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Chapter 5: Symbouc Mbthod

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1897
Section IDtheory-calculation-alternating-current-phenomena-1897-chapter-05
Locationlines 2744-3229
Statuscandidate
Word Count2030
Equation Candidates In Section31
Figure Candidates In Section0
Quote Candidates In Section0
CHAPTER V. SYMBOUC MBTHOD. 23. The graphical method of representing alternating- current phenomena by polar coordinates of time affords the best means for deriving a clear insight into the mutual rela- tion of the different alternating sine waves entering into the problem. For numerical calculation, however, the graphical method is frequently not well suited, owing to the widely •different magnitudes of the alternating sine waves repre- sented in the same diagram, which make an exact diagram- matic determination impossible. For instance, in the trans- former diagrams (cf. Figs. 18-20), the different magnitudes •will have numerical values in practice, somewhat like E-^ = 100 volts, and /j = 75 amperes, for a non-inductive secon- dary load, as of incandescent lamps. Thus the only reac- tance of the secondary circuit is that of the secondary coil, or,
CHAPTER V. SYMBOUC MBTHOD. 23. The graphical method of representing alternating- current phenomena by polar coordinates of time affords the best means for deriving a clear insight into the mutual rela- tion of the different alternating sine waves entering into the problem. For numerical calculation, however, the graphical method is frequently not well suited, owing to the widely •different magnitudes of the alternating sine waves repre- sented in the same diagram, which make an exact diagram- matic determination im ...
... ng sine waves repre- sented in the same diagram, which make an exact diagram- matic determination impossible. For instance, in the trans- former diagrams (cf. Figs. 18-20), the different magnitudes •will have numerical values in practice, somewhat like E-^ = 100 volts, and /j = 75 amperes, for a non-inductive secon- dary load, as of incandescent lamps. Thus the only reac- tance of the secondary circuit is that of the secondary coil, or, x\ = .08 ohms, giving a lag of eSj = 3.6^. We have also, fty = 30 turns. Uf, = 300 turns. (Fi = 2250 amper ...
... . If /= / +ji' is a sine wave of alternating current, and r is the resistance, the E.M.F. consumed by the re- sistance is in phase with the current, and equal to the prod- uct of the current and resistance. Or — r/= ri '\' jri\ If L is the inductance, and j: = 2 tt NL the reactance, the E.M.F. produced by the reactance, or the counter §20] SYMBOLIC METHOD. 39' E.M.F. of self-inductance, is the product of the current and reactance, and lags 90° behind the current; it is, therefore, represented by the expression — jxl =jxi — xi\ The E.M.F. requir ...
... — 7 ^ (^+J^(^+Jx) ^ er — /x , . /r + <f j: . or, if ^= ^? +yV' is the impressed E.M.F., and / = i +ji^ the current flowing in the circuit, its impedance is — Z^^ =^+J^ ^ (f +J^(' -Jn ^ ^i + ^i' I /i' - ^i' 40 ALTERNATING-CURRENT PHENOMENA, [§§ 30, 31 30. If C is the capacity of a condenser in series in a circuit of current 7=1 +/**', the E.M.F. impressed upon the terminals of the condenser is -£" = ~ , 90° behind the current ; and may be represented by —-^ — — - , or jx^ /, where x^^ = — • is the capacity reaciatice or condensance of the co ...
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Candidate IDOCR / PDF-Text CandidateSource Location
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0077100 volts, and /j = 75 amperes, for a non-inductive secon-line 2759
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0078or, x\ = .08 ohms, giving a lag of eSj = 3.6^. We haveline 2762
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0079fty = 30 turns.line 2766
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0080Uf, = 300 turns.line 2768
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0081(Fi = 2250 ampere-turns.line 2770
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0082$f = 100 ampere- turns.line 2772
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0083Er = 10 volts.line 2774
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0084£^ = 60 volts.line 2776
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  • Waves / transmission lines: Map Steinmetz’s wave and line language onto modern distributed constants, propagation velocity, standing waves, and reflections.
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  • Dielectricity / capacity: Check whether the passage treats capacity, condensers, displacement, or dielectric stress as field storage rather than only circuit algebra.
  • Alternating current: Compare Steinmetz’s AC language with modern sinusoidal steady-state analysis, RMS quantities, phase, and phasor notation.
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  • Dielectricity / capacity: A Wheeler-style reading may emphasize dielectric compression, field stress, and stored potential, but this page treats that as interpretation unless Steinmetz explicitly says it.
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