**2. Surface modifications of carbon nanotubes with polymers**

CNTs are considered ideal materials for reinforcing fibres due to their exceptional mechani‐ cal properties. Therefore, nanotube−polymer composites have potential applications in aero‐ space science, where lightweight robust materials are needed [64]. It is widely recognised that the fabrication of high performance nanotube−polymer composites depends on the effi‐ cient load transfer from the host matrix to the tubes. The load transfer requires homogene‐ ous dispersion of the filler and strong interfacial bonding between the two components [65]. A dispersion of CNT bundles is called "macrodispersion" whereas a dispersion of individu‐ al nonbundled CNT is called a nanodispersion [66, 67]. To address these issues, several strategies for the synthesis of such composites have been developed. Currently, these strat‐ egies involve physical mixing in solution, *in situ* polymerisation of monomers in the pres‐ ence of nanotubes, surfactant-assisted processing of composites, and chemical functionalisation of the incorporated tubes. As mentioned earlier, in many applications it is necessary to tailor the chemical nature of the nanotube's walls in order to take advantage of their unique properties. For this purpose, two main approaches for the surface modification of CNTs are adopted i.e. covalent and noncovalent, depending on whether or not covalent bonding between the CNTs and the functional groups and/or modifier molecules is in‐ volved in the modification surface process. Figure 2 depicts a typical representation of such surface modifications.

#### **2.1. Noncovalent attachment of polymers**

moulding, injection moulding or extrusion. However it is important that processing condi‐ tions are optimised for the whole range of polymer–nanotube combinations. High tempera‐ ture and shear forces in the polymer fluid are able to break the carbon nanotubes bundles and CNTs can additionally affect melt properties such as viscosity, resulting in unexpected polymer degradation [49]. Andrews and co-workers [50] showed that commercial polymers such as high impact polystyrene, polypropylene and acrylonitrile–butadiene–styrene (ABS) could be melt processed with CVD-MWCNT to form composites. The polymers were blend‐ ed with nanotubes at high loading level in a high shear mixer to form master batches. An example of using combined techniques was demonstrated by Tang *et al* [51]. High density polyethylene pellets and nanotubes were melted in a beaker, then mixed and compressed. The resulting solid was broken up and added to a twin screw extruder at 170°C and extrud‐ ed through a slit die. The resulting film was then compression moulded to form a thin film.

80 Syntheses and Applications of Carbon Nanotubes and Their Composites

This fabrication strategy starts by dispersing carbon nanotubes in vinyl monomers followed by polymerising the monomers (Figure 1c). This method produces polymer-grafted CNTs mixed with free polymer chains resulting in a homogeneous dispersion of CNTs. In situ rad‐ ical polymerisation was applied for the synthesis of PMMA-based composites by Jia *et al* [52] using a radical initiator and the authors suggested that π-bonds of the CNT graphitic network were opened by the radical fragments of initiator and therefore the carbon nano‐ structures could participate in PMMA polymerisation by acting as efficient radical scaveng‐ ers. Dubois et al [53] applied the in situ polymerization to olefin monomers by anchoring methylaluminoxane, a commonly used co-catalyst in metallocene-based olefin polymeriza‐ tion onto carbon nanotubes surface. Then, the metallocene catalyst was added to the surfaceactivated CNTs and the course of ethylene polymerization was found to be similar to the one without the presence of pristine MWCNTs. Epoxy nanocomposites comprise the majori‐ ty of reports using in situ polymerisation methods [54, 55], where the nanotubes are first dis‐ persed in the resin followed by curing the resin with the hardener. Zhu *et al* [56] prepared epoxy nanocomposites by this technique using end-cap carboxylated SWCNTs and an ester‐ ification reaction to produce a composite with improved tensile modulus (E is 30% higher

Rather than avoid the high viscosities of nanotube/polymer composites, some researchers have decreased the temperature to increase viscosity to the point of processing in the solid state. Sol‐ id-state mechanochemical pulverisation processes (using pan milling [57] or twin-screw pul‐ verisation [58]) have mixed MWCNTs with polymer matrices. Pulverisation methods can be used alone or followed by melt mixing. Nanocomposites prepared in this manner have the ad‐ vantage of possibly grafting the polymer on the nanotubes, which account in part for the ob‐

served good dispersion, improved interfacial adhesion, and improved tensile modulus.

**1.3. In Situ Polymerisation**

with 1 wt % SWCNT).

**1.4. Novel methods**

The noncovalent attachment, controlled by thermodynamic criteria [68], which for some pol‐ ymer chains is called wrapping, can alter the nature of the nanotube's surface and make it more compatible with the polymer matrix. Non-covalent surface modifications are based mainly on weak interactions, such as van der Waals, π−π and hydrophobic interactions, be‐ tween CNTs and modifier molecules. Non-covalent surface modifications are advantageous in that they conserve sp2 -conjugated structures and preserve the electronic performance of CNTs. The main potential disadvantage of noncovalent attachment is that the forces be‐ tween the wrapping molecule and the nanotube might be weak, thus as a filler in a compo‐ site the efficiency of the load transfer might be low.

and the surfaces of the nanotubes. Star et al [72] also synthesised the Stilbenoid dendrimers, a hyperbranched variant of the PmPV polymer, which exhibits an appropriate degree of branch‐ ing, and it was found to be more efficient at breaking up nanotube bundles, provided it is em‐

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In addition, the behavior of single walled and multi walled carbon nanotubes in aqueous solutions of Gum Arabic, a natural polysaccharide, has been described by Nativ-Roth et al [73]. They observed that while the as-prepared nanotube powders contain highly entangled ropes and bundles, the dispersions are mainly composed of individual tubes suggesting that the ability of Gum Arabic to exfoliate the bundles, and stabilize individual tubes in aqueous dispersions, can be utilized in the preparation of carbon nanotube-polymer composites. In the latter case, the dispersing polymer acts as a compatabilizer and as an adhesion promoter

It is clear from these accounts that noncovalent functionalisation of carbon nanotubes can be

Xia et al [74] has described a method to prepare polymer-encapsulated MWCNTs : it has been successfully prepared through ultrasonically initiated in situ emulsion polymerisations of n-butyl acrylate (BA) and methyl methacrylate (MMA) in presence of MWCNT. By em‐ ploying the multiple effects of ultrasound, i.e., dispersion, pulverizing, activation, and initia‐ tion, the aggregation and entanglement of carbon nanotubes in aqueous solution can be broken down, while in situ polymerization of monomer BA or MMA on the surface of

The hydrophilic regions of surfactants interact with polar solvent molecules, and the hydro‐ phobic regions can adsorb onto nanotube surfaces [75]. Thus, the process of dispersing CNTs from aggregates, bundles, or ropes into separated individual CNTs depends strongly on the length of the hydrophobic regions and the types of hydrophilic groups of the surfac‐ tant. A topological, noncovalent solution to improving the dispersion of SWNTs by encasing them in cross-linkable surfactant micelles was demonstrated by Kang and Taton [16]. SWCNTs were dispersed in the dimethylformamide (DMF) solutions of amphiphilic poly(styrene)-block-poly(acrylic acid) copolymer. Water was added to the solutions and the poly(styrene)-block-poly(acrylic acid) copolymer wrapped the SWCNTs and formed mi‐ celle. Then the PAA blocks of the micellar shells were permanently crosslinked by addition of a water-soluble diamine linker and a carbodiimide activator. This encapsulation signifi‐ cantly enhances the dispersion of SWCNTs in a wide variety of polar and nonpolar solvents and polymer matrices [76]. Encapsulated SWNTs can be used as an alternative starting ma‐ terial to pure SWNTs for the production and investigation of nanotube composite materials.

Functionalisation of carbon nanotubes with polymers is a key issue to improve the interfa‐ cial interaction between CNTs and the polymer matrix when processing polymer/CNT

achieved without disrupting the primary structure of the nanotubes themselves.

MWCNTs proceeds and the MWCNTs are coated by the formed polymer.

ployed at higher polymer-to-nanotube ratios than was the "parent" PmPV polymer.

leading to strengthening of the matrix-nanotube interface.

*2.1.2. Polymer absorption*

**2.2. Covalent attachment of polymers**

Non-covalent modification approaches typically use organic mediating molecules that range from low molecular weight molecules to supra- molecules to polymers.

**Figure 2.** Different routes for nanotubes' functionalisation: sidewall covalent functionalisation (a); defect-group cova‐ lent functionalisation (b); noncovalent polymer wrapping (c); noncovalent pi-stacking (d).

#### *2.1.1. Polymer wrapping*

O'Connell et al. [68] reported that nanotubes could be reversibly solubilised in water by nonco‐ valently associating them with a variety of linear polymers such as polyvinyl pyrrolidone (PVP) and polystyrene sulfonate (PSS). They demonstrated that the association between the polymer and the nanotubes is robust, not dependent upon the presence of excess polymer in solution, and is uniform along the sides of the tubes (Figure 1c). A general thermodynamic driving force for such wrapping in an aqueous environment has been identified [68].

Conjugated luminescent polymer poly-{(m-phenylenevinylene)-co-[(1,5-dioctyloxy-p-phe‐ nylene)-vinylene]} (PmPV) and its derivatives [69-71] have been successfully used for the wrapping around nanotubes on account of stabilising noncovalent bonding interactions, pre‐ sumably as a result of π–π stacking (Figure 1d) and van der Waals interactions between PmPV and the surfaces of the nanotubes. Star et al [72] also synthesised the Stilbenoid dendrimers, a hyperbranched variant of the PmPV polymer, which exhibits an appropriate degree of branch‐ ing, and it was found to be more efficient at breaking up nanotube bundles, provided it is em‐ ployed at higher polymer-to-nanotube ratios than was the "parent" PmPV polymer.

In addition, the behavior of single walled and multi walled carbon nanotubes in aqueous solutions of Gum Arabic, a natural polysaccharide, has been described by Nativ-Roth et al [73]. They observed that while the as-prepared nanotube powders contain highly entangled ropes and bundles, the dispersions are mainly composed of individual tubes suggesting that the ability of Gum Arabic to exfoliate the bundles, and stabilize individual tubes in aqueous dispersions, can be utilized in the preparation of carbon nanotube-polymer composites. In the latter case, the dispersing polymer acts as a compatabilizer and as an adhesion promoter leading to strengthening of the matrix-nanotube interface.

It is clear from these accounts that noncovalent functionalisation of carbon nanotubes can be achieved without disrupting the primary structure of the nanotubes themselves.

#### *2.1.2. Polymer absorption*

more compatible with the polymer matrix. Non-covalent surface modifications are based mainly on weak interactions, such as van der Waals, π−π and hydrophobic interactions, be‐ tween CNTs and modifier molecules. Non-covalent surface modifications are advantageous

CNTs. The main potential disadvantage of noncovalent attachment is that the forces be‐ tween the wrapping molecule and the nanotube might be weak, thus as a filler in a compo‐

Non-covalent modification approaches typically use organic mediating molecules that range

**Figure 2.** Different routes for nanotubes' functionalisation: sidewall covalent functionalisation (a); defect-group cova‐

O'Connell et al. [68] reported that nanotubes could be reversibly solubilised in water by nonco‐ valently associating them with a variety of linear polymers such as polyvinyl pyrrolidone (PVP) and polystyrene sulfonate (PSS). They demonstrated that the association between the polymer and the nanotubes is robust, not dependent upon the presence of excess polymer in solution, and is uniform along the sides of the tubes (Figure 1c). A general thermodynamic

Conjugated luminescent polymer poly-{(m-phenylenevinylene)-co-[(1,5-dioctyloxy-p-phe‐ nylene)-vinylene]} (PmPV) and its derivatives [69-71] have been successfully used for the wrapping around nanotubes on account of stabilising noncovalent bonding interactions, pre‐ sumably as a result of π–π stacking (Figure 1d) and van der Waals interactions between PmPV

driving force for such wrapping in an aqueous environment has been identified [68].

lent functionalisation (b); noncovalent polymer wrapping (c); noncovalent pi-stacking (d).

from low molecular weight molecules to supra- molecules to polymers.


in that they conserve sp2

*2.1.1. Polymer wrapping*

site the efficiency of the load transfer might be low.

82 Syntheses and Applications of Carbon Nanotubes and Their Composites

Xia et al [74] has described a method to prepare polymer-encapsulated MWCNTs : it has been successfully prepared through ultrasonically initiated in situ emulsion polymerisations of n-butyl acrylate (BA) and methyl methacrylate (MMA) in presence of MWCNT. By em‐ ploying the multiple effects of ultrasound, i.e., dispersion, pulverizing, activation, and initia‐ tion, the aggregation and entanglement of carbon nanotubes in aqueous solution can be broken down, while in situ polymerization of monomer BA or MMA on the surface of MWCNTs proceeds and the MWCNTs are coated by the formed polymer.

The hydrophilic regions of surfactants interact with polar solvent molecules, and the hydro‐ phobic regions can adsorb onto nanotube surfaces [75]. Thus, the process of dispersing CNTs from aggregates, bundles, or ropes into separated individual CNTs depends strongly on the length of the hydrophobic regions and the types of hydrophilic groups of the surfac‐ tant. A topological, noncovalent solution to improving the dispersion of SWNTs by encasing them in cross-linkable surfactant micelles was demonstrated by Kang and Taton [16]. SWCNTs were dispersed in the dimethylformamide (DMF) solutions of amphiphilic poly(styrene)-block-poly(acrylic acid) copolymer. Water was added to the solutions and the poly(styrene)-block-poly(acrylic acid) copolymer wrapped the SWCNTs and formed mi‐ celle. Then the PAA blocks of the micellar shells were permanently crosslinked by addition of a water-soluble diamine linker and a carbodiimide activator. This encapsulation signifi‐ cantly enhances the dispersion of SWCNTs in a wide variety of polar and nonpolar solvents and polymer matrices [76]. Encapsulated SWNTs can be used as an alternative starting ma‐ terial to pure SWNTs for the production and investigation of nanotube composite materials.

#### **2.2. Covalent attachment of polymers**

Functionalisation of carbon nanotubes with polymers is a key issue to improve the interfa‐ cial interaction between CNTs and the polymer matrix when processing polymer/CNT nanocomposites. The covalent reaction of CNT with polymers is important because the long polymer chains help to dissolve the tubes into a wide range of solvents even at a low degree of functionalisation. There are two main methodologies for the covalent attachment of poly‐ meric substances to the surface of nanotubes, which are defined as "grafting to" and 'graft‐ ing from' methods [76, 77]. The former relies on the synthesis of a polymer with a specific molecular weight followed by end group transformation. Subsequently, this polymer chain is attached to the graphitic surface of CNT. A disadvantage of this method is that the grafted polymer contents are limited because of high steric hindrance of macromolecules. The 'graft‐ ing from' method involved the immobilisation of initiators onto the substrate followed in situ surface polymerization to generate grafted polymer chains. Because the covalent attach‐ ment of the surface modifiers involves the partial disruption of the sidewall sp2 hybridiza‐ tion system, covalently modified CNTs inevitably lose some degree of their electrical and/or electronic performance properties [78].

COCl

(A)

publications.

*2.2.2. 'Grafting from' technique*

H2N

NMP, Pyridine, T=5-20°C

(A)

H N C O C

A or

Polymer Nanocomposites Containing Functionalised Multiwalled Carbon NanoTubes

C

A C

O

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O

O

C O H

n

HO OH HO OH

**Figure 3.** Synthesis of oligo-hydroxyamide-grafted MWNT. Reproduced from [80] with permission of Elsevier.

DCB, T=130°C

CH H2 <sup>R</sup> <sup>C</sup> N3 <sup>n</sup>

chemical oxidation and their conversion into acyl chlorides (Figure 5).

lizing nitroxide (Figure 6), resulting in grafting densities up to 12 wt.-%.

**Figure 4.** reaction of azide-terminatedpolystyreneonto CNTs surface. Reproduced from [80] with permission of ACS

In an analogous approach, alkyne-decorated SWCNTs and PS-N3were coupled via [3+1] Huisgen cycloaddition between the alkyne and azide end groups [85]. A new method was developed by Hung et al. [86] for preparing polystyrene-functionalized multiple-walled car‐ bon nanotubes (MWNTs) through the termination of anionically synthesized living poly‐ styryllithium with the acyl chloride functionalities on the MWNTs. The acyl chloride functionalities on the MWNTs were in turn obtained by the formation of carboxyls via

Lou et al. [87] reported the radical grafting of polyvinylpyridine chains onto the surface of nanotubes through the thermolysis of poly (2-vinylpyridine) terminated with a radical-stabi‐

Mostly, it involves the polymerisation of monomers from surface-derived initiators on either MWCNTs or SWCNTs. These initiators are covalently attached using the various functional‐ isation reactions developed for small molecules [77]. Then, the polymer is bound via in situ radical, cationic, anionic, ring opening and condensation polymerizations. The advantage of

N NH2

CH H2 R C N n

#### *2.2.1. 'Grafting to' method*

Since the curvature of the carbon nanostructures imparts a significant strain upon the sp2 hybridised carbon atoms that make up their framework, the energy barrier required to con‐ vert these atoms to sp3 hybridisation is lower than that of the flat graphene sheets, making them susceptible to various addition reactions. Therefore, to exploit this chemistry, it is only necessary to produce a polymer-centred transient in the presence of CNT material. Alterna‐ tively, defect sites on the surface of oxidized CNTs, as open-ended nanostructures with ter‐ minal carboxylic acid groups, allow covalent linkages of oligomer or polymer chains. So, the 'grafting to' method involves the chemical reaction between as-prepared or commercially available polymers with reactive end groups and nanotubes' surface functional groups or the termination of growing polymer radical, cation and anion formed during the polymeri‐ zation of various monomers in the presence of CNTs or the deactivation of living polymer chain ends with the CNT surface.

For example, oxidized SWCNTs were grafted with amino-terminated poly (N-isopropyla‐ crylamide) (PNIPAAm) by carbodiimide-activated reaction, which yielded a 8wt% polymer content[77]. In a different approach, oxidized MWCNTs were attached ontopolyacryloni‐ trile(PAN) nanoparticles through the reaction of the reduced cyano-groups of the polymer and the carboxylic moieties of CNT surface [79]. In addition, the amidation reaction was used for grafting of oligo-hydroxyamides to MWCNTs as described in figure 3 [80].

Ester-based linkages have been used by Baskaran et al. [81] by performing the reaction of hydroxy-terminated PS with thionyl chloridetreated MWCNTs, resulting in a hybrid con‐ taining 86wt% of CNTs. The esterification reaction was also used for grafting polyethylene glycol(PEG) chains to acylchloride-activated SWCNTs [82]. Silicone-functionalised CNT de‐ rivatives were prepared by opening terminal epoxy groups of functionalised polydimethyl‐ siloxanes (PDMS) by the carboxylic groups of acid-treated MWCNTs [83]. Another example of the "grafting to" approach has been reported by Qin et al. [84] through the grafting of polystyrene with azide end group onto SWCNTs (Figure 4).

**Figure 3.** Synthesis of oligo-hydroxyamide-grafted MWNT. Reproduced from [80] with permission of Elsevier.

**Figure 4.** reaction of azide-terminatedpolystyreneonto CNTs surface. Reproduced from [80] with permission of ACS publications.

In an analogous approach, alkyne-decorated SWCNTs and PS-N3were coupled via [3+1] Huisgen cycloaddition between the alkyne and azide end groups [85]. A new method was developed by Hung et al. [86] for preparing polystyrene-functionalized multiple-walled car‐ bon nanotubes (MWNTs) through the termination of anionically synthesized living poly‐ styryllithium with the acyl chloride functionalities on the MWNTs. The acyl chloride functionalities on the MWNTs were in turn obtained by the formation of carboxyls via chemical oxidation and their conversion into acyl chlorides (Figure 5).

Lou et al. [87] reported the radical grafting of polyvinylpyridine chains onto the surface of nanotubes through the thermolysis of poly (2-vinylpyridine) terminated with a radical-stabi‐ lizing nitroxide (Figure 6), resulting in grafting densities up to 12 wt.-%.

#### *2.2.2. 'Grafting from' technique*

nanocomposites. The covalent reaction of CNT with polymers is important because the long polymer chains help to dissolve the tubes into a wide range of solvents even at a low degree of functionalisation. There are two main methodologies for the covalent attachment of poly‐ meric substances to the surface of nanotubes, which are defined as "grafting to" and 'graft‐ ing from' methods [76, 77]. The former relies on the synthesis of a polymer with a specific molecular weight followed by end group transformation. Subsequently, this polymer chain is attached to the graphitic surface of CNT. A disadvantage of this method is that the grafted polymer contents are limited because of high steric hindrance of macromolecules. The 'graft‐ ing from' method involved the immobilisation of initiators onto the substrate followed in situ surface polymerization to generate grafted polymer chains. Because the covalent attach‐ ment of the surface modifiers involves the partial disruption of the sidewall sp2 hybridiza‐ tion system, covalently modified CNTs inevitably lose some degree of their electrical and/or

Since the curvature of the carbon nanostructures imparts a significant strain upon the sp2 hybridised carbon atoms that make up their framework, the energy barrier required to con‐

them susceptible to various addition reactions. Therefore, to exploit this chemistry, it is only necessary to produce a polymer-centred transient in the presence of CNT material. Alterna‐ tively, defect sites on the surface of oxidized CNTs, as open-ended nanostructures with ter‐ minal carboxylic acid groups, allow covalent linkages of oligomer or polymer chains. So, the 'grafting to' method involves the chemical reaction between as-prepared or commercially available polymers with reactive end groups and nanotubes' surface functional groups or the termination of growing polymer radical, cation and anion formed during the polymeri‐ zation of various monomers in the presence of CNTs or the deactivation of living polymer

For example, oxidized SWCNTs were grafted with amino-terminated poly (N-isopropyla‐ crylamide) (PNIPAAm) by carbodiimide-activated reaction, which yielded a 8wt% polymer content[77]. In a different approach, oxidized MWCNTs were attached ontopolyacryloni‐ trile(PAN) nanoparticles through the reaction of the reduced cyano-groups of the polymer and the carboxylic moieties of CNT surface [79]. In addition, the amidation reaction was

Ester-based linkages have been used by Baskaran et al. [81] by performing the reaction of hydroxy-terminated PS with thionyl chloridetreated MWCNTs, resulting in a hybrid con‐ taining 86wt% of CNTs. The esterification reaction was also used for grafting polyethylene glycol(PEG) chains to acylchloride-activated SWCNTs [82]. Silicone-functionalised CNT de‐ rivatives were prepared by opening terminal epoxy groups of functionalised polydimethyl‐ siloxanes (PDMS) by the carboxylic groups of acid-treated MWCNTs [83]. Another example of the "grafting to" approach has been reported by Qin et al. [84] through the grafting of

used for grafting of oligo-hydroxyamides to MWCNTs as described in figure 3 [80].

polystyrene with azide end group onto SWCNTs (Figure 4).

hybridisation is lower than that of the flat graphene sheets, making

electronic performance properties [78].

84 Syntheses and Applications of Carbon Nanotubes and Their Composites

*2.2.1. 'Grafting to' method*

vert these atoms to sp3

chain ends with the CNT surface.

Mostly, it involves the polymerisation of monomers from surface-derived initiators on either MWCNTs or SWCNTs. These initiators are covalently attached using the various functional‐ isation reactions developed for small molecules [77]. Then, the polymer is bound via in situ radical, cationic, anionic, ring opening and condensation polymerizations. The advantage of 'grafting from' approach is that the polymer growth is not limited by steric hindrance, al‐ lowing high molecular weight polymers to be efficiently grafted as well as quite high graft‐ ing density [9].

The latter procedure eliminates the need for nanotube pretreatment prior to functionaliza‐ tion and allows attachment of polymer molecules to pristine tubes without altering their

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In addition, polyethylenimine has been grafted onto the surface of MWNTs by performing a cationic polymerization of aziridine in the presence of amine-functionalized MWNTs (NH2– MWNTs [89]. The grafting of PEI was realized through two mechanisms, the activated mon‐ omer mechanism (AMM) or the activated chain mechanism (ACM), by which protonated aziridine monomers or the terminal iminium ion groups of propagation chains, respectively,

Bonduel et al. [90] reported the homogeneous surface coating of long carbon nanotubes by in situ polymerization of ethylene as catalyzed directly from the nanotube surface-treated by a highly active metallocene-based complex. It allowed for the break-up of the native nano‐ tube bundles leading, upon further melt blending with HDPE, to high-performance polyole‐ finic nanocomposites [90]. In another attempt, an easy method for preparing polystyrenegrafted multi-walled carbon nanotubes (MWCNTs) with high graft yields was developed by using free radical graft polymerisation from photoinduced surface initiating groups on MWCNTs [91]. Conventional microscopy, including optical, atomic force, sanning electronic microscopy (SEM), and transmission electronic microscopy (TEM), reveal the dispersion state or quality of CNTs within a very limited area of a given nanofiller composite [67]. High resolution-TEM image of the MWCNTs-PS (Figure 8) shows that the surface of the MWCNTs-PS is covered with 4–5nm thick amorphous PS layers while the wall surface of

purified MWCNTs was smooth, without any detectable polymer Layer [91].

**Figure 8.** HR-TEM image of PS-g-MWCNT. Reprinted from [91] with permission of Elsevier.

(see figure 9 as example).

Controlled radical polymerisation techniques such as nitroxide mediated polymerisation (NMP), atom transfer radical polymerisation (ATRP) and radical adition fragmentation transfer (RAFT) have been also used to graft polymer chains from the CNT surface [92-103]

are transferred to amines on the surface of MWNTs [89].

original structure.

**Figure 5.** substitution reaction of living polystyryllithium anions with acyl choride-modified CNTs. Reproduced from [86] with permission of John Wiley and Sons.

**Figure 6.** Radical grafting of TEMPO-end capped PVP to MWCNTs. Reproduced from [87] with permission of Elsevier.

**Figure 7.** Anionic polymerisation of styrene onto carbon nanotubes

For example, Viswanathan et al [88]. have developed a procedure based on the SWCNT sur‐ face treatment with butyllithium providing initiating sites for the anionic polymerization of styrene (Figure 6).

The latter procedure eliminates the need for nanotube pretreatment prior to functionaliza‐ tion and allows attachment of polymer molecules to pristine tubes without altering their original structure.

'grafting from' approach is that the polymer growth is not limited by steric hindrance, al‐ lowing high molecular weight polymers to be efficiently grafted as well as quite high graft‐

(PS) \* C

**Figure 5.** substitution reaction of living polystyryllithium anions with acyl choride-modified CNTs. Reproduced from

**Figure 6.** Radical grafting of TEMPO-end capped PVP to MWCNTs. Reproduced from [87] with permission of Elsevier.

For example, Viswanathan et al [88]. have developed a procedure based on the SWCNT sur‐ face treatment with butyllithium providing initiating sites for the anionic polymerization of

n n-m

O

OH

\*

PS

PS <sup>+</sup> (n + m) LiCl

C PS m

N2 ; T=45°C ; t=24h ; CH3OH

CH - Li<sup>+</sup>

CH H2 C H2 <sup>R</sup> <sup>C</sup> x

**Figure 7.** Anionic polymerisation of styrene onto carbon nanotubes

styrene (Figure 6).

ing density [9].

\* COCl

86 Syntheses and Applications of Carbon Nanotubes and Their Composites

(PS) :

[86] with permission of John Wiley and Sons.

In addition, polyethylenimine has been grafted onto the surface of MWNTs by performing a cationic polymerization of aziridine in the presence of amine-functionalized MWNTs (NH2– MWNTs [89]. The grafting of PEI was realized through two mechanisms, the activated mon‐ omer mechanism (AMM) or the activated chain mechanism (ACM), by which protonated aziridine monomers or the terminal iminium ion groups of propagation chains, respectively, are transferred to amines on the surface of MWNTs [89].

Bonduel et al. [90] reported the homogeneous surface coating of long carbon nanotubes by in situ polymerization of ethylene as catalyzed directly from the nanotube surface-treated by a highly active metallocene-based complex. It allowed for the break-up of the native nano‐ tube bundles leading, upon further melt blending with HDPE, to high-performance polyole‐ finic nanocomposites [90]. In another attempt, an easy method for preparing polystyrenegrafted multi-walled carbon nanotubes (MWCNTs) with high graft yields was developed by using free radical graft polymerisation from photoinduced surface initiating groups on MWCNTs [91]. Conventional microscopy, including optical, atomic force, sanning electronic microscopy (SEM), and transmission electronic microscopy (TEM), reveal the dispersion state or quality of CNTs within a very limited area of a given nanofiller composite [67]. High resolution-TEM image of the MWCNTs-PS (Figure 8) shows that the surface of the MWCNTs-PS is covered with 4–5nm thick amorphous PS layers while the wall surface of purified MWCNTs was smooth, without any detectable polymer Layer [91].

**Figure 8.** HR-TEM image of PS-g-MWCNT. Reprinted from [91] with permission of Elsevier.

Controlled radical polymerisation techniques such as nitroxide mediated polymerisation (NMP), atom transfer radical polymerisation (ATRP) and radical adition fragmentation transfer (RAFT) have been also used to graft polymer chains from the CNT surface [92-103] (see figure 9 as example).

#### **3. Carbon nanotubes nanocomposites based on Polyolefins**

NH-CH2 HO -COOH

COOCH3

**3.1. Radical grafting of polyethylene onto MWCNTs**

molar mass alkane representing characteristics moieties of PE.

CH3

C

C Br

O

N OH

Polymer Nanocomposites Containing Functionalised Multiwalled Carbon NanoTubes

O-C-C(CH3)2Br

O

N O-C-C(CH3)2-(CH2-C)n-Br

O C O

OCH3

CH3

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**(A)**

**(B)**

N

**Figure 9.** ATRP 'grafting from' modification approach. Reproduced from [92] with permission of ACS publications.

The main drawback of the free radical grafting is the low selectivity of the radical center,

specially at high temperatures (in the range of 150-200°C, required for extrusion of polyethy‐

lene), leading to side reactions such as coupling and chain scission [115, 118]. Moreover, per‐

forming this chemical modification by reactive processing brings in many constraints

inherent to the processing (e.g. short reaction time, viscous dissipation and high tempera‐

ture). For instance, the difference of viscosity between the monomer and the molten polymer

could enhance these side reactions. So, to separate these physical influences from the chemi‐

cal modification, the grafting reaction can be predicted with a model compound approach

based on a radical grafting reaction between peroxide-derived alkoxyl radicals, and a low

RCHO

Br

H3C H3C

**(A)**

**(B)**

Polyethylene (PE) is one of the most widely used commercial polymer due to the excellent combination of low coefficient of friction, chemical stability and excellent moisture barrier properties [104]. The combination of a soft polymer matrix such as PE with nanosized rigid filler particles may provide new nanocomposite materials with largely improved modulus and strength. To improve the stiffness and rigidity of PE, CNTs can be used to make CNT/PE composites [104-107]. The mechanical properties of polyethylene (PE) reinforced by carbon nanotubes do not improve significantly because the weak polymer-CNT interfacial adhesion prevents efficient stress transfer from the polymer matrix to CNT [108-110]. The lack of functional groups and polarity of PE backbone results in incompatibility between PE and other materials such as glass fibres, clays, metals, pigments, fillers, and most polymers. A strategy for enhancing the compatibility between nanotubes and polyolefins consists in functionalising the sidewalls of CNT with polymers either by a 'grafting to' or a 'grafting from' approach. As discussed before, the "grafting from" approach involves the growth of polymers from CNT surfaces via in situ polymerisation of olefins initiated from chemical species immobilised on the CNT. As an example, Ziegler-Natta or metallocene catalysts for ethylene polymerisation can be immobilised on nanotubes to grow PE chains from their sur‐ face. However, covalent linkages or strong interactions between PE chains and nanotubes cannot be created during polymerisation [90, 111-113]. The "grafting to" technique involves the use of addition reactions between the polymer with reactive groups and the CNT sur‐ face. However, the synthesis of end-functionalized polyethylene (PE), which is necessary in the "grafting to" approach, is difficult [114]. Another promising route for a chemical modifi‐ cation of MWCNTs by PE is to use free radical initiators such as peroxides. The general mechanism of free radical grafting of vinyl compound from hydrocarbon chains detailed by Russell [115], Chung [116] and Moad [117] seems to express a widespread view. The graft‐ ing reaction starts with hydrogen abstraction by alkoxyl radicals generated from thermal de‐ composition of the peroxide. Then, the active species generated onto the hydrocarbon backbone react with unsaturated bonds located on the MWCNTs surface. This chemical modification is thus conceivable during reactive extrusion because the radicals' lifetimes (in the range of few milliseconds) are compatible with typical residence time in an extruder (around one minute).

Polymer Nanocomposites Containing Functionalised Multiwalled Carbon NanoTubes http://dx.doi.org/10.5772/50710 89

**Figure 9.** ATRP 'grafting from' modification approach. Reproduced from [92] with permission of ACS publications.

#### **3.1. Radical grafting of polyethylene onto MWCNTs**

**3. Carbon nanotubes nanocomposites based on Polyolefins**

88 Syntheses and Applications of Carbon Nanotubes and Their Composites

(around one minute).

Polyethylene (PE) is one of the most widely used commercial polymer due to the excellent combination of low coefficient of friction, chemical stability and excellent moisture barrier properties [104]. The combination of a soft polymer matrix such as PE with nanosized rigid filler particles may provide new nanocomposite materials with largely improved modulus and strength. To improve the stiffness and rigidity of PE, CNTs can be used to make CNT/PE composites [104-107]. The mechanical properties of polyethylene (PE) reinforced by carbon nanotubes do not improve significantly because the weak polymer-CNT interfacial adhesion prevents efficient stress transfer from the polymer matrix to CNT [108-110]. The lack of functional groups and polarity of PE backbone results in incompatibility between PE and other materials such as glass fibres, clays, metals, pigments, fillers, and most polymers. A strategy for enhancing the compatibility between nanotubes and polyolefins consists in functionalising the sidewalls of CNT with polymers either by a 'grafting to' or a 'grafting from' approach. As discussed before, the "grafting from" approach involves the growth of polymers from CNT surfaces via in situ polymerisation of olefins initiated from chemical species immobilised on the CNT. As an example, Ziegler-Natta or metallocene catalysts for ethylene polymerisation can be immobilised on nanotubes to grow PE chains from their sur‐ face. However, covalent linkages or strong interactions between PE chains and nanotubes cannot be created during polymerisation [90, 111-113]. The "grafting to" technique involves the use of addition reactions between the polymer with reactive groups and the CNT sur‐ face. However, the synthesis of end-functionalized polyethylene (PE), which is necessary in the "grafting to" approach, is difficult [114]. Another promising route for a chemical modifi‐ cation of MWCNTs by PE is to use free radical initiators such as peroxides. The general mechanism of free radical grafting of vinyl compound from hydrocarbon chains detailed by Russell [115], Chung [116] and Moad [117] seems to express a widespread view. The graft‐ ing reaction starts with hydrogen abstraction by alkoxyl radicals generated from thermal de‐ composition of the peroxide. Then, the active species generated onto the hydrocarbon backbone react with unsaturated bonds located on the MWCNTs surface. This chemical modification is thus conceivable during reactive extrusion because the radicals' lifetimes (in the range of few milliseconds) are compatible with typical residence time in an extruder

The main drawback of the free radical grafting is the low selectivity of the radical center, specially at high temperatures (in the range of 150-200°C, required for extrusion of polyethy‐ lene), leading to side reactions such as coupling and chain scission [115, 118]. Moreover, per‐ forming this chemical modification by reactive processing brings in many constraints inherent to the processing (e.g. short reaction time, viscous dissipation and high tempera‐ ture). For instance, the difference of viscosity between the monomer and the molten polymer could enhance these side reactions. So, to separate these physical influences from the chemi‐ cal modification, the grafting reaction can be predicted with a model compound approach based on a radical grafting reaction between peroxide-derived alkoxyl radicals, and a low molar mass alkane representing characteristics moieties of PE.

**Figure 11.** Raman spectra of: p-MWCNTs (a) and penta-g-MWCNTs (b).

was designated as an indicator of grafting species [119].

However, the alkoxy radicals can undergo additional reactions including β-scission leading to the formation of methyl radicals [117]. These latter preferentially induce coupling reaction (Fig. 10, route b and h) or attack onto the sp2 carbon of the MWCNTs (Fig. 10, route g) whereas cumyloxyl radicals are more prone to hydrogen abstraction from pentadecane [120]. The formed pentadecyl radicals through hydrogen abstraction are able to react with MWCNTs by radical addition onto sp2 carbon of theMWCNTs (Fig.10, main route a) and with other radical species via the common radical coupling reactions (Fig. 10, routes d1 and b). According to the results of Johnston [121,122], based on a study of the crosslinking reac‐ tion of poly (ethylene-co-1-octene) in the presence of DCP at 160 °C, coupling reactions are four times more prone to happen than scission reactions so the authors assumed that penta‐ decyl radicals do not undergo scission reactions [119]. Direct evidence for covalent sidewall functionalization has been found by Raman spectroscopy [123-124]. G band is a characteris‐ tic feature of the graphitic layers and corresponds to the tangential vibration of the carbon atoms. The second characteristic mode is a typical sign for defective graphitic structures (D band). The AD/AG ratio, which was defined as the intensity ratio of the D-band to G-band of CNTs, directly indicates the structural changes in nanotubes. Some authors used D to G area ratios (AD/AG) rather than intensity [125] which is a better indicator. The relatively high area ratio of the G band relative to D band for penta-g-MWCNT (AD/AG = 1.51) in comparison with that of p-MWCNT (i.e. (AD/AG =1.20) could be designated as an indicator of grafting species. The ratio between the G band and D band is a good indicator of the changes in chemistry of CNTs. Interestingly, Raman spectra of p-MWCNTs and penta-g-MWCNTs (Figure11a and 11b, respectively) showed two main peaks around 1350cm−1 (D band) and 1586cm−1 (G band). The relatively high intensity of the G band relative to D band (*I* G/*I* D=1.25) for penta-g-MWCNT sample in comparison with that of p-MWCNT (i.e. *I* G/*I* D=0.95)

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**Figure 10.** General reactive pathways of free radical grafting of pentadecane onto MWCNTs ; Reproduced from [119] with permission of Elsevier.

#### *3.1.1. A model compound approach through the use of pentadecane*

Covalent functionalization of pentadecane-decorated multiwalled carbon nanotubes (MWCNTs) has been studied as a model compound approach for the grafting of poly (ethyl‐ ene-co-1-octene) onto MWCNTs by reactive extrusion [119]. It was accomplished through radical addition onto unsaturated bonds located on the MWCNTs' surface using dicumyl peroxide as hydrogen abstractor. Pentadecane (C15H32) has been resorted as model for poly‐ ethylene because high boiling points of long chain alkanes permit study under high temper‐ ature conditions, typically over 150°C. It also gives clues about low viscosity at 150°C, on top of that the formed products in the grafting experiment can hence be analysed more easi‐ ly than in the polymer melt. Figure 10 sums up main reactive pathways of free radical graft‐ ing of pentadecane onto MWCNTs with dicumyl peroxide as initiator. The hydrogen abstraction reactions from alkyl hydrocarbon bonds was studied starting from the reaction of DCP-derived radicals with pentadecane.

**Figure 11.** Raman spectra of: p-MWCNTs (a) and penta-g-MWCNTs (b).

**Figure 10.** General reactive pathways of free radical grafting of pentadecane onto MWCNTs ; Reproduced from [119]

Covalent functionalization of pentadecane-decorated multiwalled carbon nanotubes (MWCNTs) has been studied as a model compound approach for the grafting of poly (ethyl‐ ene-co-1-octene) onto MWCNTs by reactive extrusion [119]. It was accomplished through radical addition onto unsaturated bonds located on the MWCNTs' surface using dicumyl peroxide as hydrogen abstractor. Pentadecane (C15H32) has been resorted as model for poly‐ ethylene because high boiling points of long chain alkanes permit study under high temper‐ ature conditions, typically over 150°C. It also gives clues about low viscosity at 150°C, on top of that the formed products in the grafting experiment can hence be analysed more easi‐ ly than in the polymer melt. Figure 10 sums up main reactive pathways of free radical graft‐ ing of pentadecane onto MWCNTs with dicumyl peroxide as initiator. The hydrogen abstraction reactions from alkyl hydrocarbon bonds was studied starting from the reaction

*3.1.1. A model compound approach through the use of pentadecane*

90 Syntheses and Applications of Carbon Nanotubes and Their Composites

of DCP-derived radicals with pentadecane.

with permission of Elsevier.

However, the alkoxy radicals can undergo additional reactions including β-scission leading to the formation of methyl radicals [117]. These latter preferentially induce coupling reaction (Fig. 10, route b and h) or attack onto the sp2 carbon of the MWCNTs (Fig. 10, route g) whereas cumyloxyl radicals are more prone to hydrogen abstraction from pentadecane [120]. The formed pentadecyl radicals through hydrogen abstraction are able to react with MWCNTs by radical addition onto sp2 carbon of theMWCNTs (Fig.10, main route a) and with other radical species via the common radical coupling reactions (Fig. 10, routes d1 and b). According to the results of Johnston [121,122], based on a study of the crosslinking reac‐ tion of poly (ethylene-co-1-octene) in the presence of DCP at 160 °C, coupling reactions are four times more prone to happen than scission reactions so the authors assumed that penta‐ decyl radicals do not undergo scission reactions [119]. Direct evidence for covalent sidewall functionalization has been found by Raman spectroscopy [123-124]. G band is a characteris‐ tic feature of the graphitic layers and corresponds to the tangential vibration of the carbon atoms. The second characteristic mode is a typical sign for defective graphitic structures (D band). The AD/AG ratio, which was defined as the intensity ratio of the D-band to G-band of CNTs, directly indicates the structural changes in nanotubes. Some authors used D to G area ratios (AD/AG) rather than intensity [125] which is a better indicator. The relatively high area ratio of the G band relative to D band for penta-g-MWCNT (AD/AG = 1.51) in comparison with that of p-MWCNT (i.e. (AD/AG =1.20) could be designated as an indicator of grafting species. The ratio between the G band and D band is a good indicator of the changes in chemistry of CNTs. Interestingly, Raman spectra of p-MWCNTs and penta-g-MWCNTs (Figure11a and 11b, respectively) showed two main peaks around 1350cm−1 (D band) and 1586cm−1 (G band). The relatively high intensity of the G band relative to D band (*I* G/*I* D=1.25) for penta-g-MWCNT sample in comparison with that of p-MWCNT (i.e. *I* G/*I* D=0.95) was designated as an indicator of grafting species [119].

It is important to determine whether the results of a CNT surface modification process agree qualitatively with expectations, and equally important is the need for a quantitative assess‐ ment of the extent and nature of surface modifications. The course of the generated radical species and the extent of the grafting reaction in regards to the DCP concentration and tem‐ perature can be studied through gas chromatography and thermogravimetric analysis (TGA) [119, 126]. TGA permits measurement of the total weight fraction of surface modifiers introduced onto the surfaces of CNTs if the surface-modified CNTs are free of impurities. Indeed, it is well known that heating functionalized nanotubes in an inert atmosphere re‐ moves the organic moieties and restores the pristine nanotubes structure. TGA can indicate the degree of surface modification because the type and quantity of surface modifier is iden‐ tified. It was found that the higher grafting density, as high as 1.46 mmol/g, was obtained at 150°C. At higher temperatures, the grafting density decreases because the β-scission reaction of cumyloxyl radical accelerates as the temperature increases, leading to the formation of methyl radicals. These latter preferentially react by combination whereas cumyloxyl radicals are more prone to hydrogen abstraction from pentadecane. At 150°C, for initiator concentra‐ tion higher than 3wt%, the grafting density decreases from 1.464mmol/g to 0.371mmol/g upon increasing DCP concentration up to 5%. Thus, to get high grafting efficiency, one should opt for optimal initiator concentration, i.e. 3wt%, and choose the most favourable re‐ action temperature, i.e. 150°C. Incorporation of TEMPO as radical scavenger in the grafting reaction of pentadecane onto MWCNTs serves two purposes: firstly, it actively suppresses radical combination reactions and hence promotes pentadecyl radicals' addition to nano‐ tubes (~16% increase in grafting density); and secondly, it effectively changes the polarity balance of the grafted species, making pentadecane and TEMPO functionalised nanotubes soluble in solvents such as THF and chloroform [126].

**Figure 12.** Reaction scheme for PE grafting onto MWCNTs with TEMPO as a radical scavenger. Reproduced from [128]

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**Figure 13.** TEM images of p-MWCNTs (1) and PE-g-MWCNTs (2). Reproduced from [128] with permission of John Wi‐

The formed PE-based radicals are able to react with MWCNTs by radical addition onto sp2 carbon of the MWCNTs (Figure 12) and with other radical species via the common radical coupling reactions. As discussed using a model compound approach (section 2.1.1), the presence of TEMPO radicals creates competitive combinations reactions (that are actually re‐ versible reactions) which may favour the addition of PE-based radicals to MWCNTs (Figure 12). Before carrying out thermogravimetric analysis to gain a quantitative picture of the ex‐ tent of nanotubes' functionalisation, the adsorbed (non-covalently attached) PE chains were removed from the grafted ones (covalently attached) by extensive washings with dichloro‐ benzene (DCB). PE-grafted onto MWCNTs are well known to degrade at 300-540°C, which are nearly the same temperatures as pure PE reactants and the weight of grafted PE is esti‐ mated to be in the range 20-24% depending on the experimental procedure [128]. The corre‐ sponding grafting densities, calculated using a specific surface area (SSA) of 225m2

MWCNTs [115, 129] are varying from 1.1mg.m-2 to 1.4mg.m-2. LDPE grafting density on

/g for

with permission of John Wiley and Sons.

ley and Sons.

#### *3.1.2. Synthesis of PE grafted carbon nanotubes via peroxide*

To make full use of the strength of carbon nanotubes in a composite, it is important to have a high-stress transfer at the matrix-nanotube interface via strong chemical bonding, as dis‐ cussed by Mylvaganam et al [127]. They have investigated the possible polyethylene-nano‐ tube bonding with the aid of a quantum mechanics analysis with the polyethylene chains represented by alkyl segments, and the nanotubes modeled by nanotube segments with H atoms added to the dangling bonds of the perimeter carbons. Their study has predicted (i) covalent bond formation between alkyl radicals and carbon nanotubes is energetically fa‐ vourable; and, (ii) this reaction may take place at multiple sites of nanotubes [126]. Hence one way to improve the load transfer of carbon nanotubes/PE composite via chemical bonds at the interface is to use free-radical generators such as peroxide or incorporate nanotubes by means of in situ polymerisation.

Figure 12 sums up main reactive pathways of free radical grafting of PE onto MWCNTs with dicumyl peroxide as initiator and TEMPO as radical scavenger.

Polymer Nanocomposites Containing Functionalised Multiwalled Carbon NanoTubes http://dx.doi.org/10.5772/50710 93

It is important to determine whether the results of a CNT surface modification process agree qualitatively with expectations, and equally important is the need for a quantitative assess‐ ment of the extent and nature of surface modifications. The course of the generated radical species and the extent of the grafting reaction in regards to the DCP concentration and tem‐ perature can be studied through gas chromatography and thermogravimetric analysis (TGA) [119, 126]. TGA permits measurement of the total weight fraction of surface modifiers introduced onto the surfaces of CNTs if the surface-modified CNTs are free of impurities. Indeed, it is well known that heating functionalized nanotubes in an inert atmosphere re‐ moves the organic moieties and restores the pristine nanotubes structure. TGA can indicate the degree of surface modification because the type and quantity of surface modifier is iden‐ tified. It was found that the higher grafting density, as high as 1.46 mmol/g, was obtained at 150°C. At higher temperatures, the grafting density decreases because the β-scission reaction of cumyloxyl radical accelerates as the temperature increases, leading to the formation of methyl radicals. These latter preferentially react by combination whereas cumyloxyl radicals are more prone to hydrogen abstraction from pentadecane. At 150°C, for initiator concentra‐ tion higher than 3wt%, the grafting density decreases from 1.464mmol/g to 0.371mmol/g upon increasing DCP concentration up to 5%. Thus, to get high grafting efficiency, one should opt for optimal initiator concentration, i.e. 3wt%, and choose the most favourable re‐ action temperature, i.e. 150°C. Incorporation of TEMPO as radical scavenger in the grafting reaction of pentadecane onto MWCNTs serves two purposes: firstly, it actively suppresses radical combination reactions and hence promotes pentadecyl radicals' addition to nano‐ tubes (~16% increase in grafting density); and secondly, it effectively changes the polarity balance of the grafted species, making pentadecane and TEMPO functionalised nanotubes

To make full use of the strength of carbon nanotubes in a composite, it is important to have a high-stress transfer at the matrix-nanotube interface via strong chemical bonding, as dis‐ cussed by Mylvaganam et al [127]. They have investigated the possible polyethylene-nano‐ tube bonding with the aid of a quantum mechanics analysis with the polyethylene chains represented by alkyl segments, and the nanotubes modeled by nanotube segments with H atoms added to the dangling bonds of the perimeter carbons. Their study has predicted (i) covalent bond formation between alkyl radicals and carbon nanotubes is energetically fa‐ vourable; and, (ii) this reaction may take place at multiple sites of nanotubes [126]. Hence one way to improve the load transfer of carbon nanotubes/PE composite via chemical bonds at the interface is to use free-radical generators such as peroxide or incorporate nanotubes

Figure 12 sums up main reactive pathways of free radical grafting of PE onto MWCNTs

with dicumyl peroxide as initiator and TEMPO as radical scavenger.

soluble in solvents such as THF and chloroform [126].

92 Syntheses and Applications of Carbon Nanotubes and Their Composites

*3.1.2. Synthesis of PE grafted carbon nanotubes via peroxide*

by means of in situ polymerisation.

**Figure 12.** Reaction scheme for PE grafting onto MWCNTs with TEMPO as a radical scavenger. Reproduced from [128] with permission of John Wiley and Sons.

**Figure 13.** TEM images of p-MWCNTs (1) and PE-g-MWCNTs (2). Reproduced from [128] with permission of John Wi‐ ley and Sons.

The formed PE-based radicals are able to react with MWCNTs by radical addition onto sp2 carbon of the MWCNTs (Figure 12) and with other radical species via the common radical coupling reactions. As discussed using a model compound approach (section 2.1.1), the presence of TEMPO radicals creates competitive combinations reactions (that are actually re‐ versible reactions) which may favour the addition of PE-based radicals to MWCNTs (Figure 12). Before carrying out thermogravimetric analysis to gain a quantitative picture of the ex‐ tent of nanotubes' functionalisation, the adsorbed (non-covalently attached) PE chains were removed from the grafted ones (covalently attached) by extensive washings with dichloro‐ benzene (DCB). PE-grafted onto MWCNTs are well known to degrade at 300-540°C, which are nearly the same temperatures as pure PE reactants and the weight of grafted PE is esti‐ mated to be in the range 20-24% depending on the experimental procedure [128]. The corre‐ sponding grafting densities, calculated using a specific surface area (SSA) of 225m2 /g for MWCNTs [115, 129] are varying from 1.1mg.m-2 to 1.4mg.m-2. LDPE grafting density on nanotubes is 1.1mg.m-2 while incorporation of TEMPO raises the grafting density to 1.4mg.m-2 [128]. Then, it is usual to examine the morphological structures of p-MWCNTs and PE-grafted MWCNTs by transmission electron microscopy (TEM). In these experiments, a few drops of dilute solutions of PE-grafted nanotubes in hot DCB are initially deposited onto a carbon-coated copper grid and further observed in a dried state after evaporation of the solvent (Figure 13).

(e.g. 1.78 and 2.80µmol.m-2, respectively). These values are approximately increased by two

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95

orders of magnitude in comparison with the LDPE grafting density (e.g. 0.012µmol.m-2) sug‐

gesting that longer polymer chains cover a larger surface decreasing the grafting density, as

previously described by Jerome et al [87,136] for the attachment of poly(2-vinylpyridine)

(P2VP) and polystyrene (PS) onto MWCNTs. Indeed, they observed that PS grafting density

decreases from 0.045µmol.m-2 to 0.01µmol.m-2 by increasing the molecular weight of PS-

TEMPO from 3000g/mol to 30000g/mol [138]. The TEM observations (Figure 15) were consis‐

tent with the TGA results : the grafted polymer contents can be highered by using end-

**Figure 14.** Reaction scheme for end functionalised PE grafting onto MWCNTs: (a) via PE-TEMPO; (b) via PE-SH. Repro‐

duced from [128] with permission of John Wiley and Sons.

functionalized PE [129].

A "grafting to" approach based on a radical process can also involve a polymer with reac‐ tive end groups.

#### *3.1.3. Synthesis of PE grafted carbon nanotubes via end functionalised PE*

Recently, D'Agosto and Boisson [130-134] developed new strategies that rely on a one step *in situ* functionalisation reaction within an ethylene polymerisation reactor to introduce a variety of functional groups including alkoxyamine [130-132] and thiol [132,134] functions at the end of polyethylene chains. Di-polyethylenyl magnesium compound (MgPE2) were pre‐ pared using a neodymium metallocene complex which catalysed polyethylene chain growth on magnesium compounds. MgPE2 was in situ reacted with 2,2,6,6-tetramethylpiperidin‐ yl-1-oxy (TEMPO) radical or elemental sulphur to provide a macroalcoxyamine (PE-TEM‐ PO) and polysulphur based product (PE-Sn-PE) respectively. PE-SH was obtained by simple reduction of PE-Sn-PE. According to these results, a strategy based on the use of those poly‐ ethylenes was investigated to generate radical-terminated chains formed either by thermal loss of a nitroxide (PE-TEMPO) or H-abstraction onto a thiol (PE-SH) and graft them onto CNTs (Figure 14) [128].

Indeed, Lou [87] showed an efficient attachment of poly(2-vinylpyridine) (P2VP) end-cap‐ ped by TEMPO to CNT sidewalls by heating of TEMPO-terminated P2VP. Using the same strategy Liu [137] functionalized shortened CNTs with PS and poly[(*tert*-butyl acrylate)-*b*styrene] and Wang [138] grafted poly(4-vinylpyridine-*b*-styrene) onto CNTs. In figure 14a, the homolytic cleavage of TEMPO-terminated PE leads to the formation of stable nitroxyl radicals and PE radicals. The reversible termination of the polyethylene chain is the key step for reducing the overall concentration of the radical chain end. The extremely low concen‐ tration of reactive chain ends is expected to minimize irreversible termination reactions, such as combination or disproportionation [135] (Figure 14a). Thiol-terminated polyethylene has been also grafted onto CNTs using a similar procedure. The thiol based compounds are widely used for controlling molar mass in free radical polymerizations via a chain transfer process. The chain transfer process displays two contiguous steps: transfer of the thiyl hy‐ drogen to the growing polymer chain followed by re-initiation, whereby a thiyl radical adds to a monomeric double bond. In the presence of DCP-derived radicals and MWCNTs, thiyl radicals are formed and are expected to react by radical addition onto sp2 carbon of the MWCNTs. For both samples PE-TEMPO and PE-SH, the weight loss observed by thermog‐ ravimetric analysis (TGA) has been increased to 36% and 34%, respectively despite their low molar masses (e.g. 1400g/mol and 980g/mol) in comparison with that of LDPE (weight loss = 20-24% ; Mw = 90000g/mol ; see section 2.1.2.). These results indicated that the use of short end-functionalized PE chains has permitted a significant increase of the grafting density (e.g. 1.78 and 2.80µmol.m-2, respectively). These values are approximately increased by two orders of magnitude in comparison with the LDPE grafting density (e.g. 0.012µmol.m-2) sug‐ gesting that longer polymer chains cover a larger surface decreasing the grafting density, as previously described by Jerome et al [87,136] for the attachment of poly(2-vinylpyridine) (P2VP) and polystyrene (PS) onto MWCNTs. Indeed, they observed that PS grafting density decreases from 0.045µmol.m-2 to 0.01µmol.m-2 by increasing the molecular weight of PS-TEMPO from 3000g/mol to 30000g/mol [138]. The TEM observations (Figure 15) were consis‐ tent with the TGA results : the grafted polymer contents can be highered by using endfunctionalized PE [129].

nanotubes is 1.1mg.m-2 while incorporation of TEMPO raises the grafting density to 1.4mg.m-2 [128]. Then, it is usual to examine the morphological structures of p-MWCNTs and PE-grafted MWCNTs by transmission electron microscopy (TEM). In these experiments, a few drops of dilute solutions of PE-grafted nanotubes in hot DCB are initially deposited onto a carbon-coated copper grid and further observed in a dried state after evaporation of

A "grafting to" approach based on a radical process can also involve a polymer with reac‐

Recently, D'Agosto and Boisson [130-134] developed new strategies that rely on a one step *in situ* functionalisation reaction within an ethylene polymerisation reactor to introduce a variety of functional groups including alkoxyamine [130-132] and thiol [132,134] functions at the end of polyethylene chains. Di-polyethylenyl magnesium compound (MgPE2) were pre‐ pared using a neodymium metallocene complex which catalysed polyethylene chain growth on magnesium compounds. MgPE2 was in situ reacted with 2,2,6,6-tetramethylpiperidin‐ yl-1-oxy (TEMPO) radical or elemental sulphur to provide a macroalcoxyamine (PE-TEM‐ PO) and polysulphur based product (PE-Sn-PE) respectively. PE-SH was obtained by simple reduction of PE-Sn-PE. According to these results, a strategy based on the use of those poly‐ ethylenes was investigated to generate radical-terminated chains formed either by thermal loss of a nitroxide (PE-TEMPO) or H-abstraction onto a thiol (PE-SH) and graft them onto

Indeed, Lou [87] showed an efficient attachment of poly(2-vinylpyridine) (P2VP) end-cap‐ ped by TEMPO to CNT sidewalls by heating of TEMPO-terminated P2VP. Using the same strategy Liu [137] functionalized shortened CNTs with PS and poly[(*tert*-butyl acrylate)-*b*styrene] and Wang [138] grafted poly(4-vinylpyridine-*b*-styrene) onto CNTs. In figure 14a, the homolytic cleavage of TEMPO-terminated PE leads to the formation of stable nitroxyl radicals and PE radicals. The reversible termination of the polyethylene chain is the key step for reducing the overall concentration of the radical chain end. The extremely low concen‐ tration of reactive chain ends is expected to minimize irreversible termination reactions, such as combination or disproportionation [135] (Figure 14a). Thiol-terminated polyethylene has been also grafted onto CNTs using a similar procedure. The thiol based compounds are widely used for controlling molar mass in free radical polymerizations via a chain transfer process. The chain transfer process displays two contiguous steps: transfer of the thiyl hy‐ drogen to the growing polymer chain followed by re-initiation, whereby a thiyl radical adds to a monomeric double bond. In the presence of DCP-derived radicals and MWCNTs, thiyl

radicals are formed and are expected to react by radical addition onto sp2

MWCNTs. For both samples PE-TEMPO and PE-SH, the weight loss observed by thermog‐ ravimetric analysis (TGA) has been increased to 36% and 34%, respectively despite their low molar masses (e.g. 1400g/mol and 980g/mol) in comparison with that of LDPE (weight loss = 20-24% ; Mw = 90000g/mol ; see section 2.1.2.). These results indicated that the use of short end-functionalized PE chains has permitted a significant increase of the grafting density

carbon of the

*3.1.3. Synthesis of PE grafted carbon nanotubes via end functionalised PE*

94 Syntheses and Applications of Carbon Nanotubes and Their Composites

the solvent (Figure 13).

CNTs (Figure 14) [128].

tive end groups.

**Figure 14.** Reaction scheme for end functionalised PE grafting onto MWCNTs: (a) via PE-TEMPO; (b) via PE-SH. Repro‐ duced from [128] with permission of John Wiley and Sons.

**Figure 15.** TEM images of PEf-TEMPO-g-MWCNTs (1) and PEf-SH-g-MWCNTs (2). Reproduced from [128] with permission of John Wiley and Sons.

**Figure 16.** Reaction scheme for the addition of TMP onto CNT in the presence of DCP. Reproduced from [129] with

Polymer Nanocomposites Containing Functionalised Multiwalled Carbon NanoTubes

As shown in Figure 16, the formed peroxide radicals are prone to hydrogen abstraction from hydrocarbon substrates and it is expected that the active species generated onto the hydro‐ carbon backbone react with unsaturated bonds located on the MWCNTs surface keeping in mind that side reactions such as chain scission for PP derivatives may occur at high temper‐ atures (Figure16) [115, 118]. For experiments conducted in dichlorobenzene (DCB) as solvent

Farzi et al. [129] have successfully grafted PP onto MWCNTs through a radical grafting reac‐ tion, carried out under similar experimental conditions to PE [128] and TMP [129] (1.5wt% DCP, 160°C) and using 1,2-dichlorobenzene (DCB) as solvent able to solubilize PP partially at elevated temperature. The corresponding PP-grafted nanotubes were analysed by TGA after a purification by soxhlet extraction in DCB. However, the authors were not able to ob‐ tain reproductible results with weight losses varying from 50% to 80% for the above-men‐ tioned experiment. This behaviour was attributed to the purification procedure which did not permit to remove all the free PP chains. The authors have also speculated on the degra‐ dation behaviour of PP through the well-known β-scission reaction occurring in the pres‐ ence of radical species therefore the authors were not able to give a PP grafting density. Then, the aforementioned PP coated MWCNTs have been dispersed within a commercially available PP matrix using a contra-rotating Haake Rheomixer and the amount of nanofiller in the final composites has been fixed to 3wt%. The evaluation of MWCNTs dispersion has

SEM images of the PP/PP-*g*-MWCNTs composites MWCNTs containing of 3wt% (Figure 17) demonstrated that there were still some areas where PP-*g*-MWCNTs were not found which was obviously connected with improper filler distribution. For a simple melt blend of PP with untreated MWCNTs, SEM images of the resulting material only showed clusters of a few tens micrometers of diameter evidencing a poor interfacial adhesion in the material

.

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97

at 160°C with 1.5wt% DCP, TMP grafting density was as high as 0.92 mg/m2

been examined by using scanning electron microscopy (SEM) (Figure 17).

*3.2.2. Synthesis of PP grafted carbon nanotubes via peroxide*

permission of Elsevier.

#### **3.2. Radical grafting of polypropylene on carbon nanotubes**

Polypropylene (PP) is a widely used commercial polymer due to the excellent combination of mechanical resistance, chemical stability and excellent moisture barrier properties [104]. Although physical blending with CNTs is an economic way to modify polypropylene per‐ formance, compatibilizing agents are necessary for creating strong interface between filler particles and the polymer phase. Maleic anhydride grafted polypropylene (MA-*g*-PP) is of‐ ten used as a compatibilizer which can improve the PP/CNTs composite properties by strong hydrogen bonding between hydroxyl groups located on the acidic-treated CNTs sur‐ face and anhydride groups of MA-g-PP [139, 140]. Recently, an original and simple method for promoting mobility sensitivity of carbon nanotubes (CNTs) to an external stress field in polypropylene (PP) matrix was developed [141]. In particular, an interfacial melt reaction in‐ itiated by free radicals were used as a tool to prepare PP/CNTs nanocomposites. The pres‐ ence of tetrakis(phenylmethyl)thioperoxydi(carbothioamide) (TBzTD) increased the interfacial reaction between the PP chains and the CNTs. In addition, the grafted TBzTD to PP backbone could form a physical interaction with CNTs *via* a π–π interaction [141]. Ac‐ cording to their previous results [119, 126] based on a study of the radical grafting of poly‐ ethylene derivatives onto MWCNTs, Farzi et al. investigated MWCNTs' sidewall functionalization by tetramethylpentadecane and PP in the presence of 1wt% DCP at 160°C.

#### *3.2.2. A model compound approach through the use of 2,6,10,14-tetramethylpentadecane*

Simlilarly to the pentadecane grafting procedure (see section 2.1.1.), 2,6,10,14-tetramethyl‐ pentadecane (TMP, C19H40) has been used as model for the grafting reaction of PP onto MWCNTs [129]. Thermolysis of dicumyl peroxide initiator performed in TMP and in pres‐ ence of MWCNTs is depicted in Figure 16.

**Figure 16.** Reaction scheme for the addition of TMP onto CNT in the presence of DCP. Reproduced from [129] with permission of Elsevier.

As shown in Figure 16, the formed peroxide radicals are prone to hydrogen abstraction from hydrocarbon substrates and it is expected that the active species generated onto the hydro‐ carbon backbone react with unsaturated bonds located on the MWCNTs surface keeping in mind that side reactions such as chain scission for PP derivatives may occur at high temper‐ atures (Figure16) [115, 118]. For experiments conducted in dichlorobenzene (DCB) as solvent at 160°C with 1.5wt% DCP, TMP grafting density was as high as 0.92 mg/m2 .

#### *3.2.2. Synthesis of PP grafted carbon nanotubes via peroxide*

**Figure 15.** TEM images of PEf-TEMPO-g-MWCNTs (1) and PEf-SH-g-MWCNTs (2). Reproduced from [128] with permission

Polypropylene (PP) is a widely used commercial polymer due to the excellent combination of mechanical resistance, chemical stability and excellent moisture barrier properties [104]. Although physical blending with CNTs is an economic way to modify polypropylene per‐ formance, compatibilizing agents are necessary for creating strong interface between filler particles and the polymer phase. Maleic anhydride grafted polypropylene (MA-*g*-PP) is of‐ ten used as a compatibilizer which can improve the PP/CNTs composite properties by strong hydrogen bonding between hydroxyl groups located on the acidic-treated CNTs sur‐ face and anhydride groups of MA-g-PP [139, 140]. Recently, an original and simple method for promoting mobility sensitivity of carbon nanotubes (CNTs) to an external stress field in polypropylene (PP) matrix was developed [141]. In particular, an interfacial melt reaction in‐ itiated by free radicals were used as a tool to prepare PP/CNTs nanocomposites. The pres‐ ence of tetrakis(phenylmethyl)thioperoxydi(carbothioamide) (TBzTD) increased the interfacial reaction between the PP chains and the CNTs. In addition, the grafted TBzTD to PP backbone could form a physical interaction with CNTs *via* a π–π interaction [141]. Ac‐ cording to their previous results [119, 126] based on a study of the radical grafting of poly‐ ethylene derivatives onto MWCNTs, Farzi et al. investigated MWCNTs' sidewall functionalization by tetramethylpentadecane and PP in the presence of 1wt% DCP at 160°C.

*3.2.2. A model compound approach through the use of 2,6,10,14-tetramethylpentadecane*

ence of MWCNTs is depicted in Figure 16.

Simlilarly to the pentadecane grafting procedure (see section 2.1.1.), 2,6,10,14-tetramethyl‐ pentadecane (TMP, C19H40) has been used as model for the grafting reaction of PP onto MWCNTs [129]. Thermolysis of dicumyl peroxide initiator performed in TMP and in pres‐

**3.2. Radical grafting of polypropylene on carbon nanotubes**

96 Syntheses and Applications of Carbon Nanotubes and Their Composites

of John Wiley and Sons.

Farzi et al. [129] have successfully grafted PP onto MWCNTs through a radical grafting reac‐ tion, carried out under similar experimental conditions to PE [128] and TMP [129] (1.5wt% DCP, 160°C) and using 1,2-dichlorobenzene (DCB) as solvent able to solubilize PP partially at elevated temperature. The corresponding PP-grafted nanotubes were analysed by TGA after a purification by soxhlet extraction in DCB. However, the authors were not able to ob‐ tain reproductible results with weight losses varying from 50% to 80% for the above-men‐ tioned experiment. This behaviour was attributed to the purification procedure which did not permit to remove all the free PP chains. The authors have also speculated on the degra‐ dation behaviour of PP through the well-known β-scission reaction occurring in the pres‐ ence of radical species therefore the authors were not able to give a PP grafting density. Then, the aforementioned PP coated MWCNTs have been dispersed within a commercially available PP matrix using a contra-rotating Haake Rheomixer and the amount of nanofiller in the final composites has been fixed to 3wt%. The evaluation of MWCNTs dispersion has been examined by using scanning electron microscopy (SEM) (Figure 17).

SEM images of the PP/PP-*g*-MWCNTs composites MWCNTs containing of 3wt% (Figure 17) demonstrated that there were still some areas where PP-*g*-MWCNTs were not found which was obviously connected with improper filler distribution. For a simple melt blend of PP with untreated MWCNTs, SEM images of the resulting material only showed clusters of a few tens micrometers of diameter evidencing a poor interfacial adhesion in the material (Figure 18), as reported by Lee [140] for untreated MWCNT/PP composites MWCNTs con‐ taining of 2wt%.

tually from a rheological point of view, a direct consequence of incorporation of fillers in molten polymers is the significant change in the steady shear viscosity behavior and the vis‐ coelastic properties. The level of filler dispersion is expected to play a major role in deter‐ mining the filler effects on non linear responses of nanocomposites. Generally speaking, thermoplastic polymers filled with nano-particles show a solid-like behavior response which includes a non–terminal zone of relaxation, apparent yield stress and a shear-thin‐

Polymer Nanocomposites Containing Functionalised Multiwalled Carbon NanoTubes

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99

Since the melt rheological properties of filled polymers are sensitive to the structure, concen‐ tration, particle size, shape and surface characteristics of the fillers, rheology offers original means to assess the state of the dispersion in nanocomposites and to investigate the influ‐ ence of flow conditions upon nano-filler dispersion itself [144]. As discussed previously, one of the most important challenges in filled polymer developments and applications is to ob‐ tain a homogeneous dispersion of CNT in polymer matrix by overcoming the van der Waals interaction between elementary tubes. As a result, it can be expected that the rheological percolation, and subsequently the non-linearity effect, depend on nanotube dispersion and aspect ratio. As matter of fact, a great level of activity in the domain of the rheology of poly‐ mers filled with CNT is reported in the more recent scientific literature. The rheological be‐ havior of melt thermoplastic polymer filled with NTC was reported to depend on nanotube dispersion, aspect ratio and alignment under flow. However, among the different studies on liquid systems filled with carbon nanotubes two types of relaxation mechanisms of CNT must be differentiated according to the matrix viscosity: Do the carbon nanotubes behave as Brownian particles? The Doi-Edwards theory for dilute regime (the nantotubes are free to rotate without any contacts) allows the rotary diffusivity *D* r0 of a rod (Length: L and diame‐ ter: d) in an isotropic suspension to be calculated by equation (1), in which kB is the Boltz‐

3*kBT* (ln(*L* / *d*)−0.8)

In semi-dilute regime, the rotary diffusivity *D* r can be written as equation (2), where *A* is a

Actually, the rheological behavior of CNT suspension is observed close to the Doi-Edwards theory on the Brownian dynamics of rigid rods. However, it was observed that low shear deformations induced an aggregation mechanism, but these aggregates broke down at high

)

*Dr* <sup>=</sup> *ADr*0(*ν<sup>L</sup>* <sup>3</sup>

Consequently, the rotary diffusion of CNT varies according to matrix viscosity:

*πηm<sup>L</sup>* <sup>3</sup> (1)

*Drα*1 / *η<sup>m</sup>* (3)

<sup>−</sup><sup>2</sup> (2)

ning dependence of viscosity on particle concentration, aspect ratio and dispersion.

mann constant and ηm is the viscosity of the suspending medium

*Dr*<sup>0</sup> =

dimensionless constant whose value is generally large (A~1000).

**Figure 17.** SEM micrographs of PP/PP-g-MWCNT composites with MWCNTs loading of 3wt%. Reproduced from [129] with permission of Elsevier.

**Figure 18.** SEM micrographs of PP/MWCNTs composites with MWCNTs loading of 3wt%. Reproduced from [129] with permission of Elsevier.

It was concluded from these results that the grafting of PP onto MWCNTs provided a low steric barrier against the strong intermolecular Van der Waals interactions among nanotubes within the PP matrix.

In a similar approach, isotactic polyrpopylene (iPP) was successfully grafted onto multiwal‐ led carbon nanotubes (MWCNTs) by direct macroradical addition by sonication in hot xy‐ lene with BPO as an initiator [142]. It was found that both iPP macromolecular radicals and small-molecular benzoic acid free radicals were grafted onto MWNTs. iPP-g-MWNTs dis‐ persed more uniformly in iPP than pristine MWNTs.

#### **3.3. Rheological behaviour of polyolefin based carbon nanotubes nanocomposites**

It has been well known for a century that the addition of fillers, mostly carbon black, to rub‐ ber compounds has a strong impact on the viscoelastic properties of materials. In recent years, polymer nanocomposites have been developed as a new class of composites [143]. Ac‐ tually from a rheological point of view, a direct consequence of incorporation of fillers in molten polymers is the significant change in the steady shear viscosity behavior and the vis‐ coelastic properties. The level of filler dispersion is expected to play a major role in deter‐ mining the filler effects on non linear responses of nanocomposites. Generally speaking, thermoplastic polymers filled with nano-particles show a solid-like behavior response which includes a non–terminal zone of relaxation, apparent yield stress and a shear-thin‐ ning dependence of viscosity on particle concentration, aspect ratio and dispersion.

(Figure 18), as reported by Lee [140] for untreated MWCNT/PP composites MWCNTs con‐

**Figure 17.** SEM micrographs of PP/PP-g-MWCNT composites with MWCNTs loading of 3wt%. Reproduced from [129]

**Figure 18.** SEM micrographs of PP/MWCNTs composites with MWCNTs loading of 3wt%. Reproduced from [129]

It was concluded from these results that the grafting of PP onto MWCNTs provided a low steric barrier against the strong intermolecular Van der Waals interactions among nanotubes

In a similar approach, isotactic polyrpopylene (iPP) was successfully grafted onto multiwal‐ led carbon nanotubes (MWCNTs) by direct macroradical addition by sonication in hot xy‐ lene with BPO as an initiator [142]. It was found that both iPP macromolecular radicals and small-molecular benzoic acid free radicals were grafted onto MWNTs. iPP-g-MWNTs dis‐

It has been well known for a century that the addition of fillers, mostly carbon black, to rub‐ ber compounds has a strong impact on the viscoelastic properties of materials. In recent years, polymer nanocomposites have been developed as a new class of composites [143]. Ac‐

**3.3. Rheological behaviour of polyolefin based carbon nanotubes nanocomposites**

taining of 2wt%.

98 Syntheses and Applications of Carbon Nanotubes and Their Composites

with permission of Elsevier.

with permission of Elsevier.

within the PP matrix.

persed more uniformly in iPP than pristine MWNTs.

Since the melt rheological properties of filled polymers are sensitive to the structure, concen‐ tration, particle size, shape and surface characteristics of the fillers, rheology offers original means to assess the state of the dispersion in nanocomposites and to investigate the influ‐ ence of flow conditions upon nano-filler dispersion itself [144]. As discussed previously, one of the most important challenges in filled polymer developments and applications is to ob‐ tain a homogeneous dispersion of CNT in polymer matrix by overcoming the van der Waals interaction between elementary tubes. As a result, it can be expected that the rheological percolation, and subsequently the non-linearity effect, depend on nanotube dispersion and aspect ratio. As matter of fact, a great level of activity in the domain of the rheology of poly‐ mers filled with CNT is reported in the more recent scientific literature. The rheological be‐ havior of melt thermoplastic polymer filled with NTC was reported to depend on nanotube dispersion, aspect ratio and alignment under flow. However, among the different studies on liquid systems filled with carbon nanotubes two types of relaxation mechanisms of CNT must be differentiated according to the matrix viscosity: Do the carbon nanotubes behave as Brownian particles? The Doi-Edwards theory for dilute regime (the nantotubes are free to rotate without any contacts) allows the rotary diffusivity *D* r0 of a rod (Length: L and diame‐ ter: d) in an isotropic suspension to be calculated by equation (1), in which kB is the Boltz‐ mann constant and ηm is the viscosity of the suspending medium

$$D\_{r0} = \frac{3k\_B T \left(\ln(L\_\perp/d) - 0.8\right)}{\pi \eta\_m L\_\perp^{\frac{3}{3}}}\tag{1}$$

In semi-dilute regime, the rotary diffusivity *D* r can be written as equation (2), where *A* is a dimensionless constant whose value is generally large (A~1000).

$$D\_r = A D\_{r0} (\nu L^{-3})^{-2} \tag{2}$$

Consequently, the rotary diffusion of CNT varies according to matrix viscosity:

$$D\_r \alpha 1/\eta\_m \tag{3}$$

Actually, the rheological behavior of CNT suspension is observed close to the Doi-Edwards theory on the Brownian dynamics of rigid rods. However, it was observed that low shear deformations induced an aggregation mechanism, but these aggregates broke down at high shear, forming small aggregates with less entanglements [145]. The shear rheology of such carbon nanotube suspensions was reviewed by Hobbie [146] from the perspective of colloid and polymer science.

mitted that the increase of the CNT concentration is driving this transition. Above this critical transition, generally associated with the percolation threshold, these nanocomposites show a solid-like behavior response, which includes a non-terminal zone of relaxation lead‐ ing to apparent yield stress and a shear-thinning dependence on viscosity |*η* \* (*ω*)|*αω* <sup>−</sup><sup>1</sup>

Polymer Nanocomposites Containing Functionalised Multiwalled Carbon NanoTubes

**Figure 19.** Variation versus frequency of the storage shear modulus G'(ω) and absolute complex viscosity η\*(ω) at dif‐

This non-terminal frequency behavior is generally attributed to the formation of an intercon‐ nected nanotube network in the polymer matrix. Therefore, the solid-like behavior is associat‐ ed nanotube–nanotube interactions which increase with the CNT content. Eventually, these interactions lead to percolation and the formation of an interconnected structure of nanotubes in the matrix. Due to the high aspect ratio of CNT (generally, L/d>150), the existence of this per‐ colation threshold is expected at low concentration. For example, from Fig 19, the percolation threshold can be estimated to be less than 2% of CNT. This percolation threshold is generally observed in the range 0.5%-5% depending on CNT nature (aspect ratio, surface chemical mod‐

If a lot of works have been devoted to the linear viscoelasticity of CNT nanocomposites whereas a few works have been reported on non-linear properties such as for example the melt flow instabilities. Interestingly, Palza et al [157] showed that carbon nanotubes modify the main characteristics of the spurt instability developed by the linear polyethylene. Fur‐ thermore, the sharkskin instability, developed in short chain branched polyethylene, is re‐ duced at low amounts of MWCNT. Furthermore, the critical shear rate for the on-set of the spurt and the sharkskin instabilities decreases in the nanocomposites probably due to the physical interactions between the polymer and the nanofiller. Finally, at high shear rates, the gross melt fracture instability is completely erased in the nanocomposites based on the line‐ ar polymer whereas in short chain branched polyethylene the amplitude of this bulk distor‐ tion is rather moderated. Clearly, the carbon nanotubes have a drastic effect on the main flow instabilities observed in polyethylene. Consequently, the processing of CNT nanocom‐

ferent concentrations of CNT (1 to 7%). Reproduced from [151] with permission of John Wiley and Sons.

ification) and on the processing methods for nanocomposite preparation.

posites, i.e under non-linear deformation, is an open investigation domain.

.

101

http://dx.doi.org/10.5772/50710

According to the Doi-Edwards theory, Marceau et al [147] have shown that the suspensions of CNT, at low concentration (ϕ=0.2%) and in low fluid matrix (ηm=5 Pa.s), behave as Brow‐ nian entities (Dr=5.0x10-5 s-1). The diffusion time of these CNTs is then *τ<sup>r</sup>* =1 / <sup>2</sup>*Dr* <sup>≈</sup>10<sup>4</sup> *s* . If we imagine that these same CNT are dispersed in high viscous polymer matrix such as molten PP (ηm~1x103 Pa.s), their relaxation time will be then: *τ<sup>r</sup>* <sup>≈</sup>2*x*10<sup>6</sup> *s* . The order magnitude of the relaxation time is then one month! Consequently, the carbon nanotubes cannot be con‐ sidered anymore as Brownian entities in most of the papers that have been addressed to the viscoelastic behavior of carbon nanotubes dispersed in high viscous molten polymers. The main challenge in such nanocomposite systems is to control the dispersion of the nanotubes in high viscous fluid in order to have the lowest percolation threshold regarding the electri‐ cal properties. For example, by improving the CNT dispersion using functionalized single wall nanotubes, Mitchell et al [148] observed that the percolation threshold dropped from 3wt% to 1.5% in PS nanocomposites.

Actually, the dispersion of CNT in polymer matrix is strongly difficult mainly due to the nanotube-nanotube interactions higher than the nanotube-polymer interaction. However, optimal dispersion of CNTs can be achieved in polar polymers such as polyamides, polyest‐ ers or polycarbonate. This optimal dispersion is generally measured, at least from a qualita‐ tive point of view, from the electrical and/or rheological percolation threshold. Nevertheless, the dispersion of CNT in polyolefin (PP, PE or copolymer of ethylene) is most of the time a real challenge due to unfavorable and low nanotube-polymer interactions. On the other hand, the fact that CNT have a high aspect ratio and are not Brownian in polymer matrix leads to the conclusion that the different works of the literature are difficult to compare. The samples, studied in rheology or electric conductivity, have generally undergone different processing conditions. As a result, CNT nanocomposites are totally out of isotropic disper‐ sion and the isotropic equilibrium of CNTs can never be achieved. However, general trends in CNT nancomposite can be described from the open literature.

From a sample preparation point of view, dispersion of CNTs in polyolefins were generally prepared via conventional melt processing, i.e melt blending in batch mixer or in twin screw extruder). Marginal methods may also be used as for example solid-state shear pulveriza‐ tion [149] or in situ lubrication methods [150]. Numerous studies [151-156] have been devot‐ ed to the linear viscoelasticity of PP nanocomposites based on CNT dispersion.

All of these papers reported an increase in shear viscosity and storage and loss moduli of the nanocomposites with increasing the CNT concentration as shown in Figure 19.

Furthermore, a general rheological trend for nanocomposites studied in most of these pa‐ pers is the appearance of a transition from a liquid-like behaviour to a solid-like behaviour, i.e. the apparition of a plateau (second plateau modulus, *Go* =lim *ω*→0 *G* '(*ω*) ) of the storage mod‐ ulus at low frequency which is obviously higher than the loss modulus. Obviously, it is ad‐ mitted that the increase of the CNT concentration is driving this transition. Above this critical transition, generally associated with the percolation threshold, these nanocomposites show a solid-like behavior response, which includes a non-terminal zone of relaxation lead‐ ing to apparent yield stress and a shear-thinning dependence on viscosity |*η* \* (*ω*)|*αω* <sup>−</sup><sup>1</sup> .

shear, forming small aggregates with less entanglements [145]. The shear rheology of such carbon nanotube suspensions was reviewed by Hobbie [146] from the perspective of colloid

According to the Doi-Edwards theory, Marceau et al [147] have shown that the suspensions of CNT, at low concentration (ϕ=0.2%) and in low fluid matrix (ηm=5 Pa.s), behave as Brow‐

imagine that these same CNT are dispersed in high viscous polymer matrix such as molten

the relaxation time is then one month! Consequently, the carbon nanotubes cannot be con‐ sidered anymore as Brownian entities in most of the papers that have been addressed to the viscoelastic behavior of carbon nanotubes dispersed in high viscous molten polymers. The main challenge in such nanocomposite systems is to control the dispersion of the nanotubes in high viscous fluid in order to have the lowest percolation threshold regarding the electri‐ cal properties. For example, by improving the CNT dispersion using functionalized single wall nanotubes, Mitchell et al [148] observed that the percolation threshold dropped from

Actually, the dispersion of CNT in polymer matrix is strongly difficult mainly due to the nanotube-nanotube interactions higher than the nanotube-polymer interaction. However, optimal dispersion of CNTs can be achieved in polar polymers such as polyamides, polyest‐ ers or polycarbonate. This optimal dispersion is generally measured, at least from a qualita‐ tive point of view, from the electrical and/or rheological percolation threshold. Nevertheless, the dispersion of CNT in polyolefin (PP, PE or copolymer of ethylene) is most of the time a real challenge due to unfavorable and low nanotube-polymer interactions. On the other hand, the fact that CNT have a high aspect ratio and are not Brownian in polymer matrix leads to the conclusion that the different works of the literature are difficult to compare. The samples, studied in rheology or electric conductivity, have generally undergone different processing conditions. As a result, CNT nanocomposites are totally out of isotropic disper‐ sion and the isotropic equilibrium of CNTs can never be achieved. However, general trends

From a sample preparation point of view, dispersion of CNTs in polyolefins were generally prepared via conventional melt processing, i.e melt blending in batch mixer or in twin screw extruder). Marginal methods may also be used as for example solid-state shear pulveriza‐ tion [149] or in situ lubrication methods [150]. Numerous studies [151-156] have been devot‐

All of these papers reported an increase in shear viscosity and storage and loss moduli of the

Furthermore, a general rheological trend for nanocomposites studied in most of these pa‐ pers is the appearance of a transition from a liquid-like behaviour to a solid-like behaviour,

ulus at low frequency which is obviously higher than the loss modulus. Obviously, it is ad‐

*ω*→0

*G* '(*ω*) ) of the storage mod‐

ed to the linear viscoelasticity of PP nanocomposites based on CNT dispersion.

nanocomposites with increasing the CNT concentration as shown in Figure 19.

*s* . If we

*s* . The order magnitude of

nian entities (Dr=5.0x10-5 s-1). The diffusion time of these CNTs is then *τ<sup>r</sup>* =1 / <sup>2</sup>*Dr* <sup>≈</sup>10<sup>4</sup>

Pa.s), their relaxation time will be then: *τ<sup>r</sup>* <sup>≈</sup>2*x*10<sup>6</sup>

in CNT nancomposite can be described from the open literature.

i.e. the apparition of a plateau (second plateau modulus, *Go* =lim

and polymer science.

100 Syntheses and Applications of Carbon Nanotubes and Their Composites

3wt% to 1.5% in PS nanocomposites.

PP (ηm~1x103

**Figure 19.** Variation versus frequency of the storage shear modulus G'(ω) and absolute complex viscosity η\*(ω) at dif‐ ferent concentrations of CNT (1 to 7%). Reproduced from [151] with permission of John Wiley and Sons.

This non-terminal frequency behavior is generally attributed to the formation of an intercon‐ nected nanotube network in the polymer matrix. Therefore, the solid-like behavior is associat‐ ed nanotube–nanotube interactions which increase with the CNT content. Eventually, these interactions lead to percolation and the formation of an interconnected structure of nanotubes in the matrix. Due to the high aspect ratio of CNT (generally, L/d>150), the existence of this per‐ colation threshold is expected at low concentration. For example, from Fig 19, the percolation threshold can be estimated to be less than 2% of CNT. This percolation threshold is generally observed in the range 0.5%-5% depending on CNT nature (aspect ratio, surface chemical mod‐ ification) and on the processing methods for nanocomposite preparation.

If a lot of works have been devoted to the linear viscoelasticity of CNT nanocomposites whereas a few works have been reported on non-linear properties such as for example the melt flow instabilities. Interestingly, Palza et al [157] showed that carbon nanotubes modify the main characteristics of the spurt instability developed by the linear polyethylene. Fur‐ thermore, the sharkskin instability, developed in short chain branched polyethylene, is re‐ duced at low amounts of MWCNT. Furthermore, the critical shear rate for the on-set of the spurt and the sharkskin instabilities decreases in the nanocomposites probably due to the physical interactions between the polymer and the nanofiller. Finally, at high shear rates, the gross melt fracture instability is completely erased in the nanocomposites based on the line‐ ar polymer whereas in short chain branched polyethylene the amplitude of this bulk distor‐ tion is rather moderated. Clearly, the carbon nanotubes have a drastic effect on the main flow instabilities observed in polyethylene. Consequently, the processing of CNT nanocom‐ posites, i.e under non-linear deformation, is an open investigation domain.
