Rotational Motion Problems: Tilting Pole, a Yo-Yo, and a rolling hoop

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SUMMARY

This discussion focuses on solving three rotational motion problems involving a falling pole, a yo-yo, and a rolling hoop. The first problem requires the application of conservation of energy to determine the speed of the upper end of a 2.30-meter pole just before it hits the ground, yielding an answer of 8.22 m/s. The second problem involves calculating the linear speed of a yo-yo made of two cylindrical disks and a hub, with the final speed being 0.84 m/s and 96% of its kinetic energy being rotational. The third problem examines a hollow cylinder rolling up a 15-degree incline, where the height reached is 1.11 meters, and the time taken to return is 5.2 seconds.

PREREQUISITES
  • Understanding of conservation of energy principles
  • Familiarity with rotational kinetic energy (RKE) and translational kinetic energy (TKE)
  • Knowledge of kinematics equations for motion on inclines
  • Basic concepts of angular velocity and moment of inertia
NEXT STEPS
  • Study the conservation of energy in rotational motion
  • Learn about moment of inertia for different shapes, including solid and hollow cylinders
  • Explore kinematics equations for objects moving on inclines
  • Investigate the relationship between linear and angular velocity
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Students and educators in physics, particularly those focusing on mechanics and rotational dynamics, as well as engineers and anyone involved in motion analysis and energy conservation principles.

random26
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Okay, 3 problems I can't seem to get the right answer for..

1. A 2.30-m-long pole is balanced vertically on its tip. It starts to fall and its lower end does not slip. What will be the speed of the upper end of the pole just before it hits the ground? [Hint: Use conservation of energy.]
GPE = TKE + RKE
mgh = .5m(v^2) + (.5)(I)(w^2)
so: mgh = .5m(v^2) + (.5)[(1/3)(m)(L^2)]w^2
My problem is that I don't understand how to solve for the angular velocity [w] without the radius of the pole. The answer should be 8.22m/s. Suggestions?

2. A yo-yo is made of two solid cylindrical disks, each of mass .050kg and diameter .075m, joined by a (concentric) thin solid cylindrical hub of mass .0050kg and diameter .01m. Use conservation of energy to calculate the linear speed of the yo-yo when it reaches the end of its 1.0-m-long string, if it is released from rest. (b) What fraction of its kinetic energy is rotational?
I honestly don't even know where to begin with this problem. I guess it would have GPE at the top, and KE and GPE at the bottom, right? I don't understand how to know the height of the yo-yo at the top though for GPE = mgh. Would the height be zero? I definitely need help just getting started on this problem. The answer should be .84 m/s and 96%.

3. A hollow cylinder (hoop) is rolling on a horizontal surface at speed v=3.3m/s when it reaches a 15 degree incline. (a) How far up the incline will it go? (b) How long will it be on the incline before it arrives back at the bottom?
So it has TKE and RKE at the beginning and GPE once it's on the incline so..
.5(m)(v^2) + (.5)(m)(v^2) = mgh
therefore: (.5)(3.3^2) + (.5)(3.3^2) = (9.8)(h)
h ends up being 1.11 and when you divide it to get the hypotenuse, the answer is 4.3m up the ramp. So far so good. But I don't understand how you can relate this answer to the time you need to find in part b. Is there an equation for this I can use? The answer's supposed to be 5.2s, but I have no idea how to find that.

Thanks :)
 
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Problem 1
How is radius of a pole, which is pivoted and rotates about one end, related to its length of 2.30 m?
Problem 2
By what vertical distance is a yo-yo displaced when it drops from one end to the other of a 1-m long string?
Problem 3
You need to use the kinematics equations involving time for the second part.
 
random26 said:
its lower end does not slip
Is there a difficulty here?
When the pole length 2r is at angle θ to the ground, KE gives:
##\frac 12\frac 43mr^2\omega^2=mgr(1-\cos(\theta))##
Centripetal acceleration gives:
##mr\omega^2=mg\cos(\theta)-N\cos(\theta)-F\sin(\theta)##
where N is the normal force and F the frictional force:
##|F|\leq |N\mu_s\sin(\theta)|##
When ##\cos(\theta)=\frac 35## those equations become:
##mr^2\omega^2=mgr\frac 35##
##mr\omega^2=mg\frac 35-N\frac 35-F\frac 45##
Whence
##N\frac 35+F\frac 45=0##.
So it seems that even without slipping the pole will lose contact with the ground.
random26 said:
the radius of the pole
Not sure what you mean by that, the radius of rotation of the mass centre of the pole or its radius as a solid cylinder.
random26 said:
Would the height be zero?
You can choose the zero height wherever you like. All that will matter is the change in height.

When the yo-yo is descending at speed v, how fast is it rotating? What is its KE?
 
Last edited:

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