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Relativity and Gravitation
Relativity and Gravitation

... + qh > 0 for all r > 2m and q > 0, E and C can be real and finite only if r - 3m + 2qh > 0 (52s) and m — qh > 0. (53s) We note that for q = 0 we get r > 3m, which is precisely the condition obtained for the existence of circular motion in the Schwarzschild field11. For q < 1, Eqs. (52s) and (38) gi ...
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Preclass video slides - University of Toronto Physics

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Magnetic Fields

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Functional-Integral Representation of Quantum Field Theory {functint

... in Section 14.7, Eqs. (14.123)–(14.133), that correct finite partition functions are obtained if the infinities are removed by the method of dimensional regularization, that was used in Section 11.5 to remove divergences from Feynman integrals. Even though the operator formula (14.57) and the functi ...
Ch#28 - KFUPM Faculty List
Ch#28 - KFUPM Faculty List

... T-002:Q#1: An electron is projected into a uniform magnetic field B = (0.8 k) T. Find the magnitude of the magnetic force, on the electron when the velocity is: v = (5.0*10**5 i + 3.0*10**5 j) m/sec. (i, j and k are the unit vectors in the x, y and z directions, respectively). (Ans:7.5*10**(-14) N.) ...
PowerPoint Presentation - Slide 1 - plutonium
PowerPoint Presentation - Slide 1 - plutonium

... The direction of the induced current is given by Lenz’s law: The induced current is in a direction such that the magnetic field it creates tends to oppose the change that created it If it were in the other direction, energy would not be conserved A current produced by an induced emf moves in a direc ...
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3.4 Electromagnetism

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Q1. As shown In Figure 1 four particles form a square of side length

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Electric Forces and Electric Fields

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Charging - University of Hawaii Physics and Astronomy
Charging - University of Hawaii Physics and Astronomy

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... , where λ is a constant (called the screening length). a) Determine the E-field E(r) associated with this potential. b) Find the charge distribution ρ(r) that produces this potential. (Think carefully about what happens at the origin!) - Sketch this function ρ(r) in a manner the clearly describes it ...
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PHY 220 GENERAL PHYSICS II / 3 credits. Study of electricity

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PHY 220 GENERAL PHYSICS II / 3 credits
PHY 220 GENERAL PHYSICS II / 3 credits

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Simulation of Electromagnetic Leakage from a Microwave Oven

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Chapter 6. Magnetostatic Fields in Matter

... electron would have been orbiting the other way, it would have been slowed down by the magnetic field. Again the change in the dipole moment is opposite to the direction of B . In the presence of an external magnetic field the dipole moment of each orbit will be slightly modified, and all these cha ...
Parallel Electric Field of a Mirror Kinetic Alfvén Wave
Parallel Electric Field of a Mirror Kinetic Alfvén Wave

... There are two types of so called “kinetic Alfvén wave” depending on the electron thermal speed. When the electron thermal speed is much higher than the Alfvén speed, what causes the parallel electric field is the electron pressure, [Hasegawa, 1976], and in the opposite case (electron thermal speed ...
Halliday Resnick Walker Physics Vol II
Halliday Resnick Walker Physics Vol II

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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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