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Energy Storage in Fields Concordance

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

213 hits

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12 sources

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42 sections

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

energy of the field, energy stored, stored energy, stored in the field

SourceHitsSections
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients7510
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients719
Theory and Calculation of Transient Electric Phenomena and Oscillations4311
General Lectures on Electrical Engineering112
Theoretical Elements of Electrical Engineering31
Theory and Calculation of Electric Circuits33
Radiation, Light and Illumination21
Theory and Calculation of Alternating Current Phenomena11
Theory and Calculation of Electric Apparatus11
Four Lectures on Relativity and Space11
Theory and Calculation of Alternating Current Phenomena11
Theory and Calculation of Alternating Current Phenomena11
SectionSourceHitsWorkbenchLocation
Lecture 1: Nature And Origin Of TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients25Workbenchlines 557-1002
Lecture 1: Nature And Origin Of TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients25Workbenchlines 460-882
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
Chapter 1: The Constants Of The Electric CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations11Workbenchlines 1317-1992
Lecture 7: High Frequency Oscillations And SurgesGeneral Lectures on Electrical Engineering10Workbenchlines 3508-3780
Chapter 7: Power And Energy Of The Complex CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations10Workbenchlines 33528-34202
Lecture 6: Double-Energy TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients8Workbenchlines 3721-4369
Lecture 9: Oscillations Of The Compound CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients8Workbenchlines 6125-6803
Lecture 6: Double-Energy TransientsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients8Workbenchlines 3287-3955
Lecture 9: Oscillations Of The Compound CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients8Workbenchlines 5521-6088
Chapter 6: Transition Points And The Complex CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations6Workbenchlines 32709-33527
Lecture 2: The Electric FieldElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients5Workbenchlines 1003-1658
Lecture 3: Single-Energy Transients In Continuous Current CircuitsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients5Workbenchlines 1659-2484
Lecture 2: The Electric FieldElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients5Workbenchlines 883-1530
Lecture 3: Single-Energy Transients In Continuous Current CircuitsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients5Workbenchlines 1531-2161
Chapter 6: Oscillating Currents,Theory and Calculation of Transient Electric Phenomena and Oscillations5Workbenchlines 5312-6797
Lecture 4: Single-Energy Transients In Alternating Current CircuitsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients4Workbenchlines 2485-3386
Lecture 10: Continual And Cumulative OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients4Workbenchlines 6804-8485
Lecture 4: Single-Energy Transients In Alternating Current CircuitsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients4Workbenchlines 2162-2971
Theory Section 6: Self-inductance of Continuous-current CircuitsTheoretical Elements of Electrical Engineering3Workbenchlines 1785-2249
Chapter 7: Power And Energy Of The Complex Circuit. 513Theory and Calculation of Transient Electric Phenomena and Oscillations3Workbenchlines 1228-1261
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 6: LuminescenceRadiation, Light and Illumination2Workbenchlines 5077-6608
Chapter 3: The Natural Period Of The Transmission LineTheory and Calculation of Transient Electric Phenomena and Oscillations2Workbenchlines 21721-23178
Chapter 5: Free OscillationsTheory and Calculation of Transient Electric Phenomena and Oscillations2Workbenchlines 31451-32708
Lecture 5: Single-Energy Tra.Nsient Of Ironclad CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients1Workbenchlines 3387-3720
Lecture 5: Single-Energy Transient Of Ironclad CircuitElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients1Workbenchlines 2972-3286
Lecture 2: Conclusions From The Relativity TheoryFour Lectures on Relativity and Space1Workbenchlines 736-2388
Lecture 5: Long Distance TransmissionGeneral Lectures on Electrical Engineering1Workbenchlines 2562-3132
Chapter 32: Transformation Of Polyphase SystemsTheory and Calculation of Alternating Current Phenomena1Workbenchlines 36062-36514
Chapter 27: Tbansfobmation Of Polyphase SystemsTheory and Calculation of Alternating Current Phenomena1Workbenchlines 26428-26583
Chapter 29: Transformation Of Polyphase SystemsTheory and Calculation of Alternating Current Phenomena1Workbenchlines 24805-25135
Chapter 14: Phase Conversion And Single-Phase GenerationTheory and Calculation of Electric Apparatus1Workbenchlines 17125-18412
Chapter 10: Instability Of Circuits : The ArcTheory and Calculation of Electric Circuits1Workbenchlines 17632-21381
Chapter 11: Instability Of Circuits: Induction And Syn Chronous MotorsTheory and Calculation of Electric Circuits1Workbenchlines 21382-22633
Chapter 13: Reactance Of Synchronous MachinesTheory and Calculation of Electric Circuits1Workbenchlines 23466-24022
Chapter 2: IntroductionTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 1993-2658
Chapter 5: Resistance, Inductance, And Capacity In Series Condenser Charge And DischargeTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 4072-5311
Chapter 2: Discussion Of General EquationsTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 28695-29315
Chapter 9: Inductive DischargesTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 34897-40349
Lecture 1: Nature And Origin Of Transients - 25 hit(s)

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... re 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 the load ; for instance, the mech ...
Lecture 1: Nature And Origin Of Transients - 25 hit(s)

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... re 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 the load ; for instance, the mech ...
Lecture 8: Traveling Waves - 13 hit(s)

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... al short circuit a quantity of magnetic energy is impressed upon a part of the circuit. This energy then gradually distributes over the circuit, as indicated by the curves B, C, etc., of Fig. 39, that is, moves along the circuit, and the dissipation of the stored energy thus occurs by a flow of power along the circuit. 90 ELECTRIC DISCHARGES, WAVES AND IMPULSES. Such a flow of power must occur in a circuit containing sec- tions of different dissipation constants u. For instance, if in a circuit consisting of an unloa ...
Lecture 8: Traveling Waves - 13 hit(s)

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... al short circuit a quantity of magnetic energy is impressed upon a part of the circuit. This energy then gradually distributes over the circuit, as indicated by the curves B, C, etc., of Fig. 39, that is, moves along the circuit, and the dissipation of the stored energy thus occurs by a flow of power along the circuit. 90 ELECTRIC DISCHARGES, WAVES AND IMPULSES. Such a flow of power must occur in a circuit containing sections of different dissipation constants u. For instance, if a circuit consists of an unloaded tra ...
Chapter 1: The Constants Of The Electric Circuit - 11 hit(s)

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... t elapse during which the energy of the electric field is stored, and the generator therefore gives more power than consumed in the conductor and delivered at the receiving end; again, the flow of electric energy cannot be stopped instantly, but first the energy stored in the electric field has to be expended. As result hereof, where the flow of electric energy pulsates, as in an alternating- current circuit, continuously electric energy is stored in the field during a rise of the power, and returned to the circuit aga ...
Lecture 7: High Frequency Oscillations And Surges - 10 hit(s)

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... age ■^ occurs as electrostatic energy, or electrostatic charge due to the voltage on the line (capacity) ; and as electromag- netic energy, or magnetic field of the current in the line (inductance). In the long distance transmission line, both amounts of stored energy are very considerable, and of about equal magnitude; the former varying with the voltage, the latter with the current in the line. Any change of the voltage on the line, or the current in the line, or the relation between volt- age and current, therefore ...
Chapter 7: Power And Energy Of The Complex Circuit - 10 hit(s)

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... ction of length A' to the rest of the circuit, or received by the section from the rest of the circuit, is proportional to the length of the section, A', to its trans- fer constant, s, and to the sum of the power of main wave and reflected wave. 51. The energy stored by the inductance L of a circuit element dXj that is, in the magnetic field of the circuit, is 'LV dwl =-^~A where U = inductance per unit length of circuit expressed by the distance coordinate A. Since L = the inductance per unit length of circuit, ...
Lecture 6: Double-Energy Transients - 8 hit(s)

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LECTURE VI. DOUBLE-ENERGY TRANSIENTS. 24. In a circuit in which energy can be stored in one form only, the change in the stored energy which can take place as the result of a change of the circuit conditions is an increase or decrease. The transient can be separated from the permanent condition, and then always is the representation of a gradual decrease of energy. Even if the stored ene ...
Lecture 9: Oscillations Of The Compound Circuit - 8 hit(s)

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... ms of such circuits have been shown in the previous lecture. If we have a circuit consisting of sections 1, 2, 3 . . . , of the respective lengths (in velocity measure) Xi, X2, X3 . . . , this entire circuit, when left to itself, gradually dissipates its stored energy by a transient. As function of the time, this transient must decrease at the same rate Uq throughout the entire circuit. Thus the time decrement of all the sections must be Every section, however, has a power-dissipation constant, Ui, U2, U3 . . . , whic ...
Lecture 6: Double-Energy Transients - 8 hit(s)

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LECTURE VI. DOUBLE-ENERGY TRANSIENTS. 24. In a circuit in which energy can be stored in one form only, the change in the stored energy which can take place as the result of a change of the circuit conditions is an increase or decrease. The transient can be separated from the permanent condition, and then always is the representation of a gradual decrease of energy. Even if the stored ene ...
Lecture 9: Oscillations Of The Compound Circuit - 8 hit(s)

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... ms of such circuits have been shown in the previous lecture. If we have a circuit consisting of sections 1, 2, 3 . . . , of the respective lengths (in velocity measure) Xi, X2, X3 . . . , this entire circuit, when left to itself, gradually dissipates its stored energy by a transient. As function of the time, this transient must decrease at the same rate u0 throughout the entire circuit. Thus the time decrement of all the sections must be 6-**. Every section, however, has a power-dissipation constant, u\t Uz, u3 . . ...
Chapter 6: Transition Points And The Complex Circuit - 6 hit(s)

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... ch is the same throughout the entire circuit. In an isolated section, of time constant u, the time decrement, from Chapters III and V, is, however, e~ut; that is, with the decrement e~ut the wave dies out in the isolated sec- tion at the rate at which its stored energy is dissipated by the power lost in resistance and conductance. In a section of the circuit connected to other sections the time decrement e~U(* does not correspond to the power dissipation in the section; that is, the wave does not die out in each section ...
Lecture 2: The Electric Field - 5 hit(s)

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... electric field of the conductor. 8. The magnetic field or magnetic flux of the circuit, $, is pro- portional to the current, i, with a proportionality factor, L, which is called the inductance of the circuit. $ = L^.* (1) The magnetic field represents stored energy ly. To produce it, power, p, must therefore be supplied by the circuit. Since power is current times voltage : P = e'i, (2) * n^, if the flux <l> interlinks the circuit n fold. 12 ELECTRIC DISCHARGES, WAVES AND IMPULSES. to produce the magnetic fie ...
Lecture 3: Single-Energy Transients In Continuous Current Circuits - 5 hit(s)

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LECTURE III. SINGLE-ENERGY TRANSIENTS IN CONTINUOUS- CURRENT CIRCUITS. 13. The simplest electrical transients are those in circuits in which energy can be stored in one form only, as in this case the change of stored energy can consist only of an increase or decrease ; but no surge or oscillation between several forms of energy can exist. Such circuits are most of the low- and medium-voltage circuits, — 220 volts, 600 volts, and 2200 volts. In them the capac- ity is small, d ...
Lecture 2: The Electric Field - 5 hit(s)

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... ctric field of the conductor. 8. The magnetic field or magnetic flux of the circuit, <£, is pro- portional to the current, i, with a proportionality factor, L, which is called the inductance of the circuit. = Li. (1) The magnetic field represents stored energy w. To produce it, power, p, must therefore be supplied by the circuit. Since power is current times voltage, p = e'i. (2) 12 ELECTRIC DISCHARGES, WAVES AND IMPULSES. To produce the magnetic field $ of the current i, a voltage ef must be consumed in ...
Lecture 3: Single-Energy Transients In Continuous Current Circuits - 5 hit(s)

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LECTURE III. SINGLE-ENERGY TRANSIENTS IN CONTINUOUS- CURRENT CIRCUITS. 13. The simplest electrical transients are those in circuits in which energy can be stored in one form only, as in this case the change of stored energy can consist only of an increase or decrease ; but no surge or oscillation between several forms of energy can exist. Such circuits are most of the low- and medium-voltage circuits, — 220 volts, 600 volts, and 2200 volts. In them the capac- ity is small, d ...
Chapter 6: Oscillating Currents, - 5 hit(s)

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... an effective resistance, which increases the rapidity of the decay of the oscillation, and thus limits the power, and, when approaching the critical value, also lowers the frequency. This is obvious, since the oscillating current is the dissipation of the energy stored electrostatically in the condenser, and the higher the resistance of the circuit, the more rapidly is this energy dissipated, that is, the faster the oscillation dies out. With a resistance of the circuit sufficiently low to give a fairly well sustained ...
Lecture 4: Single-Energy Transients In Alternating Current Circuits - 4 hit(s)

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LECTURE IV. SINGLE-ENERGY TRANSIENTS IN ALTERNATING- CURRENT CIRCUITS. 17. Whenever the conditions of an electric circuit are changed in such a manner as to require a change of stored energy, a transi- tion period appears, during which the stored energy adjusts itself from the condition existing before the change to the condition after the change. The currents in the circuit during the transition period can be considered as consisting of the ...