OMMT对PA6/ABS共混体系结晶行为及热力学性能的影响

采用有机蒙脱土(OMMT)、聚酰胺6(PA6)和丙烯腈-丁二烯-苯乙烯共聚物(ABS),通过熔融共混的方法制备了PA6/ABS/OMMT共混物。利用透射电子显微镜(TEM)、差示扫描量热仪(DSC)及动态热力学分析仪(DMA)研究了OMMT在PA6/ABS(70/30)合金体系中的分布和分散状况,以及PA6/ABS/OMMT共混体系的结晶行为和热力学性能。结果表明:OMMT片层主要分散于PA6相中,PA6与ABS的两相界面处亦存在少量OMMT片层。OMMT的加入降低了PA6/ABS共混体系的结晶温度,使PA6的结晶结构发生改变,说明OMMT具有一定的增容作用。引入OMMT后,PA6/ABS共混体系的储能模量有所提升,玻璃化转变温度则变化较小。     

ABS/PA6/OMMT共混体系的结晶及热力学性能

采用丙烯腈-丁二烯-苯乙烯共聚物(ABS)、尼龙6(PA6)和有机蒙脱土(OMMT)通过熔融共混的方法制备了ABS/PA6合金。利用广角X射线衍射(WAXD)、透射电子显微镜(TEM)、差示扫描量热法(DSC)、动态热力学分析仪(DMA)研究了ABS/PA6/OMMT合金体系的结晶性能、热力学性能及OMMT在共混体系中的分布情况。结果表明,OMMT以剥离状态分布于PA6相中,PA6、ABS两相界面存在少量的OMMT片层。OMMT的加入降低了合金体系的结晶温度及结晶度,且对ABS/PA6共混体系具有一定的增容作用。添加3份OMMT到ABS/PA6体系中,其储能模量达到极值,ABS/PA6/OMMT共混体系的玻璃化转变温度变化较小。     

PA6/ABS的结构与力学性能研究

采用熔融共混法制备了苯乙烯-马来酸酐共聚物(SMA)增容的聚酰胺6/丙烯腈-丁二烯-苯乙烯共聚物(PA6/ABS)共混物,用扫描电镜(SEM)对PA6/ABS共混物结构进行了表征.结果表明,随着SMA含量的增加,PA6/ABS共混体系的橡胶相粒径减小.橡胶颗粒的多分散系数保持不变,基体层厚度逐渐减小;PA6/ABS共混体系的脆韧转变温度随SMA含量的增加先减小后增加.     

SMA增容PA1012/ABS共混物的研究

采用熔融共混方法制备一系列尼龙1012(PA1012)/丙烯腈-丁二烯-苯乙烯共聚物(ABS)/苯乙烯-马来酸酐共聚物(SMA)共混物,利用冲击试验仪、示差扫描量热仪(DSC)和扫描电子显微镜(SEM)等手段,探究增容剂SMA和ABS的添加量对PA1012/ABS共混物性能的影响。结果表明,当SMA含量为5%且ABS含量为50%时,PA1012/ABS/SMA共混物的缺口冲击强度最优,为669 J/m;随着SMA含量增加,结晶温度有先增大后减小趋势,并且与纯PA1012相比,PA1012/ABS/SMA共混物结晶温度升高了10℃,促进PA1012结晶;SMA加入后,ABS分散相粒子尺寸减小,PA1012和ABS间界面黏结作用增强,证实SMA对PA1012/ABS有明显增容作用。     

相容剂种类对PA6/ABS合金性能的影响

采用苯乙烯-马来酸酐(SMA)、苯乙烯-丙烯腈-马来酸酐(SAMAH)和苯乙烯-丙烯腈-甲基丙烯酸(SAMAA)三种共聚物增容尼龙6/丙烯腈-丁二烯-苯乙烯共聚物(PA6/ABS)共混物,利用双螺杆挤出机制备出PA6/ABS合金,对其结构及其性能进行了表征和探讨。结果表明,三种相容剂均可有效地增容PA6/ABS合金,改善ABS在PA6中的分散,大幅度提高了缺口冲击强度;通过差示扫描量热(DSC)分析发现PA6/ABS的结晶度降低,结晶速率变慢;同时通过流变实验发现PA6/ABS共混物为假塑性流体,三种相容剂均提高了其表观黏度。     

ABS高胶粉增韧PA6的结构与性能研究

采用熔融共混法制备了苯乙烯-马来酸酐共聚物（SMA）增容的PA6/ABS共混物,用透射电子显微镜对PA6/ABS共混物结构进行了表征,研究了增容剂含量对PA6/ABS共混体系结构、性能以及脆-韧转变温度的影响。结果表明,随着SMA含量的增加,PA6/ABS共混体系的橡胶相粒径先逐渐减小,后趋于平缓;橡胶颗粒的多分散系数逐渐增加;基体层厚度不断减小;PA6/ABS共混体系的拉伸强度逐渐增加;PA6/ABS共混体系的脆-韧转变温度先减小,后上升。     

高性能PA6/ABS合金的研制

分别以接枝ABS、苯乙烯-马来酸酐接枝物（SMA）和苯基马来酰亚胺共聚物为相容剂,考察了它们对PA6/ABS共混体系相容性和力学性能的影响。并研究了PA6/ABS共混体系中PA6、ABS树脂的选择对共混物冲击韧性的影响。研究表明,接枝ABS、SMA和苯基马来酰亚胺共聚物都是PA6/ABS共混体系的有效增容剂,能显著改善PA6/ABS共混物的相容性并提高共混物的机械力学性能。选用高粘度的PA6树脂有利于提高共混体系的冲击韧性,提高高胶含量ABS用量有助于获得高低温冲击性能优异的PA6/ABS合金材料。     

超韧PA6/ABS合金的制备

以苯乙烯-马来酸酐（SMA）共聚物为增容剂，考察了ABS及SMA的含量对PA6／ABS共混体系的力学性能的影响；并利用SEM研究了PA6／ABS冲击断面的相结构。研究表明：SMA是PA6／ABS共混体系的有效增容剂。随着其含量的增加，分散相ABS粒子的尺寸减小，分散更加均匀，能显著地改善PA6／ABS共混物的冲击、拉伸和弯曲性能。在该共混体系中，ABS含量的增加能够大幅度地提高PA6／ABS共混物的冲击韧性；但当ABS含量超过10％时，将使PA6／ABS共混物的拉伸和弯曲性能明显下降。SMA的添加量为0．5％，且质量比为90／10的PA6／ABS共混体系能保持较好的加工性能，制备的PA6／ABS合金具有最佳的综合力学性能和超高韧性．Izod缺口冲击强度高达1200J／m。     

组分对PA6/ABS合金力学性能的影响

通过双螺杆挤出制备了尼龙6(PA6)/丙烯腈-丁二烯-苯乙烯共聚物(ABS)合金,考察了PA6、ABS和相容剂的种类及含量对PA6/ABS合金力学性能的影响。结果表明,通过中黏度(2.4~2.7 Pa·s)的尼龙6与聚丁烯(PB)质量分数达到16%的ABS制备的PA6/ABS合金有优异的力学性能;随着PA6含量增加,PA6/ABS合金的拉伸和弯曲强度增加,冲击强度下降,ABS含量增加使PA6/ABS冲击强度上升,拉伸和弯曲强度反而下降;相容剂马来酸酐(MAH)接枝ABS(ABS-g-MAH)对PA6/ABS合金增容效果优于苯乙烯接枝马来酸酐共聚物(SMA);当ABSg-MAH质量分数为3%,PA6与ABS质量比为62/35时,制备出的PA6/ABS合金具有最佳的力学性能,缺口冲击强度可达28 kJ/m2。     

PA6/ABS共混物性能研究

将聚酰胺6（PA6）与市售的丙烯腈-丁二烯-苯乙烯（ABS）树脂共混,制备PA6/ABS共混物。研究了ABS树脂的用量对PA6/ABS共混物力学性能的影响;采用苯乙烯及丙烯腈共聚物（SAN）和ABS粉料熔融共混制得不同胶含量的ABS/SAN共混物。研究了不同胶含量的ABS/SAN共混物对PA6/ABS共混物力学性能的影响。在PA6/ABS/SAN共混物中引入苯乙烯-丙烯腈-马来酸酐共聚（SAM）树脂取代部分SAN树脂,研究了SAM树脂的加入及引入顺序的不同对共混物性能的影响。结果表明, ABS树脂的用量在50%～60%左右时共混物性能最佳。随ABS/SAN共混物胶含量提高,共混物的拉伸强度、弹性模量、弯曲强度和弯曲模量逐渐降低。随SAM树脂替代SAN量增加,共混物的拉伸和弯曲性能先降低后增加。但共混物熔体流动速率降低明显,而SAM树脂的引入顺序对共混物的力学性能影响不大。     

Gemini表面活性剂/醇/正辛烷/盐水体系微乳液的研究

以壬基酚为原料在催化剂存在下与二溴烷烃作用生成双醚,然后磺化,合成了一类Gemini阴离子表面活性剂,用悬滴法测定了其油水界面张力,结果表明,Gemini表面活性剂可使油水界面张力降低到 10-3mN/m。研究了Gemini表面活性剂 /醇 /正辛烷 /盐水体系的微乳液相行为,通过拟三元相图的方法确定了助表面活性剂醇的种类,实验结果表明,链长的比链短的醇具有更好的助活作用。通过正交实验方法得到了形成中相微乳液的最佳组成:w(GeminiD) =0 1%;w(n C6H13OH) =4 0%;w(NaCl) =1 5%。     

Formation of the Perovskite Phase in the PbMg1/3Nb2/3O3─PbTiO3 System

The reaction sequences during calcination of oxide mixtures were studied for the PbMg_1/3Nb_2/3O₃─PbTiO₃ (PMN-PT) system. The effect of reactivity and composition of the starting mixtures was investigated. In the present study, a B-site-deficient, cubic pyrochlore phase in the PbO-Nb₂O₅ system was formed at 500°C. The perovskite phase of PMN was formed at 7007deg;C through the diffusion of MgO into the pyrochlore phase. The lattice parameter of the pyrochlore phase decreased as this transformation to perovskite progressed.     

Phase Equilibria in the Spinel Region of the System FeO-Fe2O3-Al2O3

Phase relations in the spinel region of the system FeO-Fe₂O₃-Al₂O₃ were determined in CO₂ at 1300°, 1400°, and 15000°C and for partial oxygen pressures of 4 × 10⁻⁷ and 7 × 10⁻¹⁰ atmospheres at 15OO°C. The spinel field extends continuously from Fe₃O_4-x to FeAl₂O_4+z.     

EVA／APP／PER／MEL／纳米蒙脱土复合材料的研究

通过制备有机改性蒙脱土(MMT),共混改性乙烯-醋酸乙烯共聚物为主体的无卤膨胀阻燃电缆材料,发现改性MMT与聚磷酸铵(APP)/季戊四醇(PER)/三聚氰胺(MEL)三元膨胀阻燃剂(IFR)之间有力学和阻燃协效作用,能同时提高塑料的力学和阻燃性能。     

Thermodynamic Analysis of the Metastable Regions for the AI2O3-SiO2 System

The paper offers a short review of investigations conducted on the Al₂O₃-SiO₂ system, particularly from the point of view of an appearance of immiscibility gaps, below the liquidus temperatures. Based on theoretical criteria and using the data along the liquidus curves (for mullite and corundum), this investigation suggests immiscibility regions at both ends of the phase diagram. That is, it defines the Margules polynomials for calculation of the activity coefficients necessary for determining the Gibbs energy of mixing. Obtained results are in good agreement with the results reported by Risbud and Pask and other investigators who have found immiscibility gaps at rather high temperatures.     

Phase Diagram for the SiF4 Join in the System SiO2-Al2O3-SiF4

Alumina reacts with 1 atm of SiF₄ below 660°± 7°C to form A1F₃ and SiO₂. At higher temperatures the product is a mixture of fluorotopaz and AIF₃. Mixtures of fluorotopaz and AIF3 decompose in 1 atm of SiF₄ at 973°± 8°C and form tabular α-alumina. The equilibrium vapor pressure of SiF₄ above mixtures of fluorotopaz and AlF₃ is log p (atm) = 9.198 – 11460/ T (K). Fluorotopaz itself decomposes at 1056°± 5°C in 1 atm of SiF₄ to give acicular mullite, 2Al₂O₃^.1.07SiO₂. Alumina and mullite are stable in the presence of 1 atm of SiF₄ above 973° and 1056°C, respectively. The phase diagram of the system SiO₂-Al₂O₃-SiF₄ shows only gas-solid equilibria.     

Studies in the System CaO-Al2O3-SiO2H2O: III, New Data on the Polymorphism of Ca2SiO2 and Its Stability in the System CaO-SiO2- H2O

The nature of the low-temperature inversions γ-α' and α'-β was investigated by various techniques: hydrothermal and "dry" quenching runs, differential thermal analysis at atmospheric and elevated nitrogen pressures, X-ray diffractometer patterns obtained at elevated temperatures, "static" pressure techniques, and infrared absorption spectrometry. A revised energy-temperature diagram is presented for Ca₂SiO₄, with the transition γ' to α' taking place at about 725°C. and the α'-β transition, although not reversible at an exact temperature, taking place at about 670° C. At low water pressures (2000 lb. per sq. in.) the inversion γ-α' was placed at 675°C. Attempts to extrapolate the value obtained at 2000 lb. per sq. in. to obtain a more accurate reversible inversion temperature at atmospheric pressure, although limited in accuracy by the reliability of heat-of-transition data, would indicate a temperature of about 725° C. at atmospheric pressure. Three new compounds, 8CaO.3SiO₂ -3H₂O (X), 6CaO 3SiO₂.H₂O (Y), and 9CaO-6SiO₂ H₂O (Z), were found to be stable above 700°C. at H₂O pressures greater than 7500 lb. per sq. in.     

On the Formation of Fe2+ in the System MgO-Fe2O3-MgFe2O4 at High Temperatures

The formation of ferrous iron in the system MgO-Fe₂O₃MgFe₂O₄ is of interest in connection with its deleterious effect on the microwave performance of magnesium ferrite, MgFe₂O₄. The partial reduction of ferric iron in the system at relatively low temperatures is discussed in terms of the preferential diffusion of iron, and its partial stabilization as ferrous iron from lattice energy considerations.     

Preparation of the High-Quality Superconductor La1Ba2Cu3Oy

The relationship between the preparation procedure and superconducting properties of La₁Ba₂Cu₃O_y was studied. A series of samples was sintered in an N₂-gas atmosphere for various lengths of time ranging from 1 to 40 h, followed by a fixed annealing procedure in O₂. It was found that the shorter the sintering period, the higher was the oxygen content. The samples sintered for a period of less than 15 h contained excess oxygen compared with La₁Ba₂Cu₃O₇ and exhibited poor superconducting properties. The sample sintered for 40 h had an oxygen content y equal to 6.95, and had excellent superconducting properties. The mechanism for preparing high-quality La₁Ba₂Cu₃O_y is discussed.