This review develops that process of biological recognition as a problem in statistical mechanics, Counting the ways two multivalent objects can bind proves to be the classical monomer-dimer problem on a graph, with a rigorous consequence.
Abstract
Biological recognition rarely rests on one strong bond. It works by forming many weak ones at once, between crowded, deformable surfaces in water. This review develops that process as a problem in statistical mechanics. Counting the ways two multivalent objects can bind proves to be the classical monomer-dimer problem on a graph, with a rigorous consequence: the apparent switching of multivalent binding is always a smooth crossover, never a phase transition. Three constraints follow. A repulsive surface layer is obligatory rather than a design choice; bonds do not act independently; and since free energies enter rates exponentially, small changes in receptor number shift binding lifetimes by orders of magnitude. One set of equations then covers antibodies, lipoproteins, and T cell recognition. In each, what decides the outcome is not the strength of any single bond but how a fixed total is spread over many: affinity is a property of a molecule, selectivity a property of an assembly.
A minimal two-dimensional TCR–pMHC mechanochemical energy-landscape model is formulated in which peptide-dependent allosteric binding geometry, hinge elasticity, receptor extension, binding-site separation and applied force jointly determine the activation barrier and bond lifetime.
Yogesh B. Bali, Alan D. Rendall, W. Quapp· Royal Society Open Science· 0 citations
Kinetic models of protein aggregation describe populations by size, not by spatial organization or morphology. We extend Lumry-Eyring nucleated polymerization to a model in which the monomer is a density field and each aggregate is a region bounded by a level set. Growth is a flux condition on the available sites of a...
The valency-bounding correction (VBC), a many-body modification of generic short-range pairwise potentials that smoothly suppresses attraction once the neighbour count of either interacting particle exceeds a prescribed valency, is introduced.
V. Dmitriev, Ankit Gupta, A. Goloborodko· 0 citations
Systems in which the free energy density is nonuniform in space are familiar; the surface tension of a water droplet and the surface energy of a solid are good examples. Some such cases can be treated with prior theory, notably inhomogeneous solvation theory (IST), but IST is applicable only to liquids. Despite this...
Michael K. Gilson, Joe Cruz, Kun-Huan Liu et al.· Journal of Physical Chemistr...· 0 citations
Exact statements about how a system far from equilibrium responds to changes in its rate constants are scarce beyond linear response, yet they are central to the control of biochemical networks. A notable exception is mutual linearity: in a jump process, controlling the rates of a single transition makes any two statio...
Pedro E. Harunari, Guilherme Fiusa, Matteo Polettini· 1 citation