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Beta particle

physical science Maturity 11-13 Next article →

A beta particle, also known as a beta ray or beta radiation (symbol β), is a high-energy, high-speed particle emitted during radioactive decay. This process occurs when an unstable atomic nucleus undergoes beta decay to reach a more stable state. Beta particles can be either electrons or positrons. Electrons carry a negative charge, while positrons are their antimatter counterparts. These particles are a form of ionizing radiation. This means they have enough energy to knock electrons off the shells of other atoms.

Alfa beta gamma radiation
Alfa beta gamma radiation

The mechanism of beta decay depends on the balance of particles within the nucleus. In beta-minus (β−) decay, a nucleus has an excess of neutrons. A neutron transforms into a proton, an electron, and an electron antineutrino. This change is mediated by the weak interaction through a virtual W− boson. At the subatomic level, this boson turns a down quark into an up quark. This shift changes the neutron into a proton.

Beta-minus Decay
Beta-minus Decay

Conversely, beta-plus (β+) decay occurs in nuclei with too many protons. A proton converts into a neutron, a positron, and an electron neutrino. This specific type of decay only happens if the resulting daughter nucleus is in a lower-energy state than the parent nucleus.

Scientists categorize beta decay into these two distinct modes. Beta-minus decay is common in neutron-rich fission byproducts found in nuclear reactors. It also occurs during the decay of free neutrons. Beta-plus decay, or positron emission, is the source of positrons used in medical technology. A notable example is Phosphorus-32. This isotope is a beta emitter used widely in medicine. It has a short half-life of 14.29 days. When it decays into sulfur-32, it releases 1.709 MeV of energy. Most of this energy is carried by the electron, while the rest goes to the antineutrino.

Cs-137-decay
Cs-137-decay

The history of these particles involves several key scientific discoveries. Henri Becquerel first discovered unknown radiation while experimenting with uranium and photographic plates. Later, Ernest Rutherford conducted experiments to identify different types of radiation. In 1899, Rutherford published results showing that beta particles were 100 times more penetrating than alpha particles. In 1900, Becquerel measured the mass-to-charge ratio of these particles. He found the ratio was identical to that of the electron identified by J. J. Thomson. This led to the conclusion that beta particles are indeed electrons.

Beta particles have specific physical properties regarding energy and penetration. A beta particle with 0.5 MeV of energy can travel about one metre in the air. They cannot pass through clothing or thin metal sheets. However, a thin aluminium plate can stop most beta particles.

Beta radiation in a cloud chamber
Beta radiation in a cloud chamber

In water, some beta particles move faster than the speed of light in that medium. The speed of light in water is about 75% of its speed in a vacuum. When this happens, it generates a blue glow called Cherenkov radiation. This effect is visible in the water of swimming pool reactors.

TrigaReactorCore
TrigaReactorCore

These particles have significant practical applications in various fields. In medicine, beta particles are used in radiation therapy to treat bone and eye cancer. Positrons from beta-plus decay are essential for positron emission tomography, known as PET scans. In industry, beta radiation is used for quality control. Machines use it to monitor the thickness of products like paper. If the paper is too thick or too thin, the amount of radiation absorbed changes. This allows computers to adjust the rollers automatically. We also use tritium in betalights. As tritium decays, it emits beta particles that strike a phosphor to create light without external power.

Understanding beta radiation is vital for safety and science. Because they are charged particles, beta rays are more ionizing than gamma rays. However, they are less ionizing than alpha particles. This ionizing effect can cause spontaneous mutations in DNA within living tissue. For radiation protection, the absorbed dose is measured in grays (Gy). The biological effect on human tissue is measured in sieverts (Sv). For beta radiation, the conversion factor between these two units is 1. This is different from alpha particles, which have a weighting factor of 20 due to their higher ionizing power.

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🖼️ Images & Media (5)
File:Alfa beta gamma radiation.svg
Alfa beta gamma radiation.svg
File:Beta-minus Decay.svg
Beta-minus Decay.svg
File:Cs-137-decay.svg
Cs-137-decay.svg
File:TrigaReactorCore.jpeg
TrigaReactorCore.jpeg
File:Beta radiation in a cloud chamber.jpg
Beta radiation in a cloud chamber.jpg
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