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In particle physics, the strong interaction is the mechanism responsible for the strong nuclear force also called the strong force or nuclear strong forceand is one of the four known fundamental interactions, with the others being electromagnetism, the weak interaction and gravitation. At the range of 10? The strong nuclear force holds most ordinary matter together because it confines quarks into hadron particles such as proton and neutron. In addition, the strong force binds neutrons and protons to create atomic nuclei. The strong interaction is observable at two ranges: on a larger scale about denon tu 260l drawings mk2 production to 3 femtometers fmit is the force that binds protons and neutrons nucleons together to form the nucleus of an atom. On the smaller scale less than about 0. In the latter context, it is often known as the color force. The strong force inherently has such a high strength that hadrons bound by the strong force can produce new massive denon tu 260l drawings mk2 production. Thus, if hadrons are struck by high-energy particles, they give rise to new hadrons instead of emitting freely moving radiation gluons. This property of the strong force is called color confinement, and it prevents the free "emission" of the strong force: instead, in practice, jets of massive particles are produced. The strong force is described by quantum chromodynamics QCDa 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. Quarks and gluons are the only fundamental particles that carry non-vanishing color charge, and hence they participate in strong interactions only with each other. The strong force is the expression of the gluon interaction with other quark and gluon particles. All quarks and gluons 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, a group theoretical property. Nuclear binding energy is the energy that would be required to disassemble the nucleus of an atom into its component parts.



Strong interaction
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