Problem 44
Question
Iodine-131 \(\left(t_{1 / 2}=8.04 \text { days }\right),\) a \(\beta\) emitter, is used to treat thyroid cancer. (a) Write an equation for the decomposition of \(^{131}\) I. (b) If you ingest a sample of NaI containing \(^{131}\) I, how much time is required for the activity to decrease to \(35.0 \%\) of its original value?
Step-by-Step Solution
Verified Answer
(a) Decay equation:
^{131}_{53}I \rightarrow ^{131}_{54}Xe + \beta^- + \overline{\nu}_e
. (b) Time for 35% activity:
13.9
days.
1Step 1: Write the Nuclear Decay Equation
Iodine-131 ( ^{131}I ) undergoes beta decay to form Xenon-131 ( ^{131}Xe ). During beta decay, a neutron in the iodine nucleus is transformed into a proton, emitting a beta particle ( \beta^- ) and an antineutrino ( \overline{u}_e ). The nuclear equation for this decay is:\[ ^{131}_{53}I \rightarrow ^{131}_{54}Xe + \beta^- + \overline{u}_e\]
2Step 2: Understand the Half-Life Formula
The half-life ( t_{1/2} ) of a radioactive isotope is the time it takes for half of the isotope to decay. For iodine-131, t_{1/2} = 8.04 days. The general formula to calculate the remaining activity after a certain time is:\[ A = A_0 \left(\frac{1}{2}\right)^{\frac{t}{t_{1/2}}}\]where A is the remaining activity, A_0 is the initial activity, t is the time elapsed, and t_{1/2} is the half-life.
3Step 3: Calculate the Time for 35% Activity
Since we want the activity to be 35.0\% of the initial activity (A/A_0 = 0.35) , substitute this into the formula and solve for t :\[ 0.35 = \left(\frac{1}{2}\right)^{\frac{t}{t_{1/2}}}\]Taking the natural logarithm on both sides, we get:\[ \ln(0.35) = \frac{t}{t_{1/2}} \cdot \ln\left(\frac{1}{2}\right)\]Rearranging for t , we find:\[ t = \frac{\ln(0.35)}{\ln(0.5)} \cdot t_{1/2}\]Substitute t_{1/2} = 8.04 days, we get:\[ t \approx \frac{\ln(0.35)}{\ln(0.5)} \cdot 8.04\]Calculate the numeric value to find t \approx 13.9 days.
Key Concepts
Iodine-131Beta DecayHalf-life CalculationRadioactive IsotopesNuclear Equation
Iodine-131
Iodine-131 is a radioactive isotope commonly used in medical treatments, especially for thyroid cancer. Its primary role is to destroy cancerous cells in the thyroid gland due to its radioactive nature. This element has an atomic number of 53, indicating the presence of 53 protons in its nucleus.
Iodine-131 is notable for its relatively short half-life of 8.04 days, which makes it suitable for medical applications since it doesn't remain radioactive in the body for an extended period. Its rapid decay helps minimize long-term radiation exposure to the patient.
Iodine-131 is notable for its relatively short half-life of 8.04 days, which makes it suitable for medical applications since it doesn't remain radioactive in the body for an extended period. Its rapid decay helps minimize long-term radiation exposure to the patient.
Beta Decay
Beta decay is a type of radioactive decay involving the transformation of a neutron into a proton within the nucleus. As a result, the atom emits a beta particle, which is high-energy and high-speed electron or positron.
When iodine-131 undergoes beta decay, it becomes xenon-131. This process increases the atomic number by one, transforming iodine with atomic number 53 into xenon with atomic number 54. Alongside the beta particle (denoted as \(\beta^-\)), a neutral subatomic particle called an antineutrino (\(\overline{u}_e\)) is also emitted. This decay helps us understand how iodine-131 turns into xenon-131.
When iodine-131 undergoes beta decay, it becomes xenon-131. This process increases the atomic number by one, transforming iodine with atomic number 53 into xenon with atomic number 54. Alongside the beta particle (denoted as \(\beta^-\)), a neutral subatomic particle called an antineutrino (\(\overline{u}_e\)) is also emitted. This decay helps us understand how iodine-131 turns into xenon-131.
Half-life Calculation
The half-life of a radioactive isotope is crucial in determining how long a substance remains active. For iodine-131, its half-life is 8.04 days, which means the amount of iodine-131 present will reduce by half every 8.04 days.
The formula for calculating how much of the isotope remains after a given time is:
The formula for calculating how much of the isotope remains after a given time is:
- \( A = A_0 \left(\frac{1}{2}\right)^{\frac{t}{t_{1/2}}} \)
- \(A\) is the remaining activity.
- \(A_0\) is the initial activity.
- \(t\) is time elapsed.
- \(t_{1/2}\) is the half-life.
Radioactive Isotopes
Radioactive isotopes are atoms with an unstable nucleus that release radiation in the form of particles or electromagnetic waves until they transform into a more stable form.
These isotopes are essential in various fields, from medicine to archaeology. In medical treatments, like the use of iodine-131, they offer a focused way to target and destroy unhealthy cells. This is because they emit radiation that the body can absorb, directing energy at specific tissues to provide therapeutic effects. Each isotope, like iodine-131, has unique properties making it suitable for different applications depending on its half-life and type of decay.
These isotopes are essential in various fields, from medicine to archaeology. In medical treatments, like the use of iodine-131, they offer a focused way to target and destroy unhealthy cells. This is because they emit radiation that the body can absorb, directing energy at specific tissues to provide therapeutic effects. Each isotope, like iodine-131, has unique properties making it suitable for different applications depending on its half-life and type of decay.
Nuclear Equation
A nuclear equation mathematically represents a radioactive decay process. It shows the transformation of the original isotope and the products formed as a result of the decay.
For iodine-131 undergoing beta decay, the nuclear equation is:
For iodine-131 undergoing beta decay, the nuclear equation is:
- \[ ^{131}_{53}I \rightarrow ^{131}_{54}Xe + \beta^- + \overline{u}_e \]
- The starting nucleus of iodine-131 \((^{131}_{53}I)\) decays.
- Xenon-131 \((^{131}_{54}Xe)\) is formed as the product nucleus.
- A beta particle \((\beta^-)\) and an antineutrino \((\overline{u}_e)\) are emitted as by-products.
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