Combining Molecular and Spin Dynamics Simulations with Solid-State NMR: A Case Study of Amphiphilic Lysine–Leucine Repeat Peptide Aggregates
Combining Molecular and Spin Dynamics Simulations with Solid-State NMR: A Case Study of Amphiphilic Lysine–Leucine Repeat Peptide Aggregates
复制标题
将分子和自旋动力学模拟与固态 NMR 相结合:两亲性赖氨酸-亮氨酸重复肽聚集体的案例研究
DOI:
10.1021/acs.jpcb.9b09245
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发表时间:
2019
期刊:
影响因子:
--
通讯作者:
Drobny, Gary P.
中科院分区:
文献类型:
--
作者:
Emani, Prashant S.;Yimer, Yeneneh Y.;Davidowski, Stephen K.;Gebhart, Rachel N.;Ferreira, Helen E.;Kuprov, Ilya;Pfaendtner, Jim;Drobny, Gary P.
Interpreting dynamics in solid-state molecular systems requires characterization of the potentially heterogeneous environmental contexts of molecules. In particular, the analysis of solid-state nuclear magnetic resonance (ssNMR) data to elucidate molecular dynamics (MD) involves modeling the restriction to overall tumbling by neighbors, as well as the concentrations of water and buffer. In this exploration of the factors that influence motion, we utilize atomistic MD trajectories of peptide aggregates with varying hydration to mimic an amorphous solid-state environment and predict ssNMR relaxation rates. We also account for spin diffusion in multiply spin-labeled (up to 19 nuclei) residues, with several models of dipolar-coupling networks. The framework serves as a general approach to determine essential spin couplings affecting relaxation, benchmark MD force fields, and reveal the hydration dependence of dynamics in a crowded environment. We demonstrate the methodology on a previously characterized amphiphilic 14-residue lysine–leucine repeat peptide, LKα14 (Ac-LKKLLKLLKKLLKL-c), which has an α-helical secondary structure and putatively forms leucine-burying tetramers in the solid state. We measure the R1relaxation rates of uniformly13C-labeled and site-specific2H-labeled leucines in the hydrophobic core of LKα14 at multiple hydration levels. Studies of 9 and 18 tetramer bundles reveal the following: (a) for the incoherent component of13C relaxation, the nearest-neighbor spin interactions dominate, while the1H–1H interactions have minimal impact; (b) the AMBER ff14SB dihedral barriers for the leucine Cγ–Cδbond (“methyl rotation barriers”) must be lowered by a factor of 0.7 to better match the2H data; (c) proton-driven spin diffusion explains some of the discrepancy between experimental and simulated rates for the Cβand Cαnuclei; and (d)13C relaxation rates are mostly underestimated in the MD simulations at all hydrations, and the discrepancies identify likely motions missing in the 50 ns MD trajectories.