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Nitrate removal studies on polyurea membrane using nanofiltration system – membrane characterization and model development

  • Ravichand Kancherla ORCID logo , Vadeghar Ramesh Kumar , Ginuga Prabhaker Reddy and Sundergopal Sridhar EMAIL logo
Published/Copyright: September 21, 2020
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Abstract

Desalination of nitrates from brackish water is prominent in the coastal areas due to excessive disposal of pesticides by agricultural industries. Nowadays, membrane processes are growing tremendously for the desalination of brackish water. In this context, polyurea (PU) could be a useful membrane material for the treatment of brackish water. The present work deals with the removal of nitrates from synthetic water using PU membranes by nanofiltration (NF) process. Polyurea thin film composite (PU-TFC) membranes were prepared by interfacial polymerization followed by thermal crosslinking and characterized using Fourier transformed infrared spectral (FTIR), X-ray diffraction (XRD), scanning electron microscopy– energy dispersion X-ray spectroscopy (SEM–EDS), Atomic force microscopy (AFM), thermogravimetric (TGA), and universal testing machine (UTM) for structural analysis, crystallinity, morphological, compositional, thermal and mechanical properties, respectively. Experimental studies were conducted on an NF pilot plant by varying operating pressure from 2 to 10 bar and feed nitrate concentration from 60 to 200 mg/L for evaluating PU membrane performance. Experimental observations revealed a maximum water flux of 30.6 L/m2 h and nitrate rejection of 97.2% at a pressure of 10 bar for feed containing 140 mg/L of nitrate. A mass transfer model was developed on the basis of solution–diffusion mechanism for a semi-batch NF process by considering cake enhanced concentration polarization model, for laminar flow with feed recycle, using a plate and frame membrane module. A generic semi-batch NF process model was integrated taking into account concentration polarization and fouling layer resistance. The integrated model was successfully compared with existing data in literature and could be used for process scale-up. Due to the merits of hydrophilicity, negative charge, high thermal and mechanical resistance, the PU membrane can be termed as a low cost, commercially viable and ecofriendly barrier for separation of nitrates.


Corresponding author: Sundergopal Sridhar, Membrane Separations Group, Chemical Engineering Division, Indian Institute of Chemical Technology (IICT), Hyderabad 500007, India, E-mail:

Acknowledgments

Authors would like to thank the Director, CSIR-IICT, Hyderabad, India, for the support and this paper possesses IICT Manuscript Communication Number: IICT/Pubs./2020/246. We also acknowledge the National Project Implementation Unit (NPIU) and State Project Facilitation Unit (SPFU), Telangana, India, for the financial support provided through TEQIP-II.

  1. Author contribution: All the authors have accepted responsibility for the entire content of this submitted manuscript and approved submission.

  2. Research funding: None declared.

  3. Conflict of interest statement: The authors declare no conflicts of interest regarding this article.

Appendix

Various model equations used for estimating membrane transport parameters

Kedem–Katchalsky model [47]

(21) Solvent flux , J w : J w = L p ( Δ P σ Δ π s ) ,   Δ π s = R T ( C m C p )

(22) Solute flux , J s : J s = ω Δ π s + C s ¯ ( 1 σ ) J w

where

  • ΔP is hydraulic pressure difference and Δπ s is the osmotic pressure difference.

  • C f , C m , C p are solute concentrations at feed side, membrane, and the permeate side

  • C s ¯ is the logarithmic mean of C m and C p .

Model constants L p , σ, ω are specific hydraulic permeability, reflection coefficient, and local solute permeability.

Spiegler–Kedem model [48]

(23a) Solute rejection , R : R = σ ( 1 F ) ( 1 σ F )

(23b) F = exp ( ( 1 σ ) J w P ) = exp ( ( 1 σ ) J w ω   R T )

where P represents solute permeability.

Jitsuhara and Kimura model for charged membranes [41]

Reflection coefficient, σ for a negatively charged membrane [47]

(24) σ = ( Δ p Δ Π i Δ Π s ) J w = 0 = 1 X 2 Δ C s [ Z I I Z I ( 2 t 1 0 1 ) ln 2 t 1 0 1 + Z I I 2 t 1 0 1 + Z I ]

where Z = 1 + ( 2 C s X ) 2 .

Reflection coefficient, σ based on Jitsuhara and Kimura model is given by:

(25) σ = 1 + ϕ X Δ C s [ Z I I Z I ( 2 t 1 1 ) ln 2 t 1 1 + Z I I 2 t 1 1 + Z I ]

where

(26) Z =   1 + B , B = ( 2 C s ϕ X ) 2 , X = X ϕ w ,

  • X is the charge density of the membrane,

  • ϕ is osmotic coefficient, and ϕX′ is effective charge density, t is the transport number [49],

  • and the superscripts I and II represent the higher and lower pressure sides.

The other transport parameter – solute permeability P is determined from:

(27) P = R T ϕ X ϕ w k 2 F 2 Δ X C s I C s I I { ( 1 + B ) 1 ) C s } d C s C s I C s I I { ( 1 + B ) 1 ) ( 1 + B ) + 1 )   1 λ 1 0 + 1 λ 2 0 } d C s

where, ϕ w is the water content of the membrane, k 2 is tortuosity factor, ϕ w /k 2ΔX is the parameter used instead of numerous individual parameters ϕ, X′, k 2, ΔX [50].

Combined film theory Spiegler–Kedem (CFSK) model:

Observed solute rejection, R obs

(28) ln ( 1 R obs R obs ) = ln ( 1 R R ) + J w k

where k the coefficient of mass transfer.

Observed solute rejection, R obs [51] is given by:

(29) R obs = 1 1 σ ( 1 exp ( 1 σ P ) J w ) exp ( J w k ) + 1

After simplication R obs [33] can represented as:

(30) R obs 1 R obs = a 1 [ 1 exp ( J w a 2 ) ] [ exp ( J w k ) ]

(31a) a 1 =   σ 1 σ

(31b) a 2 = 1 σ P

with maximum rejection observed at:

(32) J w , min = k [ ln ( 1 + Pe ) Pe ]

where Pe is Peclet number given by:

(33) Pe = ( 1 σ ) k P

J w,min is the point where the rejection will be maximum and is equal to the mass transfer coefficient k.

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Supplementary material

The online version of this article offers supplementary material (https://doi.org/10.1515/cppm-2020-0041).


Received: 2020-05-07
Accepted: 2020-09-10
Published Online: 2020-09-21

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