Henderson R
MRC Laboratory of Molecular Biology, Cambridge, UK.
Q Rev Biophys. 1995 May;28(2):171-93. doi: 10.1017/s003358350000305x.
Radiation damage is the main problem which prevents the determination of the structure of a single biological macromolecule at atomic resolution using any kind of microscopy. This is true whether neutrons, electrons or X-rays are used as the illumination. For neutrons, the cross-section for nuclear capture and the associated energy deposition and radiation damage could be reduced by using samples that are fully deuterated and 15N-labelled and by using fast neutrons, but single molecule biological microscopy is still not feasible. For naturally occurring biological material, electrons at present provide the most information for a given amount of radiation damage. Using phase contrast electron microscopy on biological molecules and macromolecular assemblies of approximately 10(5) molecular weight and above, there is in theory enough information present in the image to allow determination of the position and orientation of individual particles: the application of averaging methods can then be used to provide an atomic resolution structure. The images of approximately 10,000 particles are required. Below 10(5) molecular weight, some kind of crystal or other geometrically ordered aggregate is necessary to provide a sufficiently high combined molecular weight to allow for the alignment. In practice, the present quality of the best images still falls short of that attainable in theory and this means that a greater number of particles must be averaged and that the molecular weight limitation is somewhat larger than the predicted limit. For X-rays, the amount of damage per useful elastic scattering event is several hundred times greater than for electrons at all wavelengths and energies and therefore the requirements on specimen size and number of particles are correspondingly larger. Because of the lack of sufficiently bright neutron sources in the foreseeable future, electron microscopy in practice provides the greatest potential for immediate progress.
辐射损伤是一个主要问题,它阻碍了使用任何类型的显微镜在原子分辨率下确定单个生物大分子的结构。无论使用中子、电子还是X射线作为照明,都是如此。对于中子,可以通过使用完全氘代和15N标记的样品以及使用快中子来减少核俘获的截面以及相关的能量沉积和辐射损伤,但单分子生物显微镜仍然不可行。对于天然存在的生物材料,目前电子在给定的辐射损伤量下能提供最多的信息。在生物分子和分子量约为10(5)及以上的大分子聚集体上使用相衬电子显微镜,理论上图像中存在足够的信息来确定单个颗粒的位置和取向:然后可以应用平均方法来提供原子分辨率结构。这需要大约10,000个颗粒的图像。分子量低于10(5)时,需要某种晶体或其他几何有序聚集体来提供足够高的组合分子量以实现对齐。实际上,目前最佳图像的质量仍低于理论上可达到的质量,这意味着必须对更多的颗粒进行平均,并且分子量限制比预测的限制要大一些。对于X射线,在所有波长和能量下,每个有用弹性散射事件的损伤量比电子大数百倍,因此对样品尺寸和颗粒数量的要求相应更高。由于在可预见的未来缺乏足够亮的中子源,实际上电子显微镜提供了取得直接进展的最大潜力。