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Field Stress, Strain, Pressure, and Tension Concordance

Field Stress, Strain, Pressure, and Tension

Section titled “Field Stress, Strain, Pressure, and Tension”

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

260 hits

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14 sources

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60 sections

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

elastic, pressure, strain, stress, tension

SourceHitsSections
Radiation, Light and Illumination628
General Lectures on Electrical Engineering548
Theory and Calculation of Electric Circuits334
Theory and Calculation of Alternating Current Phenomena275
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients165
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients165
Theory and Calculation of Transient Electric Phenomena and Oscillations137
Theory and Calculation of Alternating Current Phenomena103
Theory and Calculation of Alternating Current Phenomena103
Engineering Mathematics: A Series of Lectures Delivered at Union College82
America and the New Epoch65
Theoretical Elements of Electrical Engineering33
Four Lectures on Relativity and Space11
Investigation of Some Trouble in the Generating System of the Commonwealth Edison Co.11
SectionSourceHitsWorkbenchLocation
Lecture 6: LuminescenceRadiation, Light and Illumination31Workbenchlines 5077-6608
Chapter 2: Electric Conduction. Gas And VaporTheory and Calculation of Electric Circuits26Workbenchlines 3895-5444
Chapter 33: Efficiency Of SystemsTheory and Calculation of Alternating Current Phenomena18Workbenchlines 36515-37127
Lecture 5: Temperature RadiationRadiation, Light and Illumination17Workbenchlines 3946-5076
Lecture 17: Arc LightingGeneral Lectures on Electrical Engineering16Workbenchlines 9920-12795
Lecture 1: General ReviewGeneral Lectures on Electrical Engineering11Workbenchlines 154-565
Lecture 8: Traveling WavesElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients9Workbenchlines 5279-6124
Lecture 8: Traveling WavesElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients9Workbenchlines 4745-5520
Lecture 5: Long Distance TransmissionGeneral Lectures on Electrical Engineering7Workbenchlines 2562-3132
Lecture 11: Lightning ProtectionGeneral Lectures on Electrical Engineering7Workbenchlines 4931-5294
Chapter 28: Copper Efficiency Of SystemsTheory and Calculation of Alternating Current Phenomena7Workbenchlines 26584-27052
Chapter 30: Efficiency Of SystemsTheory and Calculation of Alternating Current Phenomena7Workbenchlines 25136-25597
Lecture 8: Arc Lamps And Arc LightingRadiation, Light and Illumination6Workbenchlines 7141-8510
Chapter 14: Dielectric LossesTheory and Calculation of Alternating Current Phenomena6Workbenchlines 14334-15409
Chapter 3: Trigonometric SeriesEngineering Mathematics: A Series of Lectures Delivered at Union College5Workbenchlines 6064-15155
Lecture 8: GenerationGeneral Lectures on Electrical Engineering5Workbenchlines 3781-4217
Chapter 1: The Constants Of The Electric CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations5Workbenchlines 1317-1992
Lecture 2: General DistributionGeneral Lectures on Electrical Engineering4Workbenchlines 566-982
Chapter 2: Potential Series And Exponential FunctionEngineering Mathematics: A Series of Lectures Delivered at Union College3Workbenchlines 3492-6063
Lecture 6: Higher Harmonics Of The Generator WaveGeneral Lectures on Electrical Engineering3Workbenchlines 3133-3507
Chapter 7: Shaping Of Waves : GeneralTheory and Calculation of Electric Circuits3Workbenchlines 12222-12961
Chapter 17: ConclusionAmerica and the New Epoch2Workbenchlines 7568-8027
Lecture 1: Nature And Origin Of TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 557-1002
Lecture 7: Line OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 4370-5278
Lecture 9: Oscillations Of The Compound CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 6125-6803
Lecture 1: Nature And Origin Of TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 460-882
Lecture 7: Line OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 3956-4744
Lecture 9: Oscillations Of The Compound CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 5521-6088
Lecture 3: Physiological Effects Of RadiationRadiation, Light and Illumination2Workbenchlines 2366-3638
Lecture 9: Measurement Of Light And RadiationRadiation, Light and Illumination2Workbenchlines 8511-9388
Lecture 12: Illumination And Illuminating EngineeringRadiation, Light and Illumination2Workbenchlines 16485-17445
Chapter 20: RiTheory and Calculation of Alternating Current Phenomena2Workbenchlines 24560-25119
Chapter 23: Effects Of Higher HarmonicsTheory and Calculation of Alternating Current Phenomena2Workbenchlines 21983-22448
Chapter 1: Electric Conduction. Soled And LiquidTheory and Calculation of Electric Circuits2Workbenchlines 959-3894
Chapter 18: Oscillating CurrentsTheory and Calculation of Electric Circuits2Workbenchlines 31657-33200
Chapter 6: Oscillating Currents,Theory and Calculation of Transient Electric Phenomena and Oscillations2Workbenchlines 5312-6797
Chapter 3: The Natural Period Of The Transmission LineTheory and Calculation of Transient Electric Phenomena and Oscillations2Workbenchlines 21721-23178
Chapter 3: The Individualistic Era: From Competition to Co-operationAmerica and the New Epoch1Workbenchlines 874-1745
Chapter 7: The Other European Nations in the Individualistic EraAmerica and the New Epoch1Workbenchlines 3207-3740
Chapter 15: The American NationAmerica and the New Epoch1Workbenchlines 6598-6974
Chapter 16: The Future CorporationAmerica and the New Epoch1Workbenchlines 6975-7567
Mathematical Appendix 5: Appendix: Synchronous OperationInvestigation of Some Trouble in the Generating System of the Commonwealth Edison Co.1WorkbenchPDF pages 27-68, lines 2165-5013
Lecture 6: Double-Energy TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients1Workbenchlines 3721-4369
Lecture 6: Double-Energy TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients1Workbenchlines 3287-3955
Lecture 2: Conclusions From The Relativity TheoryFour Lectures on Relativity and Space1Workbenchlines 736-2388
Lecture 3: Light And Power DistributionGeneral Lectures on Electrical Engineering1Workbenchlines 983-1526
Lecture 1: Nature And Different Forms Of RadiationRadiation, Light and Illumination1Workbenchlines 608-1548
Lecture 2: Relation Of Bodies To RadiationRadiation, Light and Illumination1Workbenchlines 1549-2365
Apparatus Section 6: Alternating-current Transformer: Heating and VentilationTheoretical Elements of Electrical Engineering1Workbenchlines 18461-18520
Apparatus Section 1: Synchronous Converters: GeneralTheoretical Elements of Electrical Engineering1Workbenchlines 13189-13795
Apparatus Section 9: Synchronous Converters: Inverted ConvertersTheoretical Elements of Electrical Engineering1Workbenchlines 15735-15810
Chapter 25: Distortion Of Wave-Shape And Its CausesTheory and Calculation of Alternating Current Phenomena1Workbenchlines 29375-32539
Chapter 26: Effects Of Higher HarmonicsTheory and Calculation of Alternating Current Phenomena1Workbenchlines 32540-33010
Chapter 28: General Polyphase SystemsTheory and Calculation of Alternating Current Phenomena1Workbenchlines 34777-34928
Chapter 20: Beactiox MachinesTheory and Calculation of Alternating Current Phenomena1Workbenchlines 22388-23273
Chapter 25: General Polyphase SystemsTheory and Calculation of Alternating Current Phenomena1Workbenchlines 23643-23780
Chapter 10: Mutual InductanceTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 10475-12216
Chapter 4: Arc RectificationTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 17755-19259
Chapter 7: Distribution Of Alternating-Current Density In ConductorTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 24981-26094
Chapter 9: Inductive DischargesTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 34897-40349
Lecture 6: Luminescence - 31 hit(s)

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... he disruptive voltage, while with a supply voltage exceeding the disruptive voltage of the gas between the terminals, current exists, but the terminal voltage is apparently indepen- dent of the current, that is, if the other conditions as temperature, gas pressure, etc., remain the same, the terminal voltage of the Geissler tube or the spark gap remains the same and independent of the current, and the current is determined by the impedance between the. Geissler tube or spark gap and the source of 100 RADIATION, L ...
Chapter 2: Electric Conduction. Gas And Vapor - 26 hit(s)

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... d at the terminals (hot cathode), are the conductors. Such conduction thus exists also in a perfect vacuum, and may be accompanied by practically no luminescence. 28 ELECTRIC CONDUCTION . 29 Disruptive Conduction 19. Spark conduction at atmospheric pressure is the disruptive spark, streamers, and corona. In a partial vacuum, it is the Geissler discharge or glow discharge. Spark conduction is dis- continuous, that is, up to a certain voltage, the "disruptive voltage," no conduction exists, except perhaps the ...
Chapter 33: Efficiency Of Systems - 18 hit(s)

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... minimum potential difference in the system, or the potential difference per circuit or phase of the system. 431 432 ALTERNATING-CURRENT PHENOMENA In low-potential circuits, as secondary networks, where the potential is not limited by the insulation strain, but by the potential of the apparatus connected into the system, as incan- descent lamps, the proper basis of comparison is equality of the potential per branch of the system, or per phase. On the other hand, in long-distance transmissions where the po ...
Lecture 5: Temperature Radiation - 17 hit(s)

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... ist between different bodies regarding their rate of evaporation. Thus water and benzine have practically the same boiling point, but at the same distance below the boiling point, benzine evaporates much faster than water; that is, has a much higher vapor tension. Carbon has a very high vapor tension, that is, shows a very rapid evaporation far below the boiling point, and since in the incan- descent lamp the carbon vapor condenses and is deposited on the globe and carbon is black, it blackens the globe and obstru ...
Lecture 17: Arc Lighting - 16 hit(s)

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... liquid body the vibrating particles are so close together as to interfere with each other. If you could set a body in vibration, in which the vibrating particles, atoms or molecules, are so far apart as not to interfere with each other, as in a gas at low pressure, then they would execute their own periods of vibration, and then the light from such a body would not be a radiation of all wave lengths, but we would get radiations of 244 GENERAL LECTURES only a few definite wave lengths, or a line spectrum. So in- ...
Lecture 1: General Review - 11 hit(s)

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... verter substation. The use of direct current is therefore restricted to those places where a fairly concentrated load exists, as in large cities; while in the suburbs, and in small cities and villages, where the load is too scattered to reach from one low tension supply point, sufficient customers to load a substation, the alternating current must be used, as it requires merely a step- down transformer which needs no attention. In the interior of large cities, the alternating current system is at a disadvantage, ...
Lecture 8: Traveling Waves - 9 hit(s)

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... ions 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 - 9 hit(s)

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... 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 5: Long Distance Transmission - 7 hit(s)

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... nce of the transformer building up with the line capacity. In those transformer connections in which several high 74 GENERAL LECTURES potential coils of different transformers are connected between the transmission wires, this may occur if the low tension coil of one of the transformers accidentally opens and the high potential coil of this transformer then acts as inductive react- ance in series with the line capacity in the circuit of the other transformer. ~r I ^ T Fife. 21. This may occur for ...
Lecture 11: Lightning Protection - 7 hit(s)

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... arrester. Series resistance, however, also limited the discharge current, and with very heavy discharges, such lightning arresters with series resistance failed to protect the circuits, that is, failed to discharge the abnormal voltage without destructive pressure rise. This difficulty was solved by the introduction of shunted resistances, that is, resistances shunt- ing a part of the spark gaps. All the minor discharges then pass over the resistances and the unshunted spark gaps, the LIGHTNING PROTECTION 139 r ...
Chapter 28: Copper Efficiency Of Systems - 7 hit(s)

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... n the system ; or 2d. On the basis of the minimum potential difference in the system, or the potential difference per circuit or phase of the system. In low potential circuits, as secondary networks, where the potential is not limited by the insulation strain, but by the potential of the apparatus connected into the system, as incandescent lamps, the proper basis of comparison is equality of the potential per branch of the system, or per phase. On the other hand, in long distance transmissions where the pot ...
Chapter 30: Efficiency Of Systems - 7 hit(s)

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... n the system ; or 2d. On the basis of the minimum potential difference in the system, or the potential difference per circuit or phase of the system. In low potential circuits, as secondary networks, where the potential is not limited by the insulation strain, but by the potential of the apparatus connected into the system, as incandescent lamps, the proper basis of comparison is equality of the potential per branch of the system, or per phase. On the other hand, in long distance transmissions where the pot ...
Lecture 8: Arc Lamps And Arc Lighting - 6 hit(s)

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... n of arc length and current, i, the voltage of the arc stream is ex- pressed by : k (I + I) ei = TT1-' (1 and the total arc voltage by : , *(*+*,: (2) where e0, k and Zt are constants of the terminal material (k, how- ever, varies with the gas pressure in the space in which the arc exists). This equation (2) represents the arc characteristics with good approximation, except for long low-current arcs, which usually require a higher voltage than calculated, as might be expected from the unsteady nature ...
Chapter 14: Dielectric Losses - 6 hit(s)

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... ux density in the insulating material. Thus, for instance, in the dielectric field between parallel con- ductors, at a voltage far below that which would jump from conductor to conductor, locally at the conductor surface the concentration of electrostatic stress exceeds the dielectric strength of air, and causes it to break down as corona. In solid dielectrics, under similar conditions, the breakdown due to local over-stress DIELECTRIC LOSSES 161 often may change the flux distribution so as to gradually extend ...
Chapter 3: Trigonometric Series - 5 hit(s)

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... two pressures between which the nozzle operates, is given in Fig. 54, as determined by experiment. As abscissas are used the nozzle mouth opening, that is, the widest part of the nozzle at the exhaust end, as fraction of that corresponding to the exhaust pressure, while the nozzle throat, that is, the narrowest part of the nozzle, is assumed as constant. As ordinates are plotted the efficiencies. This curve is not symmetrical, 'but falls off from the maximum, on the sides of larger nozzle mouth, far more rapidly t ...
Lecture 8: Generation - 5 hit(s)

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... ndustry; while the steam turbine in the last ten years of its development has practically replaced the steam engine in large electric generating plants. The cause of the disadvantages of the gas engine is the high maximum temperature and the high maximum pressure compared with the mean pressure in the cylinders, which is necessary to get the greater temperature range and thus the efficiency, therefore is inherent in this type of apparatus. The output depends upon the mean pressure in the cylinder, which is low; ...
Chapter 1: The Constants Of The Electric Circuit - 5 hit(s)

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... ergy always decreases from generating to receiving circuit, and the power gradient therefore is characteristic of the direc- tion of the flow of energy.) In the space outside of the conductor, during the flow of energy through the circuit, a condition of stress exists which is called the electric field of the conductor. That is, the surrounding space is not uniform, but has different electric and magnetic properties in different directions. No power is required to maintain the electric field, but energy 3 ...
Lecture 2: General Distribution - 4 hit(s)

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... .109 ohms, and so 1.88 times as great as the reactance of two con- ductors of No. I in multiple, which latter is half that of one conductor No. i, or .058 ohms, provided that the two con- ductors are used as separate circuits. In alternating current low tension distribution, the size of the conductor and so the current per conductor, is limited by the self -inductive drop, and alternating current low tension networks are therefore of necessity of smaller size than those of direct current distribution. As regar ...