Angular velocity of falling box

AI Thread Summary
The discussion focuses on calculating the angular velocity of a falling, rotating box using energy conservation principles. The initial formula for angular velocity at a horizontal point is provided, and participants discuss the relationship between potential energy (PE) and kinetic energy (KE) during the fall. Clarifications are made regarding the center of rotation and the moment of inertia, emphasizing that these factors change with the angle of rotation. The user encounters issues with their simulation results, specifically the expected graph of angular velocity not aligning with actual outputs, leading to further inquiries about the data series in the graph. The conversation highlights the complexities of simulating rotational motion and the importance of accurate data representation.
GeorgeM
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Hi,

I'm preparing a computer software to simulate the fall of an object for an academic project. The object is rotating (not rolling) over the circular bottom point. I know that the angular velocity at the horizontal point is ω = √(3g/L). I would like to calculate the angular velocity at every angle (from 90° to 180°). Can you please provide a simple formula for this?

Thanks
 

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It is your project.
Energy conservation should work. For every rotation angle, you can calculate the potential energy, the difference to the original value got converted to kinetic energy.
 
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So, you are proposing the following:

The difference in PE is equal to the KE, that is ΔPE = KE.
Ex: PE1 - PE2 = ½ m⋅v2
Then I solve for v, but this v is the vector from the COM to the ground. Will then have to calculate ω.
Or else, use the angular KE?
Is that right?
 
Last edited:
The kinetic energy of a rotating object is not 1/2 m v^2. You'll have to find the center of rotation and the moment of inertia around it, or sum rotational energy (around a different point) plus lateral motion.
 
Yes, my mistake, KE = ½⋅I⋅ω2
May I ask what you mean by the centre of rotation? Is this the pivot point on the ground?
 
GeorgeM said:
Yes, my mistake, KE = ½⋅I⋅ω2
If you measure I around a point that does not move, yes. But then I depends on the angle if you want to be precise.
May I ask what you mean by the centre of rotation? Is this the pivot point on the ground?
Yes.
 
mfb said:
But then I depends on the angle if you want to be precise
Is this because of the opposite forces of the rotating body towards the rotation point? Can you clarify this please?
 
The point that has contact to the surface changes over time.
 
Hi again,
I did the calculations on my software, but the graph of ω is not what I expect. See series 1 on attached image (x axis =frame no, y-axis = ω).
It should show a slower increase in acceleration at the beginning of the fall. Any ideas?
 

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  • #10
Where is series 1?
Yes, acceleration should increase over time.
 
  • #11
Yes, series 1, but it shouldn't accelerate at this step. It should look like the attached image. Notice that for the first frames/angles the velocity is not as accelerated as on the later frames/angles. I think something is missing here...
 

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  • #12
GeorgeM said:
Yes, series 1
I don't see series 1 there. Just 2, 3 and 4.
 
  • #13
Is only series 1 in the graph at post #11
 
  • #14
GeorgeM said:
Is only series 1 in the graph at post #11

you are still not understanding mfb's comment

there is NO series 1 plotted in your graph, only series 2, 3, and 4

so where is the series 1 data ?D
 
  • #15
There IS one series in ejs-graph-jpg
 
  • #16
Yes, but that graph shows the expected result. So where is the problem? The attachment of post 9, where you discussed the problem with "series 1", does not have a series 1.
 

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