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By the end of this section, you will be able to:
  • Describe and compare three types of nuclear radiation
  • Use nuclear symbols to describe changes that occur during nuclear reactions
  • Describe processes involved in the decay series of heavy elements

Early experiments revealed three types of nuclear “rays” or radiation: alpha ( α ) rays    , beta ( β ) rays    , and gamma ( γ ) rays    . These three types of radiation are differentiated by their ability to penetrate matter. Alpha radiation is barely able to pass through a thin sheet of paper. Beta radiation can penetrate aluminum to a depth of about 3 mm, and gamma radiation can penetrate lead to a depth of 2 or more centimeters ( [link] ).

The figure shows from left to right: paper, metal, concrete and lead. Three types of radiation enter this setup from the left. Alpha radiation does not pass through paper. Beta radiation passes through paper but not through metal. Gamma radiation passes through paper, metal and concrete, but not through lead.
A comparison of the penetration depths of alpha ( α ), beta ( β ), and gamma ( γ ) radiation through various materials.

The electrical properties of these three types of radiation are investigated by passing them through a uniform magnetic field, as shown in [link] . According to the magnetic force equation F = q v × B , positively charged particles are deflected upward, negatively charged particles are deflected downward, and particles with no charge pass through the magnetic field undeflected. Eventually, α rays were identified with helium nuclei ( 4 He ) , β rays with electrons and positrons (positively charged electrons or antielectrons    ), and γ rays with high-energy photons. We discuss alpha, beta, and gamma radiation in detail in the remainder of this section.

Figure shows a C-shaped material labeled lead. A small circle labeled radioactive source is shown in the hollow of the C-shape. Three rays radiate from this source towards the right. One curves upwards and is labeled alpha. One goes straight and is labeled gamma. The third curves downwards and is labeled beta minus. Magnetic field is shown as crosses. Two arrows originate from near the point where the rays emerge from the C-shape. The upwards pointing arrow is labeled F subscript alpha = q subscript alpha v B. The downwards pointing arrow is labeled F subscript beta = q subscript beta v B.
The effect of a magnetic field on alpha ( α ), beta ( β ), and gamma ( γ ) radiation. This figure is a schematic only. The relative paths of the particles depend on their masses and initial kinetic energies.

Alpha decay

Heavy unstable nuclei emit α radiation. In α -particle decay (or alpha decay    ), the nucleus loses two protons and two neutrons, so the atomic number decreases by two, whereas its mass number decreases by four. Before the decay, the nucleus is called the parent nucleus    . The nucleus or nuclei produced in the decay are referred to as the daughter nucleus    or daughter nuclei. We represent an α decay symbolically by

Z A X Z 2 A 4 X + 2 4 H e

where Z A X is the parent nucleus, Z 2 A 4 X is the daughter nucleus, and 2 4 H e is the α particle. In α decay, a nucleus of atomic number Z decays into a nucleus of atomic number Z 2 and atomic mass A 4 . Interestingly, the dream of the ancient alchemists to turn other metals into gold is scientifically feasible through the alpha-decay process. The efforts of the alchemists failed because they relied on chemical interactions rather than nuclear interactions.

Watch alpha particles escape from a polonium nucleus, causing radioactive alpha decay. See how random decay times relate to the half-life. To try a simulation of alpha decay, visit alpha particles

An example of alpha decay is uranium-238:

92 238 U 90 234 X + 2 4 H e .

The atomic number has dropped from 92 to 90. The chemical element with Z = 90 is thorium. Hence, Uranium-238 has decayed to Thorium-234 by the emission of an α particle, written

92 238 U 90 234 T h + 2 4 H e .

Subsequently, 90 234 T h decays by β emission with a half-life of 24 days. The energy released in this alpha decay takes the form of kinetic energies of the thorium and helium nuclei, although the kinetic energy of thorium is smaller than helium due to its heavier mass and smaller velocity.

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Source:  OpenStax, University physics volume 3. OpenStax CNX. Nov 04, 2016 Download for free at http://cnx.org/content/col12067/1.4
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