Electric field

An electric field is a vector field that shows the direction that a positively charged particle will move when placed in the field. More precisely, if a particle has an electric charge $q$ and is in an electric field ${\vec {E}}$ , the electric force the charge will feel is ${\vec {F}}=q\cdot {\vec {E}}$ . Electric fields are produced around objects that have electrical charge, or by a magnetic field that changes with time. Electric field lines are used to represent the influence of electric field. ^[1] The idea of an electric field was first made by Michael Faraday.^[2]

Electric fields are caused by electric charges, described by Gauss's law,^[3] or varying magnetic fields, described by Faraday's law of induction.^[4] The equations of both fields are coupled and together form Maxwell's equations that describe both fields as a function of charges and currents.^[5]

Related pages

Polarization electric field and ambipolar electric field

References

↑ Richard Feynman (1970). The Feynman Lectures on Physics Vol II. Addison Wesley Longman. ISBN 978-0-201-02115-8.
↑ "Michael Faraday". Retrieved 2015-06-30.
↑ Purcell, p 25: "Gauss's Law: the flux of the electric field E through any closed surface... equals 1/e times the total charge enclosed by the surface."
↑ Purcell, p 356: "Faraday's Law of Induction."
↑ Purcell, Edward & Morin, David 2013. Electricity and magnetism. 3rd ed, Cambridge University Press. New York. ISBN 978-1-107-01402-2

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[1] Richard Feynman (1970). The Feynman Lectures on Physics Vol II. Addison Wesley Longman. ISBN 978-0-201-02115-8.

[2] "Michael Faraday". Retrieved 2015-06-30.

[3] Purcell, p 25: "Gauss's Law: the flux of the electric field E through any closed surface... equals 1/e times the total charge enclosed by the surface."

[4] Purcell, p 356: "Faraday's Law of Induction."

[5] Purcell, Edward & Morin, David 2013. Electricity and magnetism. 3rd ed, Cambridge University Press. New York. ISBN 978-1-107-01402-2

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