By Ubaid Hassan

2019-04-11 14:12:22 8 Comments

If the nucleus is densely positively charged, why don’t the protons in the nucleus repel from each other and move towards the orbiting electrons? Because each proton is not only being repelled by the other protons, it is also being pulled by the oppositely charged electrons

Why don’t these conditions make the atomic model impossible? I understand that electrons are in energy levels start so cannot force their way into the nucleus, but why not the reverse?


@KV18 2019-04-11 14:26:06

There is another fundamental force of nature apart from the electromagnetic and the gravitational force. This is the strong nuclear force. Its presence is in between the interactions of protons and neutrons themselves or between protons and neutrons.

Unfortunately, the strong force has no macroscopic effect as to feel the interaction themselves because the typical range where they are stronger than the electromagnetic interactions is at the range of femtometres ($10^{-15}\ \mathrm m$).

At such ranges, the strong force is stronger than the electromagnetic repulsion between the protons to hold them together.

As for your second question on the nucleus itself travelling to the electron, if you think in terms of the centre of mass, the nucleus has higher mass than the electron and so the centre of mass of the system would be closer to the nucleus than it is to the electron. But in this case, the centre of mass is probably within the nucleus itself which is why it is a feasible idea to say that the electron reveolves around the nucleus. Although it is correct to say that the electron revolves around the combined centre of mass of the system.

EDIT: There is something that I have to add on for completeness -

As @dmckee has pointed out in his comment, the strong nuclear force is not fundamental by itself (I apologise) but is instead the result of a fundamental strong nuclear interaction originating between the gluons and the quarks that constitute these protons and neutrons.

But essentially the strong nuclear force arises from this interaction. And hence the nucleus is stable from electromangetic repulsions due to the charge the protons carry.

@Hearth 2019-04-11 21:54:58

It's not really correct to say the electron revolves around anything, really. This is the point at which things get Quantum.

@dmckee 2019-04-12 01:08:58

The "strong nuclear force" is—arguably—not properly regarded as fundamental. The fundamental strong interaction binds quarks and gluons into hadrons. Long-lived hadrons (mostly the low mass baryons AKA the neutron and the proton) are then held into clusters by the "residual strong force" (AKA nuclear force or strong nuclear force). The nuclear force bears roughly the same relationship to the fundamental strong force that van~der~Waals inter-atomic forces do the electromagnetic binding of atoms: they are the relatively weak left-overs that results from imperfect cancellation.

@Kostas 2019-04-12 20:49:00

The attraction is operative on the neighboring nucleons only, while electostatic repulsion is long-distance. The repulsion force, in any case is not so much weaker than the attraction maybe at most by a factor of 10, even close by. So once you have about 100 protons, the repulsion starts to exceed the attraction. That is why we have the Mendeleev periodic table of the elements which ends at atomic number 118.

@guest 2019-04-11 22:40:07

In navy nuke school, the analogy for the strong nuclear force was Velcro. I.e. attraction but at "touching" distances only.

The strong nuclear force is sort of like a "glue" of neutrons that hold multiproton nuclei together. There are certain ratios of neutron to proton amount than seem to work best. See this chart: Note the rough 1:1 pattern but with a bit more "neutron glue" needed as you get to heavier elements.

There are also patterns of odd/even preferences and "magic numbers" (filled nuclear shells) which shows things are more complicated than just the "glue" idea, even if that holds as a first level insight. See and

Electrons do enter the nucleus (have some wave function in there). They can get captured in a decay process called electron capture, albeit rarely. See

I would also point out that free neutrons are unstable: So, you probably don't need to worry about some sort of "electron capture death of the universe" where everything ends up neutrons.

@Kostas 2019-04-11 14:26:38

The electrostatic repulsion force is long-distance, and the nuclear attraction is short-distance. So, protons do repel, and this is precisely what makes really large nuclei unstable.

Secondly, electrons in the S-wave orbital have nonzero wavefunction at the nucleus, so effectively they are able to penetrate into the nucleus, and that is what makes reverse-beta decay possible.

@J.G. 2019-04-11 21:40:35

+1 for pointing out large nuclei suffer the effect the OP conjectured.

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