Department of Chemistry, Indian Institute of Technology Kanpur, Kanpur 208 016, UP, India.
Department of Chemistry, Indian Institute of Technology Kanpur, Kanpur 208 016, UP, India.
Spectrochim Acta A Mol Biomol Spectrosc. 2018 Jul 5;200:202-211. doi: 10.1016/j.saa.2018.04.033. Epub 2018 Apr 17.
In this study, steady state, solvation dynamics and rotational dynamics experiments have been carried out on a system of DACIA-tagged papain in bulk water and inside the water pool of cationic (cetyltrimethylammonium bromide, CTAB) and anionic (sodium bis(2-ethylhexyl)sulfosuccinate, AOT) reverse micelles with varying water contents (W = 20 to 50). While the absorption and emission maxima and the excited state lifetime did not show any noticeable change with the variation of the size of the reverse micelle, the change in solvation time, Stokes shift, rotational correlation time and residual anisotropy with the change in reverse micellar size were quite revealing. The average solvation time and Stokes shift of papain in bulk water are 0.22 ns and 125 cm respectively, which increase to 0.96 ns and 718 cm while inside CTAB reverse micelle of W = 20. The solvation time and Stokes shift values decrease with the increase in the size of reverse micelle, approaching the corresponding values in bulk water when W = 50. The solvation time and Stokes shift of the DACIA-tagged papain was found to be high while inside AOT reverse micelle also (0.47 ns and 438 cm respectively when W = 20), but there was no monotonous variation with the change in size of micellar size as in the case with CTAB reverse micelle. From the anisotropy studies, it was seen that inside CTAB and AOT reverse micelles, there is a significant amount of residual anisotropy, which is absent in the case of DACIA-tagged papain in bulk water. The rotational correlation times were also found to be higher inside the reverse micelles than those in bulk water. Both residual anisotropy and rotational correlation time were found to be more in the case with AOT reverse micelle than with CTAB reverse micelle. These behaviours could be explained based on the electrostatic forces acting between the papain having a positive surface charge and the reverse micelles of cationic CTAB and anionic AOT.
在这项研究中,我们在含有不同含水量(W=20 到 50)的阳离子(十六烷基三甲基溴化铵,CTAB)和阴离子(双(2-乙基己基)磺基琥珀酸钠,AOT)反胶束中的 DACIA 标记木瓜蛋白酶体系中进行了稳态、溶剂化动力学和旋转动力学实验。虽然吸收和发射最大值以及激发态寿命没有随着反胶束尺寸的变化而发生明显变化,但溶剂化时间、Stokes 位移、旋转相关时间和剩余各向异性随反胶束尺寸的变化却非常明显。在本体水中,木瓜蛋白酶的平均溶剂化时间和 Stokes 位移分别为 0.22ns 和 125cm,而在 W=20 的 CTAB 反胶束中则分别增加到 0.96ns 和 718cm。随着反胶束尺寸的增加,溶剂化时间和 Stokes 位移值减小,当 W=50 时,接近本体水中的相应值。当 W=20 时,DACIA 标记的木瓜蛋白酶在 AOT 反胶束中的溶剂化时间和 Stokes 位移也很高(分别为 0.47ns 和 438cm),但与 CTAB 反胶束不同,其大小变化没有单调变化。从各向异性研究中可以看出,在 CTAB 和 AOT 反胶束中,存在大量的剩余各向异性,而在本体水中的 DACIA 标记的木瓜蛋白酶中则不存在。还发现,在反胶束中,旋转相关时间比在本体水中高。与 CTAB 反胶束相比,AOT 反胶束中的剩余各向异性和旋转相关时间都更高。这些行为可以根据带正表面电荷的木瓜蛋白酶与带正电荷的 CTAB 阳离子和带负电荷的 AOT 阴离子反胶束之间的静电相互作用来解释。