How the distance from centre decides type of charge motion?

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Discussion Overview

The discussion revolves around the motion of a charge -Q in relation to its distance from the center of a uniformly charged sphere. Participants explore the differences between oscillatory motion and simple harmonic motion (SHM), particularly how the distance from the center influences the type of motion exhibited by the charge. The conversation includes theoretical considerations and interpretations of force laws.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that a charge -Q at a large distance from the center will exhibit oscillatory and periodic motion, while a charge released close to the origin will execute SHM.
  • One participant questions what is at the origin that causes this difference in motion and seeks to distinguish between "oscillatory and periodic" motion and SHM.
  • It is suggested that a diffuse, spherically symmetric cloud with uniform positive charge density centered on the origin influences the motion of the charge -Q.
  • Participants discuss the implications of the spherical shell theorem, noting that only the portion of the charge cloud closer to the origin affects the net force on the test charge.
  • There is a clarification that the net attraction experienced by the charge is proportional to its distance from the origin, due to the volume of the charge cloud being proportional to r³ and the force law being inversely proportional to r².
  • Some participants express confusion over the definitions and relationships between the distances and charges involved in the discussion.
  • There is an agreement that the portion of the charge cloud farther from the origin than the test charge produces no net electrical field on the test charge.

Areas of Agreement / Disagreement

Participants generally agree on the application of the spherical shell theorem and its implications for the net electrical field. However, there remains some confusion and lack of consensus regarding the definitions and implications of oscillatory motion versus SHM, as well as the specific relationships between the distances and charges discussed.

Contextual Notes

Some participants express uncertainty about the definitions of variables and the implications of the spherical shell theorem in this context. The discussion includes unresolved mathematical relationships and assumptions regarding the charge distribution and its effects on motion.

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If charge -Q of mass m is kept on y-axis at large distance from the center,then it will execute oscillatory and periodic motion but if it is released very close to the origin then it will execute SHM .I want to know why?I mean how the distance from centre decides type of motion oscillatory or SHM?
 
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gracy said:
If charge -Q of mass m is kept on y-axis at large distance from the center,then it will execute oscillatory and periodic motion but if it is released very close to the origin then it will execute SHM .I want to know why?I mean how the distance from centre decides type of motion oscillatory or SHM?
What is at the origin to cause this? What, in your opinion distinguishes "oscillatory and periodic" motion from simple harmonic motion?

Edit: at a guess, we have a diffuse, spherically symmetric cloud with a uniform positive charge density centered on the origin. A charge far away sees an inverse square force law (-1/r^2) and a charge located within the cloud sees a force law that is directly proportional to distance (-r).
 
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jbriggs444 said:
oscillatory and periodic" motion from simple harmonic motion?
Both are periodic. The basic difference between the two is that in shm acceleration is directly proportional to displacement which is not there in case of oscillation.
 
jbriggs444 said:
A charge far away sees an inverse square force law (-1/r^2)
This is coulomb's force,I know.
jbriggs444 said:
and a charge located within the cloud sees a force law that is directly proportional to distance (-r)
But I don't know which force are you talking about here?
 
gracy said:
This is coulomb's force,I know.
But I don't know which force are you talking about here?
The Coulomb force.

According to the spherical shell theorem, the portion of the charge cloud farther from the origin than the -Q test charge cancels out to a net of zero. So only the portion of the cloud nearer the origin than the test charge matters. That portion of the cloud has volume proportional to r3 and inverse square attraction proportional to 1/r2. That means that the net attraction is proportional to r.
 
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jbriggs444 said:
spherical shell theorem
but it is for gravitation.
 
gracy said:
but it is for gravitation.
That is for any force that follows an inverse square law.
 
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Ok.Please don't go anywhere.I have to some queries.
 
jbriggs444 said:
That portion of the cloud has volume proportional to r3 and inverse square attraction proportional to 1/r2. That means that the net attraction is proportional to r.
could you please elaborate this part?
 
  • #10
jbriggs444 said:
spherical shell theorem
That means overall(total) charge can be treated as/assumed to be concentrated at a point at its centre.
 
  • #11
jbriggs444 said:
on the origin
You meant centre of the sphere.
 
  • #12
gracy said:
That means overall(total) charge can be treated as/assumed to be concentrated at a point at its centre.
Right.

Uniform charge density. Sphere with volume that goes as r3. So total enclosed charge proportional to r3. Field equivalent to that charge at origin. Inverse square force law. So net field strength at radius r scales as r3/r2.
 
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  • #13
gracy said:
You meant centre of the sphere.
Yes, as in post #2, I am guessing that you are discussing a situation with a cloud of charge of uniform density centered at the origin. The center of a sphere of radius r centered at the origin is at the origin (by definition).
 
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  • #14
jbriggs444 said:
the portion of the charge cloud farther from the origin than the -Q test charge
If we take distance of -Q from centre of sphere i.e origin as "a" & the portion of the charge cloud to be q and radius of sphere to be r
let b be any value less than r .If r>b or r>a
that's what it means?
 
  • #15
gracy said:
If we take distance of -Q from centre of sphere i.e origin as "a" & the portion of the charge cloud to be q and radius of sphere to be r let b be any value less than r .If r>b or r>a
that's what it means?
That is nonsense. You stated that -Q is a quantity of charge. It cannot also be a distance.
 
  • #16
jbriggs444 said:
It cannot also be a distance.
Where i said -Q is distance?
 
  • #17
jbriggs444 said:
That is nonsense. You stated that -Q is a quantity of charge. It cannot also be a distance.
Edit: I apologize. You mean the distance from the origin to the charge whose value is -Q. And you want to denote that as a. I am not sure what you want q and r and b to denote.
 
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  • #18
jbriggs444 said:
You mean the distance from the origin to the charge whose value is -Q. And you want to denote that as a.
yes
 
  • #19
please make it more clear.It's my humble request
jbriggs444 said:
Uniform charge density. Sphere with volume that goes as r3. So total enclosed charge proportional to r3. Field equivalent to that charge at origin. Inverse square force law. So net field strength at radius r scales as r3/r2.
 
  • #20
gracy said:
please make it more clear.It's my humble request
What is it that you would like clarified?
 
  • #21
Uniform charge density. Sphere with volume that goes as r3. So total enclosed charge proportional to r3
Till here I understood.
 
  • #22
Field equivalent to that charge at origin. Inverse square force law. So net field strength at radius r scales as r3/r2.
I am unable to link
 
  • #23
So you agree that if we have a uniform cloud of charge centered on the origin and a test charge at distance r from the origin that the total charge closer to the origin than the test charge is proportional to r3

Do you agree that if this cloud of charge is spherical then the portion which is farther than r from the origin produces no net electrical field on the test charge? The spherical shell theorem should tell you this.

Do you agree that the field from the portion of the could which is nearer than r from the origin produces an electrical field on the test charge identical to that which would be produced if its entire charge were concentrated at the origin? The spherical shell theorem should also tell you this.
 
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  • #24
jbriggs444 said:
Do you agree that if this cloud of charge is spherical then the portion which is farther than r from the origin produces no net electrical field on the test charge? The spherical shell theorem should tell you this?
yes.
jbriggs444 said:
Do you agree that the field from the portion of the could which is nearer than r from the origin produces an electrical field on the test charge identical to that which would be produced if its entire charge were concentrated at the origin? The spherical shell theorem should also tell you this.
yes
jbriggs444 said:
So you agree that if we have a uniform cloud of charge centered on the origin and a test charge at distance r from the origin that the total charge closer to the origin than the test charge is proportional to r3
I am so sorry ;did not get you.
 
  • #25
jbriggs444 said:
So you agree that if we have a uniform cloud of charge centered on the origin and a test charge at distance r from the origin that the total charge closer to the origin than the test charge is proportional to r3
Should I think of coordinate system.
 
  • #26
jbriggs444 said:
So you agree that if we have a uniform cloud of charge centered on the origin and a test charge at distance r from the origin that the total charge closer to the origin than the test charge is proportional to r3
Yes.I understand it now .
 
  • #27
jbriggs444 said:
So you agree that if we have a uniform cloud of charge centered on the origin and a test charge at distance r from the origin that the total charge closer to the origin than the test charge is proportional to r3

Do you agree that if this cloud of charge is spherical then the portion which is farther than r from the origin produces no net electrical field on the test charge? The spherical shell theorem should tell you this.

Do you agree that the field from the portion of the could which is nearer than r from the origin produces an electrical field on the test charge identical to that which would be produced if its entire charge were concentrated at the origin? The spherical shell theorem should also tell you this.
How does it answer my OP?
 
  • #28
gracy said:
Should I think of coordinate system.
No. The coordinate system is irrelevant.

We have a uniform cloud of charge.
Somewhere within this cloud of charge is a point we call the origin.
Somewhere else within this cloud of charge we have a test charge.
We measure the distance from the origin to the test charge.
We call this distance "r".
We draw an imaginary spherical shell that is centered on the origin and has radius r.
This spherical shell encloses a certain volume -- given by 4/3 pi r3
It encloses a certain amount of charge.
The amount of charge is proportional to the volume.
The volume is proportional to r3
Can you see that the amount of charge enclosed by this shell is proportional to r3

If you keep everything else constant and double r, by what factor will the amount of enclosed charge have increased?
 
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  • #29
gracy said:
How does it answer my OP?
Your OP was unclear. I had to guess what you were talking about. 27 posts later and you still have not clarified it.
 
  • #30
jbriggs444 said:
If you keep everything else constant and double r, by what factor will the amount of enclosed charge have increased?
8 times?
 

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