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REVIEW article

Front. Energy Res., 20 August 2014
Sec. Nanotechnology for Energy Applications
Volume 2 - 2014 | https://doi.org/10.3389/fenrg.2014.00033

Three-dimensional porous architectures of carbon nanotubes and graphene sheets for energy applications

  • Division of Bioengineering, School of Chemical and Biomedical Engineering, Nanyang Technological University, Singapore, Singapore

Owing to their extraordinary physicochemical, electrical, and mechanical properties, carbon nanotubes (CNTs) and graphene materials have been widely used to improve energy storage and conversion. In this article, we briefly review the latest development on fabrication of 3D porous structures of CNTs or graphene sheets or their hybrids, and their applications in various energy devices including supercapacitors, (bio-) fuel cells, and lithium ion batteries.

Introduction

In the past decades, carbon nanotubes (CNTs) and graphen have changed the landscape of many fields in science and technology, including energy storage and conversion (Sun et al., 2011b; Liu et al., 2012; Weiss et al., 2012; Jariwala et al., 2013; Zhang et al., 2013). Although differing in structure, synthetic routes, and physicochemical properties, the two carbon allotropes share common merits for energy applications, such as good electrical conductivity, high-specific surface area, excellent mechanical strength, and flexibility. In frequent cases, integration of 1D CNT and 2D graphene materials exerts synergistic effects. Despite the great success achieved, further extending their potential, to a great extent, depends on the possibility to assemble these nanocarbon materials into macroscopic 3D architectures while preserving the intrinsic properties of individual building components.

The electrochemical electrodes used in energy devices or for other purposes are conventionally planar. Electrodes based on 3D porous nanocarbon structures can greatly improve the capacity and efficiency because of largely expanded working volume, multiplexed conduction network, 3D interfacing, or intercalation with other system components (e.g., electrolytes, reactants). However, it is non-trivial to assemble CNTs and graphene sheets into 3D architectures due to their small size as well as stacking or aggregation caused by strong hydrophobic and pi–pi interactions. In this article, we review the latest development on synthesis of macroporous CNT/graphene structures and their applications in energy devices.

Synthesis Approaches

The 3D porous CNT and graphene structures can be readily fabricated from CNT/graphene solvent dispersions via self-assembly or substrate-based deposition, which are cost-effective and easily scalable. On the other hand, chemical vapor deposition (CVD) is able to produce 3D porous CNT/graphene monoliths, with high quality and well-defined architectures. Some other approaches have also been recently developed.

3D CNT Structures

Direct deposition of dispersed CNTs onto a 3D substrate is simple and effective to construct porous architectures. For example, sponge with continuous 3D surface and good mechanical flexibility can serve as a supporting substrate. CNT-sponge composites fabricated via dip-coating method are highly porous (98%, pore size 200–500 μm) with large specific surface area of ~104 m2 m−3 (Xie et al., 2012). The thin CNT coating layer provides the composite a conductance of ~1 S cm−1. Without use of any template, self-assembled CNT foam has been made by a low temperature chemical fusion method (Figure 1) (Liu et al., 2013b). Meso-/macroporosity of the CNT foam can be tuned by the amount of ammonia carbonate, which acts as the pore former. The as-synthesized CNT foam can withstand a stress pressure as high as 1.39 MPa. Catalytic growth of CNT forests via CVD method is advantageous in well controlling the length, quality, and density of CNTs (Zheng et al., 2010; Zhan et al., 2011). Zhao et al. (2011) sputtered Fe catalysts on the surface of Ni foam for the growth of 3D randomly entangled CNTs. Shan et al. (2013) synthesized 3D sponge-like N-doped CNT architecture, employing the mixture of ferrocene, thiophene, and pyridine as CVD precursors. The N and S are proposed to synergistically promote the formation of “elbow” and “welded” junctions between CNTs. In addition, the diameter of N-doped multi-walled CNTs can be easily controlled by modulating thiophene concentration, which in turn influences the mechanical and electrical properties of N-doped MWCNT sponge.

FIGURE 1
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Figure 1. Illustration of a low temperature chemical fusion method for the synthesis of porous CNT-foam composites. Adapted with permission from Liu et al. (2013b). Copyright 2013 Royal Society of Chemistry.

3D Graphene Structures

Graphene hydrogels and aerogels

The hydrophilic edges and hydrophobic basal planes of graphene oxide (GO) render it to be amenable to solution-based processes (Sun et al., 2011a). Direct gelation of GO dispersion into porous bulk structures can be achieved by freeze-drying and hydrothermal methods (Jiang et al., 2010; Xu et al., 2010; Sun et al., 2014). Recently, Xie et al. (2013) devised a modified freeze casting process. They found that the microstructures and properties of the resulting porous graphene aerogel can be widely adjusted by the freezing temperature. Liquid nitrogen freezing confers the as-synthesized aerogel an isotopic and highly elastic structure. Wan et al. covalently cross-linked GO sheets into a monolith by conjugating the epoxy groups on GO with amine groups of a gelating polymer via ring opening reaction (Xie et al., 2013). The obtained GO hydrogel is highly elastic and can be easily converted into reduced GO (rGO) hydrogel via thermal treatment. Without using any linkage additives or chemical reducing agents, Hu et al. (2013) demonstrated substrate-assisted spontaneous reduction and assembly of GO sheets into 3D network on various conductive substrates (Figure 2A). The 3D graphene structures have also been obtained by repetitive dip-coating GO sheets into sponge, followed by GO reduction and removal of sponge by heating (Figure 2B) (Yang et al., 2014). Interestingly, Peng et al. (2014) reported a chemical unzipping approach to convert CNT sponge into graphene nanoribbon aerogel (Figure 2C). The resulting aerogel inherits the 3D network and high porosity of CNT sponge, and gains enhanced surface area and chemical functionality. It has also been shown that further hydrazine reduction helps the recovery of mechanical properties of graphene nanoribbon aerogel impaired by unzipping process. Graphene aerogel with hierarchical porous structure has also been fabricated using a so-called “sugar-blowing” approach by carbonization of a mixture of glucose and ammonia chloride (Figure 3A) (Wang et al., 2013). Such ultralight (3.0 mg cm−3) structure possesses a good mechanical strength and is highly compressible.

FIGURE 2
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Figure 2. (A) Scheme of the substrate-assisted reduction and assembly of GO on active metal substrate and arbitrary conductive target supported by active metal. Adapted with permission from Hu et al. (2013). Copyright 2013 Nature Publishing Group. (B) Schematic representation and photo images of the procedure for preparing sponge template graphene aerogel. Adapted with permission from Yang et al. (2014). Copyright 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim. (C) Illustration of the process in which a CNT sponge is directly converted into a GNR aerogel by unzipping method. Adapted with permission from Peng et al. (2014). Copyright 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

FIGURE 3
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Figure 3. (A) SEM image and schematic growth process of porous graphene structure prepared by sugar-blowing method. Adapted with permission from Wang et al. (2013). Copyright 2013 Nature Publishing Group. (B) Schematic illustrations displaying the preparation process of 3D graphene macroscopic objects. Adapted with permission from Li et al. (2013). Copyright 2013 Nature Publishing Group.

CVD Grown 3D Graphene

As first demonstrated by Chen et al. (2011), 3D defect-free graphene monolith can be obtained by CVD using Ni foam as the growth substrate. Such graphene foam exhibits macroporous structure (99.7% porosity), high-specific surface area (~850 m2 g−1), and high conductivity (~10 S cm−1). The Ni foam can be subsequently removed by acid, leaving light weighted and free-standing graphene foam (Dong et al., 2012f). Recently, Li et al. (2013) fabricated microporous 3D graphene foams via a rapid CVD process using nickel chloride hexahydrate as the catalyst precursor (Figure 3B). Prolonging the growth time enhances the thickness and strength of graphene layers. Using plasma enhanced CVD process, dense vertically oriented graphene sheets were grown on Ni foam, offering a large surface area (Ren et al., 2014).

3D CNT–Graphene Hybrids

CNT and graphene possess a plethora of different characteristics in structural and physicochemical properties. To enjoy the synergistic effects of these two graphitic allotropes, 3D CNT/graphene hybrid architectures have been prepared by hydrothermal treatment of CNT and graphene solution mixture (You et al., 2013). In this composite, the intercalating CNTs not only prevent stacking of graphene sheets but also facilitate electron and ion transport. Two-step CVD processes have been devised to grow graphene foam covered with CNT matrix (Figure 4) (Zhu et al., 2014). CNT nano-meshes on top of monolithic graphene skeleton further enhance surface area, conductivity, and charge-transfer conductance. CNT–graphene hybrid can also simply obtained by dip-coating CNT dispersion on pre-synthesized graphene foam, taking advantage of the strong hydrophobic and pi–pi interactions between CNTs and graphene (Prasad et al., 2014). Fan et al. prepared 3D CNT–graphene sandwich structure from catalyst precursor-coated GO sheets (Ma et al., 2011).

FIGURE 4
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Figure 4. Schematic illustrations of the fabricated 3D MnO2–CNT– graphene–Ni hybrids. Adapted with permission from Zhu et al. (2014). Copyright 2014 Royal Society of Chemistry.

Functionalization

The 3D nanocarbon structures can be functionalized with biomolecules, polymers, or other functional nanomaterials (e.g., precious metal nanoparticles and nanostructured metal oxides) to attain improved or new functionalities (Georgakilas et al., 2012; Chang and Wu, 2013). Functionalization of enzymes via physisorption or covalent bonding renders the 3D nanocarbon bio-catalytic capabilities. Decoration of metal or metal oxide nanoparticles renders high electrochemical or catalytic properties. Integration of conducting polymers enhances the conductivity, mechanical strength, as well as electrochemical activities. The 3D architectures not only provide a large supporting/loading surface area but also alleviate the commonly encountered problem of nanomaterial aggregation. Heteroatom doping is another effective route to modify the properties of 3D nanocarbon structures (Wang et al., 2014).

Applications

Fuel Cells

The 3D CNT/graphene structures have been employed as the electrochemical electrodes for fuel cells that convert chemical energy into electricity (Maiyalagan et al., 2012). In a direct methanol fuel cell, Huang et al. (2014) used Pt-decorated graphene/g-C3N4 composite as the anode for methanol oxidation (Figure 5A). It provides higher forward-scan peak current, better anti-poisoning capability, and superior long-term stability than Pt/graphene, Pt/carbon nitride, and commercial Pt/C electrodes. The 3D porous graphene structure is advantageous for rapid transport of ions, fuel molecules, and electrons, as well as homogeneous and dense loading of Pt nanoparticles. A novel iron nitride/nitrogen doped-graphene aerogel hybrid synthesized by a two-step hydrothermal process was used as the fuel-cell cathode for oxygen reduction reaction (ORR) (Figure 5B) (Yin et al., 2014). It demonstrated more positive onset reduction potential, higher current density, and lower charge-transfer resistance than electrodes based on iron nitride or N-doped graphene aerogel. With comparable catalytic activity, the hybrid outperforms the commercial Pt/C catalyst in methanol crossover resistance and stability. Heteroatom doping can confer 3D graphene/CNT architectures with remarkable electrocatalytic ability for ORR. The 3D N-doped CNT-arrays have been reported to exhibit excellent ORR activity with the ideal four electron pathway in both acid and alkaline conditions (Gong et al., 2009; Xiong et al., 2010). Using CVD method, Xue et al. (2013) synthesized B/N co-doped graphene foam as efficient metal-free ORR catalyst. It offers a higher reduction peak current than the commercial Pt–C/glassy carbon electrode.

FIGURE 5
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Figure 5. (A) Illustration of the synthesis of the 3D Pt/graphene– carbon nitride catalyst and its electrochemical performance in direct methanol fuel cell. Adapted with permission from Huang et al. (2014). Copyright 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim. (B) Illustration of the preparation procedure of FexN/N-doped graphene aerogel and its oxygen reduction reaction performance. Adapted with permission from Yin et al. (2014). Copyright 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

Biofuel Cells

Biofuel cells share the same design with traditional fuel cell while replacing anode catalyst with biological components (enzymes or microorganisms), which are able to harvest biochemical energy into electricity. One major problem of enzymatic biofuel cell is the poor electron transfer from the buried catalytic centers of the enzyme molecules. To tackle this issue, Prasad et al. (2014) employed enzyme decorated 3D hybrid of graphene foam and single-walled CNTs as novel biofuel cell electrodes. The as-fabricated device attains the theoretical limit of open circuit voltage (~1.2 V) and a high power density of 2.27 mW cm−2, which benefits from the large surface area and high conductivity of the 3D electrodes, and the nearly perfect electrical coupling ensured by the intimate contact between enzyme molecules and nanotopographic electrode surface. In comparison to the conventional planar electrodes, 3D carbon electrodes can greatly improve the output of microbial fuel cells by promoting colonization and loading of electrogenic bacteria and 3D electrical coupling. Xie et al. (2012) employed 3D CNT-coated macroporous sponge as the bioanode and achieved a maximum current density of 10.63 mA cm−3 in glucose media, which was 48% higher than that of CNT-textile electrode. Yong et al. (2012) demonstrated a novel 3D macroporous anode based on PANI decorated CVD-grown 3D graphene foam, which reached a powder density of ~190 mW m−2. It significantly outperforms planar carbon electrodes, e.g., carbon cloth or felt electrode with or without PANI coating.

Supercapacitors

The 3D CNT/graphene architectures, with low level aggregation and agglomeration of individual CNTs of graphene sheets, are able to provide large electric double-layer capacitance (EDLC) owing to large surface area. In addition, they permit high loading of electrochemically active nanomaterials to gain high electrochemical pseudocapacitance. The 3D carbon nanocup-CNT structures have been synthesized on anodized aluminum oxide for EDLC based supercapacitors (Hahm et al., 2012). The CNT modification gives carbon nanocup an extremely high-specific surface area (1340 m2 g−1) and enhances its capacitance to 45 F g−1 in 1 M LiPF6. Open-porous rGO foam prepared from autoclave leavening GO film is also able to provide a large EDLC (110 F g−1) which is one order higher than that of rGO films (17 F g−1) (Niu et al., 2012). Seamless and sp2-carbon connection of CVD grown graphene are advantageous to exploit the synergistic effects between CNT and graphene. The 3D graphene–CNT hybrids grown on nickel foam prepared by two-step CVD approach have been reported to exhibit a five-time-higher specific capacitance than CNT directly grown on inconel without graphene as the supporting substrate (Yan et al., 2013).

Jiang et al. (2013) prepared vertically aligned CNT forest with uniformly embedded nickel oxide nanoparticles, which delivered a 5.7 times higher specific capacitance (1.26 F cm−3) than pure CNT forest samples because of combination of both EDLC and pseduocapacitance (Figure 6A). Niu et al. (2014) reported a general strategy to prepare functional porous graphene hybrid architectures (Figure 6B). As an example, rGO/PANI nanofiber electrode offers a high-specific capacitance of 475 F g−1, much larger than that of pure rGO architecture. CVD-grown graphene foam with well-defined macroporous structure can serve as an excellent platform to prepare various functional supercapacitor electrodes (Dong et al., 2012a,d). For example, deposition of nanostructured Co3O4 on CVD-graphene foam offers a high-specific capacitance of 1100 F g−1 (Dong et al., 2012f). Zhu et al. prepared 3D MnO2–CNT–graphene–nickel hybrid foam. Such porous and highly conductive electrode delivers a specific capacitance of ~251 F g−1 (Zhu et al., 2014). Heteroatom doping and integration of CNTs can be employed to enhance the capacitive behavior. You et al. (2013) prepared N-doped 3D CNT–graphene aerogel electrode for supercapacitor application. It gives a maximum specific capacitance of 180 F g−1 at a current density of 0.5 A g−1. Addition of CNTs effectively prevents graphene aggregation and improves the conductivity.

FIGURE 6
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Figure 6. (A) Schematic of the pseudocapacitor using CNT forests functionalized with oxidized nickel nanoparticles as the electrode and its cyclic voltammetry curves in 0.1 M KOH at scan rates of 100 mV s−1. Adapted with permission from Jiang et al. (2013). Copyright 2013 American Chemical Society. (B) Schematic of preparing porous graphene hybrid structures by a hydrothermal co-assembly process and the capacitive behavior of resultant 3D graphene/polyaniline example. Adapted with permission from Niu et al. (2014). Copyright 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

Lithium Ion Batteries

The 3D porous graphene/CNT architectures are also attractive for lithium ion batter (LIB), which can improve Li ion diffusion and tolerance to mechanical stress induced by ion deintercalation process. Ruoff group first applied CVD-grown 3D graphene for LIB cathode (Ji et al., 2012). Accounting the total mass, such 3D graphene loaded with lithium iron phosphate exhibited a 23 and 170% higher specific capacity than that of Al- and Ni-foam loaded with lithium iron phosphate, respectively. Xiao et al. (2013) prepared 3D graphene aerogel/Fe2O3 composite by a one-pot hydrothermal process. The synergistic interaction between uniformly dispersed Fe2O3 nanoparticles and robust 3D graphene aerogel endows such electrode with a high reversible capacity of 995 mA h g−1, which is almost four times to that of physically mixed Fe2O3–graphene electrode. Integration of CNTs to a similar electrode further increases the reversible capacity to 1118 mA h g−1 (Liu et al., 2013a). Qiu et al. (2014) prepared TiO2 nanocrystal/graphene aerogel as LIB anode, using glucose as dispersion and linking agent. A reversible capacity of 956.2 mA h g−1was achieved, which is superior to the previously reported TiO2/carbon electrodes (Yang et al., 2012). Even at a high current density of 5000 mA h g−1, the hybrid foam electrode still gives a reversible capacity of 99 mA h g−1, four times higher than that of pure TiO2 based electrode. Gong et al. (2014) developed a bottom-up method to construct 3D LIB electrode from GO sheets and exfoliated MoS2 nanosheets. The resultant MoS2–graphene electrodes exhibit a high reversible capacity of ~1200 mA h g−1, good stability, and excellent rate performance. Cao et al. (2013) coated nanostructured MoS2 on CVD-grown graphene foam by dip-coating and annealing method and demonstrated a high reversible capacity of 877 mA h g−1 at a current density of 100 mA h g−1.

Conclusion and Perspectives

In summary, electrochemical electrodes based on 3D nanocarbon structures, as compared with conventional planar electrodes, can greatly enhance the capacity, efficiency, or stability for the energy storage and conversion devices. Although this article focuses on energy devices, electrochemical electrodes based on 3D architecture of CNTs or graphene or their hybrid are also instrumental to other applications. For example, Dong et al. (2012b) developed a hybrid foam of graphene and CNT for selective removal of oil and organic solvent from water surface. Yin et al. (2013) used 3D graphene/metal oxide composite for effective capacitive deionization from water. Ananthanarayanan et al. (2014) successfully synthesized fluorescent graphene quantum dots from 3D graphene foam. Furthermore, electrochemical sensors based on 3D nanocarbon electrodes offer higher sensitivity or larger detection range as compared to traditional planar electrodes (Dong et al., 2012c,e; Xi et al., 2013). The 3D nanocarbon substrates can also serve as supporting scaffolds to incorporate other 2D materials such as transition metal dichalcogenide nanosheets. Although with challenges, developing new strategies to controllably fabricate functional 3D electrodes while preserving the intrinsic merits of CNTs or graphene will continue to provide tremendous thrusts to energy as well as many other applications.

Conflict of Interest Statement

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Acknowledgments

We thank the support from the Agency for Science, Technology and Research (A*STAR) under a SERC Grant (102 170 0142) and Ministry of Education of Singapore under an AcRF Tier 2 grant (MOE2011-T2-2-010).

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Keywords: carbon nanotube, graphene, three-dimensional architecture, energy storage, energy conversion

Citation: Wang X, Sun G and Chen P (2014) Three-dimensional porous architectures of carbon nanotubes and graphene sheets for energy applications. Front. Energy Res. 2:33. doi: 10.3389/fenrg.2014.00033

Received: 15 July 2014; Paper pending published: 28 July 2014;
Accepted: 04 August 2014; Published online: 20 August 2014.

Edited by:

Lain-Jong Li, Academia Sinica, Taiwan

Reviewed by:

Yumeng Shi, Singapore University of Technology and Design, Singapore
Yi-Hsien Lee, National Tsing-Hua University, Taiwan

Copyright: © 2014 Wang, Sun and Chen. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) or licensor are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.

*Correspondence: Peng Chen, Division of Bioengineering, School of Chemical and Biomedical Engineering, Nanyang Technological University, 70 Nanyang Drive 637457, Singapore e-mail: chenpeng@ntu.edu.sg

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