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Chapter 12: Effective Resistance And Reactance

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1916
Section IDtheory-calculation-alternating-current-phenomena-chapter-12
Locationlines 10718-13483
Statuscandidate
Word Count5679
Equation Candidates In Section0
Figure Candidates In Section7
Quote Candidates In Section0
CHAPTER XII EFFECTIVE RESISTANCE AND REACTANCE 89. The resistance of an electric circuit is determined : 1. By direct comparison with a known resistance (Wheat- stone bridge method, etc.). This method gives what may be called the true ohmic resist- ance of the circuit. 2. By the ratio: Volts consumed in circuit Amperes in circuit In an alternating-current circuit, this method gives, not the resistance of the circuit, but the impedance, z = \/f^ + x^. 3. By the ratio: Power consumed, (Current) 2 where, however, the "power" does not include the work done by the circuit, and the counter e.m.fs. representing it, as, for instance, in the case of the counter e.m.f. of a motor. In alternating-current circuits, this value of resistance is the power coefficient of the e.m.f.. Power component of e.m.f. Total
... of most of the difficulties met in dealing analytically with alternating-current circuits containing iron. 90. The foremost sources of energy loss in alternating-current circuits, outside of the true ohmic resistance loss, are as follows : 1. Molecular friction, as, (a) Magnetic hysteresis; (6) Dielectric hysteresis. 2. Primary electric currents, as, (a) Leakage or escape of current through the insulation, brush discharge, corona. (6) Eddy currents in the conductor or unequal current distribution. EFFECTIVE RESISTANCE AND REACTANCE 113 -» ...
... omenon, first a circuit may be con- sidered, of very high inductive reactance, but negligible true ohmic resistance; that is, a circuit entirely surrounded by iron, as, for instance, the primary circuit of an alternating-current transformer with open secondary circuit. The wave of current produces in the iron an alternating mag- netic flux which generates in the electric circuit an e.ni.f. — the counter e.m.f. of self-induction. If the ohmic resistance is negligible, that is, practically no e.m.f. consuzned by the resist- ance, all the impressed e. ...
CHAPTER XII EFFECTIVE RESISTANCE AND REACTANCE 89. The resistance of an electric circuit is determined : 1. By direct comparison with a known resistance (Wheat- stone bridge method, etc.). This method gives what may be called the true ohmic resist- ance of the circuit. 2. By the ratio: Volts consumed in circuit ...
... r as heat inside of the electric conductor b}^ a current of uniform density, the effective resistance represents the total expenditure of power. Since in an alternating-current circuit, in general power is expended not only in the conductor, but also outside of it, through hysteresis, secondary currents, etc., the effective resist- ance frequently differs from the true ohmic resistance in such way as to represent a larger expenditure of power. In dealing with alternating-current circuits, it is necessarj-, therefore, to substitute everywhere the values ...
Concept CandidateHits In SectionStatus
Frequency19seeded
Magnetic permeability7seeded
Ether1seeded
Term CandidateHits In SectionStatus
effective resistance16source-located candidate
counter e.m.f.8source-located candidate
ether1seeded
Candidate IDOCR / PDF-Text CandidateSource Location
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Candidate IDOCR / PDF-Text CandidateSource Location
theory-calculation-alternating-current-phenomena-fig-081^ Fig. 81. The general character of these current waves is, that the maxi-line 11510
theory-calculation-alternating-current-phenomena-fig-082then Fig. 82. — X^line 12025
theory-calculation-alternating-current-phenomena-fig-086n = NUMBER OF TURNS Fig. 86. 350line 12600
theory-calculation-alternating-current-phenomena-fig-087/ = FREQUENCY Fig. 87. 400line 12686
theory-calculation-alternating-current-phenomena-fig-088200 250 Fig. 88. 300line 12813
theory-calculation-alternating-current-phenomena-fig-089/=CYCLES Fig. 89. 300line 12940
theory-calculation-alternating-current-phenomena-fig-090n=NUMBER OF TURNS Fig. 90. 350line 13034
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  • Magnetism: Track flux, reluctance, permeability, magnetizing force, and loss language against modern magnetic-circuit terminology.
  • Waves / transmission lines: Map Steinmetz’s wave and line language onto modern distributed constants, propagation velocity, standing waves, and reflections.
  • Impedance / reactance: Translate historical opposition terms into modern impedance, admittance, conductance, susceptance, and complex-plane notation.
  • Hysteresis: Compare the passage with modern magnetic loss, B-H loop area, lag, material memory, and empirical loss laws.
  • Alternating current: Compare Steinmetz’s AC language with modern sinusoidal steady-state analysis, RMS quantities, phase, and phasor notation.
  • Magnetism: Centrifugal/divergent magnetic-field readings are interpretive overlays, not automatic historical claims.
  • Waves / transmission lines: Standing/traveling wave passages may support richer field interpretations; the page keeps those readings separate from verified Steinmetz wording.
  • Hysteresis: An interpretive reading can treat hysteresis as field lag or memory, but the historical claim must remain Steinmetz’s actual magnetic-loss treatment.
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