A structure-based sliding-rebinding mechanism for catch bonds.

Catch bonds, whose lifetimes are prolonged by force, have been observed in selectin-ligand interactions and other systems. Several biophysical models have been proposed to explain this counterintuitive phenomenon, but none was based on the structure of the interacting molecules and the noncovalent interactions at the binding interface. Here we used molecular dynamics simulations to study changes in structure and atomic-level interactions during forced unbinding of P-selectin from P-selectin glycoprotein ligand-1. A mechanistic model for catch bonds was developed based on these observations. In the model, "catch" results from forced opening of an interdomain hinge that tilts the binding interface to allow two sides of the contact to slide against each other. Sliding promotes formation of new interactions and even rebinding to the original state, thereby slowing dissociation and prolonging bond lifetimes. Properties of this sliding-rebinding mechanism were explored using a pseudoatom representation and Monte Carlo simulations. The model has been supported by its ability to fit experimental data and can be related to previously proposed two-pathway models.

[1]  Jizhong Lou,et al.  Flow-enhanced adhesion regulated by a selectin interdomain hinge , 2006, The Journal of cell biology.

[2]  T. Springer,et al.  Remodeling of the lectin–EGF-like domain interface in P- and L-selectin increases adhesiveness and shear resistance under hydrodynamic force , 2006, Nature Immunology.

[3]  William H Guilford,et al.  Mechanics of actomyosin bonds in different nucleotide states are tuned to muscle contraction. , 2006, Proceedings of the National Academy of Sciences of the United States of America.

[4]  Y. Pereverzev,et al.  Force-induced deformations and stability of biological bonds. , 2006, Physical review. E, Statistical, nonlinear, and soft matter physics.

[5]  Lina M. Nilsson,et al.  Catch-bond model derived from allostery explains force-activated bacterial adhesion. , 2006, Biophysical journal.

[6]  D. Thirumalai,et al.  Determination of network of residues that regulate allostery in protein families using sequence analysis , 2006, Protein science : a publication of the Protein Society.

[7]  Z. Ou-Yang,et al.  Dynamic disorder in receptor-ligand forced dissociation experiments. , 2006, Physical review. E, Statistical, nonlinear, and soft matter physics.

[8]  Laxmikant V. Kalé,et al.  Scalable molecular dynamics with NAMD , 2005, J. Comput. Chem..

[9]  Oleg V Prezhdo,et al.  The two-pathway model for the catch-slip transition in biological adhesion. , 2005, Biophysical journal.

[10]  Y. Pereverzev,et al.  Distinctive features of the biological catch bond in the jump-ramp force regime predicted by the two-pathway model. , 2005, Physical review. E, Statistical, nonlinear, and soft matter physics.

[11]  V Barsegov,et al.  Dynamics of unbinding of cell adhesion molecules: transition from catch to slip bonds. , 2005, Proceedings of the National Academy of Sciences of the United States of America.

[12]  龙勉,et al.  Forced Dissociation of Selectin-ligand Complexes Using Steered Molecular Dynamics Simulation , 2005 .

[13]  Cheng Zhu,et al.  Catch bonds govern adhesion through L-selectin at threshold shear , 2004, The Journal of cell biology.

[14]  Cheng Zhu,et al.  Mechanical switching and coupling between two dissociation pathways in a P-selectin adhesion bond. , 2004, Proceedings of the National Academy of Sciences of the United States of America.

[15]  Cheng Zhu,et al.  Low Force Decelerates L-selectin Dissociation from P-selectin Glycoprotein Ligand-1 and Endoglycan* , 2004, Journal of Biological Chemistry.

[16]  P. Bongrand,et al.  Measuring Receptor/Ligand Interaction at the Single-Bond Level: Experimental and Interpretative Issues , 2002, Annals of Biomedical Engineering.

[17]  Klaus Schulten,et al.  Structure and functional significance of mechanically unfolded fibronectin type III1 intermediates , 2003, Proceedings of the National Academy of Sciences of the United States of America.

[18]  Ariel Solomon,et al.  Avidity enhancement of L-selectin bonds by flow , 2003, The Journal of cell biology.

[19]  R. Cummings,et al.  Model Glycosulfopeptides from P-selectin Glycoprotein Ligand-1 Require Tyrosine Sulfation and a Core 2-branched O-Glycan to Bind to L-selectin* , 2003, Journal of Biological Chemistry.

[20]  Cheng Zhu,et al.  Direct observation of catch bonds involving cell-adhesion molecules , 2003, Nature.

[21]  K. Schulten,et al.  Forced detachment of the CD2-CD58 complex. , 2003, Biophysical journal.

[22]  Kevin J. Naidoo,et al.  Carbohydrate solution simulations: Producing a force field with experimentally consistent primary alcohol rotational frequencies and populations , 2002, J. Comput. Chem..

[23]  Viola Vogel,et al.  Bacterial Adhesion to Target Cells Enhanced by Shear Force , 2002, Cell.

[24]  G. Waksman,et al.  Structural basis of tropism of Escherichia coli to the bladder during urinary tract infection , 2002, Molecular microbiology.

[25]  K. Schulten,et al.  Steered molecular dynamics and mechanical functions of proteins. , 2001, Current opinion in structural biology.

[26]  R. Cummings,et al.  Binding of Glycosulfopeptides to P-selectin Requires Stereospecific Contributions of Individual Tyrosine Sulfate and Sugar Residues* , 2000, The Journal of Biological Chemistry.

[27]  W. Somers,et al.  Insights into the Molecular Basis of Leukocyte Tethering and Rolling Revealed by Structures of P- and E-Selectin Bound to SLeX and PSGL-1 , 2000, Cell.

[28]  R. Alon,et al.  An Activated L-selectin Mutant with Conserved Equilibrium Binding Properties but Enhanced Ligand Recognition under Shear Flow* , 2000, The Journal of Biological Chemistry.

[29]  M. U. Nollert,et al.  Tyrosine replacement in P-selectin glycoprotein ligand-1 affects distinct kinetic and mechanical properties of bonds with P- and L-selectin. , 1999, Proceedings of the National Academy of Sciences of the United States of America.

[30]  K. Schulten,et al.  Unfolding of titin immunoglobulin domains by steered molecular dynamics simulation. , 1998, Biophysical journal.

[31]  Alexander D. MacKerell,et al.  All-atom empirical potential for molecular modeling and dynamics studies of proteins. , 1998, The journal of physical chemistry. B.

[32]  Timothy A. Springer,et al.  The Kinetics of L-selectin Tethers and the Mechanics of Selectin-mediated Rolling , 1997, The Journal of cell biology.

[33]  E. Evans,et al.  Dynamic strength of molecular adhesion bonds. , 1997, Biophysical journal.

[34]  K Schulten,et al.  VMD: visual molecular dynamics. , 1996, Journal of molecular graphics.

[35]  J. Dugdale The Electrical Properties of Disordered Metals: Comparison with experiment , 1995 .

[36]  D. Hammer,et al.  Lifetime of the P-selectin-carbohydrate bond and its response to tensile force in hydrodynamic flow , 1995, Nature.

[37]  J. Spudich,et al.  Single myosin molecule mechanics: piconewton forces and nanometre steps , 1994, Nature.

[38]  Kuo-Sen Huang,et al.  Insight into E-selectin/ligand interaction from the crystal structure and mutagenesis of the lec/EGF domains , 1994, Nature.

[39]  K. Ley,et al.  A role for the epidermal growth factor-like domain of P-selectin in ligand recognition and cell adhesion , 1994, The Journal of cell biology.

[40]  D. Torney,et al.  The reaction-limited kinetics of membrane-to-surface adhesion and detachment , 1988, Proceedings of the Royal Society of London. Series B. Biological Sciences.

[41]  G. I. Bell Models for the specific adhesion of cells to cells. , 1978, Science.

[42]  H. Kramers Brownian motion in a field of force and the diffusion model of chemical reactions , 1940 .