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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 62 Problem 63 Problem 64 Problem 65 Problem 66 Problem 67 Problem 68 Problem 69 Problem 70 Problem 71 Problem 72 Problem 73 Problem 74 Problem 75 Problem 76 Problem 77 Problem 78 Problem 79 Problem 80 Problem 81

Problem 7 Easy Difficulty

A certain type of propeller blade can be modeled as a thin uniform bar 2.50 m long and of mass 24.0 $\mathrm{kg}$ that is free to rotate about a frictionless axle perpendicular to the bar at its midpoint. If a technician strikes this blade with a mallet 1.15 $\mathrm{m}$ from the center with a 35.0 $\mathrm{N}$ force perpendicular to the blade, find the maximum angular acceleration the blade could achieve.

Answer

2.4 $\mathrm{rad} / \mathrm{s}^{2}$

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Physics 101 Mechanics

College Physics

Chapter 10

Dynamics of Rotational Motion

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Video Transcript

hello, Problem number seven models a propeller blade as a thin uniformed bar. That's that is 2.5 meters long. It has a mass of 24 kilograms. It's mass since it's a uniform bar. Its center mass would be directly in the center at one point. Top 25 kilogram are meters from the pivot point right here, which would make its weight be 24 times 9.8. This propeller blade is struck with a mallet at a location 1.15 from the center. In the force that we strike this mallet or this propeller blade with is 35 mins, were asked to find the maximum angular acceleration that the blade would receive. So we now by definition of Twerk, that tor causes angular acceleration. So the sum of all the torques acting on this propeller blooded would be equal to the moment of inertia, times the angular acceleration. There are two different forces that would provide torques. The weights would provide a clockwise tour and would be considered negative. Where they force from. The mallet would provide a counterclockwise force, and it would be a torque and it would be considered positive when we find each individual torque, we do talk times, lever arm, so we have to force or two torques. Acting one is 35. It's lever arm would actually be in its from our pivot 350.1 point 25 plus one point warm far, and the force of gravity would provide torque in the opposite direction. Uh, and it's lever on would be 1.25 Those would be equal to the moment of inertia. Times are angular acceleration. Now this is a thin rod moment of inertia for Thin Rod is 1 12 M R. Squared or 1 12 are Masses 24 and our distance from the pivot point would again be 1.25 plus 1.15 That's 2.4 squared times the angular acceleration solving for angular acceleration. We would get 3.22 radiance. Her second square. Thank you for learning with me today.

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Hugh D. Young

College Physics

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