TCR–Pmhc Kinetics Under Force in a Cell-Free System Show No Intrinsic Catch Bond, but a Minimal Encounter Duration Before Bind

TCR–Pmhc Kinetics Under Force in a Cell-Free System Show No Intrinsic Catch Bond, but a Minimal Encounter Duration Before Bind

TCR–pMHC kinetics under force in a cell-free system SEE COMMENTARY show no intrinsic catch bond, but a minimal encounter duration before binding Laurent Limozina, Marcus Bridgeb, Pierre Bongranda, Omer Dushekb, Philip Anton van der Merweb, and Philippe Roberta,1 aLaboratoire Adhesion et Inflammation, UMR INSERM 1067, UMR CNRS 7333, Aix-Marseille Université, Assistance Publique–Hôpitaux de Marseille, Case 937, 13288 Marseille Cedex 09, France; and bSir William Dunn School of Pathology, University of Oxford, Oxford OX1 3RE, United Kingdom Edited by Michael L. Dustin, Kennedy Institute of Rheumatology, Headington, United Kingdom, and accepted by Editorial Board Member Peter Cresswell June 19, 2019 (received for review February 8, 2019) The T cell receptor (TCR)–peptide-MHC (pMHC) interaction is the discrimination between pMHC, while also reducing the vari- only antigen-specific interaction during T lymphocyte activation. ability of bond lifetimes (18). For these reasons, efforts have Recent work suggests that formation of catch bonds is character- been made to measure TCR–pMHC 2D dissociation kinetics and istic of activating TCR–pMHC interactions. However, whether this the effect of mechanical force thereon. Independent studies us- binding behavior is an intrinsic feature of the molecular bond, or ing the biomembrane force probe (BFP) (19–22) or optical a consequence of more complex multimolecular or cellular re- tweezers (23) on live cells, or using optical tweezers in cell-free sponses, remains unclear. We used a laminar flow chamber to experimental setup (23, 24) reported that activating TCR– measure, first, 2D TCR–pMHC dissociation kinetics of peptides of pMHC interactions exhibit a decrease in off-rate when exposed various activating potency in a cell-free system in the force range to mechanical force in the 10- to 15-pN range, i.e., catch bonds. (6 to 15 pN) previously associated with catch–slip transitions and, It was therefore suggested that T cells might probe the TCR– second, 2D TCR–pMHC association kinetics, for which the method pMHC bond by exerting a pull on the order of 10 pN, with ac- is well suited. We did not observe catch bonds in dissociation, and tivating peptides displaying a nonintuitive increase bond lifetime INFLAMMATION the off-rate measured in the 6- to 15-pN range correlated well with that made it 10-fold higher than the lifetime of nonactivating IMMUNOLOGY AND activation potency, suggesting that formation of catch bonds is not an peptides (19). This raises 2 questions: 1) bonds formed by T cells intrinsic feature of the TCR–pMHC interaction. The association kinetics and APCs are not only bimolecular interactions but depend on were better explained by a model with a minimal encounter duration complex cellular processes (10, 11). Thus, a cell-free system is rather than a standard on-rate constant, suggesting that membrane necessary to check that the catch bond effect is a cause, not a fluidity and dynamics may strongly influence bond formation. consequence, of high activation by efficient agonists. We pre- viously measured dissociation kinetics of TCR and observed in- TCR | kinetics | force | association creases in off-rate with force, i.e., slip bonds. However, the forces BIOPHYSICS AND applied were higher than 15 pN, precluding a direct comparison COMPUTATIONAL BIOLOGY lymphocyte activation begins with the binding of the T cell with aforementioned results (25). 2) Since T cell discrimination Treceptor (TCR) on the lymphocyte surface to an antigenic peptide carried by a major histocompatibility complex (pMHC) Significance molecule on the antigen-presenting cell (APC) surface, trigger- ing a cascade of signaling events. The TCR is the only antigen- T lymphocytes use their T cell receptors (TCRs) to discriminate specific molecule of the T lymphocyte activation, making the – between similar peptide-MHC (pMHC) antigens. The mecha- TCR pMHC interaction a decisive step. A long-standing prob- nisms employed to achieve this discrimination are debated. The lem was to understand the basis of the exquisite specificity of T TCR–pMHC interaction is subjected to forces, and recent work lymphocytes. While discrimination between different pMHCs – in live T cells has suggested that force paradoxically increases seems based on quantitative properties of the TCR pMHC bond TCR–pMHC bond lifetimes for activating peptides, forming so- such as its lifetime (1), bond rupture is a stochastic event, making called “catch bonds,” facilitating discrimination from non- a single lifetime measurement insufficient to discriminate be- activating peptides. A question is whether this behavior is in- tween peptides forming bonds with only limited lifetime differ- trinsic to the TCR–pMHC bond or a cellular response. We ence (2). Several studies using surface plasmon resonance mostly – – measured TCR pMHC lifetimes under force in a cell-free sys- reported a correlation between a TCR pMHC bond off-rate tem: lifetimes correlated well with activation potency of the measured in solution (3D) and its lymphocyte activation po- TCR–pMHC bonds, while no catch bonds were observed. – tency (1, 3 6), leading to the kinetic proofreading model (7). However, a minimum encounter duration is necessary for bond – However, as the TCR pMHC interaction takes place between 2 formation, which could increase specificity. cell surfaces, it is subjected both to a disruptive force and to 2D motions linked to membrane fluidity and dynamics, which may Author contributions: P.R. designed research; L.L. and P.R. performed research; M.B. and profoundly change the kinetics of molecular interactions (8–11). P.A.v.d.M. contributed new reagents/analytic tools; L.L., P.B., O.D., P.A.v.d.M., and P.R. Furthermore, TCR triggering is sensitive to mechanical forces analyzed data; and P.R. wrote the paper. (12–16). Multiple bond lifetime measurements might be needed The authors declare no conflict of interest. by the cell to overcome the stochasticity of bond rupture (17). This article is a PNAS Direct Submission. M.L.D. is a guest editor invited by the However, due to the duration needed for such repeated assays Editorial Board. and the time constraint of T lymphocyte activation, it has been Published under the PNAS license. proposed that force application might be a way to strongly re- See Commentary on page 16669. duce the lifetime of the TCR–pMHC bonds, to allow numerous, 1To whom correspondence may be addressed. Email: [email protected]. repeated measurements in a short time (17, 18). Force might This article contains supporting information online at www.pnas.org/lookup/suppl/doi:10. also be exploited by the cell to test additional discriminating 1073/pnas.1902141116/-/DCSupplemental. parameters such as bond sensitivity to force, further improving Published online July 17, 2019. www.pnas.org/cgi/doi/10.1073/pnas.1902141116 PNAS | August 20, 2019 | vol. 116 | no. 34 | 16943–16948 Downloaded by guest on September 28, 2021 may involve multiple TCR–pMHC interactions, measuring the for 3Y, and R2 = 0.92 for 9L (SI Appendix, Fig. S1). Survival kinetics of bond formation as well as dissociation is necessary to curves remained unchanged at least for the 2 highest consecutive fully assess the properties of TCR–pMHC interaction. amounts of ligand in this range (SI Appendix, Fig. S2); arrests While several groups have examined 2D dissociation kinetics, were therefore considered to be the consequence of formation of studies of the 2D association kinetics of the TCR and pMHC are single molecular bonds. scarce and were limited by the methods used. Two-dimensional association measurements need a quantification of both the Activating pMHCs Do Not Necessarily Form Catch Bonds with TCRs. binding events and the distribution of the durations of the mo- We measured the dissociation kinetics of the 5 agonist TCR– lecular encounters that may lead to binding; these encounter pMHC pairs under force ranging from 6 to 45 pN. The slope durations need to be in a physiologically relevant range. Before of survival curves (where the logarithm of the fraction of sur- pulling, both BFP and optical tweezers bring into contact TCR viving bonds is plotted versus time; SI Appendix, Figs. S2 and S3) and pMHC-bearing surfaces for durations of several hundreds of is equal to the off-rate. To account simply for the change of slope milliseconds, much longer than membrane fluidity and dynamics with time suggesting a bond strengthening (SI Appendix, Fig. S3), would allow (11, 23). The thermal fluctuation assay relies on we chose to consider the average slope, or off-rate, on the 5 first spontaneous membrane fluctuations bringing into contact both seconds. This was justified by calculating for each force the surfaces (19). While contact durations may be much shorter than correlation between the peptide activation potency and the av- in BFP or optical tweezers, neither duration of encounter nor erage off-rate calculated at variable intervals (SI Appendix, Fig. applied force are controlled. In contrast, our laminar flow S4). An interval of 5 s ensured a maximal correlation coefficient chamber enables control of a distribution of encounter durations at each force. The corresponding average half-lives are calcu- in the millisecond range (26, 27) and is thus well suited for 2D lated from the average off-rate between 0 and 5 s [koff(0–5s)]as association measurements after molecular encounters of short equal to ln(2)/koff(0–5s). Fig. 1 shows the half-lives plotted versus duration. The description of 2D bond formation is usually based force: 3A, 3Y, and 9L behave as slip bonds, with off-rate in- on on-rates, corresponding to 1 free energy barrier leading to 1 creasing with force. H74 and 9V are little influenced by force in free energy well. Probability of bond formation as a function of this range. the duration te during which a receptor can interact with its li- gand (referred later as “encounter duration”) can be written as Dissociation Kinetics Show Good Correlation with Activation Potency Pðt Þ = f × ð − ð−k × t ÞÞ f e E 1 exp on e , where E is a proportionality from 6 to 15 pN.

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