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Pillar-assisted construction of 3D framework from 2D bilayer based on Zn/Cd hetero-metal cluster: pore tuning and gas adsorption danhua song, haiyang hou, Yu-Jie Gao, Feilong Jiang, Daqiang Yuan, Qihui Chen, Linfeng Liang, dong wu, and Maochun Hong Cryst. Growth Des., Just Accepted Manuscript • DOI: 10.1021/acs.cgd.7b01694 • Publication Date (Web): 01 Feb 2018 Downloaded from http://pubs.acs.org on February 2, 2018
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Crystal Growth & Design
1
Pillar-assisted construction of 3D framework from 2D bilayer based on Zn/Cd
2
hetero-metal cluster: pore tuning and gas adsorption
3
4
Danhua Song,a, b Haiyang Hou, a, b Yu-Jie Gao, a, b Feilong Jiang,b Daqiang Yuan, b
5
Qihui Chen,*a, b Linfeng Liang, b Dong Wu,b and Maochun Hong* a, b
6
a
College of Chemistry, Fuzhou University, Fuzhou, 350002, China
7
b
Key Laboratory of Coal to Ethylene Glycol and Its Related Technology, State Key
8
Laboratory of Structure Chemistry, Fujian Institute of Research on the Structure of
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Matter, Chinese Academy of Sciences, Fuzhou, Fujian, 350002, China
10
Abstract
11 12
Employing rational design strategy to construct porous MOFs with predictable
13
structures for specific application still remains one of the most compelling challenges.
14
Here, a novel 2D bilayer (FJI-H16) based on Zn/Cd hetero-metal clusters has been
15
constructed throughout hetero-metal strategy, further introducing pillar ligands with
16
different sizes and flexibility expand such 2D bilayer structure into two novel 3D
17
frameworks (FJI-H17, FJI-H18), in which both of pore sizes and flexibility of the
18
new-formed 3D frameworks can be tuned. Further gas adsorption researches indicate
19
that the less porous FJI-H16 has highest H2 adsorption while the much porous
20
FJI-H17 has highest CO2 adsorption. The relationship between gas adsorption
21
properties and pore characteristics also has been investigated, which will provide a
22
potential strategy that can improve the gas adsorption in designing porous MOFs.
23 24
Keyword: metal-organic framework, 2D bilayer, hetero-metal clusters, pore tuning,
25
gas adsorption
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Introduction
2
Metal-organic frameworks (MOFs), which are crystalline solids constructed via
3
self-assembly of single metal cation or metal clusters and organic ligands having
4
multiple binding sites, have been researched extensively not only due to their
5
fascinating structures but also the potential applications in gas storage, separation and
6
catalyses and so on.1-12 Generally speaking, these functions mainly depend on the pore
7
characteristics of MOFs, including pore sizes, the window metrics. For example,
8
introduction of specific functional group into MOFs will lead to corresponding
9
properties;
13-16
introduction of specific templates or tuning pores can improve
10
adsorption capacity and selectivity.17-22 Thus, the design of MOF structure with
11
predictable pore characteristic is highly critical for the synthesis of MOFs material
12
with desired properties. However, employing rational design strategy to construct
13
predictable porous MOFs still remains one of the most compelling challenges for
14
chemists.
15
To achieve MOFs with tunable pore sizes from micro-pore to meso-pore,
16
various strategies have been used23,24 and pillar-assisted strategy that employing
17
different organic linkers to systematically change size of pore has been proved as an
18
effective route to controllably prepare porous MOF materials.22,25-41 By this way, the
19
pore structures of a wide variety of MOFs can be predicted and tuned. However, to
20
the best of our knowledge, almost of pillared-layer MOFs are assembled from
21
traditional paddle-wheel M2(RCOO)4 metal clusters, so new Secondary building units
22
(SBUs) for construction of pillared-layer MOFs should be designed and synthesized.
23
Here in, a novel 2D bilayer (FJI-H16) based on Zn/Cd hetero-metal clusters has been
24
constructed throughout hetero-metal strategy, further introducing pillar ligands with
25
different sizes and flexibility expand such 2D bilayer structure into two novel 3D
26
frameworks (FJI-H17, FJI-H18), in which both of
27
new-formed 3D frameworks can be tuned. Further gas adsorption researches indicate
28
that the less porous FJI-H16 has highest H2 adsorption while the much porous
29
FJI-H17 has highest CO2 adsorption. The relationship between gas adsorption
pore sizes and flexibility of the
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Crystal Growth & Design
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properties and pore characteristics including size, chemical character, and flexibility
2
also has been investigated.
3
Experimental Section
4
General Procedures and Materials. All chemicals and solvents used were purchased
5
from commercial sources and used without further purification. The C, H, and N
6
micro analyses were performed using an Elementar Vario MICRO elemental analyzer.
7
The power X-ray diffraction (PXRD) data were collected on a Cu-Ka radiation
8
equipped RIGAKU DMAX 2500 diffractometer at room temperature. Thermal
9
gravimetric analyzer-mass spectrometry (TG-MS) was performed on a Netzsch STA
10
449C instrument and a Balzers MID instrument heated from room temperature to
11
1000 oC under a nitrogen atmosphere. Gas Sorption Measurements were measured on
12
a Micromeritics ASAP 2020 surface area analyzer.
13
Synthesis of FJI-H16. Dissolving Zn(NO3)2·6H2O (0.10 mmol, 30 mg),
14
Cd(NO3)2·4H2O (0.1 mmol, 30 mg) with ligand H3BTB (0.05 mmol, 22 mg) in a
15
mixture of 4mL DEF and 6mL ethanol solvent, then heating this solution at 85℃ for
16
4 days, after that, colorless rod-shaped crystals of FJI-H16 were obtained in a yield of
17
66%. Anal. calcd for [Zn2Cd(BTB)2(H2O)2]·0.5DEF·4H2O: C, 53.28; H, 3.84; N, 0.55.
18
Found: C, 52.90; H, 3.82; N, 0.61. FT-IR (KBr pellets, cm
19
1451, 1387, 1264, 1213, 1108, 1018, 847, 779, 702, 484.
20
Synthesis of FJI-H17. Dissolving H3BTB (0.05 mmol, 22 mg) 、Zn(NO3)2·6H2O
21
(0.10 mmol, 30 mg)、Cd(NO3)2·4H2O (0.10 mmol,30 mg) and BPY(0.1 mmol, 16 mg)
22
in 6mL DMA and 3mL H2O, then heating this solution at 85℃ for 4 days, after that,
23
colorless crystals of FJI-H17 were prepared in a yield of 66%. Anal. calcd for for
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[Zn2Cd(BPY)(BTB)2]·3H2O·3DMA: C, 57.53; H, 4.57; N, 4.41. Found: C, 57.73; H,
25
4.41; N, 4.61. FT-IR (KBr pellets, cm−1): 1705, 1602, 1547, 1384, 1180, 1015, 860,
26
784, 706, 550, 471.
27
Synthesis of FJI-H18. Dissolving H3BTB (0.05 mmol, 22 mg) 、Zn(NO3)2·6H2O
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): 1662, 1598, 1551,
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(0.10 mmol, 30 mg)、Cd(NO3)2·4H2O (0.10 mmol,30 mg) and BPE (0.1 mmol, 18 mg)
2
in 6mL DMA and 3mL H2O, then heating this solution at 85℃ for 4 days, after that,
3
colorless crystals of FJI-H18 were synthesized in a yield of 62%. Anal. calcd for
4
[Zn2Cd(BPE)(BTB)2]·(2DMA·5H2O): C, 56.92; H, 4.45; N, 3.59. Found: C, 56.58; H,
5
4.20; N, 4.06. FT-IR (KBr pellets, cm−1): 1611, 1551, 1389, 1182, 1015, 855, 811, 782,
6
704, 550, 475.
7
X-ray crystallography. Data collections were all performed on a Mercury CCD
8
diffractometer with graphite monochromated CuKa radiation (λ = 0.71073 Å). The
9
structures were solved by direct methods, and all calculations were performed using
10
the SHELXL package. The structures FJI-H16-18 were refined by full matrix
11
least-squares with anisotropic displacement parameters for non-hydrogen atoms. All
12
hydrogen atoms were generated geometrically and treated as riding. The
13
crystallographic data are summarized in Table S1. CCDC numbers (1588923-1588925)
14
contain the supplementary crystallographic data for FJI-H16-18. These data can be
15
obtained free of charge from The Cambridge Crystallographic Data Centre via
16
www.ccdc.cam.ac.uk/data_request/cif.
17
Results and Discussion
18 19 20
In order to develop new SBU, Zn and Cd metal ions with different sizes but
21
similar coordination character have been selected as metal connectors, and H3BTB
22
has been selected as organic ligand due to its better directionality and rigidity (Figure
23
1a). Here in, a novel 2D bilayer structure (FJI-H16) based on Zn/Cd hetero-metal
24
cluster has been prepared. Reaction of Zn(NO3)2·6H2O, Cd(NO3)2·4H2O and ligand
25
H3BTB in a mixture of DEF and ethanol at 85℃ for 4 days affords rod-shaped
26
crystals
27
[Zn2Cd(BTB)2(H2O)2]·0.5DEF·4H2O. Single-crystal X-ray diffraction analyses reveal
28
the FJI-H16 crystallizes in the P63/mmc space group. Its asymmetric unit contains
of
FJI-H16
with
66%
yield
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,
formulated
as
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Crystal Growth & Design
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one sixth of independent Zn(II) ion, one third of independent Cd(II) ion, and one third
2
of deprotonated BTB ligand (Figure S1). Figure 1b illustrates the geometry of the
3
Zn/Cd hetero-metal cluster (Zn2Cd(COO)6(H2O)2). Each cadmium ion is chelated by
4
six Carboxylate oxygen atoms from six different BTB ligands with a distorted
5
octahedral geometry. Each of the two symmetry terminal Zn atoms is bound to three
6
carboxylate oxygen atoms from different BTB ligands and one oxygen atom from the
7
coordinated water with four-coordinate mode. The Zn-O bond distance ranges from
8
1.9305(12) to 1.966(3) Å and the Cd-O distance is 2.2828(12) Å. These Zn/Cd
9
hetero-metal clusters (Zn2Cd(COO)6(H2O)2) further link with BTB ligands to form an
10
infinite 2D bilayer structure (Figure 1c-d). Here in, BTB ligands comprised of bilayer
11
structure are parallel to each other with a distance of 3.524Å. These 2D bilayers
12
further stack into a 3D framework in the way of ABAB through π-π interaction (3.544
13
Å) (Figure 1e-f). PLATON calculation demonstrates that the solvent accessible
14
volume of FJI-H16 is 41.4%.
15
16
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Figure 1 The structure of FJI-H16. a) The structure of BTB ligand. b) The structure
2
of Zn/Cd hereto-metal cluster: Zn2Cd(COO)6(H2O)2.
3
viewed from different directions. e-f) The 3D framework viewed from different
4
directions. (Grey balls represent C atoms, red balls represent O atoms, yellow balls
5
represent Cd atoms, and cyan balls represent Zn atoms.)
c-d) The 2D bilayer structure
6 7
As mentioned above, almost of pillared-layer MOFs are assembled from traditional
8
paddle-wheel metal clusters M2(RCOO)4, such SBUs only lead to 2D single layer
9
structure. Here in, using the Zn/Cd hetero-metal clusters as SBUs can construct more
10
complex 2D bilayer structure, which will provide a new SBU for rational construction
11
of more diverse porous MOFs with predictable structures. (Scheme 2)
12
13 14
Scheme 1 The comparison between different 2D layer structures. a) The 2D single
15
layer structure based on traditional paddle-wheel metal clusters. b) The 2D bilayer
16
structure based on Zn/Cd hetero-metal clusters.
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Crystal Growth & Design
1
If the coordinated water comprised in Zn2Cd(COO)6(H2O)2 clusters (Figure 1b)
2
can be displaced by additional pillar ligands, such bilayer structure can further extend
3
into 3D framework driven by different pillar ligands as shown as Scheme 2a.
4
Therefore, a series of pyridine derivatives with different sizes from 2.8 Å to 11.1 Å,
5
including Pyrazine (2.8 Å), 4, 4'-Bipyridine (7.0 Å), trans-1,2-Bis(4-pyridyl)ethane
6
(9.3 Å),
7
have been tried as pillar ligands, and two novel 3D frameworks (FJI-H17 and
8
FJI-H18) based on 4, 4'-Bipyridine (BPY) and trans-1,2-Bis(4-pyridyl)ethane (BPE)
9
have been synthesized respectively. (Scheme 2)
1,2-Di(pyridin-4-yl)ethyne (9.6 Å), 1,4-Bis(pyrid-4-yl)benzene (11.1 Å),
10
11 12
Scheme 2 Construction of 3D frameworks driven by different pillar ligands.
13 14
Reaction of Zn(NO3)2·6H2O, Cd(NO3)2·4H2O, ligand H3BTB, auxiliary ligand
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BPY in a mixture of DMA and H2O at 85℃ for 4 days affords rod-shaped crystals of
2
FJI-H17, formulated as [Zn2Cd(BPY)(BTB)2]·3H2O·3DMA. X-ray diffraction
3
analyses indicate that FJI-H17 belongs to the monoclinic space group C2/c. Its
4
asymmetric unit contains an independent Zn(II) ion, half of independent Cd(II) ion, a
5
deprotonated BTB ligand, and half of BPY ligand (Figure S2). Figure 2a illustrates
6
the geometry of the new formed Zn/Cd hetero-metal cluster Zn2Cd(COO)6(BPY)2, in
7
which water molecules are displaced by pillar BPY ligands as we expected. Compared
8
with Zn2Cd(COO)6(H2O)2 clusters (Figure 1a), the Zn2Cd(COO)6(BPY)2 cluster has a
9
little distorted, each Cd atom is chelated by six carboxylate oxygen atoms from
10
different ligands with six-coordinate mode, while Zinc ion is chelated by three
11
carboxylate oxygen atoms from different ligands and a nitrogen atom from BPY
12
ligand with a four-coordinated mode. The Zn-O bond distance ranges from 1.931(3)
13
to 1.946(3) Å and the Cd-O distance ranges from 2.278(3) to 2.305(3) Å, and the
14
Zn-N distance is 2.034(4) Å. Such Zn2Cd(COO)6(BPY)2 clusters further link with
15
BTB ligands to form an a little twist infinite 2D bilayer structure with weaker π-π
16
interaction (3.865 Å) (Figure 2b). The pillar BPY ligands further link these 2D
17
bilayers into 3D framework as shown as Figure 3c with a distance of 7.0 Å. The
3D
18
structure
interpenetrates
with another
3D
19
two-fold
interpenetrated
structure, in which the intermolecular π-π distance
20
between two isolated 3D structure is 5.894 Å. Although FJI-H17 has a two-fold
21
interpenetrated structure, PLATON calculation demonstrates that the solvent
22
accessible volume of FJI-H17 is also up to 43.6%, a little larger than that of
23
FJI-H16.
one
to
24
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access
to
a
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Crystal Growth & Design
1 2
Figure 2 The structure of FJI-H17. a) The structure of new-form Zn/Cd hereto-metal
3
cluster [Zn2Cd(COO)6(BPY)2]. (For clarity, only N atoms have been presented.) b)
4
The 2D bilayer structure based on [Zn2Cd(COO)6(BPY)2] clusters. c) The 3D
5
framework based on 2D bilayer structures. d) The two-fold intercatenated structure
6
based on 3D frameworks. (Grey balls represent C atoms, red balls represent O atoms,
7
yellow balls represent Cd atoms, and cyan balls represent Zn atoms.)
8
A similar 3D metal-organic framework (FJI-H18) is also obtained by
9
introducing BPE ligand to replace the coordinated H2O molecule of the original
10
Zn2Cd(COO)6(H2O) cluster. Reaction of Zn(NO3)2·6H2O, Cd(NO3)2·4H2O, ligand
11
H3BTB, auxiliary ligand BPE in a mixture of DMA and H2O at 85℃ for 4 days
12
affords
13
[Zn2Cd(BPE)(BTB)2]·(2DMA·5H2O). X-ray diffraction analyses indicate that
14
FJI-H18 belongs to the triclinic space group P-1. Its asymmetric unit contains two
15
independent Zn(II) ions, one independent Cd(II) ion, two deprotonated BTB ligands,
16
and one BPE ligand (Figure S3). Figure 3a illustrates the geometry of the new formed
rod-shaped
crystals
of
FJI-H18,
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formulated
as
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Zn/Cd hetero-metal cluster Zn2Cd(COO)6(BPE)2, which is similar with that of
2
FJI-H17 except for more distorted. The Zn-O bond distance ranges from 1.9173(13)
3
to 1.9393(13) Å and the Cd-O distance ranges from 2.2747(13) to 2.3096(12) Å, and
4
the
5
Zn2Cd(COO)6(BPE)2 clusters further link with BTB ligands to form a more twist
6
infinite 2D bilayer structure with weak π-π interaction (3.785 Å) as shown as Figure
7
3b. The pillar BPE ligands further link these 2D bilayers into a 3D framework as
8
shown as Figure 3c with a distance of 9.3 Å. The 3D structure also interpenetrates
9
with another one to give access to a 3D two-fold interpenetrated structure (Figure 3d),
10
in which the intermolecular π-π distance between two isolated 3D structure is 8.397 Å.
11
PLATON calculation demonstrates that the solvent accessible volume of FJI-H18 is
12
51.5%, highly larger than that of FJI-H16 and FJI-H17.
Zn-N
distance
ranges
from
2.0250(17)
to
2.0284(16)
Å.
Such
13
14 15
Figure 3 The structure of FJI-H18. a) The structure of new-formed Zn/Cd
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Crystal Growth & Design
1
hereto-metal cluster Zn2Cd(COO)6(BPE)2. (For clarity, only N atoms have been
2
presented.)
3
framework based on 2D bilayer structures. d) The two-fold intercatenated structure
4
based on 3D frameworks. (Grey balls represent C atoms, red balls represent O atoms,
5
yellow balls represent Cd atoms, and cyan balls represent Zn atoms.)
b) The 2D bilayer structure based on Zn2Cd(COO)6(BPE)2. c) The 3D
6
Using hetero-metal strategy lead to a new Zn/Cd hetero-metal cluster comprised
7
in a novel 2D bilayer structure (FJI-H16); further driven by different pillar ligands,
8
another two 3D frameworks (FJI-H17-18) have been constructed as we expected.
9
Here in, attempts to directly obtain FJI-H17 and 18 based on crystals of FJI-H16 are
10
failed. After expanding by pillar ligands, both of FJI-H17 and FJI-H18 show larger
11
solvent accessible volumes even that both of them have two-fold interpenetrated
12
structures, and the FJI-H18 has the largest solvent accessible volume due to the
13
longer pillar ligand. Furthermore, introduction of pillar ligand also improve their
14
flexibility and reduce their structure symmetry.
15
To check the permanent porosities of FJI-H16, 17, 18, the freshly prepared
16
samples are soaked in ether to exchange the less volatile solvents, followed by
17
evacuation under a dynamic vacuum at 100 oC for 10 h, generating dehydrated forms.
18
PXRD data display that their crystallinity are finely kept after activation (Figure S5).
19
As shown in Figure 4, all of desolvated samples display typical type-I adsorption
20
isotherms, suggesting the retention of the micro-porous structures after the removal of
21
solvents from the crystalline samples. The adsorption tests show that the highest N2
22
adsorption capacity of the FJI-H16, 17, 18 is 193.0 cm3·g-1, 197.8cm3·g-1, 98.7
23
cm3·g-1
24
Brunauer-Emmett-Teller (BET) specific surface area is 684.2,774.9,345.5 m2g-1, and
25
the corresponding Langmuir specific surface area is 836.4, 841.7, 405.8 m2g-1
26
respectively.
27
than FJI-H16 and FJI-H17 even that it has larger solvent accessible volumes
28
calculated by PLATON, which may result from following factors: the pillared ligand
29
comprised in FJI-H18 is more flexible than FJI-H17, which will lead to possible
respectively.
By
model
calculation,
the
corresponding
The FJI-H18 shows significantly lower (BET) specific surface area
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1
framework contraction, then N2 molecules is hardly to diffuse into its channels. After
2
expanding by pillar ligands, the pore sizes of both of new-formed 3D frameworks
3
(FJI-H17, 18) indeed enlarge. (Figure S6)
4 5
Figure 4 N2 adsorption isotherms of FJI-H16, 17, 18 at 77 K
6
H2 as an effective clean energy has attracted more and more attention, however,
7
the storage and transportation are still obstacles. MOFs which possess ordered pore
8
structures and high surface areas are considered to be effective candidates for storage
9
of H2.6 So we firstly investigate the hydrogen adsorption based on desolvated
10
FJI-H16, 17, 18. The H2 adsorption isotherms are carried out at 77 K, as shown as
11
Figure 5a-c, desolvated FJI-H16, 17, 18 exhibit the classical reversible type-I
12
isotherms for H2, and their total amount is 149.7 cm3 g−1 (1.34 wt%, 6.68 mmolg-1),
13
139.0 cm3 g−1 (1.24 wt%, 6.20 mmol g-1), and 77.7 cm3 g−1 (0.69 wt%, 3.45 mmol g-1)
14
respectively. FJI-H16 and FJI-H17showed a significantly larger H2 adsorption
15
capacity than FJI-H 18, and FJI-H16 is a little larger than FJI-H17. In addition, the
16
H2 adsorption value for FJI-H16 is also higher many famous reported metal organic
17
frameworks which have similar (BET) specific surface area as FJI-H16. 6 The higher
18
H2 adsorption for FJI-H16 may result from following two factors: 1) after activation,
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Crystal Growth & Design
1
a large number of open metal sites of FJI-H16 will promote H2 adsorption; 2)
2
stronger π-π interactions comprised in FJI-H16 may improve the interaction between
3
H2 molecules and MOF framework (Table S2), The significantly lower H2 uptake for
4
FJI-H18 may also due to its possible framework contraction after activation.
5
6 7
Figure 5 H2 adsorption isotherms at 77K. a-c) represents FJI-H16, 17, 18
8
respectively.
9
Considering the rapid increase of CO2 emission, there is a constant need for
10
materials which can effectively eliminate CO2, and MOF materials have been proved
11
as cost-effective and efficient porous material for CO2 capture.2 So the measurements
12
on CO2 adsorption and selectivity against N2 based on desolvated FJI-H16, 17, 18
13
also have been carried out. The CO2 and N2 adsorption isotherms are carried out at
14
273 K. As shown as Figure 6a-c, desolvated FJI-H16, 17, 18 exhibit the classical
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1
reversible type-I isotherms for CO2 and N2, and their total amount of CO2 uptake is
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78.5 cm3 g-1 (3.50 mmol g-1, 154.2mg g-1), 92.0 cm3 g−1 (4.10 mmol g-1, 180.4mg g-1),
3
and 53.4 cm3 g−1 (2.37 mmol g-1, 104.28mg g-1) respectively at 273 K and 1 atm. By
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the ideal adsorbed solution theory (IAST), the CO2/N2 selectivity of FJI-H16, 17, 18
5
for the 15/85 CO2/N2 mixture at 1 atm and 273 K is calculated to be 80, 79, and 60
6
respectively. The FJI-H17 shows a larger CO2 adsorption capacity than FJI-H16 and
7
FJI-H18 due to its much porous, which can be comparable with many famous
8
metal-organic porous compounds.2 All of three compounds display high CO2/N2
9
selectivity due to their ultra-microporous structures, in which the pore size
10
distribution of FJI-H16, 17, 18 are mainly focus on 5.9, 7.3, 6.8 Å respectively. Such
11
limited ultra-micropores prefer to allow passage of smaller CO2 molecules and
12
exclude larger N2 molecules.
13 14
Figure 6 The CO2 and N2 adsorption isotherms of FJI-H16, 17, 18 at 273 K. a-c)
15
represents FJI-H16, 17, 18 respectively. d) The CO2/N2 selectivity of FJI-H16, 17,
16
18 for the 15/85 CO2/N2 mixture at 1 atm and 273 K.
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Conclusions
1 2
In conclusion, employing rational design strategy in the construction of porous
3
MOFs with predictable structures for specific application still remains one of the most
4
compelling challenges for chemists. Here in, a novel 2D bilayer (FJI-H16) based on
5
Zn/Cd hetero-metal clusters has been constructed throughout hetreo-metal strategy,
6
introducing pillar ligands with different size and flexibility expand such bilayer
7
structure into another two much porous 3D frameworks (FJI-H17, FJI-H18), in
8
which the pore sizes have been enlarged and flexibility of frameworks have been
9
changed. Further researches indicate that the less porous FJI-H16 has highest H2
10
adsorption, while much porous FJI-H17 has highest CO2 adsorption. Such different
11
gas adsorption properties are due to their different pore characteristics including size,
12
chemical character, and flexibility, which will provide a potential strategy that can
13
improve the gas adsorption in designing porous MOFs.
14
ASSOCIATED CONTENT
15
Electronic Supplementary Information (ESI) available: Additional Crystallographic
16
data, Figures, TGA spectra and PXRD for FJI-H16-18. CCDC numbers
17
(1588923-1588925) contain the supplementary crystallographic data for FJI-H16-18.
18
AUTHOR INFORMATION
19
Corresponding Author
20
Maochun Hong
21
*E-mail:
[email protected] 22
Qihui Chen
23
*E-mail:
[email protected] 24
D. Song and H. Hou contributed equally to this work.
25
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1
The authors declare no competing financial interest.
2
ACKNOWLEDGEMENTS
3
Dedicated to professor Xin-Tao Wu on the ocassion of his 80th birthday. This work
4
was supported by the "Strategic Priority Research Program" of the Chinese Academy
5
of Sciences (XDB20000000), the 973 Program (2014CB932101), National Natural
6
Science Foundation of China (21471148, 21731006, 21390392),
7
Innovation Promotion Association CAS.
and the Youth
8 9
References
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"For Table of Contents Use Only" Pillar-assisted construction of 3D framework from 2D bilayer based on Zn/Cd hetero-metal cluster: pore tuning and gas adsorption Danhua Song, Haiyang Hou, Yu-Jie Gao, Feilong Jiang, Daqiang Yuan, Qihui Chen, * Linfeng Liang, Dong Wu, and Maochun Hong* TOC graphic
Synopsis Two novel three-dimensional frameworks with different pore sizes and flexibility have been constructed from a new-formed two-dimensional bilayer structure based on pillar-assisted strategy. Their pores characteristics and gas adsorption properties have been investigated, which will provide a potential strategy that can improve the gas adsorption in designing porous MOFs.
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