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Faraday's and disc
Such generators bear no resemblance to Faraday's homopolar disc generator of 1831, but they still rely on his electromagnetic principle that a conductor linking a changing magnetic field induces a potential difference across its ends.
Figure 1: Faraday's disc electric generator.
The experiment is described by some as a " paradox " as it seems, at first sight, to violate Faraday's law of electromagnetic induction, because the flux through the disc appears to be the same no matter what is rotating.
*" Electromagnetic induction: physics and flashbacks " ( PDF ) by Giuseppe Giuliani-details of the Lorentz force in Faraday's disc
-describes how to apply Faraday's law to Faraday's disc
-argues that only the Lorentz force can explain Faraday's disc and describes some experimental evidence for this

Faraday's and was
Faraday's and Ampère's work showed that a time-varying magnetic field acted as a source of an electric field, and a time-varying electric field was a source of a magnetic field.
Meanwhile, James Clerk Maxwell was working on Faraday's lines of force.
The relationship between electromotive force ( EMF ) or " voltage " and magnetic flux was formalized in an equation now referred to as " Faraday's law of induction ":
One of Michael Faraday's significant works was The Chemical History of a Candle, where he gives an in-depth analysis of the evolutionary development, workings and science of candles.
The value of F was first determined by weighing the amount of silver deposited in an electrochemical reaction in which a measured current was passed for a measured time, and using Faraday's law of electrolysis.
The physical principle behind production of mechanical force by the interactions of an electric current and a magnetic field, Faraday's law of induction, was discovered by Michael Faraday in 1831.
About a decade later Tyndall was appointed the successor to the positions held by Michael Faraday at the Royal Institution on Faraday's retirement.
He also investigated the diamagnetic and paramagnetic properties of substances ; and was keenly interested in the phenomena of electrochemical decomposition, accumulating much evidence in favor of Faraday's law of electrolysis and proposing a modified statement of it which was intended to cover certain apparent exceptions.
Harriet Jane Moore ( 1801 – 1884 ) was a British watercolour artist who is remembered for her drawings of Michael Faraday's work at the Royal Institution.
This 3rd London meeting house was that of Michael Faraday's youth.
An exception was Maxwell, who used Faraday's ideas as the basis of his quantitative electromagnetic theory.
The screenplay was adapted by John Kohn and Robert Bentley from Tony Kenrick's 1978 novel Faraday's Flowers.
Historically, the first time fields were taken seriously was with Faraday's lines of force when describing the electric field.
Michael Faraday's posthumous description of him was:
In the north of England it is likely that Baynes was a member of one of the Cumbrian branches but on his move to London he made his confession of faith and became a full member of the London congregation ( Paul's Alley in the Barbican ) in June 1792, some nine months after Michael Faraday's birth.
This was similar to the behavior of electric currents in an electric generator and showed that the cathode rays obeyed Faraday's law like currents in wires.
However the galvanometer did not deflect meaning there was no induced voltage, and Faraday's law does not work in this case.
At their hideout, Prankster and Victor find the information where Superman was temporarily blinded by Dr. Neal Faraday's ultra-violent light beam causing Prankster to find a way to strengthening the light ray in order to freeze Superman.

Faraday's and no
When time-varying magnetic fields are present ( which is true whenever there are time-varying electric fields and vice versa ), it is not possible to describe the electric field simply in terms of a scalar potential V because the electric field is no longer conservative: is path-dependent because ( Faraday's law of induction ).
This is a simplification of Faraday's law of induction for the special case where there is no fluctuating magnetic field linking the closed loop.
In this example, the circuit does not move, and the magnetic flux through the circuit is not changing, so Faraday's law suggests no current flows.
In the case when the disk alone spins there is no change in flux through the circuit, however, there is an electromotive force induced contrary to Faraday's law.

Faraday's and use
Faraday's law of induction makes use of the magnetic flux Φ < sub > B </ sub > through a hypothetical surface Σ whose boundary is a wire loop.
Eventually the conspirators use a field trip with a Scouts-style organization to keep Faraday's son Grant as an unknowing hostage.

Faraday's and practical
The two Maxwell equations, Faraday's Law and the Ampère-Maxwell Law, illustrate a very practical feature of the electromagnetic field.

Faraday's and generator
Faraday's disk ( see homopolar generator )

Faraday's and showed
File: Faraday. png | Michael Faraday ( 1791-1867 ): showed how a changing magnetic field can be used to generate an electric current ( Faraday's law of induction ), applied this knowledge to the development of several electrical machines, described principles of electrolysis, early pioneer in the field of low temperature study

Faraday's and generating
This is the most used form for generating electricity and is based on Faraday's law.

Faraday's and electric
Faraday's law states that the curl of an electric field is equal to the opposite of the time rate of change of the magnetic field, while Ampère's law relates the curl of the magnetic field to the current and rate of change of the electric field.
This relationship between magnetic fields and currents is extremely important, for it led to Michael Faraday's invention of the electric motor in 1821.
Faraday's Law may be stated roughly as ' a changing magnetic field creates an electric field '.
** Eddy currents: From Faraday's law of induction, the changing magnetic field can induce circulating loops of electric current in the conductive metal core.
) The other two equations describe how the fields ' circulate ' around their respective sources ; the magnetic field ' circulates ' around electric currents and time varying electric field in Ampère's law with Maxwell's correction, while the electric field ' circulates ' around time varying magnetic fields in Faraday's law.
Faraday's law describes how a time varying magnetic field creates (" induces ") an electric field.
If they did exist, both Gauss's law for magnetism and Faraday's law would need to be modified, and the resulting four equations would be fully symmetric under the interchange of electric and magnetic fields ; see magnetic monopoles for details.
Persistent electric current flows on the surface of the superconductor, acting to exclude the magnetic field of the magnet ( Faraday's law of induction ).
The gravitational force, spring force, magnetic force ( according to some definitions, see below ) and electric force ( at least in a time-independent magnetic field, see Faraday's law of induction for details ) are examples of conservative forces, while friction and air drag are classical examples of non-conservative forces.
B is the magnetic field whose time variation produces, by Faraday's Law, circulating electric fields ( which the power companies sell ).
A corollary of Faraday's Law, together with Ampère's law and Ohm's law is Lenz's law: The EMF induced in an electric circuit always acts in such a direction that the current it drives around the circuit opposes the change in magnetic flux which produces the EMF.
Electromotive force, also called EMF, ( denoted and measured in volts ), refers to voltage generated by a battery or by the magnetic force according to Faraday's Law, which states that a time varying magnetic field will induce an electric current.
This equation involves the electrostatic electric field due to charge separation E < sub > cs </ sub > and does not involve ( for example ) any non-conservative component of electric field due to Faraday's law of induction.

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