A Structural Perspective on the Dynamics of Kinesin Motors

Slides:



Advertisements
Similar presentations
Fabio Trovato, Edward P. O’Brien  Biophysical Journal 
Advertisements

Small Peptide Binding Stiffens the Ubiquitin-like Protein SUMO1
Volume 107, Issue 9, Pages (November 2014)
Molecular Analysis of the Interaction between Staphylococcal Virulence Factor Sbi-IV and Complement C3d  Ronald D. Gorham, Wilson Rodriguez, Dimitrios.
Volume 15, Issue 3, Pages (April 2016)
Young Min Rhee, Vijay S. Pande  Biophysical Journal 
Olivier Fisette, Stéphane Gagné, Patrick Lagüe  Biophysical Journal 
Adam G. Larson, Nariman Naber, Roger Cooke, Edward Pate, Sarah E. Rice 
Mechanical Anisotropy of Ankyrin Repeats
Investigating How Peptide Length and a Pathogenic Mutation Modify the Structural Ensemble of Amyloid Beta Monomer  Yu-Shan Lin, Gregory R. Bowman, Kyle A.
On the Origin of Kinesin Limping
Linda Balabanian, Christopher L. Berger, Adam G. Hendricks 
Theoretical and Computational Investigation of Flagellin Translocation and Bacterial Flagellum Growth  David E. Tanner, Wen Ma, Zhongzhou Chen, Klaus.
HyeongJun Kim, Jen Hsin, Yanxin Liu, Paul R. Selvin, Klaus Schulten 
Volume 101, Issue 2, Pages (July 2011)
Megan T. Valentine, Steven M. Block  Biophysical Journal 
Volume 28, Issue 1, Pages (October 2007)
Coupling of Retinal, Protein, and Water Dynamics in Squid Rhodopsin
Mechanism of the αβ Conformational Change in F1-ATPase after ATP Hydrolysis: Free- Energy Simulations  Yuko Ito, Mitsunori Ikeguchi  Biophysical Journal 
Changbong Hyeon, Ruxandra I. Dima, D. Thirumalai  Structure 
Rainer A. Böckmann, Helmut Grubmüller  Biophysical Journal 
Liqiang Dai, Holger Flechsig, Jin Yu  Biophysical Journal 
Volume 107, Issue 6, Pages (September 2014)
Volume 74, Issue 1, Pages (January 1998)
Binding of the Bacteriophage P22 N-Peptide to the boxB RNA Motif Studied by Molecular Dynamics Simulations  Ranjit P. Bahadur, Srinivasaraghavan Kannan,
Mark C. Leake, David Wilson, Mathias Gautel, Robert M. Simmons 
Molecular-Dynamics Simulations of the ATP/apo State of a Multidrug ATP-Binding Cassette Transporter Provide a Structural and Mechanistic Basis for the.
Crystal Structure of β-Arrestin at 1.9 Å
Volume 96, Issue 7, Pages (April 2009)
Yusuke Nakasone, Kazunori Zikihara, Satoru Tokutomi, Masahide Terazima 
Dissecting the Kinematics of the Kinesin Step
Nucleotide Effects on the Structure and Dynamics of Actin
Li Sun, Jeffrey K. Noel, Herbert Levine, José N. Onuchic 
Volume 90, Issue 8, Pages (April 2006)
Protein Collective Motions Coupled to Ligand Migration in Myoglobin
Sequential Unfolding of Individual Helices of Bacterioopsin Observed in Molecular Dynamics Simulations of Extraction from the Purple Membrane  Michele.
Volume 107, Issue 12, Pages (December 2014)
Ivan Coluzza, Daan Frenkel  Biophysical Journal 
Volume 107, Issue 5, Pages (September 2014)
Yuliang Zhang, Yuri L. Lyubchenko  Biophysical Journal 
Phosphorylation Primes Vinculin for Activation
Thomas H. Schmidt, Yahya Homsi, Thorsten Lang  Biophysical Journal 
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
Logan S. Ahlstrom, Osamu Miyashita  Biophysical Journal 
Flow-Induced β-Hairpin Folding of the Glycoprotein Ibα β-Switch
Dynamics of Myosin-V Processivity
Jing Chen, John Neu, Makoto Miyata, George Oster  Biophysical Journal 
Vinculin Activation Is Necessary for Complete Talin Binding
Structure of BamHI Bound to Nonspecific DNA
Long-Range Nonanomalous Diffusion of Quantum Dot-Labeled Aquaporin-1 Water Channels in the Cell Plasma Membrane  Jonathan M. Crane, A.S. Verkman  Biophysical.
Ana Caballero-Herrera, Lennart Nilsson  Biophysical Journal 
J.P. Junker, K. Hell, M. Schlierf, W. Neupert, M. Rief 
Volume 74, Issue 1, Pages (January 1998)
Brownian Dynamics of Subunit Addition-Loss Kinetics and Thermodynamics in Linear Polymer Self-Assembly  Brian T. Castle, David J. Odde  Biophysical Journal 
OmpT: Molecular Dynamics Simulations of an Outer Membrane Enzyme
Volume 113, Issue 12, Pages (December 2017)
Yongli Zhang, Junyi Jiao, Aleksander A. Rebane  Biophysical Journal 
Subpiconewton Dynamic Force Spectroscopy Using Magnetic Tweezers
Small Peptide Binding Stiffens the Ubiquitin-like Protein SUMO1
Shayantani Mukherjee, Sean M. Law, Michael Feig  Biophysical Journal 
Ricksen S. Winardhi, Qingnan Tang, Jin Chen, Mingxi Yao, Jie Yan 
Crystal Structure of β-Arrestin at 1.9 Å
Amir Marcovitz, Yaakov Levy  Biophysical Journal 
Volume 114, Issue 6, Pages (March 2018)
Volume 93, Issue 8, Pages (October 2007)
Zackary N. Scholl, Weitao Yang, Piotr E. Marszalek  Biophysical Journal 
Hysteresis-Based Mechanism for the Directed Motility of the Ncd Motor
Seongwon Kim, Takako Takeda, Dmitri K. Klimov  Biophysical Journal 
Yanxin Liu, Jen Hsin, HyeongJun Kim, Paul R. Selvin, Klaus Schulten 
Presentation transcript:

A Structural Perspective on the Dynamics of Kinesin Motors Changbong Hyeon, José N. Onuchic  Biophysical Journal  Volume 101, Issue 11, Pages 2749-2759 (December 2011) DOI: 10.1016/j.bpj.2011.10.037 Copyright © 2011 Biophysical Society Terms and Conditions

Figure 1 Biochemical cycle of a kinesin motor. The state of kinesin changes along the cycle. The subscript i in the notation [NT-NT]i denotes the position on MT to which the kinesin binds. In the diagram the internal conformational states that do not alter the kinesin position are aligned vertically with purple arrows, and the step is depicted with yellow arrows. The inset shows a time trace from laser optical tweezers measurement. Biophysical Journal 2011 101, 2749-2759DOI: (10.1016/j.bpj.2011.10.037) Copyright © 2011 Biophysical Society Terms and Conditions

Figure 2 Stepping dynamics of kinesin. (a) Difference of contact maps calculated with ordered and disordered NL reveals the contacts involving the NL docking and cover-neck bundle. Red arrows indicate the NL zipper contacts on the contact map and in the kinesin structure. Yellow arrows show the location of cover-neck bundle, where the N-terminal part of NL is sandwiched between two chain segments (residues 2–8 and 289–296). (b) Potential of mean force of the tethered head on the MT surface computed for disordered (left) and ordered NL (right) of the MT-bound head. (c) The average time traces from the Brownian dynamics simulation of a quasiparticle with varying τP (panel on the left) are compared with the average time traces measured using optical tweezers by Yanagida and co-workers (three panels on the right) (27). In (27), the individual single molecule time traces were partitioned into three groups depending on the stepping time i), t < 50 μs, ii), 50 μs < t < 100 μs, iii), t > 100 μs) and averaged in each group. The panels on the right are adapted from (27). Biophysical Journal 2011 101, 2749-2759DOI: (10.1016/j.bpj.2011.10.037) Copyright © 2011 Biophysical Society Terms and Conditions

Figure 3 Facilitation of kinesin binding to MTs through partial unfolding and refolding of MT-binding motifs. Binding process is monitored using the fraction of native contacts within the MT-binding motifs made of α4, α5, α6, L12, and β5 (Qp) and the fraction of interfacial contacts between kinesin and MT binding site (Qint). The inset shows an exemplary trajectory exhibiting partial local unfolding and refolding of MT-binding motifs before the binding. Biophysical Journal 2011 101, 2749-2759DOI: (10.1016/j.bpj.2011.10.037) Copyright © 2011 Biophysical Society Terms and Conditions

Figure 4 Internal tension regulated inhibition of ATP binding to the leading kinesin head. (a) For the two head-bound kinesin, the internal tension (fint) built on the NL of the leading head disrupts the catalytic site and inhibits the premature binding of ATP, whereas the trailing head configuration is close to the native state, which is shown on the right for comparison. Cα-root mean-square deviation of head domain excluding α6 helix (residues 2–315) is 1.8 Å for trailing head and 3.8 Å for leading head. (b) fint value can be estimated by using force-extension relation of the worm-like chain model. The extension of the NL in the leading head (δx) is ≈ 3.1 ± 0.8 nm (distribution on the left panel). When Lc = 15 aa × 0.38 nm/aa ≈ 5.7 nm and lp = 0.5 – 1.0 nm with δx = 3.1 nm are used, one can estimate the internal tension, fint ≈ 7.5 – 12.5 pN (right panel). Biophysical Journal 2011 101, 2749-2759DOI: (10.1016/j.bpj.2011.10.037) Copyright © 2011 Biophysical Society Terms and Conditions

Figure 5 (a) Molecular motor devised by using optomechanical cycle of polyazopeptide that undergoes cis↔trans transition upon photon absorption/emission. The figure is adapted from (67). (b) The mechanochemical cycle of kinesins and the force versus extension curves (FECs) for the NL of red motor domain. There are three FECs; two for the unzippered NL (cyan) and one for the zippered NL (purple). Each stage of kinesin cycle is marked with the yellow circles on the FECs indexed from (i) to (viii). Biophysical Journal 2011 101, 2749-2759DOI: (10.1016/j.bpj.2011.10.037) Copyright © 2011 Biophysical Society Terms and Conditions