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    RADIOACTIVITY

    PENGENALAN ASTRONOMI

    DAN

    FIZIK MODEN

    GROUP ASSIGNMENT

    GROUPMEMBERS :

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    Radioactivity

    When an unstable nucleus releases energy and/or particles.

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    Radioactive Decay

    There are 4 basic types ofradioactive decay

    Alpha Ejected Helium

    Beta Ejected Electron Positron Ejected Anti-Beta

    particle

    Gamma Ejected Energy

    You may encounter protons andneutrons being emitted as well

    n

    p

    e

    e

    He

    1

    0

    11

    0

    0

    0

    1

    0

    1

    4

    2

    K

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    Alpha decay is a type of radioactive decay

    in which an atomic nucleus emits an alpha

    particle and thereby transforms (or

    'decays') into an atom with a mass number

    4 less and atomic number 2 less.

    For example:

    4238 234 + 2He2+

    92 90Th [1]

    238 234

    U Th + a

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    .

    An alpha particle is the same

    as a helium-4 nucleus,

    and both mass numberand

    atomic number are the same

    Alpha decay is by far the most common form of cluster

    decay where the parent atom ejects a defined daughter

    collection of nucleons , leaving another defined product behind

    (in nuclear fission , a number of different pairs of daughters

    of approximately equal size are formed).

    Alpha decay is the most likely

    cluster decay because of the

    combined extremely high binding

    energy and relatively small mass of the

    helium-4 product nucleus (the alphaparticle).

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    In nuclear physics, beta decay is a type of radioactive decay in which a beta particle (anelectron or a positronis emitted

    In the case of electron emission, it is referred to as beta minus (), while in the case of apositron emission as beta plus (+)

    In electron emission, an electron antineutrino is also emitted, while positron emission isaccompanied by an electron neutrino. Beta decay is mediated by the weak force.

    Emitted beta particles have a continuous kinetic energy spectrum, ranging from 0 to themaximal available energy (Q), which depends on the parent and daughter nuclear states thatparticipate in the decay. A typical Q is around 1 MeV, but it can range from a few keV to afew tens of MeV. Since the equivalence of energy of the rest mass of electron is 511 keV, themost energetic beta particles are ultrarelativistic, with speeds very close to the speed of light

    Sometimes electron capture decay is included as a type of beta decay (and is referred to as

    "inverse beta decay"), because the basic process, mediated by the weak force is the same.However, no beta particle is emitted, but only an electron neutrino. Instead of beta-plusemission, an inner atomic electron is captured by a proton in the nucleus. This type of decay istherefore analogus to positron emission (and also happens, as an alternative decay route, in allpositron-emitters). However, the route of electron capture is the only type of decay that isallowed in proton-rich nuclides that do nothave sufficient energy to emit a positron (andneutrino). These may still reach a lower energy state, by the equivalent process of electron-capture and neutrino-emission.

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    There are3 different modes of beta decay

    Electron

    emission

    Electron capture

    Position

    emission

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    Electron emitters are found

    throughout the periodic table, from

    the lightest elements (3H) to the

    heaviest (255Es).

    Electron

    emission

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    Electron capture

    Leads to a decrease of one in the charge on the nucleus.

    The energy given off in this reaction is carried by an x-ray

    photon, which is represented by the symbol hv, where h is

    Planck's constant and v is the frequency of the x-ray

    The product of this reaction can be predicted, once

    again, by assuming that mass and charge are

    conserved.

    The electron captured by the nucleus in this reactionis usually a 1s electron because electrons in this

    orbital are the closest to the nucleus.

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    Positron

    emission