The radiation chemistry of aqueous solutions II. Radical and molecular yields for tritium β-particles

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Abstract

Assuming G (Fe 3+ ) =12.7 for aerated, acidified ferrous sulphate solutions, the following values have been measured (a) G (O 2 )Fe 2+ , Cu 2+ = 0, G (H 2 )Fe 2+ Cu 2+ = 0.51 ± 0.03, G (Fe 3+ )Cu 2+ = 1.06 ± 0.03 for the ferrous-cupric system, ( b ) G (Ce 3+ ) = 2.84 ± 0.05 for acidi­fied solutions of ceric sulphate ( c ) G Ce 3+ ) T1+ = 7.30 ± 0.025 for the ceric-thallous system ( d ) G (H 2 O 2 ) i = 1.03 + 0.06 for aerated 0.1N sulphuric acid and ( e ) G (H 2 ) = 0.935 ± 0.09 for 0.1N sulphuric acid and 0.607 ± 0.06 when 4 x 10 -5 M H 2 O 2 is also present. The equation G (Fe 3+ ) β+λ = 12.7 x + 15.5(1− x ), where x is the fraction of the total energy absorbed provided by β -particles, is valid for x = 0 to1. The following quantities are deduced: G H = 2.91 ± 0.01, G H 2 O 2 = 0.97 ± 0.02, G OH = 2.00 ± 0.08, G H 2 = 0.53 ± 0.05 5 and G -H 2 O = 3.97 ± 0.12. The predicted value for G (Fe 3+ ) -O 2 = 6.87 ± 0.13 is not attained unless [Fe 2+ ] ≥ 10 -3 M and [H 2 SO 4 ] ≥ 0.8N. These results are discussed and it is concluded that, contrary to earlier views, the primary process in T β -irradiation is closer to that of 60 Co γ -rays than that of α -particles.

Publisher

The Royal Society

Subject

Pharmacology (medical)

Reference7 articles.

1. C oatsw orth K . Collinson E. & D ainton F . S. i960 Trans. Faraday Soc. 56 1008.

2. Collinson E . D ainton F . S. & K roh J . 1962 Proc. Roy. Soc. A 265 407 (part I).

3. Disc;Faraday Soc.,1952

4. Molecular Product and Free Radical Yields of Ionizing Radiations in Aqueous Solutions

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