Baoyong Zhu1, Jian-Wei Cao2, Soumya Mukherjee3, Tony Pham4, Tao Zhang2, Teng Wang2, Xue Jiang2, Katherine A Forrest4, Michael J Zaworotko3, Kai-Jie Chen2. 1. School of Chemistry and Chemical Engineering, Dezhou University, Dezhou 253023, P.R. China. 2. Key Laboratory of Special Functional and Smart Polymer Materials of Ministry of Industry and Information Technology, Xi'an Key Laboratory of Functional Organic Porous Materials, School of Chemistry and Chemical Engineering, Northwestern Polytechnical University, Xi'an, Shaanxi 710072, P.R. China. 3. Bernal Institute, Department of Chemical Sciences, University of Limerick, Limerick V94 T9PX, Republic of Ireland. 4. Department of Chemistry, University of South Florida, 4202 East Fowler Avenue, CHE205, Tampa, Florida 33620-5250, United States.
Abstract
Ethylene production from C2 hydrocarbon mixtures through one separation step is desirable but challenging because of the similar size and physical properties of acetylene, ethylene, and ethane. Herein, we report three new isostructural porous coordination networks (NPU-1, NPU-2, NPU-3; NPU represents Northwestern Polytechnical University) that are sustained by 9-connected nodes based upon a hexanuclear metal cluster of composition [Mn6(μ3-O)2(CH3COO)3]6+. NPU-1/2/3 exhibit a dual cage structure that was systematically fine-tuned in terms of cage size to realize selective adsorption of C2H2 and C2H6 over C2H4. Dynamic breakthrough experiments demonstrated that NPU-1 produces ethylene in >99.9% purity from a three-component gas mixture (1:1:1 C2H2/C2H4/C2H6). Molecular modeling studies revealed that the dual adsorption preference for C2H2 and C2H6 over C2H4 originates from (a) strong hydrogen-bonding interactions between electronegative carboxylate O atoms and C2H2 molecules in one cage and (b) multiple non-covalent interactions between the organic linkers of the host network and C2H6 molecules in the second cage.
Ethylene production from C2 hydrocarbon mixtures through one separation step is desirable but challenging because of the similar size and physical properties of acetylene, ethylene, and ethane. Herein, we report three new isostructural porous coordination networks (NPU-1, NPU-2, NPU-3; NPU represents Northwestern Polytechnical University) that are sustained by 9-connected nodes based upon a hexanuclear metal cluster of composition [Mn6(μ3-O)2(CH3COO)3]6+. NPU-1/2/3 exhibit a dual cage structure that was systematically fine-tuned in terms of cage size to realize selective adsorption of C2H2 and C2H6 over C2H4. Dynamic breakthrough experiments demonstrated that NPU-1 produces ethylene in >99.9% purity from a three-component gas mixture (1:1:1 C2H2/C2H4/C2H6). Molecular modeling studies revealed that the dual adsorption preference for C2H2 and C2H6 over C2H4 originates from (a) strong hydrogen-bonding interactions between electronegative carboxylate O atoms and C2H2 molecules in one cage and (b) multiple non-covalent interactions between the organic linkers of the host network and C2H6 molecules in the second cage.
Ethylene (C2H4) is one of the most important
industrial products, with production levels of >150 million tons in
2016.[1] The energy footprint needed to purify
ethylene and propylene (C3H6), another high-volume
product, means that they collectively account for ca. 0.3% of global
energy.[2] Currently, C2H4 is mainly produced by steam-cracking reaction of carbon-included
feedstocks, and high-purity ethylene is afforded by energy-intensive
separation processes of downstream C2 hydrocarbon gas mixtures.[3] Acetylene (C2H2) is first
removed by catalytic hydrogenation using noble metal catalysts at
high temperature and pressure, whereas ethane is later separated from
C2H4 by cryogenic distillation. A transition
to a more energy-efficient separation technology with a much lower
energy footprint and simplified separation process (e.g., simultaneous
removal of C2H2 and C2H6 in one step) for ethylene production would be of societal relevance.Physisorption-based separation processes hold the promise for greatly
reducing energy consumption of gas separation, thanks to the low regeneration
temperature and fast sorption kinetics typical of physisorbents.[4] Porous coordination networks based upon metal–organic
materials (MOMs),[5] also known as metal–organic
frameworks (MOFs)[6,7] and porous coordination polymers
(PCPs),[8] have emerged as promising C2 light
hydrocarbonphysisorbents due to their amenability to exquisite control
of pore shape and chemistry through reticular chemistry and crystal
engineering strategies.[9,10] In this context, recent progress
has been made with respect to binary separations such as C2H2/C2H4 and C2H6/C2H4.[11−32,32] Simultaneous removal of both
C2H2 and C2H6 in a single
step would simplify the purification of C2H4 but remains a challenge for a single physisorbent. This is because
the quadrupole moment and kinetic diameter for C2H4 (1.5 × 10–26 esu cm2 and
4.1 Å) sit between those of C2H2 (7.2 ×
10–26 esu cm2 and 3.3 Å) and C2H6 (0.65 × 10–26 esu cm2 and 4.4 Å). These physicochemical properties exacerbate
the challenge for one-step C2H4 production from
C2H2 and C2H6 by either
molecular sieving or thermodynamic selectivity. Thus far, we are aware
of only three literature reports of C2H4 production
from a C2H2–C2H4–C2H6 mixture in a one-step process.
In 2018,[33] simultaneous trapping of C2H2 and C2H6 was realized
by the MOF TJT-100 thanks to the hierarchy of weak sorbent–sorbate
interactions. In 2019,[34] we introduced
the concept of synergistic sorbent separation technology (SSST) to
enable high-purity ethylene production from the ternary mixture (C2H2–C2H4–C2H6) and quaternary mixture (C2H2–C2H4–C2H6–CO2) by using tandem packing of three MOMs
in a fixed-bed sorbent. In SSST, three benchmark sorbents (SIFSIX-3-Ni, TIFSIX-2-Cu-i, and Zn-atz-ipa) were selected
for CO2, C2H2, and C2H6 removal, respectively. Most recently,[35] a Th-azole network (Azole-Th-1) enabled selective
adsorption of ethane and acetylene over ethylene. The discovery of
new physisorbents that enable selective adsorption of C2H2 and C2H6 over C2H4 is timely not just to address the practical utility of such
sorbents but also to advance our understanding of C2H2, C2H4, and C2H6 binding sites in porous materials.In this contribution, we introduce the new hexanuclear Mn cluster
[Mn6(μ3-O)2(CH3COO)3]6+ and its use as a building block for
three isostructural 9-connected (9-c) MOMs with varying pore size.
The hexanuclear metal cluster can be viewed as a fusion of two well-known
trinuclear metal clusters bridged by three acetate anions. The Mn6 cluster reported herein has the potential to sustain 12-c
networks, whereas the trinuclear parent typically serves as a 3-c,
6-c, or 9-c node (Scheme ).[36−41] The linking of the Mn6 cluster by rigid dicarboxylate
linker ligands (BDC = 1,4-benzenedicarboxylate; NPDC = naphthalene-2,6-dicarboxylate;
BPDC = biphenyl-4,4′-dicarboxylate) and the 3-connected pyridyl-based
tritopic ligand 2,4,6-tris(4-pyridyl)pyridine (Tripp) afforded
three isostructural MOMs (NPU-1, NPU-2,
and NPU-3; NPU = Northwestern Polytechnical University)
with tunable pore size and pore chemistry. We report herein the C2
sorption and separation properties of these new sorbents.
Scheme 1
M3(μ3-O) Metal Clusters Are Well Studied
and Have Previously Been Used to Construct 3-, 6-, or 9-Connected
Porous Coordination Networks (Left); Augmented 9-Connected Networks
Are Reported Herein from a New Mn6(μ3-O)2 Cluster (Right)
Results and Discussion
Single crystals of NPU-1, NPU-2, and NPU-3 were harvested following solvothermal reaction of manganeseacetate tetrahydrate, Tripp, and a dicarboxylic acid ligand (H2BDC, H2NPDC, or H2BPDC) in N,N-dimethylacetamide (DMA) at 373 K. Single-crystal
structure analysis revealed that the three materials are isostructural
3D networks based on the aforementioned hexanuclear Mn6 cluster. The novel Mn6 cluster can be regarded as the
result of fusion of two M3(μ3-O) clusters
through bridging acetate anions. Each manganese cation adopts an octahedral
geometry through coordination with two oxygen atoms from two dicarboxylate
ligands, two oxygen atoms from acetate anions, one μ3-O atom, and one nitrogen atom from Tripp (Supplementary Figure 1). Overall charge neutrality of these networks requires
mixed-valence MnIII and MnII cations, which
is supported by X-ray photoelectron spectroscopy (XPS) analysis (Supplementary Figure 2) and suggests electron
delocalization. Unsuccessful ion-exchange experiments with charged
dye molecules were conducted upon NPU-1 and NPU-3, indicating an absence of extra-framework counterions (Supplementary Figure 3). Such dye exchange experiments
have been utilized by others to verify the charge state of host coordination
networks.[45] The general formula for NPU-1/2/3 is Mn5IIMnIII(μ3-O)2(CH3COO)3(Tripp)2(L)3 (L = BDC2–/NPDC2–/BPDC2– for NPU-1/2/3, respectively).M3(μ3-O) clusters are normally connected
by three, six, or nine organic linker ligands, but the Mn6 cluster in NPU-1/2/3 is bonded to 12 linker ligands
(six dicarboxylate ligands and six Tripp ligands). The potential for
rare 12-c nodes exists,[5,42−44] but pairs of
Tripp ligands serve as parallel 3-c nodes that connect to the same
adjacent Mn6 cluster. Therefore, the Mn6 cluster
should be viewed as a 9-c node, and NPU-1/2/3 are classified
as 3,9-connected networks with pacs topology[46] (Supplementary Figure 4). A similar “double cross-linking” situation occurred
in the metal–organic polyhedron of formula [Cu2(bdc)2]12 (bdc = 1,3-benzenedicarboxylate). In
this case, the 24 accessible connection points can serve as 6-c or
24-c nodes to build augmented pcu or rht networks.[47,48] Notably, there are dual cages
(A and B) in NPU-1/2/3 (Figure ). Cage A has a trigonal bipyramidal shape,
as it is surrounded by five metal clusters, six dicarboxylate ligands,
and six Tripp ligands. Whereas the equatorial dimension of Cage A
is consistent in NPU-1/2/3 (0.79 nm after subtracting
the van der Waals radii of the nearest atoms), the axial dimension
increases with the length of the dicarboxylate linker ligands (1.26,
1.77, and 2.24 nm for NPU-1/2/3, respectively). Cage
B exhibits a distorted triangular prismatic shape, as it is formed
from six adjacent Mn6 clusters, six dicarboxylate ligands,
and four parallel Tripp ligands. The axial dimension in cage B varies
from 0.38 to 0.66 to 0.91 nm for NPU-1/2/3, respectively.
Each cage A is connected to six cage B’s in a face-shared manner,
and vice versa. The triangular interconnecting pore windows
between these cages, which are surrounded by one Tripp ligand and
two carboxylate ligands, exhibit aperture sizes of 0.48 nm for NPU-1, 0.6 nm for NPU-2, and 0.78 nm for NPU-3. As revealed below, the dual cage nature of NPU-1/2/3 is crucial to their selective adsorption of C2H2 and C2H6 over C2H4.
The porosity of NPU-1, NPU-2, and NPU-3 as calculated by PLATON[49] was found to be 50.8%, 56.8%, and 62.1%, respectively.
Figure 1
NPU-1/2/3 are isostructural coordination networks
that are based upon assembly of Mn6 clusters, Tripp ligands,
and different dicarboxylate linker ligands. The three-dimensional
pore structures comprise two distinct cages.
NPU-1/2/3 are isostructural coordination networks
that are based upon assembly of Mn6 clusters, Tripp ligands,
and different dicarboxylate linker ligands. The three-dimensional
pore structures comprise two distinct cages.Bulk purity of NPU-1/2/3 was confirmed by powder X-ray
diffraction (PXRD, Figure a and Supplementary Figures 6–8). Thermogravimetric analysis (TGA) of as-synthesized and CH2Cl2-exchanged samples revealed that the DMA solvent
in the as-synthesized phase can be fully exchanged with CH2Cl2 and that NPU-1/2/3 are thermally stable
until 573 K (Supplementary Figures 9–11). N2 sorption experiments were conducted at 77 K to establish
permanent microporosity, and NPU-1/2/3 each exhibited
reversible type-I adsorption isotherms. By assuming pore filling by
liquid N2 at 77 K and 100 kPa, the pore volumes calculated
from N2 uptake at 100 kPa are 0.47 for NPU-1, 0.66 for NPU-2, and 0.77 cm3 g–1 for NPU-3. These values match well with the values
of 0.53 for NPU-1, 0.68 for NPU-2, and 0.84
cm3 g–1 for NPU-3 calculated
from the respective crystal structures. These findings are consistent
with the absence of counterions in the pore channels of NPU-1/2/3. Langmuir and Brunauer–Emmett–Teller (BET) surface
areas were calculated to be 1557 and 1396, 1844 and 1580, and 2133
and 1834 m2 g–1 for NPU-1/2/3, respectively. Horvath–Kawazoe (pore geometry: cylinder)
and NLDFT model (pore geometry: slit)-based pore size distribution
analyses were conducted upon the corresponding N2 sorption
isotherms (Figure c and Supplementary Figure 12). A gradually
increasing trend in pore size distribution was noticed upon increasing
the length of the dicarboxylate ligands (peak position: 0.74 nm in NPU-1, 1.05 nm in NPU-2, and 1.22 nm in NPU-3), in agreement with the crystal structures.
Figure 2
PXRD patterns and sorption data for NPU-1, NPU-2, and NPU-3. (a) Experimental and calculated PXRD patterns.
(b) N2 sorption isotherms at 77 K. (c) Calculated pore-size
distribution from 77 K N2 sorption data. (d) C2 gas sorption
isotherms of NPU-1, (e) NPU-2, and (f) NPU-3 at 298 K. (g) IAST selectivity of C2H6/C2H4 (1:1 ratio) and C2H2/C2H4 (1:1 ratio) at 298 K and 100 kPa.
(h) C2 gas adsorption enthalpies at low loading. (i) Optical microscope
image of NPU-1 crystals.
PXRD patterns and sorption data for NPU-1, NPU-2, and NPU-3. (a) Experimental and calculated PXRD patterns.
(b) N2 sorption isotherms at 77 K. (c) Calculated pore-size
distribution from 77 K N2 sorption data. (d) C2 gas sorption
isotherms of NPU-1, (e) NPU-2, and (f) NPU-3 at 298 K. (g) IAST selectivity of C2H6/C2H4 (1:1 ratio) and C2H2/C2H4 (1:1 ratio) at 298 K and 100 kPa.
(h) C2 gas adsorption enthalpies at low loading. (i) Optical microscope
image of NPU-1 crystals.The microporosity of NPU-1/2/3 prompted us to collect
pure gas sorption isotherms at 273 and 298 K for C2H2, C2H4, and C2H6 up to 100 kPa (Figure d–f, Supplementary Figures 13–15). NPU-1 is the sorbent with the smallest pore size
and exhibited the largest adsorption capacity for C2H2, C2H4, and C2H6, followed by NPU-2 (intermediate pore size) and NPU-3 (largest pore size). That the gas uptake at ambient
temperatures was observed to increase with decreasing pore size is
expected for microporous (<2 nm pores) materials.[50] Notably, at 298 K, NPU-1 was found to exhibit
higher uptakes of C2H2 (5.1 mmol g–1) and C2H6 (4.5 mmol g–1)
than C2H4 (4.2 mmol g–1) at
100 kPa. This trend is maintained at relatively low pressures (0–30
kPa), implying selective adsorption of C2H2 and
C2H6 vs C2H4 across the
range of loading in NPU-1. Despite lower C2H2 (4.03 and 2.58 mmol g–1, respectively),
C2H4 (3.45 and 2.22 mmol g–1), and C2H6 uptakes (4.44 and 3.36 mmol g–1) for NPU-2 and NPU-3 at
298 K and 100 kPa vs NPU-1, a similar phenomenon for
C2H2 and C2H6 adsorption
selectivity over C2H4 was observed. This trend
also occurred in the 273 K C2 sorption isotherms. The C2H2 and C2H6 uptakes for NPU-1 exceed the values of 4.55/3.79 mmol g–1 for TJT-100 and 3.50/4.47 mmol g–1 for Azole-Th-1.Adsorption selectivity is an important metric when evaluating separation
performance. Ideal Adsorbed Solution Theory[51] (IAST) was used to calculate the adsorption selectivity of C2H2/C2H4 and C2H6/C2H4 for equimolar gas mixtures
at 298 K and 100 kPa, after fitting the single-component 298 K adsorption
isotherms to the Langmuir–Freundlich equation (Supplementary Figures 16–18). The adsorption
selectivity values for C2H6/C2H4 and C2H2/C2H4 were found to be 1.32 and 1.4 for NPU-1, 1.52 and 1.25
for NPU-2, and 3.21 and 1.32 for NPU-3 (Figure g), making the NPU-1/2/3 platform only the third reported example of C2H2 and C2H6 adsorption selectivity
vs C2H4. The C2H6/C2H4 IAST selectivity values for NPU-1/2/3 are comparable to those of the other C2H6-selective
sorbents (1.95 for MUF-15,[52] 1.8 for IRMOF-8,[53] 1.76
for NUM-7a,[54] and 1.6 for JNU-2(55)).To evaluate the interaction strengths of C2H2, C2H4, and C2H6 with NPU-1/2/3, the adsorption enthalpies (Qst) were calculated using the Clausius–Clapeyron equation
by fitting the C2H2, C2H4, and C2H6 adsorption isotherms at 273 and
298 K to the virial equation (detailed fitting curves are given in Supplementary Figures 22–24). As expected, NPU-1/2/3 interact somewhat more strongly with C2H2 and C2H6 than with C2H4. Figure h presents C2H2 (27.88 kJ mol–1 for NPU-1, 20.98 kJ mol–1 for NPU-2, and 19.93 kJ mol–1 for NPU-3) and C2H6 (29.10 kJ mol–1 for NPU-1, 19.64 kJ mol–1 for NPU-2, and 18.71 kJ mol–1 for NPU-3) adsorption enthalpies relative to C2H4 (23.95
kJ mol–1 for NPU-1, 18.18 kJ mol–1 for NPU-2, and 17.79 kJ mol–1 for NPU-3) at low loadings. Considering the differences
between the low C2 loading enthalpies, particularly those for C2H2 and C2H6, the decreasing Qst trend holds across the full C2 loading range: Qst(C2H2) ≈ Qst(C2H6) > Qst(C2H4). Increased adsorption enthalpy
for C2 hydrocarbons with decreasing pore size can be attributed to
stronger binding in tighter pores.[11,56] We note that
a relatively low adsorption enthalpy value means a relatively low
energy footprint for sorbent regeneration.Molecular simulations were performed to gain insight into the nature
of the binding sites for C2H2, C2H4, and C2H6 in NPU-1 (see Supporting Information for full
details). The modeling studies revealed that C2H2 localizes in a triangular pocket formed by two BDC linkers and one
Tripp linker (Figure a). C2H2 molecules interact with electronegative
carboxylate O atoms of the BDC linkers through their CH moieties.
C2H2 molecules also interact with the aromatic
rings of BDC and Tripp linkers. C2H4 was found
to adsorb at the same location as C2H2, although
its interaction distances are longer (Figure b), an indication that C2H4 is likely to exhibit weaker interactions with NPU-1. The calculated averaged classical potential energies for both adsorbates
about this position (see Supporting Information for details) also support weaker interactions with C2H4. In essence, the D2 symmetry of C2H4 offers a less favorable
fit compared to the D∞ symmetry of C2H2.
Figure 3
Molecular modeling determined primary adsorption sites of (a) C2H2, (b) C2H4, and (c) C2H6 in NPU-1. Adsorbed C2 molecules are presented
in space-filling mode (C(MOM), gray; C(C2 gas), orange; H, white;
O, red; N, blue; Mn, purple).
Molecular modeling determined primary adsorption sites of (a) C2H2, (b) C2H4, and (c) C2H6 in NPU-1. Adsorbed C2 molecules are presented
in space-filling mode (C(MOM), gray; C(C2 gas), orange; H, white;
O, red; N, blue; Mn, purple).In contrast to C2H2 and C2H4, C2H6 is too bulky to be adsorbed in
the triangular channels, and the modeling studies suggested that the
most favorable binding site for C2H6 is between
two adjacent Tripp linkers (Figure c). Its larger molecular dimensions and the presence
of multiple H atoms allow C2H6 to engage in
multiple weak interactions with surrounding Tripp linkers. C2H6 can also interact with the phenyl ring of a nearby
BDC linker. This binding site is quite favorable, as the potential
energy for C2H6 at this site is comparable to
that for C2H2 at its energy minimum position
on the basis of simulated annealing calculations (see Supplementary Table 3). Overall, molecular simulations
support the following trend in sorbent–sorbate interactions
for NPU-1: C2H2 ≈ C2H6 > C2H4. This trend is
consistent with the experimental findings.To evaluate separation performance, dynamic column breakthrough
experiments were performed for NPU-1 and NPU-2. Two separate columns with tightly packed powder samples of 2.9
g of NPU-1 and 2.5 g of NPU-2 were prepared
by pre-activating at 353 K under He flow (flow rate of 20 cm3 min–1). In a typical breakthrough experiment at
298 K, a 1:1:1 mixture of C2H2/C2H4/C2H6 at a total gas pressure
of 100 kPa was passed through the packed adsorbent column, and the
outlet gas signal was detected by gas chromatography. As shown in Figure a, NPU-1 effectively captured C2H2 and C2H6 from the 1:1:1 gas mixture and afforded polymer-grade
C2H4 in the effluent stream. Ethylene breakthrough
occurred first at ca. 93 min, followed by C2H2 and C2H6 at ca. 100 min. Before the breakthrough
of C2H2 and C2H6 from
the column outlet, C2H4 with polymer-grade purity
(>99.9%) was harvested, establishing the ability of NPU-1 to produce polymer-grade ethylene from 1:1:1 C2H2/C2H4/C2H6 in
a single separation step. Furthermore, dynamic breakthrough experiments
with less NPU-1 (1.3 g) exhibited similar separation
performance but with slightly reduced working capacity (Supplementary Figure 31). For the NPU-2 column, the breakthrough curve follows the same time sequence (C2H4 first, C2H2 second, and
C2H6 last) as NPU-1, but ethylene
in high purity was not afforded because of the very close breakthrough
times of C2H2 and C2H4. This result was presumably a consequence of the lower adsorption
enthalpy of all three gases for NPU-2 vs NPU-1 and the minimal differences between C2H2 and
C2H4 isotherms in NPU-2 at lower
pressures. NPU-3, with even lower adsorption capacity
and enthalpy, was not subjected to dynamic breakthrough experiments.
To confirm the ease of regeneration of NPU-1, we conducted
temperature-programmed desorption experiments after saturation of
the separation column. As seen in Figure c, the NPU-1 column can be fully
activated after heating at 313 K for 40 min under He flow (10 cm3 min–1). Upon increasing the activation
temperature to 333 K, the regeneration time was reduced to 25 min.
To test the recycling ability of NPU-1, 10 cycles of
ternary gas mixture breakthrough and single-gas ethane adsorption
experiments were conducted. No performance loss was detected. In addition,
the PXRD pattern of NPU-1 collected after exposure to
ambient air over a month verified its moisture stability.
Figure 4
Dynamic breakthrough data and stability test. Experimental breakthrough
curves at 298 K for C2H2/C2H4/C2H6 separation (1:1:1
mixture; total gas pressure of 100 kPa; total gas flow of 2.1 cm3 min–1) based on (a) NPU-1 column
with 2.9 g sample and (b) NPU-2 column with 2.5 g sample.
(c) Temperature-programmed desorption curves for NPU-1-packed column activated at 313 and 333 K under He flow of 20 cm3 min–1. (d) Dynamic breakthrough data of NPU-1 in the 1st, 5th, and 10th cycles for ternary gas separation
(C, outlet gas concentration; C0, inlet gas concentration). (e) PXRD patterns of NPU-1 under different conditions. (f) Ten-cycle comparison of C2H6 adsorption capacity at 298 K and 100 kPa for NPU-1 (n0, C2H6 uptake for first cycle; n, C2H6 uptake for the specific cycle).
Dynamic breakthrough data and stability test. Experimental breakthrough
curves at 298 K for C2H2/C2H4/C2H6 separation (1:1:1
mixture; total gas pressure of 100 kPa; total gas flow of 2.1 cm3 min–1) based on (a) NPU-1 column
with 2.9 g sample and (b) NPU-2 column with 2.5 g sample.
(c) Temperature-programmed desorption curves for NPU-1-packed column activated at 313 and 333 K under He flow of 20 cm3 min–1. (d) Dynamic breakthrough data of NPU-1 in the 1st, 5th, and 10th cycles for ternary gas separation
(C, outlet gas concentration; C0, inlet gas concentration). (e) PXRD patterns of NPU-1 under different conditions. (f) Ten-cycle comparison of C2H6 adsorption capacity at 298 K and 100 kPa for NPU-1 (n0, C2H6 uptake for first cycle; n, C2H6 uptake for the specific cycle).
Conclusion
In summary, we report a new hexanuclear metal cluster, [Mn6(μ3-O)2(CH3COO)3]6+, that can serve as a node in three porous coordination
networks (NPU-1/2/3) with the same pacs topology
and high connectivity. Pore size and pore chemistry in the dual cages
were controlled by linker ligand substitution, affording a pore environment
suitable for effective separation of C2H2 and
C2H6 from C2H4. NPU-1 thereby enabled production of polymer-grade ethylene
from a 1:1:1 C2H2/C2H4/C2H6 gas mixture at ambient
conditions in one step. Sorbent–sorbate interactions, as delineated
by molecular simulations, revealed that the dual cage nature of NPU-1 is the reason for the observed performance.
Authors: Lixia Guo; Mathew Savage; Joe H Carter; Xue Han; Ivan da Silva; Pascal Manuel; Svemir Rudić; Chiu C Tang; Sihai Yang; Martin Schröder Journal: Chem Mater Date: 2022-06-06 Impact factor: 10.508