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Resonance Concordance

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

120 hits

Total text matches across processed Steinmetz sections.

12 sources

Sources containing at least one matched alias.

52 sections

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

resonance, resonant

SourceHitsSections
Theory and Calculation of Alternating Current Phenomena2111
Theory and Calculation of Electric Circuits206
Theory and Calculation of Alternating Current Phenomena1910
General Lectures on Electrical Engineering154
Theory and Calculation of Alternating Current Phenomena137
Radiation, Light and Illumination81
Theory and Calculation of Transient Electric Phenomena and Oscillations83
Theory and Calculation of Electric Apparatus73
Engineering Mathematics: A Series of Lectures Delivered at Union College32
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients32
Theoretical Elements of Electrical Engineering22
Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients11
SectionSourceHitsWorkbenchLocation
Lecture 4: Chemical And Physical Effects Of RadiationRadiation, Light and Illumination8Workbenchlines 3639-3945
Lecture 6: Higher Harmonics Of The Generator WaveGeneral Lectures on Electrical Engineering6Workbenchlines 3133-3507
Lecture 17: Arc LightingGeneral Lectures on Electrical Engineering6Workbenchlines 9920-12795
Chapter 26: Effects Of Higher HarmonicsTheory and Calculation of Alternating Current Phenomena6Workbenchlines 32540-33010
Chapter 14: Constant-Potential Constant-Current Trans FormationTheory and Calculation of Electric Circuits6Workbenchlines 24023-27995
Chapter 2: Long-Distance Transmission LineTheory and Calculation of Transient Electric Phenomena and Oscillations6Workbenchlines 19339-21720
Chapter 20: RiTheory and Calculation of Alternating Current Phenomena5Workbenchlines 24560-25119
Chapter 23: Effects Of Higher HarmonicsTheory and Calculation of Alternating Current Phenomena5Workbenchlines 21983-22448
Chapter 10: Instability Of Circuits : The ArcTheory and Calculation of Electric Circuits5Workbenchlines 17632-21381
Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive ReactanceTheory and Calculation of Alternating Current Phenomena3Workbenchlines 4674-6992
Chapter 8: Circuits Containing Resistance, Inductance, And CapacityTheory and Calculation of Alternating Current Phenomena3Workbenchlines 3577-5333
Chapter 4: Induction Motor With Secondary ExcitationTheory and Calculation of Electric Apparatus3Workbenchlines 5555-8554
Chapter 9: Wave Screens. Even HarmonicsTheory and Calculation of Electric Circuits3Workbenchlines 16964-17631
Chapter 18: Oscillating CurrentsTheory and Calculation of Electric Circuits3Workbenchlines 31657-33200
Lecture 10: Continual And Cumulative OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients2Workbenchlines 6804-8485
Chapter 7: Numerical CalculationsEngineering Mathematics: A Series of Lectures Delivered at Union College2Workbenchlines 21989-25587
Lecture 9: Hunting Of Synchronous MachinesGeneral Lectures on Electrical Engineering2Workbenchlines 4218-4594
Chapter 24: Synchronous MotorTheory and Calculation of Alternating Current Phenomena2Workbenchlines 25682-29374
Chapter 27: Symbolic Representation Of General Alternating WavesTheory and Calculation of Alternating Current Phenomena2Workbenchlines 33011-34776
Chapter 32: Transformation Of Polyphase SystemsTheory and Calculation of Alternating Current Phenomena2Workbenchlines 36062-36514
Chapter 8: CapacityTheory and Calculation of Alternating Current Phenomena2Workbenchlines 3872-6370
Chapter 9: Kbsistanci: And Kbactance Of Transmission Iine8Theory and Calculation of Alternating Current Phenomena2Workbenchlines 6371-8268
Chapter 9: Resistance And Reactance Of Transmission LinesTheory and Calculation of Alternating Current Phenomena2Workbenchlines 5334-6956
Chapter 19: Synchronous MotorTheory and Calculation of Alternating Current Phenomena2Workbenchlines 18053-19457
Chapter 24: Symbolic Representation Of General Alternating WavesTheory and Calculation of Alternating Current Phenomena2Workbenchlines 22449-23642
Chapter 1: Speed Control Of Induction MotorsTheory and Calculation of Electric Apparatus2Workbenchlines 1368-3542
Chapter 18: Surging Of Synchronous MotorsTheory and Calculation of Electric Apparatus2Workbenchlines 20975-21712
Chapter 7: Shaping Of Waves : GeneralTheory and Calculation of Electric Circuits2Workbenchlines 12222-12961
Lecture 7: Line OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients1Workbenchlines 4370-5278
Lecture 7: Line OscillationsElementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients1Workbenchlines 3956-4744
Chapter 3: Trigonometric SeriesEngineering Mathematics: A Series of Lectures Delivered at Union College1Workbenchlines 6064-15155
Lecture 5: Long Distance TransmissionGeneral Lectures on Electrical Engineering1Workbenchlines 2562-3132
Apparatus Section 2: Induction Machines: Polyphase Induction MotorTheoretical Elements of Electrical Engineering1Workbenchlines 19166-20427
Apparatus Section 15: Synchronous Machines: Fluctuating Cross Currents in Parallel OperationTheoretical Elements of Electrical Engineering1Workbenchlines 9918-10123
Chapter 1: IntroductionTheory and Calculation of Alternating Current Phenomena1Workbenchlines 1120-1683
Chapter 10: Resistance And Reactance Of TransmissionTheory and Calculation of Alternating Current Phenomena1Workbenchlines 6993-9766
Chapter 12: Effective Resistance And ReactanceTheory and Calculation of Alternating Current Phenomena1Workbenchlines 10718-13483
Chapter 17: The Alternating-Current TransformerTheory and Calculation of Alternating Current Phenomena1Workbenchlines 16521-17716
Chapter 25: Distortion Of Wave-Shape And Its CausesTheory and Calculation of Alternating Current Phenomena1Workbenchlines 29375-32539
Chapter 37: Quarter-Phase SystemTheory and Calculation of Alternating Current Phenomena1Workbenchlines 38393-40115
Chapter 1: IntroductionTheory and Calculation of Alternating Current Phenomena1Workbenchlines 1224-1727
Chapter 10: FTheory and Calculation of Alternating Current Phenomena1Workbenchlines 8269-10499
Chapter 13: Ths Alternating^Cnrrent TraxsfobmerTheory and Calculation of Alternating Current Phenomena1Workbenchlines 12673-14088
Chapter 30: Quartbr-Fhase SystemTheory and Calculation of Alternating Current Phenomena1Workbenchlines 27501-29124
Chapter 1: IntroductionTheory and Calculation of Alternating Current Phenomena1Workbenchlines 963-1366
Chapter 10: Effective Resistance And ReactanceTheory and Calculation of Alternating Current Phenomena1Workbenchlines 6957-8383
Chapter 13: Distributed Capacity, Inductance, Resistance, And LeakageTheory and Calculation of Alternating Current Phenomena1Workbenchlines 9741-11604
Chapter 14: The Alternating-Current TransformerTheory and Calculation of Alternating Current Phenomena1Workbenchlines 11605-12682
Chapter 32: Quarter-Phase SystemTheory and Calculation of Alternating Current Phenomena1Workbenchlines 25904-27405
Chapter 8: Shaping Of Waves By Magnetic SaturationTheory and Calculation of Electric Circuits1Workbenchlines 12962-16963
Chapter 7: Resistance, Inductance, And Capacity In Series In Alternating-Current CircuitTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 6798-7825
Chapter 9: Inductive DischargesTheory and Calculation of Transient Electric Phenomena and Oscillations1Workbenchlines 34897-40349
Lecture 4: Chemical And Physical Effects Of Radiation - 8 hit(s)

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... heat when it ceases to be radiation. Thus all radiations are chemical rays, that is, produce chemical action, if they strike a body which is responsive to them. The chemical action of radiation is specific to its frequency and seems to be some kind of a resonance effect. We may picture to ourselves that the frequency of vibration of a silver atom is that of violet or ultra-violet light, and therefore, when struck by a wave of this frequency, is set in vibration by resonance, just as a tuning fork is set in vibrati ...
Lecture 6: Higher Harmonics Of The Generator Wave - 6 hit(s)

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SIXTH LECTURE HIGHER HARMONICS OF THE GENERATOR WAVE mHE open circuit reactance of the transformer is the only reactance high enough to give resonance with the line capacity at fundamental frequency. All other reactances are too low for this. Since, however, the inductive reactance increases and the capacity reactance decreases proportionally to the frequency, the two reactances come nearer together fo ...
Lecture 17: Arc Lighting - 6 hit(s)

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... convert their energy into other forms of energy, if the energy is only great enough, we get a high temperature, and thus a high chemical action, merely by the effect of temperature. But we may also get a chemical effect by what probably is some kind of a resonance phenomenon. The particles of a body, atoms or molecules, must have some rate of vibration of their own. If, then, a ray of radiation impinges upon them which is of a frequency of the same magnitude as the inherent rate of vibration of the atom, by resonan ...
Chapter 26: Effects Of Higher Harmonics - 6 hit(s)

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... rrent and of potential EFFECTS OF HIGHER HARMONICS 373 difference in the non-inductive part of the circuit more pro- nounced— intensifies the harmonics. Self-induction and capacity in series may cause an increase of voltage due to complete or partial resonance with higher har- monics, and a discrepancy between volt-amperes and watts, without corresponding phase displacement, as will be shown hereafter. 253. In long-distance transmission over lines of noticeable inductive and condensive reactance, rise of volt ...
Chapter 14: Constant-Potential Constant-Current Trans Formation - 6 hit(s)

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... 268 ELECTRIC CIRCUITS That is, if in a constant-potential circuit, of impressed e.m.f ., 60, an inductive reactance, Xo, and a condensive reactance, Xe, are connected in series with each other, and if Xe = Xo, (35) that is, the two reactances are in resonance condition with each other, any circuit shunting the capacity reactance is a constant- current circuit, and regardless of the impedance of this circuit, Z = r + jXf the current in the circuit is t = — . Xo 133. Such a combination of two equal reactanc ...
Chapter 2: Long-Distance Transmission Line - 6 hit(s)

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... hen once started, even with zero impressed e.m.f., such alternating currents traverse the lines for some time, gradually decreasing in intensity by the energy consumption in the conductor, and so fading out. The condition of this phenomenon of electrical resonance thus is that alternating impulses occur at time intervals equal to the time required for the impulse to travel the length of the line and back; that is, the time of one half wave of impressed e.m.f. is the time required by light to travel twice the length ...
Chapter 20: Ri - 5 hit(s)

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... makes the higher harmonics of current and of poten- tial difference in the non-inductive part of the circuit more pronounced — intensifies the harmonics. Self-induction and capacity in series may cause an in- crease of voltage due to complete or partial resonance. 225. In long-distance transmission over lines of notice- able inductance and capacity, rise of voltage due to reso- nance may under circumstances be expected with higher harmonics, as waves of higher frequency, while the funda- mental wave is usually o ...
Chapter 23: Effects Of Higher Harmonics - 5 hit(s)

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... makes the higher harmonics of current and of poten- tial difference in the non-inductive part of the circuit more pronounced — intensifies the harmonics. Self-induction and capacity in series may cause an in- crease of voltage due to complete or partial resonance with higher harmonics, and a discrepancy between volt-amperes and watts, without corresponding phase displacement, as will be shown hereafter. 246. In long-distance transmission over lines of notice- able inductance and capacity, rise of voltage due to ...
Chapter 10: Instability Of Circuits : The Arc - 5 hit(s)

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... ry simultaneously or in phase, current and voltage in the condenser branch circuit also must be in phase with each other, that is, the Fig. 87. frequency of the oscillation in Fig. 87 is that at which capacity, C, and inductance, L, balance, or is the resonance frequency. If circuit. A, in Fig. 87 is an arc circuit, and the resistance, r, in the shunt circuit small, instability again results, in the same man- ner as discussed before. 93. Another way of looking at the phenomena resulting from a condenser, C, s ...
Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance - 3 hit(s)

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... very much faster than in a non-inductive circuit. Series inductive reactance in a condenser circuit, and series condensive reactance in an inductive circuit, cause a rise of potential. This rise is a maximum for a:o = ± 0.8, or Xq = — X (the condition of resonance), and the e.m.f, reaches the value £■ = 167 volts, or E = Eq— This rise of potential by series reactance continues up to Xo = + 1.6, or, Xo = — 2x, where E = 100 volts again; and for Xq > 1.6 the voltage drops again. At rro = ± 0.8, x = + 0.8, the tot ...
Chapter 8: Circuits Containing Resistance, Inductance, And Capacity - 3 hit(s)

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... non-inductive circuit. RESISTANCE, INDUCTANCE, CAPACITY. 65 Series inductance in a condenser circuit, and series con- densance in an inductive circuit, cause a rise of potential. This rise is a maximum for x0 = i .8, or, x0 = — x (the condition of resonance), and the E.M.F. reaches the value, E = 167 volts, or, E = E0z] r. This rise of potential by series reactance continues up to x0 = il.6, or, x0 = — %x, Fig. 42. where E = 100 volts again ; and for x0 > 1.6 the voltage drops again. At x0 = ± -8, x = ...
Chapter 4: Induction Motor With Secondary Excitation - 3 hit(s)

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... ds toward zero when approaching synchronism, 86 ELECTRICAL APPARATUS and peculiar speed characteristics result herefrom in such a motor. At a certain slip, s, the condenser current just balances all the reactive lagging currents of the induction motor, resonance may thus be said to exist, and a very large current flows into the motor, and correspondingly large power is produced. Above this "resonance speed," however, the current and thus the power rapidly fall off, and so also below the resonance speed. It must ...
Chapter 9: Wave Screens. Even Harmonics - 3 hit(s)

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... the alternating voltage, and the inductance, L, so high as to practically open-circuit the alternating voltage, the separation — of combi- nation — ^is practically complete, and independent of the frequency of the alternating wave. Wave screens based on resonance for a definite frequency by series connection of capacity and inductance, can be used to sepa- rate the ciurent of this frequency from a complex current or voltage wave, such as those given in Figs. 56 to 63, and thus can be used for separation of comp ...
Chapter 18: Oscillating Currents - 3 hit(s)

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... oscillating discharge is Z = 0, that is, 1 o / ^ ^ 1^ T \r^C 2aL 2L If r = 0, that is, in a circuit without resistance, we have a = 0, / = /=^j that is, the currents are alternating with no decre- 2 "n"^ LC ment, and the frequency is that of resonance. If ^ty-^-t < 0, that is, r > 2-1/7^, a and / become imaginary; that is, the discharge ceases to be oscillatory. An electrical discharge assumes an oscillating nature only, if r < ^xlp- In the case r = 2 -yj^ we have a = 00 , / = 0; that is, the curren ...
Lecture 10: Continual And Cumulative Oscillations - 2 hit(s)

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... l arcing ground oscillation in Figs. 44 and 45, page 98. In Fig. 44, the beginning of the disturbance, apparently a harmonic of the generator wave builds up by the energy supply through a beginning arc, and then builds down again, by being slightly out of resonance with a multiple of the natural frequency of the circuit. In Fig. 45, the arc has completely developed, and one of the harmonics of the generator wave appears as a steady continuous oscillation. Continual and cumulative oscillations naturally are the most ...
Chapter 7: Numerical Calculations - 2 hit(s)

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... n general, the frequency of oscillation is assumed as constant, but where, as in cumulative hunting of synchronous machines, the amplitude of the swing reaches large values, an appreciable change of the period must be expected, and where the hunting is a resonance effect with some other periodic motion, as the engine rotation, the change of frequency with increase of amplitude of the oscillation breaks the complete resonance and thereby tends to limit the amplitude of the swing. 177. As example of the application ...
Lecture 9: Hunting Of Synchronous Machines - 2 hit(s)

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... or synchronous motors, it is frequently reduced by mak- ing the field excitation unequal, or putting a flywheel on one converter, or belting some other machine to it, or running an induction motor in the same station or in any other way break- ing up the resonance. 122 GENERAL LECTURES 2nd. Several converters hunting against each other in the same substation are frequently steadied by connecting the collector rings with each other, that is, by equalizer connec- tions between converter and transformer or regulat ...
Chapter 24: Synchronous Motor - 2 hit(s)

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... pedance, z = v r^ + x^, into a non-inductive circuit. Equation (34) is identical with the equation giving the maximum voltage, Ci, at current, i, which can be produced by shunting the receiving circuit with a condenser; that is, the condition of "complete resonance" of the line, z = V r^ + x^, with current, i. Hence, referring to equation (35), Ci = Co^is the maximum resonance voltage of the line reached when closed by a con- denser of reactance, — x. SYNCHRONOUS MOTOR 323 223. D. Maximum Displacement of Phase ...