H. Liu et al. / Molecular Catalysis 443 (2017) 69–77
71
addition of NaBH4 (25 mg). After 30 min, the reaction was quenched
by saturated NH4Cl, extracted with Et2O, dried over anhydrous
Na2SO4 and concentrated in vacuo. Dimethyl maleate (1 equiv.)
was added into the crude product as internal standard. The con-
version, yield, and dr were determined by 1H NMR. The ee were
determined by HPLC analysis on chiral OD-H or OJ-H column for
aromatic compounds or by Mosher’s MTPA method for aliphatic
compounds.
formed using the Andersen method [85] and the Berendsen method
[86], respectively. Long-range Coulombic interactions and van der
Waals interactions were computed by the Ewald summation tech-
nique. The simulation time-step was set to be 1 fs and the total
simulation time was 200 ps. All the simulations were performed
using the Discover module in the Material Studio software package
[87].
After the reaction terminated, the solid catalyst was recovered
by filtration and washed with 5 mL Et2O for three times. Then the
solid was dried in a vacuum oven at 313 K and used directly for the
next catalytic reaction.
3. Results and discussion
3.1. Structural properties of ˛-amine acid anions intercalated
LDH nanosheets
2.4. Detection of interlayer hydrophobicity
The nanosheets employed here are the brucite-like layers of
magnesium and aluminum hydroxides (Mg/Al-LDHs), calcium
and aluminum hydroxides (Ca/Al-LDHs), nickel and aluminum
hydroxides (Ni/Al-LDHs), and zinc and aluminum hydroxides
(Zn/Al-LDHs). The amine sites employed here are the amino group
in alpha-amino acid anion intercalated in the interlayer space of
LDHs. The intercalation of l-serine (Ser), l-alanine (Ala), l-leucine
(Leu), l-phenylalanine (Phe), l-tyrosine (Tyr), and 4-methy-l-
phenylalanine (Me-Phe) was performed by the co-precipitation
method and of l-proline (Pro) and ␣-methyl-l-proline (Me-Pro)
by the reconstruction method. The basal spacing is calculated
from the 003 reflection of the XRD patterns (Fig. 1, A) as 0.90,
0.88, 0.88, 1.80, 1.50, 1.82, 0.78, 0.78, 1.75, 1.65, and 1.82 nm for
Mg/Al-Ser-LDHs, Mg/Al-Ala-LDHs, Mg/Al-Leu-LDHs, Mg/Al-Phe-
LDHs, Mg/Al-Tyr-LDHs, Mg/Al-Me-Phe-LDHs, Mg/Al-Pro-LDHs,
Mg/Al-Me-Pro-LDHs, Ca/Al-Phe-LDHs, Ni/Al-Phe-LDHs, and Zn/Al-
Phe-LDHs. Subtracting the brucite-like layer thickness (0.48 nm)
from the calculated basal spacing, the interlayer spacing is esti-
mated to be 0.42, 0.40, 0.40, 1.32, 1.02, 1.34, 0.30, 0.30, 1.27,
or Mg/Al-Leu-LDHs, monolayer horizontal arrangement for Mg/Al-
Pro-LDHs or Mg/Al-Me-Pro-LDHs, bilayer vertical arrangement for
Mg/Al-Phe-LDHs, Mg/Al-Tyr-LDHs, Mg/Al-Me-Phe-LDHs, Ca/Al-
Phe-LDHs, Ni/Al-Phe-LDHs, or Zn/Al-Phe-LDHs (Fig. 1, B) in light
of the dimension of ␣-amino acid anions measured by Materials
Studio Program (Fig. S1). It is interesting that the aliphatic ␣-amino
acid anions are all arranged in monolayer and the aromatic ␣-
amino acid anions in bilayer in the interlayer regions. The M2+/Al3+
molar ratio was determined according to the ICP results as in a
narrow range of 1.78–2.22 for the LDHs intercalated with primary
␣-amino acid anions, and 2.70 for the LDHs intercalated with
l-proline or ␣-methyl-l-proline anions (Table S1). The interlayer
␣-amino acid anions were determined according to the CHN results
in the percentage of 21% to 33% for the case of monolayer arrange-
ment, and 64% to 97% for the case of bilayer arrangement (Table
S1). The rest of interlayer anions are co-existing carbonate and/or
To determine the interlayer hydrophobic microenvironment,
pyrene was used as a fluorescent probe [81]. Batch sorption experi-
ments were performed in 50-mL centrifuge tubes with Teflon-lined
screw caps. For each experiment, the Mg/Al-AA-LDHs with the
same amount of ␣-amine acid anions were dried under a flow of
dry N2 to remove any surface-bound solvent. Then 30 mL of the cor-
responding liquid phases (vwater/vmethanol = 1/1) was added to the
tubes. Pyrene was added to the tubes by direct injection of an aque-
ous solution of pyrene and kept constant at 1 M. The centrifuge
tubes were sealed and wrapped with aluminum foil to protect
them from light and placed on a wrist shaker for 24 h. The tubes
were removed from the shaker, placed horizontally on a bench,
and shaken for the following 2 days. Then the pyrene-loaded Mg/Al-
amine acid anions-LDHs were obtained by centrifugation. The solid
was dried under a flow of dry N2 and analyzed with a Shimadzu
RF-5301PC spectrometer. Samples were excited at = 335 nm and
pyrene emission spectra were recorded from 350 to 490 nm. Both
excitation and emission slit widths were set at 2.5 nm.
2.5. Structural model and molecular dynamics (MD) simulation
method
MD simulations were used to understand the arrangement of
␣-amine acid anions in the Mg/Al-LDHs interlayer space. The lat-
tice containing 18 Mg atoms and 9 Al atoms was built on the basis
of each [AlO6] octahedron surrounded by six [MgO6] and each
[MgO6] octahedron, in turn, surrounded by three [AlO6] octahe-
dron, because the ratio of Mg to Al is 2:1, which ensures that Al
atoms will not occupy adjacent octahedron. According to the liter-
ature [82,83], the lattice parameters of the 2-dimensional layer are
a = b = 3.142 Å. On the basis of the model of the host layer, a supercell
was constructed, with lattice parameter a = 28.278 Å, b = 9.426 Å,
and the initial interlayer spacing 17.960 Å for Mg2.03/Al-Phe0.79
-
LDHs and 18.170 Å for Mg2.03/Al-Me-Phe0.97-LDHs, ␣ = ˇ = 90◦,
ꢀ = 120◦ (equivalent to 9 × 3 × 1 in the a, b, and c directions). The
supercell was treated as P1 symmetry and all of lattice parameters
were considered as independent variables during the simulation.
A 3-dimensional periodic boundary condition was applied to the
system, so the simulated supercell can be repeated infinitely in
three directions. Then, for maintaining the whole system elec-
trically neutral and matching the chemical compositions, seven
l-phenylalanine anions, one carbonate ion, and twenty eight water
molecules were introduced into the simulated supercell randomly
for Mg2.03/Al-Phe0.79-LDHs and eight 4-methy-l-phenylalanine
anions, one nitrate ion, and thirty six water molecules were intro-
duced for Mg2.03/Al-Me-Phe0.97-LDHs. All MD simulations were
performed by adopting the LDHFF force field developed by Zhang
et al. [84]. After energy minimization was applied on the initial
models, MD simulations were performed in an isothermal–isobaric
(NPT) ensemble with the temperature of 298 K and the pressure of
0.1 MPa (about 1 atm). Temperature and pressure control were per-
nitrate. The asymmetric (ꢁCOOas) and symmetric vibrations (ꢁCOOs
)
of carboxylate group in the LDH nanosheets-attached ␣-amine acid
anions are resolved at 1607 and 1348 cm−1 for Mg2.03/Al-Ser0.21
-
LDHs, 1617 and 1357 cm−1 for Mg2.03/Al-Ala0.21-LDHs, 1580 and
1362 cm−1 for Mg1.78/Al-Leu0.22-LDHs, 1591 and 1354 cm−1 for
Mg2.03/Al-Phe0.79-LDHs, 1597 and 1362 cm−1 for Mg2.22/Al-Tyr0.71
-
LDHs, 1593 and 1363 cm−1 for Mg2.03/Al-Me-Phe0.97-LDHs, 1577
and 1369 cm−1 for Mg2.70/Al-Pro0.26-LDHs, 1581 and 1389 cm−1
for Mg2.70/Al-Pro0.33-LDHs, 1574 and 1361 cm−1 for Mg2.70/Al-
Pro0.33-LDHs, 1573 and 1354 cm−1 for Ca2.03/Al-Phe0.64-LDHs,
1579 and 1362 cm−1 for Ni1.78/Al-Phe0.97-LDHs, and 1577 and
1360 cm−1 for Zn1.86/Al-Phe0.66-LDHs in the FT-IR spectra (Fig. 1,
C). The ꢂꢁCOO (ꢁCOOas –ꢁCOOs) is 259, 260, 218, 237, 235, 230,
208, 192, 213, 219, 217, and 217 cm−1, respectively. The ꢂꢁCOO
of the corresponding ␣-amine acid sodium salt [88–95] is 207,