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- I want to write a student article specially for those who don't have a background in nuclear physics. I've been suggested to share my basic understanding & ask if they're correct.
I would be grateful if anyone could explain where my mistakes are:
(Please note that diagrams are designed just to give a simple imagination of the article & make it more understandable; they do NOT correspond precise information.)
The strong nuclear force is the strongest of the four basic forces in nature (the others are: the electromagnetic force, gravity, and the weak nuclear force). But it also has the shortest range, meaning that nucleons (protons & neutrons) must be extremely close (~1 fm) before its effects are felt.
The nuclear force can be explicated simply by analogy with the force between two small magnets: magnets are difficult to separate when stuck together, but once pulled a short distance apart, the force between them falls [almost] to zero.
This force between nucleons is done through the exchange of particles called mesons. As long as this meson exchange can happen, the strong force is able to hold the participating nucleons together.
https://www.physicsforums.com/attachments/2-jpg.248608/
For the lightest nuclei, the energy of the strong force per nucleon generally grows rapidly; because when a nucleon is added to such a small nucleus, the strong force attracts it to all the other constituent proton/s and neutron/s. I.e. the nucleus is sufficiently small that by adding each nucleon, all the others feel stronger effect.
But this trend approaches a limit corresponding to that of larger nuclei, because the nuclear force is short-range and cannot continue to act across longer nuclear length scales. (Generally, by this force a nucleon can only affect its close neighbors.)
Except for the lightest nuclei that all the nucleons are close to each other, for heavier elements the nucleons in the interior of a nucleus have more neighboring nucleons than those on the surface. So, according to the fact 'the larger a nucleus, the smaller its ratio of surface area to volume ', the energy of strong force per nucleon generally increases with the size of nucleus. (But it grows more and more slowly depending on the changes of the ratio.)
References:
http://aether.lbl.gov/elements/stellar/strong/strong.htmlhttps://en.wikipedia.org/wiki/Nuclear_binding_energy
The nuclear force can be explicated simply by analogy with the force between two small magnets: magnets are difficult to separate when stuck together, but once pulled a short distance apart, the force between them falls [almost] to zero.
This force between nucleons is done through the exchange of particles called mesons. As long as this meson exchange can happen, the strong force is able to hold the participating nucleons together.
https://www.physicsforums.com/attachments/2-jpg.248608/
For the lightest nuclei, the energy of the strong force per nucleon generally grows rapidly; because when a nucleon is added to such a small nucleus, the strong force attracts it to all the other constituent proton/s and neutron/s. I.e. the nucleus is sufficiently small that by adding each nucleon, all the others feel stronger effect.
But this trend approaches a limit corresponding to that of larger nuclei, because the nuclear force is short-range and cannot continue to act across longer nuclear length scales. (Generally, by this force a nucleon can only affect its close neighbors.)
Except for the lightest nuclei that all the nucleons are close to each other, for heavier elements the nucleons in the interior of a nucleus have more neighboring nucleons than those on the surface. So, according to the fact 'the larger a nucleus, the smaller its ratio of surface area to volume ', the energy of strong force per nucleon generally increases with the size of nucleus. (But it grows more and more slowly depending on the changes of the ratio.)
References:
http://aether.lbl.gov/elements/stellar/strong/strong.htmlhttps://en.wikipedia.org/wiki/Nuclear_binding_energy
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