close

Вход

Забыли?

вход по аккаунту

?

Some Design Aspects of Aromatic Polyamide Reverse-Osmosis Membranes.

код для вставкиСкачать
Some Design Aspects of Aromatic
Polyamide Reverse-Osmosis
Membranes
Hal Wood'. and S. Sourirajan2
' Industrial Membrane Research Institute, Department of
Chemical Engineering, University of Ottawa, 161 Louis
Pasteur, Ottawa, Ontario, Canada K1N 6N5
Department of Chemical Engineering, National University of
Singapore, 10 Kent Ridge Crescent, Singapore 05 1 7 ,
Singapore
Linear-polymer solutions are comparable to a suspension of macromolecule spheres.
Macromolecules concentrate at the interface during the membrane-forming
procedure. They coalesce with each other suficiently for the su$ace to become a
sheet of interconnected macromolecules. Interstitial voids are formed whose
magnitude is dependent on the size and packing arrangement of the macromolecules,
and is also influenced by the extent of coalescence occurring in the interstitial voids.
A subsequent gelation procedure renders the macromolecules paracrystalline.
During operation, the membrane allows permeation of solution components primarily
through the interstitial voids.Membrane design requires the ability to predict
membrane pe~ormancefrom the precursor casting conditions. This paper illustrates
the practical utility of the interstitial void modelfor membrane design purposes. Some
design aspects are presented for various reverse-osmosis membranes made from an
aromatic polyamide polymer.
Review of Polymer Membranes
Reverse osmosis (RO) and ultrafiltration (UF)membranes are made by gelling a
film of polymer solution. The resultant membrane is a dense skin-layer supported
by a more porous substrate. Changes in the casting conditions influence the
performance of the final membrane product. For a given polymer, membrane
performance is dependent primarily on the morphology of the skin layer. A
polymeric membrane skin layer generally contains a bimodal distribution of pores.
They originate from t h e interstitial void spaces in the surface layer of
paracrystalline macromolecules. The porous structure is dependent on the size,
geometric disposition, and degree of coalescence of the surface macromolecules.
The following section contains a short review of linear polymer solutions and
membrane films, including a summary of the equations that are used to determine
* To whom correspondence should be addressed.
Developments in Chemical Englneering and Mineral Processlng, Val. 1, No. 4, page 238
Design Aspects of Aromatic Polyamide Membranes
239
polymer-solution structure and membrane skin-layer morphology. The interstitial
void model is then presented, and some established membrane design principles
are reviewed. In the Evaluation section to follow, additional design aspects of
some aromatic polyamide (PA) membranes are established. The emphasis is on
large pores in skin layers of membranes made from PA/DMAc/CaC12 solutions.
Design aspects of other surface morphological constants are also discussed. The
interstitial void model is shown to be useful for determining an effective skin
layer thickness and the number of pores per membrane area, which are valuable
tools for transport analysis.
Linear polymer solutions and their resultant films
A typical linear polymer molecule occupies its own domain in the solution space.
In most RO/UF casting solutions, accurate estimates of macromolecule
dimensions can be determined from the equation:'
4xRs = VE -- 0.507 MIyN,
(1)
where Rs (cm) is the hydrodynamic radius occupied by the macromolecule
M is the polymer molecular
sphere; g is the polymer concentration (g
weight (g gmol-'); and No is Avogadro's number. The quantity v (cm3) is the
volume occupied by one polymer molecule in its crystal state, and E is an
expansion factor to account for swelling of the macromolecule when in an
appropriate solvent.
A modification to equation ( 1 ) may be required if an additive is present in the
casting solution.24 The quantity M is substituted in equation (1) by Map,,, the
apparent polymer molecular weight (g gmol-'), as determined from:
[TI)= m,,, 01
(2)
The polymer-solvent-additive intrinsic viscosity, [TI' (cm3 g-'), is compared
to the Mark-Houwink constants K (cm3 g-') and a,as determined for the polymer
in pure solvent only. Then Mapp is equal to M, unless the additive causes an
intrinsic viscosity change. From equations (1) and (2), Rs increases with either an
increase in M, or decrease in g, or an increase in intrinsic viscosity caused by the
additive.
Surface tension and/or solvent evaporation effects during the membraneforming procedure cause polymeric particles to concentrate at the interface. Due
to crowding, solvent evaporation or other effects, the polymeric particles form
permanent contacts with each other. The interfacial layer becomes an
interconnected sheet of partially coagulated macromolecules. The extent of
coalescence amongst adjacent macromolecules is dependent on the casting
composition, solution structure and membrane-forming procedure. It is unlikely
that coalescence proceeds to such an extent that the interstitial gaps become
completely closed. Eventually, the macromolecules are rendered paracrystalline,
and the resultant membrane can be used as a separation film.5
The magnitude of an interstitial void in a monolayer of spheres can be
determined from geometry considerations, and depends upon the size and packing
disposition of the spheres. The geometric values of the interstitial voids in a
macromolecule monolayer can also be determined for given values of Rs. Note
that Rs and the geometric void spaces are inherent in the casting solution
structure. However, the magnitude of an interstitial void i n a gelated
macromolecule monolayer is also dependent on the degree of coalescence
amongst the macromolecules.
H, Wood and S. Sourirajan
240
From Poiseuille's equation:
Q = AP n ~t~ ~ / p(. ~
8)
(3)
where the flux Q (cm3 cm-'s-') of solvent, of viscosity p (g cm-' s-') through a
sheet containing n (cm-') non-interacting pores of radius R (cm) and length
L (cm) is proportional to the applied pressure gradient AP (g cm-' s-').
Experimental RO/UF membrane performance data may be applied to a modified
Poiseuille transport equation in order to characterize the skin layer morphology in
terms of a porous structure. The Poiseuille equation is modified to account for
friction when the solute bumps along the pore wall, and for interfacial interactions
that can cause the solute to be attracted or repelled from the membrane material.
With ROKJF membranes, even under high operating pressures, separation can
occur even if the solute is appreciably smaller than the pore diameter.
The modified Poiseuille equation also accounts for the possibility there may
be more than one mean pore size and pore size distribution on the membrane
surface. The experimental data indicate that there are usually two average pore
sizes. There are small pores of mean radius Rbl and standard deviation 01; there
also are larger pores of mean radius Rb2 and standard deviation 62. The ratio of
the number of large to small pores (h2) can be determined. Once the membrane
surface is characterized by these constants, performance can be predicted for most
solute-solvent combinations and operating conditions. 6
The interstitial void model of membrane surfaces
It is assumed that all permeate transport occurs through the interstitial voids in the
skin layer of an RO/UF membrane. The skin layer morphological constants are
then a reflection of the size, disposition and degree of coalescence of the surface
macromolecules. For each membrane, the surface morphological constants can be
compared to the geometric interstitial void spaces, so that the disposition and
degree of coalescence of the surface macromolecules can be determined. Since
membrane performance can be predicted if the surface constants are known, then
the interstitial void model is a link that connects casting conditions to the final
membrane performance.
Salt-separation ability is possible if the channels through the membrane skin
layer are sufficiently small. According to the interstitial model, Rs must be small
and the surface macromolecules be predominantly close-packed in order to
produce the minimum possible geometric void space. Also, some coalescence
occurs amongst the surface macromolecules, which further decreases the
magnitude of the interstitial channels. The surface morphological constants Rbl
and 01 result from interstitial voids formed by close packing of surface
macromolecules. The constant h2 indicates there are also voids of size Rb2 and
standard deviation 02, formed by other packing arrangements of the surface
macromolecules. Solute-separation ability decreases if either Rs increases, or
interstitial coalescence amongst surface macromolecules decreases, or if h2
increases. The interstitial void model is supported by data for casting solution and
surface structure for RO and UF membranes made from cellulose acetate,
polyethersulfone and aromatic polyamide polymer^.^
Design Aspects of Aromatic Polyamide Membranes
241
Evaluation of Membrane Formation and Performance
The effect of casting conditions on PA membrane surface formation has previously
been reported by the author^.^^^** In general, interstitial coalescence within
close-packed voids increases with any change in casting composition that causes
an increase in Rs. For any value of Rs, the degree of coalescence within
close-packed voids is relatively independent of the type and/or quantity of
additive used in the casting solution. A minimum macromolecule radius may be
reached where permanent contacts between adjacent close-packed
macromolecules do not occur, and this is relatively independent of the
membrane-forming procedure. Deviations from close packing depend on the
polymer type, the polymer molecular weight, and the type or concentration of
additive in the solution. Large pores in RO membranes are formed by the square
packing and subsequent partial coalescence of surface macromolecules.
Membrane desalination ability decreases if the macromolecules rise into, but do
not coalesce with, the surface monolayer.
' h o UF membranes made from polyethersulfone (PES) polymer have also
been analysed according to the interstitial void model.7 Although Rs is small,
many surface PES macromolecules do not pack closely together. Also, relatively
large voids are formed because macromolecules are missing from the surface
array. These factors contribute to the substantial decrease in selectivity of a PES
membrane compared to those made from PA.
For a cellulose acetate (CA) RO me~nbrane,~
the macromolecules are small
and predominantly close-packed, and the CA polymer repulses salt ions more
strongly than does PA, Therefore, for CA membranes, the degree of coalescence
need not be so high, and some large pores may be formed by macromolecules
missing from the array without greatly reducing overall desalination ability.
In summary, membrane performance can be linked to the casting composition
by comparing the surface morphological constants to Rs and the geometric void
spaces. The interstitial void model is a useful tool for membrane design purposes.
The effect of casting conditions can be related to the porous structure of the
resultant membrane, and the structure and performance can be predicted without
first making the membrane.
The design of PA/DMAc/CaC12 membranes
The following example illustrates the practical utility of the interstitial void model
for design purposes. Membranes of various surface morphologies and ROAJF
performance abilities are made by changing the concentration of PA polymer
(M = 31,300 g gmol-') and/or CaC12 additive, in dimethylacetamide (DMAc)
~ o l v e n t .In~ all solutions to be analysed for design considerations, the CaC12
concentration is below the critical ~ a l u e . The
~ , ~ membranes are made by
evaporating DMAc from a thin film of polymer solution at 95°C for 15 minutes,
then immersing in ice-cold water for at least an hour. The macromolecule
dimensions are calculated for each casting solution, and the porous structure of
each resultant membrane is determined from experimental performance data.3
Casting composition, solution structure and the surface morphological data for
the PA/DMAc/CaC12 system are contained in Table 1. The values of Rbl, 61, 6 2
and hz are not included in Table 1 since they remain relatively constant, and
independent of the casting composition. Rbl ranges from 6.5 to 6.6 A and is
independent of Rs. this indicates that interstitial coalescence in close-packed
voids increases with an increase in Rs. The standard deviation (61) of Rbl is
H,Wood and S. Sourirajan
242
Table 1 Casting solution and surface morphological data for some PA
membranes3
7.0
9.0
10.5
12.5
14.0
0.1
0.1
0.1
0.1
0.1
64.6
59.1
55.6
52.5
50.4
31
27
23
22
20
2.8
3.9
6.1
5.4
6.3
31
27
24
21
20
7 .O
9.0
10.5
12.5
14.0
0.2
0.2
0.2
0.2
0.2
71.0
64.2
60.7
57 .O
54.6
43
34
30
29
25
-5.9
-0.4
1.7
0.8
3.5
43
35
31
27
25
7.0
9.0
10.5
12.5
14.0
0.3
0.3
0.3
0.3
0.3
72.3
66.1
62.5
58.6
56.1
50
44
36
31
29
-12.2
-9.4
-3.3
-0.4
0.3
51
42
37
32
28
* estimated from equation (8).
usually negligibly small (about 0.01 A). This shows that for a particular
membrane sample, the degree of interstitial coalescence in each close-packed void
is constant throughout the membrane surface. The ratio of the number of large to
small pores per membrane surface area is approximately 0.001. Changes in the
casting composition mainly influence the magnitude of the large pores (Rb2) on
the resultant membrane surface, while 0 2 is close to zero.
The cross-sectional (xs) void area between square (s) packed spheres can be
compared to a pore opening of equal area of radius rs xs. From geometry:
Rs/rs
xs
= [(4 - T C ) / T C ] - ~=’ ~ 1.913
(4)
Table 1 includes values of ARb2 (= rs xs - Rbz), and values close to, or greater
than zero, indicate that the large pores are comparable in size to voids formed by
the surrounding and partial coalescence of four surface macromolecules. The
variation (02) in the average size of these large pores is approximately zero.
Therefore, for each membrane, the degree of coalescence in each void formed by
the square packing of surface macromolecules is relatively constant throughout
the membrane surface. Some casting solutions made of low PA and high CaC12
content produce large pores which are much greater in magnitude than rs xs. These
voids are formed by macromolecules that migrate towards the surface during
membrane formation, but do not coalesce with the monolayer. In these
Design Aspects of Aromatic Polyamide Membranes
243
Table 2 The slope and intercept of Rs versus ARb2 data Cfrom Table I ) .
D1
g CaClz
/g PA
(A)
0.1
0.2
0.3
-3.43
-1.70
-1.12
Dz
73.28
61.41
57.53
Correlation
coefficient
0.93
0.94
0.97
membranes, the standard deviation 0 2 can be quite large, and may be estimated in
relation to the magnitude of ARbz.8
Membrane design for this PA/DMAc/CaC12 system is possible if the average
large-pore radius can be predicted from the casting composition. Data from
Table 1 are useful for this purpose, and show that there is a linear relationship
between Rs and ARbz as given by:
(5)
Rs = Dimb2 + D2
if the CaClZIPA mass ratio is constant. The values of D1 and Dz, and
corresponding correlation coefficients, are given in Table 2. The correlation
coefficients are slightly smaller than 1, possibly because Rb2 is estimated to the
closest Angstrom (A), but Rs and rs xs are calculated to a higher decimal place.
From the data of Table 2, there is a direct relation between D1 and the
CaC12/PA weight ratio in the casting solution, namely:
D, = -(gPA/gCaClz)/3
(6)
There is also a linear relation between D1 and D2, as given by:
D1 = -0.1465Dz + 7.300
(7)
The correlation coefficients for equations (6) and (7) are approximately one.
By combining equation (6) with equation (7), and substituting into equation ( 5 ) ,
upon rearrangement:
ARb2 = 3(49.8 - RS)(gCaCl2/gPA)+ 6.826
(8)
Equation (8), in combination with equations (1) and (4), may be used to
predict Rb2 from the casting composition. Values of Rb2 estimated from
equation (8) are contained in Table 1.
The critical CaClZ/PA ratio (CaC12*) is 0.33 g of CaC12 er g of PA.4 From
equations (6) and (7), Dl equals -1 and D2 equals 56.7
at CaC12*. From
equation (8), ARb2 equals zero at CaC12* when Rs equals 56.7 A. Equation (8)
shows that when the CaClz concentration is at or above CaC12*, Rb2 is greater
than rs xs when Rs is greater than 56.7 A. It is interesting to note that the
minimum calculated Rs [equations (1) and ( 2 ) ] in this PA/DMAc/CaClZ system at
CaC12* is 55.8 A. This indicates that membranes with large pores formed only by
square packing are made from solutions below CaC12*. The origin, and ultimately
the size of a large pore, is minimised if the casting composition is below CaC12*.
Consider the possibility that no CaC12 is added to the casting solution. From
equation (8):
Rbz = Ts xs - 6.826
(9)
s:
H, Wood and S. Sourirajan
244
which indicates that large pores occur, even if no CaC12 is present in the casting
solution. Since the minimum possible Rs in this PA/DMAc system is about 30 A,
then Rb2 remains relatively large, and the close-packed voids become essentially
closed when no CaC12 is present in the casting solution. Since h2 is small, low
flux nanofiltration membranes are produced.'
Flux Analysis
Macromolecules in the surface PA monolayer are predominantly close-packed.
There are two interstitial voids per close-packed macromolecule. From geometry
considerations:
= 3-112~ 2
S
where n is the number of close-packed voids per membrane area. Equation (10)
shows that n is maximised when Rs is minimised. Neglecting deviations from
close packing, for typical data in Table 1 if Rs equals 60 A and Rbl is 6.6 A, then
interstitial pores occupy about 2.2% of the total membrane surface area. This
value agrees well with published data for CA UF membranes."
Some modifications can be made to Poiseuille's equation in order to estimate
an effective pore length (skin layer thickness) for RO membranes:
a) The flux Q (cm3
s-') is substituted b the experimentally-determinedpure
water permeation rate, PWP (g cm- 2 h- 7).
b) According to Poiseuille's equation: PWP a R4. However, due to interfacial
and/or pore size distribution effects, PWP for RO membranes is trongly
affected by the pore radius, but to less than the fourth power.""' It is
estimated that PWP a R'.' for CA RO membranes.13Therefore, PWP a R'.'
is assumed to be applicable to PA RO membranes, since the dielectric
constants of PA and CA are similar, at least in comparison to that of water.
c) Since h2 for RO membranes is small, data from Table 1 and refs 2 to 4 show
that Rbi
is much greater than h2Rb2 1'5.Because salt-separating
membranes are under consideration, the effect of the large pores on flux must
be minimal. Therefore R is replaced by Rbl in the modified Poiseuille
equation.
d) Since h2 for RO membranes is small, then n can be estimated from
equation (10).
In a previous study,3 and for the data of Table 1, 13.2-cm2 membrane coupons
were tested with 25°C water at an operating pressure of 250 psig. By substituting
the above factors into the Poiseuille equation, upon rearrangement:
L -2.0773~10~
X Rbl '.'/(RS
X
PWP)
(1 1)
where L is an effective skin-layer thickness. The units of Rbl, Rs and L for
equation (11) are in Angstroms, and PWP in gl(13.2 cm2 h). An effective pore
length may be estimated if Rs, Rbl and PWP are known. For example, Rs for a
casting solution made from 10.5 wt% PA and 0.1 g CaC12/g PA is 55.6 8,
cm2 h)3. From
(Table l), and the resultant Rbl is 6.5 8, and PWP is 1.87
equation (1 l), the effective skin-layer thickness is about
skin layer thicknesses observed by electron microscopy.'
Design Aspects of Aromatic Polyamide Membranes
245
Example problem
Assuming that an Rbl value of about 3.5 A is required to achieve excellent
desalination ability with a PA membrane, estimate the optimum PWP for a
membrane made from a PA-solvent-additive solution. Compare the performance
to that of some existing PA membranes.
(a) A small Rs value is desirable to maximise n [equation (lo)]. The minimum
macromolecule radius5 for coalescence to occur within a close-packed void is
approximately 30 A. With proper choice and quantity of additive,
close-packed macromolecules (Rs approximately 35 A) can coalesce together
sufficiently to produce interstitial voids that are 3.5 A in radius.2 Then from
'~
equation (lo), if Rs equals 35 A, there are approximately 4 . 7 ~ 1 0 small
pores per square centimetre of membrane surface.
(b) The flux is maximised when the effective skin layer thickness is minimised.
Assume the casting conditions can be controlled so that the skin consists of
one monolayer of macromolecules, Then L is approximately equal to 2Rs, or
70 A, i.e. the diameter of a solution macromolecule.
From equation (1 l), for 25°C water at an operating pressure of 250 psig, the
optimal PWP is approximately 1.2 g cm-2 h. The optimal PWP can be compared
to values for some PA/DMAc/additive membranes of ref.2. Note that the Rbl
values for these membranes vary from about 3.0 to 4.0 A. From equation (1 l), the
effect of this difference in the membrane Rbl-value, compared to the design value
of 3.5 A, on the PWP is small. The PWP values for these membranes2 varies from
h, which is significantly lower than the optimum PWP.
0.07 to 0.33 g
%o major factors contribute to the decrease in the actual membrane PWP
below the optimal value. From equations (1) and (lo), the polymer concentration
is too low and/or the additive effect on swelling is too high to produce a small R s
and large n. From equations (1) and (1 l), the polymer and additive concentrations
are too low so the effective skin layer thickness is much greater than 2Rs, i.e. the
skin layer is composed of more than a monolayer thickness of macromolecules.
Conclusions
Linear polymeric RO/UF membranes have been analysed according to the
interstitial void model. Casting solution macromolecules that constitute the
surface monolayer are predominantly close-packed. Variations in the casting
conditions cause changes in the size, distribution and degree of coalescence of the
surface macromolecules, thereby affecting the overall porosity and performance
of the resultant membrane.
This paper shows that the interstitial void model can be used for membrane
design purposes. The large pores in PA/DMAc/CaC12 membranes have been
examined in detail. The flux through an RONF membrane is determined by the
interstitial model, and estimates of the number of pores per membrane area and
effective skin layer thickness can be made.
Using the interstitial model, membrane performance can be related to the
casting conditions. The performance of a membrane can be predicted, without first
having to make the membrane and test it. Membrane design is possible, regardless
of the validity of the assumptions involved in determining casting solution
structure and resultant membrane surface morphological constants.
246
H, Wood and S. Sourirajan
Acknowledgements
Hal Wood wishes t o thank the NSERC for partial support of this work. Special
thanks to T.D. Nguyen for his helpful comments and suggestions.
References
I . Wood, H. and Sourirajan, S. 1991. The effect of additives, solvent type, and polymer
concentration on macromolecule dimensions. J. Appl. Polymer Sci., 43( l), 21 3-217.
2. Nguyen, T.D., Matsuura, T. and Sourirajan, S. 1987. Effect of nonsolvent additives on
the pore size and pore size distribution of aromatic polyamide RO membranes. Chem.
Eng. Commun., 54, 17~ .
3. Nguyen, T.D., Matsuura, T. and Sourirajan, S. 1987. Effect of the casting solution on the
pore size and pore size distribution of resulting aromatic polyiunide membranes.
Chem. Eng. Commun., 57,351-369.
4. Nguyen, T.D., Chan, K., Matsuura, T. and Sourirajan, S. 1985. Viscoelastic and
statistical thermodynamic approach to the study of the structure of polymer film
casting solutions for making ROAJF membranes. Ind. Eng. Chem. Prod. Res. Dev.,
24(4), 655665.
5 . Wood, H., and Sourirajan, S. 1992. The effect of polymer solution composition and
film-forming procedure on aromatic polyamide membrane skin layer structure. J.
Colloid Inte$ace Sci., 149(1), 105-1 13.
6. Sourirajan, S. and Matsuura, T. 1985. Reverse Osmosis/Ultrafiitration Process
Principles, Chap.4. Available from Division of Chemistry, National Research Council,
Ottawa, Canada, KIA OR6; NRCC No. 24188.
7. Wood, H. and Sourirajan, S. 1993. The nature of pores in the skin layer of polymeric
reverse osmosis/ultrafiltration membranes. Dev. Chem. Eng. Min. Proc.
8. Wood, H. and Sourirajan, S. 1992. The origin of large pores on aromatic polyamide
membrane surfaces. J. Colloid Inte$ace Sci. (accepted for publication).
9. McKinney, R. 1972. Reverse osmosis separations with aromatic polyamide films and
hollow fibres. Sep. Purq Methods, 1(1), 31-115.
10. Ohya, H., Imura, Y.,Moriyama, T.and Kitaoka, M. 1974. A study on the pore size
distribution of modified ultrathin membranes. J. Appl. Polymer Sci., 18, 1855-1867.
11. Matsuura, T., Taketani, Y.and Sourirajan, S. 1983. Interfacial parameters governing
reverse osmosis for different polymer material - solution systems through gas and
liquid chromatography data. J. Colloid Interface Sci., 95(1), 10-22.
12. Matsuura, T. and Sourirajan, S. 1981. Reverse osmosis transport through capillary pores
under the influence of surface forces. Ind. Eng. Chem. Prod. Des. Dev., 20, 273-282.
13. Glueckauf, E. and Russell, P.J. 1970. The equivalent pore radius of dense cellulose
acetate membranes. Desalination, 8(3), 351-357.
Received: 16 September 1992; Accepted afier revision: 18 February 1993.
Документ
Категория
Без категории
Просмотров
1
Размер файла
560 Кб
Теги
reverse, design, polyamide, aspects, membranes, aromatic, osmosis
1/--страниц
Пожаловаться на содержимое документа