Centripetal Force & Gas Centrifuges

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Discussion Overview

The discussion revolves around centripetal force and acceleration in the context of gas centrifuges and circular motion. Participants explore the calculations of centripetal acceleration, the interpretation of acceleration in uniform circular motion, and the plausibility of the values obtained for gas centrifuges.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant calculates centripetal acceleration for a gas centrifuge but questions the plausibility of the resulting value, suggesting it seems excessively high.
  • Another participant challenges the initial formula used for calculating velocity, pointing out a unit mismatch and clarifying that acceleration is a vector quantity related to changes in velocity, not just speed.
  • A later reply attempts to correct the calculation but still questions the plausibility of the resulting acceleration for a gas centrifuge.
  • Participants discuss the interpretation of acceleration in uniform circular motion, with one expressing confusion about how to understand acceleration when speed remains constant, while others clarify that acceleration refers to a change in velocity, which includes direction.
  • One participant seeks clarification on how to visualize the concept of acceleration in terms of changing direction, particularly when speed does not change.
  • Another participant provides a link to an external resource that includes a diagram, which is appreciated by the original poster.
  • There is a discussion about the vector nature of velocity and how the magnitude remains constant in uniform circular motion, while the direction changes, leading to a non-zero vector difference.
  • One participant asserts that the calculated acceleration is of the right order of magnitude for a gas centrifuge, suggesting it may be plausible.

Areas of Agreement / Disagreement

Participants express differing views on the calculations of centripetal acceleration and its plausibility for gas centrifuges. There is also a lack of consensus on the interpretation of acceleration in uniform circular motion, with some participants clarifying concepts while others remain confused.

Contextual Notes

Some calculations presented may depend on assumptions about the parameters used, and there are unresolved questions regarding the interpretation of acceleration in circular motion. The discussion includes corrections and refinements of earlier claims without reaching a definitive conclusion.

Who May Find This Useful

Students studying circular motion, educators looking for examples of centripetal acceleration, and individuals interested in the physics of gas centrifuges may find this discussion relevant.

Jimmy87
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Hi,

I am studying circular motion at the moment and we were asked to go away and find an example of a device which has a very large centripetal acceleration. Initially I found a washing machine has up to about 300g but then I was looking at nuclear enrichment gas centrifuges which have huge accelerations. I can;t find a source that mentions the acceleration but I have found sources that tell you the information you need:

Radius of Centrifuge = 4 inches
Frequency of Rotation = 2000Hz

a = v2/r

v = 2πf

So, a = (2πf)2/r = (2π x 2000)2/0.1016 = 1.55 x 109 ms-2

So I come to my main question - what have I done wrong as this is way too high.

I also have a second question. When an object is undergoing uniform circular motion how do you interpret the acceleration. What I mean is that it is really easy to understand a car accelerating in a straight line because it tells you how many m/s his speed is increasing every second. For example, an acceleration for a car of 3m/s2 that is not changing direction means that every second the speed is increasing by 3m/s. What does 3m/s2 mean when the object is going round in a circular at constant speed though. How can 3m/s every second relate to a change in direction?

Thanks for any help,
 
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Jimmy87 said:
v = 2πf
This is obviously false as the units do not match. The left-hand side has units of length/time and the right-hand side has units of 1/time.
Jimmy87 said:
What does 3m/s2 mean when the object is going round in a circular at constant speed though. How can 3m/s every second relate to a change in direction?
Acceleration is not the change in speed, which is a scalar. It is the change in velocity, which is a vector.
 
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Orodruin said:
This is obviously false as the units do not match. The left-hand side has units of length/time and the right-hand side has units of 1/time.

Acceleration is not the change in speed, which is a scalar. It is the change in velocity, which is a vector.

Thanks - how silly of me. So would it be:

So, a = (2πfr)2/r = (2π x 2000 x 0.1016)2/0.1016 = 1.6 x 107 ms-2

That still seems very high - is that plausible for a gas centrifuge?

About my second question - I think I wasn't clear with what I was asking. I know velocity is a vector and that the speed can remain constant whilst the object is accelerating (e.g. circular motion). However, how do you interpret the value of the acceleration if the speed is remaining constant? If the acceleration is 3m/s2 for example and the speed is not changing then what does 3m/s per second actually mean? That the direction is changing by 3m/s per second? What does that even mean?
 
I am sorry, but I cannot understand how you can say this
Jimmy87 said:
I know velocity is a vector and that the speed can remain constant whilst the object is accelerating (e.g. circular motion).
and yet not be ok with this
Jimmy87 said:
However, how do you interpret the value of the acceleration if the speed is remaining constant?
Acceleration is change of velocity with time, if there is a non-zero acceleration, then the velocity will be different at a later time. If the difference in time is small, then
$$
\vec v_2 = \vec v_1 + \vec a (t_2-t_1).
$$
All that is being said is how the velocity changes with time for small times. Note that acceleration is also a vector, it has a direction - the direction in which the velocity changes.
 
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Orodruin said:
I am sorry, but I cannot understand how you can say this

and yet not be ok with this

Acceleration is change of velocity with time, if there is a non-zero acceleration, then the velocity will be different at a later time. If the difference in time is small, then
$$
\vec v_2 = \vec v_1 + \vec a (t_2-t_1).
$$
All that is being said is how the velocity changes with time for small times. Note that acceleration is also a vector, it has a direction - the direction in which the velocity changes.

I am perfectly fine with the fact that an object can accelerate even though speed is constant. Changing direction requires a resultant force and F=ma tells us there must then be an acceleration. It is not this I am not ok with it is just interpreting the value of the acceleration in terms of changing direction only. It makes perfect sense to say that an acceleration of 3m/s2 means that the speed increases by 3m/s every second. However, if the speed is constant then we are now saying that the direction changes by 3m/s every second. I can see it mathematically but can't picture what that means. Would that equation you gave work for acceleration at constant speed? The magnitude of your v2 will be different to v1 and I thought the magnitude is the speed and won't change in this example?
 
Jimmy87 said:
The magnitude of your ##v_2## will be different to ##v_1##
In uniform circular motion, the magnitude of ##v_2## and ##v_1## will be identical. But, because their directions are different, their vector difference will be non-zero. If the difference in angle between ##v_1## and ##v_2## is tiny, the vector difference can be visualized as the base of a tall, thin isoceles triangle with ##v_1## and ##v_2## as the equal sides and the vector difference as the remaining side.
 
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