(i) Half life period: It is the time during which the number of atoms of a radioactive material reduces to half of the original number.
Let N0 = number of atoms at t = 0 (at the start of the observation)
N = number of atoms after time t
So, N = N0e-λt ...........(1)
where λ is constant called disintegration constant
Let T = half life period
So, when t = T, N = -N0/2.
Substituting in Eq, (1), we have
\(\frac{N_0}{2}\) = N0e-λt
eλt = 2
λt = loge2 = 2.303 log102
= 0.693
or T = \(\frac{0.693}{\lambda}\)
(ii) Average life: The atoms of a radioactive substance are constantly disintegrating and thus the life of every atom is different.
So average life of a radioactive substance is the ratio of sum of lives of all the atoms to the total number of atoms.
Average life = \(\frac{\text {Sum of lives of all the atoms}}{\text {Total numberof atoms}}\)
Suppose dN atoms disintegrate in a time dt, t seconds after the separation of the substance, when the actual number of atoms present is N.
Then \(\frac{dN}{dt}\) = -λN
dN = -λNdt = -λN0e-λt dt
where N0 is the number of atoms in the beginning of time. Each of these dN atoms disintegrate between the time t and t + dt i.e these atoms had a life of t seconds.
∴ Total life of dN atoms = t dN
Hence total life time of all the atoms

Hence average life τa of the atom is the reciprocal of the radioactive disintegration constant λ.
Relation between average life and half life
Since average life of a radioactive element is given by
τa = \(\frac{1}{\lambda}\) ............(i)
and half life of a radioactive element is given by
T = \(\frac{0.693}{\lambda}\)
Using Eq. (i), we get
T = 0.693 τa.