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However the term QFD is rarely used because the weak force is best understood in terms of electro- weak theory (EWT). The Standard Model of particle physics, which does not address gravity, provides a uniform framework for understanding how the electromagnetic, weak, and strong interactions work. An interaction occurs when two particles, typically but not necessarily half- integer spin fermions, exchange integer- spin, force- carrying bosons. The fermions involved in such exchanges can be either elementary (e. In the case of the weak interaction, fermions can exchange three distinct types of force carriers known as the W+, W- , and Z bosons. The mass of each of these bosons is far greater than the mass of a proton or neutron, which is consistent with the short range of the weak force. The force is in fact termed weak because its field strength over a given distance is typically several orders of magnitude less than that of the strong nuclear force or electromagnetic force. Due to their large mass (approximately 9. Ge. V/c. 2) these carrier particles, termed the W and Z bosons, are short- lived with a lifetime of under 1. The weak interaction has a coupling constant (an indicator of interaction strength) of between 1. The weak interaction has a very short range (around 1. At distances around 1. At distances of around 3? The nuclear force (or nucleon–nucleon interaction or residual strong force) is the force between protons and neutrons, subatomic particles that are collectively called nucleons. The nuclear force is responsible for binding protons and neutrons into atomic nuclei. Neutrons and protons are affected by the nuclear force almost identically. Since protons have charge +1 e, they experience a strong electric field repulsion (following Coulomb's law) that tends to push them apart, but at short range the attractive nuclear force overcomes the repulsive electromagnetic force. The mass of a nucleus is less than the sum total of the individual masses of the protons and neutrons which form it. The difference in mass between bound and unbound nucleons is known as the mass defect. Energy is released when some large nuclei break apart, and it is this energy that is used in nuclear power and nuclear weapons. At distances larger than 0. Beyond this distance the force drops exponentially, until beyond about 2. Nucleons have a radius of about 0. At short distances (less than 1. Coulomb force between protons; it thus overcomes the repulsion of protons within the nucleus. However, the Coulomb force between protons has a much greater range as it varies as the inverse square of the charge separation, and Coulomb repulsion thus becomes the only significant force between protons when their separation exceeds about 2 to 2.
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