The Attractive Power of the Inverse Square Potential: Do Examples Exist?

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SUMMARY

The discussion focuses on the existence of attraction forces characterized by an inverse square potential, specifically described by the equation V(r) ∼ -1/|r|² as r approaches 0. Participants identify the electrostatic force on a dipole as a relevant example, which scales as an inverse cube force law, V ∼ -1/|r|³. The conversation also highlights the multipole expansion in molecular physics, detailing various potentials such as -1/R² for ion-dipole interactions and -1/R³ for dipole-dipole interactions. The need for clarity on the dipole's potential formulation is emphasized, particularly regarding its behavior in polar coordinates.

PREREQUISITES
  • Understanding of inverse square law in physics
  • Familiarity with electrostatics and dipole interactions
  • Knowledge of multipole expansion in molecular physics
  • Basic concepts of potential energy in physics
NEXT STEPS
  • Research the mathematical formulation of multipole expansion in molecular physics
  • Study the characteristics of dipole-dipole interactions and their potential equations
  • Explore the implications of inverse cube force laws in various physical systems
  • Examine the behavior of potentials in polar coordinates, particularly for dipoles
USEFUL FOR

Physicists, students of electromagnetism, and researchers interested in molecular interactions and potential energy dynamics will benefit from this discussion.

wrobel
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Do exist examples of attraction forces with such a type potential
##V(\boldsymbol r)\sim-\frac{1}{|\boldsymbol r|^2}, \quad |\boldsymbol r|\to 0##
in physics ?
 
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wrobel said:
Do exist examples of attraction forces with such a type potential
##V(\boldsymbol r)\sim-\frac{1}{|\boldsymbol r|^2}, \quad |\boldsymbol r|\to 0##
in physics ?
Just spit-balling here... An inverse square potential would imply an inverse cube force law. What do we have for inverse cube forces?

How about the electrostatic force on (or from) a dipole. That should scale as the differential of an inverse square, i.e. as an inverse cube.
 
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Thanks. Actually I need physics examples at least such that
##V\sim-\frac{1}{|\boldsymbol r|^n},\quad n\ge 2##
 
jbriggs444 said:
How about the electrostatic force on (or from) a dipole. That should scale as the differential of an inverse square, i.e. as an inverse cube.
Excellent response. You could do arbitrary order multipoles to get any n>0 desired
 
wrobel said:
Thanks. Actually I need physics examples at least such that
##V\sim-\frac{1}{|\boldsymbol r|^n},\quad n\ge 2##
I am not sure how the suggestion of a dipole fails to satisfy that requirement.

It is a net attractive force and consequently has a negative potential everywhere referenced to zero at infinity. So the sign is right. It approximates an inverse square potential. So the approximation is right (when r >> size of dipole). And n=2 which satisfies n>=2.
 
Look up the "multipole expansion" used in molecular physics (for example, in the textbooks by Demtröder).

You get a ##-1/R^2## potential for ion-dipole interaction, ##-1/R^3## for dipole-dipole, ##-1/R^4## for ion-induced dipole, and so on.
 
Thank you everybody so much!

It seems I still have some stupid questions. I have been thinking that dipole is the potential of the type ##V=\frac{\cos\varphi}{r^2}## (in polar coordinates) but this potential changes sign.
Could you please be more detailed?
 
wrobel said:
It seems I still have some stupid questions. I have been thinking that dipole is the potential of the type ##V=\frac{\cos\varphi}{r^2}## (in polar coordinates) but this potential changes sign.
Could you please be more detailed?
In simple terms, a "dipole" would be a pair of equal and opposite charges with some fixed separation. For example, a positive charge and an equal negative charge on opposite ends of an insulating stick.

The net charge of this dipole is zero. And we can consider its location to be the midpoint between the two charges.

Now add a fixed positive point charge at the origin of your coordinate system and have this dipole floating in space somewhere. One could use a negative point charge instead. It changes nothing. What is the force of the point charge on the dipole?

Well, the dipole is going to rotate under the influence of the field so that the negative end faces the central charge and the positive end faces away. That means that your ##cos\varphi## term goes away.

Edit: Apologies for the length and the simple mindedness of the response. I was talking my way through it until I finally got to the point of understanding how you'd arrived at your formulation.
 
Last edited:
wrobel said:
Thank you everybody so much!

It seems I still have some stupid questions. I have been thinking that dipole is the potential of the type ##V=\frac{\cos\varphi}{r^2}## (in polar coordinates) but this potential changes sign.
Could you please be more detailed?
Are you looking asymptotically for a spherically symmetric potential from a localized source ?
 

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