Carmen Racles*a,
Mihaela Alexandrua,
Adrian Belea,
Valentina E. Musteataa,
Maria Cazacua and
Dorina M. Opris*b
a“Petru Poni” Institute of Macromolecular Chemistry, Aleea Grigore Ghica Voda 41A, Iasi, 700487, Romania. E-mail: raclesc@icmpp.ro; Fax: +40 232211299; Tel: +40 232217454
bEmpa, Swiss Federal Laboratories for Materials Science and Technology, Laboratory for Functional Polymers, Ueberlandstr. 129, CH-8600, Dübendorf, Switzerland. E-mail: dorina.opris@empa.ch
First published on 11th August 2014
New polymers with tuneable dielectric properties were prepared by modifying trimethylsilyl end-terminated poly(methylhydro)siloxane with polar γ-cyanopropyl groups. The amount of polar groups was tuned by adjusting the allyl cyanide/n-hexene ratio in poly(methylhydro)siloxane co-hydrosilylation. The copolymers were characterized by FTIR and NMR spectroscopy. The distribution of the polar groups along the chain was evaluated based on 1H NMR spectroscopy. The influence of the amount of polar γ-cyanopropyl on the glass transition temperature (Tg) and on the dielectric properties was investigated by DSC and impedance spectrometry. All polymers showed Tgs well below room temperature. A linear increase in permittivity (ε′) with increasing amount of γ-cyanopropyl groups was observed. A maximum ε′ value of 15.9 for the copolymer containing 89 mol% polar groups was achieved, which is 6-fold higher than polydimethylsiloxane. The incomplete conversion of Si–H groups observed in all hydrosilylation reactions with allyl cyanide opened up the possibility of using the prepared copolymers as cross-linkers.
One class of materials of high interest for DEA applications are silicone elastomers since they have large strain at break,16,17 are resistant to oxygen, water and sunlight,18 and are biocompatible.19,20 But probably the most attractive properties of silicones for DEA are their good elastic properties over a wide range of temperatures and frequencies.21 Additionally, silicones have very high dielectric strength of more than 80 V μm−1 (ref. 22 and 23) and high energy density.24 However, the use of silicones in some DEA products is limited by the high driving voltage necessary for actuation mainly due to their ε′ which is lower than 3. Therefore, much research is presently being devoted to increase their ε′ while maintaining the electrical conductivity and the Y at low values. Modification of silicones with functional side groups is one approach that was recently explored.13,14,25 Although countless side-chain modified polysiloxanes are reported, only a few were especially designed for actuator applications.13,25
Hydrosilylation is a powerful tool for the modification of siloxane compounds.26,27 However, its application can be sometimes problematic due to catalyst's sensitivity. For example, we recently used allyl cyanide for hydrosilylation of hydroxyl end-functionalised poly(dimethyl-co-methyhydro)siloxanes and found that the conversion of the hydrosilyl (Si–H) groups to cyanopropyl was incomplete even when a large excess of allyl cyanide was used.14 Additionally, a spontaneous self-cross-linking of the starting materials as well as of the functionalised product was observed when stored in a non-protected atmosphere for a long time.
Therefore, the first goal of this work was to clarify some aspects of (co-)hydrosilylation reaction with allyl cyanide and platinum divinyltetramethyldisiloxane complex (Pt(dvs)) catalyst and to verify whether the hydroxyl end-groups are responsible for the spontaneous cross-linking reactions mentioned above. The second goal was to find out how the ε′ is influenced by the amount of cyanopropyl groups and which is the maximum value of the ε′ that can be reached with this system. To achieve such goals, a trimethylsilyl end-terminated poly(methylhydro)siloxane, which by structure carries a Si–H group on every repeat unit, was used in hydrosilylation reactions. To obtain polymers with different content of polar cyanopropyl groups, a mixture of allyl cyanide and n-hexene was used, whereby their proportion was varied. To find out how the cyanopropyl groups are distributed on the polymer chain, the 1H NMR spectra of the resulting copolymers were carefully analysed.
The infrared spectra were recorded on a Bruker Vertex 70 FT-IR instrument, in transmission mode, in the 300–4000 cm−1 range (resolution 2 cm−1, 32 scans) at ambient temperature. 1H NMR spectra were recorded on 400 MHz Bruker spectrometer in CDCl3. Differential scanning calorimetry (DSC) investigations were done on a Pyris Diamond DSC (Perkin Elmer USA) instrument. The sorption capacity of water vapours was measured in dynamic regime at 25 °C (298 K) by using an IGAsorp equipment (Hiden Analytical, Warrington UK) at different relative humidity (RH). The vapour pressure was increased and decreased in 10% RH steps between 0 and 90% for sorption and reverse for desorption, each having a pre-established equilibrium time of 15 and 30 min, respectively.
The complex dielectric permittivity was measured using Novocontrol Dielectric Spectrometer Concept 40 Alpha Analyzer equipped with a Quatro temperature controller. Measurements were carried out at frequencies between 1 and 106 Hz at room temperature. For the temperature dependence experiment, frequency scans were performed in 5 °C steps, in temperature range from −150 to +60 °C. The liquid polymers were placed between two golden plated stainless steel electrodes (diameter 20 mm) and the distance between electrodes was adjusted to 140 μm using spacers.
For feed ratios, final compositions and molecular weights please see Table 1.
Entry | C4H5Na [% mol] (feed) | C6H12 [% mol] (feed) | Conversionb [%] | Mn calculated [g mol−1] |
---|---|---|---|---|
a The feed amounts were calculated as 10% (mol) excess reported to prescribed composition, except for polymer B1 (see text).b Total conversion for hydrosilylation. | ||||
B1 | 87.8 (200) | — | 87.8 | 4050 |
B2 | 89 (110) | — | 89 | 4070 |
B3 | 62.1 (82.5) | 26.9 (27.5) | 89 | 4220 |
B4 | 38.8 (55) | 51.1 (55) | 89.9 | 4380 |
B5 | 16 (27.5) | 74 (82.5) | 90 | 4505 |
B6 | 9.2 (13.2) | 82.9 (96.8) | 92.1 | 4620 |
B7 | — | 99.6 (110) | 99.6 | 4860 |
As an example, the procedure for copolymer B3 is described. Poly(methylhydro)siloxane (5 g), allyl cyanide (4.24 g, 5.05 mL, 63.3 mmol) and n-hexene (1.78 g, 2.6 mL, 21 mmol), i.e. a total of 1.1 mol un-saturated reagents per mol of Si–H, were dissolved in dry toluene (10 mL). To the resulting solution, Karstedt's catalyst (0.4 mL, i.e. 5.2 μL per mmol of Si–H) was added and the reaction mixture was stirred at 70 °C for 6 h. Then the solvent and un-reacted reagents were removed by rotary evaporation.
1H NMR (400 MHz, CDCl3) δ, ppm: 0.17 (Si–CH3, 116H); 0.57 (CH3–(CH2)4–CH2–Si, 17H); 0.76 (NC–CH2–CH2–CH2–Si, 38H); 0.93 (CH3–(CH2)4–CH2–Si, 26H); 1.35 (CH3–(CH2)4–CH2–Si, 68H); 1.75 (NC–CH2–CH2–CH2, 41H); 2.43 (NC–CH2–CH2–CH2, 42H); 4.75 (un-reacted Si–H, 3.5H).
13C NMR (400 MHz, CDCl3) δ, ppm: −0.63 ((CH3)–Si); −0.35 (CH3–Si(CH2–CH2–CH2–CN)); 1.89 (CH3–Si(CH2)5–CH3); 14.14 (Si–(CH2)5–CH3); 16.84 (Si–CH2–CH2–CH2–CN); 17.55 (Si–CH2–CH2–CH2–CH2–CH2–CH3); 19.70 (Si–CH2–CH2–CH2–CN); 20.41 (Si–CH2–CH2–CH2–CN); 22.62 (Si–CH2–CH2–CH2–CH2–CH2–CH3); 22.98 (Si–CH2–CH2–CH2–CH2–CH2–CH3); 31.61 (Si–CH2–CH2–CH2–CH2–CH2–CH3); 33.00 (Si–CH2–CH2–CH2–CH2–CH2–CH3); 119.55 (Si–CH2–CH2–CH2–CN).
The 1H NMR and 13C NMR spectra are presented in Fig. 1S and 2S (ESI†).
In the case of copolymers B4–B6 an exothermic reaction was observed when the catalyst was introduced and therefore the reaction vessel was cooled in an iced bath within the first few minutes then mounted in the multireactor.
For copolymer B7, only n-hexene was used and therefore the procedure was slightly modified. The reaction was done in a two-neck vessel, equipped with condenser and magnetic stirring. After slow addition of the catalyst, the reaction mixture was kept at room temperature until no exothermic effect was observed. The reaction was continued for 6 h at 70 °C. The solvent and the un-reacted n-hexene were removed by rotary evaporation.
1H NMR (400 MHz, CDCl3) δ, ppm: 0.02–0.09 (Si–CH3, 116H); 0.50 (CH3–(CH2)4–CH2–Si, 65H); 0.93 (CH3–(CH2)4–CH2–Si, 98H); 1.3 (CH3–(CH2)4–CH2–Si, 260H); 4.70 (un-reacted Si–H, 0.14H).
In FT-IR spectra (Fig. 3S†) the main absorption bands were assigned to: siloxane bonds at 1022–1093 cm−1 (Si–O–Si asymmetric stretch, typical pattern for polymers), γ Si–CH3 at 743 and 801 cm−1, δ Si–CH3 at 1261 cm−1, un-reacted Si–H bonds at 2157 cm−1, and CN groups at 2247 cm−1.
1H NMR spectrum of copolymer B3 is given in Fig. 1 and the calculation of the composition is given in Fig. 1S.† Table 1 summarizes the composition of all copolymers. Although an excess of allyl cyanide was used, the conversion of Si–H groups was in all cases around 90%.
Due to the electron withdrawing cyano group, allyl cyanide is less reactive then n-hexene in hydrosilylation. An exothermic reaction was observed when the proportion between n-hexene and allyl cyanide was increased, i.e. in reactions B4–B7. Therefore, the hexyl group content found by 1H NMR was very close to the prescribed one or even higher in B3 and B4 (Table 1). Only in B6, the hexyl content was lower than prescribed (82.9% instead of 87.5%). This might be due to evaporation of n-hexene due to the above mentioned exothermic reaction, despite the precautions taken as to cool the reaction mixture in an iced bath. For copolymer B7 the conversion was 99.6% and the 1H NMR and FT-IR spectra showed little residual Si–H groups.
The polar group content was in all cases lower than expected (Table 1). Since the amount of hexyl groups is close to that prescribed, the incomplete overall conversion for the hydrosilylation is due to lower reactivity of allyl cyanide.
A precise assignment of the 0–0.4 ppm region of the 1H NMR spectra is challenging (Fig. 2). Four types of methylsilyl protons are present in this region: the (CH3)3Si chain ends (E), the Si(hexyl)CH3 non-polar groups (DN), the Si(cyanopropyl)CH3 polar groups (DP) and the un-reacted methylhydrosiloxane units (DH). The assignments of triad sequences in series B as well as of the starting homopolymer are given in Table 2. A straightforward assignment can be done only in the case of B7, where practically all Si–H groups were replaced by non-polar hexyl groups, which determined important modifications in the chemical shifts as compared to the starting homopolymer, i.e. 0.13 (CH3)3Si chain ends (E), 0.08 Si(hexyl)CH3 (DN) groups and 0.06 DN in the middle of the chain.
Polymer | Peaks (δ, ppm) and sequences | ||||||
---|---|---|---|---|---|---|---|
Homopolymer | 0.25 | 0.20 | 0.17 | ||||
DHDHDH | DHDHE | E | |||||
B1 | 0.25 | 0.23 | 0.19 | 0.16 | 0.15 | ||
DPDHDP | DHDPDP | DPDPDP | DPDPE | E | |||
B3 | 0.25–0.23 (sh) | 0.19 | 0.17 | 0.15 | 0.14 | ||
DPDHDP, DPDHDN, DNDPDH | DPDPDP | DPDPDN, DNDPDN | DPDNDP, DPDNDN | DNDND, E | |||
B4 | ∼0.23–0.18 | 0.16 | 0.15–0.14 | 0.11; 0.07 | 0.09 | ||
DPDHDP, DPDHDN, DNDPDH | DPDPDP | DPDNDP, DPDNDN, DPDPDN, DNDPDN | DNDNDN | E | |||
B5 | 0.21 | 0.19 | 0.17 | 0.14 | 0.12–0.11 | 0.09; 0.07 | |
DPDHDP | DPDHDN, DNDPDH | DPDPDP | DPDNDP DPDPDN, DNDPDN | DPDNDN, E | DNDNDN | ||
B6 | 0.21 | 0.18 | 0.16 | 0.13 | 0.12–0.11 | 0.09; 0.07 | |
DPDHDP | DPDHDN, DNDPDH | DPDPDP | DPDNDP DPDPDN, DNDPDN | DPDNDN, E | DNDNDN | ||
B7 | 0.09 | 0.04; 0.02 | |||||
E | DNDNDN |
In the other spectra of copolymers the Si(cyanopropyl)CH3 polar groups (DP) are located between 0.16 and 0.25 ppm, with a maximum at 0.19 ppm in B1 polymer (for which full functionalisation with allyl cyanide was intended). In the low field region, the methyl protons of the un-reacted methylhydrosiloxane units (around 10%) are also present, but a precise assignment of the signals is rather difficult. In copolymers B3–B6, in addition to methyl groups from DH units, new signals due to the DP and DN are present which makes the interpretation even more challenging. It is reasonable to assume that the methyl groups in polar units would be located at lower field, while those in nonpolar units at higher field. This trend is clearly observed in Fig. 2.
The proportion of protons of the methyl groups from most polar triads DPDPDP (located at 0.19 ppm in B3 and at 0.16 ppm in the other samples) reported to the total number of CH3 protons in the polar units was around 60% in all copolymers. On the other hand, the proportion of the methyl groups in nonpolar triads DNDNDN (generally at 0.11 ppm and at 0.09 ppm in B3) to the total number of CH3 protons gave variable results. The nonpolar groups in nonpolar triads were around 35% for B3 and B4, and about 65% for B5 and B6 copolymers.
To explain this trend, a model hydrosilylation reaction of a poly(dimethyl-co-methylhydro)siloxane was done according to Racles et al.14 Fig. 4S† shows the 1H NMR spectra of a poly(dimethyl-co-methylcyanopropyl)siloxane and the corresponding starting poly(dimethyl-co-methylhydro)siloxane. The assignments of chemical shifts for methylsiloxy groups in the initial copolymer (calibrated at 7.30 ppm for CHCl3) were as follows (ppm) (Fig. 4Sa and d† top): 0.09 (CH3)3Si; 0.12 (CH3)2Si in DDD, 0.14 DDDH and DHDDH; 0.16 (CH3)SiH in DDHD; 0.19 DDHDH; 0.21 DHDHDH. In the spectrum of the cyanopropyl modified copolymer (Fig. 4Sb and d† bottom), all the protons in DH centered triads disappeared and a new peak appeared at 0.135 ppm due to addition of allyl cyanide. The less reactive D centered triads remained. The same trend can be observed in the region of the Si–H protons (Fig. 4S-c†). The most polar protons (at 4.74 ppm) disappeared, while the Si–H protons in the vicinity of D units were un-reacted (less polar, at 4.73 and 4.70 ppm). Thus, it can be concluded that the most polar Si–H groups are consumed in the hydrosilylation reaction while the less reactive Si–H groups which are isolated between two dimethylsiloxy units (DDHD) remained unmodified. This is in agreement with previous studies which showed that neighbor Si–H groups are more reactive.27
Coming back to the series B copolymers, we concluded that, due to the higher reactivity of n-hexene as compared to allyl cyanide, n-hexene is less selective than allyl cyanide and therefore occupies random positions on the polysiloxane chain. Allyl cyanide prefers the more reactive Si–H neighbour positions, increasing the tendency to form short polar segments. As a result, the proportion of nonpolar short segments is reduced in copolymers containing more cyano groups.
Additional experiments were carried out, where the alkene reagents were added stepwise. Partial hydrosilylation of poly(methylhydro)siloxane with allyl cyanide or n-hexene (0.55 mol alkene to 1 mol Si–H) allowed formation of B8a and B9a, respectively. These copolymers were subsequently reacted with the complementary alkene co-reagent to afford copolymers B8 and B9. The 1H NMR spectra of the partially hydrosilylated copolymers B8a and B9a are shown in Fig. 3. When allyl cyanide was used first (B8a) most of the methyl protons from DP units were in polar triades DPDPDP, while when n-hexene was used first (B9a), only half of the methyl protons in DN units were in nonpolar triades DNDNDN. This shows the tendency of allyl cyanide to occupy vicinal positions and the more random addition of the more reactive n-hexene. It should be also mentioned here that the second hydrosilylation step done to obtain B8 was slow, e.g. 5 h after the n-hexene was added only around 10% was consumed. When additional catalyst was added, total conversion of Si–H groups was achieved. The low conversion of the n-hexene in the second step might be due to the catalyst poisoning by allyl cyanide. For the synthesis of B9 the addition of allyl cyanide in the second step afforded about 87% overall conversion of Si–H groups after 5 h.
Fig. 3 1H NMR of intermediary copolymers obtained by reacting 55% of Si–H groups in poly(methylhydrosiloxane) with either allyl cyanide (B8a) or n-hexene (B9a). |
Thus, the NMR data point towards a tendency of allyl cyanide to form short polar blocks, which is favoured by the presence of Si–H vicinal groups. However, the high reactivity and low selectivity of the n-hexene “limits” the length of the polar blocks where a mixture of alkene is used (B3–B6).
For the hydrosilylation several factors proved to have an influence on the kinetics and on the final composition of the copolymers. For example, when allyl cyanide was used either alone or in combination with n-hexene, incomplete hydrosilylation was observed. The incomplete conversion in hydrosilylation was reported before28 and discussed in relation with different reactivity of vicinal and isolated Si–H groups. In our case, attempts to increase the conversion by using excess of allyl cyanide (50%) or more catalyst (25 μL per mmol Si–H) and longer reaction time (24 h) were not successful. The 1H NMR spectrum still showed about 2.3% un-reacted Si–H groups.
The glass transition temperatures (Tg) were determined by differential scanning calorimetry (DSC) in the second heating curves. Single Tg values were obtained and no other transition was observed during DSC scans. A linear increase in Tg with increasing the cyanopropyl content was observed from −111 °C for B7 to −62 °C for B1 (Fig. 5 and 5S†). The non-polar hexyl groups act as softener for the copolymers, while the polar groups tend to increase the Tg. Compared to the starting poly(methylhydro)siloxane (Tg = −139.7 °C), all copolymers exhibited higher Tg values. The presence of a single Tg for all copolymers is an indication that no phase separation occurs. Similar results were reported for poly(dimethyl-co-methylcyanopropyl)siloxanes with polar groups content from 8.5 to 100% synthesized by ring opening polymerization of dimethyl and cyanopropyl containing monomers.29
Fig. 5 Variation of glass transition temperature in B series of copolymers as function of polar cyanopropyl groups: experimental (■) and predicted according to Gordon–Taylor equation (▲). |
Gordon–Taylor eqn (1) was used to calculate the glass transition temperatures for copolymers and blends. In our system with three types of structural units, it can be written as follows:
1/Tg = wA/TAg + wB/TBg + wC/TCg | (1) |
The Tg value of poly(methylcyanopropyl)siloxane (100% modification degree) was taken from the literature (Tg = −64.5 °C).29 Although this value is lower than that obtained by us for the copolymer with 89% modification degree, a good correlation between the calculated and experimental data was obtained (Fig. 5).
Entry | Mol% CN-modified siloxane units | wt% CN groups | ε′ at 1 Hz | ε′ at 10 kHz | ε′′ at 10 kHz | σ (S cm−1) at 10 kHz |
---|---|---|---|---|---|---|
B7 | 0 | 0 | 3.15 | 2.74 | 5 × 10−3 | 2.8 × 10−11 |
B6 | 9.2 | 1.7 | 3.8 | 3.7 | 1.9 × 10−2 | 1.1 × 10−11 |
B5 | 16 | 3.0 | 5.1 | 4.7 | 2 × 10−2 | 1.1 × 10−10 |
B4 | 38.8 | 7.5 | 13.7 | 7.4 | 1.4 × 10−1 | 8 × 10−10 |
B3 | 62.1 | 12.5 | 26.2 | 11.3 | 6.2 × 10−1 | 3.5 × 10−9 |
B1 | 87.8 | 18.5 | 261.6 | 15.7 | 3.5 | 1.9 × 10−8 |
B2 | 89 | 18.6 | 174.9 | 15.9 | 2.5 | 1.4 × 10−8 |
Fig. 6 Dielectric properties of the copolymers: dielectric permittivity (top), dielectric loss (middle), and conductivity (bottom). |
Fig. 7 Dielectric permittivity at 10 kHz of copolymers as function of polar cyano group mass content. |
The ability of a material to be polarized in an electric field increases with the polar group content. Thus, the increase in ε′ with increasing the polar cyano group content is not surprising. However, it is important to note that the maximum value for the ε′ that can be achieved with cyano polar groups is ca. 16, which means an increase by a factor of 6 compared to polydimethylsiloxane.
The ε′ increases very much at low frequencies, which is a universal phenomenon known as the low frequency dispersion.30 A strong increase in the dielectric loss for the polymers with high content of polar groups was also observed, as well as an increase in conductivity with increasing the content of cyanopropyl groups. However, in all cases, the conductivity values remained in the limits of the dielectric materials (Table 3).
The high ε′′ at low frequency, with values as high as 105, correlated with the frequency dependence – linear at low frequencies in a double logarithmic scale, with the slope of logε′′(f) close to −1 – indicate that the nature of dielectric loss is mainly conductive.
The increase in ε′ at lower frequencies was reported before, for example, in silicone films blended with cyanopropyl-modified polysiloxanes31 and was assigned to adsorbed water. Indeed, by increasing the polarity of a polymer, the amount of absorbed water from atmosphere should increase. DVS data show that the vapour sorption capacity of our copolymers is low and slightly increases with the polar groups even when exposed to high humidity. Another explanation for the dielectric relaxation in this case may be the ion conductivity. It is known that ppm concentrations of ion impurities are enough to significantly increase the ionic conductivity especially for low viscosity materials.30 The Pt catalyst was not removed from the final copolymers. Since the amount of Pt catalyst used was the same in all the reactions, the strong increase in the dielectric loss for the polymers with high content of polar groups might be due to Pt ions, formed by complexation involving CN groups, instead of Pt(0), as in the case of n-hexene addition. Thus the amount of Pt ions would increase with the number of CN groups. This is supported by the observed “poisoning” effect of allyl cyanide on Pt(dvs) catalyst. Further investigations are required to clarify this hypothesis.
The temperature dependency of dielectric properties was also investigated, within −150 to +60 °C temperature range. In Fig. 8 the ε′ and ε′′ of copolymer B3 at variable frequencies are plotted versus temperature.
The variation of both dielectric permittivity and loss suggest structural relaxation processes. In the dielectric loss curve, a low amplitude peak with maximum at about −130 °C at 1 Hz was assigned to the secondary β relaxation process due to localized motions of side groups. This peak is shifted towards higher temperature as the frequency increases, till approximately −100 °C at 106 Hz, as is characteristic for dielectric relaxation processes.
An α relaxation process associated with the glass transition was observed at −75 °C at 1 Hz, which is very close to the Tg value registered by DSC (−75.6 °C). As expected, this peak shifted to higher temperature with increasing frequency, till −40 °C at 106 Hz. The α relaxation process is also clearly visible as a stepwise increase in the dielectric permittivity (ε′) curve, which is also shifted towards higher temperatures with frequency increase.
At high temperatures and low frequencies, an abrupt increase of ε′ and ε′′ was observed, as a result of enhanced mobility of charge carriers.
Fig. 9 Modification of the IR spectrum (1800–4000 cm−1 region) of B2 stored in different conditions for 6 months. |
This process is accelerated when a solution of DBTDL catalyst in methanol is used, where after 1 h the Si–H absorption band decreased to half as compared to Si–CH3 band. Therefore, the incomplete conversion of the Si–H groups opens up the possibility of using the prepared copolymers as cross-linkers. First experiments show that homogenous thin elastomeric films with increased permittivity and good elastic properties formed from PDMS and copolymers B (Fig. 6S†). Work regarding the preparation and full characterization of such materials will be discussed in a forthcoming publication.
Footnotes |
† This paper is dedicated to the 65th anniversary of “Petru Poni” Institute of Macromolecular Chemistry of Romanian Academy, Iasi, Romania. |
‡ Electronic supplementary information (ESI) available: 1H and 13C NMR spectra, FTIR spectra, DSC curves and photos of cross-linked films. See DOI: 10.1039/c4ra06955b |
This journal is © The Royal Society of Chemistry 2014 |