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PPT - LSU Physics & Astronomy
PPT - LSU Physics & Astronomy

... 30.6: Induced Electric Fields, Reformulation of Faraday’s Law: Consider a particle of charge q0 moving around the circular path. The work W done on it in one revolution by the induced electric field is W =Eq0, where E is the induced emf. From another point of view, the work is Here where q0E is the ...
Electric Currents, Magnetic Forces
Electric Currents, Magnetic Forces

lecture1423813661
lecture1423813661

... Fields are classified as • Scalar field • Vector field. Electric charge is a fundamental property of matter. Charge exist only in positive or negative integral multiple of electronic charge, e= 1.60 × 10-19 coulombs. [It may be noted here that in 1962, Murray Gell-Mann hypothesized Quarks as the ba ...
Maxwell`s equations
Maxwell`s equations

Reference Frames and Relative Motion Uniform Circular Motion
Reference Frames and Relative Motion Uniform Circular Motion

... Magnetic Field lines: (defined in same way as electric field lines, direction and density) ...
Ch01 - lmn.pub.ro
Ch01 - lmn.pub.ro

... juxtaposition,  =  1 –  2 (fig. 2.9). This experimental fact results in the conclusion that there are two opposite types of electrification, which might eventually compensate each other. By convention, the electrification of a glass rod rubbed with a piece of fur was taken as positive, while th ...
Ch20_Magnetism_ANS
Ch20_Magnetism_ANS

... The work done by the magnetic field on the particle is.. A) positive B) negative C) Zero. Answer: The (+) particle will feel a force FE = qE due to the E-field along the direction of the Efield. As it starts moving along the E-field direction, it will acquire a velocity, and it will start to feel a ...
Positron collisions with Rydberg atoms in strong
Positron collisions with Rydberg atoms in strong

Magnetism
Magnetism

Document
Document

... Electric Potential increases as you approach positive source charges and decreases as you approach negative source charges (source charges are the charges generating the electric field) A line where Delta V= 0 V is an equipotential line (The electric force does zero work on a test charge that moves ...
Eddy currents
Eddy currents

Lecture 1 Assignment 1.1 Binomial expansion
Lecture 1 Assignment 1.1 Binomial expansion

... In the Star Trek series a so-called Transporter is used to “beam” people and their equipment from a starship to the surface of nearby planets and back. The Transporter mechanism is not explained, but it appears to work only locally. (If it could transport to remote locations, why bother with the sta ...
Powerpoint
Powerpoint

19-1 The Magnetic Field
19-1 The Magnetic Field

Chapter 20 Magnetism
Chapter 20 Magnetism

Electric Potential
Electric Potential

Lecture Notes
Lecture Notes

... design of amplifier klystrons. The intent is to provide the student or engineer with the assumptions used in their derivations so that he or she can use them correctly. These assumptions result in the approximations necessary to derive analytical expressions for the gain and bandwidth of klystrons a ...
Part 1
Part 1

... perpendicular to a uniform 0.600 T magnetic field. It is quickly pulled from the field at constant speed to a region where B drops abruptly to zero. At t=0, the right edge of the coil is at the edge of the field. It takes 0.100 s for the whole coil to reach the field-free region. The coil’s total re ...
Mastering Physics Solutions to Week 10 11 Assignment
Mastering Physics Solutions to Week 10 11 Assignment

2.5 DEFFECTS IN CRYSTALS1
2.5 DEFFECTS IN CRYSTALS1

... is independent of pO2. At low pressures the curves coincide with those of the ‘pure’ ceramic.  At the lowest pO2 values (AB) loss of oxygen from the crystal is accompanied by the formation of Vö and electrons according to equations (2.48) and (2.50). ...
Document
Document

fundamental_reality\symmetry
fundamental_reality\symmetry

... V > V+C is also a solution to Maxwell's equations and no experiment can distinguish between these two solutions. In other words the laws of physics governing electricity and magnetism (that is, Maxwell equations) are invariant under gauge transformation.[5] That is, Maxwell's equations have a gauge ...
On the spatial structure of electric fields generated by clouds with
On the spatial structure of electric fields generated by clouds with

... sailplanes have been used in recent years (Breed and Dye [1989], Mo et al. [2003]; Dye et al. [2007]), but still at great cost. Large UAV’s have been used to study the contribution of thunderstorm currents to the global circuit [Mach et al., 2009], but they have not been used for the study of develo ...
A Brief History of Electromagnetism
A Brief History of Electromagnetism

Electrostatic Force and Electric Charge
Electrostatic Force and Electric Charge

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Electrostatics



Electrostatics is a branch of physics that deals with the phenomena and properties of stationary or slow-moving electric charges with no acceleration.Since classical physics, it has been known that some materials such as amber attract lightweight particles after rubbing. The Greek word for amber, ήλεκτρον electron, was the source of the word 'electricity'. Electrostatic phenomena arise from the forces that electric charges exert on each other. Such forces are described by Coulomb's law.Even though electrostatically induced forces seem to be rather weak, the electrostatic force between e.g. an electron and a proton, that together make up a hydrogen atom, is about 36 orders of magnitude stronger than the gravitational force acting between them.There are many examples of electrostatic phenomena, from those as simple as the attraction of the plastic wrap to your hand after you remove it from a package, and the attraction of paper to a charged scale, to the apparently spontaneous explosion of grain silos, the damage of electronic components during manufacturing, and the operation of photocopiers. Electrostatics involves the buildup of charge on the surface of objects due to contact with other surfaces. Although charge exchange happens whenever any two surfaces contact and separate, the effects of charge exchange are usually only noticed when at least one of the surfaces has a high resistance to electrical flow. This is because the charges that transfer to or from the highly resistive surface are more or less trapped there for a long enough time for their effects to be observed. These charges then remain on the object until they either bleed off to ground or are quickly neutralized by a discharge: e.g., the familiar phenomenon of a static 'shock' is caused by the neutralization of charge built up in the body from contact with insulated surfaces.
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