Μαγνητική ροή: Διαφορά μεταξύ των αναθεωρήσεων

Περιεχόμενο που διαγράφηκε Περιεχόμενο που προστέθηκε
Χωρίς σύνοψη επεξεργασίας
Γραμμή 3:
 
==Description==
The [[flux]] through an element of [[area]] [[perpendicular]] to the direction of magnetic field is given by the product of the [[magnetic field density]] and the [[area]] element. More generally, magnetic flux is defined by a [[scalar product]] of the magnetic field density and the area element vector. Gauss's law for magnetism, which is one of the four [[Maxwell's equations]], states that the total magnetic flux through a closed surface is zero. This law is a consequence of the empirical observation that [[magnetic monopole]]s do not exist or are not measurable.
 
The magnetic flux is defined as the [[integral]] of the magnetic field over an area:
Γραμμή 11:
where
:<math>\Phi_m \ </math> is the magnetic flux
:'''B''' is the magnetic field density
:'''S''' is the area.
 
Γραμμή 35:
Note that this indicates the presence of electric monopoles, that is, free positive or negative charges.
 
The direction of the magnetic-flux-density field vector <math>\mathbf{B}</math> is by definition from the south to the north pole of a magnet (within the magnet). Outside of the magnet, the field lines will go from north to south.
 
A change of magnetic flux through a loop of conductive wire will cause an emf, and therefore an electric current, in the loop. The relationship is given by [[Faraday's law of induction|Faraday's law]]: