Supporting Information
|
|
- Natalie Jefferson
- 5 years ago
- Views:
Transcription
1 Supporting Information Energies and 2 -hydroxyl group orientations of RNA backbone conformations. Benchmark CCSD(T)/CBS database, electronic analysis and assessment of DFT methods and MD simulations Arnošt Mládek,* 1 Pavel Banáš, 2 Petr Jurečka, 2 Michal Otyepka, 2 Marie Zgarbová, 2 and Jiří Šponer* 1,3 1 Institute of Biophysics, Academy of Sciences of the Czech Republic, Královopolská 135, Brno, Czech Republic. 2 Regional Centre of Advanced Technologies and Materials, Department of Physical Chemistry, Faculty of Science, Palacky University, tr. 17. listopadu 12, , Olomouc, Czech Republic. 3 CEITEC Central European Institute of Technology, Campus Bohunice, Kamenice 5, Brno, Czech Republic. * Corresponding authors: arnost.mladek@gmail.com, sponer@ncbr.muni.cz
2 Table S1 List of solvent relative energies (kcal.mol -1 ) referenced against the 1a conformation. Applied methods are tagged as follows: M1: B-LYP, M2: PBE, M3: revpbe, M4: TPSS, M5: otpss, M6: B3-LYP, M7: PW6B95, M8: MPW1B95, M9: PWPB95, M10: DSD-B- LYP, M11: MP2(D,T), and M12: MP2(T,Q). For further details see Methods. MAD and MAX (both in kcal.mol -1 ) represent the mean absolute deviation and the maximum absolute deviation from the reference CBS(T) energies. MM labels force field calculations. Listed DFT energies include D3 correction; MAD and MAX values are quoted for DFs with and without D3 term. Label GGA meta-gga Hybrid Double-Hyb. MP2/CBS M1 M2 M3 M4 M5 M6 M7 M8 M9 M10 M11 M12 CBS(T) MM 1a m L &a a a a g d d d e c f j b [ b z z p t q o r a a a #a g g d d d h n i n j [ b b p p s o MAD- D MAX- D N/A N/A N/A MAD MAX
3 Table S2 List of O2 H group acceptors and respective H-bond strengths estimated by AIM analysis for RNA backbone conformations. The (i+1) designates that respective H-bond acceptor belongs to the i+1-th (i.e. 5-3 downstream) nucleotide. Electronic densities (ρ) and magnitudes of electronic density Laplacians ( ρ) at the H-bond critical point are given in a.u. δ, δ + 1, γ + 1 Group Label ρ ρ O2 H Acceptor 1a O3 1m O3 1L O3 &a O5 (i+1) O4 (i+1) 3, 3, p 7a O3 3a O3 Group I 9a O3 1g O3 7d O3 3d O3 5d O3 1e O4 (i+1) 3, 3, t 1c O5 (i+1) 1f O5 (i+1) 5j O3 1b O3 1[ O3 3, 2, p 3b O3 1z O3 Group II 5z O2P (i+1) 7p O3 3, 2, t 1t O5 (i+1) 5q O3 3, 2, m 1o O3 7r O3 2a O3 4a O3 0a O1P (i+1) O3 2, 3, p #a O1P (i+1) 4g O3 Group III 6g O3 8d O3 4d O3 6d O3 2h O3 2, 3, t 4n O1P (i+1) 0i O3 6n O3
4 6j O3 2[ O3 4b O3 2, 2, p 0b O3 Group IV 4p O3 6p O3 2, 2, t 4s O3 2, 2, m 2o O3 Comment on MD simulation protocol The simulation protocol was as follows both systems (SRL and glms, for more details see main text) were minimized, by first optimizing the waters and ions, while the positions of the RNA molecule remained constrained. Subsequently, all RNA atoms were frozen and the solvent molecules with counter-ions were allowed to move during a 1000-step minimization, followed by 10 ps long MD runs under [NpT] conditions (p = 1 atm., T = K) in order to relax the total density. After this, the solute and nucleobases were relaxed by several minimization runs, with decreasing force constants applied to the sugar-phosphate backbone atoms. After the relaxation, each system was heated from K to K for 100 ps. The particle-mesh Ewald (PME) method for treating electrostatic interactions was used, and all simulations were performed under periodic boundary conditions in the [NpT] ensemble at K using weak-coupling Berendsen thermostat with coupling time of 1 ps. The SHAKE algorithm, with a tolerance of 10 5 Å, was used to fix the positions of all hydrogen atoms, and a 10.0 Å cutoff was applied to non-bonding interactions to allow a 2 fs integration step. The simulation lengths of production phases of the simulations were 1 µs.
5 Figure S1 Hydroxyl group rotation energy profiles (kcal.mol -1 ). The zero energy refers to C3 -C2 -O2 -O2 H torsion of 180. The sequence of conformations corresponds to that in Table 1 in the main text. For methodology details, see Methods in the main text.
6
7
8
9
10
11
12
13
14
15
16
17 Cartesian coordinates (xyz format) of the conformations optimized in gas phase with respective relative CBS(T) energies (kcal.mol -1 ). System: 1a, CBS(T): 0.00 C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 1m, CBS(T): C C O C C O C O P O O
18 O C C O C C C O H H H H H H H H H H H H H H H H H H System: 1L, CBS(T): 2.60 C C O C C O C O P O O O C C O C C C O H H H H H H H H H
19 H H H H H H H H H System: &a, CBS(T): C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 7a, CBS(T): 1.20 C C O C C
20 O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 3a, CBS(T): 0.64 C C O C C O C O P O O O C C O C C C O H H H
21 H H H H H H H H H H H H H H H System: 9a, CBS(T): 0.56 C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H
22 System: 1g, CBS(T): 0.89 C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 7d, CBS(T): C C O C C O C O P O O O C C O C
23 C C O H H H H H H H H H H H H H H H H H H System: 3d, CBS(T): 1.04 C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H
24 H H H H System: 5d, CBS(T): 0.60 C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 1e, CBS(T): 1.92 C C O C C O C O P O
25 O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 1c, CBS(T): 1.22 C C O C C O C O P O O O C C O C C C O H H H H H H H H
26 H H H H H H H H H H System: 1f, CBS(T): 2.15 C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 5j, CBS(T): 4.75 C C O C
27 C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 1b, CBS(T): C C O C C O C O P O O O C C O C C C O H H
28 H H H H H H H H H H H H H H H H System: 1[, CBS(T): C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H
29 System: 3b, CBS(T): C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 1z, CBS(T): C C O C C O C O P O O O C C O
30 C C C O H H H H H H H H H H H H H H H H H H System: 5z, CBS(T): C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H
31 H H H H H System: 7p, CBS(T): C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 1t, CBS(T): 2.45 C C O C C O C O P
32 O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 5q, CBS(T): 3.19 C C O C C O C O P O O O C C O C C C O H H H H H H H
33 H H H H H H H H H H H System: 1o, CBS(T): 0.11 C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 7r, CBS(T): 0.77 C C O
34 C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 2a, CBS(T): C C O C C O C O P O O O C C O C C C O H
35 H H H H H H H H H H H H H H H H H System: 4a, CBS(T): 1.06 C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H
36 System: 0a, CBS(T): 0.52 C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: #a, CBS(T): 0.05 C C O C C O C O P O O O C C
37 O C C C O H H H H H H H H H H H H H H H H H H System: 4g, CBS(T): 3.62 C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H
38 H H H H H H System: 6g, CBS(T): C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 8d, CBS(T): 1.69 C C O C C O C O
39 P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 4d, CBS(T): 1.63 C C O C C O C O P O O O C C O C C C O H H H H H H
40 H H H H H H H H H H H H System: 6d, CBS(T): 1.99 C C O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 2h, CBS(T): 3.10 C C
41 O C C O C O P O O O C C O C C C O H H H H H H H H H H H H H H H H H H System: 4n, CBS(T): 6.51 C C O C C O C O P O O O C C O C C C O
Supporting Information. Chemical Feasibility of the General Acid/Base Mechanism of glms Ribozyme Self-Cleavage
Supporting Information to Chemical Feasibility of the General Acid/Base Mechanism of glms Ribozyme Self-Cleavage Matúš Dubecký, 1 Nils G. Walter, 2 Jiří Šponer, 3,4 Michal Otyepka 1 and Pavel Banáš *,1,3
More informationTailoring the Properties of Quadruplex Nucleobases for Biological and Nanomaterial Applications
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2014 Supporting Information for: Tailoring the Properties of Quadruplex Nucleobases
More informationNucleotides containing variously modified sugars: energetics, structure, and mechanical properties
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2015 ELECTRONIC SUPPLEMENTARY INFORMATION Nucleotides containing variously modified
More informationStructure and Dynamics of Chitin Nanofibrils in Aqueous Environment Revealed by Molecular Dynamics Simulations
Electronic Supplementary Material (ESI) for RSC Advances. This journal is The Royal Society of Chemistry 2016 Structure and Dynamics of Chitin Nanofibrils in Aqueous Environment Revealed by Molecular Dynamics
More informationPerformance of Molecular Mechanics Force Fields for RNA Simulations: Stability of UUCG and GNRA Hairpins
3836 J. Chem. Theory Comput. 2010, 6, 3836 3849 Performance of Molecular Mechanics Force Fields for RNA Simulations: Stability of UUCG and GNRA Hairpins Pavel Banáš,, Daniel Hollas, Marie Zgarbová, Petr
More informationSANDRO BOTTARO, PAVEL BANÁŠ, JIŘÍ ŠPONER, AND GIOVANNI BUSSI
FREE ENERGY LANDSCAPE OF GAGA AND UUCG RNA TETRALOOPS. SANDRO BOTTARO, PAVEL BANÁŠ, JIŘÍ ŠPONER, AND GIOVANNI BUSSI Contents 1. Supplementary Text 1 2 Sample PLUMED input file. 2. Supplementary Figure
More informationWith the advance of fast computers, explicit solvent
pubs.acs.org/jpcl Terms of Use Molecular Dynamics Simulations of Nucleic Acids. From Tetranucleotides to the Ribosome Jir í S poner,*,, Pavel Banaś, Petr Jurecǩa, Marie Zgarbova, Petra Kuḧrova, Marek Havrila,,
More informationUniversal Repulsive Contribution to the. Solvent-Induced Interaction Between Sizable, Curved Hydrophobes: Supporting Information
Universal Repulsive Contribution to the Solvent-Induced Interaction Between Sizable, Curved Hydrophobes: Supporting Information B. Shadrack Jabes, Dusan Bratko, and Alenka Luzar Department of Chemistry,
More informationPotential Energy Surface and Binding Energy in External Electric Field: Modulation of Anion π Interactions for Graphene Based Receptors
Potential Energy Surface and Binding Energy in External Electric Field: Modulation of Anion π Interactions for Graphene Based Receptors Cina Foroutan Nejad a and Radek Marek a,b a National Center for Biomolecular
More informationInteraction energy of DNA base pairs and amino acid pairs: DFT, DFTB and WFT calculations
Interaction energy of DNA base pairs and amino acid pairs: DFT, DFTB and WFT calculations Tomáš Kubař, Petr Jurečka, Jirka Černý, Honza Řezáč, Michal Otyepka, Haydée Valdés and Pavel Hobza* Institute of
More informationThiourea Derivatives as Brønsted Acid Organocatalysts
Supporting Information Thiourea Derivatives as Brønsted Acid Organocatalysts Ádám Madarász, Zsolt Dósa, Szilárd Varga, * Tibor Soós, Antal Csámpai, Imre Pápai * Institute of Organic Chemistry, Research
More informationHands-on : Model Potential Molecular Dynamics
Hands-on : Model Potential Molecular Dynamics OUTLINE 0. DL_POLY code introduction 0.a Input files 1. THF solvent molecule 1.a Geometry optimization 1.b NVE/NVT dynamics 2. Liquid THF 2.a Equilibration
More informationWhy Proteins Fold? (Parts of this presentation are based on work of Ashok Kolaskar) CS490B: Introduction to Bioinformatics Mar.
Why Proteins Fold? (Parts of this presentation are based on work of Ashok Kolaskar) CS490B: Introduction to Bioinformatics Mar. 25, 2002 Molecular Dynamics: Introduction At physiological conditions, the
More informationAdvanced in silico drug design
Advanced in silico drug design RNDr. Martin Lepšík, Ph.D. Lecture: Advanced scoring Palacky University, Olomouc 2016 1 Outline 1. Scoring Definition, Types 2. Physics-based Scoring: Master Equation Terms
More informationIntroduction. Claudio A. Morgado,, Petr Jurečka,, Daniel Svozil, Pavel Hobza,, and
1524 J. Chem. Theory Comput. 2009, 5, 1524 1544 Balance of Attraction and Repulsion in Nucleic-Acid Base Stacking: CCSD(T)/Complete-Basis-Set-Limit Calculations on Uracil Dimer and a Comparison with the
More informationARTICLE IN PRESS. Methods xxx (2009) xxx xxx. Contents lists available at ScienceDirect. Methods. journal homepage:
Methods xxx (2009) xxx xxx Contents lists available at ScienceDirect Methods journal homepage: www.elsevier.com/locate/ymeth Review Article Theoretical studies of RNA catalysis: Hybrid QM/MM methods and
More informationONETEP PB/SA: Application to G-Quadruplex DNA Stability. Danny Cole
ONETEP PB/SA: Application to G-Quadruplex DNA Stability Danny Cole Introduction Historical overview of structure and free energy calculation of complex molecules using molecular mechanics and continuum
More informationHyeyoung Shin a, Tod A. Pascal ab, William A. Goddard III abc*, and Hyungjun Kim a* Korea
The Scaled Effective Solvent Method for Predicting the Equilibrium Ensemble of Structures with Analysis of Thermodynamic Properties of Amorphous Polyethylene Glycol-Water Mixtures Hyeyoung Shin a, Tod
More informationMedical Research, Medicinal Chemistry, University of Leuven, Leuven, Belgium.
Supporting Information Towards peptide vaccines against Zika virus: Immunoinformatics combined with molecular dynamics simulations to predict antigenic epitopes of Zika viral proteins Muhammad Usman Mirza
More informationFolding of guanine quadruplex molecules funnel-like mechanism or kinetic partitioning? An overview from MD simulation studies.
Folding of guanine quadruplex molecules funnel-like mechanism or kinetic partitioning? An overview from MD simulation studies. Jiří Šponer, a,b * Giovanni Bussi, c Petr Stadlbauer, a,b Petra Kührová, b
More informationRoutine access to millisecond timescale events with accelerated molecular dynamics
Routine access to millisecond timescale events with accelerated molecular dynamics Levi C.T. Pierce, Romelia Salomon-Ferrer, Cesar Augusto F. de Oliveira #, J. Andrew McCammon #, Ross C. Walker * SUPPORTING
More informationPCCP Accepted Manuscript
PCCP Accepted Manuscript This is an Accepted Manuscript, which has been through the Royal Society of Chemistry peer review process and has been accepted for publication. Accepted Manuscripts are published
More information- 1 - Institute of Organic Chemistry and Biochemistry AS CR, v.v.i., Flemingovo náměstí 2, CZ, Praha, Czech Republic
Electronic Supplementary Material (ESI) for RSC Advances. This journal is The Royal Society of Chemistry 2014-1 - The activation of N-glycosidic bond cleavage operated by base-excision repair enzyme hogg1;
More informationSupporting Information
Supporting Information ph-responsive self-assembly of polysaccharide through a rugged energy landscape Brian H. Morrow, Gregory F. Payne, and Jana Shen Department of Pharmaceutical Sciences, School of
More informationComputational Modeling of Protein Kinase A and Comparison with Nuclear Magnetic Resonance Data
Computational Modeling of Protein Kinase A and Comparison with Nuclear Magnetic Resonance Data ABSTRACT Keyword Lei Shi 1 Advisor: Gianluigi Veglia 1,2 Department of Chemistry 1, & Biochemistry, Molecular
More informationForce Field for Water Based on Neural Network
Force Field for Water Based on Neural Network Hao Wang Department of Chemistry, Duke University, Durham, NC 27708, USA Weitao Yang* Department of Chemistry, Duke University, Durham, NC 27708, USA Department
More informationHairpins Participating in Folding of Human Telomeric Sequence Quadruplexes Studied by Standard and T-REMD Simulations
Hairpins Participating in Folding of Human Telomeric Sequence Quadruplexes Studied by Standard and T-REMD Simulations Petr Stadlbauer 1, Petra Kührová 2, Pavel Banáš 2, Jaroslav Koča 3,4, Giovanni Bussi
More informationSupporting Information
Supporting Information Constant ph molecular dynamics reveals ph-modulated binding of two small-molecule BACE1 inhibitors Christopher R. Ellis 1,, Cheng-Chieh Tsai 1,, Xinjun Hou 2, and Jana Shen 1, 1
More informationType II Kinase Inhibitors Show an Unexpected Inhibition Mode against Parkinson s Disease-Linked LRRK2 Mutant G2019S.
Type II Kinase Inhibitors Show an Unexpected Inhibition Mode against Parkinson s Disease-Linked LRRK2 Mutant G219S. Min Liu@&*, Samantha A. Bender%*, Gregory D Cuny@, Woody Sherman, Marcie Glicksman@ Soumya
More informationSupplementary Information for Electronic signature of the instantaneous asymmetry in the first coordination shell in liquid water
Supplementary Information for Electronic signature of the instantaneous asymmetry in the first coordination shell in liquid water Thomas D. Kühne 1, 2 and Rustam Z. Khaliullin 1, 1 Institute of Physical
More informationPotential Energy (hyper)surface
The Molecular Dynamics Method Thermal motion of a lipid bilayer Water permeation through channels Selective sugar transport Potential Energy (hyper)surface What is Force? Energy U(x) F = " d dx U(x) Conformation
More informationMolecular dynamics simulations of a single stranded (ss) DNA
Molecular dynamics simulations of a single stranded (ss) DNA Subhasish Chatterjee 1, Bonnie Gersten 1, Siddarth Thakur 2, Alexander Burin 2 1 Department of Chemistry, Queens College and the Graduate Center
More informationApplications of the van der Waals density functional: DNA and metal organic framework materials. Chalmers
Applications of the van der Waals density functional: DNA and metal organic framework materials Valentino R. Cooper Chalmers Svetla Chakarova-Käck Per Hyldgaard Jesper Kleis Henrik Rydberg Elsebeth Schröder
More informationJournal of Pharmacology and Experimental Therapy-JPET#172536
A NEW NON-PEPTIDIC INHIBITOR OF THE 14-3-3 DOCKING SITE INDUCES APOPTOTIC CELL DEATH IN CHRONIC MYELOID LEUKEMIA SENSITIVE OR RESISTANT TO IMATINIB Manuela Mancini, Valentina Corradi, Sara Petta, Enza
More informationXYZ file format Protein Data Bank (pdb) file format Z - matrix
Chemistry block (exercise 1) In this exercise, students will be introduced how to preform simple quantum chemical calculations. Input files for Gaussian09. Output file structure. Geometry optimization,
More informationDoping with Graphitic Nitrogen Triggers Ferromagnetism in Graphene
Supporting Information for Doping with Graphitic Nitrogen Triggers Ferromagnetism in Graphene Piotr Błoński, Jiří Tuček, Zdeněk Sofer, Vlastimil Mazánek, Martin Petr, Martin Pumera, Michal Otyepka, and
More informationSUPPLEMENTARY MATERIAL. Supplementary material and methods:
Electronic Supplementary Material (ESI) for Catalysis Science & Technology. This journal is The Royal Society of Chemistry 2015 SUPPLEMENTARY MATERIAL Supplementary material and methods: - Computational
More informationTowards accurate calculations of Zn 2+ binding free energies in zinc finger proteins
Towards accurate calculations of Zn 2+ binding free energies in zinc finger proteins UNDERGRADUATE HONORS RESEARCH THESIS Presented in Partial Fulfillment of the Requirements for the Bachelor of Science
More informationSupplementary material. From cellulose to kerogen: molecular simulation. of a geological process
Electronic Supplementary Material (ESI) for Chemical Science. This journal is The Royal Society of Chemistry 2017 Supplementary material From cellulose to kerogen: molecular simulation of a geological
More informationHairpins participating in folding of human telomeric sequence quadruplexes studied by standard and T-REMD simulations
Nucleic Acids Research Advance Access published October 3, 2015 Nucleic Acids Research, 2015 1 doi: 10.1093/nar/gkv994 Hairpins participating in folding of human telomeric sequence quadruplexes studied
More informationDesign of Efficient Catalysts with Double Transition Metal. Atoms on C 2 N Layer
Supporting Information Design of Efficient Catalysts with Double Transition Metal Atoms on C 2 N Layer Xiyu Li, 1, Wenhui Zhong, 2, Peng Cui, 1 Jun Li, 1 Jun Jiang 1, * 1 Hefei National Laboratory for
More informationMolecular Dynamics Simulations. Dr. Noelia Faginas Lago Dipartimento di Chimica,Biologia e Biotecnologie Università di Perugia
Molecular Dynamics Simulations Dr. Noelia Faginas Lago Dipartimento di Chimica,Biologia e Biotecnologie Università di Perugia 1 An Introduction to Molecular Dynamics Simulations Macroscopic properties
More informationSupplementary Materials
Supplementary Materials Atomistic Origin of Brittle Failure of Boron Carbide from Large Scale Reactive Dynamics Simulations; Suggestions toward Improved Ductility Qi An and William A. Goddard III * Materials
More information2008 Biowerkzeug Ltd.
2008 Biowerkzeug Ltd. 1 Contents Summary...3 1 Simulation...4 1.1 Setup...4 1.2 Output...4 2 Settings...5 3 Analysis...9 3.1 Setup...9 3.2 Input options...9 3.3 Descriptions...10 Please note that we cannot
More informationDFT STUDY OF Co 2+ AND Fe 2+ - URACIL COMPLEXES IN THE GAS PHASE
INTERNATIONAL JOURNAL OF RESEARCH IN PHARMACY AND CHEMISTRY Available online at www.ijrpc.com Research Article DFT STUDY OF Co 2+ AND Fe 2+ - URACIL COMPLEXES IN THE GAS PHASE Raghab Parajuli* Department
More informationMolecular dynamics simulation of Aquaporin-1. 4 nm
Molecular dynamics simulation of Aquaporin-1 4 nm Molecular Dynamics Simulations Schrödinger equation i~@ t (r, R) =H (r, R) Born-Oppenheimer approximation H e e(r; R) =E e (R) e(r; R) Nucleic motion described
More informationWATER PERMEATION THROUGH GRAPHENE NANOSLIT BY MOLECULAR DYNAMICS SIMULATION
WATER PERMEATION THROUGH GRAPHENE NANOSLIT BY MOLECULAR DYNAMICS SIMULATION Taro Yamada 1 and Ryosuke Matsuzaki 2 1 Department of Mechanical Engineering, Tokyo University of Science, 2641 Yamazaki, Noda,
More informationSupporting Information Synthesis of (D)-erythrose from glycolaldehyde aqueous solutions under electric field
Electronic Supplementary Material (ESI) for ChemComm. This journal is The Royal Society of Chemistry 2018 Supporting Information Synthesis of (D)-erythrose from glycolaldehyde aqueous solutions under electric
More informationSynergy between NMR measurements and MD simulations of protein/rna complexes: application to the RRMs, the most common RNA recognition motifs
6452 6470 Nucleic Acids Research, 2016, Vol. 44, No. 13 Published online 18 May 2016 doi: 10.1093/nar/gkw438 Synergy between NMR measurements and MD simulations of protein/rna complexes: application to
More informationClassification and Energetics of the Base-Phosphate Interactions in RNA
Bowling Green State University ScholarWorks@BGSU Chemistry Faculty Publications Chemistry 8-2009 Classification and Energetics of the Base-Phosphate Interactions in RNA Craig L. Zirbel Bowling Green State
More informationDISCRETE TUTORIAL. Agustí Emperador. Institute for Research in Biomedicine, Barcelona APPLICATION OF DISCRETE TO FLEXIBLE PROTEIN-PROTEIN DOCKING:
DISCRETE TUTORIAL Agustí Emperador Institute for Research in Biomedicine, Barcelona APPLICATION OF DISCRETE TO FLEXIBLE PROTEIN-PROTEIN DOCKING: STRUCTURAL REFINEMENT OF DOCKING CONFORMATIONS Emperador
More informationA conserved P-loop anchor limits the structural dynamics that mediate. nucleotide dissociation in EF-Tu.
Supplemental Material for A conserved P-loop anchor limits the structural dynamics that mediate nucleotide dissociation in EF-Tu. Evan Mercier 1,2, Dylan Girodat 1, and Hans-Joachim Wieden 1 * 1 Alberta
More informationMARTINI simulation details
S1 Appendix MARTINI simulation details MARTINI simulation initialization and equilibration In this section, we describe the initialization of simulations from Main Text section Residue-based coarsegrained
More informationPeptide folding in non-aqueous environments investigated with molecular dynamics simulations Soto Becerra, Patricia
University of Groningen Peptide folding in non-aqueous environments investigated with molecular dynamics simulations Soto Becerra, Patricia IMPORTANT NOTE: You are advised to consult the publisher's version
More informationS66: A Well-balanced Database of Benchmark Interaction Energies Relevant to Biomolecular Structures
pubs.acs.org/jctc S66: A Well-balanced Database of Benchmark Interaction Energies Relevant to Biomolecular Structures Jan Rezac,*, Kevin E. Riley, and Pavel Hobza, Institute of Organic Chemistry and Biochemistry,
More informationMethods for van der Waals Interactions
Methods for van der Waals Interactions Alexandre Tkatchenko Theory Department, Fritz Haber Institut der MPG Berlin, Germany tkatchen@fhi berlin.mpg.de Haber Institute FHI DFT and Beyond Workshop, Jul.
More informationSimulation of molecular systems by molecular dynamics
Simulation of molecular systems by molecular dynamics Yohann Moreau yohann.moreau@ujf-grenoble.fr November 26, 2015 Yohann Moreau (UJF) Molecular Dynamics, Label RFCT 2015 November 26, 2015 1 / 35 Introduction
More informationSUPPLEMENTARY INFORMATION
DOI: 10.1038/NCHEM.1680 On the nature and origin of dicationic, charge-separated species formed in liquid water on X-ray irradiation Stephan Thürmer, 1 Milan Ončák, 2 Niklas Ottosson, 3 Robert Seidel,
More informationSupplementary Information
Electronic Supplementary Material (ESI) for New Journal of Chemistry. This journal is The Royal Society of Chemistry and the Centre National de la Recherche Scientifique 2018 Supplementary Information
More informationSupporting Material for. Microscopic origin of gating current fluctuations in a potassium channel voltage sensor
Supporting Material for Microscopic origin of gating current fluctuations in a potassium channel voltage sensor J. Alfredo Freites, * Eric V. Schow, * Stephen H. White, and Douglas J. Tobias * * Department
More informationCanadian Journal of Chemistry. The INV24 Test Set: How Well do Quantum-Chemical Methods Describe Inversion and Racemization Barriers?
The INV24 Test Set: How Well do Quantum-Chemical Methods Describe Inversion and Racemization Barriers? Journal: Manuscript ID cjc-2016-0290.r1 Manuscript Type: Article Date Submitted by the Author: 15-Jul-2016
More informationUnit Cell-Level Thickness Control of Single-Crystalline Zinc Oxide Nanosheets Enabled by Electrical Double Layer Confinement
Unit Cell-Level Thickness Control of Single-Crystalline Zinc Oxide Nanosheets Enabled by Electrical Double Layer Confinement Xin Yin, Yeqi Shi, Yanbing Wei, Yongho Joo, Padma Gopalan, Izabela Szlufarska,
More informationMolecular Dynamics. A very brief introduction
Molecular Dynamics A very brief introduction Sander Pronk Dept. of Theoretical Physics KTH Royal Institute of Technology & Science For Life Laboratory Stockholm, Sweden Why computer simulations? Two primary
More informationVan der Waals interactions in DFT
Van der Waals interactions in DFT Maxime Dion*, Aaron Puzder*, T. Thonhauser,* Valentino R. Cooper*, Shen Li*, Eamonn Murray, Lingzhu Kong, Kyuho Lee, and David C. Langreth Department of Physics and Astronomy,
More informationProblem Set 1
2006 7.012 Problem Set 1 Due before 5 PM on FRIDAY, September 15, 2006. Turn answers in to the box outside of 68-120. PLEASE WRITE YOUR ANSWERS ON THIS PRINTOUT. 1. For each of the following parts, pick
More informationConformations of Flanking Bases in HIV-1 RNA DIS Kissing Complexes Studied by Molecular Dynamics
3932 Biophysical Journal Volume 93 December 2007 3932 3949 Conformations of Flanking Bases in HIV-1 RNA DIS Kissing Complexes Studied by Molecular Dynamics Kamila Réblová,* Eva Fadrná, y Joanna Sarzynska,
More informationSmall Details Matter: The 2 -Hydroxyl as a Conformational Switch in RNA
Small Details Matter: The 2 -Hydroxyl as a Conformational Switch in RNA Leonardo Darré 1,2, Ivan Ivani 1,2, Pablo D. Dans 1,2, Hansel Gómez 1,2, Adam Hospital 1,2 and Modesto Orozco 1,2,3 * 1 Institute
More informationExplicit Ion, Implicit Water Solvation for Molecular Dynamics of Nucleic Acids and Highly Charged Molecules
Explicit Ion, Implicit Water Solvation for Molecular Dynamics of Nucleic Acids and Highly Charged Molecules NINAD V. PRABHU, 1 MANORANJAN PANDA, 2 QINGYI YANG, 3 KIM A. SHARP 3 1 Schering-Plough, Kenilworth,
More informationIntroductory Biochemistry
Introductory Biochemistry Instructors Dr. Nafez Abu Tarboush Dr. Mamoun Ahram Recommended textbooks Biochemistry; Mary K. Campbell and Shawn O. Farrell, Brooks Cole; 6 th edition Recommended electronic
More informationSupplementary Information for Atomistic Simulation of Spinodal Phase Separation Preceding Polymer Crystallization
Supplementary Information for Atomistic Simulation of Spinodal Phase Separation Preceding Polymer Crystallization Richard H. Gee * Naida Lacevic and Laurence E. Fried University of California Lawrence
More informationStructures of the Molecular Components in DNA and RNA with Bond Lengths Interpreted as Sums of Atomic Covalent Radii
The Open Structural Biology Journal, 2008, 2, 1-7 1 Structures of the Molecular Components in DNA and RNA with Bond Lengths Interpreted as Sums of Atomic Covalent Radii Raji Heyrovska * Institute of Biophysics
More informationPseudopotentials for hybrid density functionals and SCAN
Pseudopotentials for hybrid density functionals and SCAN Jing Yang, Liang Z. Tan, Julian Gebhardt, and Andrew M. Rappe Department of Chemistry University of Pennsylvania Why do we need pseudopotentials?
More informationACMAC s PrePrint Repository
ACMAC s PrePrint Repository Properties of short polystyrene chains confined between two Gold surfaces through a combined Density Functional Theory and classical Molecular Dynamics approach Karen Johnston
More informationMM-PBSA Validation Study. Trent E. Balius Department of Applied Mathematics and Statistics AMS
MM-PBSA Validation Study Trent. Balius Department of Applied Mathematics and Statistics AMS 535 11-26-2008 Overview MM-PBSA Introduction MD ensembles one snap-shots relaxed structures nrichment Computational
More informationSupporting Information
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2016 Supporting Information Lipid molecules can induce an opening of membrane-facing
More informationRole of van der Waals Interactions in Physics, Chemistry, and Biology
Role of van der Waals Interactions in Physics, Chemistry, and Biology How can we describe vdw forces in materials accurately? Failure of DFT Approximations for (Long-Range) Van der Waals Interactions 1
More informationEvolution of Translation: Dynamics of Recognition in RNA:Protein Complexes
Evolution of Translation: Dynamics of Recognition in RNA:Protein Complexes Zaida (Zan) Luthey-Schulten Dept. Chemistry, Beckman Institute, Biophysics, Institute of Genomics Biology, & Physics NIH Workshop
More informationRanjit P. Bahadur Assistant Professor Department of Biotechnology Indian Institute of Technology Kharagpur, India. 1 st November, 2013
Hydration of protein-rna recognition sites Ranjit P. Bahadur Assistant Professor Department of Biotechnology Indian Institute of Technology Kharagpur, India 1 st November, 2013 Central Dogma of life DNA
More informationThe micro-properties of [hmpy+] [Tf 2 N-] Ionic liquid: a simulation. study. 1. Introduction
ISBN 978-1-84626-081-0 Proceedings of the 2010 International Conference on Application of Mathematics and Physics Volume 1: Advances on Space Weather, Meteorology and Applied Physics Nanjing, P. R. China,
More informationList of Figures Page Figure No. Figure Caption No. Figure 1.1.
List of Figures Figure No. Figure Caption Page No. Figure 1.1. Cation- interactions and their modulations. 4 Figure 1.2. Three conformations of benzene dimer, S is not a minimum on the potential energy
More informationLAMMPS Performance Benchmark on VSC-1 and VSC-2
LAMMPS Performance Benchmark on VSC-1 and VSC-2 Daniel Tunega and Roland Šolc Institute of Soil Research, University of Natural Resources and Life Sciences VSC meeting, Neusiedl am See, February 27-28,
More informationSupporting Information
Projection of atomistic simulation data for the dynamics of entangled polymers onto the tube theory: Calculation of the segment survival probability function and comparison with modern tube models Pavlos
More informationNoncovalent interactions in biochemistry
Noncovalent interactions in biochemistry Kevin E. Riley 1 and Pavel Hobza 2,3 Noncovalent interactions are known to play a key role in biochemistry. The knowledge of stabilization (relative) energies and
More informationApplications of Molecular Dynamics
June 4, 0 Molecular Modeling and Simulation Applications of Molecular Dynamics Agricultural Bioinformatics Research Unit, Graduate School of Agricultural and Life Sciences, The University of Tokyo Tohru
More informationImproved Resolution of Tertiary Structure Elasticity in Muscle Protein
Improved Resolution of Tertiary Structure Elasticity in Muscle Protein Jen Hsin and Klaus Schulten* Department of Physics and Beckman Institute, University of Illinois at Urbana-Champaign, Urbana, Illinois
More informationAb initio molecular dynamics
Ab initio molecular dynamics Kari Laasonen, Physical Chemistry, Aalto University, Espoo, Finland (Atte Sillanpää, Jaakko Saukkoriipi, Giorgio Lanzani, University of Oulu) Computational chemistry is a field
More informationMolecular Dynamics Simulations of Guanine Quadruplex Loops: Advances and Force Field Limitations
Biophysical Journal Volume 87 July 2004 227 242 227 Molecular Dynamics Simulations of Guanine Quadruplex Loops: Advances and Force Field Limitations Eva Fadrná,* Nad a Špačková, y Richard Štefl,* Jaroslav
More informationNWChem: Molecular Dynamics and QM/MM
NWChem: Molecular Dynamics and QM/MM Molecular Dynamics Functionality Target systems: General features: biomolecules (proteins, DNA/RNA, biomembranes) energy evaluation (SP) energy minimization (EM) molecular
More informationMolecular Dynamics. Coherency of Molecular Motions. Local Minima & Global Minimum. Theoretical Basis of Molecular Dynamic Calculations
Molecular Dynamics Molecular Dynamics provide a good approach to determine the preferred conformers and global minimum of a molecule Theoretical Basis of Molecular Dynamic Calculations Molecular dynamics
More informationSupplementary Information
Supplementary Information Resveratrol Serves as a Protein-Substrate Interaction Stabilizer in Human SIRT1 Activation Xuben Hou,, David Rooklin, Hao Fang *,,, Yingkai Zhang Department of Medicinal Chemistry
More informationJorge Kohanoff. DNA damage from first principles
DNA damage from first principles Jorge Kohanoff Atomistic Simulation Centre School of Maths and Physics Queen s University Belfast Northern Ireland UK CP2K UK Users Meeting London, 29 th January 2014 Queen
More informationSupplementary Figure 2 FF at concentration of 8 mg/ml dissolved in 100% DMSO. The molecules assemble into plate-like structures. Scale bar is 50 µm.
1 2 3 4 5 6 7 8 9 10 11 Supplementary Figure 1 Microfluidics device mixing efficiency. Yellow and blue food coloring solutions are introduced to inlets 1 and 2, respectively. After approximately one tenth
More informationI690/B680 Structural Bioinformatics Spring Protein Structure Determination by NMR Spectroscopy
I690/B680 Structural Bioinformatics Spring 2006 Protein Structure Determination by NMR Spectroscopy Suggested Reading (1) Van Holde, Johnson, Ho. Principles of Physical Biochemistry, 2 nd Ed., Prentice
More informationStatistical thermodynamics for MD and MC simulations
Statistical thermodynamics for MD and MC simulations knowing 2 atoms and wishing to know 10 23 of them Marcus Elstner and Tomáš Kubař 22 June 2016 Introduction Thermodynamic properties of molecular systems
More informationThe Molecular Dynamics Method
H-bond energy (kcal/mol) - 4.0 The Molecular Dynamics Method Fibronectin III_1, a mechanical protein that glues cells together in wound healing and in preventing tumor metastasis 0 ATPase, a molecular
More informationCan a continuum solvent model reproduce the free energy landscape of a β-hairpin folding in water?
Can a continuum solvent model reproduce the free energy landscape of a β-hairpin folding in water? Ruhong Zhou 1 and Bruce J. Berne 2 1 IBM Thomas J. Watson Research Center; and 2 Department of Chemistry,
More informationModeling Ultrafast Deactivation in Oligothiophenes via Nonadiabatic Dynamics
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2015 Supplementary Data for Modeling Ultrafast Deactivation in Oligothiophenes via Nonadiabatic
More informationSupporting Information
Supporting Information Solid-State 17 O NMR Reveals Hydrogen-Bonding Energetics: Not All Low-Barrier Hydrogen Bonds Are Strong Jiasheng Lu, Ivan Hung, Andreas Brinkmann, Zhehong Gan, Xianqi Kong, and Gang
More informationDiffusion of Water and Diatomic Oxygen in Poly(3-hexylthiophene) Melt: A Molecular Dynamics Simulation Study
Diffusion of Water and Diatomic Oxygen in Poly(3-hexylthiophene) Melt: A Molecular Dynamics Simulation Study Julia Deitz, Yeneneh Yimer, and Mesfin Tsige Department of Polymer Science University of Akron
More informationThe Molecular Dynamics Method
H-bond energy (kcal/mol) - 4.0 The Molecular Dynamics Method Fibronectin III_1, a mechanical protein that glues cells together in wound healing and in preventing tumor metastasis 0 ATPase, a molecular
More information