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1.
尼龙-1010结晶结构   总被引:11,自引:4,他引:11  
用WAXD方法测定了Nylon-1010为三斜晶系结晶结构;α=4.9(?),b=5.4(?),c=27.8(?),α=49°,β=77°,γ=63.5°,每个聚合物单胞含有一个重复单元,空间群为P(?)。模压试样用Ruland方法分析结晶度为60%。以上。电子密度相关函数法分析了SAXS现象,求得了Nylon-1010结晶片层厚度、过渡层厚度、长周期、比内表面及电子密度差。  相似文献   

2.
PVA/PVP共混物的SAXS研究   总被引:1,自引:0,他引:1  
聚乙烯醇(PVA)/聚吡咯烷酮(PVP)共混物的小角X-射线散射(SAXS)研究表明,PVA/PVP共混物的结构参数与共混物组分比及热历史密切相关。按Vonk一维电子密度相关函数法,得到PVA/PVP共混物的长周期,过渡层厚随PVP组分含量增加而增加;结晶片层厚和比内表面积却随PVP含量增加而降低。热处理可提高共混物的结晶性。  相似文献   

3.
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   

4.
尼龙-1010非等温结晶动力学   总被引:7,自引:1,他引:7  
<正> 尼龙-1010是我国独创的工程塑料品种,已被较广泛地应用于精密机械零件、仪表制造、家用电器、航空等方面。有关尼龙-1010的基础研究大多在我国学者中间进行,由于在实际加工生产过程中,如通常的融熔纺丝、注射、模压等工艺均是在非等温条件下进行,有关它的非等温结晶动力学尚未见报道,本文用几种理论方法对尼龙-1010的非等温结晶动力学过程进行研究。  相似文献   

5.
X-射线衍射法测定尼龙1010结晶度   总被引:1,自引:0,他引:1  
根据X-射线散射强度理论,使用图解多重峰方法对尼龙1010三个结晶峰及非晶峰的衍射强度进行校正,首次导出了尼龙1010结晶度计算公式,所得结果与密度及量热测定结果具有很好可比性。  相似文献   

6.
尼龙1010等温结晶球晶形态与生成条件研究   总被引:1,自引:2,他引:1  
 本文利用偏光显微镜研究了等温结晶时尼龙1010球晶的形态与生成条件,发现在原始样品熔点附近或高于原始熔点以上温度结晶,主要生成暗、亮与带正环的负光性放射状球晶;熔点以下至195℃主要生成正放射状球晶;在较宽的温度范围内可生成混合光性放射状球晶,与少量的六瓣、两瓣、不对称四瓣形三种异常光性球晶;181℃以下主要生成正环状球晶.  相似文献   

7.
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   

8.
WAXD研究表明,在结晶温度T_c≤196℃时,尼龙1010等温熔体结晶样品的结晶度X_c和微晶尺寸L_(100)随T_c升高近乎线性增大,而氢键面上的相对衍射强度R却降低;T_c>196℃后三者与T_c关系发生相反变化。结晶速率快时有利于分子链在垂直于氢键平面方向上堆砌,反之有利于在平行于氢键平面方向上生长。  相似文献   

9.
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   

10.
本文利用偏光显微镜研究了等温结晶时尼龙1010球晶的形态与生成条件,发现在原始样品熔点附近或高于原始熔点以上温度结晶,主要生成暗、亮与带正环的负光性放射状球晶;熔点以下至195℃主要生成正放射状球晶;在较宽的温度范围内可生成混合光性放射状球晶,与少量的六瓣、两瓣、不对称四瓣形三种异常光性球晶;181℃以下主要生成正环状球晶.  相似文献   

11.
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   

12.
热致液晶乙基纤维素与尼龙-1010共混物的研究   总被引:2,自引:0,他引:2  
在自制单螺杆小型挤出机上通过熔融共混的办法,制备了不同配比(5/95—25/75)的EC/Nylon—1010共混物.用WAXD、DSC、毛细管流变仪、力学性能测试等方法对共混物进行了研究.发现共混后尼龙-1010的形态结构有明显改变,其强度、模量都有提高,在高剪切速率下,共混物粘度大大降低.配比为1585时,这些性能的改进尤为明显.  相似文献   

13.
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   

14.
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   

15.
小角X-光散射方法对苯乙烯-丁二烯-苯乙烯三嵌段共聚物/聚(苯乙烯-甲基丙烯酸盐)热塑性IPN共混体系相区尺寸的研究韦雨春,袁惠根,潘祖仁(浙江大学化工系杭州310027)关键词热塑性互穿聚合物网络,小角X-光散射,透射电镜随着IPN研究的不断深人,...  相似文献   

16.
 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   

17.
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   

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