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Magnetism, Hysteresis, And Machines

Visual topic gallery

Magnetism, Hysteresis, And Machines

Visual routes through magnetic lag, hysteresis loss, rotating magnetic fields, induction machines, effective resistance, and magnetic energy.

14

modern guide diagrams

reconstructions, not historical evidence
352

figure candidates

OCR/PDF-text leads needing crop review
2266

formula candidates

math leads needing transcription review
4

source routes

source text, workbench, visual and formula maps

Layer rule: original crops, figure candidates, modern redraws, and formula candidates are separated. Use this page to browse visually, then verify in the linked source text and workbench.

Rotating Magnetic Field From Quadrature Fluxes
Rotating Magnetic Field From Quadrature Fluxes

Modern reading aid for induction-machine field language in AC and Theoretical Elements sources.

symbolic-method, magnetism, phase, induction-motor

Open SVG - all recreated visuals

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 - all recreated visuals

Magnetic And Dielectric Energy Storage
Magnetic And Dielectric Energy Storage

Modern reading aid for Steinmetz’s paired magnetic-field and dielectric-field language.

dielectric-field, magnetic-field, energy-storage

Open SVG - all recreated visuals

Admittance Plane
Admittance Plane

Modern reading aid for conductance, susceptance, and reciprocal impedance.

admittance, conductance, susceptance, symbolic-method

Open SVG - all recreated visuals

Equivalent Sine Waves And Harmonics
Equivalent Sine Waves And Harmonics

Modern reading aid for wave-shape analysis and higher harmonics.

harmonics, wave-shape, fourier-analysis

Open SVG - all recreated visuals

Hysteresis Loss Law
Hysteresis Loss Law

Modern reading aid for the Steinmetz law and magnetic energy loss per cycle.

hysteresis, magnetic-loss, effective-resistance

Open SVG - all recreated visuals

Field Of Energy Boundary
Field Of Energy Boundary

Modern reading aid for Steinmetz’s field language in Relativity and Space.

field-language, ether, relativity, energy-field

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Engineering Number Plane
Engineering Number Plane

Modern reading aid for number, direction, and symbolic calculation in Engineering Mathematics.

complex-quantities, number, symbolic-method

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AC Symbolic Method Redraw Sheet
AC Symbolic Method Redraw Sheet

Modern redraw sheet for rectangular components, resultant addition, and quarter-period j rotation.

symbolic-method, complex-quantities, phasor, operator-j

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Phasor And Symbolic Method
Phasor And Symbolic Method

Modern reading aid for vector and complex-number representation of alternating quantities.

symbolic-method, complex-quantities, phase, phasor

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Hysteresis Loop
Hysteresis Loop

Modern guide for magnetic lag, loop area, and energy loss per cycle.

hysteresis, magnetism, magnetic-loss, effective-resistance

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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

Open SVG - all recreated visuals

Illumination Inverse-Square Geometry
Illumination Inverse-Square Geometry

Modern guide for the practical bridge from radiation to visual illumination and light distribution.

illumination, radiation, light-flux, inverse-square

Open SVG - all recreated visuals

CandidateCaption leadSource sectionRoutes
radiation-light-and-illumination-fig-062
Fig. 62
is: FIG. 62. = 27r/sin<M^Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-064
Fig. 64
192 RADIATION, LIGHT, AND ILLUMINATION. FIG. 64. FIG. 65.Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-065
Fig. 65
FIG. 64. FIG. 65. FIG. 66.Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-066
Fig. 66
FIG. 65. FIG. 66. LIGHT FLUX AND DISTRIBUTION. 193Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-067
Fig. 67
direction. FIG. 67. Straight Line or Cylindrical Radiator.Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-068
Fig. 68
24 deg. above the horizontal, or in the space between a and a’ in Fig. 68. It is interesting to compare the three radiators, (1), (2), and (5), on the basis of equal maximum intensity, and on the basis ofRadiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-070
Fig. 70
> FIG. 70. FIG. 71.Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-071
Fig. 71
FIG. 70. FIG. 71. In Fig. 72 is plotted the intensity distribution in the meridianRadiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-072
Fig. 72
(7) Single-Loop Filament. FIG. 72. 200Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-073
Fig. 73
meridianal distribution of the sides A + B is : FIG. 73. 7 = 4 r/Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-074
Fig. 74
Figs. 70 and 71. FIG. 74. In the meridian of minimum intensity, the light intensity 73 produced by the projection of the half circle in its own plane,Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-075
Fig. 75
has from the center 0 of the radiator the distance FIG. 75. a = 00Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-078
Fig. 78
^ FIG. 78. 94. In Table III are givenRadiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-081
Fig. 81
V////A W/\ v////\ FIG. 81. FIG. 82.Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-082
Fig. 82
FIG. 81. FIG. 82. LIGHT FLUX AND DISTRIBUTION.Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-084
Fig. 84
As illustrations are plotted in Fig. 84 and recorded in Table IV, FIG. 84. 212 RADIATION, LIGHT, AND ILLUMINATION.Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-086
Fig. 86
I = I’ = 70 (sin ^ - tan w cos 0). (10) FIG. 86. For to = 75 deg. = and a = 0.7, the intensity distributionRadiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-087
Fig. 87
co2 the angle subtended by the outer edge of the reflector, from FIG. 87. the base of the arc, as diagrammatically illustrated in Fig. 87; then the intensity of the light flux of the main radiatorRadiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-088
Fig. 88
Table V. FIG. 88. Substituting the numerical values in the foregoing, we have:Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-089
Fig. 89
(36) FIG. 89. The distribution curve of such an illuminant is plotted in Fig. 89 and recorded in Table V for the valuesRadiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-090
Fig. 90
(36) 7 = 70 (sin <j> - 11.43 cos <j>). FIG. 90. As comparison is given in Fig. 90 the distribution curve of the magnetite arc, which is designed of the type of Fig. 89Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-091
Fig. 91
the point P receives light from all points of the envelope G as FIG. 91. 3-BRadiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-092
Fig. 92
a radiator giving the distribution curve shown in Fig. 92, curve I, FIG. 92. the distribution curve is changed by diffraction (frosted en- velope), to that shown in Fig. 92, curve II, but changed to thatRadiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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radiation-light-and-illumination-fig-093
Fig. 93
^ FIG. 93. be directed into the horizontal (or any other desired) direction, and the entire lens then appears luminous, as virtual radiator.Radiation, Light and Illumination
Lecture 10: Light Flux And Distribution
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Formula Leads That Pair With The Visual Topic

Section titled “Formula Leads That Pair With The Visual Topic”
CandidateOCR/PDF textSource sectionRoutes
engineering-mathematics-eq-candidate-0273
engineering-math
Let A = a(cos a+j sin a) be divided by J5 = 6(cos ,5+y sin /5),Engineering Mathematics: A Series of Lectures Delivered at Union College
Chapter 1: The General Number
source
workbench
engineering-mathematics-eq-candidate-0286
engineering-math
If, A=ai +ja2 = a (cos a+j sin a), thenEngineering Mathematics: A Series of Lectures Delivered at Union College
Chapter 1: The General Number
source
workbench
engineering-mathematics-eq-candidate-0150
engineering-math
and ai + ja2 = a (cos 6 + j sin d) ;Engineering Mathematics: A Series of Lectures Delivered at Union College
Chapter 1: The General Number
source
workbench
engineering-mathematics-eq-candidate-0151
engineering-math
or ai —ja2 = A(cos 0+j sin 6).Engineering Mathematics: A Series of Lectures Delivered at Union College
Chapter 1: The General Number
source
workbench
engineering-mathematics-eq-candidate-0157
engineering-math
and A ==5 (cos 37 deg. H-j sin 37 deg).Engineering Mathematics: A Series of Lectures Delivered at Union College
Chapter 1: The General Number
source
workbench
engineering-mathematics-eq-candidate-0252
engineering-math
C = AB = ah (cos a+j sin a) (cos /?+ / sin /5)Engineering Mathematics: A Series of Lectures Delivered at Union College
Chapter 1: The General Number
source
workbench
engineering-mathematics-eq-candidate-0279
engineering-math
A = ai +ja2 = a(cos a+j sin a),Engineering Mathematics: A Series of Lectures Delivered at Union College
Chapter 1: The General Number
source
workbench
theoretical-elements-electrical-engineering-eq-candidate-0102
symbolic-ac
e = 2 7r/n$ sin r the instantaneous generated e.m.f.Theoretical Elements of Electrical Engineering
Theory Section 3: Generation of E.m.f.
source
workbench
theory-calculation-alternating-current-phenomena-eq-candidate-0167
symbolic-ac
B = 6’ + jh” = 6(cos 13 + j sin /3)Theory and Calculation of Alternating Current Phenomena
Chapter 5: Symbolic Method
source
workbench
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0240
symbolic-ac
is r - j (x -f x0} = r = .6, x + x0 = 0, and tan S>0 = 0 ;Theory and Calculation of Alternating Current Phenomena
Chapter 8: Circuits Containing Resistance, Inductance, And Capacity
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workbench
theory-calculation-alternating-current-phenomena-eq-candidate-0294
symbolic-ac
is r - j {x + Xo) = r = 0.6, x -{- Xo = 0, and tan do = 0; thatTheory and Calculation of Alternating Current Phenomena
Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance
source
workbench
theory-calculation-electric-apparatus-eq-candidate-0028
symbolic-ac
= - J = (tan a - j) (7)Theory and Calculation of Electric Apparatus
Chapter 1: Speed Control Of Induction Motors
source
workbench
engineering-mathematics-eq-candidate-0127
engineering-math
20. If ai+y6i=6+2.5 J is represented by the point Pi;Engineering Mathematics: A Series of Lectures Delivered at Union College
Chapter 1: The General Number
source
workbench
engineering-mathematics-eq-candidate-0129
engineering-math
and the vertical distance 6i=2.5. If a2+jb2 = S+4:j is repre-Engineering Mathematics: A Series of Lectures Delivered at Union College
Chapter 1: The General Number
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workbench
theoretical-elements-electrical-engineering-eq-candidate-0132
symbolic-ac
If an alternating current i = I0 sin 6 passes through a resist-Theoretical Elements of Electrical Engineering
Theory Section 4: Power and Effective Values
source
workbench
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0001
symbolic-ac
1.) Ohm’s law : i = e j r, where r, the resistance, is aTheory and Calculation of Alternating Current Phenomena
Chapter 1: Introduction
source
workbench
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0001
symbolic-ac
1.) Ohm’s law : i = e j r, where r, the resistance, is aTheory and Calculation of Alternating Current Phenomena
Chapter 1: Introduction
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workbench
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0131
symbolic-ac
or, if E = e —je’ is the impressed E.M.F., and 7 = i ’ — ji’Theory and Calculation of Alternating Current Phenomena
Chapter 5: Symbolic Method
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workbench

This gallery is meant for discovery, not final citation. The strongest current source distribution is: Theory and Calculation of Alternating Current Phenomena (1168), Theory and Calculation of Electric Apparatus (313), Theoretical Elements of Electrical Engineering (310), Engineering Mathematics: A Series of Lectures Delivered at Union College (309). Promote a diagram or formula only after the scan, page label, exact caption, and mathematical notation are checked.