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      "status": "candidate",
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      "line_start": 922,
      "section_id": "radiation-light-and-illumination-lecture-01",
      "section_label": "Lecture 1: Nature And Different Forms Of Radiation",
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      "id": "radiation-light-and-illumination-fig-009",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 9,
      "caption": "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",
      "status": "candidate",
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      "line_start": 1016,
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      "section_label": "Lecture 1: Nature And Different Forms Of Radiation",
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      "id": "radiation-light-and-illumination-fig-010",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 10,
      "caption": "(red, orange and yellow) with increase in temperature, the light FIG. 10. 12",
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      "line_start": 1075,
      "section_id": "radiation-light-and-illumination-lecture-01",
      "section_label": "Lecture 1: Nature And Different Forms Of Radiation",
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      "id": "radiation-light-and-illumination-fig-011",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 11,
      "caption": "of the lower frequencies of visible radiation, red or orange. FIG. 11. In the tungsten lamp at high brilliancy and more still in the",
      "status": "candidate",
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      "line_start": 1094,
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      "section_label": "Lecture 1: Nature And Different Forms Of Radiation",
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      "id": "radiation-light-and-illumination-fig-012",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 12,
      "caption": "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-",
      "status": "candidate",
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      "id": "radiation-light-and-illumination-fig-013",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 13,
      "caption": "o — ^^ — o FIG. 13. has been measured by Herz by producing standing waves by combination of main wave and reflected wave.",
      "status": "candidate",
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      "line_start": 1268,
      "section_id": "radiation-light-and-illumination-lecture-01",
      "section_label": "Lecture 1: Nature And Different Forms Of Radiation",
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      "id": "radiation-light-and-illumination-fig-014",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 14,
      "caption": "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",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 1506,
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      "id": "radiation-light-and-illumination-fig-015",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 15,
      "caption": "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",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 1654,
      "section_id": "radiation-light-and-illumination-lecture-02",
      "section_label": "Lecture 2: Relation Of Bodies To Radiation",
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      "id": "radiation-light-and-illumination-fig-016",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 16,
      "caption": "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,",
      "status": "candidate",
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      "line_start": 1819,
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      "section_label": "Lecture 2: Relation Of Bodies To Radiation",
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      "id": "radiation-light-and-illumination-fig-017",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 17,
      "caption": "VIOLET FIG. 17. a number of very faint red and orange lines, of which three are indicated dotted in Fig. 17.",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 1885,
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      "section_label": "Lecture 2: Relation Of Bodies To Radiation",
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      "id": "radiation-light-and-illumination-fig-018",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 18,
      "caption": "perature rise, their brilliancy is greatly increased. FIG. 18. Combinations of the different types of spectra: continuous spectrum, line spectrum, band spectrum, reversed spectrum,",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 1974,
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      "section_label": "Lecture 2: Relation Of Bodies To Radiation",
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      "id": "radiation-light-and-illumination-fig-019",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 19,
      "caption": "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.",
      "status": "candidate",
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      "line_start": 2013,
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      "id": "radiation-light-and-illumination-fig-021",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 21,
      "caption": "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.",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 2582,
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      "section_label": "Lecture 3: Physiological Effects Of Radiation",
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      "id": "radiation-light-and-illumination-fig-022",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 22,
      "caption": "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",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 2618,
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      "section_label": "Lecture 3: Physiological Effects Of Radiation",
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      "id": "radiation-light-and-illumination-fig-023",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 23,
      "caption": "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",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 2694,
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      "id": "radiation-light-and-illumination-fig-024",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 24,
      "caption": "\\ FIG. 24. (1 meter-candle is the illumination produced by 1 candle power",
      "status": "candidate",
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      "line_start": 2809,
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      "id": "radiation-light-and-illumination-fig-025",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 25,
      "caption": "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",
      "status": "candidate",
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      "line_start": 2945,
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      "id": "radiation-light-and-illumination-fig-026",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 26,
      "caption": "YELLOW GREEN FIG. 26. carbon filament would be somewhat like C. That is, the physio-",
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      "line_start": 3036,
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    {
      "id": "radiation-light-and-illumination-fig-027",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 27,
      "caption": "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-",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 4062,
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      "section_label": "Lecture 5: Temperature Radiation",
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      "links": {
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      "id": "radiation-light-and-illumination-fig-028",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 28,
      "caption": "weight, exhibit a periodicity in their properties which permits FIG. 28. a systematic study of their properties. In diagram Fig. 28 the",
      "status": "candidate",
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      "line_start": 4310,
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      "section_label": "Lecture 5: Temperature Radiation",
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      "id": "radiation-light-and-illumination-fig-029",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 29,
      "caption": "\\\\ FIG. 29. power required to maintain the temperature is correspondingly less, hence the efficiency is the same and merely a larger radiator",
      "status": "candidate",
      "verification": "needs-verification",
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    {
      "id": "radiation-light-and-illumination-fig-030",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 30,
      "caption": "where colored radiation or luminescence is present. Thus the FIG. 30. radiation given by the interior of a closed body of uniform tem- perature ceases to be black body radiation if the interior is filled",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 4923,
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      "links": {
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    {
      "id": "radiation-light-and-illumination-fig-031",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 31,
      "caption": "one, the other from the other terminal. They are stationary FIG. 31. only if the gas pressure is perfectly constant, but separate and contract with the slightest change of pressure, hence are almost",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 5467,
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      "section_label": "Lecture 6: Luminescence",
      "section_slug": "lecture-06",
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      "id": "radiation-light-and-illumination-fig-032",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 32,
      "caption": "II II FIG. 32. decreasing gas pressure the voltage consumed in the space be-",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 5499,
      "section_id": "radiation-light-and-illumination-lecture-06",
      "section_label": "Lecture 6: Luminescence",
      "section_slug": "lecture-06",
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    },
    {
      "id": "radiation-light-and-illumination-fig-033",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 33,
      "caption": "and you see the striated Geissler discharge through mercury FIG. 33. vapor appear between terminals 2 and 3, giving the green light> of the mercury spectrum. The terminals are quiet, as they do",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 5680,
      "section_id": "radiation-light-and-illumination-lecture-06",
      "section_label": "Lecture 6: Luminescence",
      "section_slug": "lecture-06",
      "links": {
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    {
      "id": "radiation-light-and-illumination-fig-034",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 34,
      "caption": "3J=10 OHMS FIG. 34. and the spectrum of the arc is the spectrum of the negative ter- minal. An exception herefrom, occurs only in those cases in",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 5719,
      "section_id": "radiation-light-and-illumination-lecture-06",
      "section_label": "Lecture 6: Luminescence",
      "section_slug": "lecture-06",
      "links": {
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        "book_coverage": "/Charles-Proteus-Steinmetz-Texts-AI-Decoded/book-coverage/radiation-light-and-illumination/"
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    },
    {
      "id": "radiation-light-and-illumination-fig-035",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 35,
      "caption": "tendency exists of shifting the starting point, and the arc becomes FIG. 35. LUMINESCENCE.",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 5836,
      "section_id": "radiation-light-and-illumination-lecture-06",
      "section_label": "Lecture 6: Luminescence",
      "section_slug": "lecture-06",
      "links": {
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    },
    {
      "id": "radiation-light-and-illumination-fig-036",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 36,
      "caption": "lished by the vapor stream coming from the negative. Thus the FIG. 36. arc can be started by merely starting a conducting vapor stream from the negative, as by an auxiliary arc. As soon as this con-",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 5860,
      "section_id": "radiation-light-and-illumination-lecture-06",
      "section_label": "Lecture 6: Luminescence",
      "section_slug": "lecture-06",
      "links": {
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    {
      "id": "radiation-light-and-illumination-fig-037",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 37,
      "caption": "draw it out until the arc flame wraps itself all around terminal FIG. 37. B} but the arc does not transfer. I even insert 10 ohms resist- ance rl in series with C (Fig. 37), so that the voltage AB is about",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 5898,
      "section_id": "radiation-light-and-illumination-lecture-06",
      "section_label": "Lecture 6: Luminescence",
      "section_slug": "lecture-06",
      "links": {
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    {
      "id": "radiation-light-and-illumination-fig-038",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 38,
      "caption": "ws FIG. 38. negative, that is, at a higher potential difference and a shorter distance against A than B is. I even hold C for some time in",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 5941,
      "section_id": "radiation-light-and-illumination-lecture-06",
      "section_label": "Lecture 6: Luminescence",
      "section_slug": "lecture-06",
      "links": {
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    {
      "id": "radiation-light-and-illumination-fig-039",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 39,
      "caption": "MAA FIG. 39. current during one half-wave only, but no current at all dur- ing .the other. I show you this experimentally, using 50 volts",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 5988,
      "section_id": "radiation-light-and-illumination-lecture-06",
      "section_label": "Lecture 6: Luminescence",
      "section_slug": "lecture-06",
      "links": {
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    },
    {
      "id": "radiation-light-and-illumination-fig-040",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 40,
      "caption": "60 CYCLES FIG. 40. terminals. The cause is obvious: to maintain an arc between",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 6045,
      "section_id": "radiation-light-and-illumination-lecture-06",
      "section_label": "Lecture 6: Luminescence",
      "section_slug": "lecture-06",
      "links": {
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        "workbench": "/Charles-Proteus-Steinmetz-Texts-AI-Decoded/chapter-workbench/radiation-light-and-illumination/lecture-06/",
        "book_coverage": "/Charles-Proteus-Steinmetz-Texts-AI-Decoded/book-coverage/radiation-light-and-illumination/"
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    },
    {
      "id": "radiation-light-and-illumination-fig-041",
      "source_id": "radiation-light-and-illumination",
      "source_title": "Radiation, Light and Illumination",
      "figure_number": 41,
      "caption": "and thereby increasing radiation, etc. For a 13-mm. (0.5-in.) FIG. 41. arc it is approximately shown as Curve II in Fig. 41 : 20 volts",
      "status": "candidate",
      "verification": "needs-verification",
      "line_start": 6080,
      "section_id": "radiation-light-and-illumination-lecture-06",
      "section_label": "Lecture 6: Luminescence",
      "section_slug": "lecture-06",
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      "caption": "\\r FIG. 54. ous height follow each other. Thus with an average arc volt- age of 75, momentary peaks of 85 volts will probably be reached",
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      "caption": "as shown diagrammatically in its simplest form in Fig. 55, the FIG. 55. two white screens A and B are illuminated, the one, A, by the light, L, which is to be tested, the other, B, by the standard S,",
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      "figure_number": 89,
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      "source_title": "Radiation, Light and Illumination",
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      "caption": "(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",
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      "figure_number": 91,
      "caption": "the point P receives light from all points of the envelope G as FIG. 91. 3-B",
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      "figure_number": 93,
      "caption": "^ FIG. 93. be directed into the horizontal (or any other desired) direction, and the entire lens then appears luminous, as virtual radiator.",
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      "source_title": "Radiation, Light and Illumination",
      "figure_number": 94,
      "caption": "tions thereof are used, as prisms, as shown in Fig. 94, and this FIG. 94. method of light control thus called \"prismatic refraction,\" or, where the light does not pass through, but is reflected and turned",
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      "figure_number": 96,
      "caption": "230 RADIATION, LIGHT, AND ILLUMINATION. FIG. 96. FIG. 97,",
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      "caption": "side illumination, and are rounded off where the branches join. FIG. 98. Fig. 99 gives the intensity curves for the same angles, w = 30,",
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      "caption": "45, 60, and 75 deg., for uniform illumination only in the hori- FIG. 99. zontal plane beneath the lamp, but no illumination beyond",
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      "caption": "candle power: FIG. 100. I. The direct-current enclosed carbon arc, with clear inner",
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      "caption": "08 0,4 06 08 10 12 It 16 18 20 22 24 26 28 FIG. 101. curve of the character discussed in Fig. 92. III. The magnetite",
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      "caption": "lamp. Such a distribution curve can, for instance, be produced FIG. 107. by a spiral filament F (Fig. 108) located eccentric in a spher- ical globe G, of which the upper part is clear glass and covered",
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      "caption": "of table, etc.). FIG. 108. 244 RADIATION, LIGHT, AND ILLUMINATION.",
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      "source_title": "Radiation, Light and Illumination",
      "figure_number": 111,
      "caption": "by 7. It is given in Fig. 111. FIG. 111. The illumination, i, at any point, P, then is derived by adding the illumination ia, ib, ic, id of the four lamps a, 6, c, d, taken",
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      "caption": "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 effective negative resistance,",
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