Asst 32 exercise

course Phy 201

You are doing quite well here. See my notes.

Let me know if you need further clarification.

assignment #032 032. Moment of inertia

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21:38:14 `q001. Note that this assignment contains 3 questions. The moment of inertia of a concentrated mass m lying at a distance r from the axis of rotation is m r^2. Moments of inertia are additive--that is, if an object with a moment of inertia about some axis is added to another object with its moment of inertia about the same axis, the moment of inertia of the system about that axis is found by simply adding the moments of inertia of the two objects. Suppose that a uniform steel disk has moment of inertia .0713 kg m^2 about an axis through its center and perpendicular to its plane. If a magnet with mass 50 grams is attached to the disk at a point 30 cm from the axis, what will be the moment of inertia of the new system?

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RESPONSE --> I = mr^2 = .050kg * (.3m)^2 = .0045kgm^2 The total moment of inertia for the entire system is .0045kgm^2 + .0713kgm^2 = .076 kgm^2

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21:38:29 A mass of m = .05 kg at distance r = .30 meters from the axis of rotation has moment of inertia I = m r^2 = .05 kg * (.30 m)^2 = .0045 kg m^2. The moment of inertia of the new system will therefore be the sum .0713 kg m^2 + .0045 kg m^2 = .0758 kg m^2 of the moments of inertia of its components, the disk and the magnet.

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RESPONSE --> ok

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21:49:35 `q002. A uniform rod with mass 5 kg is 3 meters long. Masses of .5 kg are added at the ends and at .5 meter intervals along the rod. What is the moment of inertia of the resulting system about the center of the rod?

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RESPONSE --> I = mr^2 = 5kg * (3m)^2 = 45kgm^2 for the uniform rod. As for the extra masses added at the different intervals, I'm not sure if I need to find the moment of inertia for each individual interval and then add all of them together or if taking the inertia of .5kg * (.5m)^2 = 0.125kgm^2 is correct.

You need to figure out m r^2 for each of the masses individually, then add them all up. You do this below, but see my notes there.

If so, then .125kgm^2 + 45kgm^2 = 45.125kgm^2... if I have to do each interval, then: For the first interval on the rod (working from the end towards the center), the inertia is .5kg * (2.5m)^2 = 3.125kgm^2 For the second interval, .5kg * (2m)^2 = 2kgm^2 Next, .5kg * (1.5m)^2 = 1.125kgm^2 Then, .5kg * (1m)^2 = 0.5 kgm^2

This is the right idea, but the axis of rotation is the center of the bar, and the r in each m r^2 is the distance from the center. See the given solution.

Since the inertias that I have here represent one side of the bar, I squared them to get the total inertia of the bar and not just one side.

You add moments of inertia, you don't multiply them. So in a case where you have figured out moments for one of two symmetric sides, you would double your results, not square them.

Thus the total is 0.5^2 + 1.125^2 + 2^2 + 3.125^2 + 45 = 60.3kgm^2 As I said before, I have no idea if this is what I was supposed to do... it's just an elaborate guess.

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21:52:11 The rod itself, being rotated about its center, has moment of inertia 1/12 M L^2 = 1/12 * 5 kg * (3 m)^2 = 3.75 kg m^2. The added masses are at distances 1.5 meters (the two masses masses on the ends), 1.0 meters (the two masses .5 m from the ends), .5 meters (the two masses 1 m from the ends) and 0 meters (the mass at the middle of the rod) from the center of the rod, which is the axis of rotation. At 1.5 m from the center a .5 kg mass will have moment of inertia m r^2 = .5 kg * (1.5 m)^2 = 1.125 kg m^2; there are two such masses and their total moment of inertia is 2.25 kg m^2. The two masses lying at 1 m from the center each have moment inertia m r^2 = .5 kg * (1 m)^2 = .5 kg m^2, so the total of the two masses is double is, or 1 kg m^2. {}The two masses lying at .5 m from the center each have moment of inertia m r^2 = .5 kg ( .5 m)^2 = .125 kg m^2, so their total is double this, or .25 kg m^2. The mass lying at the center has r = 0 so m r^2 = 0; it therefore makes no contribution to the moment of inertia. The total moment of inertia of the added masses is therefore 2.25 kg m^2 + 1 kg m^2 + .25 kg m^2 = 3.5 kg m^2. Adding this to the he moment of inertia of the rod itself, total moment of inertia is 3.75 kg m^2 + 3.5 kg m^2 = 7.25 kg m^2. We note that the added masses, even including the one at the center which doesn't contribute to the moment of inertia, total only 3.5 kg, which is less than the mass of the rod; however these masses contribute as much to the moment of inertia of the system as the more massive uniform rod.

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RESPONSE --> Well I started off with the wrong equation, not using the one for the uniform rod... Other than that, I'm not really sure if my method was completely incorrect or not.

You had most of the right ideas, but made a couple of errors in detail. See my notes above.

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22:06:47 `q003. A uniform disk of mass 8 kg and radius .4 meters rotates about an axis through its center and perpendicular to its plane. A uniform rod with mass 10 kg, whose length is equal to the diameter of the disk, is attached to the disk with its center coinciding with the center of the disk. The system is subjected to a torque of .8 m N. What will be its acceleration and how to long will it take the system to complete its first rotation, assuming it starts from rest?

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RESPONSE --> inertia for the uniform disk is : 1/2 M R^2 = 1/2 * 8kg * (.4m)^2 = 0.64kgm^2 inertia for the uniform rod is : 1/12 M R^2 = 1/12 * 10kg * (.8m)^2 = 0.533kgm^2 Total inertia for the entire system is: 0.64kgm^2 + 0.533kgm^2 = 1.173kgm^2 With a torque of .8mN and the inertia at 1.173kgm^2, the acceleration of the system is: alpha = tau / I = 0.8mN / 1.173kgm^2 = 0.68m/s^2. I'm not sure how to get the time interval... I know that acceleration is .68m/s^2 and that initial velocity is 0m/s, but I'm not sure what other information is here that I have to work with... I want to say that I can get the distance traveled by kg * r but I don't know if that's right or not either.

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22:09:13 The moment of inertia of the disk is 1/2 M R^2 = 1/2 * 8 kg * (.4 m)^2 = .64 kg m^2. The rod will be rotating about its center so its moment of inertia will be 1/12 M L^2 = 1/12 * 10 kg * (.8 m)^2 = .53 kg m^2 (approx). ( Note that the rod, despite its greater mass and length equal to the diameter of the disk, has less moment of inertia. This can happen because the mass of the disk is concentrated more near the rim than near the center (there is more mass in the outermost cm of the disk than in the innermost cm), while the mass of the rod is concentrated the same from cm to cm. ). The total moment of inertia of the system is thus .64 kg m^2 + .53 kg m^2 = 1.17 kg m^2. The acceleration of the system when subject to a .8 m N torque will therefore be `alpha = `tau / I = .8 m N / (1.17 kg m^2) = .7 rad/s^2, approx.. To find the time required to complete one revolution from rest we note that the initial angular velocity is 0, the angular displacement is 1 revolution or 2 `pi radians, and the angular acceleration is .7 rad/s^2. By analogy with `ds = v0 `dt + 1/2 a `dt^2, which for v0=0 is `ds = 1/2 a `dt^2, we write in terms of the angular quantities `d`theta = 1/2 `alpha `dt^2 so that `dt = +- `sqrt( 2 `d`theta / `alpha ) = +- `sqrt( 2 * 2 `pi rad / (.7 rad/s^2)) = +-`sqrt( 12.56 rad / (.7 rad/s^2) ) = +-4.2 sec. We choose the positive value of `dt, obtaining `dt = +4.2 sec..

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RESPONSE --> I did everything fine up until finding the time interval. It had crossed my mind to use 2pi as the distance since it was one revolution, but I got wrapped up in finding something to work with in my notes and forgot all about using it.

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