How Is Total Kinetic Energy Calculated for a Rolling Cylinder?

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SUMMARY

The total kinetic energy (KE) of a cylindrical wooden log rolling down a ramp is calculated by combining translational KE and rotational KE. The log, with a radius of 15 cm, length of 2.0 m, and mass of 85 kg, reaches a speed of 3.0 m/s at the bottom. The total KE is derived from the equations: KE_total = (1/2)MV^2 + (1/2)Iω^2, where I for a cylinder is (1/2)MR^2. The final calculation yields a total kinetic energy of 573.75 J and a height of approximately 0.62 m when using gravitational potential energy (mgh).

PREREQUISITES
  • Understanding of kinetic energy formulas: translational and rotational.
  • Familiarity with the moment of inertia for a cylinder: Icylinder = (1/2)MR^2.
  • Knowledge of gravitational potential energy: PE = mgh.
  • Basic principles of rolling motion and energy conservation.
NEXT STEPS
  • Study the derivation of kinetic energy equations for different shapes, including spheres and cylinders.
  • Learn about energy conservation principles in rolling motion.
  • Explore the effects of friction on rolling objects and how it influences energy calculations.
  • Investigate the transition from solid objects to point particles in physics and its implications on kinetic energy.
USEFUL FOR

Physics students, educators, and anyone interested in understanding the dynamics of rolling objects and energy conservation principles in mechanics.

psruler
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Can someone help me with this problem:

A cylindrical wooden log rolls (without slipping) down a smal ramp. Tha log has radius of 15 cm, a length of 2.0m and a mass of 85kg.
What was the log's TOTAL kinetic energy at the bottom of the ramp? (Recall that Icylinder = (1/2)MR^2) .

The total angular velocity i got was 200 rad/s.

I don't know if the angular velocity will help solve the problem.

THANKS!
 
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Not enough information. How high is the log on the ramp?

cookiemonster
 
Well, that is the next question I have to solve. That's all the information. Is there a way of solving this problem if the height is not given?
 
No. The energy is determined by the height, since the only energy the log has at first is gravitational potential energy, which depends on height.

cookiemonster
 
The previous question states that the log rolls at a speed of 3.0m/s when it reaches the bottom of the ramp.
 
psruler said:
The previous question states that the log rolls at a speed of 3.0m/s when it reaches the bottom of the ramp.
Well now you have enough information!

The total KE is the sum of (1) translational KE of the center of mass (1/2MV2), and (2) rotational KE about center of mass(1/2Iω2). Since the log rolls without slipping, V =ωR.
 
Thanks Doc Al!
 
Then can I find the height using this equation:

h = v^2/2g ?
 
Find the height using energy conservation. The initial gravitational PE at the top gets transformed into the total KE at the bottom.
 
  • #10
psruler said:
Then can I find the height using this equation:

h = v^2/2g ?
No because the log also has rotational KE (1/2Iω2), not just translational KE.
 
  • #11
The answer i got is: 0.62m. Can you verify if that is correct?
 
  • #12
I get a total kinetic energy of 573.75J at the bottom and a height of 6.75/g. So if you take g to be 10.9m/s2 it's right. :wink:
 
  • #13
how did you get 6.75 as the height?
 
  • #14
psruler said:
how did you get 6.75 as the height?
I get a (slightly) different answer. Maybe we should average them all together? :wink:

Show us the equations you used, what numbers you assumed, and how you calculated the answer. (Show it algebraically first, then with numbers plugged in.)
 
  • #15
I got:

mgh = 573.75J

So:

h = \frac{573.75J}{mg} = \frac{6.75}{g}

My equation:

mgh = \frac{1}{2}mv^2 + \frac{1}{2}I\omega ^2 = \frac{1}{2}mv^2 + \frac{1}{4}mr^2\omega ^2 = \frac{3}{4}mv^2

h = \frac{3v^2}{4g}
 
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  • #16
Chen said:
h = \frac{3v^2}{4g}
I agree, of course. (I misread your answer, Chen, like psruler did. :rolleyes: )
 
  • #17
I have a question now. Let's say it is a sphere now, instead of a cylinder. The equation would be:

mgh = \frac{1}{2}mv^2 + \frac{1}{2}I\omega ^2 = \frac{1}{2}mv^2 + \frac{1}{5}mr^2\omega ^2 = \frac{7}{10}mv^2

v^2 = \frac{10gh}{7}

But now let's take that sphere and reduce its radius until it tends to zero (so we find ourselves with a "point" particle). Obviously the mass and the radius of the object do not affect the speed it would reach at the bottom of the hill, as that only depends on the height of it. So on one hand, we know that for point particles there is no such thing as rotational kinetic energy, so the speed squared would be 2gh. However, if we do count the rotational KE we find the speed squrared to be of 10gh/7. So which answer is the correct one? And where's the limit between a point particle and a sphere? i.e when in the process of reducing the object's radius will the speed change from one expression to the other?
 
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  • #18
An excellent question!

Chen said:
... So on one hand, we know that for point particles there is no such thing as rotational kinetic energy, so the speed squared would be 10gh/7. However, if we do count the rotational KE we find the speed squrared to be of 2gh. So which answer is the correct one? And where's the limit between a point particle and a sphere? i.e when in the process of reducing the object's radius will the speed change from one expression to the other?
This is an excellent question, Chen! (I think you have the cases mixed, though.) I think when you reach that limit, the normal analysis of static friction causing rotation will break down. Surface effects will dominate.
 

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