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Absorption alpha particle

Polonium-210 is very dangerous to handle in even milligram or microgram amounts, and special equipment and strict control is necessary. Damage arises from the complete absorption of the energy of the alpha particle into tissue. [Pg.149]

Boron [7440-42-8] B, is unique in that it is the only nonmetal in Group 13 (IIIA) of the Periodic Table. Boron, at wt 10.81, at no. 5, has more similarity to carbon and siUcon than to the other elements in Group 13. There are two stable boron isotopes, B and B, which are naturally present at 19.10—20.31% and 79.69—80.90%, respectively. The range of the isotopic abundancies reflects a variabiUty in naturally occurring deposits such as high B ore from Turkey and low °B ore from California. Other boron isotopes, B, B, and B, have half-Hves of less than a second. The B isotope has a very high cross-section for absorption of thermal neutrons, 3.835 x 10 (3835 bams). This neutron absorption produces alpha particles. [Pg.183]

First item in a series (for example, the first carbon linked to a carboxyl group). 2. Abbreviation for alpha particle. 3. Symbol for angle of optical rotation. 4. Symbol for degree of dissociation. 5. Symbol for electric polarizability of a molecule. 6. Often with a subscript number (i) the coefficient of [A] in the numerator of the generalized rate expression. 7. Symbol for is proportional to. 8. Symbol for Napierian absorption coefficient. 9. In brackets, symbol for specific optical rotation. [Pg.49]

The absorption of thermal neutrons in B produces alpha particles according to the following interaction ... [Pg.51]

The role of subexcitation electrons is most important when the irradiated medium contains small amounts of impurity molecules the excitation energy ha) 0j (or the ionization potential I ) of which is below h(o0l. Such additive molecules can be excited or ionized by the subexcitation electrons the energy of which is between h(o 0j and fuom, and, consequently, the relative fraction of energy absorbed by an additive will be different from what it should be if the distribution of absorbed energy were solely determined by the relative fraction of valence electrons of each component of the mixture.213 214 According to estimates of Ref. 215, this effect is observed when the molar concentration of the additive is of the order of 0.1%. This selective absorption with ionization of additives has been first pointed out by Platzman as an explanation for the increase in the total ionization produced by alpha particles in helium after small amounts of Ar, C02, Kr, or Xe were added (the so-called Jesse effect).216... [Pg.321]

Thermal Neutron Absorption Cross Section. The ease with which a given nuclide can absorb a thermal neutron (energy 33 eV) and become of a different nuclide is indicated by the cross section, given here in units of barns (1 barn = 10-24cm2). If the mode of reaction is other than in, y), it is so indicated, for example, (n,p) or (n, a), where n = neutron, p = proton, y = gamma ray, and a = alpha particle (4He). [Pg.429]

Why can you assume negligible self-absorption of the alpha particles in the samples prepared for counting ... [Pg.50]

In the second separation, uranium is extracted from thorium. Ethyl acetate is the extractant for uranium, which is bound in a nitrate complex. Thorium remains in the aqueous phase. Thorium is then co-precipitated with Nd(OH)3 to avoid absorption of the beta particles emitted by 234Th and 234mPa by the large amount of NH4N03 if the solution were simply evaporated and counted. The filter with Nd(OH)3 is mounted on a planchet for counting beta and alpha particles. [Pg.52]

Any other body which has absorptivity a fiw) = 1 for photons with energy Hui will emit radiation according to (4.1). Although the sun consists mainly of protons, alpha particles and electrons, its absorptivity is a(Tkj) = 1 for all photon energies tiw, by virtue of its enormous size. Its temperature is not homogeneous, but emitted photons originate from a relatively thin surface layer a few hundred kilometres thick, in which the temperature is constant and in which all incident photons are absorbed. Conversely, only photons emitted within this surface layer may reach the surface of the sun. The solar spectrum observed just outside the Earth atmosphere agrees well with (4.1)... [Pg.118]

The deposition of polonium on metal wires gives rise to a useful a-source. Tips of metal wires having a length 10 mm and a diameter of 0.2 mm were utilized. They were made of Al, Ni, Pd, Pt or An. Each was immersed in 100 pi of a solution containing °Po (300 Bqml ) for 15 h at 27°. Alpha particle emission was measured using a liquid scintillation system. There was an observed diminution in the a-pulse spectra for all of the wires except Al. This was attributed to the mutual diffusion between the wire metal and °Po. The °Po deposited on the Al wire had a tendency to be eluted with the liquid scintillator. This was attributed to physical absorption on the porous metal oxide layer on the Al wire and °Po. The °Po deposited by the Al wire had a tendency to be eluted with the liquid scintillator. It was possible to prepare a °Po -Al wire as a useful a-source by heating at 120° for 30 minutes. [Pg.3936]

Which of the following transmutations entails an absorption of an alpha particle and release of a proton ... [Pg.15]


See other pages where Absorption alpha particle is mentioned: [Pg.166]    [Pg.166]    [Pg.173]    [Pg.123]    [Pg.207]    [Pg.194]    [Pg.1754]    [Pg.62]    [Pg.58]    [Pg.26]    [Pg.843]    [Pg.1800]    [Pg.203]    [Pg.381]    [Pg.1407]    [Pg.42]    [Pg.173]    [Pg.273]    [Pg.302]    [Pg.313]    [Pg.214]    [Pg.34]    [Pg.510]    [Pg.34]    [Pg.116]    [Pg.163]    [Pg.164]    [Pg.181]    [Pg.219]    [Pg.34]    [Pg.289]    [Pg.288]    [Pg.677]    [Pg.669]   
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