wearing
the shoes to make that person
accelerate backward with the bus. However, when the bus stops suddenly,
the force required to accelerate the person backward with the bus is greater
than the maximum
force that static friction can supply. The shoes begin to slide across
the floor and the person skids forward in the bus.
Problem 3: Chapter 1, Case 18a-e (Pg. 75)
You’re about to go on a bicycle trip through the mountains. Being ambitious,
you decide to take two children along. The children sit in a trailer that
you pull with your bicycle.
a. As you wait to begin your trip, you and your bicycle are motionless.
What is the net force on your body?
Answer: Zero.
Why: You are not accelerating so the net force on you must be
zero!
b. You begin to bicycle into the mountains. You soon find yourself
ascending a steep grade. The road rises smoothly uphill and you’re traveling
up it at a steady pace in a straight line. You’re traveling at a constant
velocity up the hill. What is the net force on your body?
Answer: Zero.
Why: You are still not accelerating (your velocity is constant)
so the net force on you must be zero!
c. The road rises 1 m upward for every 10 m you travel along its
surface. If the children and their trailer weigh 400 N, how much uphill
force must you exert on the trailer to keep it moving uphill at a constant
velocity?
Answer: 40 N
Why: Since the children and trailer weigh 400 N, lifting them
directly upward a distance of 1 m will require 400 N-m of work (400 N of
upward force times 1 m of distance in the direction of that upward force).
Because energy is conserved, raising the children and trailer 1 m upward
through any other path will also require 400 N-m of work (assuming that
you increase only their gravitational potential energy, which is why this
problem mentions that you do everything at constant velocity). If pulling
the children and trailer up a ramp that's 10 m long will raise them 1 m,
then you will be doing 400 N-m of work over a distance of 10 m. That requires
the force you exert on the children to be 40 N, so that the work you do
(40 N of uphill force times 10 m of distance in the direction of that uphill
force) gives you 400 N-m again.
d. How much work must you do on the trailer and children as you
pull them to the top of a 500 m tall hill? Does the amount of work you
do on them depend on whether you take the long, gradually sloping road
or the short, steep road? (Answer both questions.)
Answer: 200,000 N-m (or 200,000 J) and No (it doesn't depend
on the path)
Why: The children and trailer weigh 400 N, so raising them upward
500 m will require 200,000 N-m of work (400 N of upward force times 500
m of distance in the direction of that upward force). Any path to
the top of this hill will require you to do the same amount of work on
the children and trailer because the work you do simply increases the children
and trailers' gravitational potential energy, an increase that doesn't
depend on the path taken in raising them upward 500 m.
e. How much work must you do on the trailer and children as you
pull them back down the 500 m tall hill at constant velocity?
Answer: -200,000 N-m (or -200,000 J)
Why: To lower the children and trailer down the hill at constant
velocity, you must push them uphill while they move down hill. Since the
force you exert on the children and trailer is in the direction opposite
the distance they travel, you do negative work on them (or, equivalently,
they do positive work on you). No matter how steep the hill, the work you
do in lowering them a total of 500 m at constant velocity is going to be
the same as if you had lowered them directly downward. In that case, the
upward force you exert on them is 400 N and the downward distance they
move is 500 m. The total work you do on them is -200,000 N-m, where the
minus sign comes from the fact that the force and distance are in opposite
directions.
Problem 4: Chapter 1, Case 25a-e (Pg. 76)
Advanced skiers turn by sliding the backs of their skis across the snow.
Since the fronts of their skis don’t move much, the skis end up pointed
in a new direction.
a. The amount of sideways force that a skier must exert on the
skis to slide them sideways is proportional to how hard the skis press
down on the snow beneath them. Why?
Answer: The skier experiences sliding friction when sliding
the skis sideways and sliding friction is always roughly proportional to
the forces pressing the two surfaces together.
Why: It is the nature of friction that the harder the
two surfaces are pressed together, the harder it is to slide them across
one another. The force of sliding increases almost exactly in proportion
to the forces pushing the surfaces together.
b. To make it easier to slide the skis sideways, the skier “unweights”—reduces
the force pressing their skis downward against the snow. The skier does
this by jumping upward. How can the downward force that the skier exerts
on the snow be less than the skier’s weight?
Answer: (If the skier is willing to accelerate downward,) he
or she can simply not push downward on the snow so hard.
Why: There is no law that requires the skier to push downward
on the snow with a force equal to his or her weight. In fact, if the skier
is accelerating up or down, they will not be exerting a force equal to
their weight on the snow. Acceleration requires a non-zero net force, so
the snow must push on the skier with a force that doesn't balance the skier's
weight. If the snow pushes upward extra hard on the skier, the skier will
accelerate upward. If the snow pushes upward weakly or not at all, the
skier will accelerate downward. The skier can choose the amount of upward
force the snow exerts on him or her by choosing how hard to push down on
the snow. The snow merely responds with an equal but oppositely directed
force--in accordance with Newton's third law.
c. When during the jump is it easiest to slide the skis sideways?
Answer: At the top of the jump (or, more accurately, during
the moment of maximum downward acceleration, or, equivalently, during the
moment of minimum upward force from the snow on the skier)
Why: At the top of the jump, the skier is accelerating downward
rapidly. For this downward acceleration to occur, the snow must not be
pushing upward on the skier very hard, if at all. With little or no force
pressing the skier's skis against the snow, the skis turn easily because
there is almost no sliding friction between the skis and snow.
d. Rather than jumping, some racers simply pull their legs upward
suddenly. Why does this action reduce the force pressing their skis against
the snow?
Answer: Pulling the legs upward separates the skis from the
snow so that they can't push against one another very hard (or, more accurately,
pulling upward on the skis causes the skis to accelerate upward so that
they move away from the snow and don't press on the snow hard).
Why: Lifting the legs suddenly is an effective way of reducing
the forces between the skis and snow--if they aren't touching, they can't
exert support forces on one another.
e. Less skilled skiers sometime turn without unweighting—they push
their skis sideways so hard that the skis slide anyway. This technique
is exhausting. Why does it require so much work?
Answer: Without unweighting, the force of sliding friction is
large. Since the work done against sliding friction is the product of the
force needed to slide the skis times the distance of the slide, having
a large sliding friction force to overcome makes the work required to slide
the skis sideways large.
Why: The more force pressing the skis against the snow, the
larger the force of sliding friction that opposes the slide. Since the
skier must overcome that sliding friction force in doing the work required
to turn the skis, increasing the sliding friction force increases the work
done.
Problem 5: Chapter 11, Case 4a-d (Pg. 408)
The spark lighters used in gas stoves and grills are based on small
piezoelectric crystals. When you compress a piezoelectric crystal, it produces
a charge separation. One side becomes positively charged while the other
becomes negatively charged. In a typical spark lighter, a spring-loaded
mass strikes the crystal and produces a huge charge separation. Wires attached
to the crystal allow these charges to approach one another across an air
gap and create a spark.
a. Separating charge takes energy. Show that the spring-loaded
mass does work on the crystal while compressing it.
Answer: The mass pushes the crystal's surface inward and the
crystal's surface moves inward.
Why: Compressing something always requires work because you
must exert an inward force on the object's surface and that object's surface
must move inward. Since the force and distance moved are in the same direction
(and not zero), you are doing work--force times distance in the direction
of that force.
b. Why does the amount of electric charge on each side of the crystal
affect the likelihood that a spark will jump from one wire to the other?
Answer: For charge to jump from one wire to another, it must
experience a large force. That force increases as the amount of charge
on each side of the crystal increase.
Why: Charges don't jump into the air for no reason--something
must push them. For a positive charge to leave a metal surface, that metal
surface should have many other positive charges on it and, ideally, there
should be another nearby surface covered with negative charges. That way,
the positive charge that's going to jump is pushed away from the metal
by its fellow positive charges and is pulled out of the metal by the nearby
negative charges on the other surface. The more positive charges on the
metal surface, the more force the jumping charge experiences and the more
likely it is to leave the metal.
c. To encourage a spark, the wire ends that make up the air gap
are usually thin and pointed. Why do sharp points make it easier for charge
to begin moving through the air?
Answer: A sharp point packs like charges very close together
so that they repulsive forces become very large. These repulsive forces
make it easier for a charge to enter the air.
Why: On a smooth, lightly curved metal surface, like charges
spread out evenly and experience relatively small repulsive forces. With
little pushing them away from the metal, they are unlikely to enter the
air. But at a region of severe curvature, particularly at a sharp point,
the charges bunch up into a small area and repel one another strongly.
They push one another into the air easily.
d. If the two wires become separated by too great a distance, the
spark lighter will stop working. Why does the distance separating the wires
matter at all?
Answer: As the wires separate more and more, the attractive
forces that the opposite charges on the two wires exert on one another
decrease and it becomes harder for charges to leave the wires and jump
through the air as a spark.
Why: For a positive charge to leave a surface, it needs an outward
force. Other positive charges on that surface provide some of this outward
force, but the presence of a nearby negatively charged surface helps pull
the positive charge, too. As that negatively charged surface moves away
into the distance, its attractive forces decrease and the positive charge
is less and less likely to jump.