J.F. Su, et al.
AppliedCatalysisA,General606(2020)117809
Table 2
noise. The result indicated that the orientation of facets (214) and (420)
of the electrode were not paralleled to the sample surface [58,60,61].
The intensity of all XRD patterns were normalized against stainless steel
support, the variance in peak intensity among electrodes suggested that
the electrodeposition procedure influenced the preferred orientation for
the growth of crystallites as well as crystal facet distribution. Fig. 4
gives the HRTEM image and the corresponding selected-area electron
diffraction (SAED) patterns of SS/Sn0.2Pd0.8-497 electrode. Results
showed three strong continuous lattice fringes with lattice spacing of
0.250 nm, 0.202 nm, and 0.138 nm. Note that the spacing calculated
from SAED pattern matched the d-spacing of the (214), (131), and
(420) plane in Sn3Pd phase (i.e. 0.240 nm, 0.204 nm, and 0.145 nm,
respectively, according to ICDD PDF Card No. 00-015-0575). The result
was consistent with XRD characterization, supporting the formation of
Sn3Pd alloy.
Kinetic constants, nitrate removal, selectivity of nitrite, ammonium, and ni-
trogen, nitrogen yield, and charge transfer resistance.
Samples
k (h−1
)
R2
XNO
SNO
SNH
SN
Rct (Ω)
N
2
2
3
2
4
SS/Pd0.2Sn0.8-497
SS/Sn0.8Pd0.2-497
SS/Sn0.8Pd0.2-166
SS/Sn0.8Pd0.2-332
0.32
0.24
0.14
0.24
0.96 0.74
0.96 0.65
0.91 0.47
0.98 0.63
0.98 0.56
0.99 0.60
0.92 0.88
0.02
0.03
0.03
0.02
0.03
0.03
0.02
0.30
0.09
0.13
0.18
0.13
0.14
0.09
0.68 0.50 32
0.88 0.58 40
0.84 0.38 72
0.80 0.53 41
0.84 0.48 59
0.83 0.50 48
0.89 0.79 23
SS/Sn0.8Pd0.2-1490 0.20
SS/Sn0.5Pd0.5-497
SS/Sn0.2Pd0.8-497
0.22
0.47
1. k = nitrate removal rate constant; R2 = coefficient of determination; XNO
= nitrate conversion; SNO , SNH+
, SN = selectivity of NO2−, NH4+, and N23;
2
2
4
= nitrogen yield; Rct = charge transfer resistance.
2N. 2Example electrode identification: SS/Pd0.2Sn0.8-497 = 20% Pd right on the
SS surface and 80% Sn on the outside surface prepared with total charge of
497C.
3.2. Optimizing electrode preparation procedures
Fig. 5 shows the concentration change of NO3−, NO2−, NH4+, and
N2 as a function of reaction time at constant current of −0.04 A. Results
present in Fig. 5a indicated that nitrate was readily electrochemically
[NO3 ]0 [NO3 ]t [NO2 ]t [NH4+]t
SN
2
[NO3 ]0 [NO3 ]t
(5c)
in which [NO2 ]t and [NH+
]t were the concentration of nitrite and am-
monium, respectively, at 4time t.
−
revealed that NO3 reduction follow the first-order-kinetic model
(R2 > 0.91) as shown in Fig. 5b. Electrode with Pd on the outside
surface, i.e., SS/Sn0.2Pd0.8-497 exhibited relatively greater nitrate re-
3. Results and discussion
moval rate constant and nitrate conversion (k =0.47 h−1
,
3.1. Characterization of synthesized bimetallic electrodes
XNO = 0.88) than that with Sn deposited on the outside of the elec-
3
trode, i.e., SS/Pd0.8Sn0.2-497 (k =0.24 h−1
,
XNO = 0.65) under
3
Fig. 2 shows the surface morphology of electrodes characterized by
SEM. Fig. 2a and b are the SEM micrographs of SS/Pd0.2Sn0.8-497 (Sn
on the outer layers) and SS/Sn0.8Pd0.2-497 (Pd on the outer layers),
respectively. It is clear that the electrode surface of SS/Sn0.8Pd0.2-497
composed of multiple nanoparticles, leading to higher roughness
compared to the surface of SS/Pd0.2Sn0.8-497. Fig. 2b-2e represent the
SEM micrographs of four electrodes prepared with different Q values,
exhibited distinct surface architectures among all four electrodes. Al-
though these four electrodes appeared to compose nanoparticles on the
surface, the degree of roughness was clearly different. Considering that
all samples have the same composition and deposition sequence, we
postulate that different Q applied resulted in different electrode surface
properties. SEM micrographs of Fig. 2b, f, g reveal the surface
morphologies of electrodes prepared from different Sn to Pd ratios. It is
noted that the roughness features of SS/Sn0.8Pd0.2-497 (Fig. 2b) and SS/
tures between Fig. 2g and h indicate the surface structure was retained,
demonstrating the stability of Sn-Pd bimetallic electrodes prepared in
this study.
otherwise identical conditions, indicating electrodes with Sn-rich outer
surface was beneficial to nitrate conversion.
For electrodes prepared with same Sn to Pd ratio (SS/Sn0.8Pd0.2) but
different Q, it appeared that nitrate conversion increased with in-
creasing Q, reached maximum value at Q of approximately 500 C then
slightly tailed off. The removal rate constant also revealed the same
trend with low k on SS/Sn0.8Pd0.2-166 (k =0.14 h−1) and maintaining
constant k value (k =0.24 h−1) on SS/Sn0.8Pd0.2-332 and SS/Sn0.8Pd0.2
497, except a slight drop of k on SS/Sn0.8Pd0.2-1490 (k =0.20 h−1).
-
For electrodes with the same Q of 497 C, but different Sn to Pd
ratios, namely, SS/Sn0.2Pd0.8-497, SS/Sn0.5Pd0.5-497, and SS/
Sn0.8Pd0.2-497, nitrate conversion decreased from 0.88 at Sn:Pd = 1:4
to 0.60 at Sn:Pd = 1:1 then increased to 0.65 at Sn:Pd = 4:1, while k
(h−1) decreased from 0.47 at Sn:Pd = 1:4 to 0.22 at Sn:Pd = 1:1 then
increased to 0.24 at Sn:Pd = 4:1. The SS/Sn0.2Pd0.8-497 electrode ex-
hibited the highest nitrate conversion among all bimetallic electrodes in
this work, indicating Sn:Pd metal ratio of 1:4 was sufficient for the
reduction of most nitrate ions in the solution. Further increase in Sn
loading might block Pd active sites and reduce the reaction rate and
time. In general, nitrite concentration increased with reaction time.
After 5 h, nitrite concentration and selectivity were low, indicating no
nitrite accumulation and fast reaction kinetics [62]. Fig. 5d gives the
concentration of ammonium as a function of reaction time. Results
again showed the importance of the deposition sequence of metals on
ammonium selectivity. Interestingly, ammonium selectivity was in-
hibited when Pd was deposited after Sn, i.e., Pd was on the outer layers
of the electrode structure. All electrodes prepared by depositing Sn first
The surface morphology of electrodes was also characterized by
XRD as shown in Fig. 3. Note that the major diffraction peaks of Pd
metal were located at 2θ = 40, 48, and 68 with (111), (200), and (220)
crystal facets, respectively (ICDD PDF Card No. 00-046-1043) [53–55].
The major diffraction peaks of Sn metal were located at 2θ = 30.7, 32,
and 45 with (200), (101), and (211) crystal facets, respectively (JCPDS
Card No. 04-0673) [55–57]. The surface crystal structure was assigned
by matching XRD pattern of each sample with known standard patterns
[31,58–60]. Interestingly, most samples exhibited X-ray diffraction
peaks at 2θ = 38.1, 44.4, and 64.6, excluding 2θ = 43.5, 50.8 from the
stainless steel (ICDD PDF Card No. 00-033-0397), indicating the for-
mation of Sn3Pd alloy (ICDD PDF Card No. 00-015-0575) with (214),
(131), and (420) crystal facets on the electrode surface, respectively. In
some cases, such as SS/Sn0.8Pd0.2-166, the crystal structure was pre-
sumed to be Sn3Pd alloy based on metal composition because the dif-
fraction peaks at 2θ = 38.1 and 64.6 were indistinguishable from the
+
then Pd (SS/Sn-Pd) exhibited low NH4 production, which might be
resulted from insufficient surface hydrogen on Pd sites and thus
weakening hydrogenation abilities due to the blockage of Pd active sites
by Sn metal. According to Eqs. (1c)–(1f), hydrogenation from Pd[H]
mation. In the case of SS/Pd0.2Sn0.8-497, Pd[H] might not be enough in
density or availability for the overall reaction as the active sites were
covered or blocked by Sn. Thus, the reduced N-intermediates from
7