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One type of commercial smoke detector contains a minute amount of radioactive americium- \(241\left({ }^{241} \mathrm{Am}\right)\), which decays by \(\alpha\) -particle production. The \(\alpha\) particles ionize molecules in the air, allowing it to conduct an electric current. When smoke particles enter, the conductivity of the air is changed and the alarm buzzes. a. Write the equation for the decay of \({ }_{95}^{241} \mathrm{Am}\) by \(\alpha\) -particle production. b. The complete decay of \({ }^{241}\) Am involves successively \(\alpha, \alpha, \beta\), \(\alpha, \alpha, \beta, \alpha, \alpha, \alpha, \beta, \alpha\), and \(\beta\) production. What is the final stable nucleus produced in this decay series? c. Identify the 11 intermediate nuclides.

Short Answer

Expert verified
a. The equation for the decay of Am-241 by α-particle production is: \[^{241}_{95}\text{Am} \rightarrow ^{237}_{93}\text{Np} + ^{4}_{2}\text{He}\] b. The final stable nucleus produced in this decay series is Bismuth-209 (Bi-209). c. The 11 intermediate nuclides in the decay series are: Np-237, Pa-233, U-233, Th-229, Ra-225, Ac-225, Fr-221, At-217, Bi-213, Po-213, and Pb-209.

Step by step solution

01

a. Writing the equation for α-decay of Am-241

For an α-decay, the parent nucleus loses an alpha particle (a helium nucleus) with mass number 4 and atomic number 2. So, the mass number decreases by 4 and the atomic number decreases by 2. Let's write the decay equation for Am-241: \[^{241}_{95}\text{Am} \rightarrow ^{237}_{93}\text{X} + ^{4}_{2}\text{He}\] Here, X represents the element with atomic number 93, which is Neptunium (Np). So, the decay equation becomes: \[^{241}_{95}\text{Am} \rightarrow ^{237}_{93}\text{Np} + ^{4}_{2}\text{He}\]
02

b. Finding the final stable nucleus in the decay series

The decay series is given as: α, α, β, α, α, β, α, α, α, β, α, β. We will find the final stable nucleus by successively applying each decay process to Am-241. For each α-decay, the mass number decreases by 4 and the atomic number decreases by 2. For each β-decay, the mass number remains the same, but the atomic number increases by 1. Starting with Am-241, let's apply the given decay series: \[^{241}_{95}\text{Am} \xrightarrow[\alpha]{} ^{237}_{93}\text{Np} \xrightarrow[\alpha]{} ^{233}_{91}\text{Pa} \xrightarrow[\beta]{} ^{233}_{92}\text{U} \xrightarrow[\alpha]{} ^{229}_{90}\text{Th}\] \[^{229}_{90}\text{Th} \xrightarrow[\alpha]{} ^{225}_{88}\text{Ra} \xrightarrow[\beta]{} ^{225}_{89}\text{Ac} \xrightarrow[\alpha]{} ^{221}_{87}\text{Fr}\] \[^{221}_{87}\text{Fr} \xrightarrow[\alpha]{} ^{217}_{85}\text{At} \xrightarrow[\alpha]{} ^{213}_{83}\text{Bi} \xrightarrow[\beta]{} ^{213}_{84}\text{Po}\] \[^{213}_{84}\text{Po} \xrightarrow[\alpha]{} ^{209}_{82}\text{Pb} \xrightarrow[\beta]{} ^{209}_{83}\text{Bi}\] The final stable nucleus in the decay series is Bismuth-209 (Bi-209).
03

c. Identifying the 11 intermediate nuclides

In the above step, we already identified the intermediate nuclides while applying each decay process. The 11 intermediate nuclides in the decay series are: 1. Neptunium-237 (Np-237) 2. Protactinium-233 (Pa-233) 3. Uranium-233 (U-233) 4. Thorium-229 (Th-229) 5. Radium-225 (Ra-225) 6. Actinium-225 (Ac-225) 7. Francium-221 (Fr-221) 8. Astatine-217 (At-217) 9. Bismuth-213 (Bi-213) 10. Polonium-213 (Po-213) 11. Lead-209 (Pb-209)

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Key Concepts

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

Alpha Decay
Alpha decay is a common form of radioactive decay where an unstable atomic nucleus releases an alpha particle. An alpha particle consists of two protons and two neutrons, essentially a helium nucleus. When an atom undergoes alpha decay, it loses an alpha particle, causing its mass number to decrease by 4 and its atomic number to decrease by 2. This process transforms the original element into a different element.

For example, in the decay of Americium-241 (Am-241):
  • The atomic number changes from 95 (Americium) to 93 (Neptunium).
  • The mass number changes from 241 to 237.
This process releases an alpha particle, represented as \[^{4}_{2}\text{He}\]. The equation is:
\[^{241}_{95}\text{Am} \rightarrow ^{237}_{93}\text{Np} + ^{4}_{2}\text{He}\]

Alpha decay is crucial in reducing the radioactivity of heavy elements, turning them into more stable forms over time.
Beta Decay
Beta decay is another type of radioactive decay where a beta particle is emitted from an atomic nucleus. A beta particle can either be an electron or a positron. In beta minus decay, a neutron is transformed into a proton, emitting an electron and an antineutrino. This increases the atomic number by 1, but the mass number remains unchanged.

During the decay series of \(^{241}\text{Am}\), beta decay steps were essential to stabilize the nucleus:
  • The atomic number increases by 1, such as from \(^{233}_{91}\text{Pa}\) to \(^{233}_{92}\text{U}\).
The equation looks like:
\[\text{n} \rightarrow \text{p} + \text{e}^{-} + \overline{u}\]

In contrast, beta plus decay occurs when a proton is converted into a neutron, though it's less common in this context. Understanding beta decay helps in comprehending isotopic changes and the stabilization of elements.
Radioisotopes
Radioisotopes are isotopes of an element with an unstable nucleus. These isotopes undergo radioactive decay, releasing particles or electromagnetic waves. The decay process transforms the isotope into a more stable form.

Americium-241, used in smoke detectors, is an example of a radioisotope. It undergoes alpha decay, releasing energy that is used to ionize the air in detectors. This ionization process helps detect smoke by altering the electrical conductivity of the air.

Radioisotopes have various applications beyond smoke detection, including medical imaging, cancer treatment, and carbon dating. Their ability to emit radiation makes them valuable in scientific research and industry, although handling requires strict safety measures due to the potential health risks.
Smoke Detectors
Smoke detectors are essential safety devices in homes and buildings, often utilizing radioisotopes like Americium-241. This radioisotope helps the detector sense smoke through a simple yet effective process.

Here's how it works:
  • The decay of \(^{241}\text{Am}\) produces alpha particles.
  • The alpha particles ionize the air between two electrodes, allowing a small electric current to flow.
  • When smoke enters the detector, it disrupts the ionized air, reducing conductivity and thus altering the current.
This disruption triggers the alarm, alerting occupants of potential fire. Smoke detectors are vital for early fire detection and safety, demonstrating a practical application of nuclear physics in everyday life.

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Most popular questions from this chapter

The curie (Ci) is a commonly used unit for measuring nuclear radioactivity: 1 curie of radiation is equal to \(3.7 \times 10^{10}\) decay events per second (the number of decay events from \(1 \mathrm{~g}\) radium in \(1 \mathrm{~s}\) ). a. What mass of \(\mathrm{Na}_{2}{ }^{38} \mathrm{SO}_{4}\) has an activity of \(10.0 \mathrm{mCi}\) ? Sulfur38 has an atomic mass of \(38.0\) and a half-life of \(2.87 \mathrm{~h}\). b. How long does it take for \(99.99 \%\) of a sample of sulfur- 38 to decay?

The most stable nucleus in terms of binding energy per nucleon is \({ }^{56} \mathrm{Fe}\). If the atomic mass of \({ }^{56} \mathrm{Fe}\) is \(55.9349 \mathrm{amu}\), calculate the binding energy per nucleon for \({ }^{56} \mathrm{Fe}\).

The most significant source of natural radiation is radon- \(222 .\) \({ }^{222} \mathrm{Rn}\), a decay product of \({ }^{238} \mathrm{U}\), is continuously generated in the earth's crust, allowing gaseous Rn to seep into the basements of buildings. Because \({ }^{222} \mathrm{Rn}\) is an \(\alpha\) -particle producer with a relatively short half-life of \(3.82\) days, it can cause biological damage when inhaled. a. How many \(\alpha\) particles and \(\beta\) particles are produced when \({ }^{238} \mathrm{U}\) decays to \({ }^{222} \mathrm{Rn}\) ? What nuclei are produced when \({ }^{222} \mathrm{Rn}\) decays? b. Radon is a noble gas so one would expect it to pass through the body quickly. Why is there a concern over inhaling \({ }^{222} \mathrm{Rn}\) ? c. Another problem associated with \({ }^{222} \mathrm{Rn}\) is that the decay of \({ }^{222} \mathrm{Rn}\) produces a more potent \(\alpha\) -particle producer \(\left(t_{1 / 2}=3.11\right.\) min) that is a solid. What is the identity of the solid? Give the balanced equation of this species decaying by \(\alpha\) -particle production. Why is the solid a more potent \(\alpha\) -particle producer? d. The U.S. Environmental Protection Agency (EPA) recommends that \({ }^{222} \mathrm{Rn}\) levels not exceed \(4 \mathrm{pCi}\) per liter of air \((1 \mathrm{Ci}=\) 1 curie \(=3.7 \times 10^{10}\) decay events per second; \(1 \mathrm{pCi}=1 \times\) \(10^{-12} \mathrm{Ci}\). Convert \(4.0 \mathrm{pCi}\) per liter of air into concentrations units of \(^{222} \mathrm{Rn}\) atoms per liter of air and moles of \({ }^{222} \mathrm{Rn}\) per liter of air.

When nuclei undergo nuclear transformations, \(\gamma\) rays of characteristic frequencies are observed. How does this fact, along with other information in the chapter on nuclear stability, suggest that a quantum mechanical model may apply to the nucleus?

A recently reported synthesis of the transuranium element bohrium (Bh) involved the bombardment of berkelium-249 with neon-22 to produce bohrium-267. Write a nuclear reaction for this synthesis. The half-life of bohrium-267 is \(15.0\) seconds. If 199 atoms of bohrium- 267 could be synthesized, how much time would elapse before only 11 atoms of bohrium- 267 remain? What is the expected electron configuration of elemental bohrium?

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