Electric energies between 2 pt charges

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In this discussion, the focus is on the interaction between two point charges, +2Q and -Q, separated by a distance r. Initially, these charges attract each other due to their opposite signs. When they come into contact, conduction occurs, allowing charge redistribution until both charges reach +Q/2. This process raises questions about the timing of repulsion: whether it occurs immediately after the charges equalize or only after further conduction leads to both charges becoming positive.The key points highlight that as long as one charge is negative and the other is positive, attraction persists. Once the negative charge reaches zero and the positive charge is established, repulsion begins as both charges become positive. The discussion emphasizes that this scenario is hypothetical and relies on the assumption of point charges, which lack volume and surface charge distribution, unlike charged spheres that could exhibit different behaviors due to induced charges.
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+2Q and -Q two pt charges are r apart. AS no external agent exists, they attract to each other and each gains +Q/2 after conduction. Like charges repel. At same distance at r, 2*k(2Q)(-Q)/r = 2*k(Q/2)sq /r + 2 KE...
but what i want to know is that when is the like charges repel...just after a -Q of electrons flow from -Q to 2Q they repel...does conduction happen in a very short time to share equal charge of Q/2 before repulsion?? Or just just after a -Q of electrons flow from -Q to 2Q they repel?
 
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That "conduction" is nothing but an electric charge transport process whose main purpose is to equate the electric potential.It happens till the potentials are equal.

Daniel.
 
As I understand what you are saying, there are two point charges separated by a distance r. Some mechanism such as a very thin wire provides a path for charge to flow from one point to the second point. The initial charge configuration has -Q at one point and +2Q at the other. A current will flow from one point to the other until there are equal charges of +Q/2 at both points.

As long as one point is positve and the other is negative, there will be attraction. When the charge at the initially negative point is zero, there will be no attraction. As soon as the intially negative point starts accumulating net positive charge there will be repulsion. All of this neglects any charge remaining in the conducting mechanism (wire) that allows the charge to redistribute.

It is of course a hypothetical problem, but it is very important that the charges are point charges. If the charges were distributed on the surface of sphere, for example, When one shere is neutral and the other has charge Q there would be attraction because the charge on the neutral sphere (or on the positive sphere) would not be uniformly distributed. Negative charges would be attracted to and get closer to the positive sphere, resulting in an attraction between the sheres
 
No OlderDan. You misunderstood me a bit. My view is that when two point charges separated by a distance r attracts each other spontaneously. When they contact, redistribution of charges begins. Electrons flow from Point charge of -Q to Point charge of +2Q, and when it flows -Q to point charge of +2Q, they become 0 and +Q respectively. At that time, there is no attraction between the 2 new pt charges as they are not of opposite charges. Also as they at point charges of no volume or surface, no induced charges on the neutral one.
Then, how could we said when 2 original pt charges make contact, each on then carry same charges before repulsion?
 
just after state of 0 and +Q for the two charges, further flow of charges make them same kind of charge (+charge), repulsion separates them. And no more flow of charge between them happens ><
 
It may be shown from the equations of electromagnetism, by James Clerk Maxwell in the 1860’s, that the speed of light in the vacuum of free space is related to electric permittivity (ϵ) and magnetic permeability (μ) by the equation: c=1/√( μ ϵ ) . This value is a constant for the vacuum of free space and is independent of the motion of the observer. It was this fact, in part, that led Albert Einstein to Special Relativity.
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