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F 502 – Eletromagnetismo I – Problemas adicionais
F 502 – Eletromagnetismo I – Problemas adicionais

... P 13.21, Zangwill. In 1935, the brothers Fritz and Heinz London described superconductivity using a phenomenological constitutive equation where a length δ > 0 relates the current density to the Coulomb vector potential: J=− ...
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... interesting, especially in the vicinity of the plasma neutral sheet [8]. In nonlinear mode the Buneman instability can be the starting mechanism for the onset of ion-acoustic instability [9]. The Buneman instability has many modifications (e.g., two symmetric opposite beams, beam-target instability, ...
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... separation between like charges. Therefore, excess charge resides on the outside surface of a conductor. Further, the static electric field near the surface of the conductor must be everywhere perpendicular to the surface, else a tangential component of the field would cause the free charges to move ...
Towards Understanding the Internal Symmetries of Nature: Gauge
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... A. Scalars, Vectors, Tensors and Matrices/Determinants: In a physics description of distance-time nature, we are accustomed to dealing with both extrinsic thermodynamic variables that govern the overall behavior of outer nature and the intrinsic properties of materials from a distancetime perspectiv ...
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On ion flow caused by the inductive electric field in a tokamak

... these quantities to linear combinations of radial density and temperature gradients and 共for ␻ a ) the radial electric field. In a recent paper,4 however, it was pointed out that the inductive electric field used to drive Ohmic current also contributes significantly to u a ␪ for bulk ions (a⫽i) in a ...
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... circles around an axis of symmetry, confines a plasma hardly better than no field at all. This can be understood by looking at the orbits of individual particles. The particles not only spiral around the field lines, they also drift across the field. Since a toroidal field is curved and decreases in ...
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... The magnetic field lines and pattern of iron filings in the vicinity of a bar magnet and the magnetic field lines in the gap of a horseshoe magnet. ...
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unit 102-1: electric forces and fields

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References - DSpace@MIT - Massachusetts Institute of Technology

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Dirac monopoles and gravitation

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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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