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Formation and structural transformations of nanoparticles in the TiO2-H2O system
O. V. Almjasheva
Saint Petersburg Electrotechnical University "LETI", ul. Professora Popova 5, 197376 St. Petersburg, Russia [email protected]
PACS 64.60.A-; 64.70.Nd DOI 10.17586/2220-8054-2016-7-6-1031-1049
Results thermodynamic analysis of processes in the TiO2 - H2O system in a wide range of variation of parameters determine the regions of sustainable existence of titanium dioxide in the form of rutile and anatase modification. The results of thermodynamic prediction on the possibility and conditions of sustainable existence of TiO2 with the rutile structure have been confirmed in experiments. Keywords: nanoparticles, TiO2, anatase, retile, thermodynamic analyses, structural transformations.
Received: 20 August 2016 Revised: 11 November 2016
1. Introduction
Despite the large number of works on formation, technology, structure and properties of compounds of different composition and structure in the TiO2-H2O system (for instance, see [1]), by now, there is no consensus on the stability, composition and structure of a significant number of compounds in this system. Such compounds include hydrated forms of titanium oxide. As mentioned in [2], such uncertainty exists even at the level of names for hydrated forms of TiO2. This is determined by the uncertainty of the composition of hydrated titanium dioxide that depends on the synthesis conditions and changes with time [2,3].
Data on the phase and chemical transformations in the TiO2-H2O system in the P — T-coordinates is quite limited by now. In particular, there is a diagram of transformations proposed in [4]. In addition to this work, there are a number of studies on phase transformations in titanium dioxide.
For instance, in [5-12], the structural states of titanium dioxide in a wide range of temperature and pressure changes summarized in [13] were studied. Along with the literature data, it includes the obtained data as P — T constitutional diagram for TiO2. Previous research [13], in addition to the rutile structure, which is equilibrium in a wide range of temperatures, showed the constitutional diagrams include a region for the existence of a high-pressure phase - TiO2-II, which has a structure similar to a-PbO2 [7]. In addition, these P — T-diagrams include P-T-regions for the existence of anatase and brookite titanium dioxide structures. However, in [13], it was noted that these phases were used as precursors for further studies of phase transitions in them with increasing temperature and pressure, i.e. reverse transition of rutile or TiO2 with a structure of a-PbO2 (TiO2-II) into the anatase or brookite structure was not observed. In further studies, this allowed many authors [1] to conclude that the phases of anatase and brookite were metastable. However, the unusual coincidence of the P — T-boundary of transition for anatase to rutile shown by different authors and marked on the P — T-constitutional diagram of titanium dioxide in [13] should be noted.
In [4], on the P — T-diagram, where the state of the substance was studied under hydrothermal conditions, i.e., actually - the state of TiO2 in the TiO2-H2O system, only the phase transition of anatase titanium dioxide to the rutile modification was observed. The absence of information on chemical transformation Ti(OH)4 ^TiO2+H2O in the diagram is apparently associated with the ambiguity of the information on the temperature of this transition. For example, in [15], it was stated that, during the thermal treatment of freshly prepared titanium gels without separating the solid phase from the mother liquor, crystallization of the amorphous gel of TiO2-nH2O with the formation of the anatase structure can begin at 60-100 °C. However, in [14], it was shown that the gel based on titanium dioxide is in the amorphous state up to ^200 °C, and the crystallization starts only when the temperature rises to 250-350 ° C. The crystallization onset temperature can be decreased by hydrothermal treatment of hydrated titanium dioxide [16].
The Ti(OH)4 composition is often ascribed only to freshly precipitated hydrated titanium dioxide. Freshly precipitated Ti(OH)4 (a-form) is subject to aging, which occurs rapidly, even at room temperature. The final product of aging, according to [2], is hydrated titanium dioxide (,-form), to which the conditional formula of
H2TiO3 is attributed. Heating accelerates its aging. It is supposed that ignition can induce not only dehydration, but also partial reduction of titanium dioxide. The progress of the latter process in air is in doubt due to the stability of titanium in the Ti (IV) oxidation state, which is mentioned in many works [1,3].
Along with a variety of structural modifications of hydrated titanium dioxide, there is morphological diversity of particles - from particles of isometric shape to particles of plate-like and nanotubular shapes, which are characteristic, for example, for H2Ti3O7 [17].
Thus, the uncertainty in the dependence of chemical, structural, and morphological transformations in the TiO2-H2O system on external conditions, especially the temperature, resulting from the analysis of the literature data, suggests the need for further study of these processes, including thermodynamic analysis of these transformations.
2. Thermodynamics of chemical and structural phase transformations in the TiO2-H2O system
The thermodynamic analysis of the conditions for the stable existence of titanium oxide, in which titanium has an oxidation state of less than 4+, conducted with the use of the Ivtanthermo thermodynamic database [18], depending on the temperature and oxygen partial pressure (Fig. 1), shows that the equilibrium existence of such compounds is thermodynamically possible only in a reducing atmosphere and at a sufficiently high temperatures. According to the results of thermodynamic calculations (Fig. 1), in a reducing atmosphere and at increased temperatures, the following chain of redox processes is observed:
TiO2 ^ 1 Ti„O2„-1 + 102
n n 1 1
^ 1 Ti2O3 + 2 O2
2 2 1
^ TiO +1 O2.
Reduction to TiO requires the use of significantly more stringent reducing conditions than reduction to TinO2n-1 and Ti2O3, as can be concluded based on the analysis of the calculation results (Fig. 1).
During calculation, the impact of particle size upon the thermodynamics of redox reactions was not taken into account. It seems that these effects can not significantly change the results presented in Fig. 1, at least for particles with a size of tens of nanometers. Thus, for the temperature range below that of the recrystallization processes, i.e. below the melting point of surface (nonautonomous) phase based on TiO2-Tm2n [19,20]), there is a potential possibility to obtain nanoparticles of titanium oxide in different oxidation states, less than 4+, by redox reactions.
The thermodynamic analysis of the possibility for forming titanium dioxide of different polymorph modifications during decomposition of hydrated titanium dioxide is of interest. Thermodynamic calculations were carried out with the assumption that hydrated titanium dioxide has a composition of Ti(OH)4 and is in the crystalline or amorphous state.
Fig. 1. T-lgpo2 regions of existence of titanium oxide in the "hydrogen-water vapor" atmosphere
Due to the fact that the thermodynamic data on formation enthalpy, entropy and heat capacity for Ti(OH)4 (AH(T), S(T), cp(T)) are absent in the literature, this data was obtained with the use of various approximate calculation methods. In particular, the method of comparative calculation proposed by Karapetyants [21] was used, which showed good agreement with the experimental data in the evaluation of the thermodynamic properties of a similar compound - Zr(OH)4 [22]. This method is based on a comparison of the relevant characteristics of two similar rows (I and II). To assess H298(Ti(OH)4), S298(Ti(OH)4) and cp(Ti(OH)4), thermodynamic data for the following compounds were used: AlX3, MgX2, CaX2, SrX2, FeX2, ZrX4, where X= F-, Cl-, Br-, OH- [23]. The results of the calculations are shown in Table 1.
Table 1. Thermodynamic data for Ti(OH)4
Thermodynamic property Value Note
H298, kJ/mol -1358.98 calculation according to [21]
-1084 calculation according to [24]
S298,kJ/mol-K 164.75 calculation according to [21]
127.9 calculation according to [25]
cp, kJ/mol-K 125.52 calculation according to [21]
131.1 calculation according to [25]
Due to the fact that the structure of the substance in an amorphous state, at least in the first coordination sphere, is close to the melt structure [26,27], the enthalpy of amorphization of hydrated titanium dioxide was evaluated based on empirical correlation proposed in [27].
AH298 amorphization = 0.3 — 0.5AHmeit,
where AH298 amorphization- amorphization enthalpy, kJ/mol; AHmelt - melting enthalpy, kJ/mol. Thus, the enthalpy of TiO2 • nH2O (n=2) in an amorphous state can be taken as:
AH2098 _ = AH098cr +0.4AHmeit = -1331 ± 10 kJ/mol,
AHmeit is taken as AHmeit = 68 kJ/mol (data according to the IVTANTHERMO database [18]).
Based on Gibbs energy calculations for the reaction of dehydration of titanium hydroxide, shown in Fig. 2, it can be concluded that the formation of both anatase and rutile modifications of TiO2 is possible throughout the whole calculated temperature and pressure range. This was the case, regardless of whether crystalline or amorphous Ti(OH)4 was considered as the starting material.
Fig. 2. Dependence of the Gibbs energy of dehydration of Ti(OH)4cr on the temperature and pressure for reaction Ti(OH)4=TiO2+2H2O
The inaccuracy in the determination of the thermodynamic properties of Ti(OH)4, apparently, can not affect the quality of conclusion on the instability of the hydrated form of titanium dioxide, since the AG value of the
dehydration reaction in absolute value significantly exceeds the possible errors in its calculation in the entire range of considered temperatures and pressures. Thus, the hydrated form of titanium dioxide (Ti(OH)4) in the considered range of P — T-conditions is unstable and can be transformed into both rutile and anatase forms.
Conclusion on thermodynamic instability of the hydrated form of titanium dioxide is supported by the results of experimental studies [1-3], in which it is shown that under certain conditions, even at temperatures close to room temperature, crystallization of amorphous gel of TiO2 • nH2O occurs with the formation of titanium dioxide with the anatase structure. Thus, based on the results of the analysis, it can be concluded that the kinetic factors, instead of thermodynamic factors, are determining in the dehydration process.
In addition to temperature and pressure influencing the possibility of the formation of a crystalline modification of TiO2 in the dehydration of Ti(OH)4, the influence of the size effect should be taken into account. To assess the effect of the size factor, the dependence between the Gibbs energy of the reaction of decomposition of titanium hydroxide and the size of formed particles of TiO2 was calculated. The calculation was carried out based on the known relations (for instance, see [28]).
The surface energy values for rutile and anatase titanium dioxide given in the literature are quite different. Based on the theoretical analysis given in [29,30], the surface energy value of rutile was assumed to be 1.5 J/m2 and 1.42 J/m2, respectively. Whereas, based on the results of experimental measurement of the excess enthalpy of grain boundaries [31], the value of surface energy for the rutile modification of titanium dioxide ranges from 1.3 to 1.7 J/m2. In [32,33], the rutile surface energy was taken as 1.5 J/m2, which is the average of these values, and the anatase surface energy was taken as 0.85 of the rutile surface energy, i.e. 1.275, that was associated with a corresponding increase in the molar volume of anatase compared to rutile. A more thorough analysis carried out in [34] allowed determination of the temperature dependence of the surface energy for both rutile and anatase as:
Vruta = 1.91 — 1.48 • 10-4(T — 298),
V anatase = 1.32 — 1.48 • 10-4(T — 298), where arutii, vanatase - surface energy of anatase and rutile, respectively, J/m2; T - temperature, K. It should be noted that the value of the surface energy of rutile, determined according to [34], is much higher than the values given in [29-32], while vanatase remains almost unchanged (Table 2). This may be due to higher difficulty of determining the influence of the relaxation processes on the surface energy of rutile having a higher density than titanium dioxide anatase.
In further thermodynamic calculations, the data given in [34] are used, which are more founded and can be presented as:
Vrutii = 1.9541 — 1.48 • 10-4T, (1)
vanatase = 1.364 — 1.48 • 10-4T, (2)
where the first term describes mainly the enthalpy component of the surface free energy, and the coefficient in front of temperature describes mainly the entropy component.
The dependence between the size of critical nuclei of anatase and rutile formed during dehydration of Ti(OH)4 and different values of temperature and pressure in the TiO2-H2O system was calculated (Figs. 3, 4).
T, °C. P; atm
Fig. 3. Dependence of the size of the critical nucleus of TiO2 (rutile) on the pressure and temperature during dehydration of Ti(OH)4
The obtained values for the critical nucleus sizes in the temperature range of nanocrystal formation according to the analysis of the calculation results shown in Fig. 3 and 4 range from 0.5 to 1 nm. Additionally, the lowest values
Table 2. Values of the surface energy of rutile (arutn) and anatase (aanatase) modifications of titanium dioxide
Value, J/m2 References
&rutil a anatase
1.5 - [29]
1.42 - [30]
1.3-1.7 - [31]
1.5 1.275 [32]
1.5 0.85 [32]
1.91-1.865 1.32-1.275 [34]
"clean surface" "clean surface"
(100) - 0.60 (001) -0.51
(011) -0.95 (100) - 0.39
(110) -0.47 (101) -0.35 "clean surface" - [35]
"hydrated surface" "hydrated surface" "hydrated surface " - [33]
(100) - 1.57 (001) - 1.55
(011) - 1.79 (100) - 1.13
(110) - 1.08 (101) - 1.03
0.47 - 0.95 0.35 - 0.81 [36]
0.31-1.65 0.44 - 1.09 [36]
Fig. 4. Dependence of the size of the critical nucleus of TiO2 (anatase) on the pressure and temperature during dehydration of Ti(OH)4
for critical nuclei are observed at minimum values of pressure and maximum values of dehydration temperature for Ti(OH)4. It should be noted that the calculated values of the critical nucleus size are beyond the applicability of the approach used. In particular, for surfaces with such curvature, it is necessary to take into account the dependence between the surface energy and the radius of curvature [37-39], and the term of crystalline titanium dioxide particle at such values of d does not make sense.
Comparison of sizes for the critical nuclei of anatase and rutile shows that the size of the critical nucleus for the TiO2 anatase modification is somewhat less than that of rutile one. In addition, it should be noted that the very small values for the size of the critical nucleus of rutile and anatase show an extremely weak trend in the formation of anatase nuclei compared to the formation of rutile nuclei, and the possibility of forming TiO2 of any of these modifications already at room temperature during the dehydration of Ti(OH)4.
Thermodynamic analysis of the phase transition:
TiO2 (anatase) ^ TiO2(rutil)
(3)
showed that in different variants of thermodynamic data used (IVTANTHERMO database [18], JANAF reference book [40], data given in Table 3) the bulk phase with the rutile structure is thermodynamically stable throughout solid phase titanium dioxide's range of existence (Fig. 5).
Fig. 5. Dependence of a change in the molar Gibbs energy in transition (3) on the temperature: 1) calculation based on the IVTANTHERMO data [18]; 2) calculation based on the JANAF data [40]
However, since the surface energy of anatase is lower than the surface energy of rutile (Table 2), based on the analysis of ratio:
AGanatase^rutil = AGb.p.(anatase^rutil) (T; P) + (arutil • Srutil + &anatase • Sanatase) , (4)
where, AGmnatase^rutil - change in molar Gibbs energy during transition of particles from anatase to rutile structure; AGbp (anatase^rutil) - change in molar Gibbs energy of bulk phases of TiO2 during transition of titanium dioxide from anatase to rutile structure; &rutil(anatase) - specific surface energy of rutile (anatase); Srutil(anatase) - surface of one mole of titanium dioxide with the rutile (anatase) structure. It can be expected that in the presence of a certain amount of particles of anatase, this phase will be more thermodynamically stable than the phase with the rutile structure.
Assuming that the particles have a shape close to spherical, expression (4) can be presented as:
AGb
anatase^rutil
AGm + 6
b.p.(anatase^rutil) '
r
b
rutil
drutil
+
a
b
anatase
da
(5)
where Vmatil{anatase) - molar volume of TiO2 with a rutile (anatase) structure; drutil(anatase) - diameter of the rutile (anatase) particles.
For the case when one anatase particle is transformed into one rutile particle, expression (2) can be presented
as:
AGanatase^rutil (T, P, danatase) = AGb.p.(anatase^rut,il) (T, P) +
_ Vm l _ / Vm \ 2/3 \ (6)
anatase • V anatase / ° rutil • I VrutiJ \ \ V '
6
da
a
- 1
Expression (6) does not take into account the effects of particle compression due to surface forces. This approximation can be used for larger particles [38], for example, having sizes of a few tens of nanometers or more. For small particles, taking into account the surface compression will lead to the transformation of expression (5) to the following:
AG anatase^rutÀl (T, P, danatase) AGb.p.(anatase^rutil) (T, P) +
&anatase • Vanatase I °rutil '
(6 + 4t)
%anatase anatase \Vanats
Vm
rutil
2/3
1
(7)
Table 3. Enthalpy of polymorphic transitions of TiO2
AH, kJ/mol T, K References
Anatase^Rutile
-3.761 298.15 IVTANTHERMO [18]
-3.743 948.15
-6.14 298.15 JANAF [40]
-2.61 ±0.41 ^ 298 [41]
-0.42±0.21 903 [42]
-2.93±1.26 1360 [43]
-3.26±0.84 971
-6.57±0.79 968 [44]
-8.37±5.92 298 [45]
0.42 2) 298 [46]
11.67 2) 1183 [10]
Brucite^Rutile
-0.71±0.38 971 [43]
-0.42±0.31 715 [42]
-0.84±0.42 930 [43]
41.84±9.36 2) [45]
Amorphous TiO2 ^Rutile
-20.4to-34.0 3) 298 Calculation according to depend of [27]
-24.25±0.88 4) 298 [41]
Rutile^Melt
68 2185 IVTANTHERMO [18]
Note:
1) - values recommended in [41];
2) - values indicated in [41] as causing doubt;
3) - AH2Q8 amophization = 0.3 — 0.5AHmeit, [27]; AHmeit(TiO2rut) = 68 kJ/mol IVTANTHERMO [18]
4) - Ssurf = 34596 m2/mol [41]
where t = 1 + ^^r (e - surface deformation), in accordance with [34] with reference to the data presented in [47], in this case it can be 1 < t < 2.
The results of thermodynamic calculation of limit values danatase, up to which the anatase polymorph modification of TiO2 is thermodynamically stable, for various input data options AGmnatase^.rutil (T, P, danatase), vrutil (T), vanatase (T), t (Table 2, 3) are presented in Fig. 6. The analysis of the calculated results for the limit values for anatase crystallite sizes, to which this polymorph modification is thermodynamically stable, shows that depending on possible values AGmnatase^rutil (T, P, danatase) ,<?rutii (T), v anatase (T), t, as well as on taking into account the compression of the particles due to the surface tension forces (expression (7)), limit values danatase can vary widely - from ~ 5 to ~ 37 nm (Fig. 6). It should be noted that these calculations do not take into account dependence v(d), which was mentioned, for example, in [37-39]. Taking this dependence into account is appropriate in cases where the particle size is several nanometers [28,47]. In this case, as shown by the results of calculations of danatase, dependence v(d) can be neglected.
Despite the wide range of variability for the possible limit values of danatase, associated with the choice of various thermodynamic parameters (Table 4), it is possible to determine the sensitivity of danatase to changes of
these parameters and narrow the range of the most probable values of danatase. First, it should be noted that insensitivity of limit values of danatase o temperature dependencies of values of AGmp (anatase^rutil) (T) and Vrutii(anatase) (T), both in the calculation AGmp(anatase^rutil) (T) according to the data of IVTANTHERMO [18], and according to the data of JANAF [40] (Fig. 6 a and b). In addition, the use of thermodynamic data from IVTANTHERMO and JANAF databases give substantially different limit values for danatase (compare Fig. 6 a and 6b, Fig. 6 c and 6d). Due to the fact that the thermodynamic data from IVTANTHERMO were checked for self-consistency [18], and due to the higher compliance AH(anatase^rutil) (IVTANTHERMO) with values recommended in [41] (see Table 3), in comparison with calculated according to JANAF [40], the results obtained using the IVTANTHERMO database should be considered as more reliable.
Limit values of danatase are sensitive to measurement of particle compression by surface tension (Fig. 6 b, c, d). Higher influence on the accuracy limit values of danatase is observed for uncertainty in the data on the values of the surface energy of the particles (Fig. 6 e). If we take into account the results of the analysis of the reliability of data according on arutii(anatase) and AGmp(anatase^.rutil), the range of possible limit values of danatase is narrowed to a range of -16 nm <danatase < 37 nm.
Table 4. Limit values for the sizes of the anatase particles (danatase) for various calculation parameters for cases in which one particle of TiO2 with the rutile structure is formed from one particle of TiO2 with the anatase structure
The parameters for calculating danatse, nm
Calculation according IVTANTHERMO excluding compression surface tension forces at different temperatures 15.7
Calculation according JANAF excluding compression surface tension forces at different temperatures 9.6
Calculation according IVTANTHERMO based compression of the surface tension forces
t = 1 26.25
t = 1.5 31.55
t = 2 36.80
Calculation according JANAF based compression of the surface tension forces
t = 1 14.37
t = 1.5 17.24
t = 2 20.1
Calculation according IVTANTHERMO based compression forces of surface tension (t = 1) depending on the values of a
Vrutil = 0.71 a anatase = °.58 4.9
arutil= 1.91 a anatase T32 26.3
The thermodynamic analysis of the possibility of anatase particles transforming into rutile particles, in the case of changes in the total number of particles in the system is of interest. Such mechanism is possible, for example, in the case of merger of several anatase particles into a crystallite with rutile structure, or alternatively, in the case of crushing the crystallite of anatase into several crystallites of rutile, as was observed, in particular, in [47] dedicated to the analysis of structural transformation of t-ZrO2 ^ m-ZrO2 during cooling. By designating
Fig. 6. Gibbs energy change in phase transition (3) depending on the anatase particle size (danatase) for different initial data (Table 4)
v = Nanatase/Nrutil, in the approximation of a spherical particle shape, expression (4) can be presented as:
anatase^rutil (T, P, danatase, v) = AGa.p.(anatase^rutil) (T, P) +
6 ^«sem^^f *ruta(T )• ( VZtU \ 2/3 v - 3 (8)
6 ^a„at„e(T) [Vm—) V3 - l)
In Fig. 7 and Table 5 the calculated results for the thermodynamic conversion possibilities of titanium dioxide with anatase structure into a rutile structure for different values of v are presented: 1 (no changes in the number of particles in the system); 2, 3, 4 (fusion of 2, 3 and 4 particles of anatase into one rutile crystallite); 1/2, 1/3, 1/4 (anatase particle fragmentation during phase transition). The mechanism of such phase transitions for v=1/4, 1/3, 1/2, 1, 2, 3, 4 is presented in Fig. 8.
Fig. 7. Results of calculation of changes in the Gibbs energy during structural transformations (3), associated with crushing or fusion of anatase particles (for calculations, IVTANTHERMO was used, surface energy values were calculated based on expressions (1) and (2), the effect of the surface compression of the particles was not taken into account)
Calculations of dependencies danatase(v) were carried out for Gibbs energy values for bulk phases taken from the IVTANTHERMO database, and vales arutil (T), aanatase (T) presented in the form of dependencies (1) and (2), as the most reliable, as it was shown earlier, and for the calculation option, in which the compression of particles by forces of surface tension is not considered. The results of calculations as a chart of the possible structural transformations depending on the particle size of titanium dioxide and various options crushing or fusing of particles during structural transformations are presented in Fig. 8. The results of calculations (Fig. 7, Table 5) show that if crushing of particles of anatase with the formation of several particles of rutile is possible only in the case of high values of danatase, which are significantly higher than the limit sizes of anatase particles, at which this modification of TiO2 is stable, the fusion of several particles of anatase with the formation of one particle of rutile, except for v = 2, is possible almost at all danatase values. In addition, the formed rutile particles can be unstable and undergo transition to the anatase structure (Fig. 8). In a real situation, the presence or absence of a structural transition can be influenced by the kinetic simplicity or difficulty of structural transition and growth of the particles, allowing their transition to a potentially stable, from a thermodynamic point of view, state of the rutile modification, starting with certain particle size values.
Table 5. Dependence of limit values for the sizes of anatase and rutile particles in cases of crushing (v < 1) and fusion (v > 1) of anatase particles according to the data of calculations given in Fig. 7
V The limits of particle size (d), nm
danatase drutil
1/4 51 31
1/3 42 28
1/2 31 24
1 16 16
2 3.6 4.0
3 for any values
4 for any values
Thus, according to the thermodynamic calculation carried out, during dehydration of Ti(OH)4, there is no significant thermodynamic preference to the formation of certain structural modification of titanium dioxide. The analysis of the size of the critical anatase and rutile nucleus formed during dehydration does not give reasons for discussing the preference of forming the anatase or rutile modifications of TiO2, i.e. thermodynamically and kinetically dehydration of Ti(OH)4 can lead to formation of TiO2 in both anatase and rutile modifications. In this situation, the preference in the formation of certain structural modifications of TiO2 will be observed for the modification, the genetic precursor of which is the substance, which is its structural analog, as was observed, for instance, for the formation of zirconium dioxide nanocrystals [48,49], or on the surface of the substance, which is structurally similar [50]. Analysis of the dependence between the stable state of anatase and rutile modifications and the particle size shows that in the case of formation of rutile particles during dehydration of Ti(OH)4 with a size below the limit values (Fig. 6, 7, Table 4, 5), i.e. for one of variants of calculation - less than — 15 nm (Fig. 8), transition TiO2 (rutile) ^ TiO2 (anatase) becomes possible, in contrast, for example, to zirconium dioxide, the transition of which from the thermodynamically stable monoclinic modification (m-ZrO2) to metastable modification t-ZrO2 is not possible for all particle sizes and for all P — T-conditions, up to (P, T), at which t-ZrO2 becomes equilibrium bulk phase. It should be noted that, in general, structural transitions are not always expected in the case of achieving the limit values of particle sizes,
drutil < drutil(lim)
TiO2 (rutile) — —> TiO2 (anatase),
danatase > danatase(lim)
since the existence of non-equilibrium structure of nanoparticles due to kinetic reasons is possible [47-49].
Due to the possibility of influencing the phase formation by sizes and shapes of space constraints [48,51,52], as well as the composition and structure of the wall material of these constraints, it is of interest to examine the formation of titanium dioxide taking into account these factors. Let's consider options of localization of titanium dioxide in "infinite cylinder" type channel and on the flat surface [48]. The two cases of solid phase contacts will be analyzed: coherent fusion of the material forming walls of spatial confinement with 1) the rutile form and 2) the anatase form of TiO2.
Calculations made for regions of thermodynamically stable TiO2 as rutile and anatase for the idealized cases of spatial constraints described above have shown that in the case of coherent fusion of the material of the spatially-constraining walls of "cylindrical channel" or "flat surface" types with the rutile structure, the latter will stably exist without any possibility of transformation into the anatase structure. In the cases of coherent fusion of the material of the constraining walls with the anatase structure, depending on the size of the particles of TiO2, it can exist as both anatase and rutile (Fig. 9, a, b). In addition, the stability of these structures is almost independent of temperature. It should be noted that this conclusion explains the literature data on the effect of the substrate structure and the thickness of the deposited layer on the structure of the titanium dioxide layer deposited by molecular layering [50].
Fig. 8. Chains of possible structural transformations in titanium dioxide depending on the anatase and rutile particle size based on the results of calculation presented in Fig. 7
3. Formation of TiO2 nanocrystals under hydrothermal synthesis and aerobic thermal treatment conditions
As the starting material for the experimental study of methods for titanium dioxide nanocrystal formation, X-ray amorphous hydrated titanium oxide obtained by direct precipitation with 25% ammonia solution NH4OH (extra pure grade) from diluted solution of titanium tetrachloride TiCl4 (0.3 mol/l) was used. Completeness of precipitation was controlled by pH of the solution 10). The obtained precipitate was washed with distilled water in order to remove excess ammonia and chloride ions by decantation and filtration. According to elemental analysis, the obtained precipitate did not contain any traces of chloride ions or other impurities.
The hydrothermal treatment was carried out at 200 and 250 °C, 70 MPa, and isothermal time ranged from 10 to 240 minutes.
Fig. 9. Dependence of the steady state of structural modifications of TiO2 on the nanoparticles' linear dimensions in varying types of spatially-constrained conditions: a) in "infinite cylinder" type channel b) and on the flat surface, with the assumption that the the material of the spatially-constraining walls is coherently fused with the anatase structure
The results of X-ray analysis are given in Fig. 10. According to X-ray diffraction data (Fig. 10), throughout the whole range of the hydrothermal treatment parameters, the formation of anatase crystalline titanium oxide is observed. Additionally, the size of crystallites formed is of not more than 16 nm (Fig. 11), which is consistent with the data obtained by thermodynamic analysis on the possibility of sustainable existence for the metastable anatase modification.
Analysis of X-ray diffraction data (Fig. 11) suggests that hydrothermal treatment of X-ray amorphous hydrated titanium oxide (TiO2 • nH2O) at 200 °C for 10 min leads to crystallization of about 0.2 (20%) of titanium dioxide in the anatase form. Whereas, at 250 °C, for the same time, the conversion reaches 0.85 (Fig. 10b, Fig. 10). It should be noted that the change in the crystallite size change is symbatical to the change in the conversion (Fig. 11), i.e. at 200 °C a significant increase of the size of the TiO2 crystallites occurs during a period of rapid increase in the conversion (Fig. 11), and when the conversion reaches about 0.8, the growth rate of the crystal phase and the size of the TiO2 crystallites with the anatase structure significantly decrease.
A comparison of the curve of changes in the conversion and the curve corresponding to changes in the relative values of the average volume of crystallites (v) (Fig. 12) suggests that at a temperature of 200 °C the formation of TiO2 nanocrystals in the anatase form from amorphous hydrated titanium oxide in the initial stage of hydrothermal treatment is mainly associated with the formation of new crystallites of anatase from the amorphous phase. In the case of increasing the isothermal time, the amount of amorphous phase decreases, which leads to a change in the predominant mechanism of crystallite growth. Upon reaching a conversion of 0.8, an increase in the TiO2 crystallite size is mainly due to an increase in their volume during the recrystallization process. A change in the prevailing process greatly reduces the growth rate of TiO2 crystallites (Fig. 11). At a temperature of hydrothermal treatment of 250 °C, the process for forming titanium oxide nanocrystals takes place so rapidly that after 10 minutes of isothermal time the conversion is higher than 0.80 (Fig. 11), and therefore, a further increase in the size of the crystallites takes place apparently due to the recrystallization process.
It should be noted that in the case of hydrothermal treatment of amorphous hydrated TiO2 and at a temperature of 200 °C and 250 °C, when the conversion is about 0.85, the size of crystallites is about 11 nm (Fig. 11). Also, the speed of their growth and increase in size during further isothermal treatment are very low. The low crystallite growth rate, and therefore a small change in their sizes appears to be related to the fact that in conditions of
20 30 « S 50 70 20 S Si H> 60 70
Fig. 10. X-ray diffraction patterns for samples obtained by hydrothermal treatment of hydrated titanium oxide at T=200 °C () and T=250 °C (b) and P = 70 MPa
o-1-1-1-1-1-1 o -1-1-1-1-1-1
0 40 80 120 160 200 240 z, min 0 40 80 120 160 200 240 i\min
Fig. 11. Dependence of the conversion (a) and crystallite size (d) on the duration of the hydrothermal treatment of hydrated titanium oxide at =200 °C and =250 °C, P=70 MPa
practically avalanche-like crystallization of TiO2 nanoparticles, they are characterized by relatively narrow particle size distribution, similarly to formation of ZrO2 nanoparticles [50,51].
For the samples obtained at hydrothermal treatment temperature of 250 °C, a change in the specific surface of samples has been analyzed depending on the isothermal treatment time (Fig. 13). According to the data shown in (Fig. 13), specific surface area of TiO2 nanoparticles obtained during hydrothermal treatment significantly decreases when the isothermal treatment time was changed from 30 minutes to 60 minutes. A further increase in the duration of treatment leads to a monotonic, but not significant decrease in the specific surface area of TiO2 nanoparticles.
Based on the data for the specific surface area of the titanium dioxide nanoparticles (Fig. 13), their size has been calculated assuming that the shape of particles is close to spherical. In the case of comparison of the crystallite sizes and sizes of anatase titanium dioxide particles, it can be observed that the crystallite sizes obtained based on the X-ray diffraction data are systematically lower than those of the TiO2 particles obtained based on the data on the specific surface (Fig. 14).
Fig. 12. Dependence of changes of the relative values of the average crystallite volume (v ) and the degree of conversion (a), on the duration of the hydrothermal treatment at T=200 °C (a) and T=250 °C (b), P=70 MPa
Ssurf, m2/g
90
SG-
70-
60"
50 -1-1-1-1-1-1
0 40 80 120 160 200 240
t, mill
Fig. 13. Dependence of of the specific surface (Ssp) on the duration of the hydrothermal treatment of hydrated titanium oxide at T=250 °C, P=70 MPa
This can be be due, for example, to the fact that the obtained particles contain a crystalline core, the size of which is determined based on broadening of X-ray diffraction lines and X-ray amorphous coating, the presence of which is taken into account during specific surface area determination. Such explanation of the difference in sizes of particles and crystallites is possible in cases when the proportion of the amorphous states in the system is large, i.e. at low temperatures and times of phase formation. When the temperature and time of hydrothermal treatment are T=250 °C, т >60 min as follows from the analysis of the data presented in Fig. 12, the proportion of the amorphous phase in the system is low. In this case, the difference between sizes of particles and crystallites is likely determined by the fact that the anatase TiO2 crystallites formed dense polycrystalline aggregates composed of 3-4 crystallites, as can be concluded based on the analysis of the dpart/d3ryst ratio.
The results of complex differential thermal analysis of the TiO2 nanoparticles obtained during hydrothermal treatment of the hydrated titanium oxide are given in Fig. 15. On the DSC curve, a set of thermal effects accompanied by a change in the mass of the sample is determined (Fig. 15, Table 6).
The analysis of data presented in Fig. 16 shows that the observed exothermic heat effects in the range of 200-510 °C are not accompanied by a marked change in the structural state of TiO2 nanoparticles. Up to 600 ° C, in the X-ray diffraction patterns, peaks corresponding to titanium oxide in the anatase structural modification are observed. Only after heat treatment to temperatures in the area of 1000 °C, the anatase ^ rutile transition is observed. According to this data, the structural state of titanium dioxide is shown in Table 6. The dependence of the size of crystallites on the treatment temperature is shown in Fig. 16.
Fig. 14. Dependence of the size of TiO2 nanoparticles calculated based on the data on the specific surface area (1) and the size of crystallites of TiO2 (anatase) calculated based on X-ray diffraction data (2) on the duration of the hydrothermal treatment of hydrated titanium oxide at T=250 °C, P=70 MPa
Fig. 15. Results of complex thermal analysis of TiO2 nanoparticles obtained during hydrothermal treatment of amorphous hydrated titanium oxide at T=200 °C, P=70 MPa, and 120 min isothermal treatmen
Table 6. Thermal effects and changes in the weight of the sample obtained by hydrothermal treatment of amorphous hydrated titanium dioxide at T=200 °C, P=70 MPa, and 120 min isothermal treatment
Temperature range, °C Nature of the thermal effect Weight loss, % Phase composition
25-200 endo 4 anatase
200-510 exo 3.7 anatase
850-950 exo 0.1 rutile
Fig. 16. X-ray diffraction patterns of the samples obtained during heating of titanium dioxide nanoparticles in air under conditions similar to used in the DSC heating mode
Thus, it seems that in the temperature range of 200-510 °C two processes occur: dehydration of remaining amorphous hydrated titanium oxide and its crystallization in the form of the anatase modification that leads to corresponding thermal effects on the thermogram (Fig. 15, Table 6). Based on the data on the weight loss in the temperature range of 200-510 °C, it can be assumed that amorphous hydrated titanium oxide component remaining after dehydration at 25-200 °C has the following formula: Ti02-0.18 H2O.
In the high-temperature region, the exothermic effect is accompanied by a negligible change in the weight of the sample and is associated with the Ti02-anatase^Ti02-rutile phase transformation. It should be noted that the size of the crystallites of titanium dioxide sharply increases during the transition from anatase to rutile modification and is about 50 nm.
4. Conclusion
Thermodynamic analysis of processes in the Ti02-H20 system over a wide range of varying conditions (temperature, pressure, oxygen potential and crystalline particle size), as well as the presence of various types of space constraints allowed us to determine the regions of sustainable existence for titanium dioxide in the form of rutile and anatase modification. The results of thermodynamic prediction on the possibility and conditions for the sustainable existence of Ti02 with the rutile structure have been experimentally confirmed. The conditions and mechanisms for the formation of rutile and anatase nanocrystals during thermal treatment of amorphous hydrated titanium oxide in air and hydrothermal environments have been determined. It has been shown that the transition
of titanium dioxide from the anatase to the rutile phase occurs by fusion and recrystallization of agglomerate consisting of three or four anatase particles with an average size of 50 nm.
Acknowledgements
The author would like to thank Prof. V. V. Gusarov for interest in the work and help in the interpretation of results. This work was supported by the Russian Foundation for Basic Research (project No 16-03-00532).
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