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1.
聚苯醚磺酸锂与聚乙二醇共混体系的离子导电性   总被引:2,自引:1,他引:1  
本文研究影响聚乙二醇(PEG)增塑聚苯醚磺酸锂(SPPOLi)电导率的各种因素,如摩尔比,及PEG分子量等。SPPOLi/PEG具单离子导体的特征,试样最高室温电导可达10^-5S/cm。  相似文献   

2.
为改善聚苯醚磺酸锂(SPPOLi)的导电性能,将聚酷酸乙烯酯(PVAc)与之共混,X-射线衍射分析表明,PVAc可降低SPPOLi凝聚结构的有序程度;发现共混后电导率有了较大提高,共混物的电导对温度的依赖关系不符合阿仑尼马斯方程;同时,共混物仍保持了单离子传导性.  相似文献   

3.
本文为提高聚苯醚磺酸锂(SPPOLi)的导电性能, 将聚乙二醇(PEG)与之共混,DSC分析发现SPPOLi的玻璃化转变温度随PEG的加入有所下降, 并且对于高磺化度的样品下降更为明显; X射线衍射表明, PEG可降低SPPOLi凝聚结构的有序程度;发现通过共混, 电导率有了较大提高, 并且仍保持了单离子的传导性。  相似文献   

4.
研究了同时具有最高临界互溶温度和最低临界互溶温度的羧化聚苯醚/聚苯乙烯共混体系随退火温度的变化而发生的相形态结构的变化.研究了此共混体系的相分离机理.并发现了此特殊共混体系低温和高温区的相分离机理是不同的.从分子的结构和分子间特殊相互作用上探讨了此共混体系产生特殊相行为的原因.  相似文献   

5.
经共聚改性的聚苯乙烯PS(OH)与聚甲基丙烯酸丁酯PBMA形成的互溶体系具有LCST行为。由于体系的玻璃化温度较高。分相温度与玻璃化温度接近。使分相时的浊点温度受升温速率影响很大,以致浊点曲线与相平衡曲线有一定的差距。本文以邻苯二甲酸二丁酯DBP为增塑剂加入PS(OH)/PBMA共混体系中,在一定的升温速率下测浊点温度,并对增塑剂作零浓度的外推,由此得到的浊点曲线与相平衡曲线完全一致。证实了增塑剂法的可靠性。加入增塑剂后浊点温度随升温速率变化平缓,更接近相平衡点,显示了增塑剂法的有效性。  相似文献   

6.
本工作合成了聚甲基丙烯酸齐聚氧化乙烯酯和聚甲基丙烯酸己磺酸锂两系列聚合物,研究共聚物结构对共混物的相容性和锂离子导电性的影响.结果表明,共混物的相容性是决定离子电导率的主要因素;共混物内锂离子传导发生在非晶区,聚合物的链段运动是离子传导的主要推动力.  相似文献   

7.
本工作合成了聚甲基丙烯酸齐聚氧化乙烯酯和聚甲基丙烯酸己磺酸锂两系列聚合物,研究共聚物结构对共混物的相容性和锂离子导电性的影响.结果表明,共混物的相容性是决定离子电导率的主要因素;共混物内锂离子传导发生在非晶区,聚合物的链段运动是离子传导的主要推动力.  相似文献   

8.
采用DSC方法研究了聚苯乙烯(PS)和苯甲酰化聚苯醚(APPO)共混体系的相容性.相容共混体系Gordon-Taylor方程K参数随苯甲酰化程度(取代度)增加而变小,其玻璃化转变区随取代度增加而变宽,取代度大于76mol%时,共混物呈现双玻璃化转变.APPO/PS共混体系热诱导相图同时存在LCST和UCST现象,且相行为是可逆的.  相似文献   

9.
采用DSC方法研究了聚苯乙烯(PS)和苯甲酰化聚苯醚(APPO)共混体系的相容性.相容共混体系Gordon-Taylor方程K参数随苯甲酰化程度(取代度)增加而变小,其玻璃化转变区随取代度增加而变宽,取代度大于76mol%时,共混物呈现双玻璃化转变.APPO/PS共混体系热诱导相图同时存在LCST和UCST现象,且相行为是可逆的.  相似文献   

10.
采用傅立叶变换红外光谱对PPO/PS共混合金样品的组成进行了定量分析.以1 305 cm-1峰和699 cm-1峰分别作为聚苯醚和聚苯乙烯的定量吸收峰,并将其峰面积之比作为定量分析的基础.利用郎伯-比耳定律的理论建立了定量工作曲线,可满足PPO(或者PS)在5%~95%之间的PPO/PS共混合金样品组成的定量分析.分别采用红外光谱和核磁共振对样品进行定量分析,结果显示,两种方法定量结果的相对偏差在5%以内.红外定量方法测定结果的相对标准偏差小于2.5%(n=6).该方法可快速、准确地运用于PPO/PS共混合金样品的红外定量分析.  相似文献   

11.
In the present paper, the structure and conductivity for the complex of sulfonated poly(phenylene oxide) lithium (SPPOLi) and poly(ethylene oxide) (PEG) were studied. Glass transition temperature change determined by differential scanning calorimeter analysis desmonstrated that the two components had some compatibility. X-ray diffraction showed that PEG could decrease the regularity of SPPOLi to some extent. The compatibility and PEG's effect on the regularity may be due to the interaction between the lithium ions of SPPOLi and the oxygen atoms of PEG. Under polarization by electric field, the bands between lithium ions and sulfonation groups relaxed. Meanwhile, the complexation of oxygen atoms could enhance the dissociation of the polymeric lithium salts. Then lithium ions were transported in the process of alternate complexing and decomplexing. The action between lithium ions and oxygen atoms could explain the improvement on the conductivity of SPPOLi.  相似文献   

12.
    
A simple method to determine polymer blend compositions from their Raman spectra is presented. The method is based on expanding linearly the experimentally measured Raman spectrum of the blend, in terms of Raman spectra of pure components. A smooth function has also been included in the linear expansion to take into account the fluorescence interference, inherent to Raman spectroscopy. The coefficients of the linear expansion that give the best fit to the experimentally measured Raman spectrum of the blend are found by using a standard method of parameter estimation (Marquardt–Levenberg). These coefficients are directly related to the blend composition via a simple calibration procedure. Unlike standard methods of processing Raman spectra as deconvolution and curve‐fitting—which use Gaussian and/or Lorentzian functions to approximate the spectrum bands—the proposed method does not require either baseline correction or previous knowledge of peak parameters. Also, this method requires less CPU time than deconvolution and curve‐fitting procedures, and it is easy to automate. The proposed method has been applied to blends made out of two polymers: Polystyrene (PS) and poly(phenylene oxide) (PPO), to test its precision and consistency. Excellent agreement was found between calculated and expected blend compositions. Also, the reconstructed spectra agree very well with the experimentally measured blend spectra. © 2000 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 38: 1013–1023, 2000  相似文献   

13.
Thermal and dynamic mechanical properties of PES/PPS blends   总被引:1,自引:0,他引:1  
Blends of poly(ether-sulfone) (PES) and poly(phenylene sulfide) (PPS) with various compositions were prepared using an internal mixer at 290°C and 50 rpm for 10 min. The thermal and dynamic mechanical properties of PES/PPS blends have been investigated by means of DSC and DMA. The blends showed two glass transition temperatures corresponding to PPS-rich and PES-rich phases. Both of them decreased obviously for the blends with PES matrix. On the other hand, Tg of PPS and PES phase decreased a little when PPS is the continuous phase. In the blends quenched from molten state the cold crystallization temperature of PPS was detected in the blends of PES/PPS with mass ratio 50/50 and 60/40. The melting point, crystallization temperature and the crystallinity of blended PPS were nearly unaffected when the mass ratio of PES was less than 60%, however, when the amount of PES is over 60% in the blends, the crystallization of PPS chains was hindered. The thermal and the dynamic mechanical properties of the PPS/PES blends were mainly controlled by the continued phase. This revised version was published online in August 2006 with corrections to the Cover Date.  相似文献   

14.
水基微乳液;溶剂极性对磺化聚苯醚微乳液相反转的影响  相似文献   

15.
通过溶解―铸膜法制备聚乙烯醇(PVA)-KOH-H2O碱性聚合物电解质膜。向聚合物中添加增塑剂丙三醇(GROL)和碳酸丙烯酯(PC)来提高离子电导率。X射线晶体衍射分析(XRD)结果表明,添加增塑剂未改变聚合物的物相结构,薄膜仍主要为不定形态。差示扫描热分析(DSC)结果显示,添加增塑剂后聚合物电解质膜的玻璃化转变温度降低,促进了电解质膜向不定形态转变。电解质膜室温离子电导率随增塑剂添加而增大,增塑剂超过一定量后离子电导率开始下降。PC对提高离子电导率的作用优于GROL。循环伏安测试结果显示,电解质膜的电化学稳定性窗口随增塑剂的添加而有所变窄,但仍显示了较好的电化学稳定性。  相似文献   

16.
To obtain thermally stable and mechanically strong sodium and lithium conducting polymers, we prepared Na+ and Li+ poly(phenylene terephthalamide sulfonate salts) (MW ~ 5500). We also synthesized oligo(ethylene oxide) (3, 5, or 7 units of ethylene oxide) substituted ethylene carbonate and poly[oxymethylene-oligo(oxyethylene)]. These are high boiling point liquids with high dielectric constants as well as metal chelating properties. Polyelectrolyte systems were prepared by mixing Na+ or Li+ poly(phenylene terephthalamide sulfonate) salts with various amounts of modified ethylene carbonate and/or poly[oxymethylene-oligo(oxyethylene)]. Films (0.1–0.5 mm thick) obtained from the blends were found to have considerable mechanical strength; forming free standing films. The ionic conductivities of the Na+ and Li+ polyelectrolyte systems were 10?6?10?5 S/cm at 25°C. Thermal properties of these blend systems were investigated in detail. © 1994 John Wiley & Sons, Inc.  相似文献   

17.
    
Summary: Polymer blends consisting of linear poly(phenylene sulfide) (PPS) and hyperbranched PPS (HPPS) were obtained in melt. The solid-state properties of PPS and their blends were investigated by scanning electron microscopy (SEM), thermogravimetric analyzer (TGA), extraction measurement, differential scanning calorimetry (DSC) and dynamical mechanical analysis (DMA). Blends prepared by melt mixing turned out to be reactive as shown by the TGA and extraction measurement. SEM indicated that no phase separation occurs in PPS/HPPS blends. The degree of crystallization of the blends decreased with increasing HPPS content. Both the storage modulus and loss modulus increased as HPPS content increasing.  相似文献   

18.
新型单离子聚醚/聚氨酯固体电解质制备及其离子导电性   总被引:1,自引:0,他引:1  
磺化聚醚;离子电导率;聚合物;新型单离子聚醚/聚氨酯固体电解质制备及其离子导电性  相似文献   

19.
    
“Radical‐controlled” oxidative polymerization of phenol (p‐1) by (1,4,7‐triisopropyl‐1,4,7‐triazacyclononane)copper(II) catalyst was performed and compared with that of 4‐phenoxyphenol (p‐2) in detail. Although the coupling selectivity for p‐1 seemed to be controlled by the catalyst, the C? C coupling, which was excluded completely for p‐2, occurred to some extent. The initial reaction rate of p‐1 was much smaller than that of p‐2, leading to the difference of polymerization behavior between p‐1 and p‐2. The rate‐determining step would be the coupling of controlled radicals species from the ESR measurement of the reaction mixture. The polymer resulting from p‐1 consisted mainly of phenylene oxide units, but had no crystallinity in contrast to the crystalline polymer from p‐2. However, the present polymer showed the highest thermal stability in the polymers obtained by oxidative polymerization of p‐1. © 2005 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem 43: 1955–1962, 2005  相似文献   

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