氟橡胶/硅橡胶/氟硅橡胶并用胶的性能研究

研究氟橡胶(FKM)/硅橡胶(MVQ)/氟硅橡胶(FSR)并用胶的性能。试验结果表明:FKM并用MVQ后,并用胶的物理性能和耐油性能下降,但回弹值和耐低温性能明显改善;采用FSR部分替代MVQ后,随着FSR用量的增大,并用胶的相容性改善,拉伸强度和拉断伸长率增大,耐油性能提高,耐低温性能变化不大。     

氟橡胶与硅橡胶共混胶的性能研究

研究了氟橡胶(FKM)与硅橡胶(MVQ)共混胶以及采用氟硅橡胶(FSR)为增容剂制作的FKM/MVQ共混胶性能。结果表明,氟橡胶与硅橡胶共混可改善氟橡胶的耐低温性能,但其力学性能降幅较大;以氟硅橡胶为增容剂可改善2种橡胶的相容性,其共混胶兼具硅橡胶的耐热性和耐寒性、氟橡胶的耐油性,成本较低。     

硫化条件对FKM/MVQ并用胶性能的影响

采用机械共混法制备氟橡胶(FKM)/甲基乙烯基硅橡胶(MVQ)并用胶,研究硫化条件对FKM/MVQ并用胶性能的影响。结果表明,随着一段硫化温度的升高,FKM/MVQ并用胶t10和t90缩短,邵尔A型硬度和撕裂强度变化不大,定伸应力和拉伸强度先增大后减小;当一段硫化条件为165℃×t90、二段硫化条件为250℃×4h时,FKM/MVQ并用胶的综合物理性能较好。     

氟橡胶/甲基乙烯基硅橡胶共混胶的性能

研究了氟橡胶(FKM)与甲基乙烯基硅橡胶(MVQ)的共混比、1,4-双叔丁基过氧异丙基苯(BIBP)硫化剂和三烯丙基异三聚氰酸酯(TAIC)助硫化剂用量以及硫化温度对FKM/MVQ共混胶硫化性能和力学性能的影响。结果表明,当FKM/MVQ共混比为50/50、硫化剂BIBP用量为1.0份、助硫化剂TAIC用量为2.5份、硫化温度为160℃时,FKM/MVQ共混胶的硫化性能和力学性能最优,硫化时其最大转矩为19.34 dN·m,拉伸强度为5.29 MPa,扯断伸长率为230.68%。     

乙烯丙烯酸酯橡胶共混改性硅橡胶的性能研究

将乙烯丙烯酸酯橡胶(AEM)按照不同比例与硅橡胶(MVQ)进行共混,研究并用比对MVQ/AEM并用胶的硫化特性、物理性能、耐油性能和动态力学性能的影响。结果表明:随着AEM用量的增大,MVQ/AEM并用胶的硫化时间延长,MH减小,物理性能明显改善;经过热空气老化后,并用胶的拉伸强度保持率和拉断伸长率保持率均随着AEM用量的增大而减小,耐老化性能降低;并用胶在ASTM 1#油和ASTM 3#油中浸泡后体积变化率和质量变化率减小,耐油性能改善。动态力学分析结果表明,AEM和MVQ具有良好的相容性,二者并用后低温性能下降,损耗因子逐渐增大。     

MVQ-g-TFEMA对氟橡胶/硅橡胶共混胶的增容作用

通过高温力化学接枝法制备硅橡胶接枝甲基丙烯酸-2,2,2-三氟乙酯(MVQ-g-TFE-MA),作为氟橡胶/硅橡胶共混胶的增容剂。研究增容剂用量对氟橡胶/硅橡胶共混胶的力学性能、耐油性能和低温性能的影响,采用DMA研究共混胶中氟橡胶和硅橡胶的相容性。结果表明,添加的MVQ-g-TFEMA的质量分数为4.6%时,共混胶具有良好的力学性能。随着增容剂的质量分数从0增至11.5%,共混胶的耐油性能提高,脆性温度从-36.8℃下降至-48.3℃。DMA分析表明,增容剂MVQ-g-TFEMA改善了共混胶中氟橡胶和硅橡胶的相容性。     

支化多酚羟基氢化丁腈橡胶/氟橡胶反应型并用胶的制备与性能研究

制备支化多酚羟基氢化丁腈橡胶(PHHNBR)/氟橡胶(FKM)反应型并用胶,并对其性能进行研究。结果表明:PHHNBR具有支化多酚羟基结构,PHHNBR/FKM反应型并用胶可以实现自身的硫化;FKM与PHHNBR相容性良好,并用胶的拉伸强度明显高于FKM硫化胶,撕裂强度相当,玻璃化温度明显降低,耐低温性能改善。     

共混比对AEM/MVQ共混胶性能的影响

研究了共混比对乙烯丙烯酸酯橡胶/甲基乙烯基硅橡胶（AEM/MVQ）共混胶硫化特性、力学性能、耐热老化性能、耐油性能、压缩永久变形及动态力学性能的影响。结果表明,随着AEM用量的增加,共混胶正硫化时间延长,拉伸强度、拉断伸长率和撕裂强度均增加,耐油性能提高;随着MVQ用量的增加,共混胶耐热老化性能提高,压缩永久变形减小。DMA数据显示,AEM和MVQ具有良好的相容性,共混胶低温性能比纯AEM橡胶有所改善。     

氟橡胶/甲基乙烯基硅橡胶共混弹性体的性能

通过机械共混法制备了氟橡胶(FKM)/甲基乙烯基硅橡胶(MVQ)弹性体,研究了二者的质量比对共混弹性体力学性能、耐油性能和动态力学性能的影响.结果表明,当FKM/MVQ(质量比,下同)为80/20时,共混弹性体具有较好的综合力学性能.随着FKM所占比例的增加,共混弹性体的耐油性能提高.当振动频率为1 Hz时,共混弹性体中MVQ相的玻璃化转变温度(Tg)比MVQ的Tg提高了约5.0 ℃,而FKM相的Tg改变不大;当FKM/MVQ为60/40时,随着振动频率由1 Hz增大到50 Hz,FKM相的Tg升高了12.9 ℃,而MVQ相的Tg变化不大.     

氟橡胶/三元乙丙橡胶并用胶的性能

研究了不同并用比(质量比)时氟橡胶(FKM)/三元乙丙橡胶(EPDM)并用胶动态硫化和静态硫化后的低温性能、物理机械性能、耐老化性能和热稳定性,并用扫描电子显微镜表征了并用胶.结果表明,当并用比为30/70时,并用胶有较好的相容性;EPDM可以改善FKM的低温性能;随着EPDM用量的增加,并用胶的拉伸强度及邵尔A硬度降低;动态硫化FKM/EPDM并用胶比静态硫化FKM/EPDM并用胶具有更好的耐老化性能,但老化前前者的拉伸强度稍低于后者;FKM/EPDM并用胶的热稳定性优于纯EPDM;静态硫化FKM/EPDM并用胶中片层现象严重,动态硫化FKM/EPDM并用胶的EPDM包覆在FKM中,但相畴偏大.     

Compact Swelling in Bi1.4Pb0.6Sr2Ca2Cu3.6Oy During the Formation of High-Tc Superconducting Phase

Compact swelling in Pb-doped Bi-Sr-Ca-Cu-O superconductor has been studied by observing the effects of the size of calcined powders, volatilization of materials, and sintering of high- T _c (2223) powders. The bulk density increases at the early stage of sintering, for about 20 h, and then decreases. Densification occurs when the low- T _c (2212) phase and a liquid phase exist, whereas dedensification occurs with the formation of the 2223 phase regardless of the presence of the liquid. Gas evolution from specimens does not appear to be responsible for compact swelling. Compact swelling is explained by anisotropic growth of thin, platelike 2223 grains in random orientation. When 2223 grains grow in a preferred direction, compact swelling is suppressed.     

Synthetic routes to nanoscale BxCyNz architectures

B_xC_yN_z nanoscale materials, hybrids of h-BN and graphite, have been recently synthesised using various techniques. Here, we present the latest advances in the synthesis and characterisation of B-C-N nanotubes and nanofibres. In particular, we focus on layered BC₂N, BN, BC and CN_x systems, reviewing their production methods as well as their structural and electronic properties. These materials may find important applications in the fabrication of nanotransistors, robust nanocomposites, conducting polymers, storage components and field emission sources.     

Structure Evolution from Pb(Mg1/3Nb2/3)O3 to La(Mg2/3Nb1/3)O3

The crystal structure of lanthanum-modified lead magnesium niobates having composition (Pb_{1− x} La _x ) (Mg_{(1+ x )/3}-Nb_{(2− x )/3})O₃ with X = 0 to 1 was investigated by X-ray powder diffraction. It was found that the fundamental reflections from perovskite structure remain in the whole range of composition. The superlattice reflections from the A(B'_1/2-B"_1/2)O₃ ordered structure are also well preserved for La content greater than 50 at.%; however, a series of extra peaks of mixing indices appears, with intensities gradually enhanced with the increase of La content. For the complete substitution of Pb by La, a splitting of some reflections can be observed in the diffraction pattern. The results indicate that the crystal structure evolves continuously with the La content, from disordered cubic perovskite of space group Pm 3 m for X = 0, to ordered cubic perovskite of space group Fm 3 m for X = 0.5, distorted cubic perovskite of space group Pa 3 for 0.5 < X < 0.9, and finally to a rhombohedral perovskite, possibly belonging to the space group R 3 , for X ≥ 0.9. In the evolution of structure, a linear reduction of the lattice constant of the perovskite cell from 4.048 to 3.964 Å was observed.     

Microwave Dielectric Properties of CaTiO3-CaAl1/2Nb1/2O3 Ceramics Doped with Li3NbO4

The microwave dielectric properties of CaTi_{1− x} (Al_1/2Nb_1/2) _x O₃ solid solutions (0.3 ≤ x ≤ 0.7) have been investigated. The sintered samples had perovskite structures similar to CaTiO₃. The substitution of Ti⁴⁺ by Al³⁺/Nb⁵⁺ improved the quality factor Q of the sintered specimens. A small addition of Li₃NbO₄ (about 1 wt%) was found to be very effective for lowering sintering temperature of ceramics from 1450–1500° to 1300°C. The composition with x = 0.5 sintered at 1300°C for 5 h revealed excellent dielectric properties, namely, a dielectric constant (ɛ_r) of 48, a Q × f value of 32 100 GHz, and a temperature coefficient of the resonant frequency (τ_f) of −2 ppm/K. Li₃NbO₄ as a sintering additive had no harmful influence on τ_f of ceramics.     

Preparation and properties of poly(Nε,Nε-dicarboxymethyl-l-lysine)

A new ampholytic homopolypeptide, $\text{poly}\text{(N}{}^{\mathrm{\epsilon }}\text{,N}{}^{\mathrm{\epsilon }}\text{-}\text{dicarboxy-methyl-}\text{l}\text{-lysine}\text{)}$, which has one tertiary amino and two carboxyl groups in the side chain has been derived from a hydrochloride salt of poly(L-lysine). The polymer in aqueous solution seems to be in the coil form with locally extended structure (LES) at neutral pH. In both the acidic and alkaline regions, the molar ellipticity of the polymer changes as a result of change in net charge on the side chain. The conformational changes may be from the coil with LES to other coiled forms. 5–7 M NaClO₄ and 80% aqueous methanol induce the α-helix in the polymer at neutral pH. Divalent cations, Cu²⁺ and Ca²⁺, do not induce any remarkably ordered structures such as α-helix or β-structure in the polymer in aqueous solution at any pH. Ultraviolet absorption studies show an absorption peak of the polymer-Cu²⁺ complex near 240 nm. Dependence of the peak intensity on pH at various q values ($\text{q =}\text{[}\text{Cu}{}^{\mathrm{2+}}\text{]}\text{[}\text{residue}\text{]}$) indicates the two steps of the complex formation. At q less than 0.64, the formation is described only with the first step. An average coordination number for Cu²⁺ at the first step was calculated to be about 2 by the method of Mandel and Leyte. The association constant of Cu²⁺ with the residue at the step was determined from the absorption data to be far smaller than that for the Cu²⁺-EDTA complex. The second step of the formation occurs in the case of large q but the absorption data for the second step cannot be obtained exactly due to precipitation.     

Dielectric-State Analysis in Solid-Solution Pb(Yb1/2Ta1/2)O3–Pb(Lu1/2Nb1/2)O3

The structure and temperature dependence of complex lead perovskite dielectrics were investigated for the system (1 − x )Pb(Yb_1/2Ta_1/2)O₃– x Pb(Lu_1/2Nb_1/2)O₃. Superlattice reflections for the compositions 0.8 < x < 1.0 were observed by X-ray diffractometry, and the temperature-composition dielectric-state diagram was determined. In the present study, the disordered middle composition, with 0.2 < x < 0.8, showed a diffuse paraelectric–ferroelectric phase transition, whereas the ordered end compositions, with 0 ≤ x < 0.2 and 0.8 < x ≤ 1.0, revealed successive sharp paraelectric–antiferroelectric and weak antiferroelectric–ferroelectric phase transitions. The dielectric state was confirmed by examining the variation of polarization ( P ) with electric field ( E ).