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Chapter 4 Experiment 2: Equipotentials and Electric Fields
Chapter 4 Experiment 2: Equipotentials and Electric Fields

... the electric field is regarded as having a real physical existence, rather than being a mere mathematically-defined quantity. For example when a collection of charges in one region of space move, the effect on a test charge at a distant point is not felt instantaneously, but instead is detected with ...
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... 9. Using Gauss law establish that the magnitude of electric field intensity, at a point, due to an infinite plane sheet, with uniform charge density σ is independent of the distance of the field point OR Define an electric field line. Draw the pattern of the field lines around a system of two equal ...
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The Third Electromagnetic Constant of an Isotropic Medium

... Notice that the coefficient in the first term is fixed to be the same as the coefficient in Eq. (3.1) by current conservation. Thus, in general, we have three dimensionless constants describing the electromagnetic properties of an isotropic medium: ǫ, µ and ζ. Looking back at Eq. (3.2), it now becom ...
Lecture 7
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... 51. A nonconducting spherical shell of inner radius a = 2 cm and outer radius b = 2.4 cm has a positive volume charge density  = A/r, where A is a constant and r is the distance from the center of the shell. In addition, a small ball of charge q = 45 fC is located at that center. What value should ...
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... Classical Mechanics is indeed a causal theory based on elementary physical objects satisfying Newton’s laws of motion. The exceptional success of this theory together with new technologies like photography had propagated a new view point on science during the last part of the nineteenth century with ...
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... field. This model may be applied to investigate the behaviour of the magnetic field generated by the magnetopause currents. In this picture, the Earth’s magnetic dipole is situated at the origin (Earth centre) and the dipole axis is orthogonal to the upstream solar wind direction. The magnetopause i ...
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... The magnitude FB of the magnetic force exerted on the particle is proportional to the charge, q, and to the speed, v, of the particle When a charged particle moves parallel to the magnetic field vector, the magnetic force acting on the particle is zero When the particle’s velocity vector makes any a ...
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... exerted on the particle is proportional to the charge, q, and to the speed, v, of the particle When a charged particle moves parallel to the magnetic field vector, the magnetic force acting on the particle is zero When the particle’s velocity vector makes any angle q 0 with the field, the force ac ...
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تکلیف سری اول درس آنتن1 موعد تحویل : 3/12/84
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... ? What is the axial ratio in this case? 3- A dipole antenna, with a total loss resistance of 1Ω, is connected to a generator whose internal impedance is 50Ω+j25Ω. Assume that the peak voltage of the generator is 2V and the input impedance of the dipole, excluding the loss resistance, is 73Ω+j42.5Ω. ...
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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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