ARTICLE IN PRESS
C.V. Subba Reddy et al. / Journal of Physics and Chemistry of Solids 69 (2008) 1261–1264
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2. Experimental
(a)
V2O5 powder (99.5%) was dissolved in 1 M NaOH
solution (0.33 M) at room temperature. To investigate the
influence of the pH values, a set of experiments were
designed. The pH of the solution was adjusted to 2, 4, 7,
and 10 by adding a HNO3 solution. The pH-adjusted
solution was placed in an oven for ageing at 90 1C for 5
days. The clear solution turned orange and red upon
ageing, while its viscosity progressively increased. A dense
colloid suspension with dark red color was formed. The
dense colloid suspension thus obtained was dried at 60 1C
for 48 h under static-air conditions. The products were
filtered, washed with distilled water, and dried in air.
Calcination was performed at 250 1C. This synthesis is
advantageous because it is simple and easy to control
besides being time-saving and cost-effective.
(b)
(c)
(d)
Na1.1V3O7.9(JCPDS # 45-0498)
NaVO3(JCPDS # 32-1198)
Crystallographic information of the samples was ob-
tained using a Rigaku D-max-gA X-ray powder diffract-
ometer equipped with graphite monochromatized Cu Ka
10
20
30
40
50
60
70
2θ (degree)
˚
radiation (l=1.54187 A). Diffraction data were collected
Fig. 1. XRD patterns of sodium vanadate nanostructures obtained from
solutions of various pH values: (a) Na1.1V3O7.9 (at pH ¼ 2);
(b) Na1.1V3O7.9 (at pH ¼ 4); (c) a mixture of Na1.1V3O7.9 and NaVO3
(at pH ¼ 7); (d) NaVO3 (at pH ¼ 10).
over the 2y range from 2 to 701. Fourier transform infrared
(FTIR) absorption spectra of the nanostructures were
recorded using a 60-SXB IR spectrometer of 4 cmꢁ1
resolution, over a wave number range of 400–4000 cmꢁ1
.
Raman spectra were taken under ambient condition by
using Renishaw inVia Raman microscope excited with the
514-nm light of an Ar+ laser. The morphologies of the
resulting products were characterized by field-emission
scanning electron microscopy (FESEM, JSM 6700F). The
electrochemical properties of the nanostructured sodium
vanadates were examined by cyclic voltammetric (CV)
measurements using a three-electrode cell with a platinum
counter electrode and a silver wire as a pseudo-reference
electrode. The working electrode, prepared by mixing
75 wt% of active material, 20 wt% of carbon black and
5 wt% of ethylene cellulose, was then coated on a 1.5 cm2
ITO glass. A solution of 1 M lithium perchlorate (99.99%,
Aldrich) in propylene carbonate (99.7%, Aldrich) was used
as the electrolyte. CV measurements were carried out
between the potential limits of ꢁ1.0 and 1.0 V against the
pseudo-reference Ag electrode using a potentiostat/galva-
nostat (Zahner IM6). The CV curves were recorded at a
scan rate of 1 mV/s.
˚
32-1198) with lattice parameters of a ¼ 5.36 A,
˚
˚
b ¼ 14.15 A, and c ¼ 3.65 A. The diffraction peaks of the
sample prepared from the pH ¼ 7 solution (Fig. 1c) can be
indexed as mixture of Na1.1V3O7. 9 and NaVO3.
Vanadium in its higher oxidation state is known to give
various isopolyvanadates at different pH values in aqueous
solution [14]. We were able to obtain meta-NaVO3
(at pH ¼ 10), the mixture of meta-NaVO3 and poly-
Na1.1V3O7.9 (at pH ¼ 7), and poly-Na1.1V3O7.9 vanadate
salts from the solutions of low pHs.
The size and morphology of the sodium vanadates were
examined by FESEM. Uniformly distributed nanostruc-
tures have grown from the sol evaporated from the pH-
controlled solutions as shown in (Fig. 2). The nanobelts or
flakes with the dimension of 50–500 nm in width and
1–6 mm in length are straight and have rectangular flat tips
with somewhat sharp corners. Sodium vanadates prepared
from the solutions of low pH seem to crystallize in smaller
sizes compared with that from the high pH solutions.
Raman scattering spectrum of sodium vanadate
(NaVO3) is shown in Fig. 3. The Raman peaks at 950,
915, and 892 cmꢁ1 are assigned to the stretching vibrations
(ns) of the V–O (1) and V–O (2), which are well matched
with the published data [9,15]. The bands at 737 and
562 cmꢁ1 are assigned to the asymmetric stretching (nas) of
the O–V–O, while the band at 435 cmꢁ1 is assigned to the
symmetric stretching (ns) of the O–V–O. The Raman peaks
of the low-frequency region (lower than 300 cmꢁ1) may be
related to the external vibrations, i.e. crystal lattice
translational (T) and rotational (R) modes.
3. Results and discussion
The crystal structure and phase purity of the samples
have been examined by powder XRD, which is shown in
Fig. 1. The samples are identified as Na1.1V3O7.9 and
NaVO3. The samples prepared from the solutions of
pH ¼ 2 and 4 are pure Na1.1V3O7.9, all of the reflection
peaks are indexed as monoclinic Na1.1V3O7.9 (JCPDS No:
˚
˚
45-0498) with lattice parameters of a ¼ 13 A, b ¼ 8.388 A
˚
and c ¼ 14.102 A, b ¼ 101.71. All the diffraction peaks of
the sample prepared from the solution of pH ¼ 10 (Fig. 1d)
are indexed with the orthorhombic NaVO3 (JCPDS No: