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Chapter 7: Admittance, Conductance, Susceptance

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1900
Section IDtheory-calculation-alternating-current-phenomena-1900-chapter-07
Locationlines 3132-3576
Statuscandidate
Word Count1254
Equation Candidates In Section25
Figure Candidates In Section0
Quote Candidates In Section0
CHAPTER VII. ADMITTANCE, CONDUCTANCE, SUSCEPTANCE. 38. If in a continuous-current circuit, a number of resistances, ?\, r%, r3, . . . are connected in series, their joint resistance, R, is the sum of the individual resistances If, however, a number of resistances are connected in multiple or in parallel, their joint resistance, R, cannot be expressed in a simple form, but is represented by the expression : — = J_ _l_ JL + J_ + /*! /*2 ^3 Hence, in the latter case it is preferable to introduce, in- stead of the term resistance, its reciprocal, or inverse value, the term conductance, g = 1 / r. If, then, a number of con- ductances, g^, g^, gz, . . . are connected in parallel, their joint conductance is the sum of the individual conductances, or
CHAPTER VII. ADMITTANCE, CONDUCTANCE, SUSCEPTANCE. 38. If in a continuous-current circuit, a number of resistances, ?\, r%, r3, . . . are connected in series, their joint resistance, R, is the sum of the individual resistances If, however, a number of resistances are connected in multiple or in ...
CHAPTER VII. ADMITTANCE, CONDUCTANCE, SUSCEPTANCE. 38. If in a continuous-current circuit, a number of resistances, ?\, r%, r3, . . . are connected in series, their joint resistance, R, is the sum of the individual resistances If, however, a number of resistances are connected in multiple or in parallel, their joint resistance, R, cannot be expressed in a simple form, but is represented by the expression : — = J_ _l_ JL + J_ + /*! /*2 ...
... e of a number of series-connected resis- tances is equal to the sum of the individual resistances ; the ADMITTANCE, CONDUCTANCE, SUSCEPTANCE. 53 joint conductance of a number of parallel-connected conduc~ tances is equal to the sum of the individual conductances. 39. In alternating-current circuits, instead of the term resistance we have the term impedance, Z = r —Jx, with its two components, the resistance, r, and the reactance, x, in the formula of Ohm's law, E = IZ. The resistance, r, gives the component of E.M.F. in phase with the current, or the energy c ...
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Candidate IDOCR / PDF-Text CandidateSource Location
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0163resistances, ?, r%, r3, … are connected in series, theirline 3137
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0164the term conductance, g = 1 / r. If, then, a number of con-line 3151
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0165ADMITTANCE, CONDUCTANCE, SUSCEPTANCE. 53line 3168
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0166y = Vr1 + P ;line 3232
theory-calculation-alternating-current-phenomena-1900-eq-candidate-016740. As shown, the term admittance implies resolvingline 3240
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0168reactance x = 0, or in continuous-current circuits, is theline 3251
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0169Again, only in circuits with zero resistance (r = 0) isline 3254
theory-calculation-alternating-current-phenomena-1900-eq-candidate-01701.) If r = QO , or x = oo , since in this case no currentline 3260
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  • Impedance / reactance: Translate historical opposition terms into modern impedance, admittance, conductance, susceptance, and complex-plane notation.
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