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Chen and Kumar -2011- Sol-gel TiO2 in Self-Organization Process- Growth, Ripening and Sintering

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Sol–gel TiO 2 in self-organization process: growth, ripening and sintering Hsueh-Shih Chen* and Ramachandran Vasant Kumar Received 23rd September 2011, Accepted 1st December 2011 DOI: 10.1039/c2ra00782g TiO 2 nanoparticles were synthesised by a self-organization method using a continuous water vapour hydrolysis system without mixing. Formation of TiO 2 particles was based on pure colloidal interactions of hydrolyzed alkoxide molecules generated at the interface between titanium alkoxide solution and water vapour. The effect of ethanol was proved to increase aggregation and packing of primary particles, leading to a significant size enlargement of secondary particles in a post annealing process above 500 uC. A new model to describe sol–gel TiO 2 growth has been proposed, which considers the formation of secondary particles to be the result of nucleation of oversaturated primary particles, while the primary particles are the result of irreversible oligomerization of Ti oxo molecules. Introduction The sol–gel process offers many advantages for preparing oxide materials such as low cost, high purity and a wide variety of morphologies. The synthetic process of sol–gel materials in general involves a wet-chemical process to form a precursor sol or gel solution, which can be deposited on a substrate, followed by a post heat treatment to convert the amorphous precursor into crystalline particles or thin films. 1 Typical sol–gel processing of TiO 2 nanocrystals includes the hydrolysis of titanium alkoxide by water, which can react with alkoxyl groups, generating fully or partially hydrolyzed (OR) 42n Ti(OH) n molecules. The (par- tially) hydrolyzed molecules can react with each other or with other alkoxides or hydroxides, forming an oxo bridge (–O–) between Ti atoms (oxolation) together with an elimination of a water molecule, as shown below. Briefly, the hydrolysis of Ti alkoxides leads to hydroxyl groups, which is able to change Ti(OR) 4 to Ti–O–Ti via the condensation (i.e., olation or oxolation process), and produces Ti-oxo-alkoxy or polyoxotita- nate molecular clusters, for example, [Ti 12 O 16 ](OPr i ) 16 , [Ti 11 O 13 ](OPr i ) 18 and Ti 16 O 16 (OEt) 32 . 2 The Ti–oxo–alkoxy clus- ters can further grow to larger denser nanoparticles (NPs) dispersing in a solution (i.e. sol). The sol particles can further associate with each other via collisions after aging for a certain period of time and thus form bigger isolate gel particles, gel network, or porous films depending on experimental conditions. For the hydrolysis of titanium alkoxides, it is known that the amount of water strongly affects the morphology of final products. According to the molar ratio of water to titanium alkoxides (h), the sol–gel processing of TiO 2 may be classified into two regimes; low H 2 O/Ti molar ratio (h , 10) and high H 2 O/Ti molar ratio (h . 10). At low h values, spherical TiO 2 particles with relatively uniform size about 0.5–1 mm are obtained. 3 At high h values, large aggregates of TiO 2 rapidly precipitate because fast hydrolysis leads to unstable colloids. The aggregates can be separated to nano-sized particles (,100 nm) at moderately elevated temperature by the so-called chemical peptization process using acids such as nitric acid. 4 Alcohol is often served as a solvent to slow down the hydrolysis reaction of Ti alkoxides. 5 However, effect of alcohols on the morphology and microstructure is still an argument. Park et al. reported that n-propanol acted as a dispersant for TiO 2 particles in the thermal hydrolysis of titanium tetrachloride in a mixture of n-propanol and water. 6 They found that without any n-propanol TiO 2 particles were small and agglomerated. With addition of n-propanol (n-propanol/water = 3), TiO 2 particles became uniform in size and discrete. On the other hand, Vorkapic et al. found that alcohols caused the aggregation of TiO 2 primary particles, which were synthesised via hydrolysis– condensation of alkoxides at a high h value. 7 They found that chemical factors relating to the hydrolysis and the condensation (e.g. temperature, the length of alkoxyl of alkoxide…) affected the primary particle size rather than the final particle size. Also, alcohols had a negative effect on the peptization. The smallest secondary particles (about 20 nm) were obtained without any alcohol modification. Thus, they suggested that formation of TiO 2 particles was controlled by the colloidal interactions between primary particles. Moreover, it has been reported that ethanol could cause the amorphization of TiO 2 particles. 8 Hague et al. prepared TiO 2 by hydrolyzing an isopropoxide–ethanol mixture with a large excess of water (h = 165). Before calcination, the samples were found to be the anatase. But the samples became amorphous after they were rinsed twice by ethanol. The authors suggested that this crystalline-to- amorphous transformation was possibly due to the fact that the hydrolysis reaction was slightly reversed by rinse of ethanol. Although the sol–gel process is widely applied for preparing TiO 2 , the growth mechanism of the sol–gel TiO 2 is thought to be complicated and experimental factors such as alcohol modifiers Department of Materials Science and Metallurgy, University of Cambridge, Pembroke Street, Cambridge, CB2 3QZ, U.K. E-mail: [email protected] RSC Advances Dynamic Article Links Cite this: RSC Advances, 2012, 2, 2294–2301 www.rsc.org/advances PAPER 2294 | RSC Adv., 2012, 2, 2294–2301 This journal is ß The Royal Society of Chemistry 2012 Published on 19 January 2012. Downloaded on 11/09/2013 07:46:52. View Article Online / Journal Homepage / Table of Contents for this issue
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  • Solgel TiO2 in self-organization process: growth, ripening and sintering

    Hsueh-Shih Chen* and Ramachandran Vasant Kumar

    Received 23rd September 2011, Accepted 1st December 2011

    DOI: 10.1039/c2ra00782g

    TiO2 nanoparticles were synthesised by a self-organization method using a continuous water vapour

    hydrolysis system without mixing. Formation of TiO2 particles was based on pure colloidal

    interactions of hydrolyzed alkoxide molecules generated at the interface between titanium alkoxide

    solution and water vapour. The effect of ethanol was proved to increase aggregation and packing of

    primary particles, leading to a significant size enlargement of secondary particles in a post annealing

    process above 500 uC. A new model to describe solgel TiO2 growth has been proposed, whichconsiders the formation of secondary particles to be the result of nucleation of oversaturated primary

    particles, while the primary particles are the result of irreversible oligomerization of Ti oxo molecules.

    Introduction

    The solgel process offers many advantages for preparing oxide

    materials such as low cost, high purity and a wide variety of

    morphologies. The synthetic process of solgel materials in

    general involves a wet-chemical process to form a precursor sol

    or gel solution, which can be deposited on a substrate, followed

    by a post heat treatment to convert the amorphous precursor

    into crystalline particles or thin films.1 Typical solgel processing

    of TiO2 nanocrystals includes the hydrolysis of titanium alkoxide

    by water, which can react with alkoxyl groups, generating fully

    or partially hydrolyzed (OR)42nTi(OH)n molecules. The (par-

    tially) hydrolyzed molecules can react with each other or with

    other alkoxides or hydroxides, forming an oxo bridge (O)

    between Ti atoms (oxolation) together with an elimination of a

    water molecule, as shown below. Briefly, the hydrolysis of Ti

    alkoxides leads to hydroxyl groups, which is able to change

    Ti(OR)4 to TiOTi via the condensation (i.e., olation or

    oxolation process), and produces Ti-oxo-alkoxy or polyoxotita-

    nate molecular clusters, for example, [Ti12O16](OPri)16,

    [Ti11O13](OPri)18 and Ti16O16(OEt)32.

    2 The Tioxoalkoxy clus-

    ters can further grow to larger denser nanoparticles (NPs)

    dispersing in a solution (i.e. sol). The sol particles can further

    associate with each other via collisions after aging for a certain

    period of time and thus form bigger isolate gel particles, gel

    network, or porous films depending on experimental conditions.

    For the hydrolysis of titanium alkoxides, it is known that the

    amount of water strongly affects the morphology of final

    products. According to the molar ratio of water to titanium

    alkoxides (h), the solgel processing of TiO2 may be classified

    into two regimes; low H2O/Ti molar ratio (h , 10) and high

    H2O/Ti molar ratio (h . 10). At low h values, spherical

    TiO2 particles with relatively uniform size about 0.51 mm are

    obtained.3 At high h values, large aggregates of TiO2 rapidly

    precipitate because fast hydrolysis leads to unstable colloids. The

    aggregates can be separated to nano-sized particles (,100 nm) at

    moderately elevated temperature by the so-called chemical

    peptization process using acids such as nitric acid.4

    Alcohol is often served as a solvent to slow down the

    hydrolysis reaction of Ti alkoxides.5 However, effect of alcohols

    on the morphology and microstructure is still an argument. Park

    et al. reported that n-propanol acted as a dispersant for TiO2particles in the thermal hydrolysis of titanium tetrachloride in a

    mixture of n-propanol and water.6 They found that without any

    n-propanol TiO2 particles were small and agglomerated. With

    addition of n-propanol (n-propanol/water = 3), TiO2 particles

    became uniform in size and discrete. On the other hand,

    Vorkapic et al. found that alcohols caused the aggregation of

    TiO2 primary particles, which were synthesised via hydrolysis

    condensation of alkoxides at a high h value.7 They found that

    chemical factors relating to the hydrolysis and the condensation

    (e.g. temperature, the length of alkoxyl of alkoxide) affected

    the primary particle size rather than the final particle size. Also,

    alcohols had a negative effect on the peptization. The smallest

    secondary particles (about 20 nm) were obtained without any

    alcohol modification. Thus, they suggested that formation of

    TiO2 particles was controlled by the colloidal interactions

    between primary particles. Moreover, it has been reported that

    ethanol could cause the amorphization of TiO2 particles.8 Hague

    et al. prepared TiO2 by hydrolyzing an isopropoxideethanol

    mixture with a large excess of water (h = 165). Before

    calcination, the samples were found to be the anatase. But the

    samples became amorphous after they were rinsed twice by

    ethanol. The authors suggested that this crystalline-to-

    amorphous transformation was possibly due to the fact that

    the hydrolysis reaction was slightly reversed by rinse of ethanol.

    Although the solgel process is widely applied for preparing

    TiO2, the growth mechanism of the solgel TiO2 is thought to be

    complicated and experimental factors such as alcohol modifiers

    Department of Materials Science and Metallurgy, University ofCambridge, Pembroke Street, Cambridge, CB2 3QZ, U.K.E-mail: [email protected]

    RSC Advances Dynamic Article Links

    Cite this: RSC Advances, 2012, 2, 22942301

    www.rsc.org/advances PAPER

    2294 | RSC Adv., 2012, 2, 22942301 This journal is The Royal Society of Chemistry 2012

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  • do not exhibit a similar effect on different synthetic systems. One

    of the reasons is that hydrolysiscondensation of Ti alkoxide and

    aggregation of monomers may occur simultaneously for a certain

    period, which leads to different morphologies and sizes of TiO2particles, and therefore affects the crystal growth of TiO2 in

    the post annealing process. Some growth models have been

    proposed to describe the growth of solgel TiO2. A general

    growth mechanism is that TiO2 primary particles generate from

    the nucleation of supersaturated monomers, which are produced

    by the hydrolysis of Ti alkoxides in the induction period.3 The

    TiO2 primary particles can continue the growth via additions of

    monomers and aggregation. This model assumes that monomers

    can accumulate and form embryos in a reversible process

    before they form stable nuclei when the critical concentration

    is reached. On the other hand, the growth mode of TiO2 particles

    is affected by the amount of water. For example, Oskam et al.

    obtained nanocrystalline TiO2 NPs from the hydrolysis of Ti

    alkoxide at a high water/Ti ratio, followed by peptization at

    85 uC.9 The average radius of primary particles increased linearlywith time, which was consistent with the predication made by the

    LifshitzSlyozovWagner (LSW) theory. They observed second-

    ary particles formed by epitaxial self-assembly of the primary

    particles with a size range 1.58 nm.

    In this report, we synthesised TiO2 by employing a water

    vapour hydrolysis system, in order to investigate the growth of

    solgel TiO2 NPs and the influence of the initial processing

    parameters such as alcohol on the morphology and microstruc-

    ture of TiO2 in the sintering process. In this design, no mixing is

    applied and the complexity of growth modes is simplified. The

    hydrolysis is caused by condensed water from vapour occuring at

    the interface between the alkoxide and water vapour phase,

    which has very low water/alkoxide ratio (y 1/700 for one secondvapour input). The sol particles form at the interface region and

    self-organise to gel particles via pure colloidal interactions. This

    design allows us to examine pure interactions between solgel

    particles excluding the effect of external mixing. Instead of

    considering that primary particles are from the nucleation of

    hydrolyzed monomers, a plausible model considering that TiO2secondary particles are from the nucleation of primary particles,

    which are from irreversible coalescence of monomers, is

    attempted to qualitatively describe to the growth of solgel TiO2.

    Experimental

    Materials

    Titanium(IV) tetra-isopropoxide (TTIP, 97%) and absolute

    ethanol (analytical reagent grade) were purchased form

    Aldrich. All reagents were used without any further purification.

    Doubly distilled water was used to initiate the hydrolysis and the

    condensation process.

    Synthesis of TiO2 by general approach

    5 ml absolute ethanol was first used to modify TTIP (5 ml) using

    magnetic stirring for 20 min in an argon atmosphere. Then, 5 ml

    doubly distilled water was slowly added into the mixture of

    ethanol and TTIP at room temperature to form a sol solution.

    The molar ratio of water/TTIP is 15.4. Gel solution was obtained

    by aging the sol for 18 h at room temperature. Annealing process

    was carried out at 150 uC for 1 h, followed by 600 uC for 2 h witha heating rate of 5 uC min21. White crystalline TiO2 powder wereobtained after the annealing process.

    Synthesis of TiO2 by vapour hydrolysis

    An experimental system deigned to synthesise TiO2 via slow

    hydrolysis of TTIP by water vapour is shown in Fig. 1(a). The

    water vapour was generated by heating water at 70 uC (reservoirA) and carried by argon (99.9%) into reservoir B containing

    TTIP kept at room temperature. The input rate of water vapour

    was controlled by the flow rate of argon. The amount of water

    input was estimated by the weight of water accumulated in

    the reservoir C. Plastic pipes connecting each reservoir were

    wrapped with aluminium foils to prevent water vapour from

    condensation. In order to exclude the effects of stirring on the

    formation and aggregation of particles, no stirring was applied

    to the system throughout the process. As the TTIP was kept at

    room temperature, the water vapour was expected to condense

    to liquid as it contacted the TTIP surface. Thus, the hydrolysis

    and the condensation would occur at the near surface region of

    the TTIP. A typical input rate of water vapour was set at 5.21 61026 mol s21. The molar ratio of water/TTIP was about 1/700

    for the vapour input lasting a second. The overall input time

    (aging time) was eight hours. A white precipitate eventually

    formed at the bottom of the reservoir. The product was then

    milled to a powder for subsequent characterisation. Pure TTIP

    and alcohol-modified TTIP were used as precursors. For

    investigating the structure and morphology of samples in the

    annealing process, pure TTIP or an ethanolTTIP mixture

    (volume ratio = 0.1/1) was used. The overall reaction time was

    8 h. Samples were placed into a furnace and taken out at a

    desired temperature, as shown in Fig. 1(b).

    Characterisation

    The surface morphology of TiO2 was investigated by field

    emission gun scanning electron microscopy (SEM). The average

    size of particles was estimated according to SEM images for

    more than 130 particles using computer software (ImageJ).

    Powder X-ray diffraction (XRD) was employed to study the

    crystallography of samples. The crystallite size of TiO2 is

    estimated by FWHM according to Scherrers formula, D =

    (0.9 l)/(b1/2 coshB), where D is the average grain size, l is the

    Fig. 1 (a) Experimental design of vapour hydrolysis. (b) Evolution of

    the microstructure and the morphology of samples in the annealing

    process. Red dots indicate that samples were taken out from a furnace at

    100, 200, 300, 400, 500, 600, and 600 uC (15 h).

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  • wavelength of Cu Ka (= 1.5405 A), b1/2 is the FWHM (full width

    at half maximum), and hB is the diffraction angle.

    Results and discussion

    TiO2 synthesised by general approach

    As-prepared TiO2 sol was a white suspension. After aging, larger

    white gel particles formed at the bottom of the vessel if no

    stirring was applied. Dried TiO2 gel samples have no crystal-

    linity, showing that highly crystalline TiO2 would not form at

    room temperature without heat treatment, as shown in the XRD

    data in Fig. 2 (curve a). The TiO2 crystalline phase is generated

    after a heat treatment is carried out, shown in Fig. 2 (curve b).

    The XRD data indicate that annealed TiO2 powders have an

    anatase phase with average grain size of 30.1 nm. It also shows

    that a small amount of anatase TiO2 transforms into the rutile

    phase. SEM images (Fig. 3(a)) show that the morphology of

    TiO2 particles is oval-shaped and coalesced and has a mean size

    about 1.02 mm 36%. A high magnification image in Fig. 3(b)

    shows that the TiO2 is made up of secondary particles composed

    of primary nanoparticles with diameters of 33.2 nm 25%.

    Note that the primary particle size is close to the average grain

    size estimated from the XRD data, inferring the majority of the

    primary particles are nearly single crystalline. The above SEM

    and XRD results suggest that amorphous primary particles first

    generate in the solgel process and then aggregate into secondary

    particles. Since there is no existence of TiO2 crystalline phases

    before the annealing process, the formation of the primary

    particles in this case may not be mixed with the conventional

    nucleation-growth process of crystalline materials.

    The growth of TiO2 from the general solgel process is

    schematically shown in Fig. 4(a). When water is introduced into

    the TTIP solution, Ti-oxo (or Ti-oxo-alkoxy) molecular clusters

    are generated through the hydrolysiscondensation reaction of

    the alkoxides and form particulate sol particles. The primary

    particles may be viewed as the coalesced Tioxo molecular

    clusters generated from hydrolyzed Ti alkoxides. Thus, the size

    of the primary particle should be dependent on the hydrolysis

    condensation and chemistry of the solution. For the secondary

    particles, their average size is related to the dimension of the gel

    particles that is determined by the interaction between colloidal

    particles.7

    TiO2 powders synthesised from the ordinary solgel process at

    room temperature generally show a broad amorphous XRD

    peak, which is actually contributed by numerous diffraction data

    from Ti-oxo molecular clusters and domains in a microscopic

    viewpoint. The Ti-oxo molecular clusters randomly connect with

    each other and could not form periodic structures in a fast

    hydrolysiscondenstation process. In some cases, crystalline

    materials may be obtained by standing a solution of Tioxo

    molecular clusters having a well-defined structure at room or

    Fig. 2 XRD of TiO2 synthesised by a standard solgel method (volume

    ratio TTIP/ethanol/water = 1/1/1). As-prepared sample (curves a) and

    sample annealed at 600 uC for 2 h (curve b).

    Fig. 3 SEM images of TiO2 particles synthesised by a normal solgel

    method (volume ratio TTIP/ethanol/water = 1/1/1) at pH = 7. (a) 30006.(b) 70 0006.

    Fig. 4 (a) Normal solgel process of TiO2 particles. (b) TiO2 prepared

    by solgel process in the vapour hydrolysis design.

    2296 | RSC Adv., 2012, 2, 22942301 This journal is The Royal Society of Chemistry 2012

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  • elevated temperature for a longer time (e.g., couple of days). In

    that case, stable Ti-oxo molecular clusters act as building blocks

    being able to periodically assemble in a slow assembly process.

    So the crystalline phase could be recorded by single crystal

    XRD.2c,2d

    TiO2 synthesised by vapour hydrolysis

    Fig. 5 gives SEM images of a TiO2 sample prepared by

    hydrolyzing pure TTIP in the vapour hydrolysis design. The

    sample dried at room temperature contains secondary particles,

    which are composed of primary particles. This result is similar to

    those samples prepared by the standard solgel method. In the

    experimental design of the vapour hydrolysis system, water

    vapour is continuously transported into a vessel containing

    TTIP. The vapour is condensed into liquid H2O at the interface

    between the atmosphere and the TTIP surface. For a rate of

    5.21 6 1026 mol s21, the molar ratio of water/TTIP is about1/700 for a second of the water vapour input. The water would

    not largely accumulate since reaction between water and TTIP is

    very fast. The characteristic time of the hydrolysiscondensation

    of TTIP precursor reported is in the range of tens of

    milliseconds.10,11 So it is expected that reaction between water

    and TTIP mainly occurs at the interface region, where Ti-oxo-

    alkoxy molecular clusters generate and migrate into the solution

    due to the Brownian interaction and gravity, as shown in region I

    Fig. 4(b). The generated Ti-oxo-alkoxy clusters would only

    contain single or few Ti atoms due to a limited water input. Some

    stable clusters TinOm(OiPr)4n-2m-l(OH)l, with n = 3, 11, 12, and

    17, have been found in the solutions containing TTTIP at low

    hydrolysis ratio h = [Water]/[Ti] , 1.12 The smallest stable Ti-

    oxo-alkoxy cluster observed was Ti3-oxo clusters synthesised at

    h y 0.05.13 Larger Ti-oxo clusters and nanoparticles wereobtained at higher h values (. 0.7).10

    In the vapour hydrolysis system, formations of sol and gel

    particles are based on self-organisation since there is no mixing

    applied in this system. So the collisions among the particles

    instead dominate the growth. The Ti-oxo-alkoxy molecular

    clusters are first generated at the TTIP surface where the

    hydrolysis and condensation take place. Ti-oxo-alkoxy clusters

    could grow into larger sol particles via collisions. This event then

    produces a colloidal solution (i.e. sol process, region I). If the sol

    particles link to each other, large gel particles are produced and

    fall down from near the surface region due to gravity. The

    formation of secondary particles is caused by the aggregation

    of the primary particles shown in region III in Fig. 4(b).

    Consequently, the sol and gel particles are assigned to the

    primary and the secondary particles respectively. In addition, the

    definition of the term sol particle is somewhat confusing since

    its scale (several to tens of nm) overlaps with those of molecular

    clusters and of nanoparticles. Basically, sol particles may be

    viewed as large molecular clusters (e.g., polymers) with denser

    structures and equivalent to nanoparticles with either amor-

    phous or crystalline structures. Gel particles may be viewed as

    larger coalesced sol particles in the micron scale.

    Evolution of the morphology of TiO2 obtained by annealing

    samples at various temperatures is given in SEM images in

    Fig. 5. It shows that the TiO2 secondary particles have irregular

    shapes and no significant change in the morphology takes place

    below 500 uC. For samples annealed at 600 uC and 600 uC/15 h,sintering of the particles is observed. The primary particles

    coalesced and merged, as shown in Fig. 5 (images c and d). XRD

    data show that there is no crystalline phase for an as-prepared

    sample whereas the anatase appears at 100 uC (Fig. 6(a)). Theanatase is partly transformed into rutile after heating at 600 uCfor 15 h. The final product is a mixture of anatase and rutile, as

    shown in Fig. 6(a). Variations of the crystallite size, the primary

    particles, and the secondary particles, estimated from XRD data

    and SEM images, are presented in Fig. 7 The as-prepared

    primary and secondary particles at room temperature are 14 nm

    14% and 1.3 mm 28% respectively. The size does not

    significantly change for samples annealed at temperatures below

    Fig. 5 SEM images of TiO2 dried at room temperature (a), 500 uC (b),600 uC (c), and 600 uC for 15 h (d). Samples were prepared by vapour-hydrolyzing pure TTIP.

    Fig. 6 XRD of TiO2 annealed at temperatures from room temperature

    (R.T.) to 600 uC and 600 uC for 15 h. Samples were prepared by vapour-hydrolyzing pure TTIP (a) and ethanolTTIP mixture (b).

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  • 500 uC. The stability of the particles size below 500 uC isunderstandable; there is no significant sintering of TiO2 particles

    below 500 uC observed (melting point of TiO2 y 1840 uC) sothey are able to keep their original size. But at 600 uC theprimary and the secondary particles readily enlarge since the

    sintering causes grain growth. A slight decrease in size at 100 uCis ascribed to the removal of organic compounds that lead to

    some shrinkage and/or cleavage of the large particles.

    The grain size of TiO2, on the other hand, does not correspond

    to the size of the primary particles. Initially the grain size is

    4.5 nm and increases to 7.5 nm at 500 uC. Note that 7.5 nm is stillsmaller than the diameter of the primary particles. The grain

    enlargement may be caused by the crystallisation in the primary

    particles and/or sintering between the particles. In the present

    case, the grain growth below 500 uC would be caused by thecrystallisation in the primary particles rather than the sintering

    between the particles because the crystallisation of TiO2 is able to

    take place below 500 uC, while the sintering requires a highertemperature to overcome the inter-particle diffusion barrier. The

    sintering event could be observed when the temperature is equal

    to 600 uC, as shown in Fig. 7. Both of the primary particles andthe secondary particles enlarge, indicating inter-particle grain

    growth via necking occurs. Moreover, the grain size is nearly the

    same as the primary particle size, indicating that the primary

    particles are nearly single crystalline at 600 uC. A further heattreatment (600 uC for 15 h) for grain growth or coarseningoccurs via the sintering process between the primary particles, as

    shown in Fig. 5(d). The primary particles disappear and larger

    grains appear on the TiO2 secondary particles when heated at

    600 uC for 15 h. It is noted that the sintering mainly occursamong primary particles, which transform to a certain layered

    growth mode. The necking between the secondary particles is

    hardly seen in the present study. Based on the above results,

    crystal growth of TiO2 in the heat treatment process may be

    illustrated in Fig. 8. TiO2 crystallites nucleate in the matrix of the

    primary particles and further develop to larger grains with

    increasing temperature. When the annealing temperature is high

    enough, the primary particles become single crystalline. Further

    grain growth can continue via inter-particle coalescence caused

    by sintering of primary particles.

    Influence of ethanol on the morphology of TiO2

    Although alcohols, e.g. ethanol, have been widely used to dilute

    TTIP for reducing the hydrolysis rate, however, alcohols affect

    the solution chemistry and thus alter the self-organisation

    process of TiO2 particles. For the addition of ethanol to TTIP

    solution, a certain degree of the substitution for propoxy groups

    by ethoxy ones is expected. The substitution is reversible. For

    partially hydrolyzed polyoxotitanates, e.g. [Ti11O13](OPri)18,

    [Ti11O13](OPri)13(OEt)5 could exist after reacting with ethanol.

    2

    On the other hand, it has been shown that alcohols destabilise

    the colloidal solution and enhance the rate of re-aggregation

    because alcohols decrease the dielectric constant of the solvent

    that correlates with the zeta potential of TiO2.6,14 The degree of

    aggregation of the primary particles was found to increases with

    lengthening alkyl chain of alcohols when the TiO2 powders are

    re-dispersed in various alcohols, for example, the degree of

    aggregation: propanol . ethanol . methanol.

    The effect of ethanol on the particle morphology in the vapour

    hydrolysis system can be clearly examined. As shown in SEM

    images in Fig. 9, the morphology of TiO2 particles is largely

    Fig. 7 Size variations of TiO2 primary particles, secondary particles,

    and crystallites prepared by vapour-hydrolyzing pure TTIP.

    Fig. 8 Nucleation and growth of TiO2 in the solgel process.

    Fig. 9 SEM images of TiO2 particles synthesised by pure TIP and

    ethanolTTIP (volume ratio = 5/7). The samples were annealed at 150 uCfor an hour, followed by 400 uC for another hour with a heating rate of10 uC min21.

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  • changed by introducing ethanol to modify TTIP. Increasing the

    volume ratio of ethanol (TTIP : ethanol from 5 : 0 to 5 : 7)

    results in a denser packing for TiO2 secondary particles, implying

    that ethanol is beneficial to the coalescence of the primary

    particles. The secondary particles tend to be spherical in the

    presence of ethanol. The ethanol increases the surface tension

    of the secondary particles (if treating the primary particles as

    atoms), and causes a reduction of the surface area of the

    secondary particles. This inward force could be correlated to the

    inter-particle interaction for the primary particles, which pull

    inwards the secondary particles. The inter-particle interaction

    may be related to the surface functional groups (e.g. hydroxyl

    groups) and the zeta potential of TiO2 particles. Another

    possibility is that ethanol stabilized the TTIP so that the

    generation of the monomers and the primary particles are so

    slow that the stacking of the particles is improved, which leads to

    a dense structure.

    The evolution of the crystallinity and morphology of the TiO2crystallite, the primary particles, and the secondary particles

    from the hydrolysis of the ethanol-modified TTIP with respect to

    annealing temperature are shown by XRD (Fig. 6(b)) and in

    SEM images (Fig. 10). Variations of size of the primary particles

    and the crystallites are shown in Fig. 11(a). The change in size of

    the secondary particles is shown in Fig. 11(b). As-prepared TiO2from ethanolmodified TTIP is amorphous (curve R.T. in

    Fig. 6(b)). The TiO2 crystallites form at 100 uC and have a sizeof about 2.6 nm, which is much smaller than those from pure

    TTIP (about 4.5 nm), as shown in Fig. 11(a). This result shows

    that the ethanol has a negative effect on the crystallisation of

    TiO2 in the heating process. The ethanol molecules could offer

    coordinative and hydrogen bonding to the anatase TiO2surface.15 This ethanol coordination to Ti would offer a chemical

    stabilising effect on embryos and/or crystallites that delay the

    crystallisation and crystal growth and thus the crystallite size

    reduces. We have found that alcohols with longer alkyl groups

    significantly suppressed the crystallization of TiO2 (results will

    be published elsewhere).

    The crystallite enlarges with increasing temperature from 2.6,

    4.6, 6.0, 6.4, and 9.0 nm for samples annealed at 100, 200, 300,

    400, and 500 uC, respectively, compared with those preparedwithout ethanol (4.4, 4.8, 6.0, 6.3, and 8.1 nm for 100, 200, 300,

    400, and 500 uC respectively), implying that the ethanol effect isreduced at around 200 uC. For the primary particles preparedfrom ethanol-modified TTIP, similar to those from pure TTIP,

    they become nearly single crystalline at around 600 uC and

    Fig. 10 SEM images of TiO2 synthesised by vapour-hydrolyzing

    ethanolTTIP mixture (TTIP/ethanol = 1/0.1) annealed at room

    temperature (a), 500 uC (b), 600 uC (c), and 600 uC for 15 h (d).

    Fig. 11 Evolution of sizes of the TiO2 crystallite, primary particle, and

    secondary particle in the annealing process. (a) Variations of the

    crystallite size and the primary particle size. (b) Variation of the

    secondary particle size.

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  • enlarge readily after dwelling for 15 h. For the secondary

    particles, their average size has no significant change at lower

    annealing temperatures (100500 uC), but largely increases as theannealing temperature is above 500 uC. This event is similar tothose from pure TTIP; size of the secondary particles increases

    due to the sintering of the primary particle. As the secondary

    particles from ethanol-stabilised TTIP have densely packed

    primary particles, the densification is more feasible and thus the

    secondary particles enlarge faster than those from pure TTIP.

    Growth model of TiO2 secondary nanoparticles

    The general growth model of solgel TiO2 considers that primary

    particles are the result of nucleation of supersaturated hydro-

    lyzed monomers from hydrolysis of Ti alkoxides. In the

    induction period, monomers (e.g., Ti-oxo-alkoxy) generate due

    to the hydrolysis of alkoxides that increases the monomer

    concentration.16 When the monomer concentration reaches a

    critical level, nucleation occurs. The induction time is defined by

    the visual turbidity of reaction liquid and reflects the rate at

    which critical supersaturation is achieved.3 However, it was

    found that nanoparticles already generate and grow during the

    induction period in a dynamic light scattering study.17 So the

    induction time may not precisely reflect the formation of

    particles in the nanoscopic scale. On the other hand, accumula-

    tion of monomers in the induction period is not considered in

    some studies. As the Ti-O-Ti oxo bonds are very strong and

    condensation of hydrolyzed clusters is irreversible, Ti-oxo

    clusters enlarge through the reactions or additions with other

    Ti-oxo clusters.18 In the present case, Ti-oxo-alkoxy clusters

    generated at the TTIP surface are thought to connect with each

    other via the condensation reaction between metalOH groups

    and/or metalOR groups. The coalescence of Ti-oxo-alkoxy

    clusters towards denser/bigger primary particles is considered an

    irreversible process. Then, the primary particles drop down to

    the lower pure TTIP area due to their increasing weight. The

    surface of the primary particles could be deactivated because the

    hydroxyl groups on the primary particles could be converted to

    non-reactive alkyl chains by reacting with TTIP molecules. In

    this pure TTIP region, there is no external water molecules

    provided so the irreversible condensation between the primary

    particles surfaces could be effectively suppressed. Instead, the

    reversible coalescence process becomes dominant in the aggrega-

    tion of the primary particles. The stability of coalesced primary

    particles is determined by the GibbsThompson relationship, Cr= C0exp[(2cv)/(rkT)]. As there is no stirring in the present system,

    the primary particles randomly collide with each other in the

    solution due to Brownian motion and can result in a local

    concentration fluctuation. In this situation, some primary

    particles could coalesce to a meta-stable particle aggregate,

    which could either grow larger (forward process), or dissociate

    into individual primary particles (inverse process). Therefore, the

    aggregate of the primary particles would have the critical size at

    which the aggregate is stable. The process is somewhat like the

    conventional homogeneous nucleation process of crystals, where

    the number of the nuclei containing n monomers is given by the

    Boltzmanns distribution, Nn = N(n)exp[2DGn/(kT)], where N(n)

    is a function of n, k is Boltzmanns coefficient, T is temperature,

    and DGn is the activation energy, which is a function of the

    surface energy and the volume free energy. If the number of

    monomers (n) is much more than embryos, N(n) can be assumed

    a constant (N0), Nn = N0 exp[2DGn/(kT)]. The VolmerWeber

    theory predicts the nucleation rate of oversaturated vapour

    condensing to liquid.19 The nucleation rate is proportional to

    number of the embryos at the critical size and the condensation

    rate. The condensation rate of vapour is proportional to the

    surface area of an embryo (Ac) and the probability of a vapour

    atom liquidized on the embryo per unit area and time (P). I =

    AcPNn = AcPN0 exp[2DGn/(kT)]. The VolmerWeber theory

    assumes the process to be a quasi-steady state where the atoms

    are constantly introduced to the condensation system. The model

    also assumes that once the nuclei forms the particle will continue

    to enlarge. The predication made by the theory has been found

    to be consistent with the experimental results if the atoms are

    much more than the nuclei. According to the theory, the

    nucleation rate increases with increasing concentration of the

    vapour atoms. In a colloidal system, the monomer concentration

    strongly determines the nucleation and growth. Higher monomer

    concentration allows generation of the smaller nuclei generated

    according to the GibbsThompson relationship. Variation of

    monomer concentration also affects the size and size distribution

    of crystals.20 Higher monomer concentration prevents smaller

    particles from dissolution in the solution and diminishes the size

    broadening process (i.e. Ostwald ripening).

    Fig. 12 shows that the secondary particle size decreases with

    increasing vapour input rate. The average sizes of the secondary

    particles are 0.83 mm and 0.42 mm for vapour rates of 3.47 61026, and 8.68 6 1026 mol s21, respectively. The particle sizedistribution of the samples also decreases from 73.9 to 42.3%

    with increasing vapour input rate. Considering the smallest

    stable aggregate of the primary particles to be the nuclei of the

    secondary particles, the concentration of the primary particles

    can alter the size of the secondary particles according the above

    model. In the water vapour hydrolysis system, the vapour input

    leads to the hydrolysis of TTIP at the interface that continuously

    supplies the hydrolyzed molecules and the primary particles into

    the TTIP solution, where the quasi-steady state is able to

    establish if the generation and consumption of the primary

    particles reach a dynamic equilibrium situation. This process

    resembles the model of crystallisation. The addition of the

    primary particles onto the secondary particles may be based on

    Fig. 12 SEM images of TiO2 secondary particles produced by hydro-

    lyzing pure TTIP with vapour input rates of 3.47 6 1026 mol s21 (a) and8.68 6 1026 mol s21 (b).

    2300 | RSC Adv., 2012, 2, 22942301 This journal is The Royal Society of Chemistry 2012

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  • the reductions of the surface energy of the secondary particles.

    The secondary particle size therefore decreases with increasing

    the water vapour input rate.

    Coalescence of secondary particles

    Since the generation of the TiO2 secondary particles from the

    primary particles is similar to the material crystallization process,

    it is worth to check if there is a process similar to Ostwald

    ripening occurring in the crystallization process. Fig. 13 shows

    SEM images of the secondary particles (vapour rate = 5.21 61026 mol s21, TTIP/ethanol = 5/1) dried at 400 uC for 1 h, atwhich no sintering event occurs, proved in the above data.

    The secondary particles appear to combine with each other

    (Fig. 13(a)). The junction between the particles clearly shows

    that the combination is not caused by the sintering (necking)

    between the secondary particles (Fig. 13(b)) and appears to be

    the coalescence of the secondary particles. The coalescence

    would not be caused by the evaporation of solvents in the

    separation process of products because the products formed in

    the system were a solid precipitate in the bottom of the reaction

    vessel rather than a colloidal solution. Presumably, the

    combination of the secondary particles is caused by the

    coalescence between secondary particles in the solution. This

    event is similar to Ostwald ripening based on the difference in the

    solubility of larger and smaller crystals. The driving force of

    combination of the secondary particles in the present system

    would be relating to the surface functional groups and the zeta-

    potential of the secondary particles, which is under investigation.

    Conclusion

    TiO2 was prepared in a self-organization process with an ultraslow

    hydrolysis rate via a vapour hydrolysis system without mixing and

    in a normal solgel process for reference. Experimental results

    from both methods suggest that solgel TiO2 were secondary

    particles composed of primary particles, which were amorphous

    before an annealing process was performed. The crystalline

    anatase primary particles were generated at 100 uC and becamesingle crystalline at around 600 uC. The ethanol effect on solgelTiO2 was proved to aid aggregation and packing of TiO2 primary

    particles. This phenomenon leads to a size enlargement of the

    secondary particles when the post annealing temperature is above

    500 uC. A plausible model considering that TiO2 secondaryparticles are the result of the nucleation of the primary particles is

    attempted to qualitatively describe to the growth of solgel TiO2.

    Experimental results show that the secondary particles size

    reduces with increasing vapour input rate, which is consistent

    with the prediction of the growth model.

    References

    1 P. Periyat, F. Laffir, S. A. M. Tofail and E. Magner, RSC Adv., 2011, 1, 1794.2 (a) V. W. Day, T. A. Eberspacher, W. G. Klemperer and C. W. Park, J.

    Am. Chem. Soc., 1993, 115, 8469; (b) G. Fornasieri, L. Rozes, S. L.Calve, B. Alonso, D. Massiot, M. N. Rager, M. Evain, K. Boubekeurand C. Sanchez, J. Am. Chem. Soc., 2005, 127, 4869; (c) A. Senouci, M.Yaakoub, C. Huguenard and M. Henry, J. Mater. Chem., 2004, 14,3215; (d) J. V. Barkley, J. C. Cannadine, I. Hannaford, M. M. Harding,A. Steiner, J. Tallon and R. Whyman, Chem. Commun., 1997, 1653.

    3 (a) E. A. Barringer and H. K. Bowen, Langmuir, 1985, 1, 414; (b)E. A. Barringer and H. K. Bowen, Langmuir, 1985, 1, 420; (c) J. H.Jean and T. A. Ring, Langmuir, 1986, 2, 251; (d) J. L. Look and C. F.Zukoski, J. Am. Ceram. Soc., 1992, 75, 1587; (e) J. L. Look and C. F.Zukoski, J. Am. Ceram. Soc., 1995, 78, 21.

    4 Q. Xu, M. J. Gieselmann and M. A. Anderson, Polym. Mater. Sci.Eng., 1989, 61, 889.

    5 (a) H. S. Chen, R. V. Kumar and B. A. Glowacki, Mater. Chem.Phys., 2010, 122, 305; (b) H. S. Chen, R. V. Kumar and B. A.Glowacki, J. Sol-Gel Sci. Technol., 2009, 51, 102.

    6 H. K. Park, D. K. Kim and C. H. Kim, J. Am. Ceram. Soc., 1997, 80, 743.7 D. Vorkapic and T. Matsoukas, J. Am. Ceram. Soc., 1998, 81, 2815.8 D. C. Hague and M. J. Mayo, Nanostruct. Mater., 1993, 3, 61.9 G. Oskam, Z. Hu, R. L. Penn, N. Pesika and P. C. Searson, Phys.

    Rev. E, 2002, 66, 011403.10 R. Azouani, A. Soloviev, M. Benmami, K. Chhor, J. F. Bocquet and

    A. Kanaev, J. Phys. Chem. C, 2007, 111, 16243.11 J. Livage, M. Henry and C. Sanchez, Prog. Solid State Chem., 1988, 18, 259.12 (a) L. Rozes, N. Steunou, G. Fornasieri and C. Sanchez, Monatsh.

    Chem., 2006, 137, 501; (b) L. Rozes and C. Sanchez, Chem. Soc. Rev.,2011, 40, 1006.

    13 J. Blanchard, F. Ribot, C. Sanchez, P. Bellot and A. Trokiner, J.Non-Cryst. Solids, 2000, 265, 83.

    14 Y. T. Moon, H. K. Park, D. K. Kim and C. H. Kim, J. Am. Ceram.Soc., 1995, 78, 2690.

    15 (a) M. L. Shepotko and A. A. Davydov, Theor. Exp. Chem., 1991, 27,210; (b) S. Pilkenton, S. J. Hwang and D. Raftery, J. Phys. Chem. B,1999, 103, 11152.

    16 S. Tieng, R. Azouani, K. Chhor and A. Kanaev, J. Phys. Chem.C,2011, 115, 5244.

    17 A. Soloviev, D. Ivanov, R. Tufeu and A. V. Kanaev, J. Mater. Sci.Lett., 2001, 20, 905.

    18 M. Kallala, C. Sanchez and B. Cabane, Phys. Rev. E, 1993, 48, 3642.19 M. Volmer and A. Z. Weber, Phys. Chem., 1926, 119, 227.20 (a) X. Peng, J. Wickham and A. P. Alivisatos, J. Am. Chem. Soc.,

    1998, 120, 10937; (b) Y. Chen, E. Johnson and X. Peng, J. Am. Chem.Soc., 2007, 129, 10937; (c) H. S. Chen and R. V. Kumar, Cryst.Growth Des., 2009, 9, 5343; (d) H. S. Chen and R. V. Kumar, J. Phys.Chem. C, 2009, 113, 31; (e) H. S. Chen and R. V. Kumar, J. Phys.Chem. C, 2009, 113, 12236.

    Fig. 13 Association of the secondary particles (Ostwald ripening)

    before the coarsening of grains takes place. (a) A secondary particle

    merged with two other smaller secondary particles. (b) The cross section

    of the junction of a merged secondary particle.

    This journal is The Royal Society of Chemistry 2012 RSC Adv., 2012, 2, 22942301 | 2301

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