\(T_{\frac 12}=\frac {ln\ 2}{λ}\)
\(T_{\frac12} ln\ 2=λ\)
\(T_{\frac12}=\frac 1λ\)
\((λ+T_{\frac 12})=\frac {ln\ 2}{2}\)
The relationship between the decay constant \(λ\) and the half-life \(T_{\frac{1}{2}}\) of a radioactive sample is determined by the exponential decay law. The formula linking these two quantities is:
\(T_{\frac{1}{2}} = \frac{\ln 2}{λ}\)
Here is the step-by-step derivation and explanation:
Half-life is defined as the time required for a quantity to reduce to half its initial amount. For a radioactive substance, this can be expressed using the decay law:
Exponential decay is given by the equation:
\(N(t) = N_0 \cdot e^{-λt}\)
where \(N(t)\) is the quantity remaining after time \(t\), \(N_0\) is the initial quantity, and \(λ\) is the decay constant.
To find \(T_{\frac{1}{2}}\), set \(N(T_{\frac{1}{2}}) = \frac{N_0}{2}\):
\(\frac{N_0}{2} = N_0 \cdot e^{-λT_{\frac{1}{2}}}\)
Simplify by dividing both sides by \(N_0\):
\(\frac{1}{2} = e^{-λT_{\frac{1}{2}}}\)
Take the natural logarithm on both sides to solve for \(T_{\frac{1}{2}}\):
\ln \left(\frac{1}{2}\right) = -\ln 2, as -\ln 2 = -λT_{\frac{1}{2}}
Finally, solve for \(T_{\frac{1}{2}}\) by dividing by T_{\frac{1}{2} = \frac{\ln 2}{λ}
The correct answer to the question is clearly \(T_{\frac{1}{2} = \frac{\ln 2}{λ}\), matching option 1.
The electric potential at the surface of an atomic nucleus \( (z = 50) \) of radius \( 9 \times 10^{-13} \) cm is \(\_\_\_\_\_\_\_ \)\(\times 10^{6} V\).
In a nuclear fission reaction of an isotope of mass \( M \), three similar daughter nuclei of the same mass are formed. The speed of a daughter nuclei in terms of mass defect \( \Delta M \) will be: