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word document - FacStaff Home Page for CBU
word document - FacStaff Home Page for CBU

... Since  · (  A) = 0 (for any vector, A), and since  · B = 0, we can define a vector potential, A, where B =   A . In general, A = (∫ (j /r) dV. From Faraday’s Law:   E = -B/t = -[  A] /t , or E = -A/t Putting this all together: E = -Φ - A/t ...
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... Assignment (02) Introduction to Electric Charges and Electric Field (2) Text book, chapter 21, electric chargers and electric field Problems, page 585/586 [4] What is the repulsive electrical force between two protons 4.0 X 10-15m apart from each other in an atomic nucleus? [7] Two charged spheres a ...
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... cm wide, in a uniform magnetic field with magnetic field with magnitude 0.40 T. When you run a 75-A current in the +x direction, you find by careful measurement that the potential at the left side of the slab is 0.81V higher than at the right side of the slab. From this measurement, determine the c ...
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... accordance with the fact that this field is virtual. In future we shall assume that the current j and the potentials A and B have only azimuthal components with respect to a certain symmetry axis and do not themselves depend on the azimuth. Thus, the law of conservation of charge and the Lorentz con ...
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... charged particle enters a region. This conception should change after working with the models in the activity (but it may not). URL: http://www.google.com/search?q=Misconceptions+electric+field&ie=utf-8&oe=utf8&aq=t&rls=org.mozilla:en-US:official&client=firefox-a A simple explanation of magnetic fi ...
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... 2. An electron’s mass is 1840 times smaller that one of a proton, so it’s velocity would be that much bigger, so the magnetic force will be bigger and the electron will deviate in ẑ direction. Because of the opposite charge of the electron, the electric field will act in −ẑ direction, so the magne ...
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... (b) Further, verify that the magnetic field is the curl of the vector potential and can be expressed in the form Z µ0 r − r′ B(r) = ∇ × A(r) = d3 r ′ J(r′ ) × ...
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Field (physics)



In physics, a field is a physical quantity that has a value for each point in space and time. For example, on a weather map, the surface wind velocity is described by assigning a vector to each point on a map. Each vector represents the speed and direction of the movement of air at that point. As another example, an electric field can be thought of as a ""condition in space"" emanating from an electric charge and extending throughout the whole of space. When a test electric charge is placed in this electric field, the particle accelerates due to a force. Physicists have found the notion of a field to be of such practical utility for the analysis of forces that they have come to think of a force as due to a field.In the modern framework of the quantum theory of fields, even without referring to a test particle, a field occupies space, contains energy, and its presence eliminates a true vacuum. This lead physicists to consider electromagnetic fields to be a physical entity, making the field concept a supporting paradigm of the edifice of modern physics. ""The fact that the electromagnetic field can possess momentum and energy makes it very real... a particle makes a field, and a field acts on another particle, and the field has such familiar properties as energy content and momentum, just as particles can have"". In practice, the strength of most fields has been found to diminish with distance to the point of being undetectable. For instance the strength of many relevant classical fields, such as the gravitational field in Newton's theory of gravity or the electrostatic field in classical electromagnetism, is inversely proportional to the square of the distance from the source (i.e. they follow the Gauss's law). One consequence is that the Earth's gravitational field quickly becomes undetectable on cosmic scales.A field can be classified as a scalar field, a vector field, a spinor field or a tensor field according to whether the represented physical quantity is a scalar, a vector, a spinor or a tensor, respectively. A field has a unique tensorial character in every point where it is defined: i.e. a field cannot be a scalar field somewhere and a vector field somewhere else. For example, the Newtonian gravitational field is a vector field: specifying its value at a point in spacetime requires three numbers, the components of the gravitational field vector at that point. Moreover, within each category (scalar, vector, tensor), a field can be either a classical field or a quantum field, depending on whether it is characterized by numbers or quantum operators respectively. In fact in this theory an equivalent representation of field is a field particle, namely a boson.
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