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Physics 6A - UCSB C.L.A.S.
Physics 6A - UCSB C.L.A.S.

Phys 2102 Spring 2002 - LSU Physics & Astronomy
Phys 2102 Spring 2002 - LSU Physics & Astronomy

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38 Elementary Particle - Farmingdale State College

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Student choices of models of the atom - OSU Physics

... seems to fall into three groups. There are clearly reasonable descriptions (generally agreed to be plausible by the students, ranked 1, 2, or 3; descriptions a, f, g). a. An atom is made up of protons, neutrons, and electrons. The protons and neutrons make up the nucleus, which is in the center of t ...
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Solutions to Tutorial Problem Bab

... As a man takes a step, the action is the force his foot exerts on the Earth; the reaction is the force of the Earth on his foot. In the second case, the action is the force exerted on the girl’s back by the snowball; the reaction is the force exerted on the snowball by the girl’s back. The third act ...
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Saturation Physics Yuri Kovchegov The Ohio State University

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Chapter 6: Elementary Particle Physics and The Unification of The

... have also been performed on neutrons with the same success. The scattering also confirmed the existence of some quark-antiquark pairs within the proton. Recall that quark-antiquark pairs are the constituents of mesons. The experiments also showed the existence of other particles within the nucleons, ...
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This lecture deals with atomic and nuclear structure.

... went from one orbit to another was given by this equation. Sure enough, this equation really modeled spectroscopic observations. This equation did a pretty good job of quantitatively predicting how atoms gained or lost energy. That was a good sign as far as explaining atomic behavior. We are going t ...
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Chapter 6 – Work and Kinetic Energy

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CERN Teacher Programmes: Welcome to CERN!

... nuclear forces can be traced to the work of Heisenberg in 1932. Chadwick’s announcement of the discovery of the neutron in February of that year led to a flurry of speculation about the nature of the new particle. Heisenberg published three related academic papers in the second half of the year. He ...
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Review - Cobb Learning

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Lecture 9 - University of Manitoba Physics Department

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Review - prettygoodphysics

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Nuclear force



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 Coulomb repulsion that tends to push them apart, but at short range the nuclear force is sufficiently attractive as to overcome the electromagnetic repulsive 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 nuclei break apart, and it is this energy that used in nuclear power and nuclear weapons.The nuclear force is powerfully attractive between nucleons at distances of about 1 femtometer (fm, or 1.0 × 10−15 metres) between their centers, but rapidly decreases to insignificance at distances beyond about 2.5 fm. At distances less than 0.7 fm, the nuclear force becomes repulsive. This repulsive component is responsible for the physical size of nuclei, since the nucleons can come no closer than the force allows. By comparison, the size of an atom, measured in angstroms (Å, or 1.0 × 10−10 m), is five orders of magnitude larger. The nuclear force is not simple, however, since it depends on the nucleon spins, has a tensor component, and may depend on the relative momentum of the nucleons.A quantitative description of the nuclear force relies on partially empirical equations that model the internucleon potential energies, or potentials. (Generally, forces within a system of particles can be more simply modeled by describing the system's potential energy; the negative gradient of a potential is equal to the vector force.) The constants for the equations are phenomenological, that is, determined by fitting the equations to experimental data. The internucleon potentials attempt to describe the properties of nucleon–nucleon interaction. Once determined, any given potential can be used in, e.g., the Schrödinger equation to determine the quantum mechanical properties of the nucleon system.The discovery of the neutron in 1932 revealed that atomic nuclei were made of protons and neutrons, held together by an attractive force. By 1935 the nuclear force was conceived to be transmitted by particles called mesons. This theoretical development included a description of the Yukawa potential, an early example of a nuclear potential. Mesons, predicted by theory, were discovered experimentally in 1947. By the 1970s, the quark model had been developed, which showed that the mesons and nucleons were composed of quarks and gluons. By this new model, the nuclear force, resulting from the exchange of mesons between neighboring nucleons, is a residual effect of the strong force.
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