A) \[\lambda \]
B) \[\frac{1}{2}\,\,\lambda \]
C) \[\frac{1}{4\lambda }\]
D) \[\frac{e}{\lambda }\]
Correct Answer: C
Solution :
If N is the number of radioactive nuclei present at some instant, then \[N\,\,=\,\,{{N}_{0}}{{e}^{-\lambda t}}\] The constant \[{{N}_{0}}\] represents the number of radioactive nuclei at \[t=0\] \[\frac{{{N}_{1}}}{{{N}_{2}}}\,\,=\,\,\frac{{{e}^{-{{\lambda }_{1}}t}}}{{{e}^{-{{\lambda }_{2}}t}}}\,\,\,or\,\,\frac{{{N}_{1}}}{{{N}_{2}}}\,\,=\,\frac{{{e}^{-5\lambda t}}}{{{e}^{-\lambda t}}}\,\,=\,\,{{e}^{-4\lambda t}}\] \[but\,\,\frac{{{N}_{1}}}{{{N}_{2}}}\,=\,\,\frac{1}{e}\,\,(as\,\,provided)\] Therefore, \[\frac{1}{e}=\frac{1}{{{e}^{4\lambda t}}}\,\,\,or\,\,4\lambda t=1\] \[or\,\,\,t=\frac{1}{4\lambda }\]You need to login to perform this action.
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