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Distributed Constants

Distributed constants are resistance, inductance, capacity, and leakage spread along a conductor, line, cable, or winding instead of concentrated at one point. Once constants are distributed, the circuit can behave as a wave system.

Modern transmission-line notation often uses per-unit-length constants:

R,L,G,CR,\quad L,\quad G,\quad C

For an ideal lossless line:

v=1LCv = \frac{1}{\sqrt{LC}}

Steinmetz’s transient work forces the reader to stop treating every electrical system as an instantaneous lumped circuit. Long lines, high-potential apparatus, transformer coils, cables, and conductors can require a field-propagation view.

Modern Engineering Interpretation

This becomes modern transmission-line theory, surge propagation, reflection, standing waves, and insulation coordination.

The Lightning and Surge Traveling Wave tool gives a modern visualization of a disturbance moving along a distributed line and reflecting from a terminal load.

Tesla-Era Comparison

Tesla-era high-frequency and impulse experiments often live in the same territory: distributed capacity, inductance, resonance, discharge, and wave propagation. The comparison must be technical, not mythic.

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.

252

Candidate occurrences tracked for this page.

10

Sources with at least one hit.

42

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 Transient Electric Phenomena and Oscillations with 112 candidate hits across 23 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.

distributed capacity, distributed constants, distributed inductance, standing wave, traveling wave, travelling wave, wave front, wave propagation

Distributed Constants - Wave Propagation

SourceCandidate HitsSectionsConcepts represented
Theory and Calculation of Transient Electric Phenomena and Oscillations11223Distributed Constants, Wave Propagation
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients365Distributed Constants, Wave Propagation
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients355Distributed Constants, Wave Propagation
Theory and Calculation of Alternating Current Phenomena282Distributed Constants
Theory and Calculation of Alternating Current Phenomena133Distributed Constants
Theory and Calculation of Alternating Current Phenomena122Distributed Constants
General Lectures on Electrical Engineering81Wave Propagation
Radiation, Light and Illumination42Wave Propagation
Chapter 4: Traveling Waves - 33 candidate hits

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

Location: lines 30244-31450 - Tracked concepts: Wave Propagation

Open source text - Open chapter workbench

CHAPTER IV. TRAVELING WAVES. 20. As seen in Chapter III, especially in electric power cir- cuits, overhead or underground, the longest existing standing wave has a wave length which is so small compared with the critical wave length - where the frequency becomes zero - that the effect of the damping constant on the frequency and the wave length is negligi...
... the fre- quency constant q and the wave length constant k can be neglected, that is, frequency and wave length assumed as inde- pendent of the energy loss in the circuit. Usually, therefore, the equations (74) and (75) can be applied in dealing with the traveling wave. In these equations the distance traveled by the wave per second is used as unit len...
Lecture 8: Traveling Waves - 27 candidate hits

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

Location: lines 5279-6124 - Tracked concepts: Distributed Constants, Wave Propagation

Open source text - Open chapter workbench

LECTURE VIII. TRAVELING WAVES. 33. In a stationary oscillation of a circuit having uniformly distributed capacity and inductance, that is, the transient of a circuit storing energy in the dielectric and magnetic field, current and voltage are given by the expression i = ioe-"^ cos ((/> T CO - 7), ^ . . e = eoe~"' sin ((^ =F co - 7), where <j) is the time...
... y dis- tance angle co, and at any time t, that is, time angle 0, then is p = ei, = eo^e~2"* cos (0 =F co - 7) sin (0 =F co - 7), = ^6-^«'sin2(0Ta>-7), (2) and the average power flow is Po = avg p, (3) = 0. Hence, in a stationary oscillation, or standing wave of a uni- form circuit, the average flow of power, po, is zero, and no power flows along the c...
Lecture 8: Traveling Waves - 27 candidate hits

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

Location: lines 4745-5520 - Tracked concepts: Distributed Constants, Wave Propagation

Open source text - Open chapter workbench

LECTURE VIII. TRAVELING WAVES. 33. In a stationary oscillation of a circuit having uniformly distributed capacity and inductance, that is, the transient of a circuit storing energy in the dielectric and magnetic field, current and voltage are given ^by the expression i = iQe~ut cos (0 T co - 7), ) e = e0e~ut sin (</> T co - 7), ) where 0 is the time angle...
... tance angle co, and at any time t, that is, time angle <£, then is p = ei, = e0ioe~2ut cos (</> T co - 7) sin (0 =F co - 7), = ^|V2«<sin2(c/>=Fco-7), (2) and the average power flow is Po = avg p, (3) = 0. Hence, in a stationary oscillation, or standing wave of a uni- form circuit, the average flow of power, p0, is zero, and no power flows along the ci...
Chapter 13: Distributed Capacity, Inductance, Resistance, And Leakage - 23 candidate hits

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

Location: lines 9741-11604 - Tracked concepts: Distributed Constants

Open source text - Open chapter workbench

CHAPTER XIII. DISTRIBUTED CAPACITY, INDUCTANCE, RESISTANCE, AND LEAKAGE. 107. As far as capacity has been considered in the foregoing chapters, the assumption has been made that the condenser or other source of negative reactance is shunted across the circuit at a definite point. In many ...
... hole length of the conductor, so that the circuit can be considered as shunted by an infinite number of infinitely small condensers infi nitely near together, as diagrammatically shown in Fig. 83. iiiimiiiiumiiiT TTTTTTTTTT.TTTTTTTTTT i Fig. 83. Distributed Capacity. In this case the intensity as well as phase of the current, and consequently of the c...
Chapter 3: Standing Waves - 15 candidate hits

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

Location: lines 29316-30243 - Tracked concepts: Wave Propagation

Open source text - Open chapter workbench

CHAPTER III. STANDING WAVES. 14. If the propagation constant of the wave vanishes, h = 0, the wave becomes a stationary or standing wave, and the equa- tions of the standing wave are thus derived from the general equations (50) to (61), by substituting therein h = 0, which gives R2 = V(k2 - LCm2)2; (97) hence, if k2 > LCm2, R2 = tf- LCm2; and if /c2 < LCm...
Chapter 12: Dibtbisnted Capacity, Inductance, Besistance, And - 11 candidate hits

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

Location: lines 11564-12672 - Tracked concepts: Distributed Constants

Open source text - Open chapter workbench

... capacity is distributed over the whole length of the conductor, so that the circuit can be considered as shunted by an infinite number of infinitely small condensers infi. nitely near together, as diagrammatically shown in Fig. 83. 8 3 S Fig, 83. Distributed Capacity. In this case the intensity as well as phase of the current,, and consequently of the...
... .M.Fs., but also the currents, at the beginning, end, and different points of the conductor, are different in intensity and in phase. Where the capacity effect of the line is small, it may with sufficient approximation be represented by one con- §103] DISTRIBUTED CAPACITY. 151 denser of the same capacity as the line, shunted across the line. Frequentl...
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