In a radio active material the activity at time t1 is R1 and at a later time t2, it is R2. If the decay constant of the material is λ, then
R1=R2 e−λt1−t2
R1=R2 eλt1−t2
R1=R2 t2/t1
R1=R2
R1=R0e−λt1 and R2=R0e−λt2∴ R1R2 = e−λt1 − t2