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Radiation track

Fig. 27. Scanning electron micrograph (a) and cross-sectional comparison (b) of screen and depth filters both having a nominal particulate cut-off of 0.4 flm. The screen filter (a Nuclepore radiation track membrane) captures particulates at the surface. The phase-inversion ceUulosic membrane traps the... Fig. 27. Scanning electron micrograph (a) and cross-sectional comparison (b) of screen and depth filters both having a nominal particulate cut-off of 0.4 flm. The screen filter (a Nuclepore radiation track membrane) captures particulates at the surface. The phase-inversion ceUulosic membrane traps the...
The IRT method was applied initially to the kinetics of isolated spurs. Such calculations were used to test the model and the validity of the independent pairs approximation upon which the technique is based. When applied to real radiation chemical systems, isolated spur calculations were found to predict physically unrealistic radii for the spurs, demonstrating that the concept of a distribution of isolated spurs is physically inappropriate [59]. Application of the IRT methodology to realistic electron radiation track structures has now been reported by several research groups [60-64], and the excellent agreement found between experimental data for scavenger and time-dependent yields and the predictions of IRT simulation shows that the important input parameter in determining the chemical kinetics is the initial configuration of the reactants, i.e., the use of a realistic radiation track structure. [Pg.92]

An important result of the theoretical studies of the multipair effects is that the recombination kinetics in a cluster of ions, in which the initial separation between neighboring cations is 1 nm, is faster than the corresponding decay kinetics of a single ion pair [18]. Furthermore, the escape probability is lower than the Onsager value [Eq. (15)], and decreases with increasing number of ion pairs in the cluster (a relative decrease of about 30% for two ion pairs, and about 50% for five ion pairs). The average electron escape probability in radiation tracks obviously depends on the distribution of ionization events in the tracks, which is determined by the type of radiations and their energy. [Pg.268]

Green NJB, Pilling MJ, Pimblott SM, Clifford P. (1990) Stochastic modeling of fast kinetics in a radiation track. J Phys Chem 94 251-258. [Pg.55]

The scope of applications of MF has been broadened in recent years by the introduction of inert membranes, particularly polypropylene, polycarbonate, and Teflon . In general, these materials cannot be made by the methods developed for the cellulosics because of their insolubility. Both Teflon and pol)propylene MF membranes have been made by a controlled stretching procedure in which microtears are introduced Microporous polycarbonate membranes have been prepared by a unique radiation-track-etch method A thin polycarbonate film is exposed to ionizing radiation which leaves labile sites that can later be chemically etched to produce straight-throi channels. The pore size can be controlled by the etching conditions. The pores in these membranes, contrary to those in cellulosic membranes, are quite uniform in diameter. [Pg.100]

Pagel M, Braun JJ, Disnar JR, Martinez L, Renac C, Vassem G (1997) Thermal history constraints from studies of organic matter, clay minerals, fluid inclusions and apatite fission tracks at the Ardeche paleo-margin (BAI Drill Hole, CPF Program), France. J Sed Res 67 235-245 Paretzke HG (1986) Radiation track structure theory In Freeman GR (ed) Kinetics of Homogeneons Processes. John Wiley, New York, p 89-170... [Pg.627]

In a radiation track, the geminate radical ion pairs originate in singlet state in which the partner spins are antiparallel and the total electron spin S is zero. Description of the pair spin evolution in an arbitrary magnetic field is a fairly complex problem. Common, however, is the fact that the expression for the... [Pg.67]

The feasibility of observing these effects and thus, of extracting the useful information is determined by the proper choice of charge acceptors with suitable ESR spectra. These acceptors play the role of molecular probes in studying the primary processes in a radiation track. This review is limited to the manifestations of spin coherence in the recombination of radical ion in irradiated hydrocarbon solutions. Although certain aspects of these studies are available in the literature [6,7,11], some prospects of their application for studying track processes have became evident only recently. [Pg.68]

In irradiated solutions this fraction is substantially below unity because of the complex structure of the radiation track. While isolated pairs are believed to be singlet correlated, for a double pair, the fraction might be as low as 1/2 due to cross recombination. For multi-pair spurs, the spin correlation might be completely lost. [Pg.75]

Figure 2 Schematic representation of the formation of a DNA double strand break as the radiation track deposits energy (circles). The zigzag arrows represent random diffusion of the water radicals. Figure 2 Schematic representation of the formation of a DNA double strand break as the radiation track deposits energy (circles). The zigzag arrows represent random diffusion of the water radicals.
DNA acting as a medium to facilitate charge transfer. The distance of charge transfer on the whole is probably limited otherwise the fingerprint of the radiation track, especially at high LET, would be lost and consequently the enhanced radiosensitivity of high LET radiation. The two types of clustered DNA damage discussed are... [Pg.617]

TABLE 18.2. Ionization clusters produced directly in a DNA-related target by a single radiation track. (From Goodhead, VNSCEAR) ... [Pg.479]

Ballarini F, Ottolenghi A. Models of chromosome aberration induction an example based on radiation track structure. Cytogenet Genome Res 2004 104(l-4) l49-56. [Pg.207]

Counting of High Energy Radiation Tracks. A computerized Image analyzer, the Cambridge Instrument model 900, was used to count the radiation tracks of the Irradiated polycarbonate samples. The measurements Include track size (diameter), track density In each field of view, roundness, sample area In each field, and total area of the sample. Samples of polycarbonates examined Included those prepared In our laboratory and neutron Irradiated samples provided by Dr. G. Tarle of University of California at Berkeley. [Pg.303]

The Cambridge Instruments Quantlmet 900 Image Analyzer was used to analyze the radiation tracks on exposed CR-39 polymer. This system features a computer controlled stage and focus system. Automatic focus was selected for the microscope. These accessories allow the system to automatically scan samples for features of Interest over an average area of 8cm x 10cm, while keeping the... [Pg.305]


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