Chapter 2: Circuit Control By Periodic Transient Phenomena
Research workbench, not a finished commentary page.
This page is generated from processed source text and candidate catalogs. It exists to help researchers decide what to verify, promote, and deeply decode next.
Source Metadata
Section titled “Source Metadata”| Field | Value |
|---|---|
| Source | Theory and Calculation of Transient Electric Phenomena and Oscillations |
| Year | 1909 |
| Section ID | theory-calculation-transient-electric-phenomena-oscillations-chapter-38 |
| Location | lines 15626-15962 |
| Status | candidate |
| Word Count | 788 |
| Equation Candidates In Section | 0 |
| Figure Candidates In Section | 0 |
| Quote Candidates In Section | 0 |
Opening Source Excerpt
Section titled “Opening Source Excerpt”CHAPTER II. CIRCUIT CONTROL BY PERIODIC TRANSIENT PHENOMENA. 6. As an example of a system of periodic transient phenomena, used for the control of electric circuits, may be considered an automatic potential regulator operating in the field circuit of the exciter of an alternating current system. Let, r0 = 40 ohms = resistance and L = 400 henrys = inductance of the exciter field circuit. A resistor, having a resistance, rl = 24 ohms, is inserted in series to r0, L in the exciter field, and a potential magnet, con- trolled by the alternating current system, is arranged so as to short circuit resistance, rv if the alternating potential is below, to throw resistance rl into circuit again, if the potential is above normal. With a single resistance step, rv in the one position ofSource-Located Theme Snippets
Section titled “Source-Located Theme Snippets”Field language
Section titled “Field language”CHAPTER II. CIRCUIT CONTROL BY PERIODIC TRANSIENT PHENOMENA. 6. As an example of a system of periodic transient phenomena, used for the control of electric circuits, may be considered an automatic potential regulator operating in the field circuit of the exciter of an alternating current system. Let, r0 = 40 ohms = resistance and L = 400 henrys = inductance of the exciter field circuit. A resistor, having a resistance, rl = 24 ohms, is inserted in series to r0, L in the exciter field, and a potential magnet ...Transients / damping
Section titled “Transients / damping”CHAPTER II. CIRCUIT CONTROL BY PERIODIC TRANSIENT PHENOMENA. 6. As an example of a system of periodic transient phenomena, used for the control of electric circuits, may be considered an automatic potential regulator operating in the field circuit of the exciter of an alternating current system. Let, r0 = 40 ohms = resis ...Alternating current
Section titled “Alternating current”CHAPTER II. CIRCUIT CONTROL BY PERIODIC TRANSIENT PHENOMENA. 6. As an example of a system of periodic transient phenomena, used for the control of electric circuits, may be considered an automatic potential regulator operating in the field circuit of the exciter of an alternating current system. Let, r0 = 40 ohms = resistance and L = 400 henrys = inductance of the exciter field circuit. A resistor, having a resistance, rl = 24 ohms, is inserted in series to r0, L in the exciter field, and a potential magnet, con- trolled by the alternating current system, ...Complex quantities
Section titled “Complex quantities”... e in position r0, hence a shorter time in position (r0 + rt), before the rising potential throws it over into the next position; while at light load, requiring low field excitation, the duration of the period of high resistance, 223 224 TRANSIENT PHENOMENA (TO _|_ rj} is greater, and that of the period of low resistance, r0, less. 7. Let, ^ = the duration of the short circuit of resistance rx; t2 = the time during which resistance rx is in circuit, and t0 = t, + tr During each period t0, the resistance of the exciter field, therefore, ...Chapter-Local Concept Hits
Section titled “Chapter-Local Concept Hits”| Concept Candidate | Hits In Section | Status |
|---|---|---|
| Light | 1 | seeded |
Chapter-Local Glossary Hits
Section titled “Chapter-Local Glossary Hits”| Term Candidate | Hits In Section | Status |
|---|---|---|
| No chapter-local term hits yet | - | - |
Equation Candidates
Section titled “Equation Candidates”| Candidate ID | OCR / PDF-Text Candidate | Source Location |
|---|---|---|
| No chapter-local candidates yet | - | - |
Figure Candidates
Section titled “Figure Candidates”| Candidate ID | OCR / PDF-Text Candidate | Source Location |
|---|---|---|
| No chapter-local candidates yet | - | - |
Hidden-Gem Quote Candidates
Section titled “Hidden-Gem Quote Candidates”| Candidate ID | Candidate Passage | Source Location |
|---|---|---|
| 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.
- Alternating current: Compare Steinmetz’s AC language with modern sinusoidal steady-state analysis, RMS quantities, phase, and phasor notation.
- Complex quantities: Track how Steinmetz preserves geometric rotation and quadrature while translating the same operation into symbolic form.
- 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.
- 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.