The Strong Nuclear Force (also referred to as the strong force) is one of the four basic forces in nature (the others being gravity, the electromagnetic force, and the weak nuclear force). As its name implies, it is the strongest of the four. However, it also has the shortest range, meaning that particles must be extremely close before its effects are felt. Its main job is to hold together the subatomic particles of the nucleus (protons, which carry a positive charge, and neutrons, which carry no charge. These particles are collectively called nucleons). As most people learn in their science education, like charges repel (+ +, or - -), and unlike charges attract (+ -).
If you consider that the nucleus of all atoms except hydrogen contain more than one proton, and each proton carries a positive charge, then why would the nuclei of these atoms stay together? The protons must feel a repulsive force from the other neighboring protons. This is where the strong nuclear force comes in. The strong nuclear force is created between nucleons by the exchange of particles called mesons. This exchange can be likened to constantly hitting a ping-pong ball or a tennis ball back and forth between two people. As long as this meson exchange can happen, the strong force is able to hold the participating nucleons together. The nucleons must be extremely close together in order for this exchange to happen. The distance required is about the diameter of a proton or a neutron. If a proton or neutron can get closer than this distance to another nucleon, the exchange of mesons can occur, and the particles will stick to each other. If they can't get that close, the strong force is too weak to make them stick together, and other competing forces (usually the electromagnetic force) can influence the particles to move apart. This is represented in the following graphic. The dotted line surrounding the nucleon being approached represents any electrostatic repulsion that might be present due to the charges of the nucleons/particles that are involved. A particle must be able to cross this barrier in order for the strong force to "glue" the particles together.
In the case of approaching protons/nuclei, the closer they get, the more they feel the repulsion from the other proton/nucleus (the electromagnetic force). As a result, in order to get two protons/nuclei close enough to begin exchanging mesons, they must be moving extremely fast (which means the temperature must be really high), and/or they must be under immense pressure so that they are forced to get close enough to allow the exchange of meson to create the strong force. Now, back to the nucleus. One thing that helps reduce the repulsion between protons within a nucleus is the presence of any neutrons. Since they have no charge they don't add to the repulsion already present, and they help separate the protons from each other so they don't feel as strong a repulsive force from any other nearby protons. Also, the neutrons are a source of more strong force for the nucleus since they participate in the meson exchange. These factors, coupled with the tight packing of protons in the nucleus so that they can exchange mesons creates enough strong force to overcome their mutual repulsion and force the nucleons to stay bound together. The preceding explanation shows the reason why it is easier to bombard a nucleus with neutrons than with protons. Since the neutrons have no charge, as they approach a positively charged nucleus they will not feel any repulsion. They therefore can easily "break" the electrostatic repulsion barrier to being exchanging mesons with the nucleus, thus becoming incorporated into it.
A meson is comprised of one quark and one antiquark. Another way to comment on the composition of the meson might be that it contains a quark-antiquark pair. A link can be found below for more information.
The B meson has a number of decay modes, called channels. The term "golden channel" is applied to the first one, and in that channel (decay chain or decay event), the B meson transforms into two other mesons, a J/psi meson and a K short, or KS meson, a kaon.
The lifetime of a Charmed B meson, also known as a B^0 meson, is approximately 1.5 picoseconds before it decays into other particles. This decay process typically involves the weak force and leads to the production of lighter particles such as kaons and pions.
The meson was discovered in 1935 by Japanese physicist Hideki Yukawa. His discovery helped to explain the strong nuclear force and laid the foundation for the theory of nuclear interactions.
A pi meson, also known as a pion, is a type of subatomic particle called a meson. Pions are the lightest mesons and come in three forms: positive, negative, and neutral. They play a role in the strong nuclear force that binds protons and neutrons together in atomic nuclei.
meson exchange between protons & neutrons.
Anne Meson was born in 1975.
Meson Ray was created on 1999-04-20.
El Meson Sandwiches was created in 1972.
A meson is comprised of one quark and one antiquark. Another way to comment on the composition of the meson might be that it contains a quark-antiquark pair. A link can be found below for more information.
The B meson has a number of decay modes, called channels. The term "golden channel" is applied to the first one, and in that channel (decay chain or decay event), the B meson transforms into two other mesons, a J/psi meson and a K short, or KS meson, a kaon.
there is no difference b/w meson theory an yukawa theory of nuclear forces because yukawa predicted the nuclear forces as exchange of boson(messons) b/w neutron and proton which keep them bind in an atomic nuclei. so meson theory is just another name of yukawa's theory of nuclear forces.
A Meson is a subatomic particle that comprises of 1 quark and 1 anti-quark.
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meson
They're two ways of expressing the same idea. A "color singlet" meson is a meson consisting of a red-antired, green-antigreen, or blue-antiblue quark-antiquark pair. Since X-antiX cancels out, this is essentially the same thing as saying that the meson has no net overall color charge ... that is, it's colorless.
Hideki Yukawa proposed the first theory of the strong force via meson exchange particles.