Entrainment of Second Sound in Steady-State Counterflowing Normal and Superfluid Helium II
Earl M. Johnson, Alvin F. Hildebrandt
Abstract
Earl M. Johnson, Alvin F. Hildebrandt
Abstract
The velocity dependence of second sound in liquid helium was measured as a function of the relative velocity (${\stackrel{\ensuremath{\rightarrow}}{\mathrm{v}}}_{n}\ensuremath{-}{\stackrel{\ensuremath{\rightarrow}}{\mathrm{v}}}_{s}$), where ${\stackrel{\ensuremath{\rightarrow}}{\mathrm{v}}}_{n}$ is the normal fluid velocity and ${\stackrel{\ensuremath{\rightarrow}}{\mathrm{v}}}_{s}$ is the superfluid velocity. The experimental technique consisted of measuring the time of flight of a second-sound pulse in steady-state counterflowing normal and superfluid for subcritical velocities. The results are in agreement with the theoretical predictions by Khalatnikov.
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The velocity dependence of second sound in liquid helium was measured as a function of the relative velocity (${\stackrel{\ensuremath{\rightarrow}}{\mathrm{v}}}_{n}\ensuremath{-}{\stackrel{\ensuremath{\rightarrow}}{\mathrm{v}}}_{s}$), where ${\stackrel{\ensuremath{\rightarrow}}{\mathrm{v}}}_{n}$ is the normal fluid velocity and ${\stackrel{\ensuremath{\rightarrow}}{\mathrm{v}}}_{s}$ is the superfluid velocity. The experimental technique consisted of measuring the time of flight of a second-sound pulse in steady-state counterflowing normal and superfluid for subcritical velocities. The results are in agreement with the theoretical predictions by Khalatnikov.
Key concepts: Superfluidity, Second sound, Isotopes of helium, Physics, Helium-4, Critical ionization velocity, Entrainment (biomusicology), Helium