Biology subjects

Benayad, Z.

Publications and source records attributed to Benayad, Z..

3 recordsLinked to original sources

bioRxiv2026

Structural mechanism of Gasdermin E-mediated mtDNA release from apoptotic mitochondria

During apoptosis, the permeabilization of the mitochondrial inner membrane (MIM) through still-unclear mechanisms releases mtDNA into the cytosol, triggering the inflammatory cGAS/STING pathway under low caspase activity. Here, we report that, in apoptosis, the active form of the pore-forming protein Gasdermin E (GSDME-N) damages mitochondria before plasma membrane disruption. We visualize GSDME-N pore-like nano-assemblies in the MIM of apoptotic cells and of isolated mitochondria, which we bridge with the cryo-EM structure of the GSDME-N pore in mitochondria-like membranes. Deep membrane insertion of the anchor domain, which acts as a determinant of GSDME-N cardiolipin binding preferences, supports a role in pore formation. Notably, GSDME depletion results in a reduction in cristae swelling, MIM extrusion and mtDNA release during apoptosis. Subsequently, this decreases STING activation and inflammatory responses under caspase inhibition. Our findings reveal that GSDME mediates MIM permeabilization and mtDNA release during apoptosis and define the mechanism of GSDME-mediated membrane damage.

molecular biology↗

bioRxiv2026

Chemically tunable permeability of engineered alpha-Hemolysin in synthetic cells

Controlling molecular transport across membranes is a defining feature of living cells, yet replicating this functionality in synthetic systems remains a major challenge. Self-inserting protein nanopores, such as -hemolysin (HL), offer a promising route towards programmable membrane permeability due to their robust assembly, compatibility with diverse membrane systems, and intrinsic permeability for diverse biomolecules. Here, we explored the use of chemically functionalized HL nanopores as tunable transport modules. To quantify translocation of peptide substrates across HL-containing membranes, we developed a high-throughput luminescence-based breakage-controlled assay using large unilamellar vesicles. With this assay we introduce a one-pot nanopore modification and strategy, compatible with scalable workflows. Electrophysiology and molecular simulations demonstrate that the introduction of cysteine residues at defined pore locations, combined with targeted chemical modification, enables controlled tuning of HL-nanopore selectivity based on peptide structure and charge. Together, these findings position engineered protein nanopores as versatile and responsive components for controlling membrane transport in synthetic biology.

synthetic biology↗

bioRxiv2020

Simulation of FUS protein condensates with an adapted coarse-grained model

Disordered proteins and nucleic acids can condense into droplets that resemble the membraneless organelles observed in living cells. MD simulations offer a unique tool to characterize the molecular interactions governing the formation of these biomolecular condensates, their physico-chemical properties, and the factors controlling their composition and size. However, biopolymer condensation depends sensitively on the balance between different energetic and entropic contributions. Here, we develop a general strategy to fine-tune the potential energy function for molecular dynamics simulations of biopolymer phase separation. We rebalance protein-protein interactions against solvation and entropic contributions to match the excess free energy of transferring proteins between dilute solution and condensate. We illustrate this formalism by simulating liquid droplet formation of the FUS low complexity domain (LCD) with a rebalanced MARTINI model. By scaling the strength of the nonbonded interactions in the coarse-grained MARTINI potential energy function, we map out a phase diagram in the plane of protein concentration and interaction strength. Above a critical scaling factor of c {approx} 0.6, FUS LCD condensation is observed, where = 1 and 0 correspond to full and repulsive interactions in the MARTINI model, respectively. For a scaling factor = 0.65, we recover the experimental densities of the dilute and dense phases, and thus the excess protein transfer free energy into the droplet and the saturation concentration where FUS LCD condenses. In the region of phase separation, we simulate FUS LCD droplets of four different sizes in stable equilibrium with the dilute phase and slabs of condensed FUS LCD for tens of microseconds, and over one millisecond in aggregate. We determine surface tensions in the range of 0.01 to 0.4mN/m from the fluctuations of the droplet shape and from the capillary-wave-like broadening of the interface between the two phases. From the dynamics of the protein end-to-end distance, we estimate shear viscosities from 0.001 to 0.02Pas for the FUS LCD droplets with scaling factors in the range of 0.625 to 0.75, where we observe liquid droplets. Significant hydration of the interior of the droplets keeps the proteins mobile and the droplets fluid.

biophysics↗