Find average velocity of a sphere which expands and moves
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Homework Help Overview
The discussion revolves around finding the average velocity of a sphere that is both expanding and moving. The original poster presents a scenario involving a shell with a radius R, an expansion velocity v, and a movement velocity v'. Participants explore the implications of these velocities on the average velocity of the shell.
Discussion Character
- Mixed
Approaches and Questions Raised
- Participants discuss the concept of average velocity in the context of a moving and expanding shell, with some suggesting that expansion velocities cancel out while others question this assumption. There are attempts to clarify the distinction between speed and velocity, particularly regarding the vector nature of these quantities.
Discussion Status
The discussion is ongoing, with participants raising questions about the relationship between the shell's expansion and movement velocities. Some guidance has been offered regarding the conceptual understanding of kinetic energy and the need for careful consideration of integrals in the context of the problem.
Contextual Notes
There is a noted complexity in the problem, particularly regarding the integration of velocities and the distinction between kinetic energy of the shell and the sphere. Participants express uncertainty about the correct equations and methods to apply, indicating a need for further exploration of the topic.
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Yes, that's right for an expanding ring. A spherical shell is the same except that you need a double integral.Quarlep said:Here
Let me give you a start on that. Are you familiar with Archimedes' proof of the area of a sphere?
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He effectively invented calculus. He considered a cylinder enclosing the sphere, same radius, and a thin slice through the sphere cutting the cylinder perpendicularly to its axis. By geometry, he showed that the area of cylinder within the slice was (in the limit) the same as the area of sphere surface within the slice.Quarlep said:No
Thus, if we consider a band around the sphere between an angle ##\theta## and ##\theta+d\theta## to the cylinder's axis, its surface area is ##2 \pi r \sin(\theta)d\theta##.
But because that band is not all moving in the same direction in your problem, we need to do an integral just to get the KE of that band. Have a go at that.
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Take an element on the shell in spherical polar co-ordinates. Write out its KE. If theta is the angle to the line of movement of the shell's mass centre, integrate in a band of width ##rd\theta## for ##\phi## from 0 to ##2\pi##.Quarlep said:I didnt understand.
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You can make it simpler by recognising that the KE only depends on theta, not phi.Quarlep said:I have no idea how did I get this equation but here it is
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haruspex said:You can make it simpler by recognising that the KE only depends on theta, not phi.
Ok, I ll make it simpler but my equation is full correct isn't it ? No mistake Even multiply integral with 2 ...
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Not really. Not sure what your ##v_{\theta}## and ##v_{\phi}## terms are. If they're vectors, they should all be inside the first squared term with v' and vr. I.e. the overall velocity is the sum of four vectors, v' and three velocities relative to v'. But then ##v_{\theta}## and ##v_{\phi}## would both be zero. If they're not vectors, maybe you intend them as the scalar magnitudes of those vectors, in which case the same comment applies.Quarlep said:Ok, I ll make it simpler but my equation is full correct isn't it ? No mistake Even multiply integral with 2 ...
So in your equation, throw those two away and expand the remaining squared term. Two of the resulting terms will be independent of theta and phi. The third one, the dot product of v' and vr, will be a function of theta. The integral is then easy.
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There is a nice theorem about the kinetic energy of a system if you know the kinetic energy in its center of mass system and the velocity of this center of mass. Both are easy to find here.
If you don't want to use this theorem, you can split the sphere into two parts and derive a special case of the theorem for this sphere.
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Sure, but the challenge is to resolve the apparent contradiction that Quarlep came up with by using integration methods.mfb said:There is a nice theorem about the kinetic energy of a system if you know the kinetic energy in its center of mass system and the velocity of this center of mass. Both are easy to find here.
If you don't want to use this theorem, you can split the sphere into two parts and derive a special case of the theorem for this sphere.
I gave Quarlep an easy way using symmetry, but he/she seems to want to do it using a more general approach. Certainly it looks like there is merit in Quarlep having a work-out in integration.
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As I said, just add the KEs of two diametrically opposite points in the shell.Quarlep said:I tried to to use symmetry but again I don't know how to do it.I am worling on
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Do you mean in post #31? I didn't realize that's what you had attempted to do there. If it is, you didn't do it right. The two cos terms should have opposite signs and cancel.Quarlep said:Yeah you know that I used it find KE of ring shell
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The sign of the cos term for one point will be opposite to that on the diametrically opposite point.Quarlep said:there's one cos isn't it.Or I couldn't see
You should have ##(v'+v_r\cos(\theta))^2+(v'-v_r\cos(\theta))^2##, plus the y direction terms.
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Almost. The m/2 should be a factor of the whole, and the factor 2 you have in front only applies to the sin term.Quarlep said:Is this true
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Yes, that's good, but you don't need to do an integral at all this way. When you expand the terms, all references to theta should disappear, so all the terms are constants.Quarlep said:Ok,now
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In post 31 I guess m(v^2+v'^2)
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You mean, you got the same result as integrating around a circle? Good.Quarlep said:Ok,I did it and I found what I found before.
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