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Chapter 15: Distributed Capacity, Inductance, Resistance, And Leakage

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1916
Section IDtheory-calculation-alternating-current-phenomena-chapter-15
Locationlines 15410-16076
Statuscandidate
Word Count2938
Equation Candidates In Section0
Figure Candidates In Section2
Quote Candidates In Section0
CHAPTER XV DISTRIBUTED CAPACITY, INDUCTANCE, RESISTANCE, AND LEAKAGE 127. In the foregoing, the phenomena causing loss of energy in an alternating-current circuit have been discussed; and it has been shown that the mutual relation between current and e.m.f. can be expressed by two of the four constants: power component of e.m.f., in phase with current, and = current X effective resistance, or r; reactive component of e.m.f., in quadrature with current, and = current X effective reactance, or x; power component of current, in phase with e.m.f., and = e.m.f. X effective conductance, or g; reactive component of current, in quadrature with e.m.f., and = e.m.f. X effective susceptance, or b. In many cases the exact calculation of the quantities, r, x, g, h, is not possible in the present state of the art. In
CHAPTER XV DISTRIBUTED CAPACITY, INDUCTANCE, RESISTANCE, AND LEAKAGE 127. In the foregoing, the phenomena causing loss of energy in an alternating-current circuit have been discussed; and it has been shown that the mutual relation between current and e.m.f. can be expressed by two of the four constants: ...
... the mutual relation between current and e.m.f. can be expressed by two of the four constants: power component of e.m.f., in phase with current, and = current X effective resistance, or r; reactive component of e.m.f., in quadrature with current, and = current X effective reactance, or x; power component of current, in phase with e.m.f., and = e.m.f. X effective conductance, or g; reactive component of current, in quadrature with e.m.f., and = e.m.f. X effective susceptance, or b. In many cases the exact calculation of the quantities, r, x, g, h, ...
... ility of the approximate representation of the line by one or by three condensers. Assuming, for instance, that the line conductors are of 1 cm. diameter, and at a distance from each other of 50 cm,, and that the length of transmission is 50 km., we get the capacity of the transmission line from the formula — C = 1.11 X 10-« kl H- 4 loge 2- microfarads, where k = dielectric constant of the surrounding medium = 1 in air; I = length of conductor = 5 X 10" cm.; ■ d = distance of conductors from each other = 50 cm.; 5 = diameter of conductor = 1 cm. Hence C ...
CHAPTER XV DISTRIBUTED CAPACITY, INDUCTANCE, RESISTANCE, AND LEAKAGE 127. In the foregoing, the phenomena causing loss of energy in an alternating-current circuit have been discussed; and it has been shown that the mutual relation between current and e.m.f. can be expressed by two of the four constants: ...
Concept CandidateHits In SectionStatus
Frequency4seeded
Ether3seeded
Radiation2seeded
Dielectric constant1seeded
Light1seeded
Velocity of light1seeded
Term CandidateHits In SectionStatus
effective resistance3source-located candidate
ether3seeded
counter e.m.f.1source-located candidate
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Candidate IDOCR / PDF-Text CandidateSource Location
theory-calculation-alternating-current-phenomena-fig-100JTTTTTTTTTTTTTTTTTTTTTTT- Fig. 100. In this case the intensity as well as phase of the current, and consequently of the counter e.m.f. of inductive reactance andline 15474
theory-calculation-alternating-current-phenomena-fig-101iEo Fig. 101. Denoting in Fig. 101.line 15606
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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.
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