Ether, Field Language, And Relativity
Visual topic gallery
Ether, Field Language, And Relativity
Visual routes through ether references, Faraday-Maxwell field language, field of force, field of energy, and relativity-era boundaries.
original crops
scan images routed into this topicmodern guide diagrams
reconstructions, not historical evidencefigure candidates
OCR/PDF-text leads needing crop reviewformula candidates
math leads needing transcription reviewLayer 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”Original Scan Crops
Section titled “Original Scan Crops”
Radiation, Light and Illumination
Radiation, Light and Illumination, printed page 22, PDF page 42; Fig. 15

Radiation, Light and Illumination
Radiation, Light and Illumination, printed page 28, PDF page 48; Fig. 18

Radiation, Light and Illumination
Radiation, Light and Illumination, printed page 29, PDF page 49; Fig. 19

Radiation, Light and Illumination
Radiation, Light and Illumination, printed page 17, PDF page 37; Spectrum of Radiation table preceding Fig. 14
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 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 navigation guide for Steinmetz’s electric-wave, visible-light, ultraviolet, and X-ray spectrum bridge.
radiation, electric-waves, frequency, spectrum, ether
Modern guide for permanent terms, temporary terms, decay, and oscillatory readjustment.
transient-phenomena, oscillation-damping, damping, stored-energy
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 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-001Fig. 1 | tion, the time at which the moon M should disappear from sight, FIG. 1. when seen from the earth E, by passing behind Jupiter, 7 (Fig. 1), could be exactly calculated. It was found, however, that some- | Radiation, Light and Illumination Lecture 1: Nature And Different Forms Of Radiation | source research review |
radiation-light-and-illumination-fig-002Fig. 2 | 5_MOE_S FIG. 2. direction the light reappears. If the disk is slowly revolved, alter- nate light and darkness will be observed, but when the speed in- | Radiation, Light and Illumination Lecture 1: Nature And Different Forms Of Radiation | source research review |
radiation-light-and-illumination-fig-003Fig. 3 | from the upper surface of the plain glass plate A. A beam of FIG. 3. reflected light a, thus is a combination of a beam b and a beam c. | Radiation, Light and Illumination Lecture 1: Nature And Different Forms Of Radiation | source research review |
radiation-light-and-illumination-fig-004Fig. 4 | glass plates. At those points dv dv etc. at which the distance FIG. 4. between the two glass plates is J wave length, or j, J, etc., the | Radiation, Light and Illumination Lecture 1: Nature And Different Forms Of Radiation | source research review |
radiation-light-and-illumination-fig-005Fig. 5 | etc. in the plane of the paper, and thus perpendicular to the ray FIG. 5. of light. In the former case (a longitudinal vibration, as sound) there obviously can be no difference between the directions at | Radiation, Light and Illumination Lecture 1: Nature And Different Forms Of Radiation | source research review |
radiation-light-and-illumination-fig-009Fig. 9 | it to you, by bringing the rods near to this Crookes’ radiometer, FIG. 9. which is an instrument showing the energy of radiation. It con- sists (Fig. 10) of four aluminum vanes, mounted in a moderately | Radiation, Light and Illumination Lecture 1: Nature And Different Forms Of Radiation | source research review |
radiation-light-and-illumination-fig-010Fig. 10 | (red, orange and yellow) with increase in temperature, the light FIG. 10. 12 | Radiation, Light and Illumination Lecture 1: Nature And Different Forms Of Radiation | source research review |
radiation-light-and-illumination-fig-011Fig. 11 | of the lower frequencies of visible radiation, red or orange. FIG. 11. In the tungsten lamp at high brilliancy and more still in the | Radiation, Light and Illumination Lecture 1: Nature And Different Forms Of Radiation | source research review |
radiation-light-and-illumination-fig-012Fig. 12 | They are used in wireless telegraphy, etc. I here connect (Fig. 12) FIG. 12. the condenser C of the apparatus which I used for operating the ultra-violet arc, to a spark gap Gv of which the one side is con- | Radiation, Light and Illumination Lecture 1: Nature And Different Forms Of Radiation | source research review |
radiation-light-and-illumination-fig-013Fig. 13 | o — ^^ — o FIG. 13. has been measured by Herz by producing standing waves by combination of main wave and reflected wave. | Radiation, Light and Illumination Lecture 1: Nature And Different Forms Of Radiation | source research review |
radiation-light-and-illumination-fig-014Fig. 14 | as far as possible when producing light, as they consume power FIG. 14. and so lower the efficiency; the ultra-violet rays are of importance in medicine as germ killers. They are more or less destructive | Radiation, Light and Illumination Lecture 1: Nature And Different Forms Of Radiation | source research review |
radiation-light-and-illumination-fig-015Fig. 15 | edge of the beam reaches the boundary at D its speed changes FIG. 15. by entering the medium W — decreases in the present instance. Let then Sl = speed of propagation in medium A, S2 = speed of | Radiation, Light and Illumination Lecture 2: Relation Of Bodies To Radiation | source research review |
radiation-light-and-illumination-fig-016Fig. 16 | medium into another, and the higher frequencies are deflected FIG. 16. more than the lower frequencies, thus showing that the velocity of propagation decreases with an increase of frequency, that is, | Radiation, Light and Illumination Lecture 2: Relation Of Bodies To Radiation | source research review |
radiation-light-and-illumination-fig-017Fig. 17 | VIOLET FIG. 17. a number of very faint red and orange lines, of which three are indicated dotted in Fig. 17. | Radiation, Light and Illumination Lecture 2: Relation Of Bodies To Radiation | source research review |
radiation-light-and-illumination-fig-018Fig. 18 | perature rise, their brilliancy is greatly increased. FIG. 18. Combinations of the different types of spectra: continuous spectrum, line spectrum, band spectrum, reversed spectrum, | Radiation, Light and Illumination Lecture 2: Relation Of Bodies To Radiation | source research review |
radiation-light-and-illumination-fig-019Fig. 19 | and the body thus acts as a mirror, that is, gives a virtual image FIG. 19. back of it as shown in dotted line in Fig. 18. In the latter case (Fig. 19) the light is reflected irregularly in all directions. | Radiation, Light and Illumination Lecture 2: Relation Of Bodies To Radiation | source research review |
radiation-light-and-illumination-fig-021Fig. 21 | VIOLET FIG. 21. in the ultra-red and ultra-violet, where no power of radiation can produce visibility. It thus varies about as indicated in Fig. 22. | Radiation, Light and Illumination Lecture 3: Physiological Effects Of Radiation | source research review |
radiation-light-and-illumination-fig-022Fig. 22 | the basis of equal ease in distinguishing objects. As the pur- FIG. 22. pose for which light is used is to distinguish objects, the correct comparison of lights obviously is on the basis of equal distinctness | Radiation, Light and Illumination Lecture 3: Physiological Effects Of Radiation | source research review |
radiation-light-and-illumination-fig-023Fig. 23 | v FIG. 23. meter candles (or rather log i) as abscissas, for red light, wave length 65.0; orange yellow light, wave length 59; bluish green | Radiation, Light and Illumination Lecture 3: Physiological Effects Of Radiation | source research review |
radiation-light-and-illumination-fig-024Fig. 24 | \ FIG. 24. (1 meter-candle is the illumination produced by 1 candle power | Radiation, Light and Illumination Lecture 3: Physiological Effects Of Radiation | source research review |
radiation-light-and-illumination-fig-025Fig. 25 | S FIG. 25. 62 for high intensities and changes in approximately the same range of intensities in which lwo changes; ks is also plotted in | Radiation, Light and Illumination Lecture 3: Physiological Effects Of Radiation | source research review |
radiation-light-and-illumination-fig-026Fig. 26 | YELLOW GREEN FIG. 26. carbon filament would be somewhat like C. That is, the physio- | Radiation, Light and Illumination Lecture 3: Physiological Effects Of Radiation | source research review |
radiation-light-and-illumination-fig-027Fig. 27 | fore, increase enormously with the increase of temperature. FIG. 27. With bodies in a vacuum, the radiation power is the power input and this above law can be used to calculate the tempera- | Radiation, Light and Illumination Lecture 5: Temperature Radiation | source research review |
radiation-light-and-illumination-fig-028Fig. 28 | weight, exhibit a periodicity in their properties which permits FIG. 28. a systematic study of their properties. In diagram Fig. 28 the | Radiation, Light and Illumination Lecture 5: Temperature Radiation | source research review |
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 |
|---|---|---|---|
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0195transients-oscillation | i = io cos (0 - 7) = io cos 7 cos <j> + i0 sin 7 sin | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 6: Double-Energy Transients | source research review |
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 research review |
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0220transients-oscillation | if = 140 cos 0.2 1 - 80 sin 0.2 1, | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 6: Double-Energy Transients | source research review |
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 research review |
theoretical-elements-electrical-engineering-eq-candidate-0138symbolic-ac | e.m.f., e = EQ sin 6. | Theoretical Elements of Electrical Engineering Theory Section 4: Power and Effective Values | source research review |
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0014transients-oscillation | w=j*pdt, (10) | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 2: The Electric Field | source research review |
electric-discharges-waves-impulses-1914-eq-candidate-0018transients-oscillation | f = j (13) | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 2: The Electric Field | source research review |
electric-discharges-waves-impulses-1914-eq-candidate-0029transients-oscillation | K = j^; (21) | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 2: The Electric Field | source research review |
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0037transients-oscillation | (B = -j =/z JClinespercm2. | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 2: The Electric Field | source research review |
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0039transients-oscillation | 7 = -j = yG am- | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 2: The Electric Field | source research review |
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0178transients-oscillation | io = eo y j = e02/o. (11) | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 6: Double-Energy Transients | source research review |
electric-discharges-waves-impulses-1914-eq-candidate-0135transients-oscillation | (S!,J = 20,000 lines per cm^. * | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 5: Single-Energy Tra.Nsient Of Ironclad Circuit | source research review |
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0185transients-oscillation | ii = IQ cos 7 = initial transient current. (14) | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 6: Double-Energy Transients | source research review |
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0186transients-oscillation | e = e0 sin (0 - 7), (15) | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 6: Double-Energy Transients | source research review |
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0187transients-oscillation | ei = - e0 sin 7 = initial value of transient voltage. (16) | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 6: Double-Energy Transients | source research review |
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0196transients-oscillation | i = i\ cos 1/001 sin - , (21) | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 6: Double-Energy Transients | source research review |
elementary-lectures-electric-discharges-waves-impulses-eq-candidate-0197transients-oscillation | e = e\ cos - + z0ii sin - , (22) | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 6: Double-Energy Transients | source research review |
electric-discharges-waves-impulses-1914-eq-candidate-0159transients-oscillation | T = 2.92 - { 9.21 log’^ , ,\ . + .921 log’^ i ’ ^ ^ | Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients Lecture 5: Single-Energy Tra.Nsient Of Ironclad Circuit | source research review |
Editorial Use
Section titled “Editorial Use”This gallery is meant for discovery, not final citation. The strongest current source distribution is: Elementary Lectures on Electric Discharges, Waves and Impulses, and Other Transients (445), Radiation, Light and Illumination (398), Theoretical Elements of Electrical Engineering (310), Four Lectures on Relativity and Space (189). Promote a diagram or formula only after the scan, page label, exact caption, and mathematical notation are checked.