Lecture 4: Single-Energy Transients In Alternating Current Circuits
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Source Metadata
Section titled “Source Metadata”| Field | Value |
|---|---|
| Source | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients |
| Year | 1914 |
| Section ID | electric-discharges-waves-impulses-1914-lecture-04 |
| Location | lines 2485-3386 |
| Status | candidate |
| Word Count | 5659 |
| Equation Candidates In Section | 56 |
| Figure Candidates In Section | 1 |
| Quote Candidates In Section | 0 |
Opening Source Excerpt
Section titled “Opening Source Excerpt”LECTURE IV. SINGLE-ENERGY TRANSIENTS IN ALTERNATING- CURRENT CIRCUITS. 17. Whenever the conditions of an electric circuit are changed in such a manner as to require a change of stored energy, a transi- tion period appears, during which the stored energy adjusts itself from the condition existing before the change to the condition after the change. The currents in the circuit during the transition period can be considered as consisting of the superposition of the permanent current, corresponding to the conditions after the change, and a transient current, which connects the current value before the change with that brought about by the, change. That is, if ii = current existing in the circuit immediately before, and thus at the moment of the change of circuit condition, and 12 = current which should exist at the momentSource-Located Theme Snippets
Section titled “Source-Located Theme Snippets”Field language
Section titled “Field language”... aneous values of the resultant currents (shown in drawn line) must be zero at any moment, not only during the permanent condition, but also dur- ing the transition period existing before the permanent condi- tion is reached. It is interesting to apply this to the resultant magnetic field produced by three equal three-phase magnetizing coils placed under equal angles, that is, to the starting of the three-phase rotating magnetic field, or in general any polyphase rotating magnetic field. Fig. 18. — Construction of Starting Transient of Rotating Field. A ...Transients / damping
Section titled “Transients / damping”LECTURE IV. SINGLE-ENERGY TRANSIENTS IN ALTERNATING- CURRENT CIRCUITS. 17. Whenever the conditions of an electric circuit are changed in such a manner as to require a change of stored energy, a transi- tion period appears, during which the stored energy adjusts itself from the condition existing before the c ...Magnetism
Section titled “Magnetism”... ore gradually decreases in the manner as discussed in para- graph 13, that is, with a duration T = — - The permanent current 12 may be continuous, or alternating, or may be a changing current, as a transient of long duration, etc. The same reasoning applies to the voltage, magnetic flux, etc. Thus, let, in an alternating-current circuit traversed by current i'l, in Fig. 15 A, the conditions be changed, at the moment t = 0, so as to produce the current iV The instantaneous value of the current ii at the moment t = 0 can be considered as consisting of ...Waves / transmission lines
Section titled “Waves / transmission lines”... Fig. 155, and is a maximum, if the change occurs at the moment when the two currents ii and 12 have the greatest difference, as shown in Fig. 15C, that is, at a point one-quarter period or 90 degrees distant from the intersec- tion of ii and 12. 32 ELECTRIC DISCHARGES, WAVES AND IMPULSES. If the current ii is zero, we get the starting of the alternating current in an inductive circuit, as shown in Figs. 16, A, B,C. The starting transient is zero, if the circuit is closed at the moment when the permanent current would be zero (Fig. 165), and i ...Chapter-Local Concept Hits
Section titled “Chapter-Local Concept Hits”| Concept Candidate | Hits In Section | Status |
|---|---|---|
| Frequency | 30 | seeded |
| Ether | 2 | seeded |
| Light | 2 | seeded |
Chapter-Local Glossary Hits
Section titled “Chapter-Local Glossary Hits”| Term Candidate | Hits In Section | Status |
|---|---|---|
| ether | 2 | seeded |
Equation Candidates
Section titled “Equation Candidates”| Candidate ID | OCR / PDF-Text Candidate | Source Location |
|---|---|---|
electric-discharges-waves-impulses-1914-eq-candidate-0076 | thus at the moment of the change of circuit condition, and 12 = | line 2500 |
electric-discharges-waves-impulses-1914-eq-candidate-0077 | component ii — 12 = iq. The former, 2*2, is permanent, as result- | line 2504 |
electric-discharges-waves-impulses-1914-eq-candidate-0078 | graph 13, that is, with a duration T = — - | line 2509 |
electric-discharges-waves-impulses-1914-eq-candidate-0079 | i’l, in Fig. 15 A, the conditions be changed, at the moment t = 0, | line 2517 |
electric-discharges-waves-impulses-1914-eq-candidate-0080 | current ii at the moment t = 0 can be considered as consisting | line 2519 |
electric-discharges-waves-impulses-1914-eq-candidate-0081 | of the instantaneous value of the permanent current (2, shown | line 2520 |
electric-discharges-waves-impulses-1914-eq-candidate-0082 | dotted, and the transient io = i\ — 22. The latter gradually dies | line 2521 |
electric-discharges-waves-impulses-1914-eq-candidate-0083 | Fig. 15. — Single-energy Transient of Alternating-current Circuit. | line 2543 |
Figure Candidates
Section titled “Figure Candidates”| Candidate ID | OCR / PDF-Text Candidate | Source Location |
|---|---|---|
electric-discharges-waves-impulses-1914-fig-025 | frequency, and as the result an increase of voltage and a distor- tion of the quadrature phase occurs, as shown in the oscillogram Fig. 25. Various momentary short-circuit pheno… | line 3288 |
Hidden-Gem Quote Candidates
Section titled “Hidden-Gem Quote Candidates”| Candidate ID | Candidate Passage | Source Location |
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| No chapter-local candidates yet | - | - |
Modern Engineering Reading Prompts
Section titled “Modern Engineering Reading Prompts”- Field language: Read for whether field language is mechanical, geometrical, causal, descriptive, or simply a convenient engineering model.
- Transients / damping: Separate the temporary term from the final steady-state term and compare with differential-equation response language.
- Magnetism: Track flux, reluctance, permeability, magnetizing force, and loss language against modern magnetic-circuit terminology.
- Waves / transmission lines: Map Steinmetz’s wave and line language onto modern distributed constants, propagation velocity, standing waves, and reflections.
- Radiation / light: Compare the chapter’s radiation vocabulary with modern electromagnetic radiation, spectral frequency, wavelength, absorption, and illumination engineering.
Ether-Field Interpretive Boundary
Section titled “Ether-Field Interpretive Boundary”- Field language: Field-pressure or field-gradient interpretations can be explored here only after the explicit source passage and modern engineering translation are kept distinct.
- Transients / damping: Transient collapse, impulse, and surge behavior can be compared with alternative field language, but only as a clearly marked reading.
- Magnetism: Centrifugal/divergent magnetic-field readings are interpretive overlays, not automatic historical claims.
- Waves / transmission lines: Standing/traveling wave passages may support richer field interpretations; the page keeps those readings separate from verified Steinmetz wording.
- Radiation / light: Radiation and wave language can invite ether-field comparison, but source wording, modern radiation theory, and speculative synthesis must stay separated.
Promotion Checklist
Section titled “Promotion Checklist”- Open the full source text and the scan or raw PDF.
- Verify the chapter boundary and surrounding context.
- Promote exact quotations only after checking the source image.
- Move mathematical candidates into canonical equation pages only after formula typography is corrected.
- Move diagram candidates into the diagram archive only after image extraction, crop verification, and manifest creation.
- Keep Steinmetz wording, modern translation, and ether-field interpretation in separate labeled layers.