Bragg Institute, Australian Nuclear Science and Technology Organisation, Locked Bag 2001, Kirrawee DC, NSW 2232, Australia.
Carbohydr Polym. 2013 Jan 2;91(1):444-51. doi: 10.1016/j.carbpol.2012.08.002. Epub 2012 Aug 9.
Small angle scattering (SAS) techniques have a distinguished track record in illuminating the semi-crystalline lamellar structure of the starch granule. To date, there have been few attempts to use SAS techniques to characterise larger-scale structures reported from imaging techniques such as growth rings, blocklets or pores, nor how these structures would modulate the well-known scattering arising from the semi-crystalline lamellar structure. In this study, SAS data collected over an extended q range were gathered from dry and hydrated starch powders from varied botanical sources. The use of neutrons and X-rays, as well as comparing dry and hydrated granules, allowed different levels of contrast in scattering length density to be probed and therefore selected structural regions to be highlighted. The lowest q range, 0.002-0.04 Å(-1), was found to be dominated by scattering from the starch granules themselves, especially in the dry powders; however an inflection point from a low contrast structure was observed at 0.035 Å(-1). The associated scattering was interpreted within a unified scattering framework with the inflexion point correlating with a structure with radius of gyration ~90 Å - a size comparable to small blocklets or superhelices. In hydrated starches, it is observed that there is an inflection point between lamellar and q(-4) power-law scattering regions at approximately 0.004 Å(-1) which may correlate with growth rings and large blocklets. The implications of these findings on existing models of starch lamellar scattering are discussed.
小角散射 (SAS) 技术在阐明淀粉颗粒半结晶层状结构方面有着卓越的记录。迄今为止,很少有人尝试使用 SAS 技术来描述成像技术(如生长环、块体或孔隙)所报道的较大规模结构,也很少有人尝试描述这些结构将如何调节来自半结晶层状结构的众所周知的散射。在这项研究中,从不同植物来源的干燥和水合淀粉粉末中收集了在扩展 q 范围内收集的 SAS 数据。使用中子和 X 射线,并比较干燥和水合颗粒,可以探测到不同水平的散射长度密度对比,从而突出选择的结构区域。最低的 q 范围为 0.002-0.04 Å(-1),被发现主要由淀粉颗粒本身的散射主导,尤其是在干燥粉末中;然而,在 0.035 Å(-1)处观察到一个来自低对比度结构的拐点。相关散射在统一的散射框架内进行解释,拐点与回转半径约为 90 Å 的结构相关 - 这与小的块体或超螺旋体相当。在水合淀粉中,观察到在层状和 q(-4)幂律散射区域之间存在一个拐点,大约在 0.004 Å(-1)处,这可能与生长环和大的块体有关。这些发现对现有的淀粉层状散射模型的影响将进行讨论。