Susceptance
Steinmetz Usage
Section titled “Steinmetz Usage”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:
Modern Equivalent
Section titled “Modern Equivalent”Modern notation often writes:
Steinmetz’s pages often use a different sign convention:
The archive preserves the source convention first, then translates.
Mathematical Meaning
Section titled “Mathematical Meaning”For:
one useful Steinmetz-sign reconstruction is:
therefore:
Why It Matters
Section titled “Why It Matters”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.
Related Pages
Section titled “Related Pages”Reader Synthesis
Section titled “Reader Synthesis”What Steinmetz Is Doing Here
The processed corpus gives this concept a source trail across Steinmetz’s books and lectures. Read the source distribution first, because the meaning often changes between radiation, AC calculation, apparatus, and transients.
The current strongest source route is Theory and Calculation of Alternating Current Phenomena, with 68 candidate hits across 9 sections.
Modern Translation
Translate the older wording into modern electrical-engineering language only after the source location is visible.
This page currently tracks 220 candidate occurrences across 8 sources and 38 sections.
Mathematical And Visual Route
Use the linked equation atlas and source formula maps to decide whether this concept has a mathematical layer, a diagrammatic layer, or mainly a terminology layer.
Use the math/visual bridge lower on this page to jump into formula families, source visual maps, and candidate figure leads.
Interpretive Boundary
Interpretive readings are welcome in this archive only when they are labeled and separated from Steinmetz’s explicit wording.
Layer labels stay active: source claim, modern equivalent, mathematical reconstruction, historical note, and interpretive reading are not interchangeable.
Fast Reading Path For Susceptance
Section titled “Fast Reading Path For Susceptance”| Passage | Hits | Location | Open |
|---|---|---|---|
| Chapter 10: Resistance And Reactance Of Transmission Theory and Calculation of Alternating Current Phenomena | 26 | lines 6993-9766 | read - research review |
| Chapter 9: Resistance And Reactance Of Transmission Lines Theory and Calculation of Alternating Current Phenomena | 23 | lines 5334-6956 | read - research review |
| Chapter 9: Kbsistanci: And Kbactance Of Transmission Iine8 Theory and Calculation of Alternating Current Phenomena | 20 | lines 6371-8268 | read - research review |
| Chapter 7: Admittance, Conductance, Susceptance Theory and Calculation of Alternating Current Phenomena | 17 | lines 3132-3576 | read - research review |
Research Position
Section titled “Research Position”- Tracked vocabulary: Susceptance.
- Concordance: Susceptance.
- Source discipline: the table above is for reading and navigation; exact quotation still requires scan verification.
- Editorial rule: expand this page by promoting scan-checked passages, equations, and diagrams from the linked workbench pages, not by adding unsourced generalizations.
Source-Grounded Dossier
Section titled “Source-Grounded Dossier”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.
Candidate occurrences tracked for this page.
Sources with at least one hit.
Sections, lectures, chapters, or report divisions to review.
What The Current Corpus Shows
Section titled “What The Current Corpus Shows”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 reading path: begin with Steinmetz’s source wording, then use the research links only when you need candidate counts, snippets, mathematical reconstruction, historical context, or interpretive layers.
Terms And Aliases Tracked
Section titled “Terms And Aliases Tracked”susceptance, susceptances
Concordance Records
Section titled “Concordance Records”Source Distribution
Section titled “Source Distribution”Priority Passages To Read
Section titled “Priority Passages To Read”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
... 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
... 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
... 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
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
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
... 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...Reading Layers To Build Out
Section titled “Reading Layers To Build Out”| Layer | What to add next |
|---|---|
| Steinmetz wording | Pull exact source passages only after scan verification; keep OCR text labeled until then. |
| Modern engineering reading | Translate the source usage into present electrical-engineering or physics language without erasing the older vocabulary. |
| Mathematical layer | Link equations, variables, diagrams, and worked examples when the concept has formula candidates. |
| Historical layer | Identify whether the term is still used, renamed, absorbed into modern theory, or historically obsolete. |
| Ether-field interpretation | Keep interpretive readings separate from Steinmetz’s explicit claim and from modern physics. |
| Open questions | Record places where the concordance suggests a lead but the scan or edition has not yet been checked. |
Next Editorial Actions
Section titled “Next Editorial Actions”- Open the highest-priority source-text passages above and verify the wording against scans.
- Promote exact definitions, equations, diagrams, and hidden-gem passages into this page with source references.
- Add related concept links, equation pages, and diagram pages once the evidence is scan checked.
- Keep speculative or Wheeler-style readings in explicitly labeled interpretation blocks.
Math And Visual Evidence Map
Section titled “Math And Visual Evidence Map”Generated bridge: this section crosslinks the concept page with the formula atlas, figure atlas, source visual maps, and source formula maps. It is a routing layer, not final interpretation.
Formula candidates routed to this concept.
Figure candidates routed to this concept.
Modern guide diagrams related to this concept.
Formula Families To Review
Section titled “Formula Families To Review”Impedance, Reactance, And Admittance
Source Maps For This Concept
Section titled “Source Maps For This Concept”theory-calculation-alternating-current-phenomena visuals - theory-calculation-alternating-current-phenomena formulas - theory-calculation-alternating-current-phenomena-1900 visuals - theory-calculation-alternating-current-phenomena-1900 formulas - theory-calculation-alternating-current-phenomena-1897 visuals - theory-calculation-alternating-current-phenomena-1897 formulas - theory-calculation-electric-circuits visuals - theory-calculation-electric-circuits formulas - theoretical-elements-electrical-engineering visuals - theoretical-elements-electrical-engineering formulas - theory-calculation-electric-apparatus visuals - theory-calculation-electric-apparatus formulas
Related Modern Guide Diagrams
Section titled “Related Modern Guide Diagrams”Modern reading aid for conductance, susceptance, and reciprocal impedance.
admittance, conductance, susceptance, symbolic-method
Highest-Priority Formula Leads
Section titled “Highest-Priority Formula Leads”| Candidate | Family | OCR/PDF text | Routes |
|---|---|---|---|
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0240strong-formula-candidate | symbolic-ac | is r - j (x -f x0} = r = .6, x + x0 = 0, and tan S>0 = 0 ; | source research review |
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0161strong-formula-candidate | symbolic-ac | but E = E^y I^E^j z. If x^ > - 2,t-, it raises, if ;r < - 2 jr, | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0281strong-formula-candidate | inductance-capacity | Then, if E0 = impressed E.M.F.,- | source research review |
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0176strong-formula-candidate | symbolic-ac | is r - y (.r + ;r^) = r = .6, x + x^ = 0, and tan w^ = ; | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0219strong-formula-candidate | symbolic-ac | Z -jx0 = r-j(x +#e). | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0231strong-formula-candidate | symbolic-ac | circuit •- z= 1 Qj r = 1>0> x= 0 (Curve j) | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0244strong-formula-candidate | inductance-capacity | for the constant impressed E.M.F., E0 = 100 ; for the con- | source research review |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0264strong-formula-candidate | symbolic-ac | &Q = ro JXoi ZQ = V f0 -j- Xo , | source research review |
Highest-Priority Figure Leads
Section titled “Highest-Priority Figure Leads”| Candidate | Caption lead | Section | Routes |
|---|---|---|---|
theory-calculation-alternating-current-phenomena-1900-fig-038Fig. 38 | Er Er0 Fig. 38. and the current is, /= | Chapter 8: Circuits Containing Resistance, Inductance, And Capacity | source research review |
theory-calculation-alternating-current-phenomena-1900-fig-039Fig. 39 | E Fig. 39. Z-jx0 r—j(x + x0}‘ | Chapter 8: Circuits Containing Resistance, Inductance, And Capacity | source research review |
theory-calculation-alternating-current-phenomena-1900-fig-040Fig. 40 | of reactance in series in a non-inductive circuit is, for small Fig. 40. values of reactance, independent of the sign, but propor- | Chapter 8: Circuits Containing Resistance, Inductance, And Capacity | source research review |
theory-calculation-alternating-current-phenomena-fig-049Fig. 49 | 7 1.8 Fig. 49. The sign in the complex expression of admittance is always opposite to that of impedance; this is obvious, since if the cur- | Chapter 8: Admittance, Conductance, Susceptance | source research review |
theory-calculation-alternating-current-phenomena-fig-100Fig. 100 | JTTTTTTTTTTTTTTTTTTTTTTT- Fig. 100. In this case the intensity as well as phase of the current, and consequently of the counter e.m.f. of inductive reactance and | Chapter 15: Distributed Capacity, Inductance, Resistance, And Leakage | source research review |
theory-calculation-alternating-current-phenomena-fig-101Fig. 101 | iEo Fig. 101. Denoting in Fig. 101. | Chapter 15: Distributed Capacity, Inductance, Resistance, And Leakage | source research review |
theory-calculation-alternating-current-phenomena-fig-117Fig. 117 | of admittance Yq. Thus, double transformation will be represented by diagram. Fig. 117. With this the discussion of the alternate-current transformer ends, by becoming identical with that of a divided circuit con- | Chapter 17: The Alternating-Current Transformer | source research review |
theory-calculation-alternating-current-phenomena-fig-144Fig. 144 | nal admittance of the second machine. Fig. 144. Then, er + e’r = al^• | Chapter 23: Synchronizing Alternators | source research review |