Jump to content
Main menu
Main menu
move to sidebar
hide
Navigation
Main page
Recent changes
Random page
Help about MediaWiki
Special pages
Niidae Wiki
Search
Search
Appearance
Create account
Log in
Personal tools
Create account
Log in
Pages for logged out editors
learn more
Contributions
Talk
Editing
Magnetic field
(section)
Page
Discussion
English
Read
Edit
View history
Tools
Tools
move to sidebar
hide
Actions
Read
Edit
View history
General
What links here
Related changes
Page information
Appearance
move to sidebar
hide
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
==== As different aspects of the same phenomenon ==== According to [[special relativity|the special theory of relativity]], the partition of the [[electromagnetic force]] into separate electric and magnetic components is not fundamental, but varies with the [[Frame of reference#Observational frames of reference|observational frame of reference]]: An electric force perceived by one observer may be perceived by another (in a different frame of reference) as a magnetic force, or a mixture of electric and magnetic forces. The magnetic field existing as electric field in other frames can be shown by consistency of equations obtained from [[Lorentz transformation]] of four force from [[Coulomb's law|Coulomb's Law]] in particle's rest frame with [[Maxwell's equations|Maxwell's laws]] considering definition of fields from [[Lorentz force#Lorentz force law as the definition of E and B|Lorentz force]] and for non accelerating condition. The form of magnetic field hence obtained by [[Lorentz transformation]] of [[four-force]] from the form of [[Coulomb's law]] in source's initial frame is given by:<ref name="Rosser1968">{{Cite book |last1=Rosser |first1=W. G. V. |url=https://link.springer.com/book/10.1007/978-1-4899-6559-2 |title=Classical Electromagnetism via Relativity |year=1968 |isbn=978-1-4899-6258-4 |publisher=Springer |location=Boston, MA |language=en |doi=10.1007/978-1-4899-6559-2}}</ref>{{rp|pages=29–42}} <math display="block">\mathbf{B} = \frac q {4 \pi \varepsilon_0 r^3} \frac {1- \beta^2} {(1- \beta^2 \sin^2 \theta)^{3/2}} \frac{\mathbf{v} \times \mathbf{r}}{c^2} = \frac{\mathbf{v} \times \mathbf{E}}{c^2}</math> where <math>q</math> is the charge of the point source, <math>\varepsilon_0</math> is the [[vacuum permittivity]], <math>\mathbf{r}</math> is the position vector from the point source to the point in space, <math>\mathbf{v}</math> is the velocity vector of the charged particle, <math>\beta</math> is the ratio of speed of the charged particle divided by the speed of light and <math>\theta</math> is the angle between <math>\mathbf{r}</math> and <math>\mathbf{v}</math>. This form of magnetic field can be shown to satisfy Maxwell's laws within the constraint of particle being non accelerating.<ref>{{Cite book |last=Purcell |first=Edward |url=http://dx.doi.org/10.1017/cbo9781139005043 |title=Electricity and Magnetism |date=2011-09-22 |publisher=Cambridge University Press |isbn=978-1-107-01360-5 |doi=10.1017/cbo9781139005043}}</ref> The above reduces to [[Biot–Savart law|Biot-Savart law]] for non relativistic stream of current (<math>\beta\ll 1</math>). Formally, special relativity combines the electric and magnetic fields into a rank-2 [[tensor]], called the ''[[electromagnetic tensor]]''. Changing reference frames ''mixes'' these components. This is analogous to the way that special relativity ''mixes'' space and time into [[spacetime]], and mass, momentum, and energy into [[four-momentum]].<ref>C. Doran and A. Lasenby (2003) ''Geometric Algebra for Physicists'', Cambridge University Press, p. 233. {{ISBN|0521715954}}.</ref> Similarly, the [[Magnetic energy|energy stored in a magnetic field]] is mixed with the energy stored in an electric field in the [[electromagnetic stress–energy tensor]].
Summary:
Please note that all contributions to Niidae Wiki may be edited, altered, or removed by other contributors. If you do not want your writing to be edited mercilessly, then do not submit it here.
You are also promising us that you wrote this yourself, or copied it from a public domain or similar free resource (see
Encyclopedia:Copyrights
for details).
Do not submit copyrighted work without permission!
Cancel
Editing help
(opens in new window)
Search
Search
Editing
Magnetic field
(section)
Add topic