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Problem 1 Problem 2 Problem 3 Problem 4 Problem 5 Problem 6 Problem 7 Problem 8 Problem 9 Problem 10 Problem 11 Problem 12 Problem 13 Problem 14 Problem 15 Problem 16 Problem 17 Problem 18 Problem 19 Problem 20 Problem 21 Problem 22 Problem 23 Problem 24 Problem 25 Problem 26 Problem 27 Problem 28 Problem 29 Problem 30 Problem 31 Problem 32 Problem 33 Problem 34 Problem 35 Problem 36 Problem 37 Problem 38 Problem 39 Problem 40 Problem 41 Problem 42 Problem 43 Problem 44 Problem 45 Problem 46 Problem 47 Problem 48 Problem 49 Problem 50 Problem 51 Problem 52 Problem 53 Problem 54 Problem 55 Problem 56 Problem 57 Problem 58 Problem 59 Problem 60 Problem 61

Problem 20 Medium Difficulty

Multiple-Concept Example 7 deals with the concepts that are important in this problem. A penny is placed at the outer edge of a disk (radius 0.150 m) that rotates about an axis perpendicular to the plane of the disk at its center. The period of the rotation is 1.80 s. Find the minimum coefficient of friction necessary to allow the penny to rotate along with the disk.

Answer

0.187

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Physics 101 Mechanics

Physics

Chapter 5

Dynamics of Uniform Circular Motion

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Watch More Solved Questions in Chapter 5

Problem 1
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Problem 4
Problem 5
Problem 6
Problem 7
Problem 8
Problem 9
Problem 10
Problem 11
Problem 12
Problem 13
Problem 14
Problem 15
Problem 16
Problem 17
Problem 18
Problem 19
Problem 20
Problem 21
Problem 22
Problem 23
Problem 24
Problem 25
Problem 26
Problem 27
Problem 28
Problem 29
Problem 30
Problem 31
Problem 32
Problem 33
Problem 34
Problem 35
Problem 36
Problem 37
Problem 38
Problem 39
Problem 40
Problem 41
Problem 42
Problem 43
Problem 44
Problem 45
Problem 46
Problem 47
Problem 48
Problem 49
Problem 50
Problem 51
Problem 52
Problem 53
Problem 54
Problem 55
Problem 56
Problem 57
Problem 58
Problem 59
Problem 60
Problem 61

Video Transcript

here we have to find the minimum coefficient of friction necessary. Give it penny indicated by the red dot rotating with me discredited scorn and not just lay off. So let's start by finding the angular velocity in this problem, we know that he is equal to two pi over Omega. So that means that omega must be too piratey and given team. This problem, so we have to do is put the quantity we get that omega is to pie over 1.80 seconds. And since the only above his unit ingredients, we get that omega equal to 10 pie ninth. Look, that looks like a G ninth red per second. Okay, now, from there we can analyze our forces. So since our professional force is the only force pointing inward toward the center of the circle, we know that the fresh Nall force must be responsible for a centripetal force as well. Now, the first of the fictional Force Correctional is given by F N times. The coefficient of friction, which is what we're looking for in this problem. And Evan must be equal to M G. Since, as you can see in the free body diagram it's opposing the gravitational force, so now we can right M J Times The coefficient of friction is M B squared over R and R centripetal force. We can also rewrite in terms of omega and just get and Omega Square are if you wanted to, you could also have sold for V Street from the equation or period. It really doesn't make a difference with where you approve it, because in the end it's all just known quantities. So we get MG cooperation. Friction equals and will make the square are and our enemies cancel out. Now we can right our co efficient in terms of we'll make a squared R and G and then all that is left to do is plug in. So we just calculated our omega, which is when we square it is ah 100 pi squared over anyone readings per second multiplied by our radius with 0.15 meters and that is all over our No, our co are gravitational acceleration which is 9.8 meters per second squared and who me duel that out? Plummeting toward calculator, we find that our coefficient of friction is equal to zero point 1865 that is, the minimum coefficient of friction required a pretty penny to broke eight with the circle, and that is our final answer.

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