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.
modern guide diagrams
reconstructions, not historical evidencefigure candidates
OCR/PDF-text leads needing crop reviewformula candidates
math leads needing transcription reviewsource routes
source text, workbench, visual and formula mapsLayer 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.
Source Routes
Section titled “Source Routes”Modern Guide Diagrams
Section titled “Modern Guide Diagrams”Modern reading aid for induction-machine field language in AC and Theoretical Elements sources.
symbolic-method, magnetism, phase, induction-motor
Modern reading aid for line capacity, inductance, leakage, waves, and transients.
distributed-constants, capacity, inductance, waves
Modern reading aid for Steinmetz’s paired magnetic-field and dielectric-field language.
dielectric-field, magnetic-field, energy-storage
Modern reading aid for conductance, susceptance, and reciprocal impedance.
admittance, conductance, susceptance, symbolic-method
Modern reading aid for wave-shape analysis and higher harmonics.
harmonics, wave-shape, fourier-analysis
Modern reading aid for the Steinmetz law and magnetic energy loss per cycle.
hysteresis, magnetic-loss, effective-resistance
Modern reading aid for Steinmetz’s field language in Relativity and Space.
field-language, ether, relativity, energy-field
Modern reading aid for number, direction, and symbolic calculation in Engineering Mathematics.
complex-quantities, number, symbolic-method
Modern redraw sheet for rectangular components, resultant addition, and quarter-period j rotation.
symbolic-method, complex-quantities, phasor, operator-j
Modern reading aid for vector and complex-number representation of alternating quantities.
symbolic-method, complex-quantities, phase, phasor
Modern guide for magnetic lag, loop area, and energy loss per cycle.
hysteresis, magnetism, magnetic-loss, effective-resistance
Modern reading aid for distributed constants, standing waves, traveling waves, and surge propagation.
electric-waves, distributed-constants, traveling-wave, lightning-surges
Modern guide for resistance, reactance, impedance, phase angle, and symbolic quantities.
impedance, reactance, power-factor, symbolic-method
Modern guide for the practical bridge from radiation to visual illumination and light distribution.
illumination, radiation, light-flux, inverse-square
Candidate Figure Leads
Section titled “Candidate Figure Leads”| Candidate | Caption lead | Source section | Routes |
|---|---|---|---|
radiation-light-and-illumination-fig-062Fig. 62 | is: FIG. 62. = 27r/sin<M^ | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-064Fig. 64 | 192 RADIATION, LIGHT, AND ILLUMINATION. FIG. 64. FIG. 65. | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-065Fig. 65 | FIG. 64. FIG. 65. FIG. 66. | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-066Fig. 66 | FIG. 65. FIG. 66. LIGHT FLUX AND DISTRIBUTION. 193 | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-067Fig. 67 | direction. FIG. 67. Straight Line or Cylindrical Radiator. | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-068Fig. 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 of | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-070Fig. 70 | > FIG. 70. FIG. 71. | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-071Fig. 71 | FIG. 70. FIG. 71. In Fig. 72 is plotted the intensity distribution in the meridian | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-072Fig. 72 | (7) Single-Loop Filament. FIG. 72. 200 | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-073Fig. 73 | meridianal distribution of the sides A + B is : FIG. 73. 7 = 4 r/ | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-074Fig. 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 | source workbench |
radiation-light-and-illumination-fig-075Fig. 75 | has from the center 0 of the radiator the distance FIG. 75. a = 00 | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-078Fig. 78 | ^ FIG. 78. 94. In Table III are given | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-081Fig. 81 | V////A W/\ v////\ FIG. 81. FIG. 82. | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-082Fig. 82 | FIG. 81. FIG. 82. LIGHT FLUX AND DISTRIBUTION. | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-084Fig. 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 | source workbench |
radiation-light-and-illumination-fig-086Fig. 86 | I = I’ = 70 (sin ^ - tan w cos 0). (10) FIG. 86. For to = 75 deg. = and a = 0.7, the intensity distribution | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-087Fig. 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 radiator | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-088Fig. 88 | Table V. FIG. 88. Substituting the numerical values in the foregoing, we have: | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-089Fig. 89 | (36) FIG. 89. The distribution curve of such an illuminant is plotted in Fig. 89 and recorded in Table V for the values | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-090Fig. 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. 89 | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-091Fig. 91 | the point P receives light from all points of the envelope G as FIG. 91. 3-B | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-092Fig. 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 that | Radiation, Light and Illumination Lecture 10: Light Flux And Distribution | source workbench |
radiation-light-and-illumination-fig-093Fig. 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 | source workbench |
Formula Leads That Pair With The Visual Topic
Section titled “Formula Leads That Pair With The Visual Topic”| Candidate | OCR/PDF text | Source section | Routes |
|---|---|---|---|
engineering-mathematics-eq-candidate-0273engineering-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-0286engineering-math | If, A=ai +ja2 = a (cos a+j sin a), then | Engineering Mathematics: A Series of Lectures Delivered at Union College Chapter 1: The General Number | source workbench |
engineering-mathematics-eq-candidate-0150engineering-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-0151engineering-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-0157engineering-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-0252engineering-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-0279engineering-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-0102symbolic-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-0167symbolic-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-0240symbolic-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 | source workbench |
theory-calculation-alternating-current-phenomena-eq-candidate-0294symbolic-ac | is r - j {x + Xo) = r = 0.6, x -{- Xo = 0, and tan do = 0; that | Theory and Calculation of Alternating Current Phenomena Chapter 9: Circuits Containing Resistance, Inductive Reactance, And Condensive Reactance | source workbench |
theory-calculation-electric-apparatus-eq-candidate-0028symbolic-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-0127engineering-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-0129engineering-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 | source workbench |
theoretical-elements-electrical-engineering-eq-candidate-0132symbolic-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-0001symbolic-ac | 1.) Ohm’s law : i = e j r, where r, the resistance, is a | Theory and Calculation of Alternating Current Phenomena Chapter 1: Introduction | source workbench |
theory-calculation-alternating-current-phenomena-1897-eq-candidate-0001symbolic-ac | 1.) Ohm’s law : i = e j r, where r, the resistance, is a | Theory and Calculation of Alternating Current Phenomena Chapter 1: Introduction | source workbench |
theory-calculation-alternating-current-phenomena-1900-eq-candidate-0131symbolic-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 | source workbench |
Editorial Use
Section titled “Editorial Use”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.