S. Leviev, et al.
MolecularCatalysis486(2020)110841
in the literature for the typical binding energy of Rh+3 [78–82]. These
findings demonstrate that the rhodium oxidation state was not changed
and kept its original form, which was derived from RhCl3, i.e +3. In
addition, the Cl2p spectrum consists of one doublet, corresponding to
binding energy of 198.72 (Fig. 5B), indicating a terminal Cl species
[80]. Finally, the observed atomic ratio of Rh:Cl in the heterogeneous
catalyst was around 3:1, as in the homogenous salt, as illustrated in
In order to better understand the specific interaction between the
RhCl3 and the ἰ, a physicochemical analysis was also employed.
Viscosity measurements of both aqueous ἰ solutions, with and without
RhCl3, were performed and are shown in Fig. 6. In general, both pre-
parations yielded typical non-Newtonian shear thinning behavior, in-
dicating that the shear stress reduces the viscosity. However, the ἰ-RhCl3
system yielded higher viscosity in comparison to the native ἰ solution.
This substantial increase in viscosity could be ascribed to screening of
intermolecular electrostatic repulsions by RhCl3, leading to a greater
degree of self-association [83].
The mechanical spectra of both aqueous solutions, i.e. the storage
(or elastic) modulus (G’) and viscous (or loss) modulus (G”), were also
measured as function of frequency (Fig. 7). It was found that in both
preparations, at low frequencies, the mechanical spectrum is similar to
that of dilute solutions (G” > G'), because there is sufficient time for the
chains’ relaxation. However, at high frequencies, there is no sufficient
time for recovery, and the solution responds as if it were a solid
(G' > G”). In addition, both prearations exhibited a crossover region,
while subjected to increasing frequencies, in which the storage modulus
Up to 10.58 Hz the neat ἰ aquaous solution showed higher G” than
G', indicating that the solution is more viscous than elastic (Fig. 7A).
However, in the range above 2.3 Hz ἰ solution with RhCl3 yielded G’
values that exceeded those of the G” (Fig. 7B). Moreover, the G’ values
of the solution with RhCl3 were higher than those that were measured
with the neat ἰ solution. Hence, the ἰ aqueous solution with RhCl3
yielded an elastic gel-like structured system with more stable structure,
probably by promoting the increased association of the chain poly-
saccharide molecules. However, the moduli is still frequency depen-
dent, and G' values are less than 10 times larger than G”, indicating that
the desired developed gels were yet to be achieved.
Indeed, specific metal ions of different valency can form non- and
specific interactions with carrageenan solutions. These interactions can
cause aggregation of different carrageenan forms, leading to more vis-
cous systems, with stabilized gel structures [[83–88]. For example, an
addition of divalent Ca2+ ion to ἰ solution has a pronounced helix-
stabilizing effect in inducing gel formation [87,89]. The Ca-sensitivity
of ἰ is attributed to the joint effect of Ca2+ ions and water molecules in
mediating a strong interaction between the sulfate groups of neigh-
Fig. 3. Infrared spectra of native ἰ-polysaccharide (black curve) and ἰ-RhCl3
(light blue curve) (For interpretation of the references to colour in this figure
legend, the reader is referred to the web version of this article).
former publication [37,39] (Fig. 4). This difference indicates that the
RhCl3 supplement caused a change in the overall new structure and
implies that the RhCl3 was interacting with the polysaccharide. It was
previously reported that addition of various cations of different valence
to the anionic sulfate groups in ἰ-carrageenan aqueous solution yields
ionic forces and can produce sol-gel by the formation of a ‘double-helix’
structure [72–75]. In addition, the cations can also interact with the
hydroxyl groups on the carrageenan structure, as previously proposed
regarding different metal cations supported on carrageenans [76].
However, though, addition of PdCl2(TPPTS)2 to ἰ, i.e., ἰ-PdCl2(TPPTS)2,
was characterized by porous and ordered surfaces, when compared
with native ἰ [37], addition of RhCl3 to ἰ, i.e., ἰ-RhCl3, yielded a much
more porous and ordered system, revealing that the interactions of the
polymer with RhCl3 are different. Moreover, while PdCl2 leached out
from the ἰ-PdCl2 system, RhCl3 showed no leaching from ἰ-RhCl3, im-
plying that the rhodium is immobilized to the surface.
Elemental analysis of the ἰ-RhCl3 catalyst was also performed, using
SEM-EDS (Fig. 4). As expected, the analysis indicated that RhCl3 was
embedded within the ἰ, with molar elemental ratio of Cl:Rh 3:1 as de-
rived from the homogenous salt.
A surface-sensitive technique, XPS, was also applied to analyze the
surface composition of the ἰ-RhCl3 in comparison to the native ἰ. As seen
in Table 3, there was no significant difference between the atomic basic
elemental ratios and the peak of their binding energies in both samples.
In general, the C1 s XPS spectra for each sample could be decomposed
into three main contributions at different binding energies (BE), which
are associated with different types of elements that are linked to the
carbon atoms: aliphatic carbons, CeO and OeCeO, and R-SO3–. In
addition, the S2p3 could be composed into two different elements,
which are associated with the R-SO3– binding, depending on the R
structure [77]. Indeed, all these assignments are in accordance to the
polysaccharide structure. Therefore, the XPS analyses clearly demon-
strated that no new covalent bonds were formed between the poly-
saccharide and the rhodium chloride during the xerogel preparation.
As expected, the surface area of ἰ-RhCl3 contained rhodium, whereas
no rhodium was present in the native ἰ (Table 3). This is evidence that
the rhodium was successfully embedded into the polysaccharide matrix.
Moreover, the Rh3d doublet (Fig. 5A) represents a single rhodium state
with a Rh3d5/2 binding energy of 309.92 eV, which is in good agree-
ment with the values in the range of 309.7–310.3 eV that were reported
4. Conclusions
To conclude, RhCl3 was sucessfuly immobilized to ἰ in a very simple
and straightforward method, and was sucessfuly employed in a Suzuki
cross-coupling reaction. In addition, the salt did not leach out to the
reaction mixture and the catalyst was successfully recycled with an
increase in activity in first and the second recycles. Furthermore, the
characterization of the lyophilized ἰ-RhCl3 system showed that although
there is probably no new bond between the salt and the polymer, as
demonstrated by FTIR, the salt is embedded whithin the support.
Furthermore, SEM images show that addition of RhCl3 to ἰ yielded a
more porous and ordered structure in comparison to native ἰ, implying
on an interaction between the two. Additionally, XPS analysis showed a
typical binding energy of Rh+3 where the atomic ratio of Rh:Cl in the
heterogeneous catalyst was around 3:1. Finally, viscosity measurements
also revealed that RhCl3 interacts with the polysachride, as addition of
RhCl3 to aquaous ἰ solution reslted in increase of viscosity. Thus, it was
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