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Unit 4 - CElliott
Unit 4 - CElliott

... So, a magnetic field can exert a force on a conductor, or moving charges. When a charged particle enters a magnetic field at an angle to the field lines, it experiences a force and the path of the particle curves. The magnitude of the magnetic force FM on a charged particle  Is directly proportiona ...
Conductors, Gauss`s Law
Conductors, Gauss`s Law

... • Note: if there was a tangential field outside—and of course none inside—you could accelerate an electron indefinitely on a circular path, half inside! ...
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Lecture 9 NMR 2

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Gravity Summary

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... Applying Kirchoff’s loop rule, the equation to solve is: dq q R  0 dt C  q  t   q0e t / RC Thus the elapsed time so that 10% of the charge remains is determined by: ...
TOPIC 4.2: ELECTRIC FIELDS
TOPIC 4.2: ELECTRIC FIELDS

Use the following to answer question 1. Two point charges
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... Given a long solenoid (R, n, I). Two insulating cylinders are coaxial with the solenoid: (λ, a) and (−λ, b). such that a < R < b (see figure). When the current in the solenoid is gradually reduced, the cylinders begin to rotate. where does the angular momentom come from? Tip: calculate the angular m ...
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SA1 REVISION WORKSHEET 2_0

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... /6/. An appropriate value of the effective charge number of ions has been introduced by other authors /7,8/ or image terms for the potential energy of tunneling electrons have been involved /9/. From the field evaporation data bonding distances and ...
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Benha University

... Consider a parallel plate capacitor with capacitance C = εoA/d. The potential across the capacitor is V = Ed. The electric energy stored in the capacitor is U = ½ CV2 = ½ (εoA/d)(E2d2) = ½ εo E2 Ad The electric energy density uE = U/volume = ½ εo E2. b) A current of 17 A is maintained in a single ci ...
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Gauss`s Law 3.1 Quiz

... points away from the center of the sphere. What changes in the application of Gauss’s law is the amount of charge enclosed by the Gaussian sphere: For a Gaussian sphere of radius r < R, we have Z r r4 4 π r̄2 (α r̄) dr̄ = 4 π ...
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CS110 Electric Field Meter Overview

... The electric field E is a vector quantity, having both a magnitude (field strength) and direction (direction of force exerted on a positive test charge). The units of electric field are Newtons/ Coulomb, which are equivalent to the more commonly expressed units of Volt/meter (V/m). The magnitude of ...
Elektrostatika: Hukum Coulomb
Elektrostatika: Hukum Coulomb



... field, E , and the field exerted by all other spheres in the system (which are polarized, and therefore produce a field). We now attempt to find the latter field. We focus on a single sphere, and draw a fictitious big sphere around it. That fictitious sphere is filled with other spheres, each one ex ...
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... Initially unpolarized light of intensity I0 is sent into a system of three polarizers as shown. What fraction of the initial intensity emerges from the system? What is the polarization of the exiting light? • Through the first polarizer: unpolarized to polarized, so I1=½I0. • Into the second polariz ...
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... It is also inversely proportional to the square of the distance between them (r2) Remember, the force is attractive if the charges have different signs and repulsive if the signs are the same. Force is a vector! The magnitude of the force can be written as: ...
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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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