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Chapter 24: Symbolic Representation Of General Alternating Waves

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1900
Section IDtheory-calculation-alternating-current-phenomena-1900-chapter-24
Locationlines 22449-23642
Statuscandidate
Word Count3142
Equation Candidates In Section0
Figure Candidates In Section0
Quote Candidates In Section0
CHAPTER XXIV. SYMBOLIC REPRESENTATION OF GENERAL ALTERNATING WAVES. 253. The vector representation, A = a1 +y<zu = a (cos a -\-j sin d) of the alternating wave, A — a0 cos (<£ — a) applies to the sine wave only. The general alternating wave, however, contains an in- finite series of terms, of odd frequencies, A = Al cos (<£ — #1) 4- Az cos (3 <£ — #3) + A& cos (5 <£ — #5) -f thus cannot be directly represented by one complex vector quantity. The replacement of the general wave by its equivalent sine wave, as before discussed, that is a sine wave of equal effective intensity and equal power, while sufficiently accu- rate in many cases, completely fails in other cases, espe- cially in circuits containing capacity, or in circuits containing
CHAPTER XXIV. SYMBOLIC REPRESENTATION OF GENERAL ALTERNATING WAVES. 253. The vector representation, A = a1 +y<zu = a (cos a -\-j sin d) of the alternating wave, A — a0 cos (<£ — a) applies to the sine wave only. The general alternating wave, however, contains an in- finite series of terms, of odd frequencies, A = Al cos (<£ — #1) ...
... antity. The replacement of the general wave by its equivalent sine wave, as before discussed, that is a sine wave of equal effective intensity and equal power, while sufficiently accu- rate in many cases, completely fails in other cases, espe- cially in circuits containing capacity, or in circuits containing periodically (and in synchronism with the wave) varying resistance or reactance (as alternating arcs, reaction ma- chines, synchronous induction motors, oversaturated mag- netic circuits, etc.). Since, however, the individual harmonics of the gen ...
... ine wave of equal effective intensity and equal power, while sufficiently accu- rate in many cases, completely fails in other cases, espe- cially in circuits containing capacity, or in circuits containing periodically (and in synchronism with the wave) varying resistance or reactance (as alternating arcs, reaction ma- chines, synchronous induction motors, oversaturated mag- netic circuits, etc.). Since, however, the individual harmonics of the general alternating wave are independent of each other, that is, all products of different harmonics vanish, e ...
... p- resent different frequencies, and thus cannot be combined. The general wave of E.M.F. is thus represented by, the general wave of current by, if, is the impedance of the fundamental harmonic, where xm is that part of the reactance which is proportional to the frequency (inductance, etc.). x0 is that part of the reactance which is independent of the frequency (mutual induction, synchronous motion, etc.). xc is that part of the reactance which is inversely pro- portional to the frequency (capacity, etc.). The impedance for the nth harmo ...
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Ether2seeded
Light2seeded
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ether2seeded
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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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  • Radiation / light: Radiation and wave language can invite ether-field comparison, but source wording, modern radiation theory, and speculative synthesis must stay separated.
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