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Question: (a) Deduce the expression,\[N = {N_0}{e^{ - \lambda t}}\] for the law of radioactive decay. (b) ...

(a) Deduce the expression,N=N0eλtN = {N_0}{e^{ - \lambda t}} for the law of radioactive decay.
(b)
(i) Write symbolically the process expressing the β+\beta + decay of 1122Na{}_{11}^{22}Na. Also write the basic nuclear process underlying this decay.
(ii) Is the nucleus formed in the decay of the nucleus1122Na{}_{11}^{22}Na, an isotope or isobar?

Explanation

Solution

In a radioactive decay when a material undergoes either α\alpha or β\beta orγ\gamma decay the number of nuclei undergoing the decay per unit time is directly proportional to the total number of nuclei in the given sample materials.

Complete step by step answer:
(a)Let
The total number of atoms present originally in a sample at the time t=0 be No{N_o}
The total number of atoms left un-decayed in the sample at time tt beNN
The small number of atom that disintegrate in a small interval of time dtdt be dNdN
Now according to radioactive decay we know the rate of decay is proportional to amount of nuclei written as

\-dNdtN dNdt=λN(i)  \- \dfrac{{dN}}{{dt}} \propto N \\\ \Rightarrow - \dfrac{{dN}}{{dt}} = \lambda N - - (i) \\\

Where λ\lambda is the disintegration constant
Now integrate equation (i)

dNN=λdt logN=λt+C(ii)  \int {\dfrac{{dN}}{N}} = - \lambda \int {dt} \\\ \Rightarrow \log N = - \lambda t + C - - (ii) \\\

Where C is the integration constant total number of atoms present originally in a sample is No{N_o}
Now since at timet=0t = 0 total number of atoms present originally in a sample is No{N_o}
So can write equation (ii) as

logeN0=λ×0+C C=logeN0  {\log _e}{N_0} = - \lambda \times 0 + C \\\ \Rightarrow C = {\log _e}{N_0} \\\

Hence by substituting the value of C in equation (ii) we get

logeNlogeN0=λt logeNN0=λt  {\log _e}N - {\log _e}{N_0} = - \lambda t \\\ \Rightarrow {\log _e}\dfrac{N}{{{N_0}}} = - \lambda t \\\

Hence by taking inverse integration we get

NN0=eλt N=N0eλt  \dfrac{N}{{{N_0}}} = {e^{ - \lambda t}} \\\ \Rightarrow N = {N_0}{e^{ - \lambda t}} \\\

Hence, the radioactive decay N=N0eλtN = {N_0}{e^{ - \lambda t}}
(b)
(i) Now we know the basic nuclear process underlying the β+\beta + decay is pn+e++vp \to n + {e^ + } + v, so the reaction can be written as 1122Naβ++1022Ne+v{}_{11}^{22}Na \to {\beta ^ + } + {}_{10}^{22}Ne + v
(ii) The nucleus formed in the decay of the nucleus 1122Na{}_{11}^{22}Na is 1022Na{}_{10}^{22}Na and since nucleus formed has same mass number but different atomic number then it is isobar of 1122Na{}_{11}^{22}Na .

Note:
It is very important to note that isotopes and isobars are two completely different chemical terms.
Isotopes are atomic structures of the same elements with different mass numbers while on the other hand isobars are different chemical elements having the same atomic mass.