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Chapter 13: Foucault Or Eddy Currents

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1916
Section IDtheory-calculation-alternating-current-phenomena-chapter-13
Locationlines 13484-14333
Statuscandidate
Word Count3721
Equation Candidates In Section0
Figure Candidates In Section3
Quote Candidates In Section0
CHAPTER XIII FOUCAULT OR EDDY CURRENTS 105. While magnetic hysteresis due to molecular friction is a magnetic phenomenon, eddy currents are rather an electrical phenomenon. When iron passes through a magnetic field, a loss of energy is caused by hysteresis, which loss, however, does not react magnetically upon the field. When cutting an electric conductor, the magnetic field produces a current therein. The m.m.f. of this current reacts upon and affects the magnetic field, more or less; consequently, an alternating magnetic field cannot penetrate deeply into a solid conductor, but a kind of screening effect is produced, which makes solid masses of iron unsuitable for alternating fields, and necessitates the use of laminated iron or iron wire as the carrier of magnetic flux. Eddy currents are true electric currents, though existing in minute circuits; and
CHAPTER XIII FOUCAULT OR EDDY CURRENTS 105. While magnetic hysteresis due to molecular friction is a magnetic phenomenon, eddy currents are rather an electrical phenomenon. When iron passes through a magnetic field, a loss of energy is caused by hysteresis, which loss, however, does not react magnetically upon the field. When cuttin ...
CHAPTER XIII FOUCAULT OR EDDY CURRENTS 105. While magnetic hysteresis due to molecular friction is a magnetic phenomenon, eddy currents are rather an electrical phenomenon. When iron passes through a magnetic field, a loss of energy is caused by hysteresis, which loss, however, does not react magnetically upon the field. When cutting an electric conductor, the magnetic field produces a current therein. The m.m.f. of this current reacts upon and affects the magnetic field, more or less ...
... e of laminated iron or iron wire as the carrier of magnetic flux. Eddy currents are true electric currents, though existing in minute circuits; and they follow all the laws of electric circuits. Their e.m.f. is proportional to the intensity of magnetization, B, and to the frequency, /. Eddy currents are thus proportional to the magnetization, B, the frequency, /, and to the electric conductivity, X, of the iron; hence, can be expressed by i = bXBf. The power consumed by eddy currents is proportional to their square, and inversely proportional to t ...
... E = V2Tr AnfB 10-^, it follows that, The loss of power by eddy currents is proportional to the square of the e.m.f., and proportional to the electric con- ductivity of the iron; or, P = aE^\. 136 FOUCAULT OR EDDY CURRENTS 137 Hence, that component of the effective conductance which is due to eddy currents is P . that is, The equivalent conductance due to eddy currents in the iron is a constant of the magnetic circuit; it is independent of e.m.f., frequency, etc., but proportional to the electric conductivity of the iron, X. Eddy currents, l ...
Concept CandidateHits In SectionStatus
Frequency14seeded
Ether3seeded
Light2seeded
Magnetic permeability1seeded
Term CandidateHits In SectionStatus
ether3seeded
effective resistance1source-located candidate
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theory-calculation-alternating-current-phenomena-fig-092magnetic flux inclosed by the zone is SuV. Fig. 92. Hence, the e.m.f. generated in this zone isline 13742
theory-calculation-alternating-current-phenomena-fig-09393. Fig. 93. 110. Demagnetizing, or screening effect of eddy currents.line 13860
theory-calculation-alternating-current-phenomena-fig-094du Fig. 94. The current inclosed by this zone is /„line 14074
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