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Shielding, radiation liquid

Weak beta radiation and alpha particles often cannot penetrate the covering material but the use of a scintillant, which, together with the sample, will dissolve in a suitable solvent, enables a similar technique to be used. Liquid scintillation counters usually consist of two light-shielded photomultiplier... [Pg.204]

The liquid helium evaporates in the heat exchanger and thus cools dovm the cryopanel. The waste gas which is generated (He) is used in a second heat exchanger to cool the baffle of a thermal radiation shield vi/hich protects the system from thermal radiation coming from the outside. The cold helium exhaust gas ejected by the helium pump is supplied to a helium recovery unit. The temperature at the cryopanels can be controlled by controlling the helium flow. [Pg.54]

Power supplies, 300-V for polyacrylamide gels 2000- to 3000-V for some applications Racks, for test tubes and microcentrifuge tubes Radiation shield, Lucite or Plexiglas Radioactive waste containers, for liquid and solid waste Razor blades... [Pg.1321]

The most often used unit to quantify the activity of any radioactive material is the curie (Ci). For most level detection applications, source strengths of 100 millicuries (mCi) or less are satisfactory. A 1 Ci source will produce a dose of 1 roentgen (r) at a receiver placed 1 m (3 ft) away from the source for 1 h. Radiation is attenuated when it penetrates liquids or solids, and the rate of attenuation is a function of the density of the material. The higher the density, the more attenuation the shielding material will provide. Figure 3.122 shows how various thicknesses of different materials will attenuate (reduction factor—NB) the intensity of radiation and result in different degrees of attenuation. [Pg.460]

The circular atom microwave spectroscopy experimental set-up is sketched on Fig. 1-a. A thermal beam of Li atoms crosses three sections of the apparatus the excitation, the microwave interaction region and the detection zone. The whole set-up is protected from room temperature thermal radiation by a liquid nitrogen cooled shield (which can be replaced in a later stage of the experiment by a liquid helium cooled one). [Pg.944]

Components for X-ray and radiation shielding (W, HM, HM-polymer) [7.20-7.23]. Typical examples are containers or flasks for radioactive materials and liquids, shielded syringes (Fig. 7.16), shielding eonstraction parts such as collimators in computer tomographic scanners (Fig. 7.17), radiation therapy instmments, and containers and shielding for oil prospecting using radioactive sources (Fig. 7.18). [Pg.297]

The space between the two tanks is filled with layers of thin aluminized plastic film separated by a lightweight coarse plastic screen. These serve as a shield against the passage of thermal radiation from the outer to the inner tank. The air between the tanks and around the insulation is removed with a vacuum pump. The high vacuum serves to stop heat flow by conduction. The liquid fill and gas withdrawal lines are coaxial that is, one inside the other. They are made from materials with low thermal conductivity and are coiled inside the insulation to minimize heat flow down the length of the pipe from the outside into the inner tank. [Pg.131]

Fig. 4.6. Cross-section of an optical continuous-flow cryostat (CF 204 of Oxford Instruments), with the extremity of the removable transfer tube inserted, but without sample holder. The evacuation valve at the top is masked by the sample port. The optional windows on the radiation shield can be replaced by metallic irises to reduce the field of view. This cryostat can be fitted with one or two more optical windows at 90° from the main optical axis for additional excitation, and also with a down-looking window. The arrows indicate the direction of the flow of liquid or gaseous helium. Reproduced with permission from Oxford Instruments... Fig. 4.6. Cross-section of an optical continuous-flow cryostat (CF 204 of Oxford Instruments), with the extremity of the removable transfer tube inserted, but without sample holder. The evacuation valve at the top is masked by the sample port. The optional windows on the radiation shield can be replaced by metallic irises to reduce the field of view. This cryostat can be fitted with one or two more optical windows at 90° from the main optical axis for additional excitation, and also with a down-looking window. The arrows indicate the direction of the flow of liquid or gaseous helium. Reproduced with permission from Oxford Instruments...
Present photosynthetic life is protected from harmful solar radiation by oxygen and ozone. Thus we must ask how these original creatures survived and evolved to the present state even as they formed the protective shield which their descendants would enjoy. It is possible that they were a form of algae, protected by liquid water from the sun s rays. It has also been suggested that primitive microbes could have been protected by layers of purine and pyrimidine bases, which absorb in the ultraviolet range (Sagan, 1973). [Pg.5]

Figure 6.35. DTA calorimeter cell described by Barral) et al. (94). A. B. copper sample cups. 4-mra O. D. by 6 mm C,copper reference cup D. two-conductor ceramic supports. 3-mm diameter by 50 mm E. copper radiator shield, 35-mm diameter by 53 mm F, program-sensing thermocouple G. liquid CO cooling gas jet H, electric furnace. 45-mm id by 100 cm 1. copper base plate. 38-mm diameter. Figure 6.35. DTA calorimeter cell described by Barral) et al. (94). A. B. copper sample cups. 4-mra O. D. by 6 mm C,copper reference cup D. two-conductor ceramic supports. 3-mm diameter by 50 mm E. copper radiator shield, 35-mm diameter by 53 mm F, program-sensing thermocouple G. liquid CO cooling gas jet H, electric furnace. 45-mm id by 100 cm 1. copper base plate. 38-mm diameter.

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See also in sourсe #XX -- [ Pg.403 ]




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