铁电共聚物VDF／TrFE的低温低频介电松弛

在低温低频下用介电松弛方法研究了液氮淬火，熔融慢冷和热处理结晶铁电共聚物ＶＤＦ（７３）／ＴｒＦＥ（２７）的分子运动特征，随结晶度升高，居里点温度降低，铁电－顺电相变区的介电常数增大。室温以下共聚物的频率谱由低频和高频两部分组成。低频部由非晶工区被冻结分子链段的微布朗运动贡献。高频部则由晶区和非晶区分子链段较小尺度的局域运动产生。由两个Ｃｏｌｅ－Ｃｏｌｅ函数对频率谱进行分峰拟合并根据ＷＬＦ方程和Ａｒ     

VDF（81）／TeFE（19）共聚物的低温低频介电弛豫

用经过改进的介电弛豫谱仪测得不同结晶度的铁电共聚物ＶＤＦ（８１）／ＴｅＦＥ（１９）在－１２０－４０℃、１０－２－１０４ＨＺ范围内的复介电常数．低温介电弛豫过程显示室温以下共聚物的频率谱由低频和高频两部分叠合而成．低频部分符合ＷＬＦ方程，由非晶区被冻结分子链段的微布朗运动贡献；高频部分遵从Ａｒｒｈｅｎｉｕｓ规律，由晶区和非晶区分子链段较小尺度的局域运动产生．结果说明共聚物的玻璃化转变温度是－５２℃，局域弛豫活化能为３７．７ｋＪ／ｍｏｌ．     

淬火温度对聚偏氟乙烯形态结构的影响

用透射电子显微镜（ＴＥＭ）和傅里叶交换红外光谱（ＦＴＩＲ）等方法研究了结晶温度对聚偏氟乙烯（ＰＶＦ２）晶相结构的影响．结果表明，从ＰＶＦ２熔体高速淬火到较低温度等温结晶可直接生成β相结晶，临界淬火温度为３０℃．淬火温度在４０—７０℃时，α和β相共存．当淬火温度较高时（８０—１５０℃），生成α相结晶．在淬火温度高于１６５℃时，则得到ＰＶＦ２的γ相结晶．在临界温度以下淬火的ＰＶＦ２薄膜含有β相微晶，而高于临界淬火温度时则生成α相或γ相的片晶或球晶结构．     

VDF（81）／TeFE（19）共聚物的低温低频介电驰豫

用经过改进的介电驰豫谱仪测得不同结晶度的铁电共聚物ＶＤＦ（８１）／ＴｅＦＥ（１９）在－１２０－４０℃、１０＾－２－１０＾４－Ｈｚ范围内的复介电常数，低温介电驰豫过程显示室温以下共聚物的频率谱由低频和高频两两部分叠合而成，低频部分ＷＬＦ方程，收非晶区被冻结分子链段的微布朗运动贡献；高频部分遵从Ａｒｒｈｅｎｉｕｓ规律，由晶区和非晶区子链段较小尺度的局域运动产生，结果说明共聚物的玻璃化转化变温度是－５２     

聚偏氟乙烯共混体系的压电性及其分子运动——Ⅱ.PVDF与 P(VDF-HFE)以及PVDF与P(VDF-TFE)的共混体系

本文研究了 PVDF-P(VDF-HFE)以及 PVDF-P(VDF-TFE)共混体系的压电、介电、力学松弛谱。其松弛转变过程基本与 PVDF 的相似。α,β,γ压电松弛峰分别位于40～120℃,-40℃,-85℃附近。实验结果表明后一体系的压电性大于前一体系的。同时,PVDF-P(VDF-TFE)的压电性也大于PVDF-PMMA 共混体系的。选择第二组分时,以介电常数高,模量小而本身又具有压电性的,更有助于共混薄膜压电性的提高。在同样的极化条件下,经拉伸的 P(VDF-TFE)薄膜,其压电性大于未经拉伸的薄膜,这表明分子的取向对薄膜的压电性也有影响。TSC 表明,42℃的松弛峰与晶区表面捕获的空间电荷有关,对压电性也有一定的贡献。     

聚（β－羟基丁酸酯）／聚双酚A羟基醚共混体系相容性及结构的研究

ＤＳＣ和ＦＴＩＲ测试表明，结晶／非晶共混体系聚（β－羟基丁酸酯）（ＰＨＢ）／聚双酚Ａ羟基醚（ＰＢＨＥ）是部分相容的．熔融结晶退火可以大大提高共混物的结晶度，增加其相容性，７５／２５组分ＰＨＢ相结晶度最大，５０／５０组分（０２０）、（１３０）晶面微晶尺寸最大．ＳＡＸＳ研究表明，纯ＰＨＢ的中间层约为１．５ｎｍ，片层厚约４．０ｎｍ；共混物的中间层在２．０ｎｍ左右，片层厚在５．０—７．２ｎｍ之间，５０／５０组分片层最厚．７５／２５组分晶相和非晶相的密度差最大．     

聚（β－羟基丁酸酯）／聚双酚A羟基醚共混体系相容性及结构的研究

ＤＳＣ和ＦＴＩＲ测试表明，结晶／非晶共混体系聚（β－羟基丁酸酯）（ＰＨＢ）／聚双酚Ａ羧基醚是部分相容的。熔融结晶退火可以大大提高共混物的结晶度，增加其相容性。７５／２５组分ＰＨＢ相结晶度最大，５０／５０组分晶面微晶尺寸最大。     

超速升温对玻璃态聚偏氟乙烯结晶的影响

我们曾研究超速淬火温度对聚偏氟乙烯(PVF_2)薄膜结晶结构的影响,在不同温度下淬火可分别得到α、β和γ三种晶型结构。本工作从非晶的玻璃态PVF_2出发,通过超速升温的方法,进一步研究结晶温度对PVF_2晶型结构的影响。     

非晶态聚对苯二甲酸乙二酯等温结晶的介电研究

非晶态PET的介电性质温度谱除α_a松弛和β松弛外,在120—130℃之间由于在升温过程中试样的结晶出现一个损耗峰。比较非晶态试样与结晶后试样介电常数ε′和介电损耗ε″的差别,可在97—113℃温度下用ε′和ε″来表征非晶态PET的等温结晶过程。在结晶的初期,ε′随时间的变化符合Avrami方程,即(ε′(t)-ε′(∞))/(ε′(0)-ε′(∞))=exp(-Kt~n)。在结晶的后期,由介电性质的频率谱Cole-Cole图观察介电松弛强度△ε和β参数在结晶过程的变化。     

聚偏氟乙烯基含氟聚合物介电和储能研究进展

聚偏氟乙烯（PVDF）和偏氟乙烯（VDF）／三氟乙烯（TrFE）二元共聚物以其优异的铁电、压电性能而备受关注。近年来,该类聚合物经物理／化学改性后表现出非常优异的介电、储能性能,尤其在高储能放电电容器领域被寄予厚望。经分子组成优化和挤出拉伸处理的PVDF基含氟聚合物在室温下具有高介电常数（12～60）,高击穿电场强度,...     

The relationship between chemical structure and viscoelastic properties of linear aliphatic polyesters

The effects of Chemical structure on the molecular motions in linear aliphatic polyesters have been investigated with a free-oscillation torsion pendulum. Broad-line NMR provided supplementary information. In the γ relaxation which corresponds to the local-mode motions of main chains in the noncrystalline region, the polyesters which are composed of two methylene units in the diol part of the chemical repeat unit showed an extremely asymmetric loss curve with a relatively high-loss peak temperature compared with that of the other polyesters. In addition to the two relaxations (β,γ) which have been observed in earlier dielectric measurements, a new relaxation (α) was found on the high-temperature side of the glass transition of the polyesters. The α relaxation was assigned to molecular motions of methylene segments in the crystalline region. The α and β relaxations of the two-dimensional series are situated close to the temperatures found for other polyesters with rather long methylene sequence in the chemical repeat unit. The results were explained in terms of a difference on the chain mobility in the noncrystalline regions which may be related to the difference of chemical structure of the polyesters.     

四氟乙烯-全氟4-甲基-3,6-二氧杂△~7辛基磺酰氟共聚物的分子运动

本工作用振簧仪,在-150—80℃范围内,测试了四氟乙烯-全氟4-甲基-3,6-二氧杂△~7辛基磺酰氟共聚物的动态力学性能。样品是含有不同侧基数目的部分结晶共聚物。观察到四个松弛过程,按温度下降次序记为α、γ_1-、γ_2-、γ_3-。α峰(室温附近)系玻璃化转变。γ_1峰(-50℃,～215Hz)为主链有阻碍的短链段分子运动。γ_2-峰(-60℃,～230Hz)为侧基的分子运动。γ_3-峰(-77℃,～260Hz)为的链段运动,并且γ_3-峰的强度随结晶度增加而增强。     

STUDIES ON THE CHAIN STRUCTURAL EFFECT OF PVDF AND VDF (52)/TrFE(48) COPOLYMER BY MEANS OF THE METHOD OF DIELECTRIC RELAXATION

Through improvements on a fully commercial and automatic system measuring frequency andtemperature spectra of the complex elastic, dielectric, and piezoelectric constants of polymerfilms, the precision for measuring complex dielectric constants achieved 2‰ from original 1%.The complex dielectric constants of PVDF, VDF (95 )/VF (5), VDF (52)/TrFE (48) and VDF(47. 5)/TrFE(47. 5)/HeFP (5) over a range of-120-140℃, 10-2-10~4Hz were measured bythe described system. The diminution of chain regularity due to 5mol% vinyl fluoride in the chainof PVDF led to disappearing of α-relaxation and increase in T_g (3℃) of VDF (95)/VF (5).Because of the spatial impediment of 5mol% HeFP in copolymer chain, the Curie point of VDF(52)/TrFE(48) decreased by 30℃ and T_g by 3℃. The behavior of dielectric relaxation indicatedthat 5mol% vinyl fluoride and HeFP made the relaxation strength of noncrystalline regionreduced, the activation energy of local relaxation increased and the relaxation time prolonged respectively.     

乙烯-丙烯酸共聚物非晶区结构和分子运动的固体核磁共振研究

利用固体高分辨1 3CCP MAS和变温固体质子宽线技术对乙烯 丙烯酸共聚物 (EAA)非晶区的结构和分子运动进行了研究 ,结果发现 ,非晶区中羧基之间可以形成氢键 ,其数量随着共聚物中丙烯酸共聚单体含量的增加而增加 ,使得共聚物中非晶区分子运动能力随非晶区相对含量的增加而减弱 ,这是一种与一般的乙烯共聚物相反的变化趋势 .通过交叉极化方法间接测量了非晶区中乙烯链段的1 H自旋 自旋弛豫时间 (T2 ) ,表明非晶区中乙烯链段的运动同样受到氢键的束缚 .随着温度的升高 ,羧基之间的氢键发生解离 ,非晶区的柔性增强     

The dielectric properties of dry and water-saturated nylon-12

The dielectric relaxation of 30% crystalline Nylon-12 of molecular weight 20,000 has been studied at frequencies from 12 Hz to 0.1 MHz and temperatures from 77 to 375 K, and the effect of water on the relaxation spectra has been investigated. Absorbed water increases both the rate and the intensity of both its α-and β-relaxation processes and increases the rate but decreases the intensity of its γ-relaxation process. These results are interpreted in terms of the hydrogen bonding effects of water on localized motions of dipoles in Nylon-12. The relatively large half-width of the α-relaxation, which becomes better resolved at high temperatures, is attributed mainly to the random distribution of crystalline regions in the polymer. It is suggested that water lowers the steric hindrance for the localized mode of dipolar reorientation and causes a redistribution of local sites such that the β-relaxation process grows at the expense of the γ-process.     

Internal motions in an alternating copolymer of ethylene and tetrafluoroethylene

Internal motions in an alternating copolymer of ethylene and tetrafluoroethylene were investigated by dynamic mechanical and dielectric measurements and by nuclear magnetic resonance. At 1 Hz the α, β, and γ relaxations were observed at 110, ?25, and ?120°C in a quenched sample. The activation energy was 76 kcal/mole for the α relaxation and 10.6 kcal/mole for the γ relaxation. These relaxations are attributed to the motion of long and short segments in the amorphous regions, respectively. The β relaxation, which was observed only in the dynamic mechanical experiments, appears to occur in the crystalline regions. The copolymer is isomeric with poly(vinylidene fluoride), but it has a higher melting point and a much lower dielectric loss.     

Molecular dynamics of amorphous/crystalline polymer blends studied by broadband dielectric spectroscopy

The molecular dynamics of poly(vinyl acetate), PVAc, and poly(hydroxy butyrate), PHB, as an amorphous/crystalline polymer blend has been investigated using broadband dielectric spectroscopy over wide ranges of frequency (10⁻² to 10⁵ Hz), temperature, and blend composition. Two dielectric relaxation processes were detected for pure PHB at high and low frequency ranges at a given constant temperature above the T_g. These two relaxation peaks are related to the α and α′ of the amorphous and rigid amorphous regions in the sample, respectively. The α′-relaxation process was found to be temperature and composition dependent and related to the constrained amorphous region located between adjacent lamellae inside the lamellar stacks. In addition, the α′-relaxation process behaves as a typical glass relaxation process, i.e., originated from the micro-Brownian cooperative reorientation of highly constraints polymeric segments. The α-relaxation process is related to the amorphous regions located between the lamellar crystals stacks. In the PHB/PVAc blends, only one α-relaxation process has been observed for all measured blends located in the temperature ranges between the T_g’s of the pure components. This last finding suggested that the relaxation processes of the two components are coupled together due to the small difference in the T_g’s (ΔT_g = 35 °C) and the favorable thermodynamics interaction between the two polymer components and consequently less dynamic heterogeneity in the blends. The T_g’s of the blends measured by DSC were followed a linear behavior with composition indicating that the two components are miscible over the entire range of composition. The α′-relaxation process was also observed in the blends of rich PHB content up to 30 wt% PHB. The molecular dynamics of α and α′-relaxation processes were found to be greatly influenced by blending, i.e., the dielectric strength, the peak broadness, and the dielectric loss peak maximum were found to be composition dependent. The dielectric measurements also confirmed the slowing down of the crystallization process of PHB in the blends.     

Melting and internal motion in highly alternating copolymers of ethylene and carbon monoxide

The melting point of the 1:1 copolymer of ethylene and CO is 244°C. It falls rapidly as the percent CO is reduced indicating that the heat and entropy of fusion are 0.60 kcal and 1.15 e.u./mol of chain atoms, respectively. These are lower than the values for polyethylene. Dynamic mechanical measurements showed loss peaks at ?100° and 25°C. The low temperature γ-relaxation which is also seen in dielectric data appears to be a local mode relaxation with an activation energy of about 12 kcal/mol. The room temperature relaxation is associated with a large decrease in the modulus and a large increase in the dielectric constant. It is probable that the low entropy of fusion is due in part to extensive motion in the crystal.     

Dielectric and dynamic mechanical relaxation studies on poly(aryl ether ketone)s

The relaxation behavior of four amorphous poly(aryl ether ketone)s was investigated using dielectric relaxation spectroscopy and dynamic mechanical analysis. The temperature dependence of the relaxation times of the glass transition process and the cooperative nature of this process were unaffected by changes in polymer structure. The temperature location of the loss peaks for all polymers progressed smoothly between the low frequency of the mechanical measurements and the higher frequencies of the dielectric probe. Differences were observed in mechanical activation energy and dielectric relaxation strength for one polymer which contained a significant concentration of meta linkages, compared with the para-linked polymers, while relaxation broadness was generally greater in the dynamic mechanical mode. Changes in chemical structure had little effect on the shape, intensity, and location of the β-relaxation peak, the main observation being that the Arrhenius activation energy measured by dynamic mechanical analysis was significantly higher than that calculated from the dielectric data. The dielectric β-relaxation was sensitive to absorbed moisture. © 1998 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 36: 851–859, 1998     

Broadband dielectric spectroscopy of the inter- and intramolecular dynamics of a series of random polyester copolymers

Broadband dielectric spectroscopy (1–10⁶ Hz, 183–423 K) and differential scanning calorimetry are employed to analyze the inter- and intramolecular dynamics of a series of random copolymers based on poly(ethylene terephthalate) and poly(1,4-cyclohexylene dimethylene terephthalate). In addition to an interfacial relaxation (α*-process), three dielectric relaxation processes are observed: The α-relaxation (“dynamic glass transition”) and two secondary relaxations (β- and β*-relaxations). The α-relaxation depends sensitively on the composition of the copolymer and shows a rapid slowing down with increasing content of cyclohexylene dimethylene (CHDM) linkages. Besides the β-relaxation, attributed to local motion of the ester group, an additional process (β*-relaxation) is observed on introducing the CHDM linkages. Increasing the content of the latter reduces the strength of the β-relaxation strongly and increases its activation energy by more than 30%. This proves that owing to interactions between the cylohexylene rings and the ester group the β-relaxation no longer has local character only. Received: 28 September 2000 Accepted: 29 January 2001