Cross-Flow Microfiltration Oil-in-Water Emulsion Using Polyvinylidenefluoride Membrane

Cross-Flow Microfiltration Oil-in-Water Emulsion Using Polyvinylidenefluoride Membrane

Available online at www.sciencedirect.com Procedia Engineering 44 (2012) 1974 – 1976 Euromembrane Conference 2012 [P3.129] Cross-flow microfiltratio...

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Available online at www.sciencedirect.com

Procedia Engineering 44 (2012) 1974 – 1976

Euromembrane Conference 2012 [P3.129] Cross-flow microfiltration oil-in-water emulsion using polyvinylidenefluoride membrane K. Masoudnia*, A. Raisi, A. Aroujalian, M. Fathizadeh et al AmirKabir University of Technology, Iran A large amount of oily wastewaters is generated by industrial sources. Oil-in-water emulsions are the most serious pollutants for which current treatment technologies are often costly and ineffective. In recent years, membrane processes have been applied for oily wastewater treatment. Microfiltration (MF) was successfully used in oil-in-water separations [1]. The use of membranes to treat oil-water emulsions is increasing, especially in applications where the value of the recovered materials is high, e.g., recycling aqueous cleaners and machining coolants. For separation of oil emulsions as an end-of-pipe treatment, membranes are more likely where process volumes are less than 190 m3/day [2]. Membranes could also be useful in a hybrid system when it is combined with conventional chemical treatment systems to concentrate sludges. In this research, investigations were carried out for treatment of an oily wastewater. The effect cross flow velocity which corresponds with Reynolds number (300, 1500 and 2500) on the separation performance of the microfiltration process for treatment of an oil-in-water emulsion using a flat sheet polyvinylidenefluoride (PVDF) membrane was studied. Synthetic oily wastewaters were used to investigate the performance of polymeric membranes. Oil-in-water emulsions were prepared by mixing commercial grade gas–oil and deionized water. A blender was used to homogenize the mixtures at high shear rates (12000 rpm) for 60 min. The oil concentration of the synthetic feed was 3000 ppm for all experiments. The size of oil emulsion droplets in the feed was measured by a laser diffraction particle size analyzer, Nano ZS (red badge) ZEN3600 manufactured by Malvern Co. Droplet size distribution of the emulsion is presented in Fig. 1. As observed, mean droplet size is 901.0 nm. Hydrophilic PVDF membrane (Durapore, HVLP, Millipore CO., USA) with average pore size of 0.45μm was used in the experiments. The membrane was cut into 15 u 20 cm piece and was held in a flat-frame membrane module. Highly pure NaOH and HNO3 (Merck, Darmstadt, Germany) was used to prepare aqueous solutions for rinsing the membrane. After each experiment, the membrane module was rinsed with tap water for 30 min at high cross-flow velocity (Reynolds number of 2500) and at pressure of 1 bar to remove its reversible polarized layer. The permeate flux was calculated using the following equation:

J

w Au t

(1)

where W is weight of the collected permeate (kg), A is active membrane surface area (m2) and t is time duration of the experiment (h). The concentration of oil in the feed and permeate solution was determined by COD test bas on a standard method [3] using a COD analyzer (Nano ZS (red badge) ZEN3600 manufactured by Malvern Co). The effect of Reynolds number on the permeate flux at constant transmembrane pressure (TMP) is shown in Fig. 2. As shown in this figure, an increase in the Reynolds number is led to higher permeate fluxes. The Reynolds number that can be calculated from Eq. (6) is a well known dimensionless description of the hydrodynamic conditions in the feed flow:

1877-7058 © 2012 Published by Elsevier Ltd. doi:10.1016/j.proeng.2012.09.012

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K. Masoudnia et al. / Procedia Engineering 44 (2012) 1974 – 1976

Re

Uud h P

(2)

where ρ and μ are density and viscosity of the feed solution, respectively, u is cross-flow velocity and dh is hydraulic diameter of the membrane. The cross-flow velocity affects the shear stress at the membrane surface and, consequently, reduces the concentration polarization and accumulation of retained solutes by increasing the mass transfer coefficient. The influence of the Reynolds number on the permeate oil concentration is also shown in Fig. 3. It is observed that as the Reynolds number goes to a higher level, the oil concentration permeate enhances. It can be due to the fact that polarization layer resistance reduces with increasing in the cross-flow velocity, so more oil could pass across the membrane.

Figure 1. Droplet size distribution of the feed solution.

Figure2. The effect of Reynolds number on the permeate flux.

Figure3. The effect of Reynolds number on the permeate oil concentration.

The results show that the cross-flow velocity is the major variable responsible for flux increase, as shear forces minimize oil droplet deposits on the membrane surface. On the other hands, an increase in the cross-flow velocity results in an enhancement in the permeate oil concentration and consequently the oil rejection is decreased. Therefore, the variation in the cross-flow velocity should be optimized.

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K. Masoudnia et al. / Procedia Engineering 44 (2012) 1974 – 1976

References [1] M,Abbasi, M.Mirfendereski, M.Nikbakht, M.Golshenas, T.Mohammadi, Performance study of mullite and mullite–alumina ceramic MF membranes for oily wastewaters treatment, Desalination 259 (2010) 169–178. [2] M. Cheryana N. Rajagopalan,Membrane processing of oily streams Wastewater treatment and waste reduction, Journal of Membrane Science 151 (1998) 13-28. [3] Standard Methods for the Examination of Water and Wastewater ,5220 C. Closed Reflux, Titrimetric Method. Keywords: microfiltration, oily wastewater, polyvinylidenefluoride membrane, rejection