Low-temperature molecular dynamics simulations of horse heart cytochrome c and comparison with inelastic neutron scattering data

被引:7
|
作者
Pulawski, Wojciech [1 ]
Filipek, Slawomir [1 ]
Zwolinska, Anna [2 ,3 ]
Debinski, Aleksander [1 ]
Krzysko, Krystiana [3 ,4 ]
Garduno-Juarez, Ramon [5 ]
Viswanathan, Sowmya [6 ]
Renugopalakrishnan, Venkatesan [7 ,8 ]
机构
[1] Univ Warsaw, Fac Chem, PL-02093 Warsaw, Poland
[2] Med Univ Warsaw, Fac Pharm, PL-02097 Warsaw, Poland
[3] Int Inst Mol & Cell Biol, PL-02109 Warsaw, Poland
[4] Univ Warsaw, Fac Phys, CoE BioExploratorium, PL-02089 Warsaw, Poland
[5] Univ Nacl Autonoma Mexico, Inst Ciencias Fis, Cuernavaca 62210, Morelos, Mexico
[6] Wellesley Hosp Partners Healthcare Syst, Newton, MA 02462 USA
[7] Harvard Univ, Sch Med, Childrens Hosp, Boston, MA 02115 USA
[8] Northeastern Univ, Dept Chem & Chem Biol, Boston, MA 02115 USA
来源
EUROPEAN BIOPHYSICS JOURNAL WITH BIOPHYSICS LETTERS | 2013年 / 42卷 / 04期
关键词
Cytochrome c; Molecular dynamics; Inelastic neutron scattering; Dynamic structure factor; FREQUENCY RAMAN-SPECTRA; CONFORMATIONAL PROBE; PROTEIN DYNAMICS; WATER; SPECTROSCOPY; ALGORITHM; ENERGY; MOTION; CHAIN; MODE;
D O I
10.1007/s00249-012-0874-9
中图分类号
Q6 [生物物理学];
学科分类号
071011 ;
摘要
Molecular dynamics (MD) simulation combined with inelastic neutron scattering can provide information about the thermal dynamics of proteins, especially the low-frequency vibrational modes responsible for large movement of some parts of protein molecules. We performed several 30-ns MD simulations of cytochrome c (Cyt c) in a water box for temperatures ranging from 110 to 300 K and compared the results with those from experimental inelastic neutron scattering. The low-frequency vibrational modes were obtained via dynamic structure factors, S(Q, omega), obtained both from inelastic neutron scattering experiments and calculated from MD simulations for Cyt c in the same range of temperatures. The well known thermal transition in structural movements of Cyt c is clearly seen in MD simulations; it is, however, confined to unstructured fragments of loops Omega(1) and Omega(2); movement of structured loop Omega(3) and both helical ends of the protein is resistant to thermal disturbance. Calculated and experimental S(Q, omega) plots are in qualitative agreement for low temperatures whereas above 200 K a boson peak vanishes from the calculated plots. This may be a result of loss of crystal structure by the protein-water system compared with the protein crystal.
引用
收藏
页码:291 / 300
页数:10
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