Abstract
The jump conditions at surface of discontinuity are derived for the two-fluid model of helium II from postulated balance laws for the total energy, the linear momentum of the superfluid and from an entropy production inequality. These conditions are used to discuss a contact surface and the propagation of a weak shock.
Keywords
Entropy Helium Total Energy Contact Surface Entropy ProductionNomenclature
- A
Helmholtz free energy function (A=U−ST)
- Fis
external body force acting on the superfluid
- fis
superfluid acceleration (=∂ t v i s +v k s u i,k s )
- Gis
density of supply of linear momentum to the superfluid
- gis
diffusive force of the superfluid (=G i s −m s v i s )
- ms
short notation for ∂ t ρ s +(ρ s v k s ), k
- qk
heat flux vector per unit area per unit time
- r
heat supply function per unit mass unit per time
- S
entropy per unit mass of helium II
- T
absolute temperature (> 0)
- tis
superfluid stress vector ( i s =n k σ ki s )
- U
internal energy per unit mass of helium II
- vis
superfluid velocity
- ρ
total mass density
- ρs
superfluid mass density
- σijs
superfluid stress tensor
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References
- [1]Landau, L. D., J. Phys. (U.S.S.R.) 5 (1941) 71.Google Scholar
- [2]
- [3]
- [4]Kelly, P. D., Int. J. Eng. Sci. 2 (1964) 129.Google Scholar
- [5]Eringen, A. C., Int. J. Eng. Sci., 3 (1965) 197.Google Scholar
- [6]
- [7]Kapitza, P. L., J. Phys. (U.S.S.R.), 4 (1941) 181.Google Scholar
- [8]Khalatnikov, I. M., J. Exptl. Theoret. Phys. (U.S.S.R.) 23 (1952) 253. (A translation appears in An introduction to the theory of superfluidity by I. M. Khalatnikov, W. A. Benjamin Inc. (1965))Google Scholar
- [9]Courant, R. and K. O. Friedrichs, Supersonic flow and shock waves, Interscience Publishers Inc. (1948).Google Scholar