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Class Notes Physics I, 10/26/98
Terminal Velocity, Momentum Conservation in Two Dimensions
http://youtu.be/wLpR-RvPZfY
http://youtu.be/8IdRhQM_Lkw
Careful observations have shown that when a 'doubled' coffee filter is dropped from a
height of 200 cm, the single filter dropped simultaneously from a height of 128 cm will
strike the floor at the same time.
- The possibility that one filter presents a greater area to air friction was controlled
by switching filters and confirming that this has no effect on the relative heights from
which the filters must be dropped.
- If we assume that the filters always reach terminal velocity in negligible time, we
conclude that the average velocity of a falling filter is equal to its terminal velocity.
- To the extent that our assumption is incorrect, the terminal velocity will be somewhat
greater than the average velocity.
- We also assume that every filter has mass m, which is the same for all filters.
- As depicted below, when a 'doubled' filter with its mass 2m is dropped from the 200 cm
height, a single filter dropped simultaneously from a height of 128 cm will reach the
floor at the same time.
- Assuming that both filters drop at
a constant terminal velocity, simple proportionality tells us that the velocity of the
'doubled' filter must be 200 / 128 times that of the single filter.
- If we represent the velocity of
the single filter by v1 and that of the doubled filter with its mass 2m by v2m, we see
that v2m = 200 / 128 v1 = 1.6 v1 (approx.).
- Similar observations with three
and four combined filters result in the conclusions that the velocity v3m of three filters
is 200/92 times that of the single filter, so we have v3m = 2.2 v1 (approximately), and
that v4m = 2.6 v1 (approximately).
http://youtu.be/SO0nKsYkTSg
Noting that the force of air
resistance for a freely falling object is equal and opposite to the weight of the object,
and that the weight of a single filter is the force m * g exerted on it by gravity, we see
that the velocities v1, 1.6 v1, 2.2 v1 and 2.6 v1 are associated with respective forces m
* g, 2 m * g, 3 m * g and 4 m * g.
- Graphing these results we obtain the data points and approximate curve sketched at the
right of the figure below.
- This result is in poor agreement with the result expected in light of carefully done
experiments conducted over the last two or three centuries, obviously reflecting some sort
of perverse behavior by the coffee filters used for the experiment.
http://youtu.be/jssj_--mpjI
Today's quiz problem concerned a 10 kg object moving at 20 m/second at 230 degrees with
respect to the positive x axis, colliding with a 20 kg object moving at 12 m/second at 130
degrees with respect to the positive x axis.
We begin by finding the components of the momentum of each object.
- The momentum of the first object is clearly 200 kg m/second at 230 degrees.
- The x and y components of this momentum are easily found using the cosine and sine
functions.
- The x and y momenta are respectively -128 kg m/second and -153 kg m/second.
- Treating the second object similarly we obtain x and y momentum components -154 kg m/s
and + 184 kg m/s.
Adding the x and y components, we obtain a total x momentum component of -282 kg m/s
and a total y component of 31 kg m/s.
- These momenta are sketched in the 'green' graph below.
- The magnitude and angle of this total momentum are calculated using the Pythagorean
Theorem and the inverse tangent, as in the lower right-hand corner of the figure below.
- Note that since the x component of the total momentum is negative we add 180 degrees to
the inverse tangent, obtaining angle `theta = 174 degrees. This angle is reasonably
consistent with our sketch.
http://youtu.be/s75qX9S17so
If the collision is inelastic we end up with a 30 kg object with a total momentum of
284 kg m/second at 174 degrees.
- From this we easily calculate the velocity, equal to the momentum divided by the mass.
- The velocity we obtain is 9.47 m/second at 174 degrees.
To determine whether energy is conserved in this collision we first calculate the
kinetic energy before collision, which is the sum of the kinetic energies of the 10 kg object moving at 20 m/second
and the 20 kg object moving at 10 m/second.
- This total is easily found to be 3440 Joules.
- The kinetic energy after collision is that of a 30 kg object moving at 9.47 m/second.
- This kinetic energy is found to be approximately 1350 Joules (the sure to check that
calculation, which is not been validated).
- We thus see that kinetic energy is definitely not conserved in the collision, while
momentum must be conserved.
Depending on the angle at which the objects collide, if the collision is not inelastic
the second object might end up with a wide variety of speeds and directions.
- In fact, the only limit on possible collisions (except for those involving a release of
additional energy, as in explosions), is that momentum must be conserved and the total
kinetic energy after collision cannot be greater than that before collisions.
Suppose for example that after collision the second object was moving at 4 m/second at
310 degrees from a positive x axis.
- Its momentum is therefore 40 kg m/second at 310 degrees.
- Since the total momentum is known (284 kg m/second at 174 degrees), and since the
momentum of the first and second object add up to this total, we can find the momentum of
the first object.
- We first calculate the components of the momentum of the second object, obtaining
something like p2x = 25 kg m/second and p2y = -27 kg m/second (verify these calculations,
which have not been validated).
http://youtu.be/XcLSA8AIc04
We therefore have the situation depicted in the somewhat poorly drawn figure below.
- The total momentum has components -282 kg m/second and 31 kg m/second in the x and y
directions, respectively.
- This total is made up of the momentum of the second object, with its x and y components
of 25 kg m/second and -27 kg m/second, and the unknown momentum of the first object.
- It follows that the x momentum of the first object, when added to the existing 25 kg
m/second momentum of the second, must give a result of -282 kg m/second.
- We easily conclude that the x momentum of the first object is therefore -307 kg
m/second.
- Similarly, in order to obtain the 31 kg m/second total momentum we must add 58 kg
m/second to the existing -27 kg m/second, so that the y momentum of the first object must
be 58 kg m/second.
http://youtu.be/hn2RSav4yS8
We could have calculated the momentum p1 more formally by noting that since p1 + p2 =
pTotal, p1 = pTotal - p2.
- This indicates that in order to get the components of p1, we must therefore subtract the
components of p2 from those of pTotal.
- We would therefore obtain p1x = -282 kg m/second - 25 kg m/second = -307 kg m/second,
and p1y = 31 kg m/second - (-27 kg m/second) = 58 kg m/second, in agreement with the
previous results.
Having obtain the components of the unknown momentum, we can easily find the magnitude
and direction of this momentum.
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