Susceptance Concordance
Susceptance
Section titled “Susceptance”Concordance status: generated from processed OCR/PDF text. Treat these as source-location aids until each passage is checked against the scan.
220 hits
Total text matches across processed Steinmetz sections.
8 sources
Sources containing at least one matched alias.
38 sections
Chapters, lectures, sections, or report divisions with matches.
Matched Aliases
Section titled “Matched Aliases”susceptance, susceptances
Source Distribution
Section titled “Source Distribution”| Source | Hits | Sections |
|---|---|---|
| Theory and Calculation of Alternating Current Phenomena | 68 | 9 |
| Theory and Calculation of Alternating Current Phenomena | 58 | 8 |
| Theory and Calculation of Alternating Current Phenomena | 54 | 7 |
| Theory and Calculation of Electric Circuits | 16 | 2 |
| Theoretical Elements of Electrical Engineering | 12 | 4 |
| Theory and Calculation of Electric Apparatus | 6 | 3 |
| Theory and Calculation of Transient Electric Phenomena and Oscillations | 4 | 3 |
| Engineering Mathematics: A Series of Lectures Delivered at Union College | 2 | 2 |
Section Hits
Section titled “Section Hits”Representative Source Snippets
Section titled “Representative Source Snippets”Chapter 10: Resistance And Reactance Of Transmission - 26 hit(s)
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... s, by varying the admittance, Y = g — jh, of the receiver circuit. The conductance, g, of the receiver circuit depends upon the consumption of power — that is, upon the load on the circuit — and thus cannot be varied for the purpose of regu- lation. Its susceptance, b, however, can be changed bj' shunt- ing the circuit with a reactance, and will be increased by a shunted inductive reactance, and decreased by a shunted con- densive reactance. Hence, for the purpose of investigation, the receiver circuit can be assume ...Chapter 9: Resistance And Reactance Of Transmission Lines - 23 hit(s)
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... by varying the admittance, Y = g -f jb, of the receiver circuit. The conductance, gy of the receiver circuit depends upon the consumption of power, — that is, upon the load on the circuit, — and thus cannot be varied for the purpose of reg- ulation. Its susceptance, b, however, can be changed by shunting the circuit with a reactance, and will be increased by a shunted inductance, and decreased by a shunted con- densance. Hence, for the purpose of investigation, the 84 ALTERNATING-CURRENT PHENOMENA. receiver circ ...Chapter 9: Kbsistanci: And Kbactance Of Transmission Iine8 - 20 hit(s)
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... by varying the admittance, Y = g + Jb, of the receiver circuit. The conductance, g, of the receiver circuit depends upon the consumption of power, — that is, upon the load on the circuit, — and thus cannot be varied for the purpose of reg- ulation. Its susceptance, by however, can be changed by shunting the circuit with a reactance, and will be increased by a shunted inductance, and decreased by a shunted con- densance. Hence, for the purpose of investigation, the 84 AL TERN A TIXG-CURRENT PHENOMENA, [§ 68 rece ...Chapter 8: Admittance, Conductance, Susceptance - 17 hit(s)
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CHAPTER VIII ADMITTANCE, CONDUCTANCE, SUSCEPTANCE 48. If in a continuous-current circuit, a number of resistances, Ti, r2, ?'3, . . ., are connected in series, their joint resistance, R, is the sum of the individual resistances, K = ri + r2 + ra + . . . If, however, a number of resistances are connecte ...Chapter 7: Admittance, Conductance, Susceptance - 17 hit(s)
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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 parall ...Chapter 7: Admittance, Conductance, Susceftance - 15 hit(s)
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... connection, and the use of the reciprocal term conductance in parallel connections ; therefore, The joint resistance of a number of series -connected resis- tances is equal to the sum of the individual resistances ; the § 30] 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 componen ...Chapter 15: Constant-Voltage Series Operation - 14 hit(s)
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... on the same circuit, from constant-voltage supply. 156. Let n lamps of voltage, ei, and current, ii, thus conductance ff = j^ (1) ei be connected in series into a circuit of supply voltage, eo = nei (2) and each lamp be shunted by a reactance of susceptance, b. In each consuming device, comprising lamp and reactance, the admittance thus is, vectorially, Yi^=g^jb (3) if, then, / = current in the series circuit, the voltage consumed by the device comprising lamp and reactance, thus is in a consuming de ...Chapter 11: Fouoault Or Eddy 0Ubbent8 - 10 hit(s)
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... and the E.M.F. induced in the primary circuit by the secon- dary current, /^ is £= ^^/; or, expanded, (V + ^V n^ + xi') ' Hence, ^ = —-^ — ^- = effective conductance of mutual inductance ; r,» + jf« — »f », Xi b = — ^-^^^ — ■* = effective susceptance of mutual inductance. The susceptance of mutual inductance is negative, or of opposite sign from the susceptance of self-inductance. Or, Mutual itidtutance consumes energy and decreases the self- inductatice. Dielectric and Electrostatic Phenomena, ...Chapter 14: Dielectric Losses - 9 hit(s)
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... very low) and specific capacity or permittivity k, if: I = thickness of the dielectric, A = area or cross-section, e = impressed alternating-current voltage, effective value, the dielectric capacity of the material is: JcA ^ ~~ I and the capacity susceptance: 152 ALTERNATING-CURRENT PHENOMENA hence the current passing through the dielectric as capacity- current or "displacement current," is: ^ ^^ 2 7r//cA iQ = eo — 2 TTjCe = — -. — e The conductance of the dielectric is: yA hence, the current, con ...Theory Section 17: Impedance and Admittance - 8 hit(s)
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... impedance z — - with its components, I? the resistance and reactance, its reciprocal can be introduced. e " z ' which is called the admittance. The components of the admittance are called the conduc- tance and the susceptance. Resolving the current i into a power component i\ in phase with the e.m.f. and a wattless component iz in quadrature with the e.m.f., the quantity i\_ _ power current, or current in phase with e.m.f. e e.m.f. . = ...Chapter 37: Quarter-Phase System - 6 hit(s)
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... ents, 112 admittance, 137 coefficient, 138 conductance, 137 in conductor, 144 loss with distorted wave, 377 of power, 136 Effective circuit constants, 168 Effective circuit conductance, 111 power, 180 reactance, 112 resistance, 2, 5, 9, 111 susceptance, 112 value of wave, 11 in polar diagram, 53 Efficiency of circuit with inductive line, 88, 95 induction motor, 234 Electrostatic, see Dielectric E.m.f. of self-induction, 123 Energy distance of dielectric field, 165 flow in polyphase system, 406 an ...Chapter 11: Foucault Or Eddy Currents - 6 hit(s)
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... ircuit by the secon- dary current, 7l is or, expanded, Y zr j~. 2 xm^ JXm 2 _i_ r 2 r2 i JT T^ ^i "l " •* 2 Hence, the E.M.F. consumed thereby effective resistance of mutual inductance ; ^ = effective reactance of mutual inductance. The susceptance of mutual inductance is negative, or of opposite sign from the reactance of self-inductance. Or, Mutual inductance consumes energy and decreases the self- inductance. Dielectric and Electrostatic Phenomena. 98. While magnetic hysteresis and eddy curren ...Chapter 12: Effective Resistance And Reactance - 4 hit(s)
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... ch way as to represent a larger expenditure of power. In dealing with alternating-current circuits, it is necessarj-, therefore, to substitute everywhere the values "effective re- sistance," "effective reactance," "effective conductance," and "effective susceptance," to make the calculation applicable to general alternating-current circuits, such as inductive reactances containing iron, etc. While the true ohmic resistance is a constant of the circuit, depending only upon the temperature, but not upon the e.m.f., ...Chapter 10: F - 4 hit(s)
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... nductance of the circuit. § 733 EFFECTIVE RESISTANCE AND REACTANCE. 105 In the same way, the value, _ Wattless component of E.M.F. Total current is the effective reactance, and , _ Wattless compo nent of current ■" Total E.M.F. is the effective susceptance of the circuit. While the true ohmic resistance represents the expendi- ture of energy as heat inside of the electric conductor by a current of uniform density, the effective resistance repre- sents the total expenditure of energy. Since, in an alterna ...Chapter 10: Effective Resistance And Reactance - 4 hit(s)
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... ffective conductance of the circuit. EFFECTIVE RESISTANCE AND REACTANCE. 105 In the same way, the value, _ Wattless component of E.M.F. Total current is the effective reactance, and , _ Wattless component of current TotafE.M.F. is the effective susceptance of the circuit. While the true ohmic resistance represents the expendi- ture of energy as heat inside of the electric conductor by a current of uniform density, the effective resistance repre- sents the total expenditure of energy. Since, in an alterna ...Chapter 13: Distributed Capacity, Inductance, Resistance, And Leakage - 4 hit(s)
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... imation of one ; viz., three condensers shunted across the line. 109. A.} Line capacity represented by one condenser shunted across middle of line. Let — Y = g + j b = admittance of receiving circuit ; z = r — j x = impedance of line ; be = condenser susceptance of line. DISTRIBUTED CAPACITY. 161 Denoting, in Fig. 84, the E.M.F., viz., current in receiving circuit by £, It the E.M.F. at middle of line by £', the E.M.F., viz., current at generator by E0)I0\ If We have, Fig. 84. Capacity Shunted ...Chapter 1: Speed Control Of Induction Motors - 4 hit(s)
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... agnetic circuit, are independent of the frequency, and vary relatively little with the magnetic density and thus the current, over a wide range,1 thus may approxi- mately be assumed as constant. That is, the hysteretic con- ductance is proportional to the susceptance : g' = V tan a. ((>) Thus, the exciting admittance, of a closed magnetic circuit of negligible resistance and negligible eddy-current losses, at the frequency of slip, «, is given by: Y' = g' - jb' = V (tan a - j) = - J = (tan a - j) (7) 8 8 8 1 ...Chapter 15: Distributed Capacity, Inductance, Resistance, And Leakage - 3 hit(s)
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... 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 general, r, x, g, b, are not constants of the circuit, but depend — besides upon the frequency — more or less upon e.m.f., curr ...