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Tesla-Era Overlap Concordance

Concordance status: generated from processed OCR/PDF text. Treat these as source-location aids until each passage is checked against the scan.

387 hits

Total text matches across processed Steinmetz sections.

13 sources

Sources containing at least one matched alias.

97 sections

Chapters, lectures, sections, or report divisions with matches.

hertzian, high frequency, high potential, high tension, oscillator, wireless

SourceHitsSections
Theory and Calculation of Transient Electric Phenomena and Oscillations14931
General Lectures on Electrical Engineering427
Radiation, Light and Illumination345
Theory and Calculation of Electric Apparatus344
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients305
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients235
Theory and Calculation of Alternating Current Phenomena2110
Theory and Calculation of Electric Circuits147
Theory and Calculation of Alternating Current Phenomena125
Theoretical Elements of Electrical Engineering118
Theory and Calculation of Alternating Current Phenomena84
Engineering Mathematics: A Series of Lectures Delivered at Union College54
Four Lectures on Relativity and Space42
SectionSourceHitsWorkbenchLocation
Chapter 17: Inductor MachinesTheory and Calculation of Electric Apparatus27Workbenchlines 20294-20974
Lecture 17: Arc LightingGeneral Lectures on Electrical Engineering20Workbenchlines 9920-12795
Chapter 9: High-Frequency ConductorsTheory and Calculation of Transient Electric Phenomena and Oscillations18Workbenchlines 27003-27760
Chapter 9: Inductive DischargesTheory and Calculation of Transient Electric Phenomena and Oscillations18Workbenchlines 34897-40349
Lecture 3: Physiological Effects Of RadiationRadiation, Light and Illumination14Workbenchlines 2366-3638
Chapter 8: Low Frequency Surges In High Potential SystemsTheory and Calculation of Transient Electric Phenomena and Oscillations14Workbenchlines 7826-9227
Lecture 8: Traveling WavesElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients13Workbenchlines 5279-6124
Lecture 8: Traveling WavesElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients13Workbenchlines 4745-5520
Lecture 1: Nature And Different Forms Of RadiationRadiation, Light and Illumination11Workbenchlines 608-1548
Chapter 4: Distributed Capacity Of High-Potential TransformersTheory and Calculation of Transient Electric Phenomena and Oscillations11Workbenchlines 23179-23585
Lecture 5: Long Distance TransmissionGeneral Lectures on Electrical Engineering10Workbenchlines 2562-3132
Chapter 8: Velocity Of Propagation Of Electric FieldTheory and Calculation of Transient Electric Phenomena and Oscillations10Workbenchlines 26095-27002
Lecture 10: Continual And Cumulative OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients9Workbenchlines 6804-8485
Chapter 2: Long-Distance Transmission LineTheory and Calculation of Transient Electric Phenomena and Oscillations8Workbenchlines 19339-21720
Chapter 3: Standing WavesTheory and Calculation of Transient Electric Phenomena and Oscillations8Workbenchlines 29316-30243
Chapter 10: Instability Of Circuits : The ArcTheory and Calculation of Electric Circuits7Workbenchlines 17632-21381
Lecture 7: High Frequency Oscillations And SurgesGeneral Lectures on Electrical Engineering6Workbenchlines 3508-3780
Lecture 6: LuminescenceRadiation, Light and Illumination6Workbenchlines 5077-6608
Chapter 3: The Natural Period Of The Transmission LineTheory and Calculation of Transient Electric Phenomena and Oscillations6Workbenchlines 21721-23178
Chapter 1: General EquationsTheory and Calculation of Transient Electric Phenomena and Oscillations6Workbenchlines 27761-28694
Chapter 2: IntroductionTheory and Calculation of Transient Electric Phenomena and Oscillations5Workbenchlines 1993-2658
Chapter 7: Distribution Of Alternating-Current Density In ConductorTheory and Calculation of Transient Electric Phenomena and Oscillations5Workbenchlines 24981-26094
Chapter 6: Transition Points And The Complex CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations5Workbenchlines 32709-33527
Chapter 15: Distributed Capacity, Inductance, Resistance, And LeakageTheory and Calculation of Alternating Current Phenomena4Workbenchlines 15410-16076
Chapter 27: Symbolic Representation Of General Alternating WavesTheory and Calculation of Alternating Current Phenomena4Workbenchlines 33011-34776
Chapter 13: Distributed Capacity, Inductance, Resistance, And LeakageTheory and Calculation of Alternating Current Phenomena4Workbenchlines 9741-11604
Chapter 6: Oscillating Currents,Theory and Calculation of Transient Electric Phenomena and Oscillations4Workbenchlines 5312-6797
Lecture 6: Double-Energy TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients3Workbenchlines 3721-4369
Lecture 9: Oscillations Of The Compound CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients3Workbenchlines 6125-6803
Lecture 6: Double-Energy TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients3Workbenchlines 3287-3955
Lecture 9: Oscillations Of The Compound CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients3Workbenchlines 5521-6088
Lecture 2: Conclusions From The Relativity TheoryFour Lectures on Relativity and Space3Workbenchlines 736-2388
Apparatus Section 10: Synchronous Converters: FrequencyTheoretical Elements of Electrical Engineering3Workbenchlines 15811-15892
Chapter 32: Transformation Of Polyphase SystemsTheory and Calculation of Alternating Current Phenomena3Workbenchlines 36062-36514
Chapter 12: Dibtbisnted Capacity, Inductance, Besistance, AndTheory and Calculation of Alternating Current Phenomena3Workbenchlines 11564-12672
Chapter 24: Symbolic Representation Of General Alternating WavesTheory and Calculation of Alternating Current Phenomena3Workbenchlines 22449-23642
Chapter 4: Induction Motor With Secondary ExcitationTheory and Calculation of Electric Apparatus3Workbenchlines 5555-8554
Chapter 9: High-Frequency Conductors. 403Theory and Calculation of Transient Electric Phenomena and Oscillations3Workbenchlines 1014-1042
Chapter 9: Divided CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations3Workbenchlines 9228-10474
Chapter 1: IntroductionTheory and Calculation of Transient Electric Phenomena and Oscillations3Workbenchlines 15354-15625
Chapter 1: IntroductionTheory and Calculation of Transient Electric Phenomena and Oscillations3Workbenchlines 19260-19338
Lecture 7: Line OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 4370-5278
Lecture 7: Line OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 3956-4744
Lecture 10: Inductance And Capacity Of Round Parallel ConductorsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 6089-7274
Chapter 3: Trigonometric SeriesEngineering Mathematics: A Series of Lectures Delivered at Union College2Workbenchlines 6064-15155
Lecture 6: Higher Harmonics Of The Generator WaveGeneral Lectures on Electrical Engineering2Workbenchlines 3133-3507
Lecture 8: GenerationGeneral Lectures on Electrical Engineering2Workbenchlines 3781-4217
Lecture 2: Relation Of Bodies To RadiationRadiation, Light and Illumination2Workbenchlines 1549-2365
Theory Section 19: Fields of ForceTheoretical Elements of Electrical Engineering2Workbenchlines 7737-7990
Chapter 13: Foucault Or Eddy CurrentsTheory and Calculation of Alternating Current Phenomena2Workbenchlines 13484-14333
Chapter 26: Effects Of Higher HarmonicsTheory and Calculation of Alternating Current Phenomena2Workbenchlines 32540-33010
Chapter 33: Efficiency Of SystemsTheory and Calculation of Alternating Current Phenomena2Workbenchlines 36515-37127
Chapter 11: Fouoault Or Eddy 0Ubbent8Theory and Calculation of Alternating Current Phenomena2Workbenchlines 10500-11563
Chapter 20: RiTheory and Calculation of Alternating Current Phenomena2Workbenchlines 24560-25119
Chapter 11: Foucault Or Eddy CurrentsTheory and Calculation of Alternating Current Phenomena2Workbenchlines 8384-9380
Chapter 23: Effects Of Higher HarmonicsTheory and Calculation of Alternating Current Phenomena2Workbenchlines 21983-22448
Chapter 23: ReviewTheory and Calculation of Electric Apparatus2Workbenchlines 32138-32819
Chapter 24: ConclusionTheory and Calculation of Electric Apparatus2Workbenchlines 32820-33531
Chapter 1: Electric Conduction. Soled And LiquidTheory and Calculation of Electric Circuits2Workbenchlines 959-3894
Chapter 3: Standing Waves. 442Theory and Calculation of Transient Electric Phenomena and Oscillations2Workbenchlines 1087-1111
Chapter 1: The Constants Of The Electric CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations2Workbenchlines 1317-1992
Chapter 7: Resistance, Inductance, And Capacity In Series In Alternating-Current CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations2Workbenchlines 6798-7825
Chapter 4: Arc RectificationTheory and Calculation of Transient Electric Phenomena and Oscillations2Workbenchlines 17755-19259
Chapter 5: Free OscillationsTheory and Calculation of Transient Electric Phenomena and Oscillations2Workbenchlines 31451-32708
Chapter 2: Potential Series And Exponential FunctionEngineering Mathematics: A Series of Lectures Delivered at Union College1Workbenchlines 3492-6063
Chapter 5: Methods Of ApproximationEngineering Mathematics: A Series of Lectures Delivered at Union College1Workbenchlines 15156-16482
Chapter 7: Numerical CalculationsEngineering Mathematics: A Series of Lectures Delivered at Union College1Workbenchlines 21989-25587
Lecture 1: GeneralFour Lectures on Relativity and Space1Workbenchlines 275-735
Lecture 14: Alternating Current Railway MotorGeneral Lectures on Electrical Engineering1Workbenchlines 8649-9342
Lecture 15: ElectrochemistryGeneral Lectures on Electrical Engineering1Workbenchlines 9343-9686
Lecture 8: Arc Lamps And Arc LightingRadiation, Light and Illumination1Workbenchlines 7141-8510
Apparatus Section 8: Alternating-current Transformer: AutotransformerTheoretical Elements of Electrical Engineering1Workbenchlines 18666-18812
Apparatus Section 4: Induction Machines: Induction GeneratorTheoretical Elements of Electrical Engineering1Workbenchlines 21158-21588
Apparatus Section 16: Synchronous Machines: Higher Frequency Cross Currents Between Synchronous MachinesTheoretical Elements of Electrical Engineering1Workbenchlines 10124-10189
Apparatus Section 17: Synchronous Machines: Short-circuit Currents of AlternatorsTheoretical Elements of Electrical Engineering1Workbenchlines 10190-10429
Apparatus Section 11: Synchronous Converters: Double-current GeneratorsTheoretical Elements of Electrical Engineering1Workbenchlines 15893-15982
Apparatus Section 12: Synchronous Converters: ConclusionTheoretical Elements of Electrical Engineering1Workbenchlines 15983-16064
Chapter 1: IntroductionTheory and Calculation of Alternating Current Phenomena1Workbenchlines 1120-1683
Chapter 11: Phase ControlTheory and Calculation of Alternating Current Phenomena1Workbenchlines 9767-10717
Chapter 22: Armature Reactions Of AlternatorsTheory and Calculation of Alternating Current Phenomena1Workbenchlines 23971-25134
Chapter 25: Distortion Of Wave-Shape And Its CausesTheory and Calculation of Alternating Current Phenomena1Workbenchlines 29375-32539
Chapter 28: Copper Efficiency Of SystemsTheory and Calculation of Alternating Current Phenomena1Workbenchlines 26584-27052
Chapter 30: Efficiency Of SystemsTheory and Calculation of Alternating Current Phenomena1Workbenchlines 25136-25597
Chapter 4: MagnetismTheory and Calculation of Electric Circuits1Workbenchlines 6942-9061
Chapter 7: Shaping Of Waves : GeneralTheory and Calculation of Electric Circuits1Workbenchlines 12222-12961
Chapter 13: Reactance Of Synchronous MachinesTheory and Calculation of Electric Circuits1Workbenchlines 23466-24022
Chapter 14: Constant-Potential Constant-Current Trans FormationTheory and Calculation of Electric Circuits1Workbenchlines 24023-27995
Chapter 18: Oscillating CurrentsTheory and Calculation of Electric Circuits1Workbenchlines 31657-33200
Chapter 1: Introduction. 217Theory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 659-674
Chapter 2: Long Distance Transmission Line. 279Theory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 755-835
Chapter 4: Distributed Capacity Of High-Potential Trans Former. 342Theory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 875-887
Chapter 2: Discussion Of General Equations. 431Theory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 1063-1086
Chapter 6: Transition Points And The Complex Circuit. 498Theory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 1187-1227
Chapter 10: Mutual InductanceTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 10475-12216
Chapter 6: Alternating Magnetic Flux DistributionTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 23948-24980
Chapter 2: Discussion Of General EquationsTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 28695-29315
Chapter 7: Power And Energy Of The Complex CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 33528-34202
Chapter 17: Inductor Machines - 27 hit(s)

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... etween 4>, and *2 or approximately zero, we would alternate between *i and — *i. On the other hand, the single field-coil construction gives a material advantage in the material economy of the field, and in machines having very many field poles, that is, high-frequency alternators, the economy in the field construction overbalances the lesser economy in the use of the armature, especially as at higli frequencies it is not feasible any more to push the alter- nating flux, $0, up to or near saturation values. Therefore, f ...
Lecture 17: Arc Lighting - 20 hit(s)

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... saved in alternating constant potential arc lamps, by using reactance instead of resistance, but the power factor is there- fore greatly lowered ; that is, the constant potential alternating arc lamp rarely has a power factor of over 70%. Where therefore high potential constant current circuits are permissible, as for outdoor or street lighting, arc lamps are usually operated on a constant current circuit, with series connection of from 50 to 100 lamps on one circuit. With the exception of a few of the larger cities, al ...
Chapter 9: High-Frequency Conductors - 18 hit(s)

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CHAPTER IX. HIGH-FREQUENCY CONDUCTORS. 80. As the result of the phenomena discussed in the preceding chapters, conductors intended to convey currents of very high frequency, as lightning discharges, high frequency oscillations of transmission lines, the currents used in wireless t ...
Chapter 9: Inductive Discharges - 18 hit(s)

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... o (401), is 7 ~ — U(jt, V (404) the current 72, by sub- (405) An inductance discharging into the transmission line thus gives an oscillatory distribution of voltage and current along the line. 68. As example may be considered the three-phase high- potential circuit, comprising a generating system of r = 2 ohms and L = 0.5 henry per phase and connected to a long-distance transmission line of r0= 0.4 ohm, L0 = 0.002 henry, gQ= 0.2 X 10~6 mho, (70= 0.016 X 10~6 farad per mile of conductor or phase, and of 1Q = ...
Lecture 3: Physiological Effects Of Radiation - 14 hit(s)

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... TION, LIGHT, AND ILLUMINATION. in visibility to the orange yellow for long distances, and inversely, the orange yellow is superior for short distances. At the limits of visibility the eye is very many times more sensitive to green light and, in general, high-frequency light, than to orange yellow and, in general, low-frequency light. A necessary result of the higher sensitivity of the eye for green light is the preponderance of green in gas and vapor spectra. As no special reason exists why spectrum lines should appea ...
Chapter 8: Low Frequency Surges In High Potential Systems - 14 hit(s)

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CHAPTER VIII. LOW FREQUENCY SURGES IN HIGH POTENTIAL SYSTEMS. 64. In electric circuits of considerable capacity, that is, in extended high potential systems, as long distance transmission lines and underground cable systems, occasionally destructive high potential low frequency surges occur; that is, oscil ...
Lecture 8: Traveling Waves - 13 hit(s)

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... c- tions of different dissipation constants u. For instance, if in a circuit consisting of an unloaded transformer and a transmission line, as indicated in Fig. 40, at no load on the step-down trans- ^^ Line Transformer Line Fig. 40. former, the high-tension switches are opened at the generator end of the transmission line. The energy stored magnetically and dielectrically in line and transformer then dissipates by a transient, as shown in the oscillogram Fig. 41. This gives the oscillation of a circuit consi ...
Lecture 8: Traveling Waves - 13 hit(s)

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... ions of different dissipation constants u. For instance, if a circuit consists of an unloaded transformer and a transmission line, as indicated in Fig. 40, that is, at no load on the step-down trans- ^> Line Transformer Line Fig. 40. former, the high-tension switches are opened at the generator end of the transmission line. The energy stored magnetically and dielectrically in line and transformer then dissipates by a transient, as shown in the oscillogram Fig. 41. This gives the oscillation of a circuit consi ...
Lecture 1: Nature And Different Forms Of Radiation - 11 hit(s)

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... adiation increases, 'but at the same time radiations of higher and higher frequencies appear, and ultimately the rods become visible in the dark, giving a dark red light; that is, of all the radiations sent out by the rods, a small part is of sufficiently high frequency to be visible. Still further increasing the tempera- ture, the total radiation increases, but the waves of high frequency in- crease more rapidly than those vof lower frequency ; that is, the average frequency of radiation increases or the average wave ...
Chapter 4: Distributed Capacity Of High-Potential Transformers - 11 hit(s)

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CHAPTER IV. DISTRIBUTED CAPACITY OF HIGH-POTENTIAL TRANSFORMERS. 40. In the high-potential coils of transformers designed for very high voltages phenomena resulting from distributed capacity occur. In transformers for very high voltages — 100;000 volts and more, or even considerably less in small tran ...
Lecture 5: Long Distance Transmission - 10 hit(s)

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... ductors = 2 e. For instance, wire No. 0000 D = .46" ; corona effects begin at the voltage E = 100,000 [) D^ = 46,000. ' ' For 100,000 volts the smallest diameter for which no corona effects occur is : D= ? =1" 100,000 68 GENERAL LECTURES In high potential transformers in the coils no corona effects may occur, because the diameter of the coil or the thick- ness is large enough, but the leads connecting the coils with each other and with the outside, if not chosen very large in diameter, may give corona effe ...
Chapter 8: Velocity Of Propagation Of Electric Field - 10 hit(s)

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... on, or, in other words, the electric field lags the more, the greater the distance from the conductor. Since the velocity of propagation is very high — about 3 X 1010 centimeters per second — the wave of an alternating or oscillating current even of very high frequency is of considerable length ; at 60 cycles the wave length is 0.5 X 109 centimeters, and even at a million cycles the wave length is 30,000 centimeters, or about 1000 feet, that is, very great compared with the distance to which electric fields usually exte ...
Lecture 10: Continual And Cumulative Oscillations - 9 hit(s)

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... equal to the energy supply, and the oscillation becomes continual. A continual or cumulative oscillation thus involves an energy and frequency transformation, from the low-frequency or con- tinuous-current energy of the power supply of the system to the high-frequency energy of the oscillation. 119 120 ELECTRICAL DISCHARGES, WAVES AND IMPULSES This energy transformation may be brought about by the transient of energy readjustment, resulting from a change of circuit conditions, producing again a change of circuit c ...
Chapter 2: Long-Distance Transmission Line - 8 hit(s)

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... stributed capacity and inductance as so-called "wave transmission" and the phenomena thus essentially differ from those in a short energy transmission line. 4. Therefore in very long circuits, as in lines conveying alter- nating currents of high value at high potential over extremely long distances, by overhead conductors or underground cables, or with very feeble currents at extremely high frequency, such as telephone currents, the consideration of the line resistance, which consumes e.m.fs. in phase with the current, ...
Chapter 3: Standing Waves - 8 hit(s)

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... the wave non-oscillatory, and of the frequency /0, which, in an undamped circuit, will correspond to this critical wave length lWo, can best be derived by considering some representative numerical examples. As such may be considered: (1) A high-power high-potential overhead transmission line. (2) A high-potential underground power cable. (3) A submarine telegraph cable. (4) A long-distance overhead telephone circuit. (1) High-power high-potential overhead transmission line. 16. Assume energy to be transmitted ...
Chapter 10: Instability Of Circuits : The Arc - 7 hit(s)

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... sually all three may occur, under different circuit conditions. The electric arc is the most frequent and most serious cause of instability of electric circuits, and therefore should first be sus- pected, especially if the instability assumes the form of high- frequency disturbances or abrupt changes of current or voltage, such as is shown for instance in the oscillograms. Figs. 80 and 81. Somewhat similar effects of instability are produced by pyro- electric conductors. Induction motors and synchronous motors may show ...
Lecture 7: High Frequency Oscillations And Surges - 6 hit(s)

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SEVENTH LECTURE HIGH FREQUENCY OSCILLATIONS AND SURGES 1"^ N an electric circuit, in addition to the power consump- tion by the resistance of the lines, an energy storage ■^ occurs as electrostatic energy, or electrostatic charge due to the voltage on the line (capacity) ; and as el ...
Lecture 6: Luminescence - 6 hit(s)

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... e places where the field intensity is highest, as at the needle points, before the disruptive voltage of the spark gap is reached, and then a partial break down occurs at the points of maximum field intensity, as at the needle points, or at the surface of high potential conductors, etc. A blue glow, then, appears at the needle points followed by violet streamers (in air, the color being the nitrogen spectrum; in other gases other colors appear), and gradually increases in extent with increasing voltage, the so-called " b ...