Gun'ko V M, Turov V V, Turova A A, Krupska T V, Pissis P, Leboda R, Skubiszewska-Zięba J
Chuiko Institute of Surface Chemistry, 17 General Naumov Street, 03164 Kiev, Ukraine.
Chuiko Institute of Surface Chemistry, 17 General Naumov Street, 03164 Kiev, Ukraine.
J Colloid Interface Sci. 2014 Jul 15;426:48-55. doi: 10.1016/j.jcis.2014.03.055. Epub 2014 Apr 3.
To control the properties of poly(dimethylsiloxane) (PDMS, Oxane 1000) as a bio-inert material, the characteristics of Oxane 1000 were compared for PDMS alone and interacting with silica gel Si-100 and nanosilica PS400. Low-temperature (1)H NMR spectroscopy, applied to static samples at 200-300 K, and differential scanning calorimetry (DSC) at 153-393 K were used to analyze the properties of PDMS and composites. The NMR study shows that liquid and solid-like fractions of PDMS co-exist over a broad temperature range. The cooling-heating cycles give hysteresis loops of intensity of (1)H NMR signals of methyl groups of a liquid fraction of PDMS vs. temperature depending on the silica type. The loop width differs for PDMS alone and bound to silicas, and the samples preheated at 420 K are characterized by much narrower loops. DSC measurements of the samples show a significant difference in the thermograms on the first and second DSC scans that depend on the silica type. For PDMS confined in pores of silica gel, 3D spatial structure of the polymers can be more ordered than that of PDMS located in thin layers at a surface of nanosilica. Therefore, both melting endotherms and crystallization exotherms are observed for PDMS/silica gel. However, for PDMS/nanosilica, both thermal features are much weaker and observed during only the first DSC scan.
为了控制作为生物惰性材料的聚二甲基硅氧烷(PDMS,Oxane 1000)的性能,对单独的PDMS以及与硅胶Si - 100和纳米二氧化硅PS400相互作用的Oxane 1000的特性进行了比较。使用低温(1)H核磁共振光谱法(应用于200 - 300 K的静态样品)和153 - 393 K的差示扫描量热法(DSC)来分析PDMS及其复合材料的性能。核磁共振研究表明,PDMS的液态和类固态部分在很宽的温度范围内共存。冷却 - 加热循环给出了取决于二氧化硅类型的PDMS液态部分甲基的(1)H NMR信号强度与温度的滞后回线。单独的PDMS和与二氧化硅结合的PDMS的回线宽度不同,并且在420 K预热的样品的回线要窄得多。样品的DSC测量表明,第一次和第二次DSC扫描的热谱图存在显著差异,这取决于二氧化硅类型。对于限制在硅胶孔中的PDMS,聚合物的三维空间结构可能比位于纳米二氧化硅表面薄层中的PDMS更有序。因此,在PDMS/硅胶中观察到了熔融吸热峰和结晶放热峰。然而,对于PDMS/纳米二氧化硅,这两种热特性都要弱得多,并且仅在第一次DSC扫描期间观察到。