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Low-temperature molecular dynamics simulations of horse heart cytochrome c and comparison with inelastic neutron scattering data
Authors:Wojciech Pulawski  Slawomir Filipek  Anna Zwolinska  Aleksander Debinski  Krystiana Krzysko  Ramón Garduño-Juárez  Sowmya Viswanathan  Venkatesan Renugopalakrishnan
Institution:1. Faculty of Chemistry, University of Warsaw, ul. Pasteura 1, 02-093, Warsaw, Poland
2. Faculty of Pharmacy, Medical University of Warsaw, ul. Banacha 1, 02-097, Warsaw, Poland
3. International Institute of Molecular and Cell Biology, ul. Trojdena 4, 02-109, Warsaw, Poland
4. Faculty of Physics, CoE BioExploratorium, University of Warsaw, ul. Zwirki i Wigury 93, 02-089, Warsaw, Poland
5. Instituto de Ciencias Físicas, Universidad Nacional Autónoma de México, 62210, Cuernavaca, Morelos, Mexico
6. Wellesley Hospital/Partners Healthcare System, Newton, MA, 02462, USA
7. Children’s Hospital, Harvard Medical School, 300 Longwood Ave., Boston, MA, 02115, USA
8. Department of Chemistry and Chemical Biology, Northeastern University, Boston, MA, 02115, USA
9. Children’s Hospital, Harvard Medical School, 20 Shattuck Street, Boston, MA, 02115, USA
Abstract: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, ω), 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 Ω1 and Ω2; movement of structured loop Ω3 and both helical ends of the protein is resistant to thermal disturbance. Calculated and experimental S(Qω) 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.
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