In-situ monitoring of RO membranes using electrical impedance spectroscopy: Threshold fluxes and fouling

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1 Engineering Conferences International ECI Digital Archives Advanced Membrane Technology VII Proceedings In-situ monitoring of RO membranes using electrical impedance spectroscopy: Threshold fluxes and fouling Hans G. L. Coster School of Chemical and Biomolecular Engineering, University of Sydney, Sydney, Australia, Jia Shin Ho Division of Chemistry and Biological Chemistry, School of Physical and Mathematical Sciences ; Singapore Membrane Technology Centre, Nanyang Technological University, Singapore Lee Nuang Sim Singapore Membrane Technology Centre, Nanyang Technological University, Singapore Anthony G. Fane Singapore Membrane Technology Centre ; School of Civil and Environmental Engineering, Nanyang Technological University, Singapore Follow this and additional works at: Recommended Citation Hans G. L. Coster, Jia Shin Ho, Lee Nuang Sim, and Anthony G. Fane, "In-situ monitoring of RO membranes using electrical impedance spectroscopy: Threshold fluxes and fouling" in "Advanced Membrane Technology VII", Isabel C. Escobar, Professor, University of Kentucky, USA Jamie Hestekin, Associate Professor, University of Arkansas, USA Eds, ECI Symposium Series, (2016). This Abstract and Presentation is brought to you for free and open access by the Proceedings at ECI Digital Archives. It has been accepted for inclusion in Advanced Membrane Technology VII by an authorized administrator of ECI Digital Archives. For more information, please contact franco@bepress.com.

2 In-situ Monitoring of RO Membranes using Electrical Impedance Spectroscopy: Threshold fluxes and Fouling Hans G. L. Coster School of Chemical and Biomolecular Engineering In collaboration with Singapore Membrane Technology Centre

3 Membrane Dielectric Structure Skin Layer Sub layer

4 What is involved in Impoedance Spectroscopy? Injection of sinusoidal AC currents through the membrane Measurement of the current and voltage across the membrane Measurement of the phase shift between the voltage & current Current voltage sample Phase shift Contact solution/material Sinewave signal generator

5 Electrical representation of films Homogeneous film C Film with 2 substructural layers C 1 C 2 G G 1 G 2 d d 1 d 2 C 1 = F/m 2 G 1 = S/m 2 C 2 =0.059 F/m2 G 2 =4.35 S/m 2

6 - Imaginary impedance Nyquist Plots Help to discern various processes and layers with different time constants g 1 g 1 g 2 c 1 c 1 c 2 Real impedance additional arcs appear for each element with a different time constant

7 EIS Membrane characteristics Fitted data Each dielectric element or transport process will have a characteristic electrical time-constant. These various elements/processes can be readily distinguished in a Nyguist plot of the imaginary vs the real impedance. Data for RO with NaCl 2000ppm and silica 200 ppm, crossflow 0.15 m/s: from Ho, Sim, Gu, Webster, Fane & Coster (2015).

8 Non-linear Effects: Concentration polarization membrane Build up in time of solute at surface Pressure driven flux + - Electrically driven transport of ionic solutes Ion concentration profiles will depend on the transport numbers

9 Electrical Diffusion Polarization Negatively charged Membrane The electric potential due to the back diffusion is in the same direction as the driving potential

10 AC Diffusion Polarization Effects With AC currents, the profiles undergo an inversion during each cycle At very high frequencies there is insufficient time for concentration polarization to manifest At low frequencies the concentration polarization will be much larger than at high frequencies of the AC.

11 Impedance Monitoring Cross-flow Module Cross section of module Voltage electrodes Current injecting plate electrodes

12 An Impedance Cross-flow Module for monitoring membrane fouling in situ Chamber plates/current electrodes Insulating spacers and gasket Membrane Pressure plate Exploded view of internal plates and gaskets.

13 EIS: Effect of Flux RO feed: 200 ppm silica with 2000 ppm NaCl; crossflow velocity; 0.15 m/s. Ho, Sim, Gu, Webster, Fane & Coster / Journal of Membrane Science 500 (2016) 55 65

14 EIS Nyguist plots vs Flux at low fluxes

15 EIS Nyquist plots at higher fluxes

16 Fouling: A Threshold Phenomena 0.15 m/s 0.30 m/s RO feed: 200 ppm silica with 2000 ppm NaCl. Ho, Sim, Gu, Webster, Fane & Coster / Journal of Membrane Science 500 (2016) 55 65

17 EIS detection of the Threshold 0.15 m/s 0.30 m/s RO feed: 200 ppm silica with 2000 ppm NaCl. Ho, Sim, Gu, Webster, Fane & Coster / Journal of Membrane Science 500 (2016)

18 TMP (bar) Membrane Signatures in early stages of Filtration 5 hrs silica Saline no silica 2 hrs Silica Wang, Sim, Gu, Coster & Fane J Mem Sci Time (hour)

19 Signatures of Membrane Fouling TMP (bar) 5 hrs silica 15 hrs silica 48 hrs silica Cake enhanced concentration polarization The EIS signatures changed well ahead of fouling revealed by TMP Data from Wang, Sim, Gu, Coster & Fane J. Mem Sci Time (hour)

20 Effect of Spacers Without spacer With spacer

21 Effect of Spacers on Gdp Without spacer With spacer RO feed: 200 ppm silica with 2000 ppm NaCl; crossflow velocity; 0.15 m/s Ho, Sim, Gu, Webster, Fane & Coster / Journal of Membrane Science 500 (2016)

22 Silica fouling: Suggested mechanism Slow built up of the silica layer on the membrane surface; Electrical conductance in the concentration polarization layer drops- Gdp decreases. Impact of the cake enhanced concentration polarization (CECP) effect; The increased concentration polarization of NaCl at the membrane surface increases the conductance of the concentration polarization layer and Gdp. More NaCl permeates through the membrane which shows up in a decrease in rejection. 21

23 Locating a Canary Membrane Fouling Monitor in Water Treatment Plants Brine (sludge) EIS Fouling Monitor EIS Fouling Monitor Permeate Product Feed

24

25 Collaborators Singapore SMTC, NTU A.G. Fane L. N. Sim Z.J. Wang C. Tang J. S. Ho J. Gu Australia Chemical Eng., USYD T. Chilcott J. Kavanagh G. Barton J. Cien S. Hussain T. Handelsman CMS innovations Pty Ltd Andrew Sinclair Peter Martin

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