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- W3035793281 abstract "Helium-film transfer rates ensuremath{sigma} have been measured as a function of level difference $z$ and height to the beaker rim $h$ for filling clean glass and neon-coated beakers. Observed transfer rates as a function of level difference or pressure head are described by: $ensuremath{sigma}(z)=frac{1}{[Aensuremath{-}Bmathrm{ln}z(mathrm{cm})]}$. For $T=1.65$ K and $h=7$ cm, we find $A=(1.80ifmmodepmelsetextpmfi{}0.09)ifmmodetimeselsetexttimesfi{}{10}^{4}$ sec/${mathrm{cm}}^{2}$ and $B=(8.9ifmmodepmelsetextpmfi{}1.9)ifmmodetimeselsetexttimesfi{}{10}^{2}$ sec/${mathrm{cm}}^{2}$. For $T=1.28$ K and $h=7$ cm, we find $A=(1.35ifmmodepmelsetextpmfi{}0.02)ifmmodetimeselsetexttimesfi{}{10}^{4}$ sec/${mathrm{cm}}^{2}$ and $B=(8.3ifmmodepmelsetextpmfi{}1.4)ifmmodetimeselsetexttimesfi{}{10}^{2}$ sec/${mathrm{cm}}^{2}$. Dependence of the transfer rate on film height is $ensuremath{sigma}(h)=10(frac{{ensuremath{rho}}_{s}}{ensuremath{rho}}){h}^{ensuremath{-}(0.26ifmmodepmelsetextpmfi{}0.05)}ifmmodetimeselsetexttimesfi{}{10}^{ensuremath{-}5}$ ${mathrm{cm}}^{3}$. For a glass beaker coated with Ne, the transfer rate is 16% less than the transfer rate for the same uncoated beaker. This is in reasonable agreement with our calculated helium-film thickness for a Ne substrate of $2.3 {h}^{ensuremath{-}frac{1}{3}}ifmmodetimeselsetexttimesfi{}{10}^{ensuremath{-}6}$ cm." @default.
- W3035793281 created "2020-06-25" @default.
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- W3035793281 date "1971-01-01" @default.
- W3035793281 modified "2023-10-17" @default.
- W3035793281 title "Dependence of the Helium-Film Transfer Rate on Pressure Head, Film Height, and Substrate" @default.
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- W3035793281 doi "https://doi.org/10.1103/physreva.3.191" @default.
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