Yanfeng Wei,
Qiyang Jiang,
Jinmeng Hao and
Jianxin Mu*
College of Chemistry, The Key Lab of High Performance Plastics, Ministry of Education, Jilin University, Changchun 130012, P. R. China. E-mail: jianxin_mu@jlu.edu.cn; Fax: +86-431-88498137; Tel: +86-431-8849813
First published on 19th January 2017
Three series of poly(ether sulfone)s are synthesized from POSS via nucleophilic aromatic substitution polycondensation with different fluoride bisphenols. The structures of the PESs are characterized by IR, NMR and WAXD spectroscopy. The incorporation of POSS and trifluoromethyl into a poly(ether sulfone) matrix at various molar percentages of POSS result in a dramatic decrease in dielectric constant, dielectric loss as well as a significant increase in hydrophobicity of the system. The lowest dielectric constant 2.23 (1 MHz) is obtained at 40% DDSQ–6FPH–PES (molar percent content of DDSQ = 40%). The highest water contact angle 104° is obtained at 20% DDSQ–6AF–PES. Dielectric loss of most synthetic polymers is lower than 0.002. The number of trifluoromethyl groups and the attached position of these to the polymer chain also play essential roles in the dielectric properties, hydrophobicity and thermal properties. The results are discussed and interpreted in detail.
It has been reported that the introduction of bulky trifluoromethyl moieties into the polymer chains can effectively increase solubility and thermal stability, as well as decrease the dielectric constants, water absorption because of the low polarizability and large free volume of C–F bonds.4–8 Maier et al. reported a number of polyimides incorporating trifluoromethyl groups and obtained low dielectric constant (κ) ranging from 2.4 to 2.77.9 Liu et al. demonstrated the preparation of the desired solubility and processability poly(ether ketone)s, where the bulky side group trifluoromethyl was introduced to help to decrease the dielectric constant from 3.3 to 2.69.10 Sipra Ghosh and Susanta Banerjee employed no-planar and asymmetric trifluoromethyl moiety to poly(arylene ether)s (PAEs) to prepare gas separation polymer membranes with higher permeability and permselectivity as well as low dielectric constant values and low water absorption rates.11
However, it is limited to reduce the dielectric constants of the materials just by introducing lower molecular polarizability bulky trifluoromethyl moiety. In view of the dielectric constant of air (κ = 1.01), polyhedral oligomeric silsesquioxane (POSS), as a kind of organic–inorganic nanoporous materials, has attracted attention in preparation to decrease dielectric constant. POSS possesses a cubic octameric molecule with an inner inorganic silicon and oxygen framework, which is externally surrounded by organic functions.12–14 POSS-based hybrids have been widely studied in many other areas of potential applications,15–20 such as optical devices, sensors, barrier materials and catalysts. POSS has been incorporated in polymer matrices, either physical blending or chemical copolymerization, to modify the basic properties of the system.21–24 Double-decker silsesquioxane (DDSQ)25–29 is a kind of admirable POSS with two precise reactive functional groups, which can be applied to synthesize linear and regularity distribution hybrid polymers by incorporating high content of POSS into the main chain.
In this work, three series of new aromatic poly(aryl ether sulfones) (PESs) were prepared from 2OH–DDSQ, difluorophenyl sulfone and three bisphenols containing trifluoromethyl groups, via the nucleophilic aromatic substitution polymerization. The effect of POSS content, the number of trifluoromethyl and the attached position of trifluoromethyl to the chain of polymer on the dielectric property, hydrophobicity and thermal property of the polymers are investigated in this work.
IR (cm−1): 1285 (SO), 1223 (Ar–O–Ar), 1325 (–CF3), 1253, 828 (Si–C), 1087, 482 (Si–O–Si).
IR (cm−1): 1291 (SO), 1230 (Ar–O–Ar), 1332 (–CF3), 1253, 828 (Si–C), 1087, 482 (Si–O–Si).
IR (cm−1): 1285 (SO), 1230 (Ar–O–Ar), 1325 (–CF3), 1253, 828 (Si–C), 1087, 482 (Si–O–Si).
Samples | Inherent viscositya (g dL−1) | Td5b (°C) | Residuec (%) | Tgd (°C) | CA (deg) | Dielectric constante | Dielectric lossf |
---|---|---|---|---|---|---|---|
a Determined at a concentration 0.5 g dL−1 in DMAc at 25 °C.b Temperature at which 5% weight loss was recorded by thermogravimetry at a heating rate of 10 °C min in air.c The yields of degradation residues were obtained at 800 °C in air.d DSC at a heating rate of 10 °C min−1 in nitrogen.e κ was measured at 1 MHz.f Dielectric loss was measured at 1 MHz. | |||||||
PES | 0.95 | 513.2 | 2.65 | 230 | 80 | 3.5 | 0.014 |
PES 2a I | 0.75 | 539.9 | 1.49 | 156.4 | 82.9 | 3.42 | 0.00129 |
PES 2a II | 0.78 | 423.7 | 18.19 | 148.5 | 96.6 | 3.32 | 0.00128 |
PES 2a III | 0.73 | 423.9 | 18.43 | 144.9 | 98.4 | 2.82 | 9.2 × 10−4 |
PES 2a IV | 0.72 | 418.2 | 34.29 | 142.9 | 98.7 | 2.78 | 0.00146 |
PES 2a V | 0.71 | 418.8 | 35.09 | 138.7 | 97.8 | 2.72 | 0.00125 |
PES 2a VI | 0.71 | 375.7 | 36.55 | 137 | 97.5 | 2.68 | 0.02225 |
The chain structure of the polymers was confirmed by FTIR and NMR spectra. The FTIR spectra (Fig. 1) of the polymer films show the characteristic absorption bands around 1285 cm−1 due to sulfonyl groups, around 1230 cm−1 based on aryl ether linkages, and 1325 cm−1 corresponding to trifluoromethyl moieties. 1253 cm−1, 828 cm−1 can be assigned to Si–C band and 1087 cm−1, 482 cm−1 can be attributed to Si–O band of the DDSQ. From the comparison with IR spectra of polymers, DDSQ is confirmed to have been introduced into the main chains of the PESs polymers by covalent bonds successfully. The characteristic absorption peaks at 1087 cm−1, 482 cm−1 (νas, Si–O) manifest that the structure of the DDSQ macromer remains intact.
In the 1H NMR spectra of the polymers, signals of proton at 0.20 ppm, 0.71–2.46 ppm and 3.53 ppm are assigned to the protons of methyl, methylene, and methoxy. The peaks at 6.2–8.2 ppm are assigned to the protons of aromatic ring. A typical set of NMR spectra is shown in Fig. 2, and the spectra agreed with the proposed polymer structure.
The crystallinity of the PESs was evaluated by wide angle X-ray diffraction (WAXD) (Fig. 3). All the polymers exhibited amorphous patterns. DDSQ–3FPH–PESs provide two major diffraction peaks at values of 2θ of 7.18° and 19.29°, corresponding to d-spacings of 1.23 nm and 0.46 nm, respectively;31,32 first is consistent with the size of a POSS unit and it is produced by the crystal structure of the POSS units,33 where a d-spacing of 0.46 nm is the average distance of PES segments. DDSQ–6FPH–PESs provide two major diffraction peaks at values of 2θ of 7.18° and 17.04°, corresponding to d-spacings of 1.23 nm and 0.52 nm, respectively. DDSQ–6AF–PESs provide two major diffraction peaks at values of 2θ of 7.18° and 18.89°, corresponding to d-spacings of 1.23 nm and 0.47 nm, respectively.
The diffuse peak at 7.18° indicates that the DDSQ molecules still retain their nanoscale dimensions in the polymer main chains. The broad peaks demonstrate that there is no crystalline behavior in the polymers, this is ascribed that DDSQ is homogeneous dispersion in the resulting nanocomposite films. The peak intensity at 7.18° was enhanced and half peak width at 7.18° became narrow along with the content of DDSQ increasing, indicating that the chain regularity is strengthened with the content of DDSQ increasing.
Fig. 4 The dielectric constant vs. frequency and molar content of DDSQ for PESs 2a (A), 2b (B), 2c (C); the dielectric constant and dielectric loss vs. POSS molar%. |
Comparing three kinds of polymers, the dielectric constants at the same content of DDSQ represented the following law: DDSQ–3FPH–PESs > DDSQ–6AF–PESs > DDSQ–6FPH–PESs. Due to the larger free volume, lower polarity and lower moisture absorption of the trifluoromethyl groups, the introduction of trifluoromethyl into the polymers could decrease the dielectric constants. The trifluoromethyl content of the DDSQ–3FPH–PESs is lower than DDSQ–6FPH–PESs and DDSQ–6AF–PESs, thus has the relatively high dielectric constants. The free volume of hexafluoroisopropyl group is smaller than bulky trifluoromethyl side group, therefore the κ values of DDSQ–6AF–PESs are higher than DDSQ–6FPH–PESs. The experimental results of XRD can also confirm this conclusion.
Due to the vacant cage-like structure of DDSQ itself, the introduction of DDSQ can reduce the dielectric constant by increasing the free volume; due to the large bulky and low polarity of the trifluoromethyl itself, the introduction of trifluoromethyl can also reduce the dielectric constant. The dielectric constant of PESs which were introduced into the trifluoromethyl and POSS was significantly lower than that of the traditional PESs.
Under the synergy of trifluoromethyl and POSS, the dielectric constant of DDSQ–3FPH–PESs and DDSQ–6AF–PESs decreased gradually along with the content of DDSQ in the main chain increasing. Due to the presence of trifluoromethyl and higher POSS content simultaneously, the lowest dielectric constant was obtained at 80% DDSQ–6AF–PES. Generally, the dielectric constant of DDSQ–6FPH–PESs decreased first and then increased as the content of POSS increased, the lowest κ value was obtained at 40% DDSQ–6FPH–PES. This can be attributed that the dielectric constant can be decreased by the combined consequences of bulky ditrifluoromethyl and POSS and the reduction of the dielectric constant of the bulky ditrifluoromethyl lateral group is larger than that of the POSS.
The dielectric loss of all synthetic copolymers is lower than 0.002 except 0% DDSQ–6FPH–PES (0.013), 60% DDSQ–6FPH–PES (0.003) and 100% DDSQ–PES (0.022) at 1 MHz. This type of polymers is a potential candidate for electronic packaging and large scale integrated circuit.
The contact angle experiments of three series of POSS containing polymers showed that the contact angles increased first and then decreased with the increase of DDSQ content. This is can be attributed that both low polar trifluoromethyl and low surface free energy POSS can help to enhance the hydrophobicity and the enhancement of the hydrophobicity of trifluoromethyl is larger than that of the POSS.
The best hydrophobicity can be obtained by the synergistic effect of the low polarity, low surface free energy of trifluoromethyl and POSS. The largest contact angle of DDSQ–3FPH–PESs is 98.7° at 60% DDSQ–3FPH–PES; the DDSQ–6FPH–PESs is 99.8° at 40% DDSQ–6FPH–PES; the DDSQ–6AF–PESs is 104.8° at 20% DDSQ–6AF–PES. To improve the hydrophobicity was also an effect approach to keep the stability of dielectric property.34,35
The solubility behavior of the polymers in some solvents is listed in Table 4. All of the polymers prepared were soluble at room temperature in most aprotic polar solvents such as NMP, DMAc, DMF and DMSO. The polymers without DDSQ were soluble at room temperature in the less polar solvents such as chloroform and tetrahydrofuran (THF). Due to the presence of CF3 groups in the polymers, the solubility of these polymers was better than (that of) pure PES.
Samples | Inherent viscositya (g dL−1) | Td5b (°C) | Residuec (%) | Tgd (°C) | CA (deg) | Dielectric constante | Dielectric lossf |
---|---|---|---|---|---|---|---|
a Determined at a concentration 0.5 g dL−1 in DMAc at 25 °C.b Temperature at which 5% weight loss was recorded by thermogravimetry at a heating rate of 10 °C min−1 in air.c The yields of degradation residues were obtained at 800 °C in air.d DSC at a heating rate of 10 °C min−1 in nitrogen.e κ was measured at 1 MHz.f Dielectric loss was measured at 1 MHz. | |||||||
PES 2b I | 0.76 | 550.0 | 0.943 | 164.4 | 84.6 | 3.14 | 0.00876 |
PES 2b II | 0.74 | 427.7 | 13.72 | 159.6 | 97.4 | 2.71 | 0.00123 |
PES 2b III | 0.76 | 426.8 | 26.67 | 156.4 | 99.8 | 2.23 | 0.00136 |
PES 2b IV | 0.73 | 422.6 | 32.22 | 154.3 | 99.6 | 2.36 | 0.00274 |
PES 2b V | 0.71 | 434.9 | 35.99 | 148.6 | 98.2 | 2.34 | 0.00167 |
Samples | Inherent viscositya (g dL−1) | Td5b (°C) | Residuec (%) | Tgd (°C) | CA (deg) | Dielectric constante | Dielectric lossf |
---|---|---|---|---|---|---|---|
a Determined at a concentration 0.5 g dL−1 in DMAc at 25 °C.b Temperature at which 5% weight loss was recorded by thermogravimetry at a heating rate of 10 °C min−1 in air.c The yields of degradation residues were obtained at 800 °C in air.d DSC at a heating rate of 10 °C min−1 in nitrogen.e κ was measured at 1 MHz.f Dielectric loss was measured at 1 MHz. | |||||||
PES 2c I | 0.81 | 551.2 | 0.753 | 170.7 | 95.5 | 3.34 | 0.00118 |
PES 2c II | 0.79 | 452.5 | 12.66 | 164.6 | 104.8 | 2.8 | 0.00124 |
PES 2c III | 0.81 | 444.5 | 23.22 | 162.2 | 103.8 | 2.7 | 0.00192 |
PES 2c IV | 0.79 | 422.4 | 30.61 | 158.2 | 101.3 | 2.67 | 0.00172 |
PES 2c V | 0.75 | 436.3 | 34.93 | 155.8 | 100.5 | 2.43 | 0.00121 |
Samples | NMP | DMAc | DMSO | DMF | THF | Chloroform | Acetone |
---|---|---|---|---|---|---|---|
Solubility under a mass of liquid: 0.1 g mL−1; (++) soluble at room temperature; (−−) insoluble even on heating; (+−) partially soluble or swelling on heating. | |||||||
PES | ++ | ++ | +− | +− | −− | −− | −− |
PES 2a I | ++ | ++ | ++ | ++ | ++ | ++ | ++ |
PES 2a III | ++ | ++ | ++ | ++ | −− | −− | −− |
PES 2a V | ++ | ++ | ++ | ++ | −− | −− | −− |
PES 2a VI | ++ | +− | +− | +− | −− | −− | −− |
PES 2b I | ++ | ++ | ++ | ++ | ++ | ++ | ++ |
PES 2b III | ++ | ++ | ++ | ++ | −− | −− | −− |
PES 2b V | ++ | ++ | ++ | ++ | −− | −− | −− |
PES 2c I | ++ | ++ | ++ | ++ | ++ | ++ | ++ |
PES 2c III | ++ | ++ | ++ | ++ | −− | −− | −− |
PES 2c V | ++ | ++ | ++ | ++ | −− | −− | −− |
The Tg of the three series of DDSQ–CF3–PESs copolymers decrease with the increase of POSS content. This is attributed to the increase of free volume through the introduction of bulky CF3 and the cage-like structure DDSQ.
Comparing three kinds of polymers, the Tg at the same content of DDSQ represented the following law: DDSQ–6AF–PESs > DDSQ–6FPH–PESs > DDSQ–3FPH–PESs. On the one hand, the free volume of hexafluoroisopropyl group is smaller than bulky trifluoromethyl side group, therefore Tg of DDSQ–6AF–PESs are higher than DDSQ–6FPH–PESs and DDSQ–3FPH–PESs; on the other hand, the segment movement of 3,5-ditrifluoromethylphenyl is harder than trifluoromethylphenyl, resulting in the reduction of free volume and the increase of Tg.
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