HOMEWORK 3
SOLUTIONS
1: Kids in the Back!
If the car begins stopping, the child will keep going. If the car stops quickly,
the child will still be going at 35 km/h and will hit the dashboard at that
speed. If the car stops completely before the child hits the dashboard it will
hit at 35 km/h. If the car hasn't stopped yet, the speed will be the difference
between 35 km/h and the car's speed when the child hits. To do this, I need
to estimate how far I will go before I stop from my driving experience. But
my experience is in mi/h not km/h so I have to convert. Since 1 mile = 1.6 km,
35 km/h is equal to
less than 30 mph, not a very high speed. I expect I can stop in about 50-100
feet. Let's call it 50 ft. We could work out exactly how fast the car was going
when the child hits the dashboard, but it's fairly tedious. Let's assume you've
really jammed on your brakes and things go flying forward (i.e., keep going
at the speed they were going) and that you're almost fully stopped when they
hit. This will be a bit of an overestimate (perhaps 20-30%). The world's fastest
runner runs at about 10 m/s. Converting km/h to m/s is easy if we multiply by
the right "1's":
So the child hitting the dashboard is similar to the world's fastest runner
running into a fixed dashboard (or worse, the windshield) while running as fast
as he can.
2: Tapping a Rolling Ball
From measuring the x -spacing of the dots, it seems like the x velocity slows
a bit. We note that both x and y values start positive at t = 0. We draw the
position graphs first and then extract the velocity graphs by consistency and
the force graphs from that using that net force is proportional to acceleration.
3: Free fall acceleration
The first statement is not really relevant since the book refers to "free-fall."
This doesn't just mean "dropped." Rather, it means "there are
no other forces other than gravity acting on the object" (or better, other
forces acting on the object are much less than gravity and can be ignored).
In the case of the balloon and feather, the force of gravity is very weak since
the objects are very light. Furthermore, they are not small, so air resistance
is important and cannot be ignored. For a brick, unless it is traveling at hundreds
of miles an hour, air resistance can be ignored.
Therefore, this observation does not invalidate the quoted statement.
The second statement is not relevant. The statement says objects in free fall
accelerate downward, not that they move downward. This refers only to how the
object's velocity changes. If the object has a sideways velocity and that sideways
velocity is unchanged, it does not contribute to the acceleration. The object's
downward velocity increases, so the acceleration points downward. This observation,
therefore, does not invalidate the quoted statement.
The third objection is conflicted. The first part of the statement is correct,
as you can easily test by holding the two balls in your hands. The last part
of the statement is wrong. By a = F/m, a more massive objects needs more force
than a light object to get the same acceleration. The quoted statement therefore
holds up despite the three objections.
4: The Sliding Pizza
We can think about the motion of the pizza box in terms of Newton's second
law. If the box is to change its velocity, there need to be forces acting on
it. Since we are only talking about horizontal motions (sliding to one side
or another) the forces that affect these motions must be touching forces. There
must be something touching the box to change its motion.
When I am turning left, the car and the pizza box are moving forward in a straight
line before the turn begins. To change the velocity so it turns left or right,
something must push or pull the box to the left or right while the car is turning.
The box is touching the cowl of the steering wheel and the dashboard. The cowl
of the steering wheel can only push to the right, not pull the box to the left.
The dashboard can exert friction in any direction, but this isn't very big and
may not be enough to change the box's velocity. So when I turn to the left,
the box wants to go straight. As the car turns under it, there is nothing that
can push the box to the left so it may slide (apparently moving right to the
driver moving to the left with the car), trying to continue going straight.
When I turn to the right, the cowl of the steering wheel can press against the
box, pushing it to the right and keeping it moving with the car. So I have to
worry when turning left, not right. (This is easy to see in your mind's eye
if you imagine yourself a bird flying above the car and that the car is a convertible
with its top down. The box tries to go straight while the car turns under it.)
When I start, the box wants to stay where it is. To get it moving, something
has to push it. But there is nothing touching it from behind that can push it
forward, so it will tend to slide back onto the seat. When I stop, the box is
moving and tends to keep going as the car stops. The box will then hit the windshield
so the windshield will exert a backward force on it, stopping the box. I therefore
have to worry most when starting, not when stopping.
5: Why bother with N1?
Our everyday experience does not contradict N1. When we think about trying
to move an object ourselves, we are focusing on the force we have to exert rather
than the forces the object feels. N1 only says an object will move at a constant
velocity if nothing acts on it. Remembering that we are looking for physical
forces (not common speech "forces"), any object can exert a physical
force on another object when they touch. Mostly, objects slow down because they
are touching other objects, and those other objects exert frictional forces
on them.