Find average velocity of a sphere which expands and moves

AI Thread Summary
The discussion revolves around calculating the average velocity of a moving and expanding spherical shell, where participants debate the correct approach to the problem. It is clarified that the expansion velocities do not cancel out unless considering the center of mass, leading to confusion about the kinetic energy calculations. Participants emphasize that energy is a scalar quantity, and the average kinetic energy cannot simply be derived from squaring the average velocity. The conversation also touches on the complexity of using integrals and the importance of symmetry in simplifying the problem. Ultimately, the need for a correct mathematical framework to solve the problem is highlighted.
Quarlep
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Homework Statement


Find the average velocity of shell while its moves a velocity v' and expands a velocity v.
Sphere radius is R
Expansion velocity v
Movement velocity v'

Homework Equations


I think there's no need an equation.[/B]

The Attempt at a Solution


I try to find average velocity but its vector.So I made max velocity v+v' and min velocity v-v' then I add them and divide two and I find v but I think I made a mistake.
 
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That's right. If you draw a line in any direction through the shell's centre those expansion velocities cancel out so you are just left with v
 
Expansion velocities can't cancel v is expansion velocity v' is object velocity.I didnt mention it but shell is a surface of sphere.And I didnt understand your prove
 
Ok ignore v' eg imagine the sphere is stationary what is the average velocity of the sphere shell. The speed is v but the velocity which is a vector cancels out: if you imagine any point on the sphere - there is one going in exactly the opposite direction so when you add them all up the answer is 0.
 
So that expansion velocities cancels and left only v which speed of sphere
 
I am so so sorry .I made a mistake in my equation it must be v'-v not v-v' my fault.
I want to ask another question.Before sphere moves, shell energy will be 1/2mv^2(v is shell expansion speed) but after sphere moves shell energy will be 1/2mv^2 (v is the sphere velocity) isn't it ?
 
Quarlep said:
So that expansion velocities cancels and left only v which speed of sphere

The expansion velocities don't "cancel out" unless we are considering the velocity of the center of mass of the sphere. In which case you are right, the velocity of the center of mass of the sphere should stay constant.

Quarlep said:
I want to ask another question.Before sphere moves, shell energy will be 1/2mv^2(v is shell expansion speed) but after sphere moves shell energy will be 1/2mv^2 (v is the sphere velocity) isn't it ?

No, I don't believe so. Energy is a scalar quantity, so the expansion velocities will not conveniently cancel out. The only way that I am able to come to any sort of meaningful conclusion regarding the kinetic energy of the sphere is by considering the kinetic energy of the sphere at the very instant that the sphere begins to expand. Here is a picture to help you visualize the situation.
Snapshote.jpg
 
I am not talking about kinetic energy of sphere.I am talking about shell energy
 
Quarlep said:
I am not talking about kinetic energy of sphere.I am talking about shell energy

Sorry, the shell. I accidentally used the term sphere instead of shell. Please forgive me.

Quarlep said:
shell energy will be 1/2mv^2(v is shell expansion speed) but after sphere moves shell energy will be 1/2mv^2 (v is the sphere velocity) isn't it ?

Can you explain your reasoning?
 
  • #10
When shell is not moving shell energy will be the "energy " which that energy causes expension of shell and that's the 1/2m2v2.Then shell moves and the speed of shell will be (as you mentioned vectors of speeds which you add them and calculations shows a v which is the speed of movement) so energy of shell will be 1/2mshellv2 v is speed of sphere
 
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  • #11
Quarlep said:
When shell is not moving shell energy will be the "energy " which that energy causes expension of shell and that's the 1/2m2v2.Then shell moves and the speed of shell will be (as you mentioned vectors of speeds which you add them and calculations shows a v which is the speed of movement) so energy of shell will be 1/2mshellv2 v is speed of sphere

My good chap, I am afraid that any solution to your somewhat vague question is significantly more complicated. Why don't you examine the problem further, and maybe sleep on it. Then show us what you have come up with. Perhaps my diagram will give you some inspiration.
 
  • #12
Look the prove of speed.
 

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  • #13
Quarlep said:
Look the prove of speed.
Yes, that correctly shows the expansion cancels out when computing average velocity. But average KE is not given by squaring average velocity. You have to find the KE of each element separately and then integrate.
There's an analogous result in statistics: the variance is the mean square minus the square of the mean.
 
  • #14
haruspex said:
There's an analogous result in statistics: the variance is the mean square minus the square of the mean.

I didnt understand this and here what I found
 

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  • #15
Quarlep said:
I didnt understand this and here what I found
The integrals on the left are ok, but they don't give the answer on the right. please post your steps.
 
  • #16
Here the steps
 

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  • #17
Quarlep said:
Here the steps
The integrals of sin2 and cos2 cannot cancel to zero. The integrands are non-negative everywhere.
You'll find it simpler if you collapse v2sin2 + v2 cos2 to v2.
 
  • #18
they can cancel to zero.If we integrate (sinx)2 between 0 and π we get π/2 then we integrate same thing again between π and 0 we get -π/2 there's nothing wrong look carefully.Only my first equation can be wrong.But you said that's true so we get mv2
 
  • #19
Quarlep said:
then we integrate same thing again between π and 0
There's your problem, you're running the integral backwards, getting a negative result from an integrand that's never negative.
 
  • #20
You told me the right side of the equation is true.If its true then we need to integrate backward.If you think different way prove me using math.Or my first equation is wrong.
 
  • #21
Quarlep said:
You told me the right side of the equation is true.
Yes, I'm sorry, I didn't notice the reversed bounds on the second one.
 
  • #22
Can you tell me right equation please.I couldn't figure it out myself that's way I asked in this forum.
 
  • #23
Quarlep said:
Can you tell me right equation please.I couldn't figure it out myself that's way I asked in this forum.
As I posted, the best is to simplify the expression first. sin2x+cos2x=1.
For the integral bounds, just put them in the order of increasing variable value, 0 to pi, or -pi to 0, not pi to 0.

Oh dear, I must be half asleep. I forgot this is about a spherical shell, not simply a circle. That means you should be using a double integral in spherical polar coordinates.
 
  • #24
haruspex said:
Oh dear, I must be half asleep. I forgot this is about a spherical shell, not simply a circle. That means you should be using a double integral in spherical polar coordinates.

Up past your bedtime doing double integrals, I see.

Perhaps we should assume a thin spherical shell in order to simplify this problem a little? I get the impression that finding the kinetic energy of this moving and expanding shell was not intended to be a part of this problem in the first place.
 
  • #25
Yeah its a spherical shell.All equations should change now.Can somebody telll me the full equation please ( You need to write it) As I mentioned its not a circle its a sphere.I am 18 I learned Integrals 1 week ago.I don't how to do it myself Just please can somebody calculate it for me.Its very important please.
 
  • #26
Here what I found.Is that works ?
 

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  • #27
Quarlep said:
Yeah its a spherical shell.All equations should change now.Can somebody telll me the full equation please ( You need to write it) As I mentioned its not a circle its a sphere.I am 18 I learned Integrals 1 week ago.I don't how to do it myself Just please can somebody calculate it for me.Its very important please.
I wasn't sure whether you just needed a way to get an answer or wanted to see how it could all be done with integrals. Integrals can be avoided, pretty much. Just use the symmetry. Consider two diametrically opposite mass elements and add up their KEs.
 
  • #28
haruspex said:
I wasn't sure whether you just needed a way to get an answer or wanted to see how it could all be done with integrals. Integrals can be avoided, pretty much. Just use the symmetry. Consider two diametrically opposite mass elements and add up their KEs.

Its my project homeworks one part.So I need equations. Symmetry Idea is very good.I am thinking.You didnt mention anything about my eq but can it be true
 
  • #29
Quarlep said:
Its my project homeworks one part.So I need equations. Symmetry Idea is very good.I am thinking.You didnt mention anything about my eq but can it be true
I'm afraid I could not make any sense of your latest equations. There seem to some parentheses and plus signs missing, I couldn't understand the bit about "points for which... are constant", or how you would be integrating wrt r instead of wrt theta and phi.
 
  • #30
I ll explain it in a moment but now I made a circle shell energy formula.
 
  • #31
Here
 

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  • #32
Quarlep said:
Here
Yes, that's right for an expanding ring. A spherical shell is the same except that you need a double integral.
Let me give you a start on that. Are you familiar with Archimedes' proof of the area of a sphere?
 
  • #33
No
 
  • #34
Quarlep said:
No
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.
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.
 
  • #35
I didnt understand.
 
  • #36
Quarlep said:
I didnt understand.
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##.
 
  • #37
Its too complicated isn't it ?
 
  • #38
I have no idea how did I get this equation but here it is
 

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  • #39
Quarlep said:
I have no idea how did I get this equation but here it is
You can make it simpler by recognising that the KE only depends on theta, not phi.
 
  • #40
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 ...
 
  • #41
Quarlep said:
Ok, I ll make it simpler but my equation is full correct isn't it ? No mistake Even multiply integral with 2 ...
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.
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.
 
  • #42
Spherical coordinates make this way more complicated.

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.
 
  • #43
How I need help.My math is not good enough
 
  • #44
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.
Sure, but the challenge is to resolve the apparent contradiction that Quarlep came up with by using integration methods.
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.
 
  • #45
I tried to to use symmetry but again I don't know how to do it.I am worling on
 
  • #46
Quarlep said:
I tried to to use symmetry but again I don't know how to do it.I am worling on
As I said, just add the KEs of two diametrically opposite points in the shell.
 
  • #47
Yeah you know that I used it find KE of ring shell
 
  • #48
Quarlep said:
Yeah you know that I used it find KE of ring shell
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.
 
  • #49
Theres one cos isn't it.Or I couldn't see
 
  • #50
Quarlep said:
Theres one cos isn't it.Or I couldn't see
The sign of the cos term for one point will be opposite to that on the diametrically opposite point.
You should have ##(v'+v_r\cos(\theta))^2+(v'-v_r\cos(\theta))^2##, plus the y direction terms.
 
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