161.
The half life of radioactive Radon is 3.8 days. The time at the end of which $$\frac{1}{{20}}th$$ of the radon sample will remain undecayed is (given $${\log _{10}}e = 0.4343$$ )
$$\eqalign{
& {t_{\frac{1}{2}}} = 3.8\,{\text{day}} \cr
& \therefore \lambda = \frac{{0.693}}{{{t_{\frac{1}{2}}}}} = \frac{{0.693}}{{3.8}} = 0.182 \cr} $$
If the initial number of atom is $$a = {A_0}$$ then after time $$t$$ the number of atoms is $$\frac{a}{{20}} = A.$$ We have to find $$t.$$
$$\eqalign{
& t = \frac{{2.303}}{\lambda }\log \frac{{{A_0}}}{A} = \frac{{2.303}}{{0.182}}\log \frac{a}{{\frac{a}{{20}}}} \cr
& = \frac{{2.303}}{{0.182}}\log 20 = 16.46\,{\text{days}}\left( {{\text{approx}}} \right) \cr} $$
162.
A radioactive sample consists of two distinct species having
equal number of atoms initially. The mean life time of one
species is $$\tau $$ and that of the other is $$5\tau .$$ The decay products in both cases are stable. A plot is made of the total number of radioactive nuclei as a function of time. Which of the following figures best represent the form of this plot?
$$\eqalign{
& {N_1} = {N_0}{e^{ - {\lambda _1}t}} = {N_0}{e^{ - \frac{t}{\tau }}}\,......\left( {\text{i}} \right) \cr
& {\text{as}}\,\tau = \frac{1}{{{\lambda _1}}} \cr
& {N_2} = {N_0}{e^{ - {\lambda _2}t}} = {N_0}{e^{ - \frac{t}{{5\tau }}}}\,......\left( {\text{ii}} \right)\,{\text{as }}5\tau = \frac{1}{{{\lambda _2}}} \cr} $$
Adding (i) and (ii) we get
$$N = {N_1} + {N_2} = {N_0}\left( {{e^{ - \frac{t}{\tau }}} + {e^{ - \frac{t}{{5\tau }}}}} \right)$$
(A) is NOT the correct option as there is a time $$\tau $$ for
which $$N$$ is constant which means for time $$\tau $$ there is no
process of radioactivity which does not makes sense. (B) and (C) shows intermediate increase in the number of radioactive atom which is IMPOSSIBLE as $$N$$ will only decrease exponentially.