Chapter 8: Velocity Of Propagation Op Electric Field. 387
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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-12 |
| Location | lines 972-1013 |
| Status | candidate |
| Word Count | 112 |
| Equation Candidates In Section | 9 |
| Figure Candidates In Section | 0 |
| Quote Candidates In Section | 0 |
Opening Source Excerpt
Section titled “Opening Source Excerpt”CHAPTER VIII. VELOCITY OF PROPAGATION OP ELECTRIC FIELD. 387 67. Conditions, under which the velocity of propagation of the field is of industrial importance. 387 68. Equations of decrease of electric field with the dis- tance. 388 69. Effect of return conductor on distance decrement of field. 389 70. Inductance of length I of infinitely long conductor with- out return conductor. 390 71. Equations of magnetic flux, effective resistance of radia- tion, inductance and impedance. 391 72. Evaluation of functions sil al and col al. 394 73. Self-inductive impedance, and numerical example. 395 74. Discussion of effective resistance and radiated power, as function of frequency. 396 75. Mutual inductance of two distant conductors of finite length. 398 76. Example. 399 77. Capacity of a sphere in space. 400 78. Example. 401 79. Sphere at aSource-Located Theme Snippets
Section titled “Source-Located Theme Snippets”Field language
Section titled “Field language”CHAPTER VIII. VELOCITY OF PROPAGATION OP ELECTRIC FIELD. 387 67. Conditions, under which the velocity of propagation of the field is of industrial importance. 387 68. Equations of decrease of electric field with the dis- tance. 388 69. Effect of return conductor on distance decrement of field. 389 70. Inductance of leng ...Impedance / reactance
Section titled “Impedance / reactance”... d with the dis- tance. 388 69. Effect of return conductor on distance decrement of field. 389 70. Inductance of length I of infinitely long conductor with- out return conductor. 390 71. Equations of magnetic flux, effective resistance of radia- tion, inductance and impedance. 391 72. Evaluation of functions sil al and col al. 394 73. Self-inductive impedance, and numerical example. 395 74. Discussion of effective resistance and radiated power, as function of frequency. 396 75. Mutual inductance of two distant conductors of finite length. ...Magnetism
Section titled “Magnetism”... dustrial importance. 387 68. Equations of decrease of electric field with the dis- tance. 388 69. Effect of return conductor on distance decrement of field. 389 70. Inductance of length I of infinitely long conductor with- out return conductor. 390 71. Equations of magnetic flux, effective resistance of radia- tion, inductance and impedance. 391 72. Evaluation of functions sil al and col al. 394 73. Self-inductive impedance, and numerical example. 395 74. Discussion of effective resistance and radiated power, as function of frequency. 396 ...Dielectricity / capacity
Section titled “Dielectricity / capacity”... tions sil al and col al. 394 73. Self-inductive impedance, and numerical example. 395 74. Discussion of effective resistance and radiated power, as function of frequency. 396 75. Mutual inductance of two distant conductors of finite length. 398 76. Example. 399 77. Capacity of a sphere in space. 400 78. Example. 401 79. Sphere at a distance from ground. 402Chapter-Local Concept Hits
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Equation Candidates
Section titled “Equation Candidates”| Candidate ID | OCR / PDF-Text Candidate | Source Location |
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theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0022 | the field is of industrial importance. 387 | line 976 |
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0023 | tance. 388 | line 980 |
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0024 | 69. Effect of return conductor on distance decrement of | line 982 |
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0025 | 70. Inductance of length I of infinitely long conductor with- | line 986 |
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0026 | 71. Equations of magnetic flux, effective resistance of radia- | line 990 |
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0027 | tion, inductance and impedance. 391 | line 992 |
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0028 | 74. Discussion of effective resistance and radiated power, as | line 998 |
theory-calculation-transient-electric-phenomena-oscillations-eq-candidate-0029 | 75. Mutual inductance of two distant conductors of finite | line 1002 |
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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.
- Impedance / reactance: Translate historical opposition terms into modern impedance, admittance, conductance, susceptance, and complex-plane notation.
- Magnetism: Track flux, reluctance, permeability, magnetizing force, and loss language against modern magnetic-circuit terminology.
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Ether-Field Interpretive Boundary
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