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In this experiment, a microtubule was immobilized to a biotinylated coverslip, and Ndc80 complexes, a key protein complex in the kinetochore structure, were attached to streptavidin-coated beads. By moving the bead with the C-Trap, we generated a rupture force between the microtubule and the kinetochore structure.
Researchers from David Barford’s team quantitatively assessed the outer kinetochore’s force resistance of the Dam1 and Ndc80 complexes. By comparing rupture forces of various mutations, they get a better understanding of which protein domains influence the kinetochore’s ability to withstand microtubule forces during cell division.
Case study
Measuring membrane tension is challenging as it requires precise manipulation and measurement of mechanical forces on individual tethers, which are small and difficult to control. With the C-Trap this could be resolved by combining optical tweezers for direct measurement of mechanical forces on individual tethers with optogenetics for local endogenous control of cell protrusion.
By using this combination of techniques, the lab of Bustamante was able to directly measure changes in membrane tension in response to mechanical forces generated by actin-driven protrusions. This allowed them to demonstrate that these protrusions generate rapid long-range membrane tension propagation in cells, which provides new insights into how cells respond to external stimuli and adapt to their environment.
Case study
Left: A dual-tether pulling assay to simultaneously monitor membrane tension on the far end (left, trap 1 at 180°) and on the side of the cell (top, trap 2 at 90°) during light-activated protrusion. Right: Representative time traces of dual trap forces over successive cycles of light-activated protrusion show coinciding tension increases on both membrane tethers adjacent to (trap 2) and at the opposite cell surface from (trap 1) protrusion; light: 90 s on (shaded area), 180 s off. Figure from De Belly et al. (2023), Cell
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What are the rules of membrane tension propagation in cells? For proper function, cells need to link short-range biochemical signaling events with long-range integration of cell physiology. Forces transmitted through the plasma membrane are thought to serve as this globally integrator. However, conflicting observations have left the field divided as to whether cell membranes support or resist tension propagation. This discrepancy likely originates from the use of exogenous forces that may not accurately mimic endogenous forces. We overcome this complication by leveraging optogenetics to directly control localized actin-based protrusions or actomyosin contractions while simultaneously monitoring the propagation of membrane tension using dual-trap optical tweezers. Surprisingly, actin-driven protrusions and actomyosin contractions both elicit rapid global membrane tension propagation, whereas forces applied to cell membranes alone do not. We present a simple unifying mechanical model in which mechanical forces that engage the actin cortex drive rapid, robust membrane tension propagation through long-range membrane flows.
First-generation bispecific T cell engagers (BTEs) have shown promise in preclinical models but often suffer from a short plasma half-life due to their small size and absence of an Fc domain. Additionally, limited tumor retention can lower local therapeutic concentrations and impede efficacy. Cancer cells can even adapt and evade immune targeting through antigen heterogeneity and loss, threatening sustained responses. The immunosuppressive tumor microenvironment further hinders T cell function and promotes therapeutic resistance. To develop an effective strategy, any cell engager must overcome these barriers to achieve robust, consistent targeting and immune activation.
Case study
A team led by David Weiner, PhD have examined how format-tuning bispecific T cell engagers (BTEs) boosts therapeutic efficacy against clear cell renal cell carcinoma (ccRCC). Using a novel persistent multivalent T cell engager (PMTE) to enhance cell avidity and tumor targeting, they tackle challenges like low plasma half-life, poor tumor retention, and antigen escape. Optimizing cell interactions through avidity-driven design offers a pathway to more effective, durable cancer therapies and renewed hope for advanced ccRCC patients.
Binding correlated with in vivo tumor cell-killing efficacy. Comparing the three BTE formats shows a significant delay in tumor volume increase between BTE, PBTE and PMTE. Data adapted from O’Connell et al. (CC-BY-NC)
Cell avidity curves represent the % of target cells bound with rising detachment force measured at 30 nM, 3 nM and 300 pM antibody concentration. Area-under-curve quantifications indicate the significant differences in cell avidity between PBTE and PMTE at relevant concentrations. Adapted from: O’Connell et al. (CC-BY-NC)
This study compared three BTE formats. Left: single-chain “BTE” with a tumor-targeting aCA9 linked to the T cell-targeting aCD3. Center: second-generation PBTE which reintroduces an Fc domain. Right: PMTE format which adds another tumor-targeting aCA9 part.
The following experiment highlights the forces and kinetics associated with filopodia formation. To assess the process, we studied Dictyostelium discoideum cells, a eukaryotic amoeba cell and model system that is commonly used to understand human cell processes.
Case study
We moved the bead in proximity to the D. discoideum cell, ectopically expressing GFP-Myosin 7 (blue signal) and actin filament marker RFP-LifeAct. The cell moved in the direction of the trapped bead, extending multiple protrusions towards it upon sensing the proximity of the object.
We observed a characteristic signal every time the cell engulfed the bead (Figure 2). Interestingly, we also found an occasional force spike right before bead engulfment. Since we observed the formation and retraction of one of the formed filopodia touching the bead, we suggest that this peak possibly is caused by the interaction between the cell protrusion and the bead. Thus, the maximum value shown on the graph (around 20 pN) corresponds to the force that a single protrusion exerted over the foreign object.
Sample courtesy of Prof. Dr. Margaret Titus at the University of Minnesota
Confocal images of a cell interacting with a trapped bead, including GFP-Myosin 7 (blue signal) and actin filament marker RFP-LifeAct (green signal). The graph depicts the measured forces exerted by cell protrusions on the bead over time.
The C-Trap can also manipulate small components inside of living multicellular organisms. We used the optical tweezers to manipulate intrinsic lipid droplets and study droplet fusion inside of Caenorhabditis elegans (roundworm).
Case study
Using brightfield microscopy, we can quickly scan cell samples with a micrometer-precision stage and, on top of that, obtain fine movements when needed using a nanometer-precision positioning system. These features allow us to optically trap droplets in two ways: dragging the droplets around the body, thus exposing them to each other, or keeping them at the same position and letting the stage bring other droplets into the proximity of the trapped molecule.
The approach allowed us to follow the small components in vivo and in real time and assess forces associated with the fusion process (Figure 3).
Sample courtesy of Prof. Dr. Daniel Starr at the University of California, Davis
Brightfield microscopy imaging showing directional manipulation of a lipid droplet (indicated by the red arrow) with a laser (focused in the center of the red circle) inside the C. elegans.
The C-Trap® provides the world’s first dynamic single-molecule microscope to allow simultaneous manipulation and visualization of single-molecule interactions in real time.