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Susceptance

Susceptance is the quadrature component of admittance. In the same way reactance belongs to the wattless component of e.m.f. in the impedance view, susceptance belongs to the wattless component of current in the admittance view.

For electrostatic capacity, Steinmetz gives:

b=2πfCb = 2\pi f C

Modern notation often writes:

Y=G+jBY = G + jB

Steinmetz’s pages often use a different sign convention:

Y=gjbY = g - jb

The archive preserves the source convention first, then translates.

For:

Z=r+jxZ = r + jx

one useful Steinmetz-sign reconstruction is:

Y=rjxr2+x2Y = \frac{r - jx}{r^2 + x^2}

therefore:

g=rr2+x2,b=xr2+x2g = \frac{r}{r^2+x^2},\quad b = \frac{x}{r^2+x^2}

Susceptance keeps the current-side view of field storage visible. It is central for parallel circuits, dielectric circuits, line charging, and distributed capacity.

Ether-Field Interpretive Reading

Interpretive only: susceptance can be read as a measure of how readily a field-storage path accepts quadrature current. Steinmetz’s source language supports the admittance and wattless-current structure; it does not by itself prove a later ether-field ontology.

Generated evidence layer: this dossier is built from the processed concept concordance. Counts and snippets are OCR/PDF-text aids, not final quotations. Verify against scans before making exact claims.

220

Candidate occurrences tracked for this page.

8

Sources with at least one hit.

38

Sections, lectures, chapters, or report divisions to review.

Read this concept page through the linked source passages first. Use the dossier to locate Steinmetz’s wording, then add modern, mathematical, historical, and interpretive layers only with labels.

The strongest current source concentration is Theory and Calculation of Alternating Current Phenomena with 68 candidate hits across 9 sections.

The dossier is meant to turn a concept page into a research workbench: begin with Steinmetz’s source wording, then add modern interpretation, mathematical reconstruction, historical context, and any ether-field reading as separate layers.

susceptance, susceptances

Susceptance

SourceCandidate HitsSectionsConcepts represented
Theory and Calculation of Alternating Current Phenomena689Susceptance
Theory and Calculation of Alternating Current Phenomena588Susceptance
Theory and Calculation of Alternating Current Phenomena547Susceptance
Theory and Calculation of Electric Circuits162Susceptance
Theoretical Elements of Electrical Engineering124Susceptance
Theory and Calculation of Electric Apparatus63Susceptance
Theory and Calculation of Transient Electric Phenomena and Oscillations43Susceptance
Engineering Mathematics: A Series of Lectures Delivered at Union College22Susceptance
Chapter 10: Resistance And Reactance Of Transmission - 26 candidate hits

Source: Theory and Calculation of Alternating Current Phenomena (1916)

Location: lines 6993-9766 - Tracked concepts: Susceptance

Open source text - Open chapter workbench

... 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 in...
... unted inductive reactance, and decreased by a shunted con- densive reactance. Hence, for the purpose of investigation, the receiver circuit can be assumed to consist of two branches, a conductance, g, - the non-inductive part of the circuit - shunted by a susceptance, h, which can be varied without expenditure of energy. The two components of current...
Chapter 9: Resistance And Reactance Of Transmission Lines - 23 candidate hits

Source: Theory and Calculation of Alternating Current Phenomena (1900)

Location: lines 5334-6956 - Tracked concepts: Susceptance

Open source text - Open chapter workbench

... 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 incre...
... decreased by a shunted con- densance. Hence, for the purpose of investigation, the 84 ALTERNATING-CURRENT PHENOMENA. receiver circuit can be assumed to consist of two branches, a conductance, g, - the non-inductive part of the circuit, - shunted by a susceptance, b, which can be varied without expenditure of energy. The two components of current can t...
Chapter 9: Kbsistanci: And Kbactance Of Transmission Iine8 - 20 candidate hits

Source: Theory and Calculation of Alternating Current Phenomena (1897)

Location: lines 6371-8268 - Tracked concepts: Susceptance

Open source text - Open chapter workbench

... 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 increa...
... d by a shunted con- densance. Hence, for the purpose of investigation, the 84 AL TERN A TIXG-CURRENT PHENOMENA, [§ 68 receiver circuit can be assumed to consist of two branches, a conductance, g^ - the non-inductive part of the circuit, - shunted by a susceptance, by which can be varied without expenditure of energy. The two components of current can...
Chapter 7: Admittance, Conductance, Susceptance - 17 candidate hits

Source: Theory and Calculation of Alternating Current Phenomena (1900)

Location: lines 3132-3576 - Tracked concepts: Susceptance

Open source text - Open chapter workbench

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 ...
... series 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 ADMITTANCE, CONDUCTANCE, SUSCEPTANCE. 53 joint conductance of a number of parallel-connected conduc~ tances is equal to the sum...
Chapter 8: Admittance, Conductance, Susceptance - 17 candidate hits

Source: Theory and Calculation of Alternating Current Phenomena (1916)

Location: lines 4088-4673 - Tracked concepts: Susceptance

Open source text - Open chapter workbench

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 ...
... tance of a number of series-connected resistances is equal to the sum of the individual resistances; the joint conduct- ance of a number of parallel-connected conductances is equal to the sum of the individual conductances. 64 ADMITTANCE, CONDUCTANCE, SUSCEPTANCE 55 49. In alternating-current circuits, instead of the term resist- ance we have the term...
Chapter 7: Admittance, Conductance, Susceftance - 15 candidate hits

Source: Theory and Calculation of Alternating Current Phenomena (1897)

Location: lines 3546-3871 - Tracked concepts: Susceptance

Open source text - Open chapter workbench

... 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...
... nent ^, which represents the coefficient of current in quadrature with the K.M.F., or wattless com- ponent of current, bE, g may be called the conductance^ and b the susceptanccy of the circuit. Hence the conductance, g^ is the energy component, and the susceptance, by the wattless component, of the admittance, Y = g -\-jby while the numerical value o...
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