Recent Advances in Multidisciplinary Applied Physics. by A. Méndez-Vilas (Eds.)

By A. Méndez-Vilas (Eds.)

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Instr. Meth. 203, 551-559 (1982). 7. , Kadner K. and Ktihne H. Inter-comparison study of the detection characteristics of the CR-39 SSNTD for Light ions: Present status of the BesanconDresden approaches. Radiat. Meas. 31 89-98 (1999). 8. , Rahamay, El. and Chambaudet, A. " modelized and experimental uncertainties. Nucl. Tracks Radiat. Meas. 21,357-365 (1993). 34 9. I. and Solarz, M. Measurement of general etch rate for CR-39 plastic at short distance scale. Nucl. Instr. Meth. B. 132, 109-113 (1997).

41092-Sevilla. Spain. S. Arquitectura, Universidad de Sevilla. Avda. Reina Mercedes 2, E-41012-Sevilla, Spain. 3Departamento de Fisica Aplicada I, E. T. Agricola, Universidad de Sevilla. - Sevilla, Spain. Abstract. A 3D dispersion model has been constructed in order to simulate the dispersion in marine scenarios of conservative nuclear contaminants originated in accidents or industrial releases. The model has been validated taken the Baltic Sea as the physical scenario, and selecting the ~37Cswith origin in the Chernobyl accident as the substance that experimentedthe dispersion.

A comparison Fig. 2. (a) The relationship between the V ratio and the residual range. Open circles" Experimental data; Solid line" best fit line. (b) The V functions from the present project (solid line) and from Brunet al. (1999) (dotted line). 5 MeV. Etching was conducted in 7N NaOH at 70~ The etching duration 33 ranged between 4 and 7 h. The track diameters were measured using an OLYMPUS BH2 microscope linked with an image analyzing system. 4 ~tm at a magnification of 1000. From Fig. 2(b), we can see that the trends for the two V functions are generally commensurate with one another, both of them showing a 'Bragg peak'.

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