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Chapter 25: Distortion Of Wave-Shape And Its Causes

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1916
Section IDtheory-calculation-alternating-current-phenomena-chapter-25
Locationlines 29375-32539
Statuscandidate
Word Count7023
Equation Candidates In Section0
Figure Candidates In Section9
Quote Candidates In Section0
CHAPTER XXV DISTORTION OF WAVE-SHAPE AND ITS CAUSES 232. In the preceding chapters we have considered the alter- nating currents and alternating e.m.fs. as sine waves or as replaced by their equivalent sine waves. While this is sufficiently exact in most cases, under certain circumstances the deviation of the wave from sine shape becomes of importance, and with certain distortions it may not be pos- sible to replace the distorted wave by an equivalent sine wave, since the angle of phase displacement of the equivalent sine wave becomes indefinite. Thus it becomes desirable to investi- gate the distortion of the wave, its causes and its effects. Since, as stated before, any alternating wave can be repre- sented by a series of sine functions of odd orders, the inves- tigation of distortion of wave-shape resolves itself
CHAPTER XXV DISTORTION OF WAVE-SHAPE AND ITS CAUSES 232. In the preceding chapters we have considered the alter- nating currents and alternating e.m.fs. as sine waves or as replaced by their equivalent sine waves. While this is sufficiently exact in most cases, under certain circumstances the deviation ...
... m.f. a distorting effect will cause distortion of the current wave, while with a sine wave of current passing through the circuit, a dis- torting effect will cause higher harmonics of e.m.f. 233. In a conductor revolving with uniform velocity through a uniform and constant magnetic field, a sine wave of e.m.f. is generated. In a circuit with constant resistance and constant reactance, this sine wave of e.m.f. produces a sine wave of current. Thus distortion of the wave-shape or higher har- monics may be due to lack of uniformity of the velocity of the ...
... assing through the circuit, a dis- torting effect will cause higher harmonics of e.m.f. 233. In a conductor revolving with uniform velocity through a uniform and constant magnetic field, a sine wave of e.m.f. is generated. In a circuit with constant resistance and constant reactance, this sine wave of e.m.f. produces a sine wave of current. Thus distortion of the wave-shape or higher har- monics may be due to lack of uniformity of the velocity of the revolving conductor; lack of uniformity or pulsation of the magnetic field; pulsation of the resistance ...
... m.f. a distorting effect will cause distortion of the current wave, while with a sine wave of current passing through the circuit, a dis- torting effect will cause higher harmonics of e.m.f. 233. In a conductor revolving with uniform velocity through a uniform and constant magnetic field, a sine wave of e.m.f. is generated. In a circuit with constant resistance and constant reactance, this sine wave of e.m.f. produces a sine wave of current. Thus distortion of the wave-shape or higher har- monics may be due to lack of uniformity of the velocity of the revol ...
Concept CandidateHits In SectionStatus
Frequency12seeded
Ether5seeded
Light2seeded
Magnetic permeability1seeded
Term CandidateHits In SectionStatus
ether5seeded
effective resistance1source-located candidate
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theory-calculation-alternating-current-phenomena-fig-1721 180 Fig. 172. Even with an unsymmetrical distribution of the magnetic flux in the air-gap, the e.m.f. wave generated in a full-pitchline 29650
theory-calculation-alternating-current-phenomena-fig-173180 Fig. 173. magnetic reluctance, or its reciprocal, the magnetic reactance of the circuit. In consequence thereof the magnetism per field-line 29845
theory-calculation-alternating-current-phenomena-fig-178’ Fig. 178. tage drops with the further increase of current, and then rises again with the decreasing current, until at C, the intersectionline 31252
theory-calculation-alternating-current-phenomena-fig-1791 Fig. 179. flux and the current, therefore, cannot both be sine waves; if the magnetic flux and therefore the generated e.m.f. are sine waves,line 31517
theory-calculation-alternating-current-phenomena-fig-180-B Fig. 180. the e.m.f., e = J? sin </>, and a wattless component, i” , in quadra-line 31654
theory-calculation-alternating-current-phenomena-fig-181where Fig. 181. c„ = /a„2 + 6n^, 6„line 31840
theory-calculation-alternating-current-phenomena-fig-182\v Fig. 182. B. Sine Wave of Currentline 31959
theory-calculation-alternating-current-phenomena-fig-183y Fig. 183. As seen, with a sine wave of current traversing an iron-clad reactance, the e.m.f. wave is very greatly distorted, and theline 32214
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