There are more than one center of mass for a n-particles system

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Discussion Overview

The discussion revolves around the concept of the center of mass (COM) in a system of n particles, specifically addressing whether there can be more than one center of mass and the implications of different equations representing the COM. Participants explore the definitions and mathematical formulations related to the COM, including the role of external forces and the uniqueness of the COM.

Discussion Character

  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that there is a unique center of mass, referencing the definition provided by equation [2].
  • Others argue that adding a constant vector to the COM does not change the acceleration, suggesting that this indicates a lack of uniqueness in the COM.
  • One participant proposes starting from equation [2] as a definition and transitioning to equation [1] to illustrate the relationship between them.
  • Some participants contend that equation [1] can describe multiple points acting as if all mass is concentrated at those points, challenging the uniqueness of the COM.
  • There is a discussion about the sufficiency of equation [1] in defining the COM, with some stating it only addresses translational acceleration and is therefore inadequate for defining a unique center of mass.
  • Concerns are raised about the implications of external forces on the definition of the COM, with some participants questioning the validity of equation [2] in scenarios without external forces.
  • One participant mentions the practical application of the COM in finding the balance point of a non-uniform beam, suggesting that the definition provided by equation [2] is necessary for such cases.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the uniqueness of the center of mass. Multiple competing views are presented regarding the definitions and implications of the equations discussed, particularly between equations [1] and [2].

Contextual Notes

There are unresolved questions regarding the assumptions behind the definitions of the center of mass, particularly in relation to external forces and the conditions under which the equations apply. The discussion highlights the complexity of the topic and the nuances in the mathematical representations of the COM.

ManishR
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RCOM is a vector from an inertial frame to the point called the center of mass. The system behaves as if all the mass is concentrated at the center of mass and all the external forces act at that point. so

[tex]\frac{d^{2}}{dt^{2}}\overrightarrow{R}{}_{COM}=\frac{\sum m_{i}\frac{d^{2}}{dt^{2}}\overrightarrow{r_{i}}}{\sum m_{i}}[/tex] ...[1]

or

[tex]\frac{d^{2}}{dt^{2}}(\overrightarrow{R}{}_{COM}+\overrightarrow{k})=\frac{\sum m_{i}\frac{d^{2}}{dt^{2}}\overrightarrow{r_{i}}}{\sum m_{i}}[/tex]

so there are more than one center of mass for a system.

but if center of mass is

[tex]\overrightarrow{R}{}_{COM}=\frac{\sum m_{i}\overrightarrow{r_{i}}}{\sum m_{i}}[/tex] ...[2]

or there is unique center of mass for a system.

whats wrong here ? how did we reach from [1] to [2] ?
 
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There is a unique center of mass. If you add a constant vector and then take a derivative, there is no difference in the result, since the derivative of a constant is zero.
 
I think it's more instructive to start at [2] and go to [1]. You can think of [2] as a definition.
 
mathman said:
There is a unique center of mass. If you add a constant vector and then take a derivative, there is no difference in the result, since the derivative of a constant is zero.

yes, but it means COM is not unique.

let say RCOM is the position vector of COM from inertial frame then from the same inertial frame a position vector = (RCOM vector + K vector) also satisfy the equation [1].
or
mathematically, differentiation of something is actually a function, so the "something" has more than one value not unique value.

JohnSimpson said:
I think it's more instructive to start at [2] and go to [1]. You can think of [2] as a definition.

the idea behind COM is that, it is a point such that all mass of system is concentrated into that point and the external forces that were acting on each particle of the system, act on that COM. so
F=ma
F = sum of all external forces
m = mass of system
a = acceleration of COM from an inertial frame

so, the position of RCOM is given by equation [1].

Equation [1] is what we have to start with, not equation [2]

however its equation [2] which tells us that there is unique COM.
 
ManishR said:
the idea behind COM is that, it is a point such that all mass of system is concentrated into that point and the external forces that were acting on each particle of the system, act on that COM. so
F=ma
F = sum of all external forces
m = mass of system
a = acceleration of COM from an inertial frame

so, the position of RCOM is given by equation [1].
I'd say that was incorrect. Equation [1] is not the defining equation for COM. If all you care about is acceleration, you can always add a constant to the COM and get the same acceleration. So what?

Your equation [2] is the definition of COM.
 
Doc Al said:
I'd say that was incorrect. Equation [1] is not the defining equation for COM. If all you care about is acceleration, you can always add a constant to the COM and get the same acceleration. So what?

Your equation [2] is the definition of COM.

yes that's the only explanation, but why ?

look jpg which is pg 116 of An Introduction to Mechanics by Daniel Kleppner, Robert J. Kolenkow

every point according to equation [1] will act as if all mass is concentrated into that point.
but it seems like in all those points we prefer a point which is defined by equation [2]
but i don't understand why ? its wrong too because equation [2] does not even account for external force. if there is no external force, equation [2] still says COM is unique but it should not be unique.
 

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ManishR said:
every point according to equation [1] will act as if all mass is concentrated into that point.
No. Equation [1] just deals with translational acceleration. It is insufficient to define a unique center of mass.

Say you wanted to find the balance point of a non-uniform beam. The COM (defined by equation [2]) answers that question. Adding an arbitrary constant won't work.
 
Doc Al said:
manishr said:
every point according to equation [1] will act as if all mass is concentrated into that point.
No.
consider a system and if there is a particle whose mass is equal to the mass of system and the force on it is equal to sum of all external force then the position vector R of that point is

[tex]\frac{d^{2}}{dt^{2}}\overrightarrow{R}=\frac{\sum m_{i}\frac{d^{2}}{dt^{2}}\overrightarrow{r_{i}}}{\sum m_{i}}[/tex]

Doc Al said:
Equation [1] just deals with translational acceleration.
No.

since mi is a point size particle so rotation of the point on its own axis is not possible. however the rotation of system on its own axis is possible and it is defined by equation [1]. so equation [1] deals with any kind of motion.
Doc Al said:
Say you wanted to find the balance point of a non-uniform beam. The COM (defined by equation [2]) answers that question. Adding an arbitrary constant won't work.
No.
thats different thing. COM is not a point which balance a body.
 

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