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course Phy 201
q001: A rubber band chain is stretches from the point (10 cm, 5 cm) to the point (50 cm, 35 cm). The tension vs. length graph for this chain has horizontal intercept 42 cm and slope .15 N / cm.What is the length of the rubber band chain?
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What therefore is its tension?
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What are the x and y components of a vector from the (10 cm, 5 cm) point to the (50 cm, 35 cm) point?
The X component is 40, and the Y component is 30.
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What therefore is the length of this vector?
The length of this vector is 1.3cm.
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What do you get if you divide this vector's x and y components by its length?
When you divide the X component by the length I got 30, for the Y component I got 1.
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The results of the preceding are the x and y components of the unit vector in the direction of the rubber band. If you multiply these components by the tension force, you get the x and y components of the tension force vector. What are these components?
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What therefore are the magnitude and angle of the tension force vector?
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How much work would have to be done to extend the rubber band one more centimeter?
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1q002. If the rubber band chain in the preceding suspends a 40 gram mass, holding it in equilibrium against the force of gravity on the mass, then how long will the chain be?
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If the 40 gram mass is pulled down until rubber band chain is 50 cm long, and the mass is released, what will be the net force on the mass the instant after release?
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In the preceding, with what force was the mass pulled down before being released?
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How much work will be done by the tension force on the mass as it returns to its equilibrium position?
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If the rubber band tension was conservative, what would be its velocity upon return to equilibrium?
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`q003. A 40 gram mass is dropped from rest at a height of 2 meters above the floor. What is its momentum just before it strikes the floor?
The momentum just before the mass hit the floor is about 250.4g m/s. I found this by finding the v_f then multiplying that by the mass.
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How fast is the mass going when it first loses contact with the floor on its rebound, given that it rebounds to a maximum height of 1.5 meters?
It is going at a velocity of -5.422 given that up is in the negative direction.
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What therefore is its momentum when just after leaving the floor on its rebound?
By how much does its momentum change during the interval from just before contacting the floor to just after leaving the floor on its rebound? Be sure to choose a positive direction and answer relative to that direction.
The momentum just after the mass leaves the floor is about -216.88 g m/s. The momentum changes by 467.28 g m/s.
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`q004. A steel ball 25 mm in diameter has mass about 70 grams. A point on that ball which lies 9.9 mm from its axis of rotation is moving in a circular path about that axis, traveling at 30 cm / second.
How many times does that point go around the circle in a second?
That point goes around the circle about 75 cm / second.
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What is its angular velocity in radians per second?
I may be wrong here but I think that I need how many rotations the steel ball is making per second because I cannot convert the cm per second to rotations because I do not know how many cm are in 1 rotation.
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What is the moment of inertia of the ball?
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The angular velocity of the steel ball about that axis is the same as that of the point. What therefore is the angular kinetic energy of the ball?
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`q005. If you are in a car traveling at 70 mph behind another car traveling in the same direction at 60 mph, then your velocity relative to that car is 10 mph in your direction of motion. If you are traveling at 70 mph and another car is traveling at 60 mph in the opposite direction, then your velocity relative to that car is 130 mph in your direction of motion (and its velocity is -130 mph in your direction of motion).
A ball moving at 50 cm/s approaches another ball moving toward it at 20 cm/s. The balls collide and both balls reverse their directions, the first moving at 10 cm/s while the second moves at 60 m/s.
Before collision, what is the velocity of the first ball relative to the second?
After collision, what is the velocity of the first ball relative to the second?
Before collision it is 70 cm/s. After collision it is -50 cm/s.
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What is the magnitude of the velocity change of the first ball, and what is the magnitude of the velocity change of the second?
The magnitude velocity change for the 1st ball is -60 cm/s, and for the second it is -80 cm/s.
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Which ball do you conclude had the greater mass?
I think that the 1st ball, the one moving at 50 cm/s before, has the greater mass.
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Given solutions for 111107 assignment, to be compared with your solutions:
Your data for the first two experiments should be submitted promptly. Your analysis should be submitted within a week, as should the rest of the assignment.
Balancing dominoes experiment:
Report all relevant data from the experiment, being sure to clearly identify the quantities you report and what they mean.
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Find the torque produced by the weight of each domino on the first beam, about the point of rotation. You may assume domino weights of 15 grams each.
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The dominoes on one side of the balancing point tend to rotate the system in one direction, while the domino on the other side tends to rotate it in the other.
A counterclockwise rotation is generally regarded as positive, and a clockwise rotation is generally regarded as negative.
So of your three torques, two will be opposite in sign to a third.
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Candy bar experiment:
How many oscillations did the candy bar complete in a minute?
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What was the length of the rubber band chain when supporting 4 dominoes?
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What was the length of the rubber band chain when supporting 8 dominoes?
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Through how many radians did the reference point move during the 1-minute timing (it moved through a complete circle for every cycle you counted)?
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Every complete cycles corresponds to the reference point moving through 2 pi radians. If you multiply the number of cycles counted during the minute, therefore, you will get the number of radians in that minute.
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What therefore was the angular velocity omega of the reference point?
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If you divide the number of radians calculated in the preceding by 1 minute, you will get the number of radians per minute.
If you divide the same number of radians by 60 seconds, you will get the number of radians per second.
For example 100 cycles in a minute corresponds to 200 pi radians, so the angular velocity is 200 pi rad / minute, which is the same as 200 pi rad / (60 seconds) = 10/3 pi rad / second.
200 pi rad / minute, or 100 cycles / minute, or 5/3 pi cycles / second, are all valid angular velocities. But when you do the physics, the most convenient unit for angular velocity is the radian / second.
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How far was it, on the average, from the lowest point to the highest point in the candy bar's oscillation (you didn't measure this; just visualize the motion and make an estimate)?
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The diameter of the reference circle is equal to the estimate you made for the preceding question. How fast was that reference point moving around the arc of that circle?
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The radius is half the diameter. If you multiply the number of radians in an angle by the radius you get the distance along the arc.
So the easiest way to get the speed of the reference point is to multiply the number of radians per second by the radius; since the number of radians multiplied by the radius tells you how far, the number of radians per second multiplied by the radius tells you how far per second. That is the speed along the arc.
Most students will use a different approach, based on the circumference of the circle. There's nothing wrong with this, since it requires insight and yields the correct answer, but it's not the easiest way to approach the problem.
For example suppose the one-minute result is 100 cycles, and the diameter of the reference circle is 10 cm. Then the circumference is 10 pi cm, or about 31 cm. At 100 cycles per minute, this would imply 100 * 31 cm = 3100 cm in a minute, so the speed would be 3100 cm / (60 sec) = 52 cm / sec, approx..
Contrast this with the recommended approach. At 100 cycles in a minute, the angular velocity is about 10/3 pi rad / second, or about 10.5 rad / sec. The radius is 5 cm, so 10.5 rad corresponds to 10.5 * 5 cm = 53 cm. Thus 10.5 rad / sec * 5 cm = 53 cm / sec, again approximately. This is in good agreement with the 52 cm/s result previously obtained; the two agree to within roundoff error.
This latter calculation corresponds to v = omega * r. We have v = omega * r = 10.5 rad / sec * 5 cm = 53 cm/s.
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What is the slope of the force vs. length graph for your rubber band chain? If you measured the domino stack then you can use the fact that for every millimeter of height the stack has mass 1.9 grams. If not just assume a mass of 15 grams.
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Using 15 gram dominoes, the supported masses would typically be 30, 60, 90, 120 and 150 grams. Gravity exerts forces of about .3, .6, .9, 1.2 and 1.5 Newtons on these masses.
For a rubber band which had lengths 60, 66,71, 79 and 85 cm when supporting the masses, the tension vs. length graph will have points
(60, .3)
(66, .6)
(71, .9)
(79, 1.2)
(85, 1.5)
where x coordinates are lengths in cm and y coordinates are tensions in Newtons.
A graph of these points shows that they lie close to but not on a straight line. Trying to fit the best straight line to the points, then selecting two points on the line, you might find that the points
(61 cm, .29 Newtons) and (90 cm, 1.6 Newtons)
lie on the line, giving you an estimated slope of
slope = (1.6 N - .19 N) / (90 cm - 61 cm) = .047 N / cm.
In SI units this would be
slope = .047 N / cm = .047 N / (.01 meter) = 4.7 N / m.
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Your last answer is your estimate of k, and your count resulted in your previous answer for omega. What therefore is m?
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For the preceding example we would have k = 4.7 N / m
If the count was 100 cycles in a minute, then, omega = 10.5 rad / sec (see previous solutions).
Since omega = sqrt(k / m), we can solve the equation for m:
omega = sqrt(k / m). Squaring both sides
omega^2 = k / m. Multiplying both sides by m we have
m omega^2 = k. Dividing both sides by omega we have
m = k / omega^2 = 4.7 N / m / (10.5 rad / sec)^2 = .043 kg = 43 grams.
This is about 1.5 ounces, which is close to the typical mass of a candy bar.
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Experiment with 3 rubber bands
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The analysis for this experiment follows that included in given solutions to other problem sets.
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What are the magnitudes of each of the three length vectors?
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Divide the x and y components of each of these vectors by its length. What are your results? The vectors you get here are called 'unit vectors', because if you divide a vector by its length you get a vector of length 1 (i.e., a vector of unit length).
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According to your calibration of the colored calibrating chain, what was the tension in each of the rubber bands?
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Multiply the tension by the x and y components of the corresponding unit vector. Your result for each rubber band chain will be the components of its tension vector.
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Add up the x components of your three tension vectors. What do you get?
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Add up the y components of your three tension vectors. What do you get?
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The sum of your x components is the x component of the resultant vector; the sum of the y components is the y component of the resultant vector. What therefore is the magnitude of your resultant vector?
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The resultant vector represents the total effect of the three forces acting on the paper clip in the middle. The paper clip has zero acceleration, so the net force is actually zero. One measure of how accurate this experiment might be is the comparison between your resultant and the ideal. A reasonable way to make the comparison is to compare the magnitude of your calculated resultant with the largest of the three tension forces.
What is the magnitude of your resultant, as a percent of the magnitude of the largest of the three tension forces?
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`q001. The mass of the Earth is about 6 * 10^24 kg. The mass of the Moon is about 8 * 10^22 kg. The two are separated by about 400 000 kilometers. G = 6.67 * 10^-11 N m^2 / kg^2.
What is the gravitational force between the Earth and the Moon?
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m1=6*10^24kg m2
m2 = =8*10^22kg
r = 4 * 10^8 m
F=G*(m1*m2)/r^2
6.67*10^-11 (N * m^2/kg^2)*((6*10^24kg)*(8*10^22kg))/(4.0*10^8m)^2
=2*10^20N
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What is the acceleration of the Moon toward the Earth?
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a = F_net / m = 2 * 10^20 N / (8 * 10^22 kg) = 2.5 * 10^-3 N / kg = (2.5 * 10^-3 kg m / s^2 ) / kg = 2.5 * 10^-3 m/s^2, approx..
This can be checked against known information:
The Moon's orbit is an approximate circle of radius r = 4 * 10^8 m, giving it a circumference 2 pi r of about 2.5 * 10^9 m. It completes a revolution around the Earth in about 28 days, which is about 2.4 * 10^6 seconds, so its orbital velocity is about 2.5 * 10^9 m / (2.4 * 10^6 sec) = 1.04 * 10^3 m/s.
Thus its centripetal acceleration should be about
a_cent = v^2 / r = (1.04 * 10^3 m/s)^2 / (4 * 10^8 m) = 2.8 * 10^-3 m/s^2.
Within roundoff and other approximation errors, the two results are consistent.
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What is the acceleration of the Earth toward the Moon?
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The Earth is attracted toward the Moon by the same force, about 2 * 10^20 N.
So its acceleration is about
a = F_net / m = 2 * 10^20 N / (6 * 10^24 kg) = 3 * 10^-5 m/s^2, roughly.
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Assuming that the Moon's path in its orbit is a circle (which is pretty much the case) of radius about 400 000 kilometers, and that it takes 28 days to complete one orbit (again pretty close to the actual time required), then how fast is it moving?
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What therefore its its centripetal acceleration?
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`q002. Summary of SHM:
If the force vs. length graph of an elastic object is linear then its slope is called its force constant.
If the tension force exerted this object is (in a certain way not yet specified) responsible for the net force on an object then that force will be of the form F_net = - k x, where x is the position of the object relative to its equilibrium position.
If the net force on a mass m at position x is - k x, then the mass will either remain in its equilibrium position (x = 0), or will oscillate in a manner modeled by the projection on a line through the origin of a reference point moving around a circle with angular velocity omega = sqrqt(k/m).. You should understand how to use the formula omega = sqrt(k / m), and you should understand motion around a circle which is characterized by a constant angular velocity omega. You can expect that it will take a few examples and more explanation for you to understand the part about the projection..
If A is the radius of the circle then the amplitude of the motion is A, the speed of the point about the reference circle is v = A * omega, the maximum KE of the object occurs at the equilibrium point and is equal to 1/2 m v^2, the total mechanical energy of the oscillation is 1/2 m v^2, and the potential energy at position x relative to the x = 0 position is 1/2 k x^2.
An object of mass 50 grams is suspended from a rubber band chain. When it supports a hanging mass weighing .5 Newtons the chain is 70 cm long. When it supports a hanging mass weighing .9 Newtons the chain is 90 cm long.
What is the average slope of the force vs. length graph for the given length interval?
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Lengths and weights are .5 N at length 70 cm and .9 N at length 90 cm, yielding an average slope
k = slope = (.9N-.5N)/(90cm-70cm)=0.4N/20cm = .4 N / (.2 m) = 2 N / m.
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Assuming that the force vs. length graph is linear (not really so for a rubber band chain, but close enough not to make a big difference in the oscillation of our object), what is the value of k for this chain?
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What therefore should be the angular velocity of our reference point?
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omega = sqrt( k / m) = sqrt( (2 N / m) / (.05 kg) ) = sqrt( 40 s^-2) = 6.3 s^-1, meaning 6.3 rad / s.
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How long should it take the reference point to complete one circuit around the circle?
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A complete circuit corresponds to 2 pi radians. At 6.3 rad / sec the time for a circuit is
T = 2 pi rad / (6.3 rad/s) = 1.0 second.
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`q003. A vector `R of constant length 1 has its initial point at the origin. Its terminal point moves at a constant speed around the circle, so that the vector moves like a spinning dial. It should be clear that the circle has radius 1.
When the vector makes an angle of 15 degrees with the x axis, what are its x and y components?
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Answer the same for angle 30 degrees.
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Answer for angle 45 degrees.
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The x component of a length vector is length * cos(theta) and the y component is length * sin(theta), where theta is its angle as measured counterclockwise from the positive x axis.
The length of the vector is 1, so the x and y components are approximately as follows:
1 * cos(15 deg) = .97 and 1 * sin(15 deg) = .26
1 * cos(30 deg) = .87 and 1 * sin(30 deg) = .50
1 * cos(45 deg) = .71 and 1 * sin(45 deg) = .71
See my notes, then check your solutions and your thinking against the discussion given above. Questions and revisions are always welcome.
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