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What are transuranium elements and how are they synthesized?

Short Answer

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Transuranium elements are synthetic chemical elements with atomic numbers greater than 92, which are not found naturally. They are synthesized through a series of neutron capture and beta decay processes. Neutron capture increases the mass of an atom without changing its atomic number, followed by beta decay which converts a neutron into a proton, creating a new element. This process can be repeated to create higher atomic number elements. To create heavier transuranium elements, particle accelerators are used to smash atomic nuclei together. However, synthesizing these elements is challenging due to their short half-lives and instability.

Step by step solution

01

Transuranium Elements Definition

Transuranium elements are chemical elements with atomic numbers greater than 92, uranium being the last naturally occurring element. These elements do not exist in nature and are synthetically produced.
02

Neutron Capture

The synthesis of transuranium elements starts with a process called neutron capture, in which an atom captures one or more neutrons. This addition of neutrons increases the mass of the atom but does not change the atomic number.
03

Beta Decay

The atom, after gaining neutrons through neutron capture, undergoes a process called beta decay. In beta decay, a neutron is converted into a proton by emitting an electron (also known as a beta particle). This process increases the atomic number of the atom by 1, effectively creating a new element.
04

Repetition of Process

To synthesize transuranium elements with higher atomic numbers, the neutron capture and beta decay processes are repeated multiple times. Each repetition increases the atomic number of the synthesized element and gets us closer to the desired transuranium element.
05

Particle Accelerator

To speed up the synthesis process and create heavier transuranium elements, scientists use particle accelerators. These machines accelerate atomic nuclei to extremely high speeds and smash them into target nuclei. The collision can result in the creation of new elements, including transuranium elements.
06

Challenges in Synthesis

The synthesis of transuranium elements can be challenging due to short half-lives and instability. Many of these elements decay very quickly, which makes their detection and characterization difficult. Researchers continue to investigate new ways to create and study these elements in hope of gaining a better understanding of their properties and potential applications.

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Most popular questions from this chapter

Much of the research on controlled fusion focuses on the problem of how to contain the reacting material. Magnetic fields appear to be the most promising mode of containment. Why is containment such a problem? Why must one resort to magnetic fields for containment?

A living plant contains approximately the same fraction of carbon-14 4 as in atmospheric carbon dioxide. Assuming that the observed rate of decay of carbon-14 4 from a living plant is 13.6 counts per minute per gram of carbon, how many counts per minute per gram of carbon will be measured from a \(15,000\) -year-old sample? Will radiocarbon dating work well for small samples of 10 \(\mathrm{mg}\) or less? (For \(^{14} \mathrm{C}, t_{1 / 2}=5730\) years.)

Rubidium- 87 decays by \(\beta\) -particle production to strontium- 87 with a half-life of \(4.7 \times 10^{10}\) years. What is the age of a rock sample that contains 109.7 \mug of \(^{87} \mathrm{Rb}\) and 3.1\(\mu \mathrm{g}\) of \(^{87} \mathrm{Sr} ?\) Assume that no \(^{87}\) Sr was present when the rock was formed. The atomic masses for \(^{87}\mathrm{Rb}\) and \(^{87} \mathrm{Sr}\) are 86.90919 \(\mathrm{u}\) and 86.90888 u, respectively.

In the bismuth-214 natural decay series, Bi-214 initially undergoes \(\beta\) decay, the resulting daughter emits an \(\alpha\) particle, and the succeeding daughters emit a \(\beta\) and a \(\beta\) particle in that order. Determine the product of each step in the Bi-214 decay series.

The rate constant for a certain radioactive nuclide is \(1.0 \times 10^{-3} \mathrm{h}^{-1} .\) What is the half-life of this nuclide?

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