Dominico Vigil, Stephen C. Gallagher, Jill Trewhella, Angel E. García 

Slides:



Advertisements
Similar presentations
Po-chia Chen, Jochen S. Hub  Biophysical Journal 
Advertisements

Volume 107, Issue 9, Pages (November 2014)
Philippe Derreumaux, Tamar Schlick  Biophysical Journal 
Volume 109, Issue 6, Pages (September 2015)
Induced Fit and the Entropy of Structural Adaptation in the Complexation of CAP and λ- Repressor with Cognate DNA Sequences  Surjit B. Dixit, David Q.
Vishwanath Jogini, Benoît Roux  Biophysical Journal 
Molecular Dynamics Simulations of the Lipid Bilayer Edge
Jing Han, Kristyna Pluhackova, Tsjerk A. Wassenaar, Rainer A. Böckmann 
Structure and Dynamics of Calmodulin in Solution
Investigating How Peptide Length and a Pathogenic Mutation Modify the Structural Ensemble of Amyloid Beta Monomer  Yu-Shan Lin, Gregory R. Bowman, Kyle A.
Modeling Zymogen Protein C
Christopher Wostenberg, W.G. Noid, Scott A. Showalter 
Molecular Dynamics Simulations on SDF-1α: Binding with CXCR4 Receptor
Transconformations of the SERCA1 Ca-ATPase: A Normal Mode Study
Supriyo Bhattacharya, Nagarajan Vaidehi  Biophysical Journal 
Volume 84, Issue 1, Pages (January 2003)
Po-Chao Wen, Emad Tajkhorshid  Biophysical Journal 
Shozeb Haider, Gary N. Parkinson, Stephen Neidle  Biophysical Journal 
Large-Scale Conformational Dynamics of the HIV-1 Integrase Core Domain and Its Catalytic Loop Mutants  Matthew C. Lee, Jinxia Deng, James M. Briggs, Yong.
Volume 98, Issue 2, Pages (January 2010)
Volume 74, Issue 1, Pages (January 1998)
G. Fiorin, A. Pastore, P. Carloni, M. Parrinello  Biophysical Journal 
Volume 16, Issue 5, Pages (May 2008)
A Molecular Dynamics Study of Ca2+-Calmodulin: Evidence of Interdomain Coupling and Structural Collapse on the Nanosecond Timescale  Craig M. Shepherd,
Volume 87, Issue 6, Pages (December 2004)
Michael E Wall, James B Clarage, George N Phillips  Structure 
Molecular-Dynamics Simulations of the ATP/apo State of a Multidrug ATP-Binding Cassette Transporter Provide a Structural and Mechanistic Basis for the.
Volume 96, Issue 7, Pages (April 2009)
Nucleotide Effects on the Structure and Dynamics of Actin
Ligand Binding to the Voltage-Gated Kv1
Atomistic Ensemble Modeling and Small-Angle Neutron Scattering of Intrinsically Disordered Protein Complexes: Applied to Minichromosome Maintenance Protein 
Protein Collective Motions Coupled to Ligand Migration in Myoglobin
Karunesh Arora, Tamar Schlick  Biophysical Journal 
The Unbinding of ATP from F1-ATPase
Marcos Sotomayor, Klaus Schulten  Biophysical Journal 
Volume 108, Issue 10, Pages (May 2015)
Dissecting DNA-Histone Interactions in the Nucleosome by Molecular Dynamics Simulations of DNA Unwrapping  Ramona Ettig, Nick Kepper, Rene Stehr, Gero.
Zara A. Sands, Alessandro Grottesi, Mark S.P. Sansom 
Investigating Lipid Composition Effects on the Mechanosensitive Channel of Large Conductance (MscL) Using Molecular Dynamics Simulations  Donald E. Elmore,
Activation of the Edema Factor of Bacillus anthracis by Calmodulin: Evidence of an Interplay between the EF-Calmodulin Interaction and Calcium Binding 
Volume 88, Issue 4, Pages (April 2005)
Structural Flexibility of CaV1. 2 and CaV2
Volume 107, Issue 9, Pages (November 2014)
Volume 77, Issue 1, Pages (July 1999)
Volume 98, Issue 12, Pages (June 2010)
Molecular Dynamics Simulation of Protein Folding by Essential Dynamics Sampling: Folding Landscape of Horse Heart Cytochrome c  Isabella Daidone, Andrea.
Dynamics of the BH3-Only Protein Binding Interface of Bcl-xL
Dynamics of Nuclear Receptor Helix-12 Switch of Transcription Activation by Modeling Time-Resolved Fluorescence Anisotropy Decays  Mariana R.B. Batista,
Open-State Models of a Potassium Channel
Volume 114, Issue 1, Pages (January 2018)
Amedeo Caflisch, Martin Karplus  Structure 
Conformational Transitions in Protein-Protein Association: Binding of Fasciculin-2 to Acetylcholinesterase  Jennifer M. Bui, Zoran Radic, Palmer Taylor,
Coupling of S4 Helix Translocation and S6 Gating Analyzed by Molecular-Dynamics Simulations of Mutated Kv Channels  Manami Nishizawa, Kazuhisa Nishizawa 
The Talin Dimer Structure Orientation Is Mechanically Regulated
Coupling of S4 Helix Translocation and S6 Gating Analyzed by Molecular-Dynamics Simulations of Mutated Kv Channels  Manami Nishizawa, Kazuhisa Nishizawa 
Ana Caballero-Herrera, Lennart Nilsson  Biophysical Journal 
Structure and Dynamics of Zymogen Human Blood Coagulation Factor X
Nevra Ozer, Celia A. Schiffer, Turkan Haliloglu  Biophysical Journal 
Volume 85, Issue 5, Pages (November 2003)
Mechanism of Interaction between the General Anesthetic Halothane and a Model Ion Channel Protein, III: Molecular Dynamics Simulation Incorporating a.
Po-chia Chen, Jochen S. Hub  Biophysical Journal 
Y. Zenmei Ohkubo, Emad Tajkhorshid  Structure 
Volume 98, Issue 2, Pages (January 2010)
Volume 78, Issue 6, Pages (June 2000)
Volume 94, Issue 11, Pages (June 2008)
Volume 98, Issue 4, Pages (February 2010)
Progressive DNA Bending Is Made Possible by Gradual Changes in the Torsion Angle of the Glycosyl Bond  Leonardo Pardo, Nina Pastor, Harel Weinstein  Biophysical.
Ultraslow Water-Mediated Transmembrane Interactions Regulate the Activation of A2A Adenosine Receptor  Yoonji Lee, Songmi Kim, Sun Choi, Changbong Hyeon 
Yanxin Liu, Jen Hsin, HyeongJun Kim, Paul R. Selvin, Klaus Schulten 
Molecular Dynamics Simulation of a Synthetic Ion Channel
Presentation transcript:

Functional Dynamics of the Hydrophobic Cleft in the N-Domain of Calmodulin  Dominico Vigil, Stephen C. Gallagher, Jill Trewhella, Angel E. García  Biophysical Journal  Volume 80, Issue 5, Pages 2082-2092 (May 2001) DOI: 10.1016/S0006-3495(01)76182-6 Copyright © 2001 The Biophysical Society Terms and Conditions

Figure 1 Relationship between the fluctuations in Ca2+ bound nCaM and Rg. (A) Rg values as a function of simulation time. (B) Projection of the MD trajectory along the principal component of motion that describes most of the system fluctuations. (C) Correlation between the first principal component and the time series of Rg values during the entire simulation. (D) Correlation between the first principal component and the time series of Rg values during the last 2.54ns of simulation. Biophysical Journal 2001 80, 2082-2092DOI: (10.1016/S0006-3495(01)76182-6) Copyright © 2001 The Biophysical Society Terms and Conditions

Figure 2 (A) Rg values of residues 4–74 during the second nCaM simulation (B) of the N- and (C) C-domains of CaM. For the second nCaM simulation, the structure closes at 0.4ns, and then opens again at the end of the simulation. For the whole CaM simulation, the N-domain closes at t=1ns and remains closed for the rest of the simulation, and the C-domain shows small fluctuations around the crystal structure value. Biophysical Journal 2001 80, 2082-2092DOI: (10.1016/S0006-3495(01)76182-6) Copyright © 2001 The Biophysical Society Terms and Conditions

Figure 3 MSDs of the Cα atoms for Ca2+-bound nCaM. The top plot shows the MSDs along the principal component axis (blue) superimposed on the total MSDs (green). The bottom plot shows the MSDs along the second principal component axis. It can be seen that the principal component of motion accounts for almost all of the motion. The secondary structure of nCaM is as follows: Helix 1, 5–19; Ca2+-binding loop 1, 20–28; helix 2, 29–37; helix linker, 38–44; helix 3, 45–55; Ca2+-binding loop 2, 56–64; helix 4, 65–75. Biophysical Journal 2001 80, 2082-2092DOI: (10.1016/S0006-3495(01)76182-6) Copyright © 2001 The Biophysical Society Terms and Conditions

Figure 4 (A) Stereo representations of the starting configuration of the Ca2+-bound nCaM MD simulation, (B) the final configuration, and (C) average apo nCaM configuration. Methionine residues that are implicated in target binding are shown explicitly. Note that there is a drastic closing of the structure during the simulation and that many key hydrophobic residues are at least partially buried from the solvent. Even though this structure is closed, as is the apo form, it is still quite different in detail from the apo form. Helical structures are defined using the program Stride (Frishman and Argos, 1995) as implemented in VMD (Humphrey et al., 1996). Biophysical Journal 2001 80, 2082-2092DOI: (10.1016/S0006-3495(01)76182-6) Copyright © 2001 The Biophysical Society Terms and Conditions

Figure 5 (A) Displacement along the principal component of motion for apo nCaM during the simulation. (B) Rg during simulation. It is clear that there are no large changes in Rg during the simulation and that there is no correlation between Rg and the principal component of motion. Biophysical Journal 2001 80, 2082-2092DOI: (10.1016/S0006-3495(01)76182-6) Copyright © 2001 The Biophysical Society Terms and Conditions

Figure 6 MSDs of the Cα atoms for apo nCaM. The top plot shows the MSDs along the principal component axis (blue) superimposed on the total MSDs (green). The bottom plot shows the MSDs along the second principal component axis. It can be seen that the principal component of motion accounts for almost all the total motion. The secondary structure of nCaM is as follows: Helix 1, 5–19; calcium-binding loop 1, 20–28; helix 2, 29–37; helix linker, 38–44; helix 3, 45–55; Ca2+-binding loop 2, 56–64; helix 4, 65–75. Biophysical Journal 2001 80, 2082-2092DOI: (10.1016/S0006-3495(01)76182-6) Copyright © 2001 The Biophysical Society Terms and Conditions

Figure 7 X-ray scattering data for the 1–77nCaM with and without bound Ca2+ overlaid with the corresponding scattering curve calculated from the best-fit model. Biophysical Journal 2001 80, 2082-2092DOI: (10.1016/S0006-3495(01)76182-6) Copyright © 2001 The Biophysical Society Terms and Conditions

Figure 8 (Top) Three views of the crystal structure of Ca2+-loaded nCaM (gray ribbon), the final simulation structure of the Ca2+-loaded nCaM (red ribbon), and the best-fit model of the Ca2+-loaded nCaM calculated from solution small-angle x-ray scattering data (green crosses). It is easily seen that the final simulation structure is very close in overall size and shape to the model derived from the scattering data. The crystal structure, on the other hand, is much more elongated than the others. Biophysical Journal 2001 80, 2082-2092DOI: (10.1016/S0006-3495(01)76182-6) Copyright © 2001 The Biophysical Society Terms and Conditions