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Bistability in a simple fluid network due to viscosity contrast. Brian Storey, John Geddes, David Gardner Franklin W. Olin College of Engineering Russell Carr University of New Hampshire. Problem and model. Fluids in inlet 1 and 2 have different viscosities,
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Bistability in a simple fluid network due to viscosity contrast Brian Storey, John Geddes, David Gardner Franklin W. Olin College of Engineering Russell Carr University of New Hampshire
Problem and model Fluids in inlet 1 and 2 have different viscosities, but are otherwise simple Newtonian fluids.
Set flow Q1 and Q2– 2 states Q1 Q1 Qc Qc Q2 Q2
Viscosity ratio = 1 Q1 Qc Q2 Q1 Qc Q2
Viscosity ratio = 2 Q1 Qc Q2 Q1 Qc Q2
Viscosity ratio = 10 Q1 Qc Q2 Q1 Qc Q2
Pressure driven- 4 states P1 P1 P1 P1 Qc Qc Qc Qc P2 P2 P2 P2
Viscosity ratio =1 Q2=0 QC=0 Q1=0
Viscosity ratio=10 Q2=0 QC=0 Q1=0
Experimental setup Water P1 Qc Water + Sugar P=0 P2
Experimental data of sugar in inlet 2 (μ2)
Criterion for existence of bistability Arrhenius viscosity law General viscosity law
Conclusions • This work could have been done ~100 years ago. • We predict and observe bistability in a simple network with laminar flow of Newtonian fluids. Flow direction depends on history. • Perhaps the simplest example of bistability in (micro)fluidics? Quake Prakash and Gershenfeld Groisman et al
Stratified flow – effective viscosity Immiscible Miscible, diffuse Fully mixed
Viscosity ratio = 5 Q1 Qc Q2 Q1 Qc Q2
Viscosity ratio=5 Q2=0 QC=0 Q1=0
Q1 Qc Q2
Q1 Qc Q2
Q1 Qc Q2
Q1 Qc Q2