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VectorCalcTheorems
VectorCalcTheorems

... This is the differential form of Gauss’ Law. It holds for every point in space. When combined with further differential laws of electromagnetism (see next section), we can derive a differential equation for electromagnetic waves. For example, consider a constant electric field: E  E0 xˆ . It is eas ...
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The Biot-Savart Law and Ampere`s Law

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... A radial electric field surrounds a point charge. Point charges q and Q at separation r in a vacuum exert equal and opposite forces on each other given by Coulomb's law Qq F 4 0 r 2 where 0 is the permittivity of free space. The electric field F/q at a distance r from a point charge Q is Q E 4 ...
Capacitors - Honors Physics Website (Blue 5)
Capacitors - Honors Physics Website (Blue 5)

...  It is now used in computers, radios, televisions, and camera flashes. ...
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... E = kq/r2 and is parallel to dA everywhere on the surface F = ∫ E·dA = E ∫dA = EA For q = +3.0nC, flux through sphere of radius r=.20 m? ...
Calculating and displaying the electric field of a dipole
Calculating and displaying the electric field of a dipole

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Physics 221 Second Hourly Examination Prepared August 2006

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1. Look at the drawing given in the figure which has been drawn

... Scientists are working hard to develop nuclear fusion reactor. Nuclei of heavy hydrogen, known as deuteron and denoted by D can be thought of as a candidate for fusion reactor. The D-D reaction is 2H1 + 2H1 --> 3H2 + n + energy. In the core of fusion reactor, a gas fo heavy hydrogen is fully ionized ...
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... For many people this term implies an electric field free area, that translates to absolute shielding. Protective bags and tote boxes can only behave as a 'Faraday Cage' for a static field (stationary in time). Faraday showed by his ice pail experiment that electric charges placed on the inside surfa ...
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... held in a fixed position. At an instant when the distance between the two particles is 2.0 m, the kinetic energy of the moving particle is 16 J. Determine the distance separating the two particles when the moving particle is momentarily stopped. a. 0.75 m b. 0.84 m c. 0.95 m d. 0.68 m e. 0.56 m ____ ...
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Chapter 23: Electric Potential

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1. What happens when electrical charges are brought together? A

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Equipotential Lines - Tenafly Public Schools

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... used to describe how materials respond on the microscopic level to an applied magnetic field; to categorize the magnetic phase of a material. For example, the most well known form of magnetism is ferromagnetism such that some ferromagnetic materials produce their own persistent magnetic field. Howev ...
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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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