Hyper Physics
Transcript of Hyper Physics
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Radioactivity
Radioactivity refers to the particles which are
emitted from nuclei as a result of nuclear instability.
Because the nucleus experiences the intense conflict
between the two strongest forces in nature, it should
not be surprising that there are many nuclear
isotopes which are unstable and emit some kind of
radiation. The most common types of radiation are
called alpha,beta, and gamma radiation, but there
are several other varieties of radioactive decay.
Radioactive decay rates are normally stated in terms of theirhalf-lives, and the
half-life of a given nuclear species is related to its radiation risk. The different types
of radioactivity lead to different decay paths which transmute the nuclei into other
chemical elements. Examining the amounts of the decay products makes possibleradioactive dating.
Radiation from nuclear sources is distributed equally in all directions, obeying the
inverse square law.
Natural radioactive decay series. Radioactive items you can buy. Some history.
Illustration of alpha, beta and gamma radiation
Index
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Alpha Radioactivity
Composed of two protons and two neutrons, the
alpha particle is a nucleus of the element helium.
Because of its very large mass (more than 7000
times the mass of thebeta particle) and its
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charge, it has a very short range. It is not suitable
for radiation therapy since its range is less than a
tenth of a millimeter inside the body. Its main
radiation hazard comes when it is ingested into
the body; it has great destructive power within its
short range. In contact with fast-growing
membranes and living cells, it is positioned for
maximum damage.
Alpha particle emission is modeled as abarrier penetration process. The alpha
particle is the nucleus of the helium atom and is the nucleus ofhighest stability.
Alpha role in deuterium-tritium fusion Proton fusion Radioactivity
Index
Alpha
particle
concepts
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Alpha Barrier Penetration
The energy of emitted alpha particles
was a mystery to early investigators
because it was evident that they did not
have enough energy, according to
classical physics, to escape the nucleus.
Once an approximate size of the nucleus
was obtained by Rutherford scattering,one could calculate the height of the
Coulomb barrier at the radius of the
nucleus. It was evident that this energy
was several times higher than the
observed alpha particle energies. There
was also an incredible range of half lives
for the alpha particle which could not be
explained by anything in classical
physics.
Index
Alpha
Decay
Concepts
References
Blatt
Ch 15
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The resolution of this dilemma came
with the realization that there was a finite
probability that the alpha particle could
penetrate the wall by quantum
mechanical tunneling. Using tunneling,
Gamow was able to calculate a
dependence for the half-life as a
function of alpha particle energy whichwas in agreement with experimental
observations.
Modeling of tunneling in polonium
Tipler
Ch 40
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Alpha Binding Energy
The nuclearbinding energy of the alpha particle is extremely high, 28.3 MeV. It is
an exceptionally stable collection of nucleons, and those heavier nuclei which can
be viewed as collections of alpha particles (carbon-12, oxygen-16, etc.) are also
exceptionally stable. This contrasts with a binding energy of only 8 MeV forhelium-3, which forms an intermediate step in theproton-proton fusion cycle.
Nuclear units
Index
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Alpha, Beta, and Gamma
Historically, the products ofradioactivity were called alpha,beta, and gamma when
it was found that they could be analyzed into three distinct species by either a
magnetic field or an electric field.
Index
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Penetration of Matter
Though the most massive and most energetic ofradioactive emissions, the alpha
particle is the shortest in range because of its strong interaction with matter. The
electromagnetic gamma ray is extremely penetrating, even penetrating considerable
thicknesses of concrete. The electron ofbeta radioactivity strongly interacts with
matter and has a short range.Index
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