two-fluid model

In condensed matter physics, the two-fluid model is a macroscopic model to explain superfluidity. The idea was suggested by László Tisza in 1938 and reformulated by Lev Landau in 1941 to explain the behavior of superfluid helium-4.{{Cite book |last=Khalatnikov |first=I.M. |title=An Introduction to the Theory of Superfluidity. |publisher=Westview Press |year=2000 |isbn=978-0738203003}}{{Cite journal |last=Balibar |first=S. |date=2017 |title=Laszlo Tisza and the two-fluid model of superfluidity. |url=https://comptes-rendus.academie-sciences.fr/physique/articles/10.1016/j.crhy.2017.10.016/ |journal=Comptes Rendus Physique |volume=18 |issue=9-10 |pages=586–591 |doi=10.1016/j.crhy.2017.10.016}} This model states that there will be two components in liquid helium below its lambda point (the temperature where superfluid forms). These components are a normal fluid and a ideal fluid component. Each liquid has a different density and together their sum makes the total density, which remains constant. The ratio of superfluid density to the total density increases as the temperature approaches absolute zero.

Equations

The two-fluid model can be described by a system of coupled inviscid and viscous fluid system, in the low velocity limit, the equations are given by{{Cite book |last=Tilley |first=D. R. |url=https://www.google.fr/books/edition/Superfluidity_and_Superconductivity/I6JtWd3J8MIC?hl=en&gbpv=1&dq=two+fluid+model+euler+equations&pg=PA73&printsec=frontcover |title=Superfluidity and Superconductivity |last2=Tilley |first2=J. |date=1990-01-01 |publisher=CRC Press |isbn=978-0-7503-0033-9 |language=en}}

: $\rho_{\rm n} \frac{\partial \mathbf v_{\rm n}}{\partial t}+\rho_{\rm n} (\mathbf v_{\rm n} \cdot \nabla) \mathbf v_{\rm n}=-\frac{\rho_{\rm n}}{\rho}\nabla p - \rho_{\rm s} \sigma \nabla T +\eta\nabla^2 \mathbf v_{\rm n} ;$

: $\rho_{\rm s} \frac{\partial \mathbf v_{\rm s}}{\partial t}+\rho_{\rm s} (\mathbf v_{\rm s} \cdot\nabla) \mathbf v_{\rm s}=-\frac{\rho_{\rm s}}{\rho}\nabla p + \rho_{\rm s} \sigma \nabla T,$

where the $P$ is the pressure, $T$ is the temperature, $\eta$ is the viscosity of the normal component, $\sigma$ is the entropy per unit mass, and $\rho=\rho_{\rm s}+\rho_{\rm n}$ is the density as the sum of the density of the two components such that it follows a continuity equation

: $\frac{\partial \rho}{\partial t}+\nabla \cdot \mathbf J =0,$

where the total flow is given by

: $\mathbf J = \rho_{\rm s} \mathbf v_{\rm s} +\rho_{\rm n} \mathbf v_{\rm n} .$

These corresponds to a coupled Navier-Stokes equations (normal component) to Euler equations (ideal superfluid component).

Application to traffic

There is also a two-fluid model also refers to a macroscopic traffic flow model to represent traffic in a town/city or metropolitan area, put forward in the 1970s by Ilya Prigogine and Robert Herman.{{cite journal|title=A Two-Fluid Approach to Town Traffic|journal=Science|date=April 1979|volume=204|issue=4389|pages=148–151|doi=10.1126/science.204.4389.148|first1=Robert|last1=Herman|first2=Ilya|last2=Prigogine|author-link2=Ilya Prigogine|url=http://pchen.ccer.edu.cn/homepage/A%20Two-Fluid%20Approach%20to%20Town%20Traffic.pdf|pmid=17738075|bibcode=1979Sci...204..148H |s2cid=20780759 |url-status=dead|archive-url=https://web.archive.org/web/20120330005347/http://pchen.ccer.edu.cn/homepage/A%20Two-Fluid%20Approach%20to%20Town%20Traffic.pdf|archive-date=2012-03-30}} It was inspired by the superluid model.

References

External links

[http://www.yutopian.com/Yuan/TFM.html] Two Fluid Model of Superfluid Helium

Category:Mathematical modeling

Category:Traffic flow

Category:Superfluidity

Category:Fluid dynamics

Category:Liquid helium