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Smoke laser

As said earlier in this chapter, the use of properly arranged ilkunination will improve the visibility of the smoke markedly. Extra light should be arranged so that the light beams ace directed almost directly into the eyes of the observer or into the lens of a camera. Direct dazzling must be avoided with tlie help of some shield. The use of a laser beam expanded to a sheet makes it possihle to isualize the airflow in a special layer in the room. This technique makes it possible to study the airflow in more detail, e.g, near an enclosure or around a machine. ... [Pg.1114]

With the discoveiy of electricity, the evolution of communications occurred at a rapid rate. Smoke signals that were used for hundreds of years to convey information at a word or two per minute were first replaced by the use of copper-based conductors, such as the telegraph, that transmitted twenty to forty words per minute. By the end of the twentieth century, lasers with fiber optic wires transmitted an entire book around the world in under a second. [Pg.277]

The incident flux used in the NBS smoke chamber is only a single value, at 2.5 w/cm2, which is a relatively mild flux for a fire, and cannot, thus represent all the facets of a fire. The light source is polychromatic, which causes problems of soot deposits and optics cleaning, as compared to measurements done using a monochromatic (laser) beam. Finally, the units of the normal output of this smoke chamber are fairly arbitrary and the data is of little use in fire hazard assessment. [Pg.524]

As shown in Fig. 12 fluid flow can be determined by measuring the doppler shift in laser radiation scattered from particles in the moving fluid stream. No sensor is required in the moving stream. The laser radiation focal point can be moved across the flow tube to measure velocity profiles. Fluid linear flows from 0.01 to 5000 inches (0.03 centimeter to 127 mctersi per second hate been measured. Contaminants, such as smoke, may have to be added to gases to provide scattering centers for the laser beam. [Pg.918]

CdO is used in connection with the stabilization of poly(vinyl chloride). This is discussed below in more detail. It also finds application in modifying the thermal properties of teflon and some rubbers. CdS is used in some smoke detectors, in lasers and in phosphors. The cadmium(II) halides are important as catalysts and are also used in pyrotechnics. Cadmium borates of the general type (Cd0)x(B203), are also used as phosphors. CdS04 is employed in the Weston cell, which is important as a voltage standard.137... [Pg.1026]

She went up to the city and bought a stack of new records, incense, bath salts, fresh meat for the cats. Found a bud forgotten weeks ago at the back of the candle drawer, smoked it and put on Kriider Dorfmeister. She was in debt thousands, the laser hit the best track. She turned it up and cooked dinner dancing. [Pg.47]

This technique involves the creation of a two-dimensional image of skin perfusion. It operates by emitting laser light on to the skin tissue, which upon partial absorption and diffuse scattering, is then reflected with doppler shifted frequencies from blood cells and with unshifted frequencies from stationary tissue. It is a popular method, as it is easy to use and non-invasive, however subjects must refrain from smoking for 4 h prior to measurements and no caffeine intake is permitted 1 h prior to measurements.26... [Pg.510]

The standard Cone Calorimeter (Section 14.3.3.2.1) described in ASTM E 1354 includes a smoke photometer to measure light extinction in the exhaust duct. The system is based on a laser light source. The same system is also standardized internationally, although it is described in a separate document from the main Cone Calorimeter standard (ISO 5660-2). Smoke measurements are reported in terms of the average specific extinction area (ASTM E 1354 and ISO 5660-2) and the smoke production rate and total smoke production for the period prior to ignition and the flaming period (ISO 5660-2). [Pg.376]

A major area of concern is the possibility that asbestos fibers adsorb carcinogens in smoke, such as benzidine, N,N-dimethylanaline, and benzo(a)pyrene, and carry them to cells. Investigations are being carried out to detect such chemical impurities on asbestos fiber surfaces by a technique known as laser microprobe mass analysis (Warner 1988). [Pg.220]

The quantities produced with the laser vaporization method were however not even sufficient for doing experiments to verify the proposed structure. This was solved by Kratschmer, Huffman and their students who had as early as in 1982, [144-146] i.e. three years before the discovery of Ceo in 1985, produced Ceo without knowing it. They used an electric arc in a helium atmosphere of 150 torr and produced a special kind of soot with a unique type of optical absorption known as the camel hump smoke in the UV region. Their recorded spectrum fitted however very nicely to some predictions of the present author [147]. After a number of trials, they found in 1990 [148] that the special carbon soot could be dissolved in benzene, which provided the possibility to separate Ceo from the carbon particles [149], record a UV visible spectrum and even fabricate crystals of Ceo and C70 and determine the crystal structure. Suddenly a new kind of carbon material had been found in addition to the commonly known diamond and graphite. [Pg.31]

Figure 15 shows the pattern made by the normal reflection of a detonation on a glass plate coated lightly with carbon soot, which may be from either a wooden match or a kerosene lamp. The cellular structure of the detonation front is quite evident. If a similarly soot-coated polished metal (or mylar) foil is inserted into a detonation tube, the passage of the detonation wave will leave a characteristic fish-scale pattern on the smoked foil. Figure 16 is a sequence of laser-Schlieren... [Pg.253]

The mass spectrum of the smoke produced directly without further processing gives strong peaks at miz = 720 and 840. However, the material which is solvent extracted gives the spectrum shown in Fig. 1. This should be compared with the laser vaporisation results -- and shows that the fullerencs C (n = 62,64,66,68, etc.) are also present and apparently stable in air. [Pg.36]

Figure 8.7 Schematic of visualization setup 5-watt Argon Laser illuminates smoke for capture on digital video. Figure 8.7 Schematic of visualization setup 5-watt Argon Laser illuminates smoke for capture on digital video.

See other pages where Smoke laser is mentioned: [Pg.396]    [Pg.401]    [Pg.1114]    [Pg.1172]    [Pg.463]    [Pg.527]    [Pg.1043]    [Pg.298]    [Pg.474]    [Pg.156]    [Pg.320]    [Pg.349]    [Pg.349]    [Pg.627]    [Pg.434]    [Pg.349]    [Pg.349]    [Pg.273]    [Pg.396]    [Pg.884]    [Pg.236]    [Pg.373]    [Pg.371]    [Pg.156]    [Pg.130]    [Pg.347]    [Pg.225]    [Pg.272]    [Pg.413]    [Pg.415]    [Pg.3843]    [Pg.2]    [Pg.35]    [Pg.663]    [Pg.641]   
See also in sourсe #XX -- [ Pg.280 ]




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