Derivation of the Law of Radioactive Decay:
The law of radioactive decay states that the rate of disintegration of radioactive nuclei in a sample is directly proportional to the number of undecayed nuclei present at that instant.
Let \(N\) be the number of undecayed nuclei in a sample at time \(t\), and \(dN\) be the number of nuclei that decay in a small time interval \(dt\). The rate of decay is \( -dN/dt \).
According to the law:
\[ -\frac{dN}{dt} \propto N \]
\[ -\frac{dN}{dt} = \lambda N \]
where \(\lambda\) is the decay constant, a positive constant characteristic of the radioactive substance.
Rearranging the equation to separate the variables:
\[ \frac{dN}{N} = -\lambda dt \]
To find the number of nuclei remaining after a time \(t\), we integrate this equation. Let \(N_0\) be the initial number of nuclei at time \(t=0\), and \(N\) be the number of nuclei at time \(t\).
\[ \int_{N_0}^{N} \frac{dN}{N} = \int_{0}^{t} -\lambda dt \]
\[ [\ln N]_{N_0}^{N} = -\lambda [t]_0^t \]
\[ \ln N - \ln N_0 = -\lambda(t - 0) \]
\[ \ln\left(\frac{N}{N_0}\right) = -\lambda t \]
Taking the exponential of both sides:
\[ \frac{N}{N_0} = e^{-\lambda t} \]
\[ N(t) = N_0 e^{-\lambda t} \]
This is the mathematical expression for the law of radioactive decay, which shows that the number of undecayed nuclei decreases exponentially with time.
Definition of Becquerel (Bq):
One becquerel is the unit of activity of a radioactive sample in the SI system. It is defined as one disintegration (or decay) per second.
\[ 1 \, \text{Bq} = 1 \, \text{decay/second} \]