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A sample of radioactive nuclei has \(N_{0}\) nuclei at time \(t=0 .\) The half- life of the decay is \(T_{1 / 2}\). In terms of \(N_{0}\), how many decays occur in the time period between \(t=0\) and \(t=0.500 T_{1 / 2} ?\)

Short Answer

Expert verified
The decays that occur in the time period between \(t=0\) and \(t=0.500T_{1/2}\) is \(N_{0}(1 - 1/\sqrt{2})\).

Step by step solution

01

Understand the concept of half-life

The half-life of a radioactive substance is the time it takes for half of the substance to decay. This means that after one half-life has passed, half of the initial substance will have decayed. The remaining will be \(N_{0}/2\). After 0.5 half-life, more than half of the substance remains, specifically \(N_{0}/ \sqrt{2}\).
02

Calculate the number of nuclei remaining after 0.5 half-life

The number of nuclei \(N(t)\) of a substance that has not decayed after a time \(t\) is given by the equation \(N(t) = N_{0} \times 0.5^{(t/T_{1/2})}\) where \(N_{0}\) is the initial amount of the substance and \(T_{1/2}\) is the half-life time of the substance. By plugging in \(t = 0.500T_{1/2}\) into the equation we get \(N(t) = N_{0} \times 0.5^{(0.500T_{1/2}/T_{1/2})} = N_{0} / \sqrt{2}\).
03

Calculate the number of decays that occurred

The number of decays is calculated by subtracting the remaining amount of substance from the initial amount. Therefore, the number of decays \(D\) during the time period from \(t=0\) to \(t=0.500T_{1/2}\) is \(D = N_{0} - N(t) = N_{0} - N_{0}/\sqrt{2} = N_{0}(1 - 1/ \sqrt{2})\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Half-life
Half-life is a core concept in the study of radioactive decay. It represents the time taken for half of a given sample of radioactive nuclei to undergo decay. When a radioactive substance has a half-life of, say, 10 years, this means that in 10 years, only half of the original sample's radioactive nuclei will remain undecayed. The remaining half would have transformed into a different, non-radioactive form or a different element altogether.
When describing half-life:
  • The measurement is specific to each radioactive element or isotope.
  • Half-life is unaffected by environmental conditions like pressure or temperature.
  • It offers a straightforward method to estimate the time needed for a substance's decay.
Understanding half-life helps to explain how quickly or slowly a radioactive sample decreases over time, without needing to monitor every individual nucleus. This concept is essential in calculating how much of a substance remains or has decayed after a certain number of half-lives.
Radioactive Nuclei
In the context of radioactive decay, radioactive nuclei are the atoms that are unstable and undergo spontaneous transformations. These transformations often involve the release of energy in the form of radiation. Each radioactive nucleus is unstable because it possesses an excess of energy or an imbalance in the number of protons and neutrons within its core.
Let's explore these further:
  • Radioactive nuclei are the fundamental sources of radiation emissions, which can be alpha particles, beta particles, or gamma rays.
  • Over time, these nuclei transform into more stable configurations, sometimes changing elementally in the process.
  • The instability and decay of radioactive nuclei form the basis of nuclear energy production and diagnostic medicine applications.
A key point about radioactive nuclei is that although individual transformations are unpredictable, overall predictions can be made about the behavior of large numbers of nuclei—leading to concepts like half-life and decay constants. Recognizing these properties aids in practical applications, such as carbon dating in paleontology or dosimetry in radiation therapy.
Decay Calculation
The calculation of radioactive decay involves determining the amount of an initial sample that remains, as well as the quantity that has decayed over a specific time. This is done using mathematical equations that rely on the understanding of exponential decay behavior.
To calculate decay:
  • We use the equation: \[ N(t) = N_{0} \times 0.5^{(t/T_{1/2})} \]This equation provides the number of undecayed nuclei remaining, where \(N(t)\) is the quantity left after time \(t\), \(N_{0}\) is the original quantity, and \(T_{1/2}\) is the half-life.
  • If asked for how many have decayed, subtract \(N(t)\) from \(N_{0}\): \[ D = N_{0} - N(t) \]and specifically for a time equal to half of a half-life, the equation helps to evaluate quickly how many nuclei haven't decayed.
Using these decay equations, one can calculate decay over any time frame, given the half-life value. Such calculations are crucial in fields like nuclear physics and health physics, where understanding decay rates ensures safety and efficacy in using radioactive materials.

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Most popular questions from this chapter

Energy from Nuclear Fusion. Calculate the energy released in the fusion reaction $$ { }_{2}^{3} \mathrm{He}+{ }_{1}^{2} \mathrm{H} \rightarrow{ }_{2}^{4} \mathrm{He}+{ }_{1}^{1} \mathrm{H} $$

Radioactive Tracers. Radioactive isotopes are often introduced into the body through the bloodstream. Their spread through the body can then be monitored by detecting the appearance of radiation in different organs. One such tracer is \({ }^{131} \mathrm{I}\), a \(\beta^{-}\) emitter with a half-life of \(8.0 \mathrm{~d}\). Suppose a scientist introduces a sample with an activity of \(325 \mathrm{~Bq}\) and watches it spread to the organs. (a) Assuming that all of the sample went to the thyroid gland, what will be the decay rate in that gland 24 d (about \(3 \frac{1}{2}\) weeks) later? (b) If the decay rate in the thyroid 24 d later is measured to be 17.0 Bq, what percentage of the tracer went to that gland? (c) What isotope remains after the I-131 decays?

If a \(6.13 \mathrm{~g}\) sample of an isotope having a mass number of 124 decays at a rate of \(0.350 \mathrm{Ci}\), what is its half-life?

The carbon isotope \({ }_{6}^{11} \mathrm{C}\) undergoes \(\beta^{+}\) (positron) decay. The atomic mass of \({ }_{6}^{11} \mathrm{C}\) is \(11.011433 \mathrm{u}\). (a) How many protons and how many neutrons are in the daughter nucleus produced by this decay? (b) How much energy, in \(\mathrm{MeV},\) is released in the decay of one \({ }_{6}^{11} \mathrm{C}\) nucleus?

Comparison of Energy Released per Gram of Fuel. (a) When gasoline is burned, it releases \(1.3 \times 10^{8} \mathrm{~J}\) of energy per gallon \((3.788 \mathrm{~L}) .\) Given that the density of gasoline is \(737 \mathrm{~kg} / \mathrm{m}^{3},\) express the quantity of energy released in \(\mathrm{J} / \mathrm{g}\) of fuel. (b) During fission, when a neutron is absorbed by a \({ }^{235} \mathrm{U}\) nucleus, about \(200 \mathrm{MeV}\) of energy is released for each nucleus that undergoes fission. Express this quantity in \(\mathrm{J} / \mathrm{g}\) of fuel. \((\mathrm{c})\) In the proton-proton chain that takes place in stars like our sun, the overall fusion reaction can be summarized as six protons fusing to form one \({ }^{4}\) He nucleus with two leftover protons and the liberation of \(26.7 \mathrm{MeV}\) of energy. The fuel is the six protons. Express the energy produced here in units of \(\mathrm{J} / \mathrm{g}\) of fuel. Notice the huge difference between the two forms of nuclear energy, on the one hand, and the chemical energy from gasoline, on the other. (d) Our sun produces energy at a measured rate of \(3.86 \times 10^{26} \mathrm{~W}\). If its mass of \(1.99 \times 10^{30} \mathrm{~kg}\) were all gasoline, how long could it last before consuming all its fuel? (Historical note: Before the discovery of nuclear fusion and the vast amounts of energy it releases, scientists were confused. They knew that the earth was at least many millions of years old, but could not explain how the sun could survive that long if its energy came from chemical burning.)

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