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Chapter 6: Alternating Magnetic Flux Distribution

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FieldValue
SourceTheory and Calculation of Transient Electric Phenomena and Oscillations
Year1909
Section IDtheory-calculation-transient-electric-phenomena-oscillations-chapter-46
Locationlines 23948-24980
Statuscandidate
Word Count2710
Equation Candidates In Section0
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Quote Candidates In Section0
CHAPTER VI. ALTERNATING MAGNETIC FLUX DISTRIBUTION. 48. As carrier of magnetic flux iron is used, as far as possible, since it has the highest permeability or magnetic conductivity. If the magnetic flux is alternating or otherwise changing rapidly, an e.m.f. is generated by the change of magnetic flux in the iron, and to avoid energy losses and demagnetization by the currents produced by these e.m.fs. the iron has to be subdivided in the direction in which the currents would exist, that is, at right angles to the lines of magnetic force. Hence, alternating magnetic fields and magnetic structures desired to respond very quickly to changes of m.m.f. are built of thin wires or thin iron sheets, that is, are laminated. Since the generated e.m.fs. are proportional to the frequency of the alternating magnetism, the laminations
CHAPTER VI. ALTERNATING MAGNETIC FLUX DISTRIBUTION. 48. As carrier of magnetic flux iron is used, as far as possible, since it has the highest permeability or magnetic conductivity. If the magnetic flux is alternating or otherwise changing rapidly, an e.m.f. is generated by the change of magnetic flux in t ...
... t angles to the lines of magnetic force. Hence, alternating magnetic fields and magnetic structures desired to respond very quickly to changes of m.m.f. are built of thin wires or thin iron sheets, that is, are laminated. Since the generated e.m.fs. are proportional to the frequency of the alternating magnetism, the laminations must be finer the higher the frequency. To fully utilize the magnetic permeability of the iron, it there- fore has to be laminated so as to give, at the impressed frequency, practically uniform magnetic induction throughout its ...
... ), and (24), as ^2Ve+2d + e-*'I + 2cos2d, (25) o CB1 = >e+2^ + £-2^o + 2cos2c/0, (26) (B = and 2 cos 2 (28) 52. Where the thickness of lamination, 2 Z0, or the frequency/, is so great as to give cZ0 a value sufficiently high to make e~cl°, or the reflected wave, negligible compared with the main wave e+cl°, the equations can be simplified by dropping s~cl. In this case the flux density, (B, is very small or practically nothing in the interior, and reaches appreciable values only near the surface. It then is preferable to count the ...
... dl from the center line of the lamination, and 2 10 = the total thickness of the lamination. If then / = the current density in the layer dl, and E = the e.m.f.'per unit length generated in the zone dl by the alternating magnetic flux, we have The magnetic flux density (Bj at the surface I = 10 of the lamination corresponds to the Fig. 92. Alter- jmpresseci or external m.m.f. The' density (B natmg magnetic ,, 77 , ,, fluxdistribution m the zone dl corresponds to the impressed in solid iron. m.m.f. plus the sum of all the m.m.fs. in the zone ...
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Magnetic permeability3seeded
Light1seeded
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wave length10seeded
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