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Dielectric Loss

In the dielectric-loss chapter, Steinmetz treats the dielectric path with an admittance language. The dielectric may carry a capacity current, but it can also consume real power through leakage, dielectric hysteresis, corona, and related loss effects.

Modern engineering may describe these effects as:

  • dielectric loss,
  • leakage conductance,
  • loss tangent,
  • equivalent parallel conductance,
  • equivalent series resistance,
  • insulation loss.

The dielectric has an electrostatic capacity:

CC

and a capacity susceptance:

b=2πfCb = 2\pi f C

The real loss path is represented by conductance:

gg

Together they form a dielectric admittance model.

This is one of the archive’s key field-language bridges. Steinmetz does not treat a dielectric as a perfect empty insulator. It has storage, leakage, loss, and frequency behavior.

Modern Electrical Engineering Interpretation

Modern capacitor models often hide dielectric behavior behind ideal capacitance plus ESR or loss tangent. Steinmetz’s treatment keeps the dielectric material and its field behavior closer to the surface.

Ether-Field Interpretive Reading

Interpretive only: a Wheeler-style reading may treat dielectric loss as field compression/storage with lag, leakage, or internal dissipation. The source-grounded layer is that Steinmetz explicitly models dielectric capacity current and real-power loss in dielectric media.

What Steinmetz Is Doing Here

Dielectric terms lead from capacity and insulation into field stress, loss, and stored electric energy.

The current strongest source route is Theory and Calculation of Alternating Current Phenomena, with 365 candidate hits across 33 sections.

Modern Translation

Modern readers can connect this to capacitance, dielectric field, permittivity, loss angle, insulation stress, and displacement current.

This page currently tracks 1569 candidate occurrences across 14 sources and 140 sections.

Mathematical And Visual Route

Follow capacity, condensive reactance, susceptance, charging current, energy storage, and frequency dependence.

Use the math/visual bridge lower on this page to jump into formula families, source visual maps, and candidate figure leads.

Interpretive Boundary

This is a legitimate place to compare dielectric-field language with ether-field vocabulary, provided the comparison is labeled.

Layer labels stay active: source claim, modern equivalent, mathematical reconstruction, historical note, and interpretive reading are not interchangeable.

PassageHitsLocationOpen
Chapter 14: Dielectric Losses
Theory and Calculation of Alternating Current Phenomena
217lines 14334-15409read - research review
Lecture 2: The Electric Field
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients
114lines 1003-1658read - research review
Lecture 2: The Electric Field
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients
114lines 883-1530read - research review
Theory Section 19: Fields of Force
Theoretical Elements of Electrical Engineering
81lines 7737-7990read - research review
  • Tracked vocabulary: Dielectricity, Dielectric Field, Dielectric constant.
  • Concordance: Dielectricity - Dielectric Field - Dielectric constant.
  • 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.

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.

1569

Candidate occurrences tracked for this page.

14

Sources with at least one hit.

140

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 365 candidate hits across 33 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.

dielectric, dielectricity, displacement, displacement current, electrostatic, dielectric field, dielectrics, Dielectric constant, dielectric-constant

Dielectricity - Dielectric Field - Dielectric constant

Chapter 14: Dielectric Losses - 217 candidate hits

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

Location: lines 14334-15409 - Tracked concepts: Dielectric Field, Dielectricity

CHAPTER XIV DIELECTRIC LOSSES Dielectric Hysteresis 116. Just as magnetic hysteresis and eddy currents give a power component in the inductive reactance, as "effective resistance," so the energy losses in the dielectric lead to a power component in the condensive reactance, ...
CHAPTER XIV DIELECTRIC LOSSES Dielectric Hysteresis 116. Just as magnetic hysteresis and eddy currents give a power component in the inductive reactance, as "effective resistance," so the energy losses in the dielectric lead to a power component in the condensive reactance, which may be repre- ...
Lecture 2: The Electric Field - 114 candidate hits

Source: Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients (1914)

Location: lines 1003-1658 - Tracked concepts: Dielectric Field, Dielectricity

... hile power flows through the conductors A, power is con- sumed in these conductors by JV[ conversion into heat, repre- sented by ^2r. This, however, Fig. 7. is not all, but in the space surrounding the conductor cer- tain phenomena occur: magnetic and electrostatic forces appear. Fig. 8. - Electric Field of Conductor. The conductor is surrounded by a...
... wn in Fig. 8. By the return conductor, the circles 10 THE ELECTRIC FIELD. 11 are crowded together between the conductors, and the magnetic field consists of eccentric circles surrounding the conductors, as shown by the drawn lines in Fig. 9. An electrostatic, or, as more properly called, dielectric field, issues from the conductors, that is, a dielect...
Lecture 2: The Electric Field - 114 candidate hits

Source: Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients (1911)

Location: lines 883-1530 - Tracked concepts: Dielectric Field, Dielectricity

... While power flows through the conductors A, power is con- sumed in these conductors by conversion into heat, repre- sented by i?r. This, however, Fig. 7. is not all, but in the space surrounding the conductor cer- tain phenomena occur: magnetic and electrostatic forces appear. Fig. 8. - Electric Field of Conductor. The conductor is surrounded by a mag...
... wn in Fig. 8. By the return conductor, the circles 10 THE ELECTRIC FIELD. 11 are crowded together between the conductors, and the magnetic field consists of eccentric circles surrounding the conductors, as shown by the drawn lines in Fig. 9. An electrostatic, or, as more properly called, dielectric field, issues from the conductors, that is, a dielect...
Theory Section 19: Fields of Force - 81 candidate hits

Source: Theoretical Elements of Electrical Engineering (1915)

Location: lines 7737-7990 - Tracked concepts: Dielectric Field, Dielectricity

... e earth, and water to run down hill - and this space thus is a field of gravitational force, the earth the gram- motive force. In the space surrounding conductors having a high potential difference, we observe a field of dielectric force, that is, electro- static or dielectric forces are exerted, and the potential difference between the conductors is...
... is space thus is a field of gravitational force, the earth the gram- motive force. In the space surrounding conductors having a high potential difference, we observe a field of dielectric force, that is, electro- static or dielectric forces are exerted, and the potential difference between the conductors is the electromotive force of the dielectric fi...
Lecture 10: Continual And Cumulative Oscillations - 60 candidate hits

Source: Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients (1914)

Location: lines 6804-8485 - Tracked concepts: Dielectric Field, Dielectricity

... enon by which the stored energy readjusts itself to a change of circuit conditions. In an oscilla- tory transient, the difference of stored energy of the previous and the after condition of the circuit, at a circuit change, oscillates between magnetic and dielectric energy. As there always must be some energy dissipation in the circuit, the oscillatin...
... hen, with an overlap of successive oscillations, no dead period occurs, during which the energy, which oscillates during the next wave train, is supplied to the line, this energy must be supplied during the oscillation, that is, there must be such a phase displacement or lag within the oscil- lation, which gives a negative energy cycle, or reversed hy...
Chapter 1: The Constants Of The Electric Circuit - 59 candidate hits

Source: Theory and Calculation of Transient Electric Phenomena and Oscillations (1909)

Location: lines 1317-1992 - Tracked concepts: Dielectric Field, Dielectric constant, Dielectricity

... rostatic actions. The magnetic action is a maximum in the direction concen- tric, or approximately so, to the conductor. That is, a needle- shaped magnetizable body, as an iron needle, tends to set itself in a direction concentric to the conductor. The electrostatic action has a maximum in a direction radial, or approximately so, to the conductor. Tha...
... etizable body, as an iron needle, tends to set itself in a direction concentric to the conductor. The electrostatic action has a maximum in a direction radial, or approximately so, to the conductor. That is, a light needle- shaped conducting body, if the electrostatic component of the field is powerful enough, tends to set itself in a direction radial...
LayerWhat to add next
Steinmetz wordingPull exact source passages only after scan verification; keep OCR text labeled until then.
Modern engineering readingTranslate the source usage into present electrical-engineering or physics language without erasing the older vocabulary.
Mathematical layerLink equations, variables, diagrams, and worked examples when the concept has formula candidates.
Historical layerIdentify whether the term is still used, renamed, absorbed into modern theory, or historically obsolete.
Ether-field interpretationKeep interpretive readings separate from Steinmetz’s explicit claim and from modern physics.
Open questionsRecord places where the concordance suggests a lead but the scan or edition has not yet been checked.
  1. Open the highest-priority source-text passages above and verify the wording against scans.
  2. Promote exact definitions, equations, diagrams, and hidden-gem passages into this page with source references.
  3. Add related concept links, equation pages, and diagram pages once the evidence is scan checked.
  4. Keep speculative or Wheeler-style readings in explicitly labeled interpretation blocks.

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.

855

Formula candidates routed to this concept.

59

Figure candidates routed to this concept.

1

Modern guide diagrams related to this concept.

Inductance, Capacity, And Stored Energy - Magnetism, Hysteresis, And Core Loss - Power, Energy, Work, And Efficiency

Magnetic And Dielectric Energy Storage

Modern reading aid for Steinmetz’s paired magnetic-field and dielectric-field language.

dielectric-field, magnetic-field, energy-storage

Open SVG - recreated visual index

CandidateFamilyOCR/PDF textRoutes
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0195
strong-formula-candidate
transients-oscillationi = io cos (0 - 7) = io cos 7 cos <j> + i0 sin 7 sinsource
research review
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0240
strong-formula-candidate
symbolic-acis r - j (x -f x0} = r = .6, x + x0 = 0, and tan S>0 = 0 ;source
research review
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0220
strong-formula-candidate
transients-oscillationif = 140 cos 0.2 1 - 80 sin 0.2 1,source
research review
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0161
strong-formula-candidate
symbolic-acbut 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-0281
strong-formula-candidate
inductance-capacityThen, if E0 = impressed E.M.F.,-source
research review
electric-discharges-waves-impulses-1914-eq-candidate-0135
strong-formula-candidate
transients-oscillation(S!,J = 20,000 lines per cm^. *source
research review
electric-discharges-waves-impulses-1914-eq-candidate-0159
strong-formula-candidate
transients-oscillationT = 2.92 - { 9.21 log’^ , ,\ . + .921 log’^ i ’ ^ ^source
research review
electric-discharges-waves-impulses-1914-eq-candidate-0162
strong-formula-candidate
transients-oscillationdivision with log^^e = .4343.source
research review
CandidateCaption leadSectionRoutes
electric-discharges-waves-impulses-1914-fig-003
Fig. 3
G O Fig. 3. the stored energy has to be supplied from the source of power; that is, for a short time power, in supplying the stored energy, flows notLecture 1: Nature And Origin Of Transientssource
research review
theory-calculation-alternating-current-phenomena-fig-065
Fig. 65
loss of power. Fig. 65. Then, if Eo = impressed e.m.f., the current in receiver circuit isChapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactancesource
research review
theory-calculation-alternating-current-phenomena-fig-096
Fig. 96
^ m Fig. 96. )JChapter 14: Dielectric Lossessource
research review
theory-calculation-alternating-current-phenomena-fig-097
Fig. 97
’ m Fig. 97. throughout the field section, but the voltage gradient in theChapter 14: Dielectric Lossessource
research review
theory-calculation-alternating-current-phenomena-fig-098
Fig. 98
do so. Fig. 98. Fig. 99.Chapter 14: Dielectric Lossessource
research review
theory-calculation-alternating-current-phenomena-fig-099
Fig. 99
Fig. 98. Fig. 99. h’5Chapter 14: Dielectric Lossessource
research review
theory-calculation-alternating-current-phenomena-fig-100
Fig. 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 andChapter 15: Distributed Capacity, Inductance, Resistance, And Leakagesource
research review
theory-calculation-alternating-current-phenomena-fig-101
Fig. 101
iEo Fig. 101. Denoting in Fig. 101.Chapter 15: Distributed Capacity, Inductance, Resistance, And Leakagesource
research review