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General Relativity: An Informal Primer 1 Introduction
General Relativity: An Informal Primer 1 Introduction

... General relativity, and its application to cosmological models such as inflation, is a remarkably beautiful and elegant theory. Yet newcomers to the field often face at least three types of challenges: conceptual, mathematical, and notational. Over the past century, physicists and mathematicians hav ...
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... Any charge given to a conductor resides on its outer surface, and charge density is greater at sharper regions on the surface. Any charge given to an insulator stays in place. Hence, a plastic object can have charge spread throughout its volume; this is not possible for a conducting object where the ...
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Asymmetric Electrostatic Force - Scientific Research Publishing
Asymmetric Electrostatic Force - Scientific Research Publishing

... asymmetric conductor was made by hand, the cylinder surface of the asymmetric conductor is not perfectly parallel to the direction of the electric field and the disk surface is not perfectly perpendicular to the direction of the electric field. Figure 6 shows the schematic layout of the improved exp ...
Electric field dependence of magnetic properties
Electric field dependence of magnetic properties

... In the first definition of hab,gd the electric dipole polarizability tensor aab is introduced. The second definition, taken from Eq. ~3! above, is directly related to the technique used in this work to compute hab,gd , in the sense that hab,gd is obtained by numerical differentiation of analytically ...
Effects of large horizontal winds on the equatorial electrojet
Effects of large horizontal winds on the equatorial electrojet

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this PDF file - American International Journal of

... introduce an impedance matrix [3–7](Wei Hu & Hong Guo, 2002; Danae, D. et al., 2002; Larruquert, J. I., 2001; Koludzija, B. M., 1999; Ehlers, R. A. & Metaxas, A. C., 2003). It is determined from experiments or, in some cases, theoretically from quantum representations [8–12](Barta, O.; Pistora, I.; ...
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Selected MC questions on electrostatics

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Chapter 20 Electric Forces and Fields

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Many-electron transport in strongly correlated nondegenerate two-dimensional electron systems *

... change the total momentum of the electron system, it may mediate the momentum transfer to the scatterers, and thus strongly affect the long-wavelength conductivity. It was suggested in Ref. 31 that, for quantizing magnetic fields \ v c @T and yet not too low temperatures, one may describe many-elect ...
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... ⬍ 0 and 2 ⬍ 兩Vb兩 / Gb ⬍ 1, these electronic properties are associated to a closed-shell interaction with a significant covalent character 共zone II兲. According to the natural bond orbital 共NBO兲 analysis,31 it is in zone II that the reorganization of the MOs giving rise to the bonding orbital between ...
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... charges, which do not move means, they are static. Electrostatic phenomena arise from the forces that electric charges exert on each other. Electroscope is device used to detect static charge. Electrostatic induction: It is a redistribution of electrical charge in an object, caused by the influence ...
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The Standard Model of Electroweak Interactions

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Parallel electric fields in the upward current region of the aurora

... Figure 2共b兲 plots the dc electric field perpendicular to B in the direction closest to the spacecraft velocity 共positive is mostly northward and nearly parallel to the satellite’s velocity兲. The large positive excursion at ⬃22:20:01 UT is followed by a large negative deflection at ⬃22:20:08 UT. This ...
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Electro Magnetic Fields

Chapter 30 Maxwell`s Equations and Electromagnetic Waves
Chapter 30 Maxwell`s Equations and Electromagnetic Waves

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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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