The State Diagram for Cell Adhesion Mediated by Two Receptors

Slides:



Advertisements
Similar presentations
Analysis of Kinetic Intermediates in Single-Particle Dwell-Time Distributions Daniel L. Floyd, Stephen C. Harrison, Antoine M. van Oijen Biophysical Journal.
Advertisements

The Dynamics and Mechanics of Endothelial Cell Spreading Cynthia A. Reinhart-King, Micah Dembo, Daniel A. Hammer Biophysical Journal Volume 89, Issue 1,
A Hydrodynamic Model for Hindered Diffusion of Proteins and Micelles in Hydrogels Ronald J. Phillips Biophysical Journal Volume 79, Issue 6, Pages
Chenghai Sun, Cristiano Migliorini, Lance L. Munn  Biophysical Journal 
Neutrophil-Bead Collision Assay: Pharmacologically Induced Changes in Membrane Mechanics Regulate the PSGL-1/P-Selectin Adhesion Lifetime  K.E. Edmondson,
Volume 112, Issue 10, Pages (May 2017)
Thomas J. English, Daniel A. Hammer  Biophysical Journal 
Masahiro Ueda, Tatsuo Shibata  Biophysical Journal 
Multiparticle Adhesive Dynamics
Sukant Mittal, Ian Y. Wong, William M. Deen, Mehmet Toner 
Effect of Microvillus Deformability on Leukocyte Adhesion Explored Using Adhesive Dynamics Simulations  Kelly E. Caputo, Daniel A. Hammer  Biophysical.
Neutrophil String Formation: Hydrodynamic Thresholding and Cellular Deformation during Cell Collisions  K.E. Kadash, M.B. Lawrence, S.L. Diamond  Biophysical.
Volume 84, Issue 6, Pages (June 2003)
Volume 99, Issue 11, Pages (December 2010)
Volume 86, Issue 4, Pages (April 2004)
A Model of H-NS Mediated Compaction of Bacterial DNA
James W. Piper, Robert A. Swerlick, Cheng Zhu  Biophysical Journal 
Hydrodynamics of Sperm Cells near Surfaces
Model Studies of the Dynamics of Bacterial Flagellar Motors
Platelet Adhesive Dynamics
Supriyo Bhattacharya, Nagarajan Vaidehi  Biophysical Journal 
Volume 102, Issue 11, Pages (June 2012)
Structure–Function Relation of Efomycines, a Family of Small-Molecule Inhibitors of Selectin Functions  B. Gregor Wienrich, Thomas Krahn, Margarete Schön,
Volume 99, Issue 5, Pages (September 2010)
Volume 103, Issue 12, Pages (December 2012)
Andrey S. Shaw, Michael L. Dustin  Immunity 
Luthur Siu-Lun Cheung, Konstantinos Konstantopoulos 
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.
Anil K. Dasanna, Christine Lansche, Michael Lanzer, Ulrich S. Schwarz 
Defective neutrophil rolling and transmigration in acute uremia
Mesoscale Simulation of Blood Flow in Small Vessels
Volume 103, Issue 4, Pages (August 2012)
Kelly E. Caputo, Dooyoung Lee, Michael R. King, Daniel A. Hammer 
Dmitry A. Fedosov, Bruce Caswell, George Em Karniadakis 
Noise Underlies Switching Behavior of the Bacterial Flagellum
Colocalization of Multiple DNA Loci: A Physical Mechanism
Low Spring Constant Regulates P-Selectin-PSGL-1 Bond Rupture
Volume 86, Issue 6, Pages (June 2004)
Flow-Enhanced Stability of Rolling Adhesion through E-Selectin
Nano-to-Micro Scale Dynamics of P-Selectin Detachment from Leukocyte Interfaces. III. Numerical Simulation of Tethering under Flow  Michael R. King, Volkmar.
Intrinsic Bending and Structural Rearrangement of Tubulin Dimer: Molecular Dynamics Simulations and Coarse-Grained Analysis  Yeshitila Gebremichael, Jhih-Wei.
Volume 102, Issue 2, Pages (January 2012)
Luthur Siu-Lun Cheung, Konstantinos Konstantopoulos 
N.A. N’Dri, W. Shyy, R. Tran-Son-Tay  Biophysical Journal 
Cholesterol Modulates the Dimer Interface of the β2-Adrenergic Receptor via Cholesterol Occupancy Sites  Xavier Prasanna, Amitabha Chattopadhyay, Durba.
Chetan Poojari, Dequan Xiao, Victor S. Batista, Birgit Strodel 
Yihua Zhao, Shu Chien, Sheldon Weinbaum  Biophysical Journal 
Leukocyte adhesion: High-speed cells with ABS
Daniel Coombs, Micah Dembo, Carla Wofsy, Byron Goldstein 
Toshinori Namba, Masatoshi Nishikawa, Tatsuo Shibata 
Chemically Mediated Mechanical Expansion of the Pollen Tube Cell Wall
Leukocyte Rolling on P-Selectin: A Three-Dimensional Numerical Study of the Effect of Cytoplasmic Viscosity  Damir B. Khismatullin, George A. Truskey 
Jamie L. Maciaszek, Biree Andemariam, Greg Huber, George Lykotrafitis 
Jennifer D. Stone, Jennifer R. Cochran, Lawrence J. Stern 
A Flexible Approach to the Calculation of Resonance Energy Transfer Efficiency between Multiple Donors and Acceptors in Complex Geometries  Ben Corry,
Integrin Molecular Tension within Motile Focal Adhesions
Volume 83, Issue 4, Pages (October 2002)
Dagmar Flöck, Volkhard Helms  Biophysical Journal 
Volume 108, Issue 9, Pages (May 2015)
Water Movement during Ligand Unbinding from Receptor Site
Anomalous Flexural Behaviors of Microtubules
Force as a Facilitator of Integrin Conformational Changes during Leukocyte Arrest on Blood Vessels and Antigen-Presenting Cells  Ronen Alon, Michael L.
Volume 112, Issue 3, Pages (February 2017)
Volume 111, Issue 3, Pages (August 2016)
Anil K. Dasanna, Christine Lansche, Michael Lanzer, Ulrich S. Schwarz 
Joana Pinto Vieira, Julien Racle, Vassily Hatzimanikatis 
Volume 109, Issue 10, Pages (November 2015)
A Model of H-NS Mediated Compaction of Bacterial DNA
Bistability of Cell Adhesion in Shear Flow
Volume 108, Issue 9, Pages (May 2015)
Presentation transcript:

The State Diagram for Cell Adhesion Mediated by Two Receptors Sujata K. Bhatia, Michael R. King, Daniel A. Hammer  Biophysical Journal  Volume 84, Issue 4, Pages 2671-2690 (April 2003) DOI: 10.1016/S0006-3495(03)75073-5 Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 1 Schematic diagram of adhesive dynamics. Adhesion molecules are randomly placed on the surface of a sphere and plane wall. Adhesive receptor-ligand pairs are tested for bond formation according to deviation length-dependent binding kinetics. Biophysical Journal 2003 84, 2671-2690DOI: (10.1016/S0006-3495(03)75073-5) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 2 Representative cell trajectories for adhesive behavior states. (A) No adhesion is observed at a selectin density of 1 molecule/μm2 and an ICAM-1 density of 0 sites/μm2. The ratio of cell velocity to hydrodynamic velocity, V/VH, is 60%. (B) Rolling adhesion is observed at a selectin density of 10 molecules/μm2 and an ICAM-1 density of 0 sites/μm2. V/VH is 4%. (C) Firm adhesion is observed at a selectin density of 10 molecules/μm2 and an ICAM-1 density of 4 sites/μm2. V/VH is 0.3%. Calculations are performed with an integrin-ICAM-1 association rate of kf0,integrin=1000s−1. Biophysical Journal 2003 84, 2671-2690DOI: (10.1016/S0006-3495(03)75073-5) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 3 The state diagram for adhesion mediated by two receptors. The boundary of rolling adhesion is shown for three different integrin-ICAM-1 association rates: kf0,integrin=1000, 100, and 10s−1. For each rolling state, the boundary represents a mean velocity of 0.02 VH. Biophysical Journal 2003 84, 2671-2690DOI: (10.1016/S0006-3495(03)75073-5) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 4 Effect of ICAM-1 site density on cell trajectories and instantaneous velocity distributions. The surface density of selectin is 10 molecules/μm2. ICAM-1 surface density is (A and B) 0 molecules/μm2; (C and D) 1 molecule/μm2; (E and F) 2 molecules/μm2; and (G and H) 4 molecules/μm2. Calculations are performed with an integrin-ICAM-1 association rate of kf0,integrin=1000s−1. Biophysical Journal 2003 84, 2671-2690DOI: (10.1016/S0006-3495(03)75073-5) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 5 Percentage of time paused as a function of ICAM-1 site density and selectin site density, calculated at kf0,integrin=1000s−1. Biophysical Journal 2003 84, 2671-2690DOI: (10.1016/S0006-3495(03)75073-5) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 6 Effect of selectin-site density on cell trajectories and instantaneous velocity distributions. The surface density of ICAM-1 is 1 molecule/μm2. Selectin surface density is (A and B) 1 molecule/μm2; (C and D) 10 molecules/μm2; (E and F) 30 molecules/μm2; and (G and H) 60 molecules/μm2. Calculations are performed with an integrin-ICAM-1 association rate of kf0,integrin=1000s−1. Biophysical Journal 2003 84, 2671-2690DOI: (10.1016/S0006-3495(03)75073-5) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 7 The state diagram with shear rate ranging from 100 to 1000s−1. The boundary of rolling adhesion is shown for three different shear rates (100, 400, and 1000s−1), calculated at an integrin-ICAM-1 association rate of (A) kf0,integrin=1000s−1 and (B) kf0,integrin=10s−1. For each rolling state, the boundary represents a mean velocity of 0.02 VH. Biophysical Journal 2003 84, 2671-2690DOI: (10.1016/S0006-3495(03)75073-5) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 8 The boundary of rolling adhesion for three different integrin-ICAM-1 reactive compliances (γ0,integrin=0.4, 1.0, and 4.0Å), calculated at an integrin-ICAM-1 association rate of (A) kf0,integrin=1000s−1 and (B) kf0,integrin=10s−1. For each rolling state, the boundary represents a mean velocity of 0.02 VH. Biophysical Journal 2003 84, 2671-2690DOI: (10.1016/S0006-3495(03)75073-5) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 9 Effect of β2-integrin cell surface density on cell trajectories and instantaneous velocity distributions. The surface density of ICAM-1 is 5 molecules/μm2, and the surface density of selectin is 15 molecules/μm2. β2-integrin site density is (A and B) 0 molecules/μm2; (C and D) 1 molecule/μm2; (E and F) 2 molecules/μm2; and (G and H) 4 molecules/μm2. Calculations are performed with an integrin-ICAM-1 association rate of kf0,integrin=1000s−1. Biophysical Journal 2003 84, 2671-2690DOI: (10.1016/S0006-3495(03)75073-5) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 10 The state diagram for neutrophil activation. The boundary of rolling adhesion is shown for three different integrin-ICAM-1 reactive compliances (γ0,integrin=0.4, 1.0, and 4.0Å), calculated at a shear rate of (A) 100s−1 and (B) 1000s−1. The surface density of ICAM-1 is 1000 molecules/μm2, and the surface density of selectin is 40 molecules/μm2. For each rolling state, the boundary represents a mean velocity of 0.02 VH. Biophysical Journal 2003 84, 2671-2690DOI: (10.1016/S0006-3495(03)75073-5) Copyright © 2003 The Biophysical Society Terms and Conditions

Figure 11 Comparison of two-receptor adhesive dynamic simulations to experiment. (A) Representative neutrophil rolling trajectories in wild-type, CD18−/−, and E−/− mice, as reported in Forlow et al. (2000). (B) Comparison of experimental CD18−/− neutrophil rolling trajectory to simulated cell motion; calculated results for three different selectin densities (14, 20, 25 sites/μm2) are shown. (C) Comparison of experimental E−/− neutrophil rolling trajectory to simulated cell motion; calculated results for three different integrin-ICAM-1 association rates (10, 100, 1000s−1) are shown. (D) Comparison of experimental wild-type neutrophil rolling trajectory to simulated cell motion; calculated results for three different integrin-ICAM-1 association rates (10, 100, 1000s−1) are shown. (E) Comparison of average neutrophil rolling velocities, as reported by Kunkel et al. (2000), to average rolling velocities predicted by simulations; this calculation is performed at kf0,integrin=1000s−1. Experimental velocities are represented by blue bars, and simulated results are represented by red bars. Biophysical Journal 2003 84, 2671-2690DOI: (10.1016/S0006-3495(03)75073-5) Copyright © 2003 The Biophysical Society Terms and Conditions