Skip to content

Chapter 35: Balanced Symmetrical Polyphase Systems

Research workbench, not a finished commentary page.

This page is generated from processed source text and candidate catalogs. It exists to help researchers decide what to verify, promote, and deeply decode next.

FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1916
Section IDtheory-calculation-alternating-current-phenomena-chapter-35
Locationlines 37453-37957
Statuscandidate
Word Count2178
Equation Candidates In Section0
Figure Candidates In Section0
Quote Candidates In Section0
CHAPTER XXXV BALANCED SYMMETRICAL POLYPHASE SYSTEMS 303. In most applications of polyphase systems the system is a balanced symmetrical system, or as nearly balanced as possible. That is, it consists of n equal e.m.fs. displaced in phase from each other by - period, and producing equal currents of equal phase displacement against their e.m.fs. In such systems, each e.m.f. and its current can be considered separately as constituting a single-phase system, that is, the polyphase system can be resolved into n equal single-phase systems, each of which consists of one conductor of the polyphase system, with zero impedance as return circuit. Hereby the investigation of the polyphase system resolves itself into that of its constituent single-phase system. So, for instance, the polyphase system shown in Fig. 208, at balanced load, can be considered as consisting
... .m.fs. In such systems, each e.m.f. and its current can be considered separately as constituting a single-phase system, that is, the polyphase system can be resolved into n equal single-phase systems, each of which consists of one conductor of the polyphase system, with zero impedance as return circuit. Hereby the investigation of the polyphase system resolves itself into that of its constituent single-phase system. So, for instance, the polyphase system shown in Fig. 208, at balanced load, can be considered as consisting of the equal single- phase syst ...
... he line, Z = ^ +j| = 26 + 44johms. Choosing the voltage at the receiving end as zero vector, e = 46,100 volts, at 90 per cent, power-factor and therefore 43.6 per cent, induc- tance factor, the current is represented by 7 = 80 (0.9 - 0.436 j) =72-35 j. ^ Or. ii fi = permeability, k = dielectric constant of the medium sur- rounding the conductor, it is hence, V [^ I = \W or. C = (4) 452 ALTERNATING-CURRENT PHENOMENA This gives: Voltage at receiver circuit, e = 46,100 volts; current in receiver circuit, Z = 72 — 35 j amp. ; impeda ...
... HASE SYSTEMS 303. In most applications of polyphase systems the system is a balanced symmetrical system, or as nearly balanced as possible. That is, it consists of n equal e.m.fs. displaced in phase from each other by - period, and producing equal currents of equal phase displacement against their e.m.fs. In such systems, each e.m.f. and its current can be considered separately as constituting a single-phase system, that is, the polyphase system can be resolved into n equal single-phase systems, each of which consists of one conductor of the polyphase sy ...
... tem are star, or (in a three- phase system) Y quantities, it usually is more convenient to reduce all quantities to Y connection, and use one of the F-cir- cuits as the equivalent single-phase circuit. 304. As an example may be considered the calculation of a long-distance transmission line, delivering 10,000 kw., three-phase power at 60 cycles, 80,000 volts and 90 per cent, power-factor at 100 miles from the generating station, with approximately 10 per cent, loss of power in the transmission line, and with the line conductors arranged in a triangle 6 ft. dist ...
Concept CandidateHits In SectionStatus
Frequency3seeded
Dielectric constant1seeded
Light1seeded
Magnetic permeability1seeded
Wave length1seeded
Term CandidateHits In SectionStatus
wave length1seeded
Candidate IDOCR / PDF-Text CandidateSource Location
No chapter-local candidates yet--
Candidate IDOCR / PDF-Text CandidateSource Location
No chapter-local candidates yet--
Candidate IDCandidate PassageSource Location
No chapter-local candidates yet--
  • Impedance / reactance: Translate historical opposition terms into modern impedance, admittance, conductance, susceptance, and complex-plane notation.
  • Magnetism: Track flux, reluctance, permeability, magnetizing force, and loss language against modern magnetic-circuit terminology.
  • Dielectricity / capacity: Check whether the passage treats capacity, condensers, displacement, or dielectric stress as field storage rather than only circuit algebra.
  • Waves / transmission lines: Map Steinmetz’s wave and line language onto modern distributed constants, propagation velocity, standing waves, and reflections.
  • Complex quantities: Track how Steinmetz preserves geometric rotation and quadrature while translating the same operation into symbolic form.
  • Magnetism: Centrifugal/divergent magnetic-field readings are interpretive overlays, not automatic historical claims.
  • 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.
  • Waves / transmission lines: Standing/traveling wave passages may support richer field interpretations; the page keeps those readings separate from verified Steinmetz wording.
  1. Open the full source text and the scan or raw PDF.
  2. Verify the chapter boundary and surrounding context.
  3. Promote exact quotations only after checking the source image.
  4. Move mathematical candidates into canonical equation pages only after formula typography is corrected.
  5. Move diagram candidates into the diagram archive only after image extraction, crop verification, and manifest creation.
  6. Keep Steinmetz wording, modern translation, and ether-field interpretation in separate labeled layers.