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Chapter 6: Magnetism

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FieldValue
SourceTheory and Calculation of Electric Circuits
Year1917
Section IDtheory-calculation-electric-circuits-chapter-06
Locationlines 11051-12221
Statuscandidate
Word Count4468
Equation Candidates In Section44
Figure Candidates In Section1
Quote Candidates In Section0
CHAPTER VI MAGNETISM MECHANICAL FORCES 1. General 61. Mechanical forces appear wherever magnetic fields act on electric currents. The work done by all electric motors is the result of these forces. In electric generators, they oppose the driving power and thereby consume the power which finds its equivalent in the electric power output. The motions produced by the electromagnet are due to these forces. Between the primary and the secondary coils of the transformer, between conductor and return conductor of an electric circuit, etc., such mechanical forces appear. The electromagnet, and all electrodynamic machinery, are based on the use of these mechanical forces between electric conductors and magnetic fields. So also is that type of trans- former which transforms constant alternating voltage into con- stant alternating current. In most other cases, however, these mechanical forces
CHAPTER VI MAGNETISM MECHANICAL FORCES 1. General 61. Mechanical forces appear wherever magnetic fields act on electric currents. The work done by all electric motors is the result of these forces. In electric generators, they oppose the driving power and thereby consume the power which fin ...
... the pull, and the pull or force of the electromagnet pulsates with double frequency between and 2F. 63. In the alternating-current electromagnet usually the vol- tage consumed by the resistance of the winding, tV, can be neglected compared with the voltage consumed by the reactance of the winding, ioXy and the latter, therefore, is practically equal to the terminal voltage, e, of the electromagnet. We have then, by the general equation of self-induction, e = 27r fLio (20) 96 ELECTRIC CIRCUITS where / = frequency, in cycles per second. From which ...
CHAPTER VI MAGNETISM MECHANICAL FORCES 1. General 61. Mechanical forces appear wherever magnetic fields act on electric currents. The work done by all electric motors is the result of these forces. In electric generators, they oppose the driving power and thereby consume the power which finds its equivalent in the electric power output. The motions produced by the electromag ...
CHAPTER VI MAGNETISM MECHANICAL FORCES 1. General 61. Mechanical forces appear wherever magnetic fields act on electric currents. The work done by all electric motors is the result of these forces. In electric generators, they oppose the driving power and thereby consume the power which finds its equivalent in the electric power output. The motions produced by the electromagnet ar ...
Concept CandidateHits In SectionStatus
Frequency3seeded
Ether1seeded
Term CandidateHits In SectionStatus
ether1seeded
Candidate IDOCR / PDF-Text CandidateSource Location
theory-calculation-electric-circuits-eq-candidate-0257energy produced, + increase of the stored magnetic energy. (1)line 11124
theory-calculation-electric-circuits-eq-candidate-0258mechanical energy t^o =Fl by (1), and therefrom the mechanicalline 11137
theory-calculation-electric-circuits-eq-candidate-02592. The Constant-current Electromagnetline 11175
theory-calculation-electric-circuits-eq-candidate-0260to its final position 2,1 = the length of this motion, or the strokeline 11183
theory-calculation-electric-circuits-eq-candidate-0261L=-^10-8 (2)line 11189
theory-calculation-electric-circuits-eq-candidate-0262$, = Mil 108 (3)line 11196
theory-calculation-electric-circuits-eq-candidate-0263^, = 12^ 108 (4)line 11203
theory-calculation-electric-circuits-eq-candidate-0264e’ = n_lO« = t.^ (5)line 11214
Candidate IDOCR / PDF-Text CandidateSource Location
theory-calculation-electric-circuits-fig-045density is uniform for the width lo between the coil surfaces, Fig. 45. and then decreases toward the interior of the coils, over the dis- tance K respectively ^, to zero at the…line 11784
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  • Magnetism: Track flux, reluctance, permeability, magnetizing force, and loss language against modern magnetic-circuit terminology.
  • Impedance / reactance: Translate historical opposition terms into modern impedance, admittance, conductance, susceptance, and complex-plane notation.
  • Field language: Read for whether field language is mechanical, geometrical, causal, descriptive, or simply a convenient engineering model.
  • Alternating current: Compare Steinmetz’s AC language with modern sinusoidal steady-state analysis, RMS quantities, phase, and phasor notation.
  • Radiation / light: Compare the chapter’s radiation vocabulary with modern electromagnetic radiation, spectral frequency, wavelength, absorption, and illumination engineering.
  • Magnetism: Centrifugal/divergent magnetic-field readings are interpretive overlays, not automatic historical claims.
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