Everything about Strong Nuclear Force totally explained
In particle physics, the
strong interaction, or
strong force, or
color force, holds
quarks and
gluons together to form protons and neutrons.
» For an understanding of the interaction that holds protons and neutrons together to form atomic nuclei, see
nuclear force.
The term 'strong interaction' is also used to describe
food webs.
The strong interaction is one of the four fundamental interactions, along with
gravitation, the
electromagnetic force and the
weak interaction.
Of the four fundamental forces, the strong interaction is the most powerful.
The strong force is thought to be mediated by
gluons, acting upon
quarks,
antiquarks, and the
gluons themselves. This is detailed in the theory of
quantum chromodynamics (QCD).
History
Before the
1970s,
protons and
neutrons were thought to be indivisible
fundamental particles.
It was known that:
» 1. Protons carried a positive electrical charge,
2.
electric repulsion made same-charge particles
repel each other, and
» 3.
Multiple protons were bound together in the
atomic nucleus.
So, what held protons together in the nucleus?
Another, stronger,
attractive force was postulated to explain how protons were held together in the atomic nucleus, overcoming electromagnetic repulsion.
For its high strength (at short distances), it was dubbed the "strong force".
It was thought, at that time, this strong force was a fundamental force acting directly on the protons.
It was later discovered this phenomena was only a
residual side-effect of another, truly fundamental, force acting directly on particles
inside protons called quarks and gluons.
This newly-discovered force was initially called the "color force." This has no relation to visible color.
Today, the term "strong force" is used for that strong nuclear force that acts directly on quarks and gluons.
The
original strong force that acts on protons is today called the
nuclear force or
residual strong nuclear force.
Details
The strong force is postulated in
Quantum chromodynamics, QCD.
QCD is a part of the
standard model of particle physics.
Mathematically, QCD is a
non-Abelian gauge theory based on a local (gauge)
symmetry group called
SU(3).
All particles in QCD interact with each other through the strong force.
The strength of interaction is parametrized by the strong
coupling constant.
This strength is modified by the gauge
color charge of the particle. This refers to a
group theoretical property explained in the article on
color charge.
Quarks and gluons are the
only fundamental particles which carry non-vanishing color charge, and hence participate in strong interactions.
The strong force itself acts
directly upon only elementary quark and gluon particles.
A residual effect of the strong force is called the
nuclear force.
The nuclear force acts between
hadrons, such as
nucleons in atomic nuclei.
The strong force, acting indirectly, transmits gluons that form part of the virtual pi and rho
mesons, which, in turn, transmit the nuclear force between nucleons.
The strong force, unlike other forces, does
not diminish in strength with increasing distance. As a result, quarks are always permanently bound together into hadrons. It is impossible to separate individual quarks as can be done with protons. In QCD, this phenomenon is called
confinement. So only hadrons can be observed. This has been shown by many failed
free quark searches. The elementary quark and gluon particles affected are unobservable directly.
Further Information
Get more info on 'Strong Nuclear Force'.
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