Li Pai-Chi, Makarov Dmitrii E
Department of Chemistry and Biochemistry, Institute for Theoretical Chemistry, University of Texas at Austin, Austin, Texas 78712, USA.
J Chem Phys. 2004 Sep 8;121(10):4826-32. doi: 10.1063/1.1778152.
Motivated by the recent experimental atomic force microscopy (AFM) measurements of the mechanical unfolding of proteins pulled in different directions [D. J. Brockwell et al., Nat. Struct. Biol. 10, 731 (2003); M. Carrion-Vazquez et al., ibid 10, 738 (2003)] we have computed the unfolding free energy profiles for the ubiquitin domain when it is stretched between its (A) N and C termini, (B) Lys48 and C terminus, (C) Lys11 and C terminus, and (D) N terminus and Lys63. Our results for cases (A) and (B) are in good agreement with the experimental unfolding forces measured for the N-C and Lys48-C linked polyubiquitin, in particular, indicating a considerably lower unfolding force in the latter case. Mechanical unfolding in case (A) involves longitudinal shearing of the terminal parallel strands while in case (C) the same strands are "unzipped" by the force. The computed unfolding forces in case (C) are found to be very low, less than 50 pN for pulling rates typical of AFM experiments. The unfolding free energy barrier found in case (C) is approximately 13 kcal/mol, which corresponds to a zero-force unfolding rate constant that is comparable to the rate of chemical unfolding extrapolated to zero denaturant concentration. The unfolding barrier calculated in case (A) in the limit of zero force is much higher, suggesting that mechanical unfolding in this case follows a pathway that is different from that of thermal/chemical denaturation.
受近期关于沿不同方向拉伸蛋白质的机械解折叠的实验原子力显微镜(AFM)测量结果的启发[D. J. Brockwell等人,《自然结构生物学》10, 731 (2003);M. Carrion-Vazquez等人,同上,10, 738 (2003)],我们计算了泛素结构域在以下情况下的解折叠自由能分布:(A) N端和C端之间拉伸时;(B) Lys48和C端之间拉伸时;(C) Lys11和C端之间拉伸时;以及(D) N端和Lys63之间拉伸时。我们对情况(A)和(B)的结果与针对N-C和Lys48-C连接的多聚泛素测量的实验解折叠力高度吻合,特别是表明后一种情况下的解折叠力要低得多。情况(A)中的机械解折叠涉及末端平行链的纵向剪切,而在情况(C)中,相同的链被力“拉开”。发现情况(C)中的计算解折叠力非常低,对于AFM实验典型的拉伸速率,小于50 pN。在情况(C)中发现的解折叠自由能势垒约为13 kcal/mol,这对应于一个零力解折叠速率常数,该常数与外推到零变性剂浓度的化学解折叠速率相当。在零力极限下情况(A)中计算的解折叠势垒要高得多,这表明这种情况下的机械解折叠遵循的途径与热/化学变性不同。