[10] Preparation of Inner-side Tubular Zeolite NaA Membranes in a Continuous Flow System

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    Separation and Purification Technology 59 (2008) 141150

    Preparation of inner-side tubular zeolite NaA membranesin a continuous flow system

    Marc Pera-Titus 1, Marta Bausach 1, Joan Llorens , Fidel Cunill

    Chemical Engineering Department, University of Barcelona, 08028 Barcelona, Spain

    Received 21 February 2007; received in revised form 30 May 2007; accepted 31 May 2007

    Abstract

    Zeolite NaA membranes were synthesized on the inner side of porous titania (rutile) asymmetric tubular supports in a flow system where the

    synthesis gel was circulated through the support with flow rates in the range 1.54 mL min1

    by the action of gravity. The syntheses were carriedout hydrothermally at 358 K for 67 h either with or without previous brush-seeding of the supports. The membranes (1020m in thickness)

    showed great ability to dehydrate ethanol/water mixtures (92:8, w/w) by pervaporation with selectivities and fluxes, respectively, up to 8500 and

    1.2kgm2 h1 at 323 K. The role of intercrystalline defects in the pervaporation performance of the synthesized membranes was also investigated.

    2007 Elsevier B.V. All rights reserved.

    Keywords: Zeolite membrane; Continuous synthesis; Pervaporation; Alcohol dehydration; Intercrystalline pathways

    1. Introduction

    The research field on zeolite membranes has gained increas-

    ing attention in the last two decades in both materials science

    and chemical engineering owing to their potential applicationsas membrane separators, catalytic membrane reactors, selec-

    tive sensors and components in micro-electronic devices [15].

    In particular, a great deal of studies have been devoted to the

    preparation of hydrophilic zeolite membranes for dehydrating

    azeotropic and close-boiling liquid mixtures by pervaporation

    [611]. Among these zeolites, zeolite NaA has been the target of

    many investigationsdue to itshigh Al/Si ratio andsmallpore size

    (4.1 A). Under non-acidic conditions, zeolite NaA membranes

    offer the double advantage of high selectivity towards water sep-

    aration (>10,000) and high water fluxes. These attributes make

    them attractive for dehydrating solvents at industrial level [12].

    Among the different synthetic strategies reported in the lit-

    erature for zeolite membrane synthesis [1319], zeolite NaA

    membranes have been conventionally prepared by hydrother-

    mal synthesis onto a porous support in one or several batch

    Corresponding author. Tel.: +34 934034872; fax: +34 934021291.

    E-mail addresses: [email protected](M. Pera-Titus),

    [email protected] (J. Llorens).1 Present address: Institut de Recherches sur la Catalyse et lEnvironnement

    de Lyon (IRCELYON), UMR5256, CNRS/Universite Claude Bernard, Lyon 1,

    France.

    cycles, either in situ or with a preliminary seeding step (i.e.

    secondary growth method). The seeding of the support helps

    improving the quality and reproducibility of the zeolite layers by

    decoupling the nucleation and crystal growth steps [20,21]. By

    carefully controlling the seed layer coating the support throughthe use of a convenient technique (e.g. cross-flow filtration [22]

    or vacuum seeding [23]), the synthesized membranes show an

    improved separation performance and a preferential crystalline

    orientation. Table 1 shows a detailed survey of the most relevant

    seeding and hydrothermal synthesis conditions together with

    the available lab-scale techniques for zeolite NaA membrane

    preparation.

    Regarding the methods presented in Table 1, most of the stud-

    ies have been devoted to preparing zeolite films on flat supports

    or onto the outer surface of tubular supports. In the special case

    of inner-side tubular membranes, more suitable for developing

    full-size industrial modules, gel renewal constitutes an effec-

    tive strategy to partially overcome nutrient depletion due to the

    restricted accessibility of the synthesis solution to the lumen of

    the support. We have recently reported the batch preparation of

    high quality inner-side zeolite NaA membranes on -alumina

    under a low-g centrifugal field [26], which creates an axial flow

    that renews the synthesis solution in contact with the membrane.

    In order to reduce the number of synthesis cycles, we have

    also addressed the preparation of inner-side zeolite NaA mem-

    branes using a semi-continuous synthesis system [24]. This

    technique, earlier conceived by Pina et al. [25] for outer-side

    1383-5866/$ see front matter 2007 Elsevier B.V. All rights reserved.

    doi:10.1016/j.seppur.2007.05.038

    mailto:[email protected]:[email protected]://localhost/var/www/apps/conversion/tmp/scratch_11/dx.doi.org/10.1016/j.seppur.2007.05.038http://localhost/var/www/apps/conversion/tmp/scratch_11/dx.doi.org/10.1016/j.seppur.2007.05.038mailto:[email protected]:[email protected]
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    142 M. Pera-Titus et al. / Separation and Purification Technology 59 (2008) 141150

    Nomenclature

    a activity

    A parameters in the Antoine equation for vapor sat-

    uration pressure (K1)

    Si (0) MS surface diffusivity of water at zero coverage

    (m2 s1)ESw activation energy of water diffusion (kJ mol

    1)

    ESw,eff effective activation energy of water diffusion

    defined by Eq. (2) (kJmol1)

    KSw adsorption constant of water (Pa1)

    thickness of the zeolite layer (m)

    M molecular weight (kg mol1)

    NSw surface flux of water (kg m2 s1)

    P0w saturation vapor pressure of water (Pa)

    R constant of gases (8.314 Pa m3 mol1 K1)

    SWG seeding weight gain (mg cm2)

    T temperature (K)

    xw molar fraction of water in the liquid feedXw weight fraction of water in the liquid feed

    Yw weight fraction of water in the vapor permeate

    Greek symbols

    H0w adsorption enthalpy of water on zeolite NaA

    (kJ mol1)

    S density of zeolite NaA (1900 kg m3)

    zeolite NaA membrane synthesis, allows pulse-renewal of the

    synthesis solution in an autoclave at periodic intervals by the

    action of a set of electro-pneumatic valves. Layer formation canbe controlled by adjusting the gel renewal rate (i.e. the rate at

    which fresh gel is introduced into and used gel removed out

    of the autoclave). The membranes with the best pervaporation

    performance are those prepared with gel renewal rates lying

    in the range 1/41/7 min1 (i.e. introduction of fresh gel every

    47 min). These membranes give selectivities and fluxes up to

    16,000 and 0.6kg m2 h1, respectively, for the separation of

    92:8 (w/w) ethanol/water mixtures at 323 K.

    Despite the benefits of the semi-continuous synthesis sys-

    tem in terms of layer growth control, this technique presents

    some drawbacks regarding large-scale implementation. First, it

    involves the synthesis of membranes in an autoclave filled with

    a volume of 155 mL of synthesis gel that surrounds the tube(95% of total volume), but which itself is not employed in

    the synthesis of inner-side layers, thus contributing negatively

    to the economy of the process. A second shortcoming is related

    to the periodical pulse-renewal of the gel in the lumen of the

    support, which might sweep away the zeolite seeds and remove

    the amorphous gel layer covering the support surface during

    the synthesis. Finally, two semi-continuous synthesis cycles are

    often required to ensure good PV performance.

    To overcome all the above stated limitations, an alternative

    method for gel renewal can focus on using a flow system where

    the gel is continuously circulated in the lumen of the tubes.

    However, only a few studies dealing with the synthesis of inner-

    side tubular zeolite membranes by inducing a forced flow have

    been reported in theliterature.In this way, Richter et al.[34] have

    reported the synthesis of ZSM-5 membranes on the inner side

    of-alumina tubes and capillaries at 423K for 72 h by pumping

    the synthesis gel in the lumen of the supports at a flow rate in the

    range 414 mL min1 (0.25 cm min1). Culfaz et al. [35] have

    also prepared good quality MFI-type zeolite membranes on -

    alumina tubular supports at 355368 K for 7276 h in one to

    three cycles with a circulation of the synthesis gel by the action

    of a peristaltic pump at a flow rate of 648 mL min1.

    To our knowledge, the use of a flow system for zeolite NaA

    membrane synthesis has only been reported by Yamazaki and

    Tsutsumi [36] on flat supports, but has not already been reported

    for inner-side tubular configurations. Accordingly, this study is

    aimed at the hydrothermal synthesis of inner-side zeolite NaA

    membranes in a continuous flow system where the synthesis gel

    is flown by the action of gravity. The technique is promising for

    scaling up the synthesis process and for zeolite NaA synthesis

    in multi-channel tubes and capillaries.

    2. Experimental

    The zeolite NaA membranes were prepared by in situ and

    seeded hydrothermal synthesison the inner-sideof tubular asym-

    metric supports of 8 mm i.d. and 10 mm o.d. (TAMI, France).

    At the innermost part of these supports there was a 0.8m pore-

    size titania (rutile) layer of approximately 40m in thickness.

    Before the synthesis, the tubes were subjected to enameling at

    both ends with a commercial glaze (Duncan AN 313 Antique

    Blue) and a home-made glaze, both resistant to strong alkali,

    leaving an effective permeation length of approximately 5 cm

    and inner area of 12.6 cm

    2

    . The glazed tubes were dried at roomtemperature for a few minutes and then heated to 1173 K for

    15 min with a heating ramp of 1 K min1.

    2.1. Seeding of the supports

    Prior to secondary growth synthesis, the inner surface of the

    tubular supports was brush-seeded with A-type zeolite crys-

    tals (2m) supplied by IQE (Industrias Qumicas del Ebro,

    Zaragoza, Spain). To this end, zeolite NaA crystals were pow-

    dered on a thin test-tube brush capable of penetrating the lumen

    of the supports. Then the inner side of the supports was seeded

    by rotating the zeolite-loaded brush along the tube axis. The

    zeolite layer coating the support after the seeding was measuredin terms of seeding weight gain (SWG) [mg of seeds cm2 of

    surface area].

    2.2. Hydrothermal syntheses

    The hydrothermal syntheses were carried out in one cycle

    for periods of 37 h at atmospheric pressure in the tempera-

    ture range 353363 K with a cloudy synthesis gel of molar

    composition 1.0 Al2O3:1.8 SiO2:3.9 Na2O:270 H2O. The gel

    was prepared using two aluminate and silicate precursor solu-

    tions according to the procedure reported previously [22]. The

    aluminate solution was prepared by dissolving the appropri-

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    Table1

    ConditionsforzeoliteNaAmembranepreparationbyhydrothermalsynthesis

    Reactorconfiguration

    Compositionofthesynthesissolution

    (Al2O3:SiO2:

    Na2O:H2O:templates)

    T(K)

    Tim

    e(h)/cycles

    Support

    Seedingtechnique

    Seedsize(m)

    References

    Semi-continuous(AC)

    (1/41/16min1)

    1:1.8:3.9:273

    363373

    5/12

    -Al2O3innertube

    Brushseeding;C-Ffiltration

    2

    [24]

    Semi-continuous(AC)

    (1/131/25min1)

    1:1.8:3.9:273

    363

    5/1

    -Al2O3outertube

    Rubbing

    1

    [25]

    Centrifugalfield(VS)

    (100rpm)

    1:2:2:120400

    363373

    3/24

    -Al2O3innertube

    C-Ffiltration

    2,4

    [22]

    Centrifugalfield(VS)

    (5202520rpm)

    1:1.8:3.6:270

    373

    3/23

    -Al2O3innertube

    Brushseeding

    1

    [26]

    Dynamic(AC)(75rpm)

    1:5:55.1:1004

    .7

    323

    48/1

    ZrO2/Csheet

    [8]

    Static(VS)

    1:5:50:1000

    333

    24/1

    -Al2O3outertube

    C-Ffiltration

    0.33.0

    [22]

    1:2:3:200

    363

    24/1

    Hollowfiber

    [27]

    1:2:3:200

    363

    16

    24/13

    -Al2O3disk

    Dipcoating

    1

    [28]

    1:4.4:41.9:833.3

    353

    4/1

    TiO2disk

    UV(32W)

    [29]

    1:5:50:1000

    363

    16

    /1

    -Al2O3disk

    Dipcoating

    1

    [30]

    1:2:2:120

    373

    3.5/1

    Mullite,-Al2O3outertubes

    1

    [9]

    Static(VSwithdistiller)

    1:2:2:80144

    353373

    36

    /1

    -Al2O3outertube

    Rubbing;Dipcoating

    200mesh

    [6]

    Static(VS-MW

    2450MHz)

    1:2:3:200

    363

    54

    0min/1

    -Al2O3disk

    Rubbing

    NA

    [31]

    1:5:50:1000

    363

    15min/1

    Rubbing

    NA

    [32]

    Static(AC)

    1:9:80:5000

    353

    5/1

    -Al2O3disk

    Rubbing;Dipcoating

    0.7

    [33]

    Notation:Autoclave(AC);vesselopentoatmosphere(VS).

    Fig. 1. Scheme of the continuous flow system used for inner-side zeolite NaA

    membrane synthesis.

    ate amount of sodium aluminate powder supplied by Aldrich

    (Al2O3 = 53 wt.%, Na2O=43wt.%, Fe2O3 = 4 wt.%) in deion-

    ized water at 343 K under vigorous stirring in a closed flask. The

    silicate solution was prepared by dissolving a sodium silicate

    solution supplied by Aldrich (SiO2 =27wt.%,NaOH=14wt.%)

    in the remaining water under stirring. The silicate solution was

    added in three consecutive steps to the aluminate solution under

    vigorous stirring and the temperature was kept to 343 K.

    The scheme of the experimental set-up used for inner-side

    zeolite NaA membrane synthesis is depicted in Fig. 1. In general

    terms, the support, with the outer surface wrapped with Teflon

    tape to avoid crystal deposition, was placed inside a moduleimmersed in a temperature-controlled oilbath.The gelwas flown

    through the lumen of the tube by the action of gravity from a

    reservoir (2 L) preheated at 323 K and kept under mild stirring

    to a discharge vessel. A thermocouple positioned in the lumen

    of the tube was used to monitor any temperature fluctuation

    with gel introduction. In this work, the gel flow rate was fixed

    at a value in the range 1.54 mL min1 for all the synthesized

    membranes, which is expected not to sweep away the growing

    zeolite layer on the support inner surface. Thegel flow rate could

    be regulated by means of the height difference between the level

    of the gel in the reservoir and that at the outlet of the system.

    The height difference was progressivelyincreasedfrom an initialvalue of10 cm, in the beginning of thesynthesis to compensate

    the reduction of the gel level in the reservoir. At the end of the

    synthesis, the as-synthesized membranes were removed from

    the module, washed with boiling water for 1 h and dried in an

    oven at 373 overnight under vacuum (

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    zeolite layer. The dehydration performance of the as-synthesized

    membranes was first studied by vacuum PV for the separation of

    a 92:8 (w/w) ethanol/water mixture at 323 K with the permeate

    pressure kept

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    Fig. 2. XRD patterns of zeolite NaA layers grown onto the inner

    surface of seeded and unseeded tubular supports (T= 358 K; synthe-

    sis time= 67 h; gel flow rate= 1.54 mLmin

    1

    ). (a) Membrane ZA02,SWG=0.11mgcm2; (b) membrane ZA04, SWG = 0.13 mgcm2; (c) mem-

    brane ZA07, SWG= 0 mgcm2. The asterisk shows the location of rutile peaks

    from the support.

    secondary growth method shows higher and more definite peaks

    than that of membrane ZA07 prepared by in situ hydrothermal

    synthesis.Accordingly, the seeding of the support appears to pro-

    vide more crystalline layersdue to a more uniform andcontrolled

    growth of the zeolitic material.

    Fig. 3 shows some SEM micrographs of membranes ZA02,

    ZA04 and ZA07. The inspection of the top view micrographs

    of these membranes (see Fig. 3a1c1) reveals in all cases the

    presence of well-intergrown layers constituted by a randomlyoriented distribution of cubic and truncated-side cubic crys-

    tals. In good keeping with the XRD patterns plotted in Fig. 2,

    the differences in surface morphology observed for membrane

    ZA07 (Fig. 3a1) compared to membranes ZA02 and ZA04

    (Fig. 3a1b1) might be attributed to the presence of amorphous

    material on the layer. Fig. 3a2c2 show that the membranes con-

    sist of three layers: (1) synthesized zeolite layer, (2) intermediate

    titania layer and (3) bulk support constituted by large crystals

    that generates a macroporous array of7m mean pore size.

    In all cases, the thickness of the zeolite layer lies in the range

    1020m and increases with the synthesis time. The seeding of

    the support does not seem to exert an effect on layer thickness,

    in agreement to what is observed when preparing membranes inthe semi-continuous system.

    3.3. PV performance of the as-synthesized membranes

    The results of the PV tests carried out on the as-synthesized

    membranes towards the dehydration of ethanol/water mixtures

    are summarized in Table 3. For comparison, Table 3 also includes

    some reported data concerning the PV performance of some

    membranes synthesized under a centrifugal field and in a semi-

    continuous system. As can be seen, in the optimal synthesis

    conditions, a continuous flow system provides membranes with

    excellent selectivities and high total fluxes. A stability test car-

    Table 3

    PV performance of the membranes prepared in the continuous flow system in

    comparison with those reported in our previous literature

    Membrane Synthesis technique PV resultsa

    Selectivity

    (W/E)

    NT (kg m2 h1)

    ZA01

    Continuous flow system

    51 0.93ZA03 1091 0.76

    ZA04 495 1.16

    ZA05 8538 0.89

    ZA08 160 0.72

    ZA09 76 0.97

    ZA10bSemi-continuous system

    2444 0.48

    ZA11b 1050 0.48

    ZA12cCentrifugal field

    502 0.62

    ZA13c 294 0.32

    ZA14 Batch synthesis 1.50

    a PV conditions: feed pressure, 13bar; feed water fraction, 89wt.%; T,

    323 K; permeate pressure, 13mbar.

    b From ref. [15]renewal rate: (at a) 1/7min1; (at b) 1/4min1; (at c) twosynthesis cycles; -Al2O3 support.

    c From ref. [17]rotational speed, 100rpm; (at c) three synthesis cycles;

    -Al2O3 support.

    ried out for membrane ZA05 (see Fig. 4) reveals that this

    membrane preserves its PV performance for at least 100 h of

    continuous operation.

    It should be noted that the fluxes for the membranes prepared

    in this work are ca. twice the value that can be obtained for

    membranes synthesized under a centrifugal force field and in a

    semi-continuous synthesis system (see Table 3). This result is

    consistent with the reduction up to half of the layer thickness forthe membranes prepared in a continuous flow system compared

    to those prepared with the other two aforementioned techniques.

    In addition, these fluxes are as high as the best values reported

    in the literature for the PV separation of ethanol/water mixtures

    using both flat and inner-/outer-side zeolite NaA membranes

    at the same temperature and feed composition (see Table 4 for

    comparison) and are comparable with those that can be obtained

    with commercial zeolite NaA membranes [41,42].

    Fig.5 showsacorrelationbetweentheN2 permeanceand both

    the total flux and water/ethanol selectivity for the membranes

    listed in Table 2. As expected, the water/ethanol selectivity is

    reduced with the N2 permeance, while the total flux across the

    membrane shows the opposite trend. The membranes are onlyable to separate ethanol/water mixtures efficiently when their

    N2 permeance is

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    Fig. 3. SEM micrographs of tri-layered membranes ZA02, ZA04 and ZA07 grown on asymmetric TiO2 supports. Top views, a1c1; cross-sections, a2c2. Synthesis

    conditions as in Fig. 2.

    number of gel pulses in the lumen of the support using the semi-

    continuous system seems to make it more difficult to prevent the

    membranes from defect formation, thus requiring thicker layers

    to achieve a similar PV performance.

    3.4. Effect of feed composition and temperature on the PV

    performance: role of intercrystalline domains

    Fig. 6 plots the effect of the feed composition on the total

    flux and water/ethanol selectivity at low feed water fractions

    (210 wt.%) for membrane ZA05 prepared in a continuous flow

    system and for membranes ZA11ZA13 prepared using either

    a semi-continuous synthesis system or in the presence of a cen-

    trifugal field (see Table 3). As can be seen in Fig. 6a, the total

    flux shows a linear increase with the water composition or water

    activity in the feed for all the membranes, as expected on the

    basis of the strong hydrophilic character of zeolite NaA. Given

    the trends shown in Fig. 6a, the surface diffusivities of water at

    zero coverage can be calculated using an adsorptiondiffusion

    model based on the MaxwellStefan diffusion theory as was

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    Table 4

    PV performance of zeolite NaA membranes towards dehydration of ethanol/water mixtures

    Thickness (m) Support Water in feed (wt.%) T(K) Selectivity (W/E) Flux (kg m2 h1) Reference

    1020 TiO2 tube (i) 10 323 8500 0.81.0 This study

    30 -Al2O3 tube (i) 8 323 600 0.50 [22]

    2030 -Al2O3 tube (i) 8 323 >10000 0.50 [24]

    10 -Al2O3 tube (o) 10 398 3600 3.80 [25]

    7 -Al2O3 tube (i) 9 366 130 2.50 [26]NA ZrO2/C sheet 10 323343 9001000 0.160.18 [8]

    3.5 TiO2 disk 5 318 >10000 0.86 [29]

    10 Mullite tube (o) 10 323 >10000 0.77 [9]

    30 -Al2O3 tube (o) 10 323 1700 0.79 [6]

    4 -Al2O3 disk 10 303 10000 1.00 [33]

    NA Mullite tube (o) 5 298 >10000 0.68 [37]

    30 Mullite tube (o) 10 333 1000 1.20 [7]

    5 SS tube (o) 10 313 180 0.079 [38]

    7 -Al2O3 disk 10 298 3000 0.072 [39]

    10 -Al2O3 disk 10 333 >10000 0.57 [19]

    56 -Al2O3 tube (i) 5 323 >10000 1.50 [40]

    Notation: Outer tube (o); inner tube (i); not available (NA).

    Fig. 4. Water/EtOH (W/E), selectivity () and flux () as a function of time

    for membrane ZA05. PV conditions as in Table 3.

    outlined in a previous work[43]

    Sw(0) =NSTYwZA

    SqMMwKSwaw,LP0w

    (1)

    where the activity coefficients have been estimated by the

    UNIFAC method [44] and a value of 104 Pa1 has been

    considered for the adsorption constant of water, KSw. In thepresent calculations, the contribution of the support to the over-

    all mass transfer has been omitted, since it has been found

    to be

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    Fig. 6. Evolution of (a) total flux and (b) water/ethanol selectivity with water feed composition for membranes: (a) ZA5 (), (b) ZA11 (), (c) ZA12 () and (d)

    ZA13 (). PV conditions as in Table 3. The straight and dashed lines refer to the trends observed for membrane ZA5 and for the set of membranes ZA11ZA13,

    respectively.

    the basis of their lower water/ethanol selectivities compared to

    those of membrane ZA05.

    Fig. 7 shows the effect of temperature on the water flux

    and selectivity for the set of membranes ZA03, ZA05, ZA11

    and ZA12. As expected, an Arrhenius trend of the water flux

    with temperature is observed for all the tested membranes (see

    Fig. 7a), with effective activation energies lying in the range

    3340 kJmol1. These values agree, within the limits of the

    experimental error, with those reported by Kondo et al. [9] (see

    Table 5). Taking into account all the contributions to water mass

    transfer in the PV process according to an adsorptiondiffusion

    model [43], the effective activation energy of water includes the

    following contributions:

    ESw,eff= ESw +H

    w + RA (2)

    where Ew is the activation energy for water surface diffusion,

    Hw the adsorption enthalpy of water on zeolite NaA andparameter A belongs to the Antoine equation that accounts for

    the evolution of saturation vapor pressure with the temperature

    (A =5300K1 for water in the temperature range 293363 K).

    Taking a value of43kJ mol1 for the adsorption enthalpy

    of water [43], the computed activation energy of water found

    in this study approaches the effective activation energy val-

    ues (note that RA = 44.06 kJ mol1Hw =43kJmol1!!).

    Therefore, the activation energy of water diffusion falls into the

    interval 3340 kJ mol1, which compares well with the value

    reported by Zhu et al. [45] from the separation of water/N2mixtures using zeolite NaA membranes.

    Regarding the evolution of the water/ethanol selectivity with

    the temperature at low water fractions and in the tempera-

    ture range 303363 K (see Fig. 7b), a maximum appears to be

    observed at 325 K for the best quality membranes, namely

    membranes ZA03 and ZA05 prepared in the continuous flow

    system. However, for membranes ZA11 and ZA13, a posi-

    tive trend of the selectivity with the temperature seems to be

    observed. In agreement with the above stated considerations

    dealing with the role of intercrystalline domains, the discrepancy

    between both trends might be ascribed to the higher contribution

    of large defects in the latter membranes. For these membranes,

    when operated at low feed water fractions, a temperature raise

    might enhance water diffusion acrossthe zeolite layer, thus com-

    pensating to a certain extent the preferential mass transfer of

    ethanol through large defects and therefore giving rise to anincrease in the membrane selectivity.

    More insight into the effect of large intercrystalline pores in

    the PV performance in zeolite NaA membranes can be gained

    by comparing their ability towards dehydration of short- and

    long-chain primary alcohols. Fig. 8 plots the evolution of the

    total flux and selectivity towards water separation of membrane

    ZA13 with the length of chain of the primary alcohol in the

    liquid mixture at low water fractions (2.5 and 4.5 mol%) and at

    323 K. As can be seen, while the total flux appears to be only

    Fig. 7. Evolution of (a) total flux and (b) water/ethanol selectivity with temperature for membranes: (a) ZA3 (), (c) ZA5 (), (b) ZA11 () and (d) ZA13 (). PV

    conditions as in Table 3. The straight and dashed lines refer to the trends observed for membranes ZA3 and ZA5 and for membranes ZA11ZA13, respectively.

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    M. Pera-Titus et al. / Separation and Purification Technology 59 (2 008) 1411 50 149

    Table 5

    Effective activation energies of water flux across zeolite NaA membranes

    Membrane Synthesis technique Xw range (wt.%) Trange (K) Ew,eff (kJmol1)a Reference

    ZA03Continuous flow system

    4.34.7

    303363

    34 1 This study

    ZA05 3.94.2 39 2 This study

    ZA11 Semi-continuous 2.559.0 40 4 This study

    ZA13 Centrifugal field 4.85.2 33 3 This study

    Zeolite NaA (outer-side) Static batch 10100313353

    35 [9]

    Zeolite NaA (flat) Static batch 10 5152 [7]

    a Typical error for a probability level of 95%.

    Fig. 8. Evolution of (a) total flux and (b) water/alcohol selectivity with the number of carbon atoms in the alcohol for membrane ZA13. Feed composition: ( )

    xw = 2.5mol% and () xw = 4.5 mol%. Other PV conditions as in Table 4. The straight lines refer to the trends observed.

    slightly affected by the length of chain of the alcohol, except for

    methanol, whose molecule ressembles more to that of water, the

    selectivity becomes strongly promoted. As has been outlined by

    Okamoto et al. [6] when studying the performance of zeolite

    NaA membranes towards the dehydration of methanol, ethanol,

    acetone and DMF mixtures, the selectivity of the membranes is

    promoted as the ability of the solvent to adsorb on zeolite NaAis reduced. Moreover, despite the presence of a certain number

    of large defects in the zeolite layer, their contribution to mass

    transfer is compensated by that within zeolite pores due to their

    stronger hydrophilic character, which favors the adsorption of

    smaller molecules.

    4. Conclusions

    A continuous flow system has been presented in this work

    that allows the synthesis of good quality zeolite NaA mem-

    branes on the inner-side of tubular ceramic supports. Compared

    to other reported methods for inner-side zeolite NaA membranesynthesis (i.e. semi-continuous and centrifugal force field), this

    technique is economically advantageous, since only the gel fill-

    ing the lumen of the support is refreshed along the synthesis.

    Taking into account that this technique can be easy to scaled-up,

    it constitutes a promising option for inner-side zeolite mem-

    brane synthesis at large scale and for zeolite NaA synthesis in

    multichannel tubes and capillaries. The selectivities and fluxes

    of the membranes prepared using this technique approach the

    best values reported in the literature for inner-side zeolite NaA

    membranes. This latter aspect is especially promising in terms

    of membrane area economy. Notwithstanding the presence of a

    large number of defects, zeolite NaA membranes can be used

    confidently in PV applications that involve dehydration of heavy

    non-adsorbing species, like 1-butanol and 1-pentanol.

    Acknowledgements

    The authors would like to express their gratitude to the Span-

    ish Ministry of Education and Science for financial support(projects PPQ2000-0467-P4-02 and CTQ2005-08346-C02-01).

    The comments of Dr. Sylvain Miachon have been very useful in

    the preparation of this paper.

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