
The fundamental force that binds protons and neutrons together in the atomic nucleus.The nuclear force, also known as the strong nuclear force or residual strong force, is the fundamental interaction that binds protons and neutrons (nucleons) together in the atomic nucleus. It is a short-range force, acting over distances of about 1 femtometer (10^-15 meters), and it is responsible for the stability of atomic nuclei. Without it, the positively charged protons would repel each other and nuclei would fly apart.
The nuclear force was first proposed by Hideki Yukawa in 1935, who predicted the existence of the pion as the mediator of the force. The discovery of the pion in 1947 confirmed his theory, and the modern understanding of the strong force as a quark-gluon interaction was developed in the 1970s with quantum chromodynamics.
The nuclear force is a residual effect of the strong force that binds quarks together inside protons and neutrons. In the nucleus, nucleons exchange particles called mesons (such as pions), which mediate the force. This exchange creates an attractive force at short distances, but it becomes repulsive at extremely short ranges (less than 0.5 femtometers) due to the Pauli exclusion principle and the underlying quark interactions. The nuclear force is charge-independent, meaning it acts similarly between protons and neutrons, and it has a spin-dependent component.
The nuclear force is harnessed in nuclear power generation and nuclear weapons, where the binding energy released when nuclei split (fission) or merge (fusion) is converted into heat and electricity.
The nuclear force is about 100 times stronger than the electromagnetic force at short distances, but it acts only over a range of a few femtometers, which is why nuclei are so small and dense.




