Результаты исследований: Вклад в журнал › Статья › Рецензирование
Результаты исследований: Вклад в журнал › Статья › Рецензирование
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TY - JOUR
T1 - Mass-spectroscopic study of the diffusion and solubility of helium in submicrocrystalline palladium
AU - Zhiganov, A.
AU - Kupryazhkin, A.
AU - Mulyukov, R.
AU - Bitkulov, I. Kh.
N1 - R.R. Mulyukov and I.Kh. Bitkulov are grateful to the Russian Foundation for Basic Research (grant no. 02-01-97924-r2002agidel a) and the Integrated program “Nanocrystals and Supramolecular Systems” of the Russian Academy of Sciences for partial financial support.
PY - 2002
Y1 - 2002
N2 - By the method of helium thermal desorption from submicrocrystalline palladium presaturated in the gaseous phase, the diffusion coefficient Dff and solubility coefficient Ceff of helium are measured in the range P = 0-3 MPa and T = 293-508 K. The pressure dependence of Ceff flattens at high pressures. At low saturation pressures, the temperature dependences of the diffusion and solubility coefficients may be divided into (1) high-temperature (400-508 K) and (2) low-temperature (293-400 K) ranges described by the exponentials D1, 2 = D0exp(-E1,2D/kT) and C1, 2 = C0exp(-E1,2S/kT). The energies of diffusion activation are E2D = 0.0036 ± 0.0015 eV and E1D = 0.33 ± 0.03 eV, and the solution energies are E2S = -0.025 ± 0.008 eV and E1S = 0.086 ± 0.008 eV in the low- and high-temperature ranges, respectively. Mechanisms behind the diffusion and solution of helium are discussed. © 2002 MAIK "Nauka/Interperiodica".
AB - By the method of helium thermal desorption from submicrocrystalline palladium presaturated in the gaseous phase, the diffusion coefficient Dff and solubility coefficient Ceff of helium are measured in the range P = 0-3 MPa and T = 293-508 K. The pressure dependence of Ceff flattens at high pressures. At low saturation pressures, the temperature dependences of the diffusion and solubility coefficients may be divided into (1) high-temperature (400-508 K) and (2) low-temperature (293-400 K) ranges described by the exponentials D1, 2 = D0exp(-E1,2D/kT) and C1, 2 = C0exp(-E1,2S/kT). The energies of diffusion activation are E2D = 0.0036 ± 0.0015 eV and E1D = 0.33 ± 0.03 eV, and the solution energies are E2S = -0.025 ± 0.008 eV and E1S = 0.086 ± 0.008 eV in the low- and high-temperature ranges, respectively. Mechanisms behind the diffusion and solution of helium are discussed. © 2002 MAIK "Nauka/Interperiodica".
UR - https://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcAuth=tsmetrics&SrcApp=tsm_test&DestApp=WOS_CPL&DestLinkType=FullRecord&KeyUT=000179042600015
UR - http://www.scopus.com/inward/record.url?partnerID=8YFLogxK&scp=0036861902
U2 - 10.1134/1.1522114
DO - 10.1134/1.1522114
M3 - Article
VL - 47
SP - 1440
EP - 1443
JO - Technical Physics
JF - Technical Physics
SN - 1063-7842
IS - 11
ER -
ID: 43957264