How to Commonly Classify the Induction Phenomena?!
Posted: Sunday, October 14, 2007
by Alexander SIDOROVICH
fenomena
Along with the known notions of an electric (electrostatic) induction and a magnetic induction the physical sense of the number of dynamical induction phenomena is defined by their mutual bond with the basic Laws and phenomena of dynamical induction – “Magnetoelectric induction" [1831] and “Electromagnetic induction" [1751 – 1862 - 1980] (which are symmetric) with account of novations and consequences of recent time period, as following:
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LAW of MAGNETOELECTRIC INDUCTION (M. Faraday, 1831; J. C. Maxwell, 1864).
-- Faraday M. Experimental Researches in Electricity [Ser. 1, pt. 2. Evolution of electricity from magnetismus] // Philosoph. Trans. of the Royal Soc., 1832, p. 133 – 145.
-- Maxwell J. C. A Dynamical Theory of the Electromagnetic Field. -- Royal Society
Transactions, v. CLV, 1864.
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MAGNETOELECTRIC INDUCTION (M. Faraday, 1831) {phenomenon].
-- Faraday M. Experimental Researches in Electricity [Ser. 1, pt. 2. Evolution of electricity from magnetismus] // Philosoph. Trans. of the Royal Soc., 1832, p. 133 – 145.
Magnetoelectric induction is the phenomenon of excitement of the electromotive force (EMF) of induction in contour as a result of change of magnetic flux (or magnetic flux linkage) across surface, bounded by this contour, because of change of magnetic field itself or motion of the contour (of electroconductor, dielectric or another body) in the stationary magnetic field.
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ELECTRIC MUTUAL INDUCTION (M. Faraday, 1831) {phenomenon].
-- Faraday M. Experimental Researches in Electricity [Ser. 1, pt. 1. Induction of electric currents] // Philosoph. Trans. of the Royal Soc., 1832, p. 126 – 133.
Electric mutual induction is the phenomenon of exciting of the electromotive force (EMF) in contour of an electric circuit due to the magnetoelectric induction, caused by change of the magnetic flux, which is linked with the contour and is attributed to electric currents in other contours
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UNIPOLAR MAGNETOELECTRIC INDUCTION (M. Faraday, 1831) [phenomenon]
-- Faraday M. Experimental Researches in Electricity [Ser. 1, pt. 4.] // Philosoph. Trans. of the Royal Soc., 1832, p. 156 – 182.
Unipolar magnetoelectric induction is the phenomenon of exciting of the electromotive force (EMF) of magnetoelectric induction in result of a motion of electroconductive or dielectric body or medium (electroconductor, dielectric, magnetic, magnet, magnetodielectric) transverse to external or own magnetic field.
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ELECTRIC SELF-INDUCTION (J. Henry, 1832; M. Faraday, 1834 - 1835) [phenomenon].
-- Henry J. On the production of currents and sparks from magnetism // American Journal of Science, vol. 22, 1832, p. 403 – 408.
-- Faraday M. On the magneto-electric spark and shock and on a peculiar condition of electric and magnetoelectric induction // Philosoph. Mag., vol. 5, 1834, p. 349 – 354.
-- Faraday M. Experimental Researches in Electricity [Ser. 9, pt. 15] // Philosoph. Trans. of the Royal Soc., 1835, p. 41- 68.
Electric self-induction is the phenomenon of exciting of the electromotive force (EMF) in contour of an electric circuit due to magnetoelectric induction, caused by the change of the magnetic flux, which is linked with contour and is attributed to the electric current in this same contour.
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LAW of ELECTROMAGNETIC INDUCTION (J. C. Maxwell, 1862; A. M. Sidorovich, 1980).
-- Maxwell J. C. On Physical Lines of Force. Pt. 3 // Phil. Mag., 1862, vol. XXIII, p. 12 - 24.
-- Sidorovich A. M., To binary-inversion interpretation of Maxwell’s equations and the induction phenomena // News of Acad. Sci. BSSR. Ser. phys.-mat. sci., 1980, No 3, p. 126 (In Russian).
-- Sidorovich A. M., Electromagnetic Induction (New Conception). -- Proc. Int. Symp. (ISEF’87), Pavia, Italy, September 1987, p. 25 - 27.
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ELECTROMAGNETIC INDUCTION (B. Franclin, 1751; J. C. Maxwell, 1862; A. M. Sidorovich, 1980) [phenomenon].
-- Franclin B. Experiments and Observations on Electricity, 1770. [Benjamin Franklin’s Experiments. – Cambridge, Massashusetts, 1941].
-- Maxwell J. C. On Physical Lines of Force. Pt. 3 // Phil. Mag., 1862, vol. XXIII, p. 12 - 24.
-- Sidorovich A. M., To binary-inversion interpretation of Maxwell’s equations and the induction phenomena // News of Acad. Sci. BSSR. Ser. phys.-mat. sci., 1980, No 3, p. 126 (In Russian).
-- Sidorovich A. M., Electromagnetic Induction (New Conception). – Proc. Int. Symp. (ISEF’87), Pavia, Italy, September 1987, p. 25 - 27.
Electromagnetic induction is the phenomenon of excitement of the magnetomotive force (MMF) of induction in a contour as a result of change of an electric induction flux (or electric flux linkage of the contour) across surface, bounded by this contour, because of change of field itself or motion of the contour (magnetic, magnetodielectric or another magnetisable body) in stationary electric field.
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MAGNETIC NUTUAL INDUCTION (A. M. Sidorovich, 1980) [phenomenon].
-- Sidorovich A. M., To binary-inversion interpretation of Maxwell’s equations and the induction phenomena // News of Acad. Sci. BSSR. Ser. phys.-mat. sci., 1980, No 3, p. 126 (In Russian).
= Sidorovich A. M., Electromagnetic Induction (New Conception). -- Proc. Int. Symp. (ISEF’87), Pavia, Italy, September 1987, p. 25 - 27.
Magnetic mutual induction is the phenomenon of excitation of the magnetomotive force (MMF) in contour of a magnetic circuit due to the electromagnetic induction, caused by change of the electric induction flux, which is linked with the contour and is attributed to magnetic currents in other contours.
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UNIPOLAR ELECTROMAGNETIC INDUCTION (A. M. Sidorovich, 1980) [phenomenon].
-- Sidorovich A. M., To binary-inversion interpretation of Maxwell’s equations and the induction phenomena // News of Acad. Sci. BSSR. Ser. phys.-mat. sci., 1980, No 3, p. 126 (In Russian).
-- Sidorovich A. M., Electromagnetic Induction (New Conception). -- Proc. Int. Symp. (ISEF’87), Pavia, Italy, September 1987, p. 25 - 27.
Unipolar electromagnetic induction is the phenomenon of excitation of the magnetomotive force (MMF) of electromagnetic induction in result of a motion of magnetisable body or medium (magnetodielectric, ferrite, electret or other) transverse to external or own electric field.
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MAGNETIC SELF-INDUCTION (A. M. Sidorovich, 1980) [phenomenon].
-- Sidorovich A. M., To binary-inversion interpretation of Maxwell’s equations and the induction phenomena // News of Acad. Sci. BSSR. Ser. phys.-mat. sci., 1980, No 3, p. 126 (In Russian).
-- Sidorovich A. M., Electromagnetic Induction (New Conception). -- Proc. Int. Symp. (ISEF’87), Pavia, Italy, September 1987, p. 25 - 27.
Magnetic self-induction is the phenomenon of excitation of the magnetomotive force (MMF) in contour of a magnetic circuit due to electromagnetic induction, caused by the change of the electric induction flux, which is linked with contour and is attributed to the magnetic current in this same contour.
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With such interpretation of the induction phenomena (notions, terms and essense) M. Faraday and J. C. Maxwell are also in solidarity [namely, -- as for phenomenon of “Magnetoelectric induction of Faraday" (1831)].
The phenomena of “Magnetoelectric induction" (1831), “Electric mutual induction" (1831) and “Unipolar magnetoelectric induction" (1831) were discovered by M. Faraday actially simultaneously in 1831. As well the phenomenon “Electric self-induction" (1832, 1834 -1835) is special case of the phenomenon “Electric mutual induction" (1831) and the phenomenon “Magnetoelectric induction" (1831).
Similarly the phenomena “Magnetic self-induction" (1980), “Magnetic mutual induction" (1980) and “Unipolar electromagnetic induction" (1980) are the consequences of “Law of electromagnetic induction" (1862, 1980) and also the special cases of the phenomenon “Electromagnetic induction" (1751 - 1862 - 1980).
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