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Activity measurements at the microfluidic scale: towards osmotic pressure measurements

GDR CNRS AMC2 October 20-22, Sète. Activity measurements at the microfluidic scale: towards osmotic pressure measurements. ZIANE Nadia. Supervisors : J . Leng and JB . Salmon. Introduction. Dialysis process : P erfect control of the environment

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Activity measurements at the microfluidic scale: towards osmotic pressure measurements

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  1. GDR CNRS AMC2 October 20-22, Sète Activity measurements at the microfluidic scale: towards osmotic pressure measurements ZIANE Nadia Supervisors: J. Lengand JB. Salmon

  2. Introduction • Dialysisprocess: • Perfect control of the environment • Concentration of non-volatile solutes in aqueous solutions • Towards phase diagrams • Microfluidicsinterests: • Lineargeometry • Easy observations of confinedvolume • Easyanalysis and fastexperiments

  3. Microfluidic chip L0 PDMS h PDMS membrane e = 30 – 40 µm rectangularchannel w = 50 – 60 µm h = 30 – 40 µm L0 = 1,5 – 3 cm nL glass slide Randall and al., 2005 Salmon and Leng, 2010

  4. Water pervaporation

  5. Channel geometry: confined drop Step 1 Filldead-end microchannels Step 2 Injection of a fluorinatedoil or air Step 3 Evaporation of confineddroplets 60 µm L0 = 1,5-3 cm Noblin and al., 2008

  6. Simple model for solutions and dispersions Continuousand uniformconcentration  (t) = 0 L0 /L(t) Evaporation rate controlled by activity  • Hypotheses: • No initial gradients • Pe = hV/D < 1  no vertical gradients • Pervaporation rate uniformalong x • Quasi steadyregime for water pervaporation

  7. Absorbance measurements Bleu brillantFCF at 0,1 mM (10x) 200 µm  No gradients for molecular solutions

  8. Fluorescence meausurements Fluorescent latex (40x) Diameter = 20 nm 50 µm • Gradients at x=0 : • evidence of « leakage » velocity x=Lg x=0 J. Angly and al., 2012

  9. Fluorescence meausurements Fluorescent latex (40x) Diameter = 200 nm 50 µm • Gradients at x=0 : • evidence of « leakage » velocity • Gradients at x=Lg: • is not true < 1 x=Lg x=0 h T = h/V TD = h²/D

  10. Pure water Image analysis Time ~ 1h30

  11. Pure water Vf ~ 0,52 µm/s Te ~ 1500 s  Accurate estimation of humidyusing 1D model

  12. Binary water/glycerol mixture Ninni and al., 2000 Water/glycerol2% v/v Room humidity = 60% h = 26 µm, time ~ 2 hr

  13. Binary water/glycerol mixture Te ~ 2200 s

  14. Binary water/glycerol mixture

  15. Binary water/glycerol mixture

  16. Conclusion & outlooks • Robust measurements of the activity of aqueous solutions at the nanoliterscale • New chip design

  17. Conclusion & outlooks Estimation of liquid-liquidtransition of ternary system PEG/water/ammonium sulfate PEG: 5% w/w Ammonium sulfate: 5% w/w Time ~ 1h20

  18. Conclusion & outlooks Microdialysisprocess Hsieh, 2007 Jensen and al., 2008 • Development and characterization of new microfluidic devices including dialysis membranes • Control of osmotic exchanges at a nanoliter scale • Quantitative measurements of thermodynamic properties of complex fluids

  19. Thankyou Questions ?

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