Annotation The presented experiment is a proof of the fact that a stationary flow of electromagnetic energy creates electromagnetic induction.

Transcription

1 Khmelnik S.I. The Expeiment Confiming the Existence of the Fouth Electomagnetic Induction Annotation The pesented expeiment is a poof of the fact that a stationay flow of electomagnetic enegy ceates electomagnetic induction. Contents 1. Intoduction 2. The Expeiment 3. The Expeiment Analysis Refeences 1. Intoduction In [1] it is eing poved that thee exists a so-called fouth electomagnetic induction ceated y the electomagnetic enegy flow. It is eing poved that such induction is eing ceated also in a stationay flow of electomagnetic enegy. The poof can e given y an expeiment that cannot e explained in any othe way. Recently the autho has discoveed a desciption of an expeiment [2] which (in the autho's opinion) can e explained only y the fact that electomagnetic induction is ceated also y a stationay flow of electomagnetic enegy. 2. The Expeiment In [2] descies the following expeiment see Fig. 1 fom [2], whee 1 coppe conducto of diamete 5 mm and length 200 mm, 2 spial-shape coppe wie of diamete 1 mm, spial diamete 30 mm, 3 "excitation winding' aound the wie 2, nume of tuns 1700, G galvanomete. The main expeiment was as follows. Diect cuent I flowed though the excitation winding. Simultaneously a diect cuent I np, измеряемый гальванометром G, flows though the conducto 1. The cuent I сhanged fom 0.05 till 0.2A. The otained dependence I f ( I ) was linea. In paticula, if I 13 np mka, then I 0. 18A. np 1

2 Fig. 1. Anothe expeiment was as follows. Two conductos with thei spial-shaped excitation windings wee connected in paallel see Fig. 2 whee 1 is the fist conducto, 2 the second conducto, 3 and 4 excitation windings of the fist and second conductos accodingly. When connecting the windings oppositely, the cuent I 0. But when the np excitation windings wee connected accodingly "the cuents values ecame so high, that the galvanomete needle instantly went off scale", which coesponded to I 13 np mka. 2 Fig. 2.

3 The authos of expeiment indicate that "thee exist seveal explanations of the otained effect" [3, 4]. On the ase of the aove desciptions these expeiments can e explained using only the Maxwell equations. So it can e agued that these expeiments ae an expeimental poof of the existence of a fouth electomagnetic induction. 1 I 3 D C O B2 A B1 Fig. 3. 3

4 3. The Expeiment Analysis Let us conside Fig. 3, showing a Fagment of Excitation winding 3. This fagment epesents a tooidal solenoid whee cuent I is flowing. On evey tun of this solenoid the cuent I ceates a magnetic field with induction B 1. The solenoid coves the coppe conducto 1. The magnetic field of sepaate tuns as a whole ceates inside the conducto 1 a cicula magnetic field with induction B 2. In this way the excitation winding 3 has ceated along all the conducto 1 length a cicula field with induction B 2. Thus induction coesponds to a magnetic intensity which we'll denote as H. Hee is the adius of the cicle ОС. It is impotant to note that y symmety the intensity H depends only on (ut does not depend on the location of adius). With a lage esistance of excitation winding thee exists potential diffeence etween any point's А and D of the tooidal solenoid. The coesponding intensity of electical field in a point С has a pojection on the adius passing the point С. The sum of all such pojections (fom chods passing the point С) we shall denote as E. It is impotant to note that y symmety the intensity E depends only on (ut does not depend on the location of adius). So the excitation winding 3 excites in the conducto 1 a cicula magnetic intensity H and adial electical intensity. These intensities ceate a flow of electomagnetic enegy with the density S ( ) E ( ) H ( ). (1) This enegy flow is diected along the axis of the conducto 1. The flow passing a cicle of a adius, is S ( ) 4 2 S ( ) d. (2) The full enegy flow along the axis S S ) d (. (3) Is equal to powe P, tansmitted y the conducto, and is dissipated in the esistance of conducto 1. Thus, if admit the existence of the fouth electomagnetic induction (which was poved theoetically in [1]), then the consideed expeiment ecomes explainale. E 4

5 Refeences 1. Khmelnik S.I. The Fouth Electomagnetic Induction 'vixa Funding', 2. Toshin V.V., Busygin B.P., Pashchenko F.F., Kukovskiy L.E. The effect of constant electic cuent geneation in the stationay conducto in a constant magnetic field. The Institute of Contol Polems of Russian Science Academy named afte V.A. Tapenikov. The Almanac of Moden Science and Education, issue 12, 2008, in Russian, 3. Toshin V.V., Busygin B.P. Theoetical ackgound discovey of the effect of constant electic cuent geneation in the stationay conducto in a constant magnetic field, iid, 4. Toshin V.V., Busygin B.P., Pashchenko F.F. Logical methods in electodynamics. - M.: CP WASIZDAST, p., in Russian. 5