K. Liu et al. / Electrochimica Acta 318 (2019) 236e243
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2. Experiment
applying a potential promotes reaction (2). As the reaction time
went on, the diffraction peaks of NaCl became weaker and weaker,
which indicates the pellets have a good diffusion channel for ions.
The theoretical decomposition potential of CaCl2 at 900 ꢀC is
3.137V, which is calculated from thermodynamic data according to
Nernst equation [17]. In experiments, the observed decomposition
potential of CaCl2 agrees well with the calculated value. Fig. 2a
shows the typical current vs. time (I-t) curve during the electro-
chemical reduction experiments performed with a Na2Ti3O7 pellet
as the cathode and a graphite rod as the anode under an applied
voltage of 3.1V. The current jumped to about 3A in the moment the
voltage was applied and then decreased sharply in 1 min, which
could be attributed to the double layer charging and the accumu-
lation of adatoms on the electrode. In the next minutes, the current
increased quickly again to about 3A. According to 3PIs (three-phase
interlines) propagation models in initial phase of electro-
deoxidation, that could be due to the expansion of the 3PIs [18].
After passing through the maximum value, the current decayed
with time. Until about 4 h later, the current levelled out at about
0.7A. The decreasing again of the current occurred after about 16 h.
Finally the current decreased to about 0.3A in 22 h. Curves of cur-
rent against time for an experiment are closely related to the rate of
reaction, with a faster rate corresponding to a higher current. And
the rate of reaction could be again related with the phase compo-
sitions of electrode. For the experiments here, the sudden change of
the current tends to imply the possible change of the phase com-
positions of cathode pellets. On the I-t curve, two peaks (A, B), two
inflection points (C and D) and two shoulders (E and F) appeared
successively. Thereby these time points were chose as the termi-
nating time points of polarisation.
Table 1 lists the experiment conditions and the corresponding
results. After about 6min of polarisation, the sample (S1) was
found to be predominantly composed of CaTiO3 and Ti2O3. Magneli
phases, such as Ti4O7 and Ti3O5, were not detected here. But they
were detected in the sample quenched after 10min of polarisation
when cutting down the voltage to 2.8V, as shown in Fig. S2 (in the
supplementary materials). Prolonging the polarisation time to
about 10min, the sample (S2) consisted of CaTiO3, Ti2O3 and little
TiO; to ~37min, the sample (S3) was mainly comprised of CaTiO3,
Ti-O solid solution (Ti2O) and little CaTi2O4; and to 4 h, the sample
(S4) consisted mainly of Ti-O solid solution (Ti3O) and little CaTiO3.
Fig. 2c shows the XRD patterns of the partially reduced samples.
During around 6e37min of polarisation, CaTiO3 was much more
than other phases and decreased slightly with electrolysis times;
titanium suboxides gradually disappeared; Ti-O solid solution and
CaTi2O4 began to form. During around 0.6e4 h of polarisation,
CaTi2O4 disappeared completely, CaTiO3 diminished dramatically
and Ti-O solid solution (Ti3O) increased substantially. After about
16 h of polarisation, the sample (S5) was reduced into Ti metal but
the oxygen content was up to 1.6 wt%. Prolonging the polarisation
time to 22 h, the oxygen content of the sample (S6) decreased to
about 0.6 wt%. At the same time, it was found that the pellets
became thinner and thinner with the step-by-step reduction of the
pellets.
Anhydrous CaCl2 (10005861 Sinopharm) was dried for 4 h at
300 ꢀC under vacuum before use. The CaO content of the dried salt
was estimated by acid-base titration method and was found to be
about 0.045% wt%. Sodium titanite (98 wt%, Na2Ti3O7, Shanghai
Dian Yang Industry co. Ltd) powder was pressed into pellets under
the axial pressure of 40 MPa. Then these pellets were sintered for
4 h at 900 ꢀC. The sintered pellets (3.00 0.03g, 28.7 mm diameter
and 1.83 mm thickness), whose porosity was measured by Mercury
Porosimeter and is about 20%, were attached to a molybdenum
wire (2 mm diameter, 700 mm long) that was employed as the
current collector of cathode. A high-purity graphite rod (10 mm
diameter, 80 mm long) was used as anode, which was connected
with a stainless steel collector. Alumina crucibles (80 mm inner
diameter and 120 mm high) were used as containers for molten
CaCl2. 500g dried CaCl2 salt was taken in an alumina crucible and
placed in a leak tight reactor vessel. Before heated, the vessel was
evacuated to 10Pa and then was replenished with high-purity Ar
gas. This process was repeated twice. Then Ar gas passed contin-
uously through the reactor vessel at 2L/min until the end of each
experiment. The vessel was heated by silicon carbide rods. When
the salt was heated to 900 ꢀC, the graphite anode and the sodium
titanate pellet were inserted into molten salt through electrode
holes at the furnace cover. The applied voltage between the cathode
and anode was 3.1V.
The partially reduced samples were obtained after different
electrolysis times. After each experiment, the sample was moved
out from molten salt and cooled down rapidly at argon atmosphere.
Then they were rinsed with flowing tap water to remove the so-
lidified molten salt clinging to the surface of samples and were
dried in vacuum oven at room temperature. The microstructure and
constituents of samples were analysed by SEM and EDS (S-4800,
Hitachi). The phase compositions of the partially reduced samples
were analysed by X-ray diffraction analyser (X'Pert Pro
MPDDY2094, PANalytical B.V with CuKa radiation). The content of
oxygen in final product was tested by oxygen/nitrogen analyser
(TC500 LECO).
3. Results
Fig. 1a presents the XRD spectrum of the precursor material
after sintering for 4 h at 900 ꢀC. The main phase is Na2Ti3O7. The
SEM image (in Fig. 1b) shows the Na2Ti3O7 present rod-like parti-
cles ranging from 1 mm to 3 mm in length. Fig. 1d is the sectional
SEM image of a sodium titanite (Na2Ti3O7) pellet after 4 h of sub-
merging in molten CaCl2 at 900 ꢀC. The particles were still rod-like,
but the phase compositions of the pellets had become a mixture of
TiO2, CaTiO3 and little Ca2Ti2O6 as shown in Fig. 1c. At the same
time, it was observed that the space between the particles was
filled with electrolyte. Fig. S1 (in the supplementary materials)
shows the X-ray diffraction patterns of Na2Ti3O7 pellets submerg-
ing in CaCl2 melted salt for different times at 900 ꢀC. Na2Ti3O7 re-
acts with molten CaCl2 easily to form Ca2Ti2O6, TiO2 and NaCl in
~30min. And then in the next 3.5 h, Ca2Ti2O6 was transformed into
CaTiO3 completely. The involved reactions are as follows.
Fig. 2b shows the SEM images of the cross sections of S1-S6. The
samples began to delaminate after 6min of polarisation. The outer
layer is the reduced region and the core is the less reduced region.
As the polarisation time went on, the outer layer grew thick and the
core shrunk progressively. The pellets were gradually reduced from
outside to inside. After 4 h of polarisation, the reduced region was
found to be porous and sintered slightly, and the less reduced re-
gion was compact. During 4e22 h of polarisation, the pellet was
sintered fast and finally became a compact metal sheet of about
0.7 mm in thickness.
2Na2Ti3O7 þ 2CaCl2 / Ca2Ti2O6 þ 4TiO2 þ 4NaCl
Ca2Ti2O6 / 2CaTiO3
(3)
(4)
When a voltage of 3.1V was applied between a Na2Ti3O7 cathode
and a graphite anode in molten CaCl2, the Na2Ti3O7 pellet trans-
formed into a mixture of CaTiO3, Ti2O3 and little Ca2Ti2O6 in ~ 6min
as shown in Fig. 2c(S1). From the experiments, it was found that