A wooden artifact from an Indian temple nas a ' of 42 counts per minute as compared with an activity of 58.2 counts per minute for a standard zero age. From the half-life of \({ }^{14} \mathrm{C}\) decay, 5715 years, calculate the age of the artifact.

Short Answer

Expert verified
The age of the wooden artifact from the Indian temple is approximately 1960.95 years.

Step by step solution

01

Identify the given information

We are given the following information: - Activity of the artifact: 42 counts per minute - Activity of a standard zero age: 58.2 counts per minute - Half-life of \({ }^{14} \mathrm{C}\) decay: 5715 years
02

Understand the radioactive decay formula

The formula for radioactive decay is given by: \[ N_t = N_0 e^{-\lambda t} \] where - \( N_t \) is the remaining number of radioactive atoms at time \(t\), - \( N_0 \) is the initial number of radioactive atoms, - \(\lambda\) is the decay constant, and - \(t\) is the time.
03

Calculate the decay constant

We can find the decay constant (\(\lambda\)) using the half-life formula: \[ T_{1/2} = \frac{\ln(2)}{\lambda} \] Where \(T_{1/2}\) is the half-life. Now, let's calculate the decay constant: \begin{align*} \lambda &= \frac{\ln(2)}{T_{1/2}} \\ &= \frac{\ln(2)}{5715} \\ &\approx 1.21 \times 10^{-4} \,\mathrm{year}^{-1} \end{align*}
04

Find the age of the artifact

Now, let's plug in the given information into the radioactive decay formula: \begin{align*} \frac{N_t}{N_0} &= e^{-\lambda t} \\ \end{align*} Where \( N_t \) is the remaining activity, which is 42 counts per minute, and \( N_0 \) is the initial activity, which is 58.2 counts per minute. \begin{align*} \frac{42}{58.2} &= e^{- (1.21 \times 10^{-4})t} \\ 0.721 &= e^{- (1.21 \times 10^{-4})t} \end{align*} Taking the natural logarithm of both sides, we get: \[ \ln(0.721) = - (1.21 \times 10^{-4})t \] Now, let's solve for \(t\): \begin{align*} t &= \frac{\ln(0.721)}{-(1.21 \times 10^{-4})} \\ &\approx 1960.95 \, \mathrm{years} \end{align*} The age of the artifact is approximately 1960.95 years.

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