Skip to content

Dielectric Field Concordance

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

561 hits

Total text matches across processed Steinmetz sections.

11 sources

Sources containing at least one matched alias.

58 sections

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

dielectric, dielectric field, dielectrics

SourceHitsSections
Theory and Calculation of Alternating Current Phenomena14510
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients1258
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients1228
Theoretical Elements of Electrical Engineering543
Theory and Calculation of Alternating Current Phenomena357
Theory and Calculation of Alternating Current Phenomena336
Theory and Calculation of Transient Electric Phenomena and Oscillations277
Four Lectures on Relativity and Space113
Theory and Calculation of Electric Circuits54
Radiation, Light and Illumination21
Theory and Calculation of Electric Apparatus21
SectionSourceHitsWorkbenchLocation
Chapter 14: Dielectric LossesTheory and Calculation of Alternating Current Phenomena106Workbenchlines 14334-15409
Lecture 2: The Electric FieldElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients55Workbenchlines 1003-1658
Lecture 2: The Electric FieldElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients55Workbenchlines 883-1530
Theory Section 19: Fields of ForceTheoretical Elements of Electrical Engineering40Workbenchlines 7737-7990
Lecture 10: Continual And Cumulative OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients28Workbenchlines 6804-8485
Lecture 6: Double-Energy TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients26Workbenchlines 3721-4369
Lecture 6: Double-Energy TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients26Workbenchlines 3287-3955
Lecture 10: Inductance And Capacity Of Round Parallel ConductorsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients25Workbenchlines 6089-7274
Chapter 11: Foucault Or Eddy CurrentsTheory and Calculation of Alternating Current Phenomena20Workbenchlines 8384-9380
Chapter 11: Fouoault Or Eddy 0Ubbent8Theory and Calculation of Alternating Current Phenomena19Workbenchlines 10500-11563
Chapter 37: Quarter-Phase SystemTheory and Calculation of Alternating Current Phenomena18Workbenchlines 38393-40115
Theory Section 20: NomenclatureTheoretical Elements of Electrical Engineering12Workbenchlines 7991-8291
Chapter 1: The Constants Of The Electric CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations12Workbenchlines 1317-1992
Chapter 15: Distributed Capacity, Inductance, Resistance, And LeakageTheory and Calculation of Alternating Current Phenomena9Workbenchlines 15410-16076
Chapter 12: Dibtbisnted Capacity, Inductance, Besistance, AndTheory and Calculation of Alternating Current Phenomena8Workbenchlines 11564-12672
Chapter 13: Distributed Capacity, Inductance, Resistance, And LeakageTheory and Calculation of Alternating Current Phenomena8Workbenchlines 9741-11604
Chapter 2: Long-Distance Transmission LineTheory and Calculation of Transient Electric Phenomena and Oscillations8Workbenchlines 19339-21720
Lecture 1: Nature And Origin Of TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients6Workbenchlines 557-1002
Lecture 1: Nature And Origin Of TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients6Workbenchlines 460-882
Lecture 2: Conclusions From The Relativity TheoryFour Lectures on Relativity and Space6Workbenchlines 736-2388
Chapter 33: Efficiency Of SystemsTheory and Calculation of Alternating Current Phenomena5Workbenchlines 36515-37127
Lecture 5: Single-Energy Tra.Nsient Of Ironclad CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients4Workbenchlines 3387-3720
Lecture 5: Single-Energy Transient Of Ironclad CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients4Workbenchlines 2972-3286
Lecture 4: The Characteristics Of Space A. The Geometry Of The Gravitational FieldFour Lectures on Relativity and Space4Workbenchlines 3595-6820
Chapter 9: Inductive DischargesTheory and Calculation of Transient Electric Phenomena and Oscillations3Workbenchlines 34897-40349
Lecture 3: Single-Energy Transients In Continuous Current CircuitsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 1659-2484
Lecture 7: Line OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 4370-5278
Lecture 8: Traveling WavesElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 5279-6124
Lecture 3: Single-Energy Transients In Continuous Current CircuitsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 1531-2161
Lecture 7: Line OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 3956-4744
Lecture 8: Traveling WavesElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 4745-5520
Lecture 2: Relation Of Bodies To RadiationRadiation, Light and Illumination2Workbenchlines 1549-2365
Theory Section 11: Capacity and CondensersTheoretical Elements of Electrical Engineering2Workbenchlines 3586-3760
Chapter 1: IntroductionTheory and Calculation of Alternating Current Phenomena2Workbenchlines 1120-1683
Chapter 1: IntroductionTheory and Calculation of Alternating Current Phenomena2Workbenchlines 1224-1727
Chapter 28: Copper Efficiency Of SystemsTheory and Calculation of Alternating Current Phenomena2Workbenchlines 26584-27052
Chapter 1: IntroductionTheory and Calculation of Alternating Current Phenomena2Workbenchlines 963-1366
Chapter 30: Efficiency Of SystemsTheory and Calculation of Alternating Current Phenomena2Workbenchlines 25136-25597
Chapter 14: Phase Conversion And Single-Phase GenerationTheory and Calculation of Electric Apparatus2Workbenchlines 17125-18412
Chapter 1: Electric Conduction. Soled And LiquidTheory and Calculation of Electric Circuits2Workbenchlines 959-3894
Lecture 3: Gravitation And The Gravitational FleldFour Lectures on Relativity and Space1Workbenchlines 2389-3594
Chapter 6: Topographic MethodTheory and Calculation of Alternating Current Phenomena1Workbenchlines 3267-3618
Chapter 12: Effective Resistance And ReactanceTheory and Calculation of Alternating Current Phenomena1Workbenchlines 10718-13483
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 35: Balanced Symmetrical Polyphase SystemsTheory and Calculation of Alternating Current Phenomena1Workbenchlines 37453-37957
Chapter 10: FTheory and Calculation of Alternating Current Phenomena1Workbenchlines 8269-10499
Chapter 21: Dibtobtiox Of Wavs-Shafe And Its CausesTheory and Calculation of Alternating Current Phenomena1Workbenchlines 23274-24559
Chapter 6: Topographic MethodTheory and Calculation of Alternating Current Phenomena1Workbenchlines 2774-3131
Chapter 10: Effective Resistance And ReactanceTheory and Calculation of Alternating Current Phenomena1Workbenchlines 6957-8383
Chapter 22: Distortion Of Wave-Shape And Its CausesTheory and Calculation of Alternating Current Phenomena1Workbenchlines 21190-21982
Chapter 5: MagnetismTheory and Calculation of Electric Circuits1Workbenchlines 9062-11050
Chapter 9: Wave Screens. Even HarmonicsTheory and Calculation of Electric Circuits1Workbenchlines 16964-17631
Chapter 18: Oscillating CurrentsTheory and Calculation of Electric Circuits1Workbenchlines 31657-33200
Chapter 2: IntroductionTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 1993-2658
Chapter 5: Distributed Series CapacityTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 23586-23947
Chapter 1: General EquationsTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 27761-28694
Chapter 3: Standing WavesTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 29316-30243
Chapter 14: Dielectric Losses - 106 hit(s)

Open source text | Open chapter workbench

CHAPTER XIV DIELECTRIC LOSSES Dielectric Hysteresis 116. Just as magnetic hysteresis and eddy currents give a power component in the inductive reactance, as "effective resistance," so the energy losses in the dielectric lead to a power component in the condensive reactance, ...
Lecture 2: The Electric Field - 55 hit(s)

Open source text | Open chapter workbench

... ircles 10 THE ELECTRIC FIELD. 11 are crowded together between the conductors, and the magnetic field consists of eccentric circles surrounding the conductors, as shown by the drawn lines in Fig. 9. An electrostatic, or, as more properly called, dielectric field, issues from the conductors, that is, a dielectric flux passes between the conductors, which is measured by the number of lines of dielectric force ^. With a single conductor, the lines of dielectric force are radial straight lines, as shown dotted in Fig ...
Lecture 2: The Electric Field - 55 hit(s)

Open source text | Open chapter workbench

... ircles 10 THE ELECTRIC FIELD. 11 are crowded together between the conductors, and the magnetic field consists of eccentric circles surrounding the conductors, as shown by the drawn lines in Fig. 9. An electrostatic, or, as more properly called, dielectric field, issues from the conductors, that is, a dielectric flux passes between the conductors, which is measured by the number of lines of dielectric force ty. With a single conductor, the lines of dielectric force are radial straight lines, as shown dotted in Fi ...
Theory Section 19: Fields of Force - 40 hit(s)

Open source text | Open chapter workbench

... e earth, and water to run down hill — and this space thus is a field of gravitational force, the earth the gram- motive force. In the space surrounding conductors having a high potential difference, we observe a field of dielectric force, that is, electro- static or dielectric forces are exerted, and the potential difference between the conductors is the electromotive force of the dielectric field. The force exerted by the earth as gravimotive force, o ...
Lecture 10: Continual And Cumulative Oscillations - 28 hit(s)

Open source text | Open chapter workbench

... enon by which the stored energy readjusts itself to a change of circuit conditions. In an oscilla- tory transient, the difference of stored energy of the previous and the after condition of the circuit, at a circuit change, oscillates between magnetic and dielectric energy. As there always must be some energy dissipation in the circuit, the oscillating energy of the transient must steadily decline, that is, the transient must die out, at a rate depending on the energy dissipation in the cir- cuit. Thus, the oscilla ...
Lecture 6: Double-Energy Transients - 26 hit(s)

Open source text | Open chapter workbench

... energy is stored by the current i, as magnetic field. To = -, (2) r where L = inductance = coefficient of energy storage by the cur- rent, r = resistance = coefficient of power dissipation by the current. If the energy is stored by the voltage e, as dielectric field, the duration of the transient would be TV - -, (3) g 59 60 ELECTRIC DISCHARGES, WAVES AND IMPULSES. where C = capacity = coefficient of energy storage by the volt- age, in the dielectric field, and g = conductance = coefficient of power consumpt ...
Lecture 6: Double-Energy Transients - 26 hit(s)

Open source text | Open chapter workbench

... , if energy is stored by the current i, as magnetic field, T0 = £, (2) where L = inductance = coefficient of energy storage by the cur- rent, r = resistance = coefficient of power dissipation by the current. If the energy is stored by the voltage e, as dielectric field, the duration of the transient would be TJ = -, (3) s/ 59 60 ELECTRIC DISCHARGES, WAVES AND IMPULSES. where C = capacity = coefficient of energy storage by the volt- age, in the dielectric field, and g = conductance = coefficient of power consump ...
Lecture 10: Inductance And Capacity Of Round Parallel Conductors - 25 hit(s)

Open source text | Open chapter workbench

... inkages of the mag- netic flux to the current, £ = ?- (i) i/ where <i> = magnetic flux or number of lines of magnetic force, and n the number of times which each line of magnetic force interlinks with the current i. The capacity is the ratio of the dielectric flux to the voltage, where \f/ is the dielectric flux, or number of lines of dielectric force, and e the voltage which produces it. With a single round conductor without return conductor (as wireless antennae) or with the return conductor at infinite d ...
Chapter 11: Foucault Or Eddy Currents - 20 hit(s)

Open source text | Open chapter workbench

... mutual inductance ; ^ = effective reactance of mutual inductance. The susceptance of mutual inductance is negative, or of opposite sign from the reactance of self-inductance. Or, Mutual inductance consumes energy and decreases the self- inductance. Dielectric and Electrostatic Phenomena. 98. While magnetic hysteresis and eddy currents can be considered as the energy component of inductance, con- densance has an energy component also, namely, dielectric hysteresis. In an alternating magnetic field, energy is co ...
Chapter 11: Fouoault Or Eddy 0Ubbent8 - 19 hit(s)

Open source text | Open chapter workbench

... b = — ^-^^^ — ■* = effective susceptance of mutual inductance. The susceptance of mutual inductance is negative, or of opposite sign from the susceptance of self-inductance. Or, Mutual itidtutance consumes energy and decreases the self- inductatice. Dielectric and Electrostatic Phenomena, 98. While magnetic hysteresis and eddy currents can be considered as the energy component of inductance, cori- densance has an energy component also, called dielectric hysteresis. In an alternating magnetic field, energy is c ...
Chapter 37: Quarter-Phase System - 18 hit(s)

Open source text | Open chapter workbench

... ts of half-axis OB' downward; the complex imaginary or general numbers are represented by the points outside of the coordinate axes. INDEX Absolute values of complex quanti- ties, 37 Actual generated e.m.f., alternator, 272 Admittance, 55 of dielectric, 154 due to eddy currents, 137 to hysteresis, 129 Admittivity of dielectric circuit, 160 Air-gap in magnetic circuit, 119, 132 Ambiguity of vectors, 39 Amplitude, 6, 20 Apparent capacity of distorted wave, 386 efficiency of induction motor, 234 i ...
Theory Section 20: Nomenclature - 12 hit(s)

Open source text | Open chapter workbench

... I. E. E., but as far as possible standard letters have been used, and script letters avoided as impracticable or at least inconvenient in writing and still more in typewriting. Therefore F has been chosen for m.m.f., and dielectric field intensity changed to K. Also, a few symbols not contained in the Standardization Rules had to be added. NOMENCLATURE TABLE OP SYMBOLS 119 Symbol Name Unit Character E, e. Voltage Volt Electrical I, i. . Pote ...
Chapter 1: The Constants Of The Electric Circuit - 12 hit(s)

Open source text | Open chapter workbench

... as that factor of the electric power P which is proportional to the electrostatic field. Current i and voltage e, therefore, are mathematical fictions, factors of the power P, introduced to represent respectively the magnetic and the electrostatic or " dielectric " phenomena. The current i is measured by the magnetic action of a circuit, as in the ammeter; the voltage e, by the electrostatic action of a circuit, as in the electrostatic voltmeter, or by producing a current i by the voltage e and measuring this cur ...
Chapter 15: Distributed Capacity, Inductance, Resistance, And Leakage - 9 hit(s)

Open source text | Open chapter workbench

... r, x, g, b, will always be consid- ered as the coefficients of the power and reactive components of current and e.m.f. — ^that is, as the effective quantities — so that the results are directly appHcable to the general electric circuit containing iron and dielectric losses. Introducing now, in Chapters VIII, to XI, instead of "ohmic resistance," the term "effective resistance," etc., as discussed in the preceding chapter, the results apply also — within the range discussed in the preceding chapter — to circuits cont ...
Chapter 12: Dibtbisnted Capacity, Inductance, Besistance, And - 8 hit(s)

Open source text | Open chapter workbench

... nstance, that the line conductors are of 1 cm diameter, and at a distance from each other of 50 cm, and that the length of transmission is 50 km, we get the capacity of the transmission line from the formula — c = microfarads, 4 log nat -^ where K = dielectric constant of the surrounding medium = 1 in air ;. / = length of conductor = 5 X 10* cm. ; d = distance of conductors from each other = 50 cm. ; 8 = diameter of conductor = 1 cm. Since C = .3 microfarads, the capacity reactance is 10« . 152 AL ...
Chapter 13: Distributed Capacity, Inductance, Resistance, And Leakage - 8 hit(s)

Open source text | Open chapter workbench

... e conductors are of 1 cm. diameter, and at a distance from each other of 50 cm., and that the length of transmission is 50 km., we get the capacity of the transmission line from the formula — C = 1.11 X 10 -«K/ -=- 4 loge 2 d/ 8 microfarads, where K = dielectric constant of the surrounding medium = 1 in air ; / = length of conductor = 5 x 106 cm. ; d = distance of conductors from each other = 50 cm. ; 8 = diameter of conductor = 1 cm. Since C = .3 microfarads, the capacity reactance is x — 106 / 2 TT NC ohm ...
Chapter 2: Long-Distance Transmission Line - 8 hit(s)

Open source text | Open chapter workbench

... very serious at high fre- quencies such as those of telephone currents. The effect of eddy currents has already been referred to under " mutual inductance," of which if is a power component. The alternating electrostatic field of force expends power in dielectrics by what is called dielectric hysteresis. In concentric cables, where the electrostatic gradient in the dielectric is com- paratively large, the dielectric hysteresis may at high potentials consume considerable amounts of power. The dielectric hystere- sis ...
Lecture 1: Nature And Origin Of Transients - 6 hit(s)

Open source text | Open chapter workbench

... d does not represent the entire phenome- non. While electric power flows over the line A, there is a magnetic field surrounding the line conductors, and an electrostatic field issuing from the line conductors. The magnetic field and the electrostatic or " dielectric " field represent stored energy. Thus, during the permanent conditions of the flow of power through the circuit Fig. 3, there is electric energy stored in the space surround- ing the line conductors. There is energy stored also in the genera- tor and in t ...