1. CFD Modelling of Spiral
Membrane Modules
A Seminar in Chemical Engineering
Kaushal Sanjayrao Kaloo
16CHE135
Department of Chemical Engineering
Institute of Chemical Technology,
Mumbai
2. 1. Introduction
and Scope of
the study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
2
Figure: Feed spacer configurations: (a) non-woven (b)
partially woven (c) middle layer (d) fully woven
Two essential functions of feed spacer:
1. Structural support to the adjacent membranes
2. Enhanced mass transfer through the membrane
surface.
Objectives of ongoing research:
1. minimizing the trans-membrane pressure drop
2. decreasing concentration polarization
3. minimizing membrane fouling
3. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on
flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
3
lf = 2mm
lf = 2mm
Figure: Variation in the velocity profiles with Reynold's number
and axial distance between two filaments (Sousa, et al. 2014).
Gradient: Blue=0.0 m/s to Red: 0.58 m/s
lf = 8mm
lf = 8mm
Re=250
Re=10
Figure: Eddy generation at high velocities (Liang, et al.
2016) . Gradient: Blue=0 m/s to Red=3.4 m/s
Re=64
4. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on
flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
4
0
4000
8000
12000
16000
0 100 200 300
οP/L(Pa/m)
Re
L=4 mm L=2 mm
Figure: Variation of pressure drop with Reynold's number and
filament spacing (Sousa, et al. 2014)
Factors that influence pressure drop (Shakaib et al. 2009):
Feed
attack
angle
(Ξ±)
Filament
thickness
Filament
spacing
5. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on
flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
5
Figure : Pressure gradient along the membrane surface
with spacer (Vrouwenvelder, et al. 2010). Gradient:
Blue=0.0 kPa to Red=0.06 kPa
Pressure drop in spacer-filled membrane channel
β’ Discretized drop in pressure along the direction of
flow
β’ Within spacer diamonds, almost no pressure
gradient is observed
β’ Resistance offered by the spacer filaments to the
flow is much higher than that offered by the
membrane wall
6. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
6
Figure: Concentration polarization in membrane (a) without spacer (b)
with spacer (Li, Bui and Chao 2016). Gradient: Blue: 13 mol/m3 to Red:
15.5 mol/m3
(a)
(b)
Concentrated island
β’ Li, Bui and Chao (2016) found that near the
spacer filaments, the convective flux is low. This
isolates the stagnant zone with smaller flux.
β’ Salt concentration increases immediately before
and after the flow impinges on a spacer
filament.
β’ Higher likelihood of fouling
7. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
7
Figure 10: Concentration polarization in different spacer geometries: (a) non-woven (b) partially woven (c) middle
layer and (d) fully woven (Gu, Adjiman and Xu 2017) Gradient: Blue: 605 mol/m3 to Red: 650 mol/m3
(a) (b)
(c) (d)
8. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
8
0
5
10
15
20
25
30
0 50 100 150 200 250
SCEx10^4
Re
Empty channel Non-woven
Middle layer Fully woven
0
0.5
1
1.5
2
100 125 150 175 200
SCEx10^4
Re
Spacer Configuration Efficacy
β’ Kavianipour, Ingram and Vuthaluru (2017) took
trade-off between mass transfer enhancement
and pumping energy requirements in devising SCE
β’ ππΆπΈ =
πβ
ππ
; High SCE values are desirable for
spacer configurations.
β’ Non-woven geometry has the highest SCE for low
Reynolds numbers (Re<120) while for higher Re
(Re>120) the fully-woven configuration has a
slightly better SCE.
9. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane
fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
9
Membrane fouling
β’ Biomass attachment: expressed as mole of
biomass attached to spacer mesh per unit area of
membrane per day
β’ Biomass growth: Monod growth kinetics
(expressed as mole of biomass per unit time)
β’ Biomass detachment: Based on stress created by
liquid past biofilm
(a)
(b)
(c)
Figure: Biofouling in (a) non-woven (b) fully
woven (c) middle-layer spacer configurations
(Radu et al. 2010)
10. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane
fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
10
Figure: Vortex shedding due to forced slip velocity (Lim, et al.
2018) Gradient: Blue=0 m/s to Red= 0.28 m/s
No vortex shedding
Vortex shedding
Permeate flux enhancement
β’ 5-7% higher pumping energy requirements
β’ more than 2X increase in maximum shear stress
β’ Flow perturbation at resonant frequency
β’ Potential reduction in biofouling
11. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
11
Authors Pressure drop Mass transfer Spacer characteristics
Guillen and Hoek
(2009)
π = 0.25 +
189.29
π π
; π π
= 200 π‘π 500
πβ = 0.46 π π0.36
ππ0.36
; ππ
= 620
L/D = 9
ο’ not specified
Circular, middle
layer
Koutsou et al. (2009) Not available πβ = 0.13π π0.66 ππ0.4; ππ
= 1 β 100
L/D =6 to 8
ο’ =90β¦ to 120
Configuration not
mentioned
Koutsou and
Karabelas (2015)
βπ
πΏ
= 5.82π πβ0.64; π π
= 100 β 200
πβ β π π π; π
= 0.66 β 0.73;
Sc = 1 β 100
L/D= 10
ο’ = 120β¦
Novel spacer
Li et al. (2016) π = π πβ0.33 ; π π = 100 β
300
πβ π π0.4 ; ππ = 560 L/D = 6
ο’ not specified
Circular, fully
woven
Kavianipour et al.
(2017)
οπ
πΏ ο΅π π π;
π π = 100 β 400;
π = 1.06 π‘π 1.55
πβ π π π ; ππ = 660;
a = 0.257 β 0.549
L/D = 8
ο’ =90β¦
Circular, different
configurations
12. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
12
Figure 13: Comparison of pressure drop in ideal vs real
spacer geometry (Picioreanu, Vrouwenvelder and van
Loosdrecht 2009)
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
0 2 4 6 8 10 12 14 16 18 20
Pressure(kPa)
Module Length (mm)
Real geometry Ideal geometry
Idealized spacer geometry
Figure: (Left) Microscopic image of the spacer diamond; (Right)
Realistic spacer geometry; (Right after transition) Idealized spacer
geometry
13. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
13
2D vs 3D modelling
β’ Vrouwenvelder, et al. (2010) observed that the velocity field at 75% of the
channel height showed a profile that differs strongly from the channel
centre.
β’ With the presence of a spacer, the velocity flow nearer to the membrane
is mostly parallel to the spacer filaments. This behaviour is not observed
at the channel centre.
β’ Local phenomena such as mass transfer, velocity profiles vary
significantly in the transverse direction.
14. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
14
Boundary conditions
1. Permeable wall
β’ Local permeate flux calculation
β’ Membrane permeability is not constant
β’ Higher computational time and cost
2. Impermeable wall
β’ Constant concentration at the wall
1. 100% w/w of solute (worst-case fouling)
2. Saturated concentration of solute
β’ Easier computation
15. 1. Introduction
and Scope of the
study
2. Fluid Dynamics
2.1 Velocity profiles, flow transition
2.2 Pressure drop
2.3 Effect of spacer geometry on flow
3. Mass Transfer
3.1 Concentration polarization
3.2 Effect of spacer geometry
on mass transfer
4.1 Membrane fouling
4.2 Permeate flux
enhancement
5. Critical
Review
CFD Study of Spiral Membrane Modules
15
Study Sherwood
number, Sh
Power number, Pn
x 10-3
Spacer configuration
efficacy, SCE x 104
Saeed et al. (2015) 29 473.1 0.66
Kavianipour et al. (2017)
with same boundary
conditions as Saeed et al.
(2015)
27.6 296.8 0.93
Kavianipour et al. (2017) 54.2 294.6 1.84
16. CFD Study of Spiral Membrane Modules
16
Effect of spacer geometry on
fluid dynamics and mass
transfer (Koutsou, et al./
Shakaib et al./Guillen and
Hoek)
2009
2010
Effect of spacer
geometry on
membrane
biofouling
(Radu, et al.)
2014
Hydrodynamics
and mass
transfer
characteristics of
RO membrane
(Sousa, et al.)
Novel spacer
design to enhance
mass transfer
(Koutsou and
Karabelas)
2015
Spacer
Configuration
Efficacy
(Kavianipour, et al.)
2017
2018
Permeate flux
enhancement
using forced
velocity slip
(Lim, et al.)
Flow transition
dynamics
(Qamar, et al.)
2019
Editor's Notes
A vital component of spiral-wound membrane modules is the feed spacer. It performs two essential functions:
Structural support to the adjacent membranes
Enhanced mass transfer through the membrane surface.
Fundamental understanding of hydrodynamics associated with these spacer designs is critical to improve the permeate flux performance by :
minimizing the trans-membrane pressure drop
decreasing concentration polarization
minimizing membrane fouling
The average mass transfer coefficient increases with the increase in transverse filament thickness.
The increase in thickness however restricts the higher mass transfer coefficient values to a small portion
and distribution becomes non-uniform.
For each spacer type, the highest average water flux is achieved with a mesh angle of 60Β°.
In case of non-woven and partially woven geometries:
upper wall of the membrane received slightly more flux than the lower one.
This results in asymmetric mixing patterns on either sides of the membrane.
Spacer filaments are in direct contact with the upper membrane wall all the way through the feed channel. As a result, maximum accumulation of the solute at the side edges was observed
middle-layer spacer geometries:
mixing was fairly symmetrical
thick axial filaments completely block the side openings
Partially woven and fully woven spacers:
the mixing pattern differed with mesh angle.
exhibit uniform solute concentration distribution as the filaments are not in direct contact with membrane surface
An interesting observation was made for fully woven geometry that there are distinct areas of concentration polarization in the middle between axial filaments, where the cross flow velocity is particularly low as the inflow stream is split by the front transverse filament.
The empty channel has the maximum SCE due to its very low pressure drop, but it is an uncommon configuration to choose due to the absence of recirculation zones, which results in a high probability of deposit build-up on the membrane surface.
1. feed spacer geometry had little impact on mass transfer; hence, engineering spacers to improve concentration polarization, trans-membrane osmotic pressure, or product water
quality may prove difficult and yield limited benefits. In contrast, thinner filaments spread further apart significantly reduced hydraulic losses with negligible impacts to mass transfer. In addition, a few noncircular filament shapes produced even lower hydraulic losses, which might prove beneficial for RO/NF treatment of low salinity waters where hydraulic losses through spiral wound elements contribute significantly to the total process energy consumption