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Homework 7: Linear Dielectrics outside of the dielectric
Homework 7: Linear Dielectrics outside of the dielectric

... the displacement is a constant, the sum of the contributions cancels all displacement outside the capacitor and gives ⃗ ̂ inside the capacitor (pointing downward). Therefore, the displacement has the same value and direction in either dielectric. Using linear dielectric theory, the electric field in ...
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... force, which is directed toward the center of the circle. For a satellite in a circular orbit around the Earth, the centripetal force is gravity. • In uniform (constant speed) circular motion, the net force is the centripetal force. Thus, this net force is always perpendicular to the velocity. • Not ...
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... An electric current produces a magnetic field. • If you arrange magnetic compasses around a current-carrying wire, the compasses will align with the magnetic field around the wire. • A current-carrying coil of wire with many loops is an electromagnet. A piece of iron inside the coil increases the ma ...
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11. Some Applications of Electrostatics

... charges. The point form of Ohm's law does not hold. In rarefied gases the paths of accelerated ions between two successive collisions are relatively long, so that they can acquire a considerable kinetic energy. As a consequence, various new effects can be produced. The best known is probably a chain ...
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... Using the relationship between energy, frequency, and wavelength (i.e., E = hν = hc/λ), you can see that a FM radio station that broadcasts at a frequency of 100 MHz emits radio waves that are 3 m long and have an energy of 4.13 x 10-7 eV. An AM radio station broadcasting at 1000 kHz (i.e., 1 MHz) e ...
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... 49) Two charged particles attract each other with a force F. If the charges of both particles are doubled, and the distance between them also doubled, then the force of attraction will be A) F. B) 2 F. C) F/2. D) F/4. E) none of these 50) When a single charge q is placed on one corner of a square, ...
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Electric Potential and Capacitance

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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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