The radioactive decay process involves alpha and beta decay sequences. We can break down the steps as follows:
The original \(^{230}_{90}Th\) nucleus undergoes alpha decay, emitting an alpha particle (\(\alpha\)). After this decay, the resulting nucleus is \(^{226}_{88}Ra\).
The \(^{226}_{88}Ra\) nucleus undergoes alpha decay again, resulting in \(^{222}_{86}Rn\), emitting another alpha particle (\(\alpha\)).
The \(^{222}_{86}Rn\) nucleus undergoes alpha decay to form \(^{218}_{84}Po\), emitting another alpha particle (\(\alpha\)).
The \(^{218}_{84}Po\) nucleus undergoes alpha decay to form \(^{214}_{82}Pb\), emitting yet another alpha particle (\(\alpha\)).
The \(^{214}_{82}Pb\) nucleus undergoes beta decay, emitting a beta particle (\(\beta\)), and transforming into \(^{214}_{83}Bi\).
The \(^{214}_{83}Bi\) nucleus undergoes beta decay again, emitting a second beta particle (\(\beta\)), and transforming into \(^{214}_{84}Po\), which is the final product.
Thus, we see that there are 4 alpha decays and 2 beta decays. Therefore, the ratio of the number of alpha particles to beta particles is:
\[ \text{Ratio of } \alpha \text{ to } \beta = \frac{4}{2} = 2 \]
The ratio of the number of alpha particles to the number of beta particles emitted in this process is \(2\).
Let $ S $ denote the locus of the point of intersection of the pair of lines $$ 4x - 3y = 12\alpha,\quad 4\alpha x + 3\alpha y = 12, $$ where $ \alpha $ varies over the set of non-zero real numbers. Let $ T $ be the tangent to $ S $ passing through the points $ (p, 0) $ and $ (0, q) $, $ q > 0 $, and parallel to the line $ 4x - \frac{3}{\sqrt{2}} y = 0 $.
Then the value of $ pq $ is
Let $ y(x) $ be the solution of the differential equation $$ x^2 \frac{dy}{dx} + xy = x^2 + y^2, \quad x > \frac{1}{e}, $$ satisfying $ y(1) = 0 $. Then the value of $ 2 \cdot \frac{(y(e))^2}{y(e^2)} $ is ________.