| Literature DB >> 33816731 |
Tarik Eljaddi1, Deisy Lizeth Mejia Mendez1, Eric Favre1, Denis Roizard1.
Abstract
The data contained in this publication refers to a new approach to design composite pervaporation membranes that could be useful in water treatment. The work is based on the rational prediction of the membrane mass transfer coefficient using the resistance in series model and the corresponding experimental membranes were tested with several aqueous solutions comparatively to a commercially available porous distillation membrane (PVDF). All the related data, i.e. permeation water fluxes and conductivity of the permeate, were collected for hours, in the range 3 to 7 h. The strategy was to develop pervaporation membranes by coating a porous PVDF support (122µm) with various dense layers (hydrophobic polymers: Teflon™ AF2400, PMP, PTMSP). The objective was to avoid definitely the wetting problem observed in membrane distillation while keeping approximately the permeance than the porous support. The data reported here are related to the surface property of the membranes (contact angles), to the mechanical resistance of the membranes, to the wetting phenomena observed directly and recorded by observing the variation of water flux through the membranes and to the conductivity of the water condensed at the permeate side.Entities:
Keywords: Conductivity; Contact angles; Desalination; Hydrophobic composite membranes; Water permeance
Year: 2021 PMID: 33816731 PMCID: PMC8005762 DOI: 10.1016/j.dib.2021.106943
Source DB: PubMed Journal: Data Brief ISSN: 2352-3409
Fig. 1a) View of the flat cell used for the desalination experiments: total area 40cm2, direct contact membrane distillation configuration (DCMD). The downstream side is shown here with a piece of a PVDF membrane in place. The cell was home-made using a transparent glassy material (PMMA) to help the visualization of the tangential flow and of the wetting phenomenon.
b) A drop a water was deposed on the membrane: the spherical shape of the drop is due to the hydrophobic property of the membrane surface (contact angle: 125°).
Fig. 2Automatic recording of the permeate weight: steady state is reached after about 1h. The main governing parameter is the temperature regulation. The stabilized slope is 85.6 g/h for pristine PVDF.
Fig. 3Example of the stability of feed and permeate temperatures versus time. Case of PVDF and Teflon™ AF2400 experiments with pure water.
Fig. 4Example of flux stability versus time. Case of PVDF and of the composite membranes with pure water.
Fig. 5Example of flux stability versus time. Case of PVDF coated with Teflon™ AF 2400, long lasting experiment with pure water.
Fig. 6Investigation of the wetting resistance of the membranes versus feeds containing successively NaCl (up to 10g/L) and NaCl with a surfactant (SDS 1g/L). The addition of the surfactant induces first the partial the wetting of the membrane (time≈3h) and then a liquid convective flux through all pores (time≈5.5h).
Fig. 7Visualization of the wetting phenomena with a porous PVDF membrane, from the feed inlet to the feed outlet. Feed: NaCl 10g/L + 1g/L SDS à 50°C. On the Fig. 7_b) and Fig. 7_c) the dark strips indicate some partial wetting.
Permeability of glassy polymers for water (P, Barrer) and related mass transfer coefficient versus thickness of the active layer [2,3].
| PVDF | PTMSP | PMP | Teflon AF2400 | |
|---|---|---|---|---|
| Porous | Dense layer | Dense layer | Dense layer | |
| Permeability (Barrer ±10%) | NA | 11 200 | 1 000 | 4000 |
Calculated from the measured water permeance according to the reference [4]
Calculated from the water permeability data [2,3,5]
Contact angle measurements of pristine PVDF and composite membranes.
| Contact angle | ||||||||
|---|---|---|---|---|---|---|---|---|
| Membrane | 1 | 2 | 3 | 4 | 5 | average (°) | Deviation | Ref |
| PMP+PVDF | 97.4 | 89.8 | 98.2 | 97.7 | 96 | 2.99 | ||
| PTMSP+PVDF | 82.3 | 82.5 | 80.3 | 80.9 | 90.1 | 83 | 2.75 | |
| Teflon AF2400 +PVDF | 103.4 | 113.6 | 113 | 116.2 | 115.8 | 112 | 3.6 | |
| PVDF pristine | 121.2 | 127 | 127.3 | 126.6 | 126 | 2.16 |
Pull-Off adhesion test measurements of pristine PVDF and composite membranes.
| Experiment | PVDF pristine | PMP | PTMSP | Teflon AF2400 |
|---|---|---|---|---|
| 1 | 0.26 | 1.63 | 1.44 | 3.34 |
| 2 | 0.2 | 1.45 | 1.48 | 3.27 |
| 3 | 0.24 | 1.51 | 1.75 | 3.24 |
| Average (MPa) | 0.2 | 1.5 | 1.6 | 3.3 |
| Deviation | 0.02 | 0.07 | 0.13 | 0.04 |
| Subject | Chemical Engineering |
| Specific subject area | desalination, pervaporation, membrane distillation |
| Type of data | Table, Image, Figure |
| How data were acquired | The porous and composites membranes were tested in direct contact configuration cell with an active surface of 40 cm2. The centrifuge pumps, temperature, and flux sensors are provided from RS Components, the bench conductivity meter is a Jenway 4520 and the balance is from Sartorius (0.01 g). The data related to mass transfer were recorded using LabVIEW software, the images were recorded in 12 megapixels size with the camera of a smartphone (Samsung 7). The contact angles were measured with the apparatus Dataphysics Instruments GmbH (DI) Germany equipped with a goniometer OCA-PSA Drop 8 using the software SCA20. |
| Data format | Raw and Analyzed |
| Parameters for data collection | The porous support and hydrophobic composite membranes were prepared and characterized by several solutions (Distillated water, salt solutions with or without surfactant, i.e. SDS) |
| Description of data collection | The operating conditions are as follows: Both the feed and the permeate solutions were circulated in close loops Cross flow is ensured on each side of the membrane Flow rates are respectively 1 L/min on the feed side and 0.8 L/min on the permeate side Water vapor is condensed on the cold side and is continuously weighted by the balance as the water in excess the conductivity of water is continuously measured and recorded in |
| For each experiment, the feed solution, initially pure water on the feed side, is circulated during about 2 hours to reach steady state conditions linked to the stabilization of temperatures on both side of the membrane. The warm and cold temperatures are recorded at the inputs and outputs of the membrane cell.The water vapor which permeates through the membrane is condensed on the downstream side in the flowing cold liquid. The excess of liquid is directly collected and weighted. In these conditions of steady state, the mass increase is linear versus time | |
| Data source location | Université de Lorraine, CNRS, LRGP, F-54000 Nancy, France |
| Data accessibility | With the article as Excel file |
| Related research article | Tarik Eljaddi, Deisy Lizeth Mejia Mendez, Eric Favre, Denis Roizard, Development of new pervaporation composite membranes for desalination: theoretical and experimental investigations, |