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Physical chemistry     208


        radiation can be emitted  during radioactive decay;  α-particles,  β-particles  or  γ-
        radiation.
           The activity of a radioactive source is measured in bequerel (Bq) which is defined as
                                                                               10
        one nuclear disintegration per second. (The older unit of curie (Ci) is equal to 3.7×10
        disintegrations per second.) The unit of absorbed dose is the gray (Gy) which is defined
        as one joule per kilogram.

        α-decay
        An α-particle consists of two protons and two neutrons and is effectively the nucleus of a
        helium-4 atom,    . Therefore, the daughter isotope resulting from emission of an α-
        particle has atomic mass number, A, four units less than the parent isotope and atomic
        number, Z, two units less, and is an isotope of the element two places to the left in the
        periodic table. Decay by α-particle emission usually only occurs amongst the heaviest
        elements which have mass numbers greater than 200. An example of  α-decay is the
        transmutation of the uranium-238 isotope to an isotope of thorium:


        α-particles are the most massive and highly charged (+2 charge units) of the particles
        emitted during spontaneous radioactive decay and travel relatively slowly, approximately
        10% of the speed of light Since α-particles readily lose their energy and neutralize their
        charge in collisions with surrounding elements, their effects are short-range  (a  few
        millimeters) and, in general, α-emitters are not considered particularly hazardous since
        they cannot penetrate through skin. However, they may cause burns to the outer layers of
        skin and are dangerous if ingested.

        β-decay
        A  β-particle is an electron. It therefore has a small mass, and a charge of  −1 atomic
        charge unit. β-decay occurs when a neutron spontaneously converts into a proton, which
        remains in the nucleus, and an electron, which is emitted. Consequently, the parent and
        daughter nuclides have identical atomic mass number, A, but the daughter nuclide is an
        isotope of the element one atomic unit higher than the parent. An example is the β-decay
        of the carbon-14 radioisotope into the equivalent mass number isotope of nitrogen:


        The velocities of β-particles are greater than those of α-particles, because of the much
        lighter  mass,  and  it is possible for high-energy β-particles to penetrate skin and reach
        internal organs.

        γ-decay
        Gamma (γ) rays are very high energy photons often released during  α- and  β-decay
        processes when the daughter nuclide decays from an excited to a more stable state. Since
        γ-rays are photons of the electromagnetic spectrum they have no mass and no charge
        and travel at the speed of light. Photons of γ-rays are even more energetic than those of
        X-rays and are thus extremely penetrating and highly damaging. The subsequent β-decay
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