2
84
SINITSKII et al.
instance of more homogeneous starting mixtures, the
effect of the chemical history of aluminum oxide on its
reactivity with lithium carbonate will be weaker.
(a)
Li CO
2
3
This assumption is strongly supported by the results
obtained for the mixtures of lithium carbonate and alu-
minum oxide prepared by grinding with water and then
reacted at 600°C for 3 h (Fig. 4). The XRD patterns dis-
played in Fig. 4 (comparison of sample 2, prepared by
decomposing aluminum oxalate, and sample 3, pre-
pared by decomposing aluminum hydroxide obtained
via a nitrate route) indicate that, for the mixtures
ground with water (Figs. 4c, 4d), the differences in the
solid-state reactivity of lithium carbonate with alumi-
num oxide are much smaller compared to those ground
in acetone (Figs. 4a, 4b).
γ-LiAlO2
γ-LiAlO2
(b)
Li CO
2
3
γ-LiAlO2
Figure 5 illustrates the reaction between Li CO and
γ-LiAlO2
2
3
Al O at 700°C over a period of 1 h.
2
3
Whereas Li CO is almost nonreactive with sam-
2
3
ples 2 and 5 at 600°C (Figs. 2a, 3a), the rate of
γ-LiAlO formation at 700°C is rather high (Fig. 5a).
2
The reaction of Li CO with samples 1 and 3 proceeds
2
3
(c)
in almost the same way as at 600°C (Fig. 5b). Finally,
in the case of sample 4, γ-LiAlO begins to transform
2
into α-LiAlO , as evidenced by the splitting of the dif-
fraction peaks with d = 3.98, 3.15, and 2.72 Å into two
components (Fig. 5c).
2
γ-LiAlO2
γ-LiAlO2
γ-Al O
2
3
Thus, our results demonstrate that the chemical his-
tory of x-ray amorphous aluminum oxide has a signifi-
cant effect on its solid-state reactivity with Li CO .
2
3
2
0
25
30
35
40
45
50
θ, deg
ACKNOWLEDGMENTS
2
We are grateful to A.V. Knot’ko for carrying out the
electron-microscopic studies.
This work was supported by the Leading Scientific
Schools Program, grant no. 00-15-97435.
Fig. 5. XRD patterns from 1 : 1 reaction mixtures of Li CO
2
3
and Al O after firing at 700°C for 60 min; (a–c) same as in
2
3
Fig. 2.
In the case of samples 1 and 3, the intensity of the
reflections from γ-LiAlO2 remains unchanged
Figs. 2b, 3b), indicating that increasing the firing time
REFERENCES
(
1
2
. Tret’yakov, Yu.D., Tverdofaznye reaktsii (Solid-State
Reactions), Moscow: Khimiya, 1978.
. Zubov, V.I., Size Effects and Properties of Ultradisperse
Systems, Zh. Vses. Khim. O–va. im. D.I. Mendeleeva,
1991, vol. 36, no. 2, pp. 5–9.
does not change the extent of reaction. This finding sug-
gests that, during the first 15 min of firing, the reaction
of Li CO with samples 1 and 3 takes place on the sur-
2
3
face of the reactants and that the diffusional flux at
6
00°C is insufficient for volume reaction.
3
. Schmalzried, H., Chemical Kinetics of Solids, Wein-
heim: VCH, 1995.
An important point is that, even though diffusion is
impeded at 600°C, phase transitions proceed rather rap-
4. Osipov, K.A., Amorfnye i ul’tradispersnye kristalli-
cheskie materialy (Amorphous and Ultrafine Crystalline
Materials), Moscow: Nauka, 1972.
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Zh. Vses. Khim. O–va. im. D.I. Mendeleeva, 1991,
vol. 36, no. 2, pp. 3–4.
idly. In the case of sample 4, the γ-Al O formed in the
2
3
first 15 min of firing rapidly converts into γ-LiAlO in
2
5
the course of subsequent firing for 3 h, as evidenced by
the small number and low intensity of reflections from
γ-Al O (Fig. 3c).
2
3
Thus, the homogeneity of the starting mixture has a
profound effect on the reaction rate and path because,
at 600°C, diffusion is impeded, and a higher homoge-
neity of the reaction system ensures a larger reaction
area. It is, therefore, reasonable to expect that, in the
6
. Toropov, N.A., Barzakovskii, V.P., Lapin, V.V., and Kurt-
seva, N.N., Diagrammy sostoyaniya silikatnykh sistem:
Spravochnik (Phase Diagrams of Silicate Systems: A
Handbook), issue 1: Dvoinye sistemy (Binary Systems),
Moscow: Nauka, 1965.
INORGANIC MATERIALS Vol. 39 No. 3 2003