2009
DOI: 10.1103/physreve.79.051913
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Allosteric role of the large-scale domain opening in biological catch-binding

Abstract: The proposed model demonstrates the allosteric role of the two-domain region of the receptor protein in the increased lifetimes of biological receptor/ligand bonds subjected to an external force. The interaction between the domains is represented by a bounded potential, containing two minima corresponding to the attached and separated conformations of the two protein domains. The dissociative potential with a single minimum describing receptor/ligand binding fluctuates between deep and shallow states, dependin… Show more

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Cited by 28 publications
(40 citation statements)
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“…The two-state model has been subsequently used to explain catch-slip data from a number of biological systems like the bacterial FimH adhesive protein (Thomas et al, 2006; Pereverzev et al, 2009), kinetochore-microtubule attachments (Akiyoshi et al, 2010), cell surface sulfatase and glycosaminoglycan interactions (Harder et al, 2015) and cadherin-catenin interactions (Buckley et al, 2014). Among all these experiments, the work by Akiyoshi et al on kinetochore-microtubule attachments (Akiyoshi et al, 2010) is a remarkable validation of the two-state model.…”
Section: Phenomenological Theoriesmentioning
confidence: 99%
“…The two-state model has been subsequently used to explain catch-slip data from a number of biological systems like the bacterial FimH adhesive protein (Thomas et al, 2006; Pereverzev et al, 2009), kinetochore-microtubule attachments (Akiyoshi et al, 2010), cell surface sulfatase and glycosaminoglycan interactions (Harder et al, 2015) and cadherin-catenin interactions (Buckley et al, 2014). Among all these experiments, the work by Akiyoshi et al on kinetochore-microtubule attachments (Akiyoshi et al, 2010) is a remarkable validation of the two-state model.…”
Section: Phenomenological Theoriesmentioning
confidence: 99%
“…These include energy landscapes with one bound state and two unbinding pathways 43 ; an energy landscape with two bound states, one of which is preferentially stabilized by force 44,45 ; bond dissociation along a multidimensional landscape where the direction of the tensile force and the reaction coordinate are misaligned [46][47][48] ; a freeenergy landscape with dynamic disorder that thermally fluctuates with time 49,50 ; and allosteric deformation models where external force changes the structure of the receptor either directly at the ligand-binding site 51 or at a distal location that ultimately propagates the deformation to the binding pocket [52][53][54][55] . Our simulations suggest that X-dimers form catch bonds via a slidingrebinding mechanism where a pulling force flexes the ectodomain and slides opposing EC1 domains resulting in the formation of de novo, force-induced H-bonds.…”
Section: Article Nature Communications | Doi: 101038/ncomms4941mentioning
confidence: 99%
“…11, and in Ref. 43. Further, the properties of function h ( f ) rationalize the rapid drop in the number of bonds surviving by time t , as discussed below.…”
Section: Comparison With Experimentsmentioning
confidence: 78%
“…As a result, the average lifetimes of the systems shown in Fig. 5 are well described using the following particularly simple expression τ¯(f)[k12(f)+k21(f)]/[k1(f)k21(f)+k2(f)k12(f)] that was used in our earlier work 43. The lines computed using Eq.…”
Section: Comparison With Experimentsmentioning
confidence: 84%
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