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Permanent radiation source

In the last several decades, both experimental data and theoretical studies [5, 9, 13-15] have revealed the effect of similar defect aggregation in the course of the bimolecular A+B —> 0 reaction under permanent particle source (irradiation) - the phenomenon similar to that discussed in previous Chapters for the diffusion-controlled concentration decay. Radiation-induced aggregation of similar defects being observed experimentally at 4 K after prolonged X-ray irradiation [16] via both anomalously high for random distribution concentration of dimer F2 centres (two nearest F centres) and directly in the electronic microscope [17], permits to accumulate defect concentrations whose saturation value exceed by several times that of the Poisson distribution. [Pg.388]

At low temperatures dissimilar-defect segregation arises under permanent particle source due to local fluctuations of particle (defect) densities. Radiation-induced production by a change of two or more similar defects (say, A) nearby creates a germ of their aggregate which is more stable and has a greater chance to survive rather than two isolated defects A since the probability that two or more defects B will be created statistically in the same... [Pg.388]

The analysis conducted in this Chapter dealing with different theoretical approaches to the kinetics of accumulation of the Frenkel defects in irradiated solids (the bimolecular A + B —> 0 reaction with a permanent particle source) with account taken of many-particle effects has shown that all the theories confirm the effect of low-temperature radiation-stimulated aggregation of similar neutral defects and its substantial influence on the spatial distribution of defects and their concentration at saturation in the region of large radiation doses. The aggregation effect must be taken into account in a quantitative analysis of the experimental curves of the low-temperature kinetics of accumulation of the Frenkel defects in crystals of the most varied nature - from metals to wide-gap insulators it is universal, and does not depend on the micro-mechanism of recombination of dissimilar defects - whether by annihilation of atom-vacancy pairs (in metals) or tunnelling recombination (charge transfer) in insulators. [Pg.461]

Quantitative measurements of diffusion coefficients under bombardment, made recently, substantiate the existence of an enhancement. In lead (122a), a flux of 3 x lO a cm 2 sec i increased the self-diffusion coefficient by a factor of about 100 at 20° and 10 at 40°. The effect was a dynamic one, not the result of permanent damage, since the original rate was again observed after the radiation source was removed. Heit-kamp, Biermann, and Lundy (122b) found an increase in the diffusion coefficient of lead in silver under alpha bombardment, and the increase agrees satisfactorily with that for lead in lead. Thus a flux of 1 X lO i cm 2 sec i gave rise to an 8.8% increase in diffusion coefficient for lead in silver at 438°, and one of 3 x lO o to an increase of 3.3% for lead in lead at 84°. [Pg.182]

Pressure-sensitive adhesives are the essential components of adhesive tapes and labels. They are polymers with permanent tack, usually applied on substrates (plastic/metal films, siliconized papers). To enhance their tack, compounds with high inherent tack are added, for example, resins, plasticizers. Pressure-sensitive adhesives reach their adhesion on the material to be bonded by contact pressure, from which the term pressure-sensitive adhesive (PSA) derives. Apart from electron radiation, also UV-radiation curing described in Section 4.3.2 is applied in adhesive tape manufacturing. The monomer molecules to be polymerized are applied, in liquid form, to the substrates to be coated by rolling and are continuously cured to a polymer layer within seconds under a UV-radiation source. Depending on their composition, predetermined adhesion values can be adjusted. The adhesive tapes can be subsumed under the systems shown in Figure 5.4 ... [Pg.53]

A. Thermoluminescent dosimeter (TLD) badges used to provide a permanent record of the cumulative exposure to the whole body must be worn on the trunk (below the shoulders and above the hips) outside of clothing on the portion or area of the body nearest the radiation source. The dosimeter window must face out from the body. [Pg.96]

As was discussed in the preceding sections, in many operating nuclear power plants the buildup of contamination results in radiation levels at the systems and components which lead to considerable radiation exposure of workers, in particular during the course of inspection and repair work. In order to meet this situation, permanent or temporary shieldings are frequently installed and, as far as necessary, remote-controlled and automatically operating equipment is employed to reduce, as far as possible, the stay time of people in the radiation field. Nevertheless, there are often operations to be carried out whose preparation and execution make the removal or at least a radical reduction in the radiation sources, i. e. a decontamination of the respective regions, necessary. [Pg.376]

At the Savannah River Ecology Laboratory, a mobile radiation source was developed that could be used within the permanent study area adjacent to the laboratory or trucked into the field to specific sites of interest (Golley and McCormick, 1966 McCormick and Golley, 1966). It consisted of 9200 Ci Cs encased in a stainless steel capsule that was placed in a lead container (Figure... [Pg.32]

To our knowledge, only one study utilizing a radiation source in the field was conducted to evaluate the effects of exclusively low levels of ionizing radiation on an ecosystem. This interesting study was developed by Dr. Norman R. French at the U.S. Atomic Energy Commission s Nevada Test Site. A 20-acre circular area, enclosed with a rodent-proof fence, was irradiated by a 33,000-Ci Cs source located in the center of the circular area (French, 1964). A shield of varying thickness was used in an attempt to develop a reasonably uniform radiation level over the circular area. The shield was fixed permanently at the... [Pg.38]

UV-curable adhesives, and, in general, radiation-curable adhesives, use UV light or other radiation sources to initiate curing. A permanent bond forms without application of heat by means of free-radical chemistry. The advantages of UV curing include lower application temperature (120—140° C),... [Pg.174]

Figure 10.9—Schematic diagram of various infrared spectrometers, a) Single beam model its principle is still used for measurements at a single wavelength b) double beam model c) single beam Fourier transform instrument. Contrary to UV/VIS spectrometers, the sample is placed immediately after the light source. Since photon energy in this range is insufficient to break chemical bonds and degrade the sample, it can be permanently exposed to the full radiation of the source. Figure 10.9—Schematic diagram of various infrared spectrometers, a) Single beam model its principle is still used for measurements at a single wavelength b) double beam model c) single beam Fourier transform instrument. Contrary to UV/VIS spectrometers, the sample is placed immediately after the light source. Since photon energy in this range is insufficient to break chemical bonds and degrade the sample, it can be permanently exposed to the full radiation of the source.
In our opinion, this book demonstrates clearly that the formalism of many-point particle densities based on the Kirkwood superposition approximation for decoupling the three-particle correlation functions is able to treat adequately all possible cases and reaction regimes studied in the book (including immobile/mobile reactants, correlated/random initial particle distributions, concentration decay/accumulation under permanent source, etc.). Results of most of analytical theories are checked by extensive computer simulations. (It should be reminded that many-particle effects under study were observed for the first time namely in computer simulations [22, 23].) Only few experimental evidences exist now for many-particle effects in bimolecular reactions, the two reliable examples are accumulation kinetics of immobile radiation defects at low temperatures in ionic solids (see [24] for experiments and [25] for their theoretical interpretation) and pseudo-first order reversible diffusion-controlled recombination of protons with excited dye molecules [26]. This is one of main reasons why we did not consider in detail some of very refined theories for the kinetics asymptotics as well as peculiarities of reactions on fractal structures ([27-29] and references therein). [Pg.593]


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