Mechanotransduction from the extracellular matrix into the cell is primarily supervised by a transmembrane receptor, integrin, and a cytosolic protein, talin. Integrin binds ligands on the extracellular side, whereas talin couples integrin receptors to the actin cytoskeleton and later acts as a "force buffer". Talin and integrin together form a mechanosensitive signaling hub that regulates crucial cellular processes and pathways, including cell signaling and formation of focal adhesion complexes, which help cells to sense their mechanoenvironment and transduce the signal accordingly. Although both proteins function in tandem, most literature focuses on them individually. Here, we provide a focused review of the talin−integrin mechano-interactome network in light of its role in the process of mechanotransduction and its connection to diseases. While working under force, these proteins drive numerous biomolecular interactions and form adhesion complexes, which in turn control many physiological processes such as cell migration; thus, they are invariably associated with several diseases from leukocyte adhesion deficiency to cancer. Gaining insights into their role in the occurrence of these pathological disorders might lead us to establish treatment methods and therapeutic techniques.

Talin as a critical focal adhesion mechanosensor exhibits force-dependent folding dynamics and concurrent interactions. Being a cytoplasmic protein, talin also might interact with several cytosolic chaperones; however, the roles of chaperones in talin mechanics remain elusive. To address this question, we investigated the force response of a mechanically stable talin domain with a set of well-known unfoldase (DnaJ, DnaK) and foldase (DnaKJE, DsbA) chaperones, using single-molecule magnetic tweezers. Our findings demonstrate that chaperones could affect adhesion proteins’ stability by changing their folding mechanics; while unfoldases reduce their unfolding force from ~11 pN to ~6 pN, foldase shifts it upto ~15 pN. Since talin is mechanically synced within 2 pN force ranges, these changes are significant in cellular conditions. Furthermore, we determined that chaperones directly reshape the energy landscape of talin: unfoldases decrease the unfolding barrier height from 26.8 to 21.7 kBT, while foldases increase it to 33.5 kBT. We reconciled our observations with eukaryotic Hsp70 and Hsp40 and observed their similar function of decreasing the talin unfolding barrier. Quantitative mapping of this chaperone-induced talin folding landscape directly illustrates that chaperones perturb the adhesion protein stability under physiological force, thereby, influencing their force-dependent interactions and adhesion dynamics.

Structure-function dynamics of protein, as a flexible polymer, is essential to describe their biological functions. Here, using a single-molecule magnetic tweezers, we have studied the effect of ionic strength on...

Protein folding under force is an integral source of generating mechanical energy in various cellular processes, ranging from protein translation to degradation. Although chaperones are well known to interact with proteins under mechanical force, how they respond to force and control cellular energetics remains unknown. To address this question, we introduce a real-time magnetic tweezer technology herein to mimic the physiological force environment on client proteins, keeping the chaperones unperturbed. We studied two structurally distinct client proteins––protein L and talin with seven different chaperonesindependently and in combination and proposed a novel mechanical activity of chaperones. We found that chaperones behave differently, while these client proteins are under force, than their previously known functions. For instance, tunnel-associated chaperones (DsbA and trigger factor), otherwise working as holdase without force, assist folding under force. This process generates an additional mechanical energy up to ∼147 zJ to facilitate translation or translocation. However, well-known cytoplasmic foldase chaperones (PDI, thioredoxin, or DnaKJE) do not possess the mechanical folding ability under force. Notably, the transferring chaperones (DnaK, DnaJ, and SecB) act as holdase and slow down the folding process, both in the presence and absence of force, to prevent misfolding of the client proteins. This provides an emerging insight of mechanical roles of chaperones: they can generate or consume energy by shifting the energy landscape of the client proteins toward a folded or an unfolded state, suggesting an evolutionary mechanism to minimize energy consumption in various biological processes.

Studies of free energy, kinetics or elasticity are common to most disciplines of science. Detailed quantification of these properties demands number of specialized technologies. Furthermore, monitoring 'perturbation' in any of these properties, in presence of external stimuli (protein/DNA/drugs/nanoparticles etc.), requires multiple experiments. However, none of these available technologies can monitor these perturbations simultaneously in real time on the very same molecule in a single shot experiment.Here we present real-time microfluidics-magnetic tweezers technology with the unique advantage of tracking a single protein dynamics for hours, in absence of any significant drift, with the flexibility of changing physical environment in real time. Remarkable stability of this technique allows us to quantify five molecular properties (unfolding kinetics, refolding kinetics, conformational change, chain flexibility, and ∆G for folding/unfolding), and most importantly, their dynamic perturbation upon interacting with salt on the same protein molecule from a single experiment. We observe salt reshapes the energy landscape by two specific ways: increasing the refolding kinetics and decreasing the unfolding kinetics, which is characterized as mean first passage time. Importantly, from the same trajectory, we calculated the flexibility of the protein polymer, which changes with salt concentration and can be explained by our modified 'electrolyte FJC model'. The correlation between ∆G, kinetics and polymer elasticity strongly argues for a stiffness driven energy landscape of proteins. Having the advantage of sub nanometer resolution, this methodology will open new exciting window to study proteinsone such examples is demonstrated in this article: electrolyte driven conformational fluctuation under force, which was not studied before.