logo
CONTENT TYPES

Preparation of Vortex Porous Graphene Chiral Membrane for Enantioselective Separation

  • Hongxin Tan
    Hongxin Tan
    CAS Key Laboratory of Chemistry of Northwestern Plant Resources and Key Laboratory for Natural Medicine of Gansu Province, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, China
    University of Chinese Academy of Sciences, Chinese Academy of Sciences, Beijing 100049, China
    More by Hongxin Tan
  • Tianqi Liu
    Tianqi Liu
    CAS Key Laboratory of Chemistry of Northwestern Plant Resources and Key Laboratory for Natural Medicine of Gansu Province, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, China
    More by Tianqi Liu
  • Xin Zhang
    Xin Zhang
    School of Nuclear Science and Technology, Lanzhou University, Lanzhou 730000, China
    More by Xin Zhang
  • Qiang Shan
    Qiang Shan
    School of Nuclear Science and Technology, Lanzhou University, Lanzhou 730000, China
    More by Qiang Shan
  • Jia Chen
    Jia Chen
    CAS Key Laboratory of Chemistry of Northwestern Plant Resources and Key Laboratory for Natural Medicine of Gansu Province, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, China
    More by Jia Chen
  • Zhan Li*
    Zhan Li
    CAS Key Laboratory of Chemistry of Northwestern Plant Resources and Key Laboratory for Natural Medicine of Gansu Province, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, China
    *E-mail: [email protected]
    More by Zhan Li
  • Hirotaka Ihara
    Hirotaka Ihara
    CAS Key Laboratory of Chemistry of Northwestern Plant Resources and Key Laboratory for Natural Medicine of Gansu Province, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, China
  • , and 
  • Hongdeng Qiu*
    Hongdeng Qiu
    CAS Key Laboratory of Chemistry of Northwestern Plant Resources and Key Laboratory for Natural Medicine of Gansu Province, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, China
    University of Chinese Academy of Sciences, Chinese Academy of Sciences, Beijing 100049, China
    *E-mail: [email protected]
    More by Hongdeng Qiu
Cite this: Anal. Chem. 2020, 92, 20, 13630–13633
Publication Date (Web):August 24, 2020
https://doi.org/10.1021/acs.analchem.0c02446
Copyright © 2020 American Chemical Society
Article Views
1718
Altmetric
-
Citations
LEARN ABOUT THESE METRICS

Article Views are the COUNTER-compliant sum of full text article downloads since November 2008 (both PDF and HTML) across all institutions and individuals. These metrics are regularly updated to reflect usage leading up to the last few days.

Citations are the number of other articles citing this article, calculated by Crossref and updated daily. Find more information about Crossref citation counts.

The Altmetric Attention Score is a quantitative measure of the attention that a research article has received online. Clicking on the donut icon will load a page at altmetric.com with additional details about the score and the social media presence for the given article. Find more information on the Altmetric Attention Score and how the score is calculated.

PDF (3 MB)
Supporting Info (1)»

Abstract

Chiral materials are usually the key to the separation of chiral membranes. In this work, we propose a new strategy that chiral porous graphene membrane can be fabricated from nonchiral porous graphene by mechanical stirring to induce vortex structure. Porous graphene with controlled, nanosized pores was synthesized by a newly designed, one-pot process directly from graphite as opposed to graphene oxide. Then porous graphene was immobilized on ultrafiltration membrane through filtering while stirring to form porous graphene membrane, which was applied for enantioselective separation toward DL-amino acids: for example, the separation factor of l-/d-phenylalanine reached 4.76. Interestingly, we first observed that the front and back sides of the porous graphene membrane exhibited opposite optical activities.

Chirality plays an essential role in aspects of the origin of life, environment, and drug manufacture.(1,2) As we know, different isomers of chiral compounds have different biological activities and pharmacological effects.(3) Enantioselective synthesis is an ideal way, but this approach is very expensive in practical application. Therefore, the resolution of racemic mixtures of chiral molecules is essential to medication safety and development.(4) Commonly used chromatographic methods require expensive equipment and consume large amounts of solvents.(5) Meanwhile, membrane separation outperforms other chiral resolution techniques due to its no phase change, low energy consumption, highly selective, fast, and easy scale-up.(6) Hence, it is necessary to develop a superior-performance chiral separation membrane.

Porous graphene (PG) and its derivative membranes have been used in various fields including water desalination,(7−9) gas separation and purification,(10,11) and ionic selective separation.(12) PG is a derivative of graphene wherein nanoscale pores with various sizes, shapes, and functionalities are introduced on the sheets of graphene.(13−17) Owing to existing pores, it exhibits unique features as compared to pristine graphene such as higher surface area and mass diffusion rate.(18,19) Interestingly, based on computational simulations, Yan et al. reported that the stacked porous graphene channels with chiral helical profiles can exhibit brilliant enantioselectivity toward molecular transport.(20) Moreover, Kim et al. reported a chiral film of bilayer graphene with a controlled interlayer rotation (θ) and polarity by layer-by-layer deposition of graphene sheets,(21) but the stacking approach is hard to achieve a scalable synthesis of the chiral membrane. Simpler than the above method, physical stirring has been widely used for the facile and rapid preparation of noncovalent chiral materials.(22−24) It is reported that graphene oxide (GO) chirality can be altered by mechanical vortexes, which originate from the chiral structure of GO sheets stacked into a helical shape in the solution. Then, the obtained chirality was successfully transferred to GO support and the host molecules after simply clockwise (CW) and counterclockwise (CCW) dropcast stirring.(25)

Based on the above, here we report a new type of enantioselective porous graphene membrane (PGM) by mechanical stirring. The front and back of the membrane display mirror-image circular dichroism (CD) signals. By rhodamine-B staining, the stripes of the vortex structure can be observed on the membrane. Therefore, our method has some advantageous merits compared with conventional graphene-based functional membranes: for example, (1) no chirality is needed in graphene materials for membrane production because the chiral environment can be provided by simply stirring; (2) chiral function can be adjustable by controlling the mechanical process of stirring; and (3) PG with controlled pores can be produced by the one-pot process and easily immobilized on the ultrafiltration membrane for chiral separation. This work also demonstrates the exceptionally effective enantioselective separation for dl-amino acids.

PG was synthesized by a one-step combustion strategy from graphite. In the Hummers method, the oxidizing agents diffused into graphite galleries for producing the oxidized graphite. The product sulfates (MnSO4 and K2SO4) from the oxidizing reaction would remain and imperfectly cover the surface of the graphite inner layer and then convert to the oxides by heating. The metal oxide nanoparticles as an etcher underwent a carbothermal reaction between the graphite oxide layers for producing PG (Figures 1 and S1). Importantly, we further confirmed that only MnSO4 is the initiator for producing pores in the combustion process (Figures S2–S6). With the decrease of the concentration of the yellow mixture from the Hummers method, the size of the obtained metal oxide nanoparticle decreases (Figures S2 and S3). According to the previous report, the pore size of PG is proportional to the size of the oxide nanoparticle.(26,27) As shown in Figure 2a–c, the pore size of PG is mediated to ∼25, 11, and 3.5 nm by diluting the yellow mixture, respectively. More characterizations are displayed in Figures S7–S10 and Table S1.

Figure 1

Figure 1. Synthesis of PGM with vortex structures. Sulfate is derived from the reaction byproducts in the Hummers method, which forms nanoparticles between layers of graphite oxides in combustion, then the pore is etched by the carbothermal reaction on each layer of graphite oxide at high temperature, and PG is obtained after washing and ultrasound treatment. PGM with vortex structures is prepared by mechanical stirring. The optical activities of the front of PGM are opposite to that of the back.

Figure 2

Figure 2. Characterizations of PG and PGMs with different pore sizes. (a–c) transmission electron microscopy (TEM) images of PG. (d–f) Surface SEM images of PGM. (g–i) Cross-sectional SEM images of PGM. (j) Schematic of chiral separation equipment; the racemic and HCI solution are placed as the feed and permeate solutions, respectively. (k) Photograph of PGM.

PG membranes (PGMs) are prepared by rapid filtration of well-dispersed suspension of PG (pH = 11.4) with different size pores after stirring for 30 min (Figure S11). Figure 2d–f shows the SEM images of PGMs surface morphology with many pores. The cross-section scanning electron microscopy (SEM) images show the layered structures of these PGMs (Figure 2g–i). The schematic diagram of separation equipment and pictures of PGMs with a definite filter area of 1.77 cm2 are shown in Figure 2j and k, respectively. As shown in the typical stress–strain curves of the prepared PGMs (Figure S12), the tensile strength and toughness of the pure polyvinylidene fluoride (PVDF) films are 1.66 MPa and 0.11 MJ m–3, respectively. With the thickness of the PGM increasing from 210 to 415 μm, the tensile strength is increased from 1.65 to 1.78 MPa. More importantly, the toughness of the PGM with a 415 μm thickness is up to 0.45 MJ m–3, which is 4× higher than that of PVDF film. The improvement of mechanical property can be ascribed to the increased π–π conjugated interaction and friction between the PG sheets.(28,29)

Subsequently, the prepared PGMs were used for molecular chiral separation. Figure S13 shows that the larger the pore size on PG causes the higher the permeation toward d-phenylalanine (d-Phe); thus, the PG with the largest pore size of ∼25 nm is selected as a membrane material for the following separation of enantiomers. The permeation dynamics of d-Phe through PGM under 2 and 4 M HCl driven solution are shown in Figure 3a, which suggests that the increase of the acidity in the driven solution can promote the permeation of d-Phe through PGM, also meaning that the permeation processes may be ionic exchange on functional groups between ionized d-Phe and H+.(12) The permeation of l-phenylalanine (l-Phe) through PGM is 1.74 and 1.77 times that of d-Phe under the driven 2 and 4 M HCl at 48 h, respectively (Figure 3b). Figure 3c shows that the permeation of l-/d-Phe reduces, but the separation factor (SF) increases from 1.12 to 1.75 as the thickness of PGM increased from 210 to 415 μm, which is consistent with the existing permeation theory.(30) Importantly, PGM can also be used to separate l-glutamic (l-Glu) and d-glutamic (d-Glu), and the selectivity of PGM to l-/d-Glu is 2.45 and 2.17 at 36 and 48 h, respectively (Figure 3d).

Figure 3

Figure 3. Separation of enantiomer molecules through PGM under an acidic environment. (a) Permeation dynamics of d-Phe through PGM under acidity driven with 2 and 4 M HCl. (b) Separation of l-Phe and d-Phe under acidity driven with 2 and 4 M HCl after 48 h. (c) Separation of l-Phe and d-Phe as a function of the membrane thickness under acidity driven with 4 M HCl after 48 h. (d) Separation of l-Glu and d-Glu under acidity driven with 4 M HCl after 36 and 48 h. The concentration of the initial feed solution is 0.01 M.

To further explore the relation between the stirring vortex and chiral separation, and thus improving the SF of PGM to enantiomer molecules, PGM is prepared by mechanical stirring while filtering after a certain period of time of stirring (Figures 4b and S14). Figure 4a shows the picture of symmetrically folded PGM with a vortex structure, indicating that PGM thickness decreases gradually from the inside to the edge. The stripes of the vortex structure can be seen through the enlarged view of the middle area.

Figure 4

Figure 4. Characterizations and separation performance of PGM prepared by stirring and filtering. (a) Picture of PGM prepared by clockwise stirring. Inset: a high-resolution image of vortex structure on the PGM surface. (b) Schematic diagram of stirring and filtering equipment. (c) Vortex pattern after stirring for different times, observed on rhodamine-B dyed PGM by confocal laser scanning microscope; the yellow arrows identify the vortex structure. (d) CD spectra of stirred PG suspensions at 0, 5, 15, and 30 min, with a stirring speed of 600 rpm. (e) CD spectra of the front and back of PGM. (f) SF of l-/d-Phe through PGM prepared by filtration without stirring, stirring before filtration, and stirring filtration. The feed solution is 0.01 M of racemic l-/d-Phe solution; driven solution is 4 M HCl. (g) Vortex pattern after separation for a different time, and the yellow arrows identify the vortex structure.

As shown in Figure 4c, with the increase of the stirring time, concentric circles (20–100 μm) can be obviously observed by a confocal laser scanning microscope on the rhodamine-B dyed PGM, which confirms the existence of a vortex structure. The CD spectra of PG suspensions after stirring are performed as shown in Figures 4d and S15. A peak at ∼290 nm can be observed, and the magnitude of the CD peak increases with the increase of stirring time from 0 to 30 min, but it is independent of stirring speed. Therefore, 30 min and 600 rpm of stirring were selected to prepare PGM. Moreover, PG deposited on the glass surface under stirring was prepared to perform CD spectra. Mirror image CD signals are observed for the front and back of the glass in Figure 4e, indicating that PGM with vortex structures exhibits chiral properties. Subsequently, the vortex PGM was used to achieve highly selective separation of l-/d-Phe. As shown in Figure S16, the permeation of l-Phe from the front to the back of PGM is higher than that of d-Phe, but permeation of d-Phe from the back of PGM to the front is higher than l-Phe. As a control, the permeation performance of the PG membrane without stirring was also conducted (Figures S17 and S18), displaying no selectivity for l-/d-Phe, and SF remains ∼1 from 24 to 48 h (Figure 4f). However, PGM prepared by stirring before filtration shows SF of ∼2.7 at 24 h, and then SF decreases gradually from 24 to 48 h. More importantly, PGM prepared by stirring and filtration after stirring for 30 min, exhibiting very excellent separation performance toward l-/d-Phe (SF ≈ 4.76 at 24 h). The decrease of SF from 24 to 48 h can be attributed to the decrease of the concentration gradient between feed and driven solutions.(12) Nevertheless, the vortex PGM still maintains higher selectivity for l-/d-Phe after separation for 48 h, and the SF is up to 1.79. As shown in Figure 4g, the vortex structure still existed, indicating the excellent stability of PGM. In particular, the separation performance of vortex PGM is higher than that of chiral molecularly imprinted nanofiber membranes and a homochiral metal–organic framework membrane.(4,31) However, there is no direct evidence that the vortex caused by stirring controls stacking of PG sheets into a chiral shape in this work. Therefore, the mechanism of vortex deposition leading to chiral separation needs further study.

In summary, we have developed a facile, rapid, and low-cost approach for the fabrication of PG from graphite. The byproducts, in the form of salts, from the Hummers method are completely utilized. The preparation measures of PG are simplified from two steps to one step using the combustion of graphite oxides. The resulting PG was successfully used to prepare PGM for achieving selective separation of chiral molecules. We believe this strategy will open an avenue toward the construction of a nanoporous chiral graphene membrane, but further research is still needed about how the vortex causes chiral separations.

Supporting Information

ARTICLE SECTIONS
Jump To

The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.analchem.0c02446.

  • Experimental; Preparation and formation mechanism of PG; Characterizations of PG; Characterizations and chiral separation performance of PGM (PDF)

Terms & Conditions

Most electronic Supporting Information files are available without a subscription to ACS Web Editions. Such files may be downloaded by article for research use (if there is a public use license linked to the relevant article, that license may permit other uses). Permission may be obtained from ACS for other uses through requests via the RightsLink permission system: http://pubs.acs.org/page/copyright/permissions.html.

Author Information

ARTICLE SECTIONS
Jump To

  • Corresponding Authors
    • Zhan Li - CAS Key Laboratory of Chemistry of Northwestern Plant Resources and Key Laboratory for Natural Medicine of Gansu Province, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, China Email: [email protected]
    • Hongdeng Qiu - CAS Key Laboratory of Chemistry of Northwestern Plant Resources and Key Laboratory for Natural Medicine of Gansu Province, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, ChinaUniversity of Chinese Academy of Sciences, Chinese Academy of Sciences, Beijing 100049, ChinaOrcidhttp://orcid.org/0000-0002-2702-9415 Email: [email protected]
  • Authors
    • Hongxin Tan - CAS Key Laboratory of Chemistry of Northwestern Plant Resources and Key Laboratory for Natural Medicine of Gansu Province, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, ChinaUniversity of Chinese Academy of Sciences, Chinese Academy of Sciences, Beijing 100049, China
    • Tianqi Liu - CAS Key Laboratory of Chemistry of Northwestern Plant Resources and Key Laboratory for Natural Medicine of Gansu Province, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, China
    • Xin Zhang - School of Nuclear Science and Technology, Lanzhou University, Lanzhou 730000, China
    • Qiang Shan - School of Nuclear Science and Technology, Lanzhou University, Lanzhou 730000, China
    • Jia Chen - CAS Key Laboratory of Chemistry of Northwestern Plant Resources and Key Laboratory for Natural Medicine of Gansu Province, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, China
    • Hirotaka Ihara - CAS Key Laboratory of Chemistry of Northwestern Plant Resources and Key Laboratory for Natural Medicine of Gansu Province, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, China
  • Author Contributions

    H.T., Z.L., and H.Q. designed the research. The manuscript was written through the contributions of all authors.

  • Notes

    The authors declare no competing financial interest.

Acknowledgments

ARTICLE SECTIONS
Jump To

This study was conducted with financial assistance from the National Natural Science Foundation of China (Nos. 21974146, 21822407, and 21675164), the Foundation for Sci and Tech Research Project of Gansu Province (18JR3RA387), CAS “Light of West China” Program, and CAS President’s International Fellowship Initiative (2020VBA0009).

References

ARTICLE SECTIONS
Jump To

This article references 31 other publications.

  1. 1
    Rekoske, J. E. Chiral separations. AIChE J. 2001, 47, 25,  DOI: 10.1002/aic.690470102
  2. 2
    Sun, P. Z.; Zheng, F.; Zhu, M.; Wang, K. L.; Zhong, M. L.; Wu, D. H.; Zhu, H. W. Realizing Synchronous Energy Harvesting and Ion Separation with Graphene Oxide Membranes. Sci. Rep. 2015, 4, 15,  DOI: 10.1038/srep05528
  3. 3
    Hauser, A. W.; Mardirossian, N.; Panetier, J. A.; Head-Gordon, M.; Bell, A. T.; Schwerdtfeger, P. Functionalized Graphene as a Gatekeeper for Chiral Molecules: An Alternative Concept for Chiral Separation. Angew. Chem., Int. Ed. 2014, 53, 99579960,  DOI: 10.1002/anie.201403145
  4. 4
    Wang, W. J.; Dong, X. L.; Nan, J. P.; Jin, W. Q.; Hu, Z. Q.; Chen, Y. F.; Jiang, J. W. A homochiral metal-organic framework membrane for enantioselective separation. Chem. Commun. 2012, 48, 70227024,  DOI: 10.1039/c2cc32595k
  5. 5
    Ward, T. J.; Baker, B. A. Chiral Separations. Anal. Chem. 2008, 80, 43634372,  DOI: 10.1021/ac800662y
  6. 6
    Xie, R.; Chu, L. Y.; Deng, J. G. Membranes and membrane processes for chiral resolution. Chem. Soc. Rev. 2008, 37, 12431263,  DOI: 10.1039/b713350b
  7. 7
    Surwade, S. P.; Smirnov, S. N.; Vlassiouk, I. V.; Unocic, R. R.; Veith, G. M.; Dai, S.; Mahurin, S. M. Water desalination using nanoporous single-layer graphene. Nat. Nanotechnol. 2015, 10, 459464,  DOI: 10.1038/nnano.2015.37
  8. 8
    Cohen-Tanugi, D.; Grossman, J. C. Water Desalination across Nanoporous Graphene. Nano Lett. 2012, 12, 36023608,  DOI: 10.1021/nl3012853
  9. 9
    O’Hern, S. C.; Jang, D.; Bose, S.; Idrobo, J.-C.; Song, Y.; Laoui, T.; Kong, J.; Karnik, R. Nanofiltration across Defect-Sealed Nanoporous Monolayer Graphene. Nano Lett. 2015, 15, 32543260,  DOI: 10.1021/acs.nanolett.5b00456
  10. 10
    Boutilier, M. S. H.; Sun, C. Z.; O’Hern, S. C.; Au, H.; Hadjiconstantinou, N. G.; Karnik, R. Implications of Permeation through Intrinsic Defects in Graphene on the Design of Defect-Tolerant Membranes for Gas Separation. ACS Nano 2014, 8, 841849,  DOI: 10.1021/nn405537u
  11. 11
    Koenig, S. P.; Wang, L. D.; Pellegrino, J.; Bunch, J. S. Selective molecular sieving through porous graphene. Nat. Nanotechnol. 2012, 7, 728732,  DOI: 10.1038/nnano.2012.162
  12. 12
    Li, Z.; Liu, Y. Q.; Zhao, Y.; Zhang, X.; Qian, L. J.; Tian, L. L.; Bai, J.; Qi, W.; Yao, H. J.; Gao, B.; Liu, J.; Wu, W. S.; Qiu, H. D. Selective Separation of Metal Ions via Monolayer Nanoporous Graphene with Carboxyl Groups. Anal. Chem. 2016, 88, 1000210010,  DOI: 10.1021/acs.analchem.6b02175
  13. 13
    Sun, P. Z.; Wang, K. L.; Zhu, H. W. Recent Developments in Graphene-Based Membranes: Structure, Mass-Transport Mechanism and Potential Applications. Adv. Mater. 2016, 28, 22872310,  DOI: 10.1002/adma.201502595
  14. 14
    Wang, L. D.; Boutilier, M. S. H.; Kidambi, P. R.; Jang, D.; Hadjiconstantinou, N. G.; Karnik, R. Fundamental transport mechanisms, fabrication and potential applications of nanoporous atomically thin membranes. Nat. Nanotechnol. 2017, 12, 509522,  DOI: 10.1038/nnano.2017.72
  15. 15
    Jiang, L. L.; Fan, Z. J. Design of advanced porous graphene materials: from graphene nanomesh to 3D architectures. Nanoscale 2014, 6, 19221945,  DOI: 10.1039/C3NR04555B
  16. 16
    Li, Z.; Zhang, X.; Tan, H.; Qi, W.; Wang, L.; Ali, M. C.; Zhang, H.; Chen, J.; Hu, P.; Fan, C.; Qiu, H. Combustion Fabrication of Nanoporous Graphene for Ionic Separation Membranes. Adv. Funct. Mater. 2018, 28, 1805026,  DOI: 10.1002/adfm.201805026
  17. 17
    Zhang, M.; Bao, W. X.; Liu, X. L.; Yu, B. Z.; Ren, Z. Y.; Bai, J. T.; Fan, H. M. Large-scale synthesis of porous graphene through nanoscale carbothermal reduction etching. J. Mater. Sci. 2015, 50, 78757883,  DOI: 10.1007/s10853-015-9309-1
  18. 18
    Han, S.; Wu, D. Q.; Li, S.; Zhang, F.; Feng, X. L. Porous Graphene Materials for Advanced Electrochemical Energy Storage and Conversion Devices. Adv. Mater. 2014, 26, 849864,  DOI: 10.1002/adma.201303115
  19. 19
    Song, L.; Zhang, H.; Cai, T.; Chen, J.; Li, Z.; Guan, M.; Qiu, H. Porous graphene decorated silica as a new stationary phase for separation of sulfanilamide compounds in hydrophilic interaction chromatography. Chin. Chem. Lett. 2019, 30, 863866,  DOI: 10.1016/j.cclet.2018.10.040
  20. 20
    Yan, Y. G.; Li, W.; Kral, P. Enantioselective Molecular Transport in Multilayer Graphene Nanopores. Nano Lett. 2017, 17, 67426746,  DOI: 10.1021/acs.nanolett.7b02846
  21. 21
    Kim, C. J.; Sanchez-Castillo, A.; Ziegler, Z.; Ogawa, Y.; Noguez, C.; Park, J. Chiral atomically thin films. Nat. Nanotechnol. 2016, 11, 520524,  DOI: 10.1038/nnano.2016.3
  22. 22
    Morrow, S. M.; Bissette, A. J.; Fletcher, S. P. Transmission of chirality through space and across length scales. Nat. Nanotechnol. 2017, 12, 410,  DOI: 10.1038/nnano.2017.62
  23. 23
    Dzwolak, W. Vortex-induced chiral bifurcation in aggregating insulin. Chirality 2010, 22, E154E160,  DOI: 10.1002/chir.20896
  24. 24
    D’Urso, A.; Randazzo, R.; Lo Faro, L.; Purrello, R. Vortexes and Nanoscale Chirality. Angew. Chem., Int. Ed. 2010, 49, 108112,  DOI: 10.1002/anie.200903543
  25. 25
    Di Mauro, A.; Randazzo, R.; Spano, S. F.; Compagnini, G.; Gaeta, M.; D’Urso, L.; Paolesse, R.; Pomarico, G.; Di Natale, C.; Villari, V.; Micali, N.; Fragala, M. E.; D’Urso, A.; Purrello, R. Vortexes tune the chirality of graphene oxide and its non-covalent hosts. Chem. Commun. 2016, 52, 1309413096,  DOI: 10.1039/C6CC05177D
  26. 26
    Zhou, D.; Cui, Y.; Xiao, P. W.; Jiang, M. Y.; Han, B. H. A general and scalable synthesis approach to porous graphene. Nat. Commun. 2014, 5, 4716,  DOI: 10.1038/ncomms5716
  27. 27
    Tan, H. X.; Zhang, X.; Li, Z.; Qiu, H. D. Small-Scale Nanoparticles Pyrolyzed from Layered Hydrotalcite between Graphene Interlayers as Intermediates for Self-Assembly into Metal Oxide Nanosheets and Hollow Nanospheres. ChemNanoMat 2020, 6, 12701275,  DOI: 10.1002/cnma.202000224
  28. 28
    Cheng, Q. F.; Wu, M. X.; Li, M. Z.; Jiang, L.; Tang, Z. Y. Ultratough Artificial Nacre Based on Conjugated Cross-linked Graphene Oxide. Angew. Chem., Int. Ed. 2013, 52, 37503755,  DOI: 10.1002/anie.201210166
  29. 29
    Wan, S. J.; Hu, H.; Peng, J. S.; Li, Y. C.; Fan, Y. Z.; Jiang, L.; Cheng, Q. F. Nacre-inspired integrated strong and tough reduced graphene oxide-poly (acrylic acid) nanocomposites. Nanoscale 2016, 8, 56495656,  DOI: 10.1039/C6NR00562D
  30. 30
    Huang, H. B.; Mao, Y. Y.; Ying, Y. L.; Liu, Y.; Sun, L. W.; Peng, X. S. Salt concentration, pH and pressure controlled separation of small molecules through lamellar graphene oxide membranes. Chem. Commun. 2013, 49, 59635965,  DOI: 10.1039/c3cc41953c
  31. 31
    Sueyoshi, Y.; Fukushima, C.; Yoshikawa, M. Molecularly imprinted nanofiber membranes from cellulose acetate aimed for chiral separation. J. Membr. Sci. 2010, 357, 9097,  DOI: 10.1016/j.memsci.2010.04.005

Cited By


This article is cited by 2 publications.

  1. Tianqi Liu, Zhan Li, Juanjuan Wang, Jia Chen, Ming Guan, Hongdeng Qiu. Solid membranes for chiral separation: A review. Chemical Engineering Journal 2021, 410 , 128247. https://doi.org/10.1016/j.cej.2020.128247
  2. Hongxin Tan, Xin Zhang, Zhan Li, Qing Liang, Jinsheng Wu, Yanli Yuan, Shiwei Cao, Jia Chen, Juewen Liu, Hongdeng Qiu. Nitrogen-doped Nanoporous Graphene Induced by a Multiple Confinement Strategy for Membrane Separation of Rare Earth. iScience 2020, , 101920. https://doi.org/10.1016/j.isci.2020.101920
  • Abstract

    Figure 1

    Figure 1. Synthesis of PGM with vortex structures. Sulfate is derived from the reaction byproducts in the Hummers method, which forms nanoparticles between layers of graphite oxides in combustion, then the pore is etched by the carbothermal reaction on each layer of graphite oxide at high temperature, and PG is obtained after washing and ultrasound treatment. PGM with vortex structures is prepared by mechanical stirring. The optical activities of the front of PGM are opposite to that of the back.

    Figure 2

    Figure 2. Characterizations of PG and PGMs with different pore sizes. (a–c) transmission electron microscopy (TEM) images of PG. (d–f) Surface SEM images of PGM. (g–i) Cross-sectional SEM images of PGM. (j) Schematic of chiral separation equipment; the racemic and HCI solution are placed as the feed and permeate solutions, respectively. (k) Photograph of PGM.

    Figure 3

    Figure 3. Separation of enantiomer molecules through PGM under an acidic environment. (a) Permeation dynamics of d-Phe through PGM under acidity driven with 2 and 4 M HCl. (b) Separation of l-Phe and d-Phe under acidity driven with 2 and 4 M HCl after 48 h. (c) Separation of l-Phe and d-Phe as a function of the membrane thickness under acidity driven with 4 M HCl after 48 h. (d) Separation of l-Glu and d-Glu under acidity driven with 4 M HCl after 36 and 48 h. The concentration of the initial feed solution is 0.01 M.

    Figure 4

    Figure 4. Characterizations and separation performance of PGM prepared by stirring and filtering. (a) Picture of PGM prepared by clockwise stirring. Inset: a high-resolution image of vortex structure on the PGM surface. (b) Schematic diagram of stirring and filtering equipment. (c) Vortex pattern after stirring for different times, observed on rhodamine-B dyed PGM by confocal laser scanning microscope; the yellow arrows identify the vortex structure. (d) CD spectra of stirred PG suspensions at 0, 5, 15, and 30 min, with a stirring speed of 600 rpm. (e) CD spectra of the front and back of PGM. (f) SF of l-/d-Phe through PGM prepared by filtration without stirring, stirring before filtration, and stirring filtration. The feed solution is 0.01 M of racemic l-/d-Phe solution; driven solution is 4 M HCl. (g) Vortex pattern after separation for a different time, and the yellow arrows identify the vortex structure.

  • References

    ARTICLE SECTIONS
    Jump To

    This article references 31 other publications.

    1. 1
      Rekoske, J. E. Chiral separations. AIChE J. 2001, 47, 25,  DOI: 10.1002/aic.690470102
    2. 2
      Sun, P. Z.; Zheng, F.; Zhu, M.; Wang, K. L.; Zhong, M. L.; Wu, D. H.; Zhu, H. W. Realizing Synchronous Energy Harvesting and Ion Separation with Graphene Oxide Membranes. Sci. Rep. 2015, 4, 15,  DOI: 10.1038/srep05528
    3. 3
      Hauser, A. W.; Mardirossian, N.; Panetier, J. A.; Head-Gordon, M.; Bell, A. T.; Schwerdtfeger, P. Functionalized Graphene as a Gatekeeper for Chiral Molecules: An Alternative Concept for Chiral Separation. Angew. Chem., Int. Ed. 2014, 53, 99579960,  DOI: 10.1002/anie.201403145
    4. 4
      Wang, W. J.; Dong, X. L.; Nan, J. P.; Jin, W. Q.; Hu, Z. Q.; Chen, Y. F.; Jiang, J. W. A homochiral metal-organic framework membrane for enantioselective separation. Chem. Commun. 2012, 48, 70227024,  DOI: 10.1039/c2cc32595k
    5. 5
      Ward, T. J.; Baker, B. A. Chiral Separations. Anal. Chem. 2008, 80, 43634372,  DOI: 10.1021/ac800662y
    6. 6
      Xie, R.; Chu, L. Y.; Deng, J. G. Membranes and membrane processes for chiral resolution. Chem. Soc. Rev. 2008, 37, 12431263,  DOI: 10.1039/b713350b
    7. 7
      Surwade, S. P.; Smirnov, S. N.; Vlassiouk, I. V.; Unocic, R. R.; Veith, G. M.; Dai, S.; Mahurin, S. M. Water desalination using nanoporous single-layer graphene. Nat. Nanotechnol. 2015, 10, 459464,  DOI: 10.1038/nnano.2015.37
    8. 8
      Cohen-Tanugi, D.; Grossman, J. C. Water Desalination across Nanoporous Graphene. Nano Lett. 2012, 12, 36023608,  DOI: 10.1021/nl3012853
    9. 9
      O’Hern, S. C.; Jang, D.; Bose, S.; Idrobo, J.-C.; Song, Y.; Laoui, T.; Kong, J.; Karnik, R. Nanofiltration across Defect-Sealed Nanoporous Monolayer Graphene. Nano Lett. 2015, 15, 32543260,  DOI: 10.1021/acs.nanolett.5b00456
    10. 10
      Boutilier, M. S. H.; Sun, C. Z.; O’Hern, S. C.; Au, H.; Hadjiconstantinou, N. G.; Karnik, R. Implications of Permeation through Intrinsic Defects in Graphene on the Design of Defect-Tolerant Membranes for Gas Separation. ACS Nano 2014, 8, 841849,  DOI: 10.1021/nn405537u
    11. 11
      Koenig, S. P.; Wang, L. D.; Pellegrino, J.; Bunch, J. S. Selective molecular sieving through porous graphene. Nat. Nanotechnol. 2012, 7, 728732,  DOI: 10.1038/nnano.2012.162
    12. 12
      Li, Z.; Liu, Y. Q.; Zhao, Y.; Zhang, X.; Qian, L. J.; Tian, L. L.; Bai, J.; Qi, W.; Yao, H. J.; Gao, B.; Liu, J.; Wu, W. S.; Qiu, H. D. Selective Separation of Metal Ions via Monolayer Nanoporous Graphene with Carboxyl Groups. Anal. Chem. 2016, 88, 1000210010,  DOI: 10.1021/acs.analchem.6b02175
    13. 13
      Sun, P. Z.; Wang, K. L.; Zhu, H. W. Recent Developments in Graphene-Based Membranes: Structure, Mass-Transport Mechanism and Potential Applications. Adv. Mater. 2016, 28, 22872310,  DOI: 10.1002/adma.201502595
    14. 14
      Wang, L. D.; Boutilier, M. S. H.; Kidambi, P. R.; Jang, D.; Hadjiconstantinou, N. G.; Karnik, R. Fundamental transport mechanisms, fabrication and potential applications of nanoporous atomically thin membranes. Nat. Nanotechnol. 2017, 12, 509522,  DOI: 10.1038/nnano.2017.72
    15. 15
      Jiang, L. L.; Fan, Z. J. Design of advanced porous graphene materials: from graphene nanomesh to 3D architectures. Nanoscale 2014, 6, 19221945,  DOI: 10.1039/C3NR04555B
    16. 16
      Li, Z.; Zhang, X.; Tan, H.; Qi, W.; Wang, L.; Ali, M. C.; Zhang, H.; Chen, J.; Hu, P.; Fan, C.; Qiu, H. Combustion Fabrication of Nanoporous Graphene for Ionic Separation Membranes. Adv. Funct. Mater. 2018, 28, 1805026,  DOI: 10.1002/adfm.201805026
    17. 17
      Zhang, M.; Bao, W. X.; Liu, X. L.; Yu, B. Z.; Ren, Z. Y.; Bai, J. T.; Fan, H. M. Large-scale synthesis of porous graphene through nanoscale carbothermal reduction etching. J. Mater. Sci. 2015, 50, 78757883,  DOI: 10.1007/s10853-015-9309-1
    18. 18
      Han, S.; Wu, D. Q.; Li, S.; Zhang, F.; Feng, X. L. Porous Graphene Materials for Advanced Electrochemical Energy Storage and Conversion Devices. Adv. Mater. 2014, 26, 849864,  DOI: 10.1002/adma.201303115
    19. 19
      Song, L.; Zhang, H.; Cai, T.; Chen, J.; Li, Z.; Guan, M.; Qiu, H. Porous graphene decorated silica as a new stationary phase for separation of sulfanilamide compounds in hydrophilic interaction chromatography. Chin. Chem. Lett. 2019, 30, 863866,  DOI: 10.1016/j.cclet.2018.10.040
    20. 20
      Yan, Y. G.; Li, W.; Kral, P. Enantioselective Molecular Transport in Multilayer Graphene Nanopores. Nano Lett. 2017, 17, 67426746,  DOI: 10.1021/acs.nanolett.7b02846
    21. 21
      Kim, C. J.; Sanchez-Castillo, A.; Ziegler, Z.; Ogawa, Y.; Noguez, C.; Park, J. Chiral atomically thin films. Nat. Nanotechnol. 2016, 11, 520524,  DOI: 10.1038/nnano.2016.3
    22. 22
      Morrow, S. M.; Bissette, A. J.; Fletcher, S. P. Transmission of chirality through space and across length scales. Nat. Nanotechnol. 2017, 12, 410,  DOI: 10.1038/nnano.2017.62
    23. 23
      Dzwolak, W. Vortex-induced chiral bifurcation in aggregating insulin. Chirality 2010, 22, E154E160,  DOI: 10.1002/chir.20896
    24. 24
      D’Urso, A.; Randazzo, R.; Lo Faro, L.; Purrello, R. Vortexes and Nanoscale Chirality. Angew. Chem., Int. Ed. 2010, 49, 108112,  DOI: 10.1002/anie.200903543
    25. 25
      Di Mauro, A.; Randazzo, R.; Spano, S. F.; Compagnini, G.; Gaeta, M.; D’Urso, L.; Paolesse, R.; Pomarico, G.; Di Natale, C.; Villari, V.; Micali, N.; Fragala, M. E.; D’Urso, A.; Purrello, R. Vortexes tune the chirality of graphene oxide and its non-covalent hosts. Chem. Commun. 2016, 52, 1309413096,  DOI: 10.1039/C6CC05177D
    26. 26
      Zhou, D.; Cui, Y.; Xiao, P. W.; Jiang, M. Y.; Han, B. H. A general and scalable synthesis approach to porous graphene. Nat. Commun. 2014, 5, 4716,  DOI: 10.1038/ncomms5716
    27. 27
      Tan, H. X.; Zhang, X.; Li, Z.; Qiu, H. D. Small-Scale Nanoparticles Pyrolyzed from Layered Hydrotalcite between Graphene Interlayers as Intermediates for Self-Assembly into Metal Oxide Nanosheets and Hollow Nanospheres. ChemNanoMat 2020, 6, 12701275,  DOI: 10.1002/cnma.202000224
    28. 28
      Cheng, Q. F.; Wu, M. X.; Li, M. Z.; Jiang, L.; Tang, Z. Y. Ultratough Artificial Nacre Based on Conjugated Cross-linked Graphene Oxide. Angew. Chem., Int. Ed. 2013, 52, 37503755,  DOI: 10.1002/anie.201210166
    29. 29
      Wan, S. J.; Hu, H.; Peng, J. S.; Li, Y. C.; Fan, Y. Z.; Jiang, L.; Cheng, Q. F. Nacre-inspired integrated strong and tough reduced graphene oxide-poly (acrylic acid) nanocomposites. Nanoscale 2016, 8, 56495656,  DOI: 10.1039/C6NR00562D
    30. 30
      Huang, H. B.; Mao, Y. Y.; Ying, Y. L.; Liu, Y.; Sun, L. W.; Peng, X. S. Salt concentration, pH and pressure controlled separation of small molecules through lamellar graphene oxide membranes. Chem. Commun. 2013, 49, 59635965,  DOI: 10.1039/c3cc41953c
    31. 31
      Sueyoshi, Y.; Fukushima, C.; Yoshikawa, M. Molecularly imprinted nanofiber membranes from cellulose acetate aimed for chiral separation. J. Membr. Sci. 2010, 357, 9097,  DOI: 10.1016/j.memsci.2010.04.005
  • Supporting Information

    Supporting Information

    ARTICLE SECTIONS
    Jump To

    The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.analchem.0c02446.

    • Experimental; Preparation and formation mechanism of PG; Characterizations of PG; Characterizations and chiral separation performance of PGM (PDF)


    Terms & Conditions

    Most electronic Supporting Information files are available without a subscription to ACS Web Editions. Such files may be downloaded by article for research use (if there is a public use license linked to the relevant article, that license may permit other uses). Permission may be obtained from ACS for other uses through requests via the RightsLink permission system: http://pubs.acs.org/page/copyright/permissions.html.

Pair your accounts.

Export articles to Mendeley

Get article recommendations from ACS based on references in your Mendeley library.

Pair your accounts.

Export articles to Mendeley

Get article recommendations from ACS based on references in your Mendeley library.

You’ve supercharged your research process with ACS and Mendeley!

STEP 1:
Click to create an ACS ID

Please note: If you switch to a different device, you may be asked to login again with only your ACS ID.

Please note: If you switch to a different device, you may be asked to login again with only your ACS ID.

Please note: If you switch to a different device, you may be asked to login again with only your ACS ID.

OOPS

You have to login with your ACS ID befor you can login with your Mendeley account.

MENDELEY PAIRING EXPIRED
Your Mendeley pairing has expired. Please reconnect

This website uses cookies to improve your user experience. By continuing to use the site, you are accepting our use of cookies. Read the ACS privacy policy.

CONTINUE