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Contents
Contents

5 Discrete Symmetries
5 Discrete Symmetries

Electric potential differences across auroral generator interfaces
Electric potential differences across auroral generator interfaces

File S1.
File S1.

4. Concurrent 43 and 86 GHz VLBA Polarimetry Observations of the
4. Concurrent 43 and 86 GHz VLBA Polarimetry Observations of the

... Summary of New Results ...
Chapter 31
Chapter 31

... Under the influence of the force, the electrons move to the lower end of the conductor and accumulate there. As a result of the charge separation, an electric field is produced inside the conductor. The charges accumulate at both ends of the conductor until they are in equilibrium with regard to the ...
Capacitors
Capacitors

Ch 25 Lecture
Ch 25 Lecture

... These particular two types of rods are different materials, charged in a somewhat different way, and they attract each other rather than repel. © 2013 Pearson Education, Inc. ...
The Electric Organ Discharges of the Gymnotiform Fishes
The Electric Organ Discharges of the Gymnotiform Fishes

07_chapter 1
07_chapter 1

Waveguide coupling by apertures: (from Collin)
Waveguide coupling by apertures: (from Collin)

Deflection of Electrons by Electric and Magnetic Fields
Deflection of Electrons by Electric and Magnetic Fields

E1 ELECTRIC FIELDS AND CHARGE
E1 ELECTRIC FIELDS AND CHARGE



Parallel Electric Field of a Mirror Kinetic Alfvén Wave
Parallel Electric Field of a Mirror Kinetic Alfvén Wave

Electromagnetic force and torque in Lorentz and Einstein
Electromagnetic force and torque in Lorentz and Einstein

... It has been suggested that magnetic dipoles cannot exist in classical physics. A famous argument in support of this assertion is given in Niels Bohr’s PhD dissertation (1911).1 The argument is now known as the Bohr-van Leeuwen theorem. Feynman also mentions this point briefly in his Lectures on Phys ...
Polarizability of a dielectric hemisphere
Polarizability of a dielectric hemisphere

PREPARING FOR THE AP PHYSICS EXAM
PREPARING FOR THE AP PHYSICS EXAM

Section 3
Section 3

Book 4 in the Light and Matter series of free - IA
Book 4 in the Light and Matter series of free - IA

10-Tutorial Packet
10-Tutorial Packet

... That which feels the force of a gravitational field (namely mass) is also what causes the gravitational field to exist. Electric charge plays the same dual role for electric field; it both feels the force of an existing electric field and causes electric fields to exist. The same is true of the magn ...
The phenolic glass: a new material for the RPC electrodes
The phenolic glass: a new material for the RPC electrodes

Magnetic field lines
Magnetic field lines

physics - Regents
physics - Regents

MAGNETISM
MAGNETISM

< 1 ... 59 60 61 62 63 64 65 66 67 ... 479 >

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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