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. 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
ρ n ∂ v n ∂ t + ρ n ( v n ⋅ ∇ ) v n = − ρ n ρ ∇ p − ρ s σ ∇ T + η ∇ 2 v n ; {\displaystyle \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}};}
ρ s ∂ v s ∂ t + ρ s ( v s ⋅ ∇ ) v s = − ρ s ρ ∇ p + ρ s σ ∇ T , {\displaystyle \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 {\displaystyle P} is the pressure, T {\displaystyle T} is the temperature, η {\displaystyle \eta } is the viscosity of the normal component, σ {\displaystyle \sigma } is the entropy per unit mass, and ρ = ρ s + ρ n {\displaystyle \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
∂ ρ ∂ t + ∇ ⋅ J = 0 , {\displaystyle {\frac {\partial \rho }{\partial t}}+\nabla \cdot \mathbf {J} =0,}
where the total flow is given by
J = ρ s v s + ρ n v n . {\displaystyle \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. It was inspired by the superfluid model.
References
External links [1] Two Fluid Model of Superfluid Helium
