Chapter 3: Standing Waves. 442
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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-16 |
| Location | lines 1087-1111 |
| Status | candidate |
| Word Count | 65 |
| Equation Candidates In Section | 5 |
| Figure Candidates In Section | 0 |
| Quote Candidates In Section | 0 |
Opening Source Excerpt
Section titled “Opening Source Excerpt”CHAPTER III. STANDING WAVES. 442 14. Oscillatory, critical and gradual standing wave. 442 15. The wave length which divides the gradual from the oscillatory wave. 446 16. High-power high-potential overhead transmission line. Character of waves. Numerical example. General equations. 449 17. High-potential underground power cable. Character of waves. Numerical example. General equations. 452 18. Submarine telegraph cable. Existence of logarithmic waves. 454 19. Long distance telephone circuit. Numerical example. Effect of leakage. Effect of inductance or "loading." 454Source-Located Theme Snippets
Section titled “Source-Located Theme Snippets”Waves / transmission lines
Section titled “Waves / transmission lines”CHAPTER III. STANDING WAVES. 442 14. Oscillatory, critical and gradual standing wave. 442 15. The wave length which divides the gradual from the oscillatory wave. 446 16. High-power high-potential overhead transmission line. Character of waves. Numerical example. General equations. 449 17. Hi ...Radiation / light
Section titled “Radiation / light”CHAPTER III. STANDING WAVES. 442 14. Oscillatory, critical and gradual standing wave. 442 15. The wave length which divides the gradual from the oscillatory wave. 446 16. High-power high-potential overhead transmission line. Character of waves. Numerical example. General equations. 449 17. High-potential underground power cable. Character of waves. Numerical example. General ...Chapter-Local Concept Hits
Section titled “Chapter-Local Concept Hits”| Concept Candidate | Hits In Section | Status |
|---|---|---|
| Wave length | 1 | seeded |
Chapter-Local Glossary Hits
Section titled “Chapter-Local Glossary Hits”| Term Candidate | Hits In Section | Status |
|---|---|---|
| wave length | 1 | seeded |
Equation Candidates
Section titled “Equation Candidates”| Candidate ID | OCR / PDF-Text Candidate | Source Location |
|---|---|---|
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0041 | CHAPTER III. STANDING WAVES. 442 | line 1087 |
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0042 | 14. Oscillatory, critical and gradual standing wave. 442 | line 1089 |
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0043 | 18. Submarine telegraph cable. Existence of logarithmic | line 1104 |
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0044 | 19. Long distance telephone circuit. Numerical example. | line 1108 |
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0045 | Effect of leakage. Effect of inductance or “loading.” 454 | line 1110 |
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| No chapter-local candidates yet | - | - |
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| No chapter-local candidates yet | - | - |
Modern Engineering Reading Prompts
Section titled “Modern Engineering Reading Prompts”- 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”- 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.
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