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the existence of an interaction between the cobalt nanoparticles and the
tube surface, and the interaction becomes significantly strong in the
narrowest tubes. In contrast, the Co 2p3/2 binding energy decreased to
7
80.7 eV upon transfer of all the particles to the exterior tube surface.
The finding indicated that the chemical state of the Co species encapsu-
lated within the CNT channels is remarkably different in comparison
to that of the Co species on the exterior tube surface. It is reported
that π-electron density is shifted from the concave inner to the convex
outer surface, and the shift is enhanced as the CNT cross-section
becomes smaller [19,20]. Therefore, the interaction between the
electron-deficient concave surface of the nanotube and the anionic
oxygen in CoO could lead to a weakened bonding strength of Co–O
and the reduction of CoO nanoparticles is facilitated considerably within
2
the smaller CNT inner tubes [21,22]. The characterization of H -TPR
confirms that the reduction of metal oxides is more facile upon the
decrease of the inner diameter. The reduction temperature of CuCoCe/
CNT(8) was 13 °C lower compared with that of CuCoCe/CNT(30) and
CuCoCe/CNT(20) (Fig. S1).
Furthermore, it is reported that the Co–CeO2−x interface could be
suitable for the formation of alcohols in FT reactions [11,12]. The relative
surface concentrations of cobalt and cerium were calculated for the
fresh samples. Samples CuCoCe/CNT(30), CuCoCe/CNT(20), and
CuCoCe/CNT(8) displayed a Co/Ce value of 1.09, 1.16, and 1.41, respec-
tively. The results indicated that more Co–CeO2−x interfaces may be
formed in CuCoCe/CNT(8) after reduction, and the interface accelerates
x
the dissociation of the C–O bond and provides more CH intermediates.
Therefore, it remarkably increases the rate of the first C–C bond forma-
tion in the nanotube channels and accelerates the formation of higher
alcohols.
3.2.3. ASF plots
The ASF plots (logarithm of mole fraction vs. carbon number) for the
distribution of alcohols obtained over the four studied catalysts are
shown in Fig. 5. As shown in Fig. 5, the carbon number distributions of
alcohols obtained over CuCoCe/CNT(30) obeyed the ASF distribution.
Deviation from the ASF distribution was observed for CuCoCe/
CNT(20). When these active components were introduced to the
smallest CNT(8) tubes, it was clear that methanol showed a negative de-
viation and ethanol showed a positive deviation from the ASF behavior.
Furthermore, in the slurry reactor, the selectivity of methanol decreased
considerably and the selectivity of ethanol increased remarkably; thus,
ethanol became the major product among the resulting alcohols.
Based on the characterization analysis of the catalysts discussed above,
it is clear that different carbon tubes (inner diameter and wall thick-
ness) could modify the geometric and electronic interactions among
copper–cobalt–ceria active sites, which brings the deviations from the
ASF behavior, and the slurry reactor may be more favor for HAS than
fixed bed.
Fig. 4. (a) Cu 2p and (b) Co 2p XPS spectra of the fresh catalysts.
3
.2.2. XPS
XPS is typically employed to analyze the composition and oxidation
states of catalyst surface species. As shown in Fig. 4a, the Cu 2p3/2
spectra of the four fresh catalysts were characterized by asymmetrical
major peaks and satellite structures. Two peaks at about 932.5 and
9
34.6 eV were attributed to Cu+ and Cu2+ oxides, respectively,
and the peak at approximately 942.8 eV was assigned to the
2
+
satellite peak of Cu oxidation states [17]. It was found that the relative
2
+
area/intensity of the profiles of the Cu
oxides increased upon
4. Conclusions
increasing the CNT wall thickness; the values of Cu2 /(Cu +Cu
+
2+
+
)
are 29.8%, 46.7% and 62.1% for CuCoCe/CNT(8), CuCoCe/CNT(20),
CuCoCe/CNT(30) respectively, and 33.1% for the CuCoCe-out-
CNT(8) sample. The analysis suggested that the interaction
between metals and CNTs increased upon decreasing wall
thickness of carbon tubes and CNT(8) had the strongest interaction
with copper, which prevented most of the cuprous oxide from forming
copper oxide.
The Co 2p XPS spectra of the four fresh samples are shown in Fig. 4b.
The Co 2p3/2 main peak was observed at ~780.7 eV, along with a satellite
peak at 786.7 eV. The peak observed at 780.7 could be associated with
the Co2+ component [18], and Co 2p3/2 binding energy of CuCoCe/
CNT(8) shifted to a high energy of 0.6 and 0.5 eV relative to that of
CuCoCe/CNT(20) and CuCoCe/CNT(30), respectively. This shift indicates
We have demonstrated that ternary CuCoCe/CNT(8) catalyst
displayed a rather high selectivity for the formation of ethanol
(39.0%) and C2+ alcohols (67.9%) with a narrow range distribution
during CO hydrogenation. The smaller channels have a superior
space restriction and the thinner walls have stronger electronic
interaction between the tube surface and the confined material.
Encapsulated particles, facilitated reduction of CoO species, and
high concentrations of Co/Ce could be obtained in the narrowest
CNT channels, which contributes to the remarkable enhancement
in space-time yield and selectivity of higher alcohols. The catalytic
CO hydrogenation results show that the ternary catalyst may have
potential for scale-up in industrial applications to produce higher
alcohols.