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A radioactive nucleus can decay by two differnt modes. The half life for the first mode is T1 and that for the second mode is T2 . The effective half life T of the nucleus would be

(1) T = T1 + T2

(2) \(\frac{1}{T}=\frac{1}{T_1}+\frac{1}{T_2}\)

(3) \(ln(\frac{1}{T})=ln(\frac{1}{T_1})+ln(\frac{1}{T_2})\)

(4) \(\frac{1}{T}=\frac{1}{(T_1+T_2)}\)

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 (2) \(\frac{1}{T}=\frac{1}{T_1}+\frac{1}{T_2}\)

Denoting by λ1 and λ2 the decay constants of the two modes by which nucleus can decay we have

The probability that an active nucleus decay by first mode in a small time dt is λ1 dt and that for the second mode is λ2 dt. Then the probability that it decays either by first process or second process is (λ1dt + λ2 dt). Now we can say that λ is the effective decay constant. Hence the probability that the nucleus decay by effective value of λ in small time dt is λdt. 

Hence we must have

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