In this method, there are some steps which result critical to guarantee a successful grafting process. First, the biphasic catalytically mediated oxidation reaction (Step 1.1) should be carried out with recently dispersed carbon nanotubes (Step 1.1.1.5). If dispersion results unviable according to the recommendations in the protocol, the use of an ultrasonic tip sonicator would be helpful if using the same indications (Step 1.1.1.6). Using shorter MWCNTs may also help in solving dispersion issues. Second, setting of the vacuum filtration system is crucial in purification efficiency (Step 1.2.2). In this sense, centering the membrane on the sintered glass area of the filter support surface (Step 1.2.2.5) may result in membrane wrinkles if the procedure is not followed appropriately (particularly, Steps 1.2.2.5 - 1.2.2.6). If the latter occurs, repeat Steps 1.2.2.3 to 1.2.2.5 until homogeneous filter adhesion is obtained. Alternatively, also try with non-wetted membrane versions (i.e. do not follow Steps 1.2.2.2 - 1.2.2.4) and observe filtration results. The use of dry membranes prevents the occurrence of membrane wrinkles during their fixation in Steps 1.2.2.5 - 1.2.2.6, while, depending on the membrane material used and selected manufacturer, cutoff size may vary between dry and wet versions and filtration efficiency might be affected depending on the case. Third, the polymerization reaction is the last critical step (Step 2.2). The most common source of inefficient polymerization is the use of non-purified monomer. Make sure to use freshly purified styrene using an alumina gel preparative column, cover the container with aluminum foil to protect the monomer from light and keep stored at 4 °C until used. The use of MWCNTs with a larger diameter or shorter lengths should not reflect any representative variation in the final outcomes. However, limitations may arise if SWCNTs, double-wall carbon nanotubes or MWCNTs with a shorter diameter are used. The use of the previous three examples may result into decomposition of the nanotube structure if the oxidation reaction (Step 1.1.3) is carried out for the same reaction time. Troubleshooting of the latter may be done by testing shorter times and performing TGA and FT-IR analysis to confirm optimal results.
TGA is the simplest method for monitoring the success in each chemical modification step. A direct analysis of the mass losses and temperature values where these occur in TGA curves obtained between room temperature and 1000 °C allow for a quantification of the modification yield in the products (Figure 1). The TGA curve for the pristine MWCNTs exhibits one single drop in mass between 550 °C and 820 °C for up to 96% in weight (black curve in Figure 1). This loss in mass corresponds to the decomposition of the nanotubes when the analysis is carried out under air flow. Beyond 820 °C a constant weight is observed due to remaining inorganic impurities in the raw product. Under the same analysis conditions, MWCNT-OH (red curve in Figure 1) shows an additional weak drop between 200 °C and 300 °C in comparison with the MWCNT curve.22 The difference in weight percent between the MWCNT curve and the MWCNT-OH at the end of the previous range indicates the content in hydroxyl groups inserted to the nanotube sidewalls during the biphasic catalytically mediated oxidation reaction. Typical hydroxyl content for MWCNT-OH is found between 2% and 5% in weight. Besides, an absence of this additional weight drop indicates that the hydroxylation reaction did not occur. Beyond that temperature range, a complete decomposition of the nanotubes occurs earlier at 800 °C, while higher temperatures afford a constant weight value. On the other hand, a typical TGA curve for MWCNT-O-TMSPMA shows two consecutive drops in weight under the same air flow conditions (blue curve in Figure 1). The first mass loss is found between 380 °C and 470 °C, which corresponds to the decomposition of the methacrylic moieties from the TMSPMA inserted to the hydroxylic groups; the temperature interval is in agreement with the literature22,25 for TMSPMA similarly inserted to different types of nanostructures via covalent chemistry. The second drop starts at 550 °C and ends at 790 °C. This weight loss is originated by the decomposition of carbon in the nanotubes. The constant value in mass observed after this temperature interval corresponds to both the remaining inorganic matter from the original nanotubes and non-volatile silicate derivatives formed during the decomposition of the TMSPMA moieties. The relationship between the first weight drop compared with the second one corresponds to the content in TMSPMA in the nanotubes. In this sense, the first loss is typically of 8% to 12% in weight compared with the second drop. The absence of the first weight drop is evidence of failure in the coupling of TMSPMA to the hydroxyl groups. Finally, a representative TGA curve for MWCNT-O-PS (green curve in Figure 1) shows three clear variations in weight under air flow, if compared with the pristine counterparts. The first drop occurs between 270 °C and 380 °C and is produced when the polystyrene chains grafted to the nanotubes are decomposed; this interval of temperature is in accordance with the literature22,26 for PS grafted to different types of carbon materials through covalent procedures. The second weight loss starts at ca. 400 °C and ends at 480 °C, which is produced by the loss of the methacrylic component from TMSPMA. The third drop appears at around 600 °C and ends at 780 °C and is a result of the decomposition of the nanotubes. The ratio between the first weight drop and the third one provides the PS content in the polymer-grafted nanotubes. Typical content in PS for MWCNT-O-PS is found between 30% and 40% in weight compared with the nanotube content.23 Lack of the first weight drop is evidence of failure in the polymerization step.
The FT-IR spectra can be useful to confirm the presence of the reactive functional groups introduced to the pristine MWCNTs (Figure 2). Those groups include the hydroxyls and the silylated methacrylic moieties. Typically, spectra from MWCNT-OH (red curve, Figure 2a) show a broad strong band at 3427 cm-1, which corresponds to the stretching of O-H groups. Additionally, a weak but clear band can also be found at 1193 cm-1 produced by the stretching of the bonds between the aromatic carbons in the nanotube walls and the OH groups. On the contrary, spectra from MWCNT-O-TMSPMA (blue curve, Figure 2b) show a strong band at 3442 cm-1 produced by the stretching of Si-OH bonds. The same bonds also produce two additional moderate bands at 1030 cm-1 and 812 cm-1, respectively. In addition, the carbonyl C=O bond in the ester group of the methacrylic moieties afford a weak stretching band at 1718 cm-1. Moreover, Si-OC bonds formed between the TMSPMA group and the nanotube give two typical moderate bands appearing at 1102 cm-1 and 801 cm-1, whereas the last band is partially overlapped to the neighboring band at 812 cm-1 from Si-OH. Methacrylic C=C bonds in the inserted TMSPMA moieties give one moderate stretching band at 1646 cm-1. Finally, Si-C bonds contained in the silylated portion provide a weak but clear stretching band at 707 cm-1. An absence of the bands at 1102 cm-1 and 801 cm-1 indicates two possibilities: 1) failure in the covalent linking between TMSPMA and the hydroxyl groups at the nanotubes and 2) inefficient elimination of reactants. The lack of the bands at 1718 cm-1 and 1646 cm-1 shows that undesired hydrolysis of the ester group occurred during product purification (e.g. by mistakenly washing with acids or bases).
Microscopic analysis of drop-cast solutions using THF as solvent can show the typical self-assembly behavior in MWCNT-O-PS which does not occur in pristine counterparts (Figure 3).23 Solutions from pristine MWCNTs analyzed by TEM after evaporation afford typical random networks of nanotubes or clusters (Figure 3a). However, equivalent samples prepared from MWCNT-O-PS provide aligned nanostructures which contain collinear nanotubes self-assembled by the walls (Figure 3b). This auto-organization behavior is produced by the anisotropic patchiness generated by the polystyrene chains grafted to the sidewalls of the nanotubes. Typical examples for self-organized nanotubes provide assembled bodies which contain between two and six nanotubes adhered to each other along the longitudinal axis thereof. Failure in polymer-grafting typically results in absence of that trend.
We have demonstrated a method for obtaining multiwalled carbon nanotubes with anisotropic self-assembly properties via grafting polystyrene chains on the sidewalls using a free-radical polymerization route. Such a selective modification of the surface properties of the nanotubes is obtained by successive chemical modification steps to insert reactive functional groups selectively to the sidewalls. These successive modifications allow for the modulation of the surface patchiness which finally results into collinearly auto-organized nanostructures through non-covalent interactions. We expect that this strategy can be re-applied to other acrylic- or vinyl-derivative polymer types and new hybrid materials and composites could arise in a future. Moreover, we believe that this method would open new opportunities in carbon nanotube processing strategies under attractive conditions for the industry and academia.