0
Research Papers

# Synthesis and Characterization of Dielectric Elastomer Nanocomposites Filled With Multiwalled Carbon NanotubesPUBLIC ACCESS

[+] Author and Article Information
Yu Wang

Department of Chemical Engineering
and Materials Science,
University of California,
Irvine, CA 92697

L. Z. Sun

Department of Chemical Engineering
and Materials Science;
Department of Civil
and Environmental Engineering,
University of California,
Irvine, CA 92697
e-mail: lsun@uci.edu

1Corresponding author.

Contributed by the Materials Division of ASME for publication in the JOURNAL OF ENGINEERING MATERIALS AND TECHNOLOGY. Manuscript received June 10, 2016; final manuscript received September 14, 2016; published online February 9, 2017. Assoc. Editor: Xi Chen.

J. Eng. Mater. Technol 139(2), 021018 (Feb 09, 2017) (8 pages) Paper No: MATS-16-1177; doi: 10.1115/1.4035490 History: Received June 10, 2016; Revised September 14, 2016

## Abstract

Dielectric elastomers (DEs) have been attracting great attention in the field of electro-mechanical actuation and sensing. In this paper, we develop a new type of silicone-based DEs by incorporating multiwalled carbon nanotubes (MWNTs) to the DEs as fillers. The dispersion of MWNTs during the material processing plays a significant role in deciding the final properties of the nanocomposites. In this work, acetone and ultrasonication along with characterization tools such as scanning electron microscopy (SEM) and transmission electron microscopy (TEM) are utilized to examine the MWNT dispersion quality within DE nanocomposites. Furthermore, microstructural MWNT dispersion and filler–matrix interfacial bonding as well as the overall dynamic mechanical responses are investigated to reveal the correlation between them. It is concluded that the processing of DE nanocomposites strongly affects the dynamic mechanical properties, which can inversely provide with microstructural information for the nanocomposites.

<>

## Introduction

Polymeric composites filled with carbon nanotubes (CNTs) are promising materials demonstrating excellent thermal, mechanical, and electrical functionalities due to the unique properties such as high aspect ratio and high conductivity of CNTs. Traditionally, many research efforts have been conducted to utilize CNTs as fillers to reinforce the mechanical properties and increase the electrical conductivity of the polymeric composites [16].

Within the family of electro-active polymers (EAPs), DEs have been attracting great attention in the field of energy harvesting materials [7,8] as well as actuating materials for potential applications such as artificial muscles, capacitors, sensors, and even generators due to their high electromechanical efficiency, durability, stability, lightweight, low cost, and easy processing [812]. Pelrine et al. first demonstrated the potential of DEs [9,13,14] and developed models to describe the behavior of silicone-based DEs to seek the possibility to be used as actuators. They numerically showed how the Maxwell stress correlated with the electromechanical response of DE materials. An electromechanical response is the physical response of a mechanical system to electrical stimulation and vice versa. Despite the advantages of DEs, technical challenges must be resolved for wider applications. A high electric field of at least 10–30 V/μm is required for DEs to actuate, which hinders the practical applications especially in biomedical fields [8,15].

For wider applications, the required electric fields need to be reduced. In this paper, it is proposed to utilize CNTs as fillers to further improve performance of DEs [1620] by enhancing the dielectric response of DEs. Among CNTs, MWNTs are commercially the cheapest and easiest to obtain in the market. Specifically, we aim to develop a new generation of silicone-based DEs by incorporating MWNTs to the DEs as fillers at low cost. The idea comes from that only a small amount of conductive CNT fillers can drastically increase the dielectric constant [2123] while avoiding the unwanted increase of materials rigidity [23]. There have been efforts to implement ceramic powder DEs with high dielectric constants such as $TiO2$ particles [24], $BaTiO3$ nanoparticles [2527], and $PbTiO3$ [28,29]. However, high loading of these particles up to 20–30 vol. % are required for meaningful increase, at which the ceramic powders-filled composites can lose its flexibility, leading to limited improvement of the electromechanical response. Higher dielectric constant of nanocomposites brings more charges on the electrodes, resulting in larger deformation under the application of the electric fields. It is known that MWNTs in a polymer matrix can increase the dielectric constant, especially, around the electrical percolation threshold [21,30]. Charge accumulation occurs at the interface of DE matrix and MWNTs with different charge carrier relaxation time (Maxwell–Wagner effect) [31,32].

The critical challenge to enable DE nanocomposites filled with MWNTs, however, is the dispersion control of MWNTs inside polymer matrix. CNTs can easily form aggregates and bundles due to van der Waals force. Aggregation of CNTs can easily be the sites of electrical conduction paths and a source of cracks [33]. Moreover, these aggregates work as stress concentration and initiator of cracks. In the practical application, the thickness of the DEs is in the range of 50–200 μm [11,33]. The size of the MWNT aggregates, as we will see in Sec. 3.1, is in the similar range as the thickness of the DEs, which causes the DEs to fail. Thus, the dispersion of MWNT is the critical issue that needs attention for DE applications.

For the past decade, dispersion of CNTs has been under extensive investigations. CNTs surface functionalization [3440] and the utilization of solvent [4148] such as acetone and ketone have been attempted to improve the dispersion in polymer matrix as well. The selection of solvent has a significant influence on the dispersion of CNTs in elastomer matrix. Acetone is a simple polar organic solvent and a common chemical commodity. Acetone is utilized as a solvent to dilute the pure elastomer and reduce the viscosity during the fabrication process [47].

In this paper, synthesis and characterization of DE nanocomposites filled with MWNTs are studied. The techniques to disperse MWNTs are discussed. Furthermore, the damage to MWNTs due to the processing techniques is investigated. The correlation between the dispersion of MWNTs and properties of DE nanocomposites is revealed.

## Materials and Method

Alumilite HS III RTV high-strength mold-making silicone rubber is chosen as the DE matrix. Acetone, from Fisher Scientific, is used as a solvent to help CNTs disperse in elastomers. MWNTs, purchased from Cheap Tubes,2 are used as fillers in DEs. MWNTs have outer diameter 20–30 nm, inside diameter 5–10 nm, length 10–30 μm, and specific surface area 110 m2/g according to Cheap Tubes.

Figure 1 shows the flowchart of the DE nanocomposite processing steps. The fabrication process consists of the following seven steps: (1) grinding the pristine MWNT aggregates with a mortar and pestle, (2) stirring MWNTs in acetone solution by ultrasonic processor (Sonics & Materials, Inc., Newtown, CT, VCX 130) for hours, (3) pouring the elastomer matrix into the solution, (4) adding the curing agent once acetone evaporates and mixing the solution, and (5) vacuum degassing the mixture for minutes using MZ2C+2AK oil-free vacuum pump, (6) spin coating the materials to obtain thin film specimens with controlled thickness, and (7) pouring the materials to the mold. The curing process takes approximately 72 h.

Uniform dispersion of MWNTs in elastomer matrix can be a common challenge. Therefore, based on our previous development [49], grinding and solution mixing with ultrasonication are applied to break the van der Waals forces between MWNTs to minimize the formation of MWNT aggregates. Vacuum degassing is utilized to eliminate air voids in the cured material. DE Nanocomposite samples for mechanical testing are prepared by using the molding as shown in Fig. 1. The mold is in cylinder shape with diameter 9.5 mm and height 9.5 mm following ASTM Standard D 5992-96.

Next, spin coating technique is utilized to prepare nanocomposite films for electromechanical and dielectric property measurement. The thickness of the films for DEs and DE nanocomposites is controlled to be about 150 μm by adjusting the revolution per minute (RPM) of the spin coater (Laurell Photoresist Spinner). The spin coating time is 40 s. Then the thickness of the film is measured by Digital Instruments Dektak 3 surface profiler.

After fabrication, each sample is observed by FEI Quanta three-dimensional FEG SEM. FEI/Philips CM-20 TEM is utilized to investigate the damage to MWNTs after the processing. Furthermore, mechanical properties of DE matrix and DE nanocomposites are characterized by dynamic mechanical analysis (DMA) to investigate the correlation with MWNTs dispersion. All the mechanical testing is carried out at room temperature of 24 °C by BOSE ElectroForce 3200.

## Results and Discussion

###### Minimizing the Size of MWNT Aggregates.

The DE Nanocomposites with 0.3 wt.% MWNTs are examined to investigate the acetone effect. The pristine MWNTs are shown in Fig. 2. Due to the van der Waals forces, MWNTs naturally tend to form aggregates as shown in Fig. 2.

The nanocomposites processed with and without acetones are compared. Figure 3 shows SEM images of MWNT aggregates found in the nanocomposite processed without acetone. Various sizes of MWNT clusters are observed. The typical size of the observed aggregates is in the range of 10–50 μm. For application, the DE films are typically 50–200 μm in thickness; thus, aggregates with 10–50 μm in size could easily be the sites of electrical conduction paths and a source of cracks [33], causing the DEs to fail. Figure 4 shows SEM images of DE nanocomposites processed with acetone. The typical size of the MWNT aggregates is found to be 5–20 μm, which is smaller than that of aggregates observed in the DE nanocomposites processed without acetone as shown in Fig. 3. This shows that the acetone is playing a crucial role in improving the dispersion of MWNTs. Acetone dilutes the elastomer and reduces the viscosity during the fabrication process, which enables easier mixing between the elastomer matrix and each MWNT. As a result, smaller size of MWNT aggregates is obtained.

Next, in order to further improve the dispersion of DE nanocomposites filled with MWNTs, ultrasonication is utilized. Ultrasonication is a technique to utilize high-intensity acoustic energy to mix and disperse materials [33]. Figures 57 show the dispersion of MWNTs before and after 0.5 h or 4.0 h ultrasonication. It is observed that aggregates of MWNTs still exist even with 0.5 h ultrasonication. However, as observed in Fig. 5, the typical size of MWNT aggregates is 3–8 μm, which is smaller than those observed in DE nanocomposites filled with 0.3 wt.% MWNTs processed without ultrasonication shown in Fig. 4. Figure 7 shows the typical DE nanocomposites after 4.0 h ultrasonication. As shown in Fig. 7, the aggregates are rarely observed in the DE nanocomposite processed with 4.0 h ultrasonication process, and uniformly dispersed individual MWNTs are observed.

It is also observed that the viscosity of DE matrix is significantly increased for the nanocomposites with 4.0 h ultrasonication than ones with 0.5 h ultrasonication [34]. This is due to the DE matrix–MWNT interaction, making the viscosity of DE nanocomposites higher than pure DE matrix. This is another indication that the dispersion of MWNTs is improved by longer ultrasonication technique.

Although ultrasonication significantly improves the dispersion of MWNTs in DE matrix, the damage is caused to MWNTs [33,5053] because of the energy introduced by ultrasonication. It is reported that the aspect ratio strongly depends on the material processing, and 420, 80, and 8 are reported as MWNT average aspect ratio under different treatments even for the same type of MWNTs [52].

Here, TEM is utilized to investigate the aspect ratio of MWNTs after the processing. Figure 8 shows three typical images obtained from TEM. Based on images obtained from TEM as shown in Fig. 8, the typical length of MWNTs after 4.0 h ultrasonication ranges from 400 nm to 1 μm. This is significantly shorter than the pristine MWNTs with 20–30 nm in diameter, and 10–30 μm in length. This is most likely due to the lengthy time of ultrasonication, resulting in the breakage of MWNTs. Table 1 shows the calculated approximate aspect ratio of MWNTs. After the 4.0 h ultrasonication, the aspect ratio significantly dropped. Ultrasonication introduces shearing along the axis, causing failure between MWNTs at stresses much below the intrinsic properties of a single nanotube [54]. As a result, ends of each MWNT, for instance, are damaged and opened, leading to higher reactivity of MWNTs. Figure 8(b) shows an example of the probable damage to MWNTs.

###### Relationship Between the MWNT Dispersion and Mechanical Properties of Nanocomposites.

Silicone-based DEs are viscoelastic in nature. Thus, dynamic mechanical analysis is used to investigate the responses of DE nanocomposites with MWNT dispersions. The response of viscoelastic materials to a sinusoidal loading is usually represented by storage modulus, loss modulus, and $tan δ$. Storage modulus represents the elastic portion and loss modulus represents the viscous portion. The value of $tan δ$ represents the ratio of the dissipated energy over the stored energy, showing the damping capacity of the materials.

Figure 9 shows the dynamic mechanical analysis results of nanocomposites with 0.3 wt.% MWNTs at 10 Hz. The introduction of 0.3 wt.% MWNTs in elastomer matrix enhances the storage modulus of the DE nanocomposites. The specimen with 4.0 h ultrasonication improves the storage modulus by about 25% at all the dynamic strain amplitude range while the specimen with 0.5 h ultrasonication also improves the modulus by around 11% at all the dynamic strain amplitude. This demonstrates that more load transfer under compression is enabled after longer ultrasonication. This is made possible by improved MWNT dispersion together with the higher reactivity due to the damages to MWNTs as discussed earlier, leading to the larger interaction area between DE matrix and MWNTs. As a result, higher storage modulus is obtained. It is worth pointing out that the well dispersed MWNTs significantly improve the storage modulus compared to poorly dispersed MWNTs due to the increased interaction between DEs and MWNTs. While MWNTs with lower aspect ratio decrease the storage modulus of nanocomposites compared with MWNTs with higher aspect ratio, there should be a competition between these two mechanisms of aspect ratio and dispersion of MWNTs. It is believed that uniform MWNT dispersion can play a leading role with respect to the increasing mechanical properties of nanocomposites.

It is also shown that the loss modulus and loss factor are increased with the longer ultrasonication. The 0.5 h ultrasonication increases the loss modulus up to 9% while the 4.0 h ultrasonication increases the loss modulus by 40%. Moreover, the 0.5 h ultrasonication increases the loss factor up to 15% while the 4.0 h ultrasonication increases loss factor by 20–25%. One possible reason behind this is related to the nature of bonding between DE matrix and MWNTs. Although improved dispersion enables the larger interaction area between DE matrix and MWNTs, the bonding between them is partially weak. As a result, energy loss by interfacial frictions between the MWNTs and elastomer matrix under dynamic mechanical loading becomes more significant as the interfacial area between MWNTs elastomers increases [55].

This phenomenon is not prominent for samples with 0.5 h ultrasonication compared to those with 4.0 h ultrasonication as the existence of aggregates significantly reduces the effective interfacial areas between the elastomer matrix and MWNTs. However, the DE nanocomposites processed with 4.0 h ultrasonication show the significant energy loss. Figure 10 shows the two-dimensional schematic image of the MWNTs and MWNT aggregates within DE nanocomposites. For simplicity, complex geometric features such as waviness [56,57] are not included. Dash lines in the figure show the interfacial area between DE matrix and MWNT aggregates. As the MWNT dispersion improves, interfacial area between DE matrix and MWNT aggregates is replaced by that between DE matrix and individual MWNTs, resulting in significantly more interfacial sliding and energy loss under dynamic mechanical loading. As a result, DE nanocomposites processed with 4.0 h ultrasonication shows larger loss modulus and loss factor.

In summary, dynamic mechanical analysis is a simple material characterization tool to study the dispersion of filler in DE nanocomposites. Along with characterization techniques such as SEM and TEM, DMA can be utilized to investigate the quality of DE nanocomposites and processing procedures.

## Conclusions

Acetone and ultrasonication are demonstrated to be an effective approach to disperse MWNTs in DE matrix for dielectric elastomer nanocomposites. Acetone reduces the size of the aggregates and the viscosity of elastomer, resulting in improved mixing of DEs and MWNTs. Ultrasonication further improves the dispersion of MWNTs by adding energy to break the van der Waals force between each MWNT. Another important outcome of ultrasonication is the damage to MWNTs as mentioned earlier, resulting in shortened aspect ratio.

Under dynamic mechanical loading, higher load transfer and larger energy dissipation are observed from the DE nanocomposites filled with MWNTs as a result of improved MWNTs in DE matrix. Dynamic mechanical properties of DE nanocomposites have been proven to be closely correlated with the dispersion of MWNTs. The increase of the storage modulus is associated with the enhanced elastic properties of DE nanocomposites due to the MWNT dispersion improvement. As the dispersion improves, more elastomer–MWNT interaction is enabled. As a result, more dynamic load can be carried due to the extended interfacial area between elastomer and MWNTs. The loss modulus and loss factor are associated with the nature of the bonding between elastomer and MWNTs. As the dispersion improves, more elastomer–MWNT interaction is enabled. Although interfacial area between elastomer and pristine MWNTs increases, the weak bonding between two phases enables sliding. As a result, the friction is generated at the weak bonding sites when dynamic mechanical loading is applied.

## Acknowledgements

This work was sponsored by the National Science Foundation (NSF) under Grants Nos. CMMI-0800417 and CMMI-1229405. The supports are gratefully acknowledged.

## References

Hou, Y. , Tang, J. , Zhang, H. B. , Qian, C. , Feng, Y. Y. , and Liu, J. , 2009, “ Functionalized Few-Walled Carbon Nanotubes for Mechanical Reinforcement of Polymeric Composites,” ACS Nano, 3(5), pp. 1057–1062. [PubMed]
Huang, Y. Y. , and Terentjev, E. M. , 2010, “ Tailoring the Electrical Properties of Carbon Nanotube-Polymer Composites,” Adv. Funct. Mater., 20(23), pp. 4062–4068.
Xu, X. J. , Thwe, M. M. , Shearwood, C. , and Liao, K. , 2002, “ Mechanical Properties and Interfacial Characteristics of Carbon-Nanotube-Reinforced Epoxy Thin Films,” Appl. Phys. Lett., 81(15), pp. 2833–2835.
Coleman, J. N. , Khan, U. , Blau, W. J. , and Gun'ko, Y. K. , 2006, “ Small but Strong: A Review of the Mechanical Properties of Carbon Nanotube-Polymer Composites,” Carbon, 44(9), pp. 1624–1652.
Shao, L. H. , Luo, R. Y. , Bai, S. L. , and Wang, J. , 2009, “ Prediction of Effective Moduli of Carbon Nanotube-Reinforced Composites With Waviness and Debonding,” Compos. Struct., 87(3), pp. 274–281.
Bhuiyan, M. A. , Pucha, R. V. , Karevan, M. , and Kalaitzidou, K. , 2011, “ Tensile Modulus of Carbon Nanotube/Polypropylene Composites–A Computational Study Based on Experimental Characterization,” Comput. Mater. Sci., 50(8), pp. 2347–2353.
Koh, S. J. A. , Zhao, X. , and Suo, Z. , 2009, “ Maximal Energy That Can Be Converted by a Dielectric Elastomer Generator,” Appl. Phys. Lett., 94(26), p. 262902.
Brochu, P. , and Pei, Q. , 2010, “ Advances in Dielectric Elastomers for Actuators and Artificial Muscles,” Macromol. Rapid Commun., 31(1), pp. 10–36. [PubMed]
Pelrine, R. , Kornbluh, R. , Joseph, J. , Heydt, R. , Pei, Q. B. , and Chiba, S. , 2000, “ High-Field Deformation of Elastomeric Dielectrics for Actuators,” Mater. Sci. Eng., C, 11(2), pp. 89–100.
Kang, G. , Kim, K.-S. , and Kim, S. , 2011, “ Note: Analysis of the Efficiency of a Dielectric Elastomer Generator for Energy Harvesting,” Rev. Sci. Instrum., 82(4), p. 046101. [PubMed]
O'Halloran, A. , O'Malley, F. , and McHugh, P. , 2008, “ A Review on Dielectric Elastomer Actuators, Technology, Applications, and Challenges,” J. Appl. Phys., 104(7), p. 071101.
Anderson, I. A. , Gisby, T. A. , McKay, T. G. , O'Brien, B. M. , and Calius, E. P. , 2012, “ Multi-Functional Dielectric Elastomer Artificial Muscles for Soft and Smart Machines,” J. Appl. Phys., 112(4), p. 041101.
Pelrine, R. , 2000, “ High-Speed Electrically Actuated Elastomers With Strain Greater Than 100%,” Science, 287(5454), pp. 836–839. [PubMed]
Pelrine, R. , Sommer-Larsen, P. , Kornbluh, R. , Heydt, R. , Kofod, G. , Pei, Q. B. , and Gravesen, P. , 2001, “ Applications of Dielectric Elastomer Actuators,” Proc. SPIE, 4329, pp. 335–349.
O'Brien, B. M. , Calius, E. P. , Inamura, T. , Xie, S. Q. , and Anderson, I. A. , 2010, “ Dielectric Elastomer Switches for Smart Artificial Muscles,” Appl. Phys. A, 100(2), pp. 385–389.
Wang, L. , and Dang, Z. M. , 2005, “ Carbon Nanotube Composites With High Dielectric Constant at Low Percolation Threshold,” Appl. Phys. Lett., 87(4), p. 042903.
Basu, R. , and Iannacchione, G. S. , 2008, “ Dielectric Response of Multiwalled Carbon Nanotubes as a Function of Applied AC-Electric Fields,” J. Appl. Phys., 104(11), p. 114107.
Dang, Z. M. , Wang, L. , Yin, Y. , Zhang, Q. , and Lei, Q. Q. , 2007, “ Giant Dielectric Permittivities in Functionalized Carbon-Nanotube/Electroactive-Polymer Nanocomposites,” Adv. Mater., 19(6), pp. 852–857.
Galantini, F. , Bianchi, S. , Castelvetro, V. , and Gallone, G. , 2013, “ Functionalized Carbon Nanotubes as a Filler for Dielectric Elastomer Composites With Improved Actuation Performance,” Smart Mater. Struct., 22(5), p. 055025.
Wang, Y. , Kim, S. , Li, G. P. , and Sun, L. Z. , 2015, “ Filler Orientation Effect on Relative Permittivity of Dielectric Elastomer Nanocomposites Filled With Carbon Nanotubes,” Comput. Mater. Sci., 104, pp. 69–75.
Pötschke, P. , Dudkin, S. M. , and Alig, I. , 2003, “ Dielectric Spectroscopy on Melt Processed Polycarbonate—Multiwalled Carbon Nanotube Composites,” Polymer, 44(17), pp. 5023–5030.
Dang, Z. M. , Wang, L. , Yin, Y. , Zhang, Q. , and Lei, Q. Q. , 2007, “ Giant Dielectric Permittivities in Functionalized Carbon-Nanotube/Electroactive-Polymer Nanocomposites,” Adv. Mater., 19(6), pp. 852–857.
Underhill, R. S. , and Michalchuk, B. W. , 2005, Carbon Nanotube-Elastomer Composites for Use in Dielectric Polymer Actuators, IEEE Computer Society, Los Alamitos, CA.
Ouyang, G. , Wang, K. , and Chen, X. Y. , 2012, “ TiO2 Nanoparticles Modified Polydimethylsiloxane With Fast Response Time and Increased Dielectric Constant,” J. Micromech. Microeng., 22(7), p. 074002.
Huang, X. , Xie, L. , Hu, Z. , and Jiang, P. , 2011, “ Influence of BaTiO3 Nanoparticles on Dielectric, Thermophysical and Mechanical Properties of Ethylene-Vinyl Acetate Elastomer/BaTiO3 Microcomposites,” IEEE Trans. Dielectr. Electr. Insul., 18(2), pp. 375–383.
Wang, Z. P. , Nelson, J. K. , Hillborg, H. , Zhao, S. , and Schadler, L. S. , 2013, “ Dielectric Constant and Breakdown Strength of Polymer Composites With High Aspect Ratio Fillers Studied by Finite Element Models,” Compos. Sci. Technol., 76, pp. 29–36.
Yang, D. , Tian, M. , Dong, Y. , Kang, H. , Gong, D. , and Zhang, L. , 2013, “ A High-Performance Dielectric Elastomer Consisting of Bio-Based Polyester Elastomer and Titanium Dioxide Powder,” J. Appl. Phys., 114(15), p. 154104.
Gallone, G. , Carpi, F. , De Rossi, D. , Levita, G. , and Marchetti, A. , 2007, “ Dielectric Constant Enhancement in a Silicone Elastomer Filled With Lead Magnesium Niobate–Lead Titanate,” Mater. Sci. Eng., C, 27(1), pp. 110–116.
Bai, Y. , Cheng, Z. Y. , Bharti, V. , Xu, H. S. , and Zhang, Q. M. , 2000, “ High-Dielectric-Constant Ceramic-Powder Polymer Composites,” Appl. Phys. Lett., 76(25), pp. 3804–3806.
Shi, S. L. , and Liang, J. , 2006, “ Effect of Multiwall Carbon Nanotubes on Electrical and Dielectric Properties of Yttria-Stabilized Zirconia Ceramic,” J. Am. Ceram. Soc., 89(11), pp. 3533–3535.
Iwamoto, M. , 2012, Maxwell–Wagner Effect, Springer, Dordrecht, The Netherlands.
Tchmutin, I. A. , Ponomarenko, A. T. , Shevchenko, V. G. , Ryvkina, N. G. , Klason, C. , and McQueen, D. H. , 1998, “ Electrical Transport in 0-3 Epoxy Resin Barium Titanate Carbon Black Polymer Composites,” J. Polym. Sci., Part B: Polym. Phys., 36(11), pp. 1847–1856.
Montazeri, A. , and Chitsazzadeh, M. , 2014, “ Effect of Sonication Parameters on the Mechanical Properties of Multi-Walled Carbon Nanotube/Epoxy Composites,” Mater. Des., 56, pp. 500–508.
Sun, L. , Warren, G. L. , O'Reilly, J. Y. , Everett, W. N. , Lee, S. M. , Davis, D. , Lagoudas, D. , and Sue, H.-J. , 2008, “ Mechanical Properties of Surface-Functionalized SWCNT/Epoxy Composites,” Carbon, 46(2), pp. 320–328.
Riggs, J. E. , Guo, Z. X. , Carroll, D. L. , and Sun, Y. P. , 2000, “ Strong Luminescence of Solubilized Carbon Nanotubes,” J. Am. Chem. Soc., 122(24), pp. 5879–5880.
Paiva, M. C. , Zhou, B. , Fernando, K. A. S. , Lin, Y. , Kennedy, J. M. , and Sun, Y. P. , 2004, “ Mechanical and Morphological Characterization of Polymer-Carbon Nanocomposites From Functionalized Carbon Nanotubes,” Carbon, 42(14), pp. 2849–2854.
Qu, L. W. , Lin, Y. , Hill, D. E. , Zhou, B. , Wang, W. , Sun, X. F. , Kitaygorodskiy, A. , Suarez, M. , Connell, J. W. , Allard, L. F. , and Sun, Y.-P. , 2004, “ Polyimide-Functionalized Carbon Nanotubes: Synthesis and Dispersion in Nanocomposite Films,” Macromolecules, 37(16), pp. 6055–6060.
Mitchell, C. A. , Bahr, J. L. , Arepalli, S. , Tour, J. M. , and Krishnamoorti, R. , 2002, “ Dispersion of Functionalized Carbon Nanotubes in Polystyrene,” Macromolecules, 35(23), pp. 8825–8830.
Zeng, H. L. , Gao, C. , and Yan, D. Y. , 2006, “ Poly(Epsilon-Caprolactone)-Functionalized Carbon Nanotubes and Their Biodegradation Properties,” Adv. Funct. Mater., 16(6), pp. 812–818.
Zhang, L. , Ni, Q. Q. , Natsuki, T. , and Fu, Y. Q. , 2009, “ Carbon Nanotubes/Magnetite Hybrids Prepared by a Facile Synthesis Process and Their Magnetic Properties,” Appl. Surf. Sci., 255(20), pp. 8676–8681.
Shih, Y.-H. , and Li, M.-S. , 2008, “ Adsorption of Selected Volatile Organic Vapors on Multiwall Carbon Nanotubes,” J. Hazard. Mater., 154(1–3), pp. 21–28. [PubMed]
Xie, X. L. , Mai, Y. W. , and Zhou, X. P. , 2005, “ Dispersion and Alignment of Carbon Nanotubes in Polymer Matrix: A Review,” Mater. Sci. Eng., R, 49(4), pp. 89–112.
Ryszkowska, J. , Jurczyk-Kowalska, M. , Szymborski, T. , and Kurzydlowski, K. J. , 2007, “ Dispersion of Carbon Nanotubes in Polyurethane Matrix,” Phys. E, 39(1), pp. 124–127.
Varela-Rizo, H. , Rodriguez-Pastor, I. , and Martin-Gullon, I. , 2012, “ Effect of Solvent Nature in Casting-Based Carbon Nanofiber/Poly(Methyl-Methacrylate) Nanocomposites,” J. Appl. Polym. Sci., 125(4), pp. 3228–3238.
Kazachkin, D. , Nishimura, Y. , Irle, S. , Morokuma, K. , Vidic, R. D. , and Borguet, E. , 2008, “ Interaction of Acetone With Single Wall Carbon Nanotubes at Cryogenic Temperatures: A Combined Temperature Programmed Desorption and Theoretical Study,” Langmuir, 24(15), pp. 7848–7856. [PubMed]
Lee, C. U. , and Dadmun, M. D. , 2008, “ Improving the Dispersion and Interfaces in Polymer-Carbon Nanotube Nanocomposites by Sample Preparation Choice,” J. Polym. Sci., Part B: Polym. Phys., 46(16), pp. 1747–1759.
Liao, Y. H. , Marietta-Tondin, O. , Liang, Z. Y. , Zhang, C. , and Wang, B. , 2004, “ Investigation of the Dispersion Process of SWNTs/SC-15 Epoxy Resin Nanocomposites,” Mater. Sci. Eng., A, 385(1–2), pp. 175–181.
Lau, K. T. , Lu, M. , Lam, C. K. , Cheung, H. Y. , Sheng, F. L. , and Li, H. L. , 2005, “ Thermal and Mechanical Properties of Single-Walled Carbon Nanotube Bundle-Reinforced Epoxy Nanocomposites: The Role of Solvent for Nanotube Dispersion,” Compos. Sci. Technol., 65(5), pp. 719–725.
Li, R. , and Sun, L. Z. , 2011, “ Dynamic Mechanical Behavior of Magnetorheological Nanocomposites Filled With Carbon Nanotubes,” Appl. Phys. Lett., 99(13), p. 131912.
Fiedler, B. , Gojny, F. H. , Wichmann, M. H. G. , Nolte, M. C. M. , and Schulte, K. , 2006, “ Fundamental Aspects of Nano-Reinforced Composites,” Compos. Sci. Technol., 66(16), pp. 3115–3125.
Lu, K. L. , Lago, R. M. , Chen, Y. K. , Green, M. L. H. , Harris, P. J. F. , and Tsang, S. C. , 1996, “ Mechanical Damage of Carbon Nanotubes by Ultrasound,” Carbon, 34(6), pp. 814–816.
Bai, J. B. , and Allaoui, A. , 2003, “ Effect of the Length and the Aggregate Size of MWNTs on the Improvement Efficiency of the Mechanical and Electrical Properties of Nanocomposites-Experimental Investigation,” Compos., Part A, 34(8), pp. 689–694.
Qian, D. , Dickey, E. C. , Andrews, R. , and Rantell, T. , 2000, “ Load Transfer and Deformation Mechanisms in Carbon Nanotube-Polystyrene Composites,” Appl. Phys. Lett., 76(20), pp. 2868–2870.
Breuer, O. , and Sundararaj, U. , 2004, “ Big Returns From Small Fibers: A Review of Polymer/Carbon Nanotube Composites,” Polym. Compos., 25(6), pp. 630–645.
Li, R. , and Sun, L. Z. , 2013, “ Viscoelastic Responses of Silicone-Rubber-Based Magnetorheological Elastomers Under Compressive and Shear Loadings,” ASME J. Eng. Mater. Technol., 135(2), p. 021008.
Fisher, F. T. , Bradshaw, R. D. , and Brinson, L. C. , 2003, “ Fiber Waviness in Nanotube-Reinforced Polymer Composites—I: Modulus Predictions Using Effective Nanotube Properties,” Compos. Sci. Technol., 63(11), pp. 1689–1703.
Bradshaw, R. D. , Fisher, F. T. , and Brinson, L. C. , 2003, “ Fiber Waviness in Nanotube-Reinforced Polymer Composites—II: Modeling Via Numerical Approximation of the Dilute Strain Concentration Tensor,” Compos. Sci. Technol., 63(11), pp. 1705–1722.
View article in PDF format.

## References

Hou, Y. , Tang, J. , Zhang, H. B. , Qian, C. , Feng, Y. Y. , and Liu, J. , 2009, “ Functionalized Few-Walled Carbon Nanotubes for Mechanical Reinforcement of Polymeric Composites,” ACS Nano, 3(5), pp. 1057–1062. [PubMed]
Huang, Y. Y. , and Terentjev, E. M. , 2010, “ Tailoring the Electrical Properties of Carbon Nanotube-Polymer Composites,” Adv. Funct. Mater., 20(23), pp. 4062–4068.
Xu, X. J. , Thwe, M. M. , Shearwood, C. , and Liao, K. , 2002, “ Mechanical Properties and Interfacial Characteristics of Carbon-Nanotube-Reinforced Epoxy Thin Films,” Appl. Phys. Lett., 81(15), pp. 2833–2835.
Coleman, J. N. , Khan, U. , Blau, W. J. , and Gun'ko, Y. K. , 2006, “ Small but Strong: A Review of the Mechanical Properties of Carbon Nanotube-Polymer Composites,” Carbon, 44(9), pp. 1624–1652.
Shao, L. H. , Luo, R. Y. , Bai, S. L. , and Wang, J. , 2009, “ Prediction of Effective Moduli of Carbon Nanotube-Reinforced Composites With Waviness and Debonding,” Compos. Struct., 87(3), pp. 274–281.
Bhuiyan, M. A. , Pucha, R. V. , Karevan, M. , and Kalaitzidou, K. , 2011, “ Tensile Modulus of Carbon Nanotube/Polypropylene Composites–A Computational Study Based on Experimental Characterization,” Comput. Mater. Sci., 50(8), pp. 2347–2353.
Koh, S. J. A. , Zhao, X. , and Suo, Z. , 2009, “ Maximal Energy That Can Be Converted by a Dielectric Elastomer Generator,” Appl. Phys. Lett., 94(26), p. 262902.
Brochu, P. , and Pei, Q. , 2010, “ Advances in Dielectric Elastomers for Actuators and Artificial Muscles,” Macromol. Rapid Commun., 31(1), pp. 10–36. [PubMed]
Pelrine, R. , Kornbluh, R. , Joseph, J. , Heydt, R. , Pei, Q. B. , and Chiba, S. , 2000, “ High-Field Deformation of Elastomeric Dielectrics for Actuators,” Mater. Sci. Eng., C, 11(2), pp. 89–100.
Kang, G. , Kim, K.-S. , and Kim, S. , 2011, “ Note: Analysis of the Efficiency of a Dielectric Elastomer Generator for Energy Harvesting,” Rev. Sci. Instrum., 82(4), p. 046101. [PubMed]
O'Halloran, A. , O'Malley, F. , and McHugh, P. , 2008, “ A Review on Dielectric Elastomer Actuators, Technology, Applications, and Challenges,” J. Appl. Phys., 104(7), p. 071101.
Anderson, I. A. , Gisby, T. A. , McKay, T. G. , O'Brien, B. M. , and Calius, E. P. , 2012, “ Multi-Functional Dielectric Elastomer Artificial Muscles for Soft and Smart Machines,” J. Appl. Phys., 112(4), p. 041101.
Pelrine, R. , 2000, “ High-Speed Electrically Actuated Elastomers With Strain Greater Than 100%,” Science, 287(5454), pp. 836–839. [PubMed]
Pelrine, R. , Sommer-Larsen, P. , Kornbluh, R. , Heydt, R. , Kofod, G. , Pei, Q. B. , and Gravesen, P. , 2001, “ Applications of Dielectric Elastomer Actuators,” Proc. SPIE, 4329, pp. 335–349.
O'Brien, B. M. , Calius, E. P. , Inamura, T. , Xie, S. Q. , and Anderson, I. A. , 2010, “ Dielectric Elastomer Switches for Smart Artificial Muscles,” Appl. Phys. A, 100(2), pp. 385–389.
Wang, L. , and Dang, Z. M. , 2005, “ Carbon Nanotube Composites With High Dielectric Constant at Low Percolation Threshold,” Appl. Phys. Lett., 87(4), p. 042903.
Basu, R. , and Iannacchione, G. S. , 2008, “ Dielectric Response of Multiwalled Carbon Nanotubes as a Function of Applied AC-Electric Fields,” J. Appl. Phys., 104(11), p. 114107.
Dang, Z. M. , Wang, L. , Yin, Y. , Zhang, Q. , and Lei, Q. Q. , 2007, “ Giant Dielectric Permittivities in Functionalized Carbon-Nanotube/Electroactive-Polymer Nanocomposites,” Adv. Mater., 19(6), pp. 852–857.
Galantini, F. , Bianchi, S. , Castelvetro, V. , and Gallone, G. , 2013, “ Functionalized Carbon Nanotubes as a Filler for Dielectric Elastomer Composites With Improved Actuation Performance,” Smart Mater. Struct., 22(5), p. 055025.
Wang, Y. , Kim, S. , Li, G. P. , and Sun, L. Z. , 2015, “ Filler Orientation Effect on Relative Permittivity of Dielectric Elastomer Nanocomposites Filled With Carbon Nanotubes,” Comput. Mater. Sci., 104, pp. 69–75.
Pötschke, P. , Dudkin, S. M. , and Alig, I. , 2003, “ Dielectric Spectroscopy on Melt Processed Polycarbonate—Multiwalled Carbon Nanotube Composites,” Polymer, 44(17), pp. 5023–5030.
Dang, Z. M. , Wang, L. , Yin, Y. , Zhang, Q. , and Lei, Q. Q. , 2007, “ Giant Dielectric Permittivities in Functionalized Carbon-Nanotube/Electroactive-Polymer Nanocomposites,” Adv. Mater., 19(6), pp. 852–857.
Underhill, R. S. , and Michalchuk, B. W. , 2005, Carbon Nanotube-Elastomer Composites for Use in Dielectric Polymer Actuators, IEEE Computer Society, Los Alamitos, CA.
Ouyang, G. , Wang, K. , and Chen, X. Y. , 2012, “ TiO2 Nanoparticles Modified Polydimethylsiloxane With Fast Response Time and Increased Dielectric Constant,” J. Micromech. Microeng., 22(7), p. 074002.
Huang, X. , Xie, L. , Hu, Z. , and Jiang, P. , 2011, “ Influence of BaTiO3 Nanoparticles on Dielectric, Thermophysical and Mechanical Properties of Ethylene-Vinyl Acetate Elastomer/BaTiO3 Microcomposites,” IEEE Trans. Dielectr. Electr. Insul., 18(2), pp. 375–383.
Wang, Z. P. , Nelson, J. K. , Hillborg, H. , Zhao, S. , and Schadler, L. S. , 2013, “ Dielectric Constant and Breakdown Strength of Polymer Composites With High Aspect Ratio Fillers Studied by Finite Element Models,” Compos. Sci. Technol., 76, pp. 29–36.
Yang, D. , Tian, M. , Dong, Y. , Kang, H. , Gong, D. , and Zhang, L. , 2013, “ A High-Performance Dielectric Elastomer Consisting of Bio-Based Polyester Elastomer and Titanium Dioxide Powder,” J. Appl. Phys., 114(15), p. 154104.
Gallone, G. , Carpi, F. , De Rossi, D. , Levita, G. , and Marchetti, A. , 2007, “ Dielectric Constant Enhancement in a Silicone Elastomer Filled With Lead Magnesium Niobate–Lead Titanate,” Mater. Sci. Eng., C, 27(1), pp. 110–116.
Bai, Y. , Cheng, Z. Y. , Bharti, V. , Xu, H. S. , and Zhang, Q. M. , 2000, “ High-Dielectric-Constant Ceramic-Powder Polymer Composites,” Appl. Phys. Lett., 76(25), pp. 3804–3806.
Shi, S. L. , and Liang, J. , 2006, “ Effect of Multiwall Carbon Nanotubes on Electrical and Dielectric Properties of Yttria-Stabilized Zirconia Ceramic,” J. Am. Ceram. Soc., 89(11), pp. 3533–3535.
Iwamoto, M. , 2012, Maxwell–Wagner Effect, Springer, Dordrecht, The Netherlands.
Tchmutin, I. A. , Ponomarenko, A. T. , Shevchenko, V. G. , Ryvkina, N. G. , Klason, C. , and McQueen, D. H. , 1998, “ Electrical Transport in 0-3 Epoxy Resin Barium Titanate Carbon Black Polymer Composites,” J. Polym. Sci., Part B: Polym. Phys., 36(11), pp. 1847–1856.
Montazeri, A. , and Chitsazzadeh, M. , 2014, “ Effect of Sonication Parameters on the Mechanical Properties of Multi-Walled Carbon Nanotube/Epoxy Composites,” Mater. Des., 56, pp. 500–508.
Sun, L. , Warren, G. L. , O'Reilly, J. Y. , Everett, W. N. , Lee, S. M. , Davis, D. , Lagoudas, D. , and Sue, H.-J. , 2008, “ Mechanical Properties of Surface-Functionalized SWCNT/Epoxy Composites,” Carbon, 46(2), pp. 320–328.
Riggs, J. E. , Guo, Z. X. , Carroll, D. L. , and Sun, Y. P. , 2000, “ Strong Luminescence of Solubilized Carbon Nanotubes,” J. Am. Chem. Soc., 122(24), pp. 5879–5880.
Paiva, M. C. , Zhou, B. , Fernando, K. A. S. , Lin, Y. , Kennedy, J. M. , and Sun, Y. P. , 2004, “ Mechanical and Morphological Characterization of Polymer-Carbon Nanocomposites From Functionalized Carbon Nanotubes,” Carbon, 42(14), pp. 2849–2854.
Qu, L. W. , Lin, Y. , Hill, D. E. , Zhou, B. , Wang, W. , Sun, X. F. , Kitaygorodskiy, A. , Suarez, M. , Connell, J. W. , Allard, L. F. , and Sun, Y.-P. , 2004, “ Polyimide-Functionalized Carbon Nanotubes: Synthesis and Dispersion in Nanocomposite Films,” Macromolecules, 37(16), pp. 6055–6060.
Mitchell, C. A. , Bahr, J. L. , Arepalli, S. , Tour, J. M. , and Krishnamoorti, R. , 2002, “ Dispersion of Functionalized Carbon Nanotubes in Polystyrene,” Macromolecules, 35(23), pp. 8825–8830.
Zeng, H. L. , Gao, C. , and Yan, D. Y. , 2006, “ Poly(Epsilon-Caprolactone)-Functionalized Carbon Nanotubes and Their Biodegradation Properties,” Adv. Funct. Mater., 16(6), pp. 812–818.
Zhang, L. , Ni, Q. Q. , Natsuki, T. , and Fu, Y. Q. , 2009, “ Carbon Nanotubes/Magnetite Hybrids Prepared by a Facile Synthesis Process and Their Magnetic Properties,” Appl. Surf. Sci., 255(20), pp. 8676–8681.
Shih, Y.-H. , and Li, M.-S. , 2008, “ Adsorption of Selected Volatile Organic Vapors on Multiwall Carbon Nanotubes,” J. Hazard. Mater., 154(1–3), pp. 21–28. [PubMed]
Xie, X. L. , Mai, Y. W. , and Zhou, X. P. , 2005, “ Dispersion and Alignment of Carbon Nanotubes in Polymer Matrix: A Review,” Mater. Sci. Eng., R, 49(4), pp. 89–112.
Ryszkowska, J. , Jurczyk-Kowalska, M. , Szymborski, T. , and Kurzydlowski, K. J. , 2007, “ Dispersion of Carbon Nanotubes in Polyurethane Matrix,” Phys. E, 39(1), pp. 124–127.
Varela-Rizo, H. , Rodriguez-Pastor, I. , and Martin-Gullon, I. , 2012, “ Effect of Solvent Nature in Casting-Based Carbon Nanofiber/Poly(Methyl-Methacrylate) Nanocomposites,” J. Appl. Polym. Sci., 125(4), pp. 3228–3238.
Kazachkin, D. , Nishimura, Y. , Irle, S. , Morokuma, K. , Vidic, R. D. , and Borguet, E. , 2008, “ Interaction of Acetone With Single Wall Carbon Nanotubes at Cryogenic Temperatures: A Combined Temperature Programmed Desorption and Theoretical Study,” Langmuir, 24(15), pp. 7848–7856. [PubMed]
Lee, C. U. , and Dadmun, M. D. , 2008, “ Improving the Dispersion and Interfaces in Polymer-Carbon Nanotube Nanocomposites by Sample Preparation Choice,” J. Polym. Sci., Part B: Polym. Phys., 46(16), pp. 1747–1759.
Liao, Y. H. , Marietta-Tondin, O. , Liang, Z. Y. , Zhang, C. , and Wang, B. , 2004, “ Investigation of the Dispersion Process of SWNTs/SC-15 Epoxy Resin Nanocomposites,” Mater. Sci. Eng., A, 385(1–2), pp. 175–181.
Lau, K. T. , Lu, M. , Lam, C. K. , Cheung, H. Y. , Sheng, F. L. , and Li, H. L. , 2005, “ Thermal and Mechanical Properties of Single-Walled Carbon Nanotube Bundle-Reinforced Epoxy Nanocomposites: The Role of Solvent for Nanotube Dispersion,” Compos. Sci. Technol., 65(5), pp. 719–725.
Li, R. , and Sun, L. Z. , 2011, “ Dynamic Mechanical Behavior of Magnetorheological Nanocomposites Filled With Carbon Nanotubes,” Appl. Phys. Lett., 99(13), p. 131912.
Fiedler, B. , Gojny, F. H. , Wichmann, M. H. G. , Nolte, M. C. M. , and Schulte, K. , 2006, “ Fundamental Aspects of Nano-Reinforced Composites,” Compos. Sci. Technol., 66(16), pp. 3115–3125.
Lu, K. L. , Lago, R. M. , Chen, Y. K. , Green, M. L. H. , Harris, P. J. F. , and Tsang, S. C. , 1996, “ Mechanical Damage of Carbon Nanotubes by Ultrasound,” Carbon, 34(6), pp. 814–816.
Bai, J. B. , and Allaoui, A. , 2003, “ Effect of the Length and the Aggregate Size of MWNTs on the Improvement Efficiency of the Mechanical and Electrical Properties of Nanocomposites-Experimental Investigation,” Compos., Part A, 34(8), pp. 689–694.
Qian, D. , Dickey, E. C. , Andrews, R. , and Rantell, T. , 2000, “ Load Transfer and Deformation Mechanisms in Carbon Nanotube-Polystyrene Composites,” Appl. Phys. Lett., 76(20), pp. 2868–2870.
Breuer, O. , and Sundararaj, U. , 2004, “ Big Returns From Small Fibers: A Review of Polymer/Carbon Nanotube Composites,” Polym. Compos., 25(6), pp. 630–645.
Li, R. , and Sun, L. Z. , 2013, “ Viscoelastic Responses of Silicone-Rubber-Based Magnetorheological Elastomers Under Compressive and Shear Loadings,” ASME J. Eng. Mater. Technol., 135(2), p. 021008.
Fisher, F. T. , Bradshaw, R. D. , and Brinson, L. C. , 2003, “ Fiber Waviness in Nanotube-Reinforced Polymer Composites—I: Modulus Predictions Using Effective Nanotube Properties,” Compos. Sci. Technol., 63(11), pp. 1689–1703.
Bradshaw, R. D. , Fisher, F. T. , and Brinson, L. C. , 2003, “ Fiber Waviness in Nanotube-Reinforced Polymer Composites—II: Modeling Via Numerical Approximation of the Dilute Strain Concentration Tensor,” Compos. Sci. Technol., 63(11), pp. 1705–1722.

## Figures

Fig. 1

DE nanocomposite processing steps

Fig. 2

SEM micrograph of pristine MWNTs before the processing: (a) and (b) aggregates of MWNTs, (c) zoomed in view of the box in (b). Each individual MWNT can be seen from the aggregates in (c).

Fig. 3

(a) SEM images of nanocomposites with 0.3 wt.% MWNTs processed without acetone and (b) zoomed in view of the box in (a)

Fig. 4

(a) SEM images of nanocomposites with 0.3 wt.% MWNTs processed with acetone and (b) zoomed in view of the box in (a)

Fig. 5

(a) SEM images of nanocomposites with 0.3 wt.% MWNTs processed with acetone without ultrasonication treatment and (b) zoomed in view of the box in (a)

Fig. 6

(a) SEM images of nanocomposites with 0.3 wt.% MWNTs processed with acetone with 0.5 h ultrasonication treatment and (b) zoomed in view of the box in (a)

Fig. 7

(a) SEM images of nanocomposites with 0.3 wt.% MWNTs processed with acetone with 4.0 h ultrasonication treatment and (b) zoomed in view of the box in (a)

Fig. 8

TEM images of MWNTs processed with acetone and 4.0 h ultrasonication treatment. (a)–(c) show different MWNTs.

Fig. 9

Dynamic strain sweeps of DE nanocomposites filled with 0.3 wt.% MWNTs processed with acetone and ultrasonication: (a) storage moduli, (b) loss moduli, and (c) loss factors under compression loading. The test frequency is 10 Hz.

Fig. 10

Schematic image of the dispersion of MWNTs in DE nanocomposites

## Tables

Table 1 Aspect ratio of MWNTs before and after processing
aSpecifications provided by CheapTubes.com

## Discussions

Some tools below are only available to our subscribers or users with an online account.

### Related Content

Customize your page view by dragging and repositioning the boxes below.

Related Journal Articles
Related Proceedings Articles
Related eBook Content
Topic Collections