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Theory and Calculation of Electric Circuits Visual Map

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Distributed Constants Of A Transmission Line
Distributed Constants Of A Transmission Line

Modern reading aid for line capacity, inductance, leakage, waves, and transients.

distributed-constants, capacity, inductance, waves

Open SVG - recreated visual index

Reactors And Synchronizing Power
Reactors And Synchronizing Power

Modern reading aid for the Commonwealth Edison report and system-stability mathematics.

synchronizing-power, power-limiting-reactors, reactance

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Field Wave Line
Field Wave Line

Modern reading aid for distributed constants, standing waves, traveling waves, and surge propagation.

electric-waves, distributed-constants, traveling-wave, lightning-surges

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Impedance And Reactance Triangle
Impedance And Reactance Triangle

Modern guide for resistance, reactance, impedance, phase angle, and symbolic quantities.

impedance, reactance, power-factor, symbolic-method

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Commonwealth Edison System Reactor Map
Commonwealth Edison System Reactor Map

Modern reading aid for station sections, power-limiting reactors, tie cables, and synchronism.

power-limiting-reactors, synchronizing-power, reactance, power-systems

Open SVG - recreated visual index

CandidateCaption leadSectionRoutes
theory-calculation-electric-circuits-fig-001
Fig. 1
L Fig. 1. A characteristic of metallic conductoi^ is that the resistanceChapter 1: Electric Conduction. Soled And Liquidsource
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theory-calculation-electric-circuits-fig-002
Fig. 2
/ Fig. 2. ance over a very wide range of temperature is extremely difficult, and often no more accurate.Chapter 1: Electric Conduction. Soled And Liquidsource
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theory-calculation-electric-circuits-fig-004
Fig. 4
mm Fig. 4. though the temperature coefficient remains negative, like in electrolytic conductors.Chapter 1: Electric Conduction. Soled And Liquidsource
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theory-calculation-electric-circuits-fig-005
Fig. 5
a Fig. 5. often plotted with -\/i as abscissae, to show the ranges in betterChapter 1: Electric Conduction. Soled And Liquidsource
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theory-calculation-electric-circuits-fig-010
Fig. 10
M Fig. 10. This, however, still further increases the required voltage andChapter 1: Electric Conduction. Soled And Liquidsource
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theory-calculation-electric-circuits-fig-013
Fig. 13
L Fig. 13. ticity, metallic luster, etc., and electrically it has a relativelyChapter 1: Electric Conduction. Soled And Liquidsource
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theory-calculation-electric-circuits-fig-021
Fig. 21
at low currents the voltage rises again, due to the arc not filling the entire tube. Such a volt-ampere characteristic is given in Fig. 21. 26. Herefrom then follows, that the voltage gradient in the mercury arc, for…Chapter 2: Electric Conduction. Gas And Vaporsource
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theory-calculation-electric-circuits-fig-031
Fig. 31
(13) Fig. 31. the maximum possible hysteresis loss.Chapter 4: Magnetismsource
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theory-calculation-electric-circuits-fig-032
Fig. 32
)f Fig. 32. wChapter 4: Magnetismsource
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theory-calculation-electric-circuits-fig-034
Fig. 34
s Fig. 34. half-scale, as curve 1, and the magnetization curve of magnetite , FeaO^ — which is about the same as the black scale of iron— ic*.Chapter 4: Magnetismsource
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theory-calculation-electric-circuits-fig-035
Fig. 35
3 1 Fig. 35. ^ under the assumption that cither material rigidly follows the 1-8 power law up to the highest densities, by the equation,Chapter 4: Magnetismsource
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theory-calculation-electric-circuits-fig-045
Fig. 45
density is uniform for the width lo between the coil surfaces, Fig. 45. and then decreases toward the interior of the coils, over the dis- tance K respectively ^, to zero at the coil centers. All the coilChapter 6: Magnetismsource
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theory-calculation-electric-circuits-fig-053
Fig. 53
one-half the other. Fig. 53. 61. Distribution of the winding over an arc of the periphery^ o^Chapter 7: Shaping Of Waves : Generalsource
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theory-calculation-electric-circuits-fig-064
Fig. 64
that harmonic n, where n8 = 180**. Fig. 64. IfChapter 7: Shaping Of Waves : Generalsource
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theory-calculation-electric-circuits-fig-063
Fig. 63
The magnetic flux wave, B, becomes more and more 9at-topped with increasing saturation, and finally practically rectangular, in Fig. 63. The curves 60 to 63 are drawn with the same maximum valuesChapter 8: Shaping Of Waves By Magnetic Saturationsource
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theory-calculation-electric-circuits-fig-070
Fig. 70
\\ Fig. 70. The enormous reduction of the voltage peak by an air-gap ofChapter 8: Shaping Of Waves By Magnetic Saturationsource
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theory-calculation-electric-circuits-fig-073
Fig. 73
rmmM Fig. 73. r eChapter 9: Wave Screens. Even Harmonicssource
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theory-calculation-electric-circuits-fig-074
Fig. 74
r e Fig. 74. proportional to frequency and voltage, the condenser shimts theChapter 9: Wave Screens. Even Harmonicssource
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theory-calculation-electric-circuits-fig-076
Fig. 76
Qii Lnf ggi Fig. 76. where / = frequency of the fundamental wave.Chapter 9: Wave Screens. Even Harmonicssource
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theory-calculation-electric-circuits-fig-084
Fig. 84
As the two parallel arcs must have the same voltage, the oper- ating point is the point, a, of the intersection of A and -4’ in Fig. 84. The arcs thus would divide the current, each operating at 3 amp.Chapter 10: Instability Of Circuits : The Arcsource
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theory-calculation-electric-circuits-fig-085
Fig. 85
g Fig. 85. itself; ft and c, however, are unstable. Thus, at the latter points,Chapter 10: Instability Of Circuits : The Arcsource
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theory-calculation-electric-circuits-fig-086
Fig. 86
1 Fig. 86. condition of arcs with resistance in series and in shunt, on constant, voltage supply, etc.Chapter 10: Instability Of Circuits : The Arcsource
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theory-calculation-electric-circuits-fig-087
Fig. 87
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.Chapter 10: Instability Of Circuits : The Arcsource
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theory-calculation-electric-circuits-fig-088
Fig. 88
S~ Fig. 88. the curves of the arc voltage, eo,Chapter 10: Instability Of Circuits : The Arcsource
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theory-calculation-electric-circuits-fig-089
Fig. 89
SHUNTING ARC Fig. 89. As long as the current in the circuit, A — whether resistance or arc — is steady, no current passes the condenser circuit, and theChapter 10: Instability Of Circuits : The Arcsource
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theory-calculation-electric-circuits-fig-094
Fig. 94
of effective resistances, 22, as the values of r-., for pulsations between i + bi and i — bi, and such a curve is shown as R in Fig. 94. We may say, that the arc, when shunted by an oscillating circuit, has an effecti…Chapter 10: Instability Of Circuits : The Arcsource
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theory-calculation-electric-circuits-fig-006
Fig. 6
I Fig. 06. first increases, but then decreases again, down to zero, so that the cumulative oscillations produced by this arc are self-limitii^,Chapter 10: Instability Of Circuits : The Arcsource
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theory-calculation-electric-circuits-fig-107
Fig. 107
^i-1.9 00 - 60°; ^0=7.6. Fig. 107. and the magnetic distribution in the transformer, during the moments marked as a, 6, c, d, e, /, g, in Fig. 107, is shown inChapter 12: Reactance Of Induction Apparatussource
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theory-calculation-electric-circuits-fig-105
Fig. 105
and the magnetic distribution in the transformer, during the moments marked as a, 6, c, d, e, /, g, in Fig. 107, is shown in Fig. 105. In Fig. 105a, the primary flux is larger than the secondary, and all leakage fluxe…Chapter 12: Reactance Of Induction Apparatussource
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theory-calculation-electric-circuits-fig-109
Fig. 109
the primary coil equals its resistance drop, eo = roi, then the Fig. 109. voltage across the secondary coil, s, gives the total reactance, x^, for s as primary,Chapter 12: Reactance Of Induction Apparatussource
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theory-calculation-electric-circuits-fig-115
Fig. 115
/ Fig. 115. give the best regulation; series inductive reactance with an in- ductive, and series condensive reactance with leading current inChapter 14: Constant-Potential Constant-Current Trans Formationsource
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theory-calculation-electric-circuits-fig-117
Fig. 117
O < Fig. 117. and the tangent of the primary phase angleChapter 14: Constant-Potential Constant-Current Trans Formationsource
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theory-calculation-electric-circuits-fig-119
Fig. 119
square will be more fully discussed. Fig. 119. A. T-Connection or Resonating CircuitChapter 14: Constant-Potential Constant-Current Trans Formationsource
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theory-calculation-electric-circuits-fig-123
Fig. 123
8INQLE-PHA8E Fig. 123. Different arrangements can also be used of the constant-current control, for instance, the inductive and condensive reactances inChapter 14: Constant-Potential Constant-Current Trans Formationsource
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theory-calculation-electric-circuits-fig-124
Fig. 124
8INQIC*PHA8E Fig. 124. the losses in these transformers have not been included, sinceChapter 14: Constant-Potential Constant-Current Trans Formationsource
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theory-calculation-electric-circuits-fig-125
Fig. 125
SINOLE-PHASE Fig. 125. cuits instead of being operated from the three-phase secondaries of the step-down transformers can be operated directly from theChapter 14: Constant-Potential Constant-Current Trans Formationsource
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theory-calculation-electric-circuits-fig-127
Fig. 127
That is, the regulation is improved, by the line and leakage reactance, from g = 4 per cent, to 5 = 1.5 per cent, as seen in Fig. 127. 163. In paragraph 161 and the preceding, the shunted react- ances, 61 and 62, have…Chapter 15: Constant-Voltage Series Operationsource
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