共查询到17条相似文献,搜索用时 46 毫秒
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不同分子量尼龙1010的结晶与熔融*朱诚身王经武王友文杨桂萍(郑州大学材料工程系郑州450052)陈玉莫志深(东北师范大学分析测试中心长春130024)(中国科学院长春应用化学研究所长春130022)关键词尼龙1010,分子量,结晶,熔融*1994_... 相似文献
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尼龙1010非等温结晶动力学与机理研究 总被引:3,自引:0,他引:3
尼龙1010非等温结晶动力学与机理研究朱诚身,王经武,李卓美(郑州大学材料工程系郑州450052)(中山大学高分子研究所广州510275)关键词尼龙1010,非等温结晶动力学,结晶机理,动力学结晶能力尼龙1010的结晶动力学,无论是等温还是非等温,研... 相似文献
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碳纤维-尼龙1010界面形态的研究 总被引:4,自引:2,他引:4
通过偏光显微镜,研究了碳纤维-尼龙1010的界面形态,发现石墨、高模量碳纤维(M40)诱发尼龙1010形成横晶的能力大于高强度、中强度碳纤维;界面横晶形态强烈地依赖于结晶温度。 相似文献
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From Wide-Angle X-ray Scattering (WAXS) pattern of uniaxially orientated fibers, the crystal structure of Nylon-1010 was determined. The Nylon-1010 crystallizes in the triclinic system, with lattice dimensions: a=4.9A, b=5.4A, c=27.8, α=49 °, β=77 °,γ=63.5 °, the unit cell contains one monomeric unit and the space group is P. The degree of crystallinity of polymer was deter mined as about 60%, using Ruland's method.The structures of Nylon-1010 with different draw ratio have been investigated by using Small-Angle X-ray Scattering (SAXS). The results indicate that the draw ratio of samples has a significant effect on microstructure of Nylon-1010. The long period and thickness of amorphous layer obviously increase but the invariant, average lameUar and interphase zone show almost independent of draw ratio, long period increases because amorphous layer increases with draw ratio. The electron density fluctuation values increased with draw ratio, but inner surface O_s is drecreased. 相似文献
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热致液晶共聚酯/Nylon-1010共混物的研究 总被引:4,自引:0,他引:4
利用偏光显微镜(PLM),差示扫描量热计及广角X-射线衍射等手段研究了热致液晶共聚酯/Nylon-1010共混体系.发现当热致液晶共聚酯(HTH10)含量达到30%时共混物微结构与纯HTH10相似.尼龙-1010的结晶度先是随HTH10含量增加而增加,随后又随之下降,但其结晶温度却随HTH10加入而单调下降,共混物的熔融热焓△Hm在HTH10含量为30%时与计算值有较大的偏差,广角X-射线衍射结果表明,此时共混物结构发生了较为明显的变化,两组份之间在此时存在一定的相互作用. 相似文献
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Films obtained via drying a polymeric latex dispersion are normally colloidal crystalline where latex particles are packed into a face centered cubic (fcc) structure.Different from conventional atomic crystallites or hard sphere colloidal crystallites,the crystalline structure of these films is normally deformable due to the low glass transition temperature of the latex particles.Upon tensile deformation,depending on the drawing direction with respect to the normal of specific crystallographic plane,one ... 相似文献
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Films obtained via drying a polymeric latex dispersion are normally colloidal crystalline where latex particles are packed into a face centered cubic (fcc) structure. Different from conventional atomic crystallites or hard sphere colloidal crystallites, the crystalline structure of these films is normally deformable due to the low glass transition temperature of the latex particles. Upon tensile deformation, depending on the drawing direction with respect to the normal of specific crystallographic plane, one observes different crystalline structural changes. Three typical situations where crystallographic c-axis, body diagonal or face diagonal of the fcc structure of the colloidal crystallites being parallel to the stretching direction were investigated. Tilting angle and d-spacing of several crystallographic planes as a function of draw ratio at each situation were derived. Experimental evidences for such relationships were also given by considering in-situ synchrotron small angle X-ray scattering data of a typical latex film during stretching. It turns out that the experimental results are fully in accordance with the mathematical calculations. 相似文献
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Jun-tingXu Bo-taoLi Zhi-qiangFan 《高分子科学》2004,(3):279-287
The fractions of one metallocene-based (mPE) and one conventional (znPE) ethylene-butene copolymer eluted at 80-82℃ from temperature rising elution fractionation were selected for DSC and time-resolved small angle X-ray scattering (SAXS) and wide angle X-ray scattering (WAXS) characterization. The DSC and WAXS results show that two crystal structures exist in both mPE and znPE: structure A with higher melting temperature and structure B with lower melting temperature. It was found that original znPE (s-znPE) contains more highly ordered structure A than original mPE (s-mPE) in spite of the higher comonomer content of znPE. Another structure C is also identified because of higher crystallinity measured by WAXS than by DSC and is attributed to the interfacial region. The SAXS data were analyzed with correlation function and two maxima were observed in s-mPE and s-znPE, in agreement with the conclusion of two crystal populations drawn from DSC and WAXS results. These two crystal populatiorts have close long periods in s-mPE, but very different long periods in s-znPE. In contrast, freshly crystallized mPE and znPE (f-mPE and f-znPE) contain only a single crystal population with a broader distribution of long period 相似文献