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Question: Radioactive carbon-14, in a wood sample, decays with a half-life of 5700 years. The fraction of the ...

Radioactive carbon-14, in a wood sample, decays with a half-life of 5700 years. The fraction of the radioactive carbon-14, that remains after a decay period of 17,10017,100 year is?

Explanation

Solution

Recall the relationship between the initial amount of radioactive substance and the final amount after a certain time t. In other words, we know that this is an exponential relation. Use this relation to obtain the final amount in terms of the half-life period by using the fact that the quantity remaining at the half-life is half the initial quantity of the radioactive substance. Substitute the given values and solve this arithmetically to arrive at the appropriate result.

Formula Used: Exponential radioactive decay: N=N0(12)tt1/2N = N_0\left(\dfrac{1}{2}\right)^{\dfrac{t}{t_{1/2}}}

Complete step-by-step solution:
We know that radioactive decay is an exponential decay, and is given as:
N=N0eλtN = N_0e^{-\lambda t}, where N0N_0 is the initial quantity of the radioactive substance, N is the remaining quantity after time t, and λ\lambda is the decay constant. A negative sign indicates that there is a decrease in the material remaining with time.
Now, the half-life of a radioactively decaying substance is defined as the time required for the substance to reduce to half its initial quantity. Therefore, if t1/2t_{1/2} is the half life of a substance at which N=N02N = \dfrac{N_0}{2}, the equation becomes:
N02=N0eλt1/2eλt1/2=12\dfrac{N_0}{2} = N_0e^{-\lambda t_{1/2}} \Rightarrow e^{-\lambda t_{1/2}} = \dfrac{1}{2}
Now, rewriting the first equation by multiplying and dividing the power of the exponential by λt1/2-\lambda t_{1/2}:
N=N0eλt.λt1/2λt1/2=N0e(λt1/2).λtλt1/2N = N_0e^{-\lambda t.\dfrac{-\lambda t_{1/2}}{-\lambda t_{1/2}}} = N_0e^{(-\lambda t_{1/2}).\dfrac{-\lambda t}{-\lambda t_{1/2}}}
Now, substituting eλt1/2=12 e^{-\lambda t_{1/2}} = \dfrac{1}{2} we get:
N=N0(12)λtλt1/2N=N0(12)tt1/2N= N_0\left(\dfrac{1}{2}\right)^{\dfrac{-\lambda t}{-\lambda t_{1/2}}} \Rightarrow N = N_0\left(\dfrac{1}{2}\right)^{\dfrac{t}{t_{1/2}}}
Now, we are given that for the radioactive carbon-14, t1/2=5700  yrst_{1/2} = 5700\;yrs and t=17,100  yrst = 17,100\;yrs.
Substituting this in the expression that we derived we get:
N=N0(12)171005700=N0(12)3=N023N = N_0\left(\dfrac{1}{2}\right)^{\dfrac{17100}{5700}} = N_0 \left(\dfrac{1}{2}\right)^{3} = \dfrac{N_0}{2^3}
N=18×N0\Rightarrow N = \dfrac{1}{8}\times N_0.
Therefore, there is one-eighth of the initial quantity left after a period of 17,100 years.

Note: Remember that there is an alternate form of expressing the exponential radioactive decay:
N=N0etτN=N_0e^{\dfrac{-t}{\tau}}, where τ\tau is the mean lifetime of the decaying quantity.
Also, the decay constant λ\lambda can be expressed in terms of half-life by taking N=N02N = \dfrac{N_0}{2} at t=t1/2t=t_{1/2}:
N02=N0eλt1/2eλt1/2=12λt1/2=ln(12)=ln  1ln  2=00.693=0.693\dfrac{N_0}{2} = N_0 e^{-\lambda t_{1/2}} \Rightarrow e^{-\lambda t_{1/2}} = \dfrac{1}{2} \Rightarrow -\lambda t_{1/2} = ln\left(\dfrac{1}{2}\right) = ln\; 1 – ln\; 2 = 0 -0.693 = -0.693
λ=0.693t1/2\Rightarrow \lambda = \dfrac{0.693}{t_{1/2}}