Preparation problems
N = No 2-t/t1/2
t1/2 = 3.82 days (from table 43-2)(a) N(1 day) = No 2-1/3.82 = 0.834 No so 83.4% of original remains after 1 day
(b) N(1 week) = No 2-7/3.82 = 0.281 No so 28.1% of original remains after 1 week
(c) N(1 month) = No 2-30/3.82 = 0.004 No so 0.4% of original remains after 1 month
R(t) = Ro 2 -t/t1/2
ln( R(t)/Ro ) = - (t/t1/2) ln2
t = - t1/2 [ ln ( R(t)/Ro ) ] / ln 2
= ( - 8.04 days / 0.693 ) ln ( R(t)/Ro )
= ( - 11.6 days ) ln ( R(t)/Ro ) Poland: t = ( - 11.6 d ) ln (1000/2000) = 8.04 days
Sweden: t = ( - 11.6 d ) ln (2000/2900) = 4.31 days
Austria: t = ( - 11.6 d ) ln (370/1500) = 16.23 days
Germany: t = ( - 11.6 d ) ln (500/1184) = 10.0 days
(a) According to Fig 43-19, Po-210 is a decay product of Bi-210 (from b decay), so the equation is
21083Bi -> 21084Po + e- + v (b) Also from Fig 43-19, Po-210 decays by a decay into Pb-206, so the equation is
21084Po -> 20682Pb + 42He (c) If you look at the effect of one cigarette, the helath effects would be much better for a different half-life. A half life of 1 day would mean that much of the Po would decay before the cigarette was even smoked. A half-life of 10 years would mean that there would bevery little radiation, since R = lN and a big half-life makes a small l. On the other hand, for a regular smoker, it will probably not make much difference either way. Because the smoker is constantly replenishing the Po in his/her lungs, the Po level would reach some equilibrium value. If the half-life were very short, there would not be much Po in the lung at any given time, but with the large decay constant the activity would still be fairly high. If the half-life were very long, then there would be a large amount of Po built up, but the activity would be about the same since the decay constant is smaller for this case. The bottom line is that it is hard to change R. If l is big, then N is small, but if l is small, then N gets big, so the product of the two is more or less constant and depends more on how many cigarettes he smokes rather than the half-life.
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