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atom - cloudfront.net
atom - cloudfront.net

... •Scientists and engineers use models to represent things that are difficult to visualize— or picture in your mind. •Scaled-down models allow you to see either something too large to see all at once, or something that has not been built yet •Scaled-up models are often used to visualize things that ar ...
What are the four fundamental forces of nature?
What are the four fundamental forces of nature?

... atoms together at high speeds, they found the pions predicted by Yukawa. They also found that protons and neutrons were made of smaller particles called quarks. So, the strong force held the quarks together, which in turn held the nucleus together. One other nuclear phenomenon had to be explained: r ...
Section 15.3 Coulomb`s Law
Section 15.3 Coulomb`s Law

... An electron is released a short distance above the surface of the Earth. A second electron directly below it exerts an electrostatic force on the first electron just great enough to cancel the gravitational force on it. How far below the first electron is the second? ...
Calculating Work - Northern Illinois University
Calculating Work - Northern Illinois University

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Structure of Nuclear Matter

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A. Das and T. Ferbel - Ritter Illustration

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ppt - Cyclotron Institute

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PowerPoint Presentation - Chapter 15

... protons and 2 neutrons).  The nucleus remaining after the decay has 88 - 2 = 86 protons, 226 4 = 222 nucleons, and 222 - 86 = 136 neutrons.  This is the element radon-222. ...
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... 1.It is the only interaction capable of changing flavour. 2.It is the only interaction which violates parity symmetry P (because it almost exclusively acts on left-handed particles). ...
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Force, Net Force, and Inertia

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#NSLive Mysteries of matter: What the LHC will discover next

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... physicist Charles Augustin de Coulomb, who developed the equation. Every electrically charged particle is surrounded by a field of force. This field may be represented by lines of force showing the direction of the electrical forces that would be experienced by an imaginary positive test charge with ...
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The Structure of an Atom

... POSITIVELY charged particle located in the nucleus of an atom  Each element contains at least 1 proton  Each proton has a charge of +1  Rutherford discovered that the amount of positive charge varies among elements ...
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... Acts between all objects that have electric charge Can be either attractive or repulsive, depending on the charges on the objects Holds the atom together Coulomb’s law expresses the magnitude of the electrostatic force between two charged particles q1 q2 Fe = ke 2 where ke = 8.99 × 109N · m2/C 2 r ...
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DO NOW:

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1 Newton`s Laws

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the work is just the area under the curve

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Study Notes Lesson 23 Atomic and Nuclear Physics

... Criteria: particles are classified according to the types of interactions they have with other particles. If the force carrier particles (such as gluons, gravitons, etc.) are excluded, all particles can be classified into two groups – hadrons and leptons. Hadron – a particle that interacts through a ...
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Week 1: Nuclear timeline (pdf, 233 KB)
Week 1: Nuclear timeline (pdf, 233 KB)

... not only describe the other discoveries made by these scientists but also describe their personalities and other activities. They make for very interesting reading. They weren’t all boy scouts.! ...
TIMELINE OF NUCLEAR PHYSICS
TIMELINE OF NUCLEAR PHYSICS

< 1 ... 68 69 70 71 72 73 74 75 76 ... 82 >

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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