Molecular Basis of Fibrin Clot Elasticity

Slides:



Advertisements
Similar presentations
Volume 14, Issue 3, Pages (March 2006)
Advertisements

Volume 15, Issue 3, Pages (April 2016)
Volume 112, Issue 7, Pages (April 2017)
Using Enhanced Sampling and Structural Restraints to Refine Atomic Structures into Low-Resolution Electron Microscopy Maps  Harish Vashisth, Georgios.
A Naturally Occurring Repeat Protein with High Internal Sequence Identity Defines a New Class of TPR-like Proteins  Jacob D. Marold, Jennifer M. Kavran,
Sudha Chakrapani, Luis G. Cuello, D. Marien Cortes, Eduardo Perozo 
Volume 101, Issue 4, Pages (August 2011)
Steered Molecular Dynamics Studies of Titin I1 Domain Unfolding
Mechanical Anisotropy of Ankyrin Repeats
Volume 23, Issue 1, Pages (January 2015)
Theory and Simulation of Water Permeation in Aquaporin-1
Complex Energy Landscape of a Giant Repeat Protein
Mechanical Strength of the Titin Z1Z2-Telethonin Complex
Volume 25, Issue 11, Pages e5 (November 2017)
Volume 23, Issue 7, Pages (July 2015)
Volume 14, Issue 3, Pages (March 2006)
HyeongJun Kim, Jen Hsin, Yanxin Liu, Paul R. Selvin, Klaus Schulten 
Volume 106, Issue 6, Pages (March 2014)
A Model for the Solution Structure of the Rod Arrestin Tetramer
Volume 14, Issue 6, Pages (June 2006)
Volume 96, Issue 2, Pages (January 2009)
Anton Arkhipov, Wouter H. Roos, Gijs J.L. Wuite, Klaus Schulten 
Changbong Hyeon, Ruxandra I. Dima, D. Thirumalai  Structure 
Douglas D. Root, Vamsi K. Yadavalli, Jeffrey G. Forbes, Kuan Wang 
A Highly Strained Nuclear Conformation of the Exportin Cse1p Revealed by Molecular Dynamics Simulations  Ulrich Zachariae, Helmut Grubmüller  Structure 
Volume 24, Issue 8, Pages (August 2016)
Volume 22, Issue 4, Pages (April 2014)
Volume 17, Issue 12, Pages (December 2009)
Multiple Conformations of F-actin
A Conformational Switch in the CRIB-PDZ Module of Par-6
Regulation of the Protein-Conducting Channel by a Bound Ribosome
Discovery Through the Computational Microscope
Volume 20, Issue 12, Pages (December 2012)
Volume 17, Issue 6, Pages (June 2009)
Raf-1 Cysteine-Rich Domain Increases the Affinity of K-Ras/Raf at the Membrane, Promoting MAPK Signaling  Shuai Li, Hyunbum Jang, Jian Zhang, Ruth Nussinov 
A Gating Mechanism of the Serotonin 5-HT3 Receptor
Volume 20, Issue 3, Pages (March 2012)
Nucleotide Effects on the Structure and Dynamics of Actin
PcrA Helicase, a Prototype ATP-Driven Molecular Motor
Sequential Unfolding of Individual Helices of Bacterioopsin Observed in Molecular Dynamics Simulations of Extraction from the Purple Membrane  Michele.
Volume 16, Issue 8, Pages (August 2008)
Comparative Studies of Microtubule Mechanics with Two Competing Models Suggest Functional Roles of Alternative Tubulin Lateral Interactions  Zhanghan.
Probing the Energy Landscape of the Membrane Protein Bacteriorhodopsin
Unfolding Barriers in Bacteriorhodopsin Probed from the Cytoplasmic and the Extracellular Side by AFM  Max Kessler, Hermann E. Gaub  Structure  Volume.
Zara A. Sands, Alessandro Grottesi, Mark S.P. Sansom 
Volume 107, Issue 5, Pages (September 2014)
Yuliang Zhang, Yuri L. Lyubchenko  Biophysical Journal 
Volume 26, Issue 1, Pages e4 (January 2018)
Volume 21, Issue 10, Pages (October 2013)
Grischa R. Meyer, Justin Gullingsrud, Klaus Schulten, Boris Martinac 
Cholesterol Modulates the Dimer Interface of the β2-Adrenergic Receptor via Cholesterol Occupancy Sites  Xavier Prasanna, Amitabha Chattopadhyay, Durba.
Velocity-Dependent Mechanical Unfolding of Bacteriorhodopsin Is Governed by a Dynamic Interaction Network  Christian Kappel, Helmut Grubmüller  Biophysical.
Hierarchical Cascades of Instability Govern the Mechanics of Coiled Coils: Helix Unfolding Precedes Coil Unzipping  Elham Hamed, Sinan Keten  Biophysical.
Volume 20, Issue 8, Pages (August 2012)
The Atomistic Mechanism of Conformational Transition in Adenylate Kinase: A TEE-REX Molecular Dynamics Study  Marcus B. Kubitzki, Bert L. de Groot  Structure 
Volume 108, Issue 12, Pages (June 2015)
In Search of the Hair-Cell Gating Spring
Volume 27, Issue 7, Pages e5 (July 2019)
Volume 113, Issue 12, Pages (December 2017)
A Model for the Solution Structure of the Rod Arrestin Tetramer
Matthieu Chavent, Elena Seiradake, E. Yvonne Jones, Mark S.P. Sansom 
Y. Zenmei Ohkubo, Emad Tajkhorshid  Structure 
Fine Details of IGF-1R Activation, Inhibition, and Asymmetry Determined by Associated Hydrogen /Deuterium-Exchange and Peptide Mass Mapping  Damian Houde,
Eric H. Lee, Jen Hsin, Olga Mayans, Klaus Schulten  Biophysical Journal 
Volume 20, Issue 8, Pages (August 2012)
An Efficient Null Model for Conformational Fluctuations in Proteins
Unfolding Barriers in Bacteriorhodopsin Probed from the Cytoplasmic and the Extracellular Side by AFM  Max Kessler, Hermann E. Gaub  Structure  Volume.
Volume 21, Issue 10, Pages (October 2013)
Yanxin Liu, Jen Hsin, HyeongJun Kim, Paul R. Selvin, Klaus Schulten 
Volume 24, Issue 8, Pages (August 2016)
Presentation transcript:

Molecular Basis of Fibrin Clot Elasticity Bernard B.C. Lim, Eric H. Lee, Marcos Sotomayor, Klaus Schulten  Structure  Volume 16, Issue 3, Pages 449-459 (March 2008) DOI: 10.1016/j.str.2007.12.019 Copyright © 2008 Elsevier Ltd Terms and Conditions

Figure 1 Fibrinogen Structure and AFM Imaging (A) Crystal structure of fibrinogen (PDB code: 1m1j) showing the central E region connected to the distal D regions by two sets of three-stranded coiled coils (labeled α1β1γ1 and α2β2γ2). (B and C) Schematic diagram of a fibrin protofibril showing (B) the half staggered double-stranded configuration and (C) trimodular interactions between the central E and distal D regions, with crosslinking between the D regions involving Factor XIII. Liquid tapping mode AFM images of single fibrinogen molecules showing the expected trinodular structure (D) and fibrin protofibrils showing linear strands (that are 250 ± 75 nm long (n = 35 protofibril strands) consisting of seven to ten fibrin monomers (E)). Structure 2008 16, 449-459DOI: (10.1016/j.str.2007.12.019) Copyright © 2008 Elsevier Ltd Terms and Conditions

Figure 2 Geometry of AFM Measurement, with Fibrinogen and Fibrin Force-Extension Curves and Histograms (A) Diagram illustrating the geometry of the AFM pulling fibrinogen. Initially, the molecule is straightened from its relaxed conformation (R phase). This is followed by an extension of the coiled-coil region during a P (plateau) phase, ending with a “dip” in the force. Finally, further extension is characterized by an E (exponential) phase reflecting a steep rise in the needed force. (B) Force extension curve for stretching a single fibrinogen molecule, showing the R, P, and E phases. The inset shows the complete force extension curve obtained for a single fibrinogen molecule depicting two consecutive triphasic signatures, each presumably corresponding to the unfolding of one of the coiled coils in fibrinogen (see Figure 1A). The rectangle denotes the highlighted region. The expanded figure shows a plateau height of 60 pN and a plateau length of 15 nm. The plateau height was calculated relative to the force baseline before the R phase (see Experimental Procedures). AFM traces demonstrating consistency of the triphasic RPE response across multiple trials are shown in Figure S5. (C and D) Histograms showing the plateau force (C) and plateau length (D) distributions (pH 7.4 and calcium concentration of 2.5 mM). Black lines in each histogram are moving averages. (E) Force-extension curve for the linear polymeric fibrin strands (protofibrils) showing a blunted “sawtooth” pattern of four triphasic coiled-coil signatures exhibiting hysteresis (extension in red and relaxation in blue). The AFM data reveal a characteristic force plateau related to the unfolding of the fibrinogen's coiled coils. Structure 2008 16, 449-459DOI: (10.1016/j.str.2007.12.019) Copyright © 2008 Elsevier Ltd Terms and Conditions

Figure 3 Stretching Fibrinogen Using Steered Molecular Dynamics Simulations (A–C) Force-extension profile of fibrinogen stretched at 0.025 Å/ps over the course of simulation simB2 (see Table 1). The marked time points along the trace denote unfolding events highlighted in (B) and (C). (B) Snapshots of unfolding events show (i) the initial equilibrated fibrinogen molecule before stretching at t = 0 ns; (ii) unfolding of fibrinogen's double helical region at t = 3.2 ns (blue circles); (iii) unfolding of fibrinogen's triple helical region at t = 8.5 ns (red circles); (iv) unraveling of fibrinogen's central domain at t = 14 ns (green circle); (v) unfolding of the terminal regions made of four helices at t = 18 ns (purple circles); (vi) full extension of the coiled-coil segments of fibrinogen at t = 22.4 ns. (C) Detailed views of unfolding events in ii–v corresponding to a partially unraveled helical or central domain region. Disulfide bonds are highlighted through circles in (iv). Unfolding of coiled coils results in a force plateau, while unraveling and unfolding of the central region gives rise to a “dip” (iv) in the force-extension profile. All snapshots show the protein in cartoon representation, with each subunit colored differently (water not shown for clarity). Structure 2008 16, 449-459DOI: (10.1016/j.str.2007.12.019) Copyright © 2008 Elsevier Ltd Terms and Conditions

Figure 4 Changes in Coiled-Coil Plateau Force and Plateau Length with Changes in pH and Calcium (A) Representative force-extension curve (left panel) for AFM stretching of fibrinogen protofibrils at physiological pH 7.4 and calcium concentration of 2.5 mM. The inset in this and subsequent panels shows the raw force-extension curve with an overall linear increase in force. The dashed rectangle denotes the region highlighted in the main plot. The middle and right panels show the plateau force and plateau length histograms. (B) Force-extension curve and histograms for stretching protofibrils at pH 3.1. (C) Force-extension curve and histograms for stretching protofibrils at a calcium concentration of 10 mM. (The black lines in each histogram are moving averages.) Structure 2008 16, 449-459DOI: (10.1016/j.str.2007.12.019) Copyright © 2008 Elsevier Ltd Terms and Conditions