Biology subjects

Umeda, K.

Publications and source records attributed to Umeda, K..

4 recordsLinked to original sources

bioRxiv2023

High-speed AFM reveals fluctuations and dimer splitting of the N-terminal domain of GluA2-γ2

AMPA glutamate receptors (AMPARs) enable rapid excitatory synaptic transmission by localizing to the postsynaptic density of glutamatergic spines. AMPARs possess large extracellular N-terminal domains (NTDs), which participate in AMPAR clustering at synapses. Nevertheless, the dynamics of NTDs and the molecular mechanism governing their synaptic clustering remain elusive. Here, we employed high-speed atomic force microscopy (HS-AFM) to directly visualize the conformational dynamics of NTDs in the GluA2 subunit with TARP {gamma}2 in lipid environments. HS-AFM videos of GluA2-{gamma}2 in the resting and open states revealed fluctuations in NTD dimers. Conversely, in the desensitized state, the two NTD dimers adopted a separated conformation with less fluctuation. Notably, we visualized individual NTD dimers transitioning into monomers. Furthermore, this NTD-dimer splitting resulted in intersubunit exchange between NTD dimers and an increased number of binding sites with the synaptic protein neuronal pentraxin 1. Therefore, our findings illuminate the significance of NTD dynamics in the synaptic clustering of AMPARs.

neuroscience↗

bioRxiv2023

Deciphering the actin structure-dependent preferential cooperative binding of cofilin

The mechanism underlying the preferential and cooperative binding of cofilin and the expansion of clusters toward the pointed-end side of actin filaments remains poorly understood. To address this, we conducted a principal component analysis based on available filamentous actin (F-actin) and C-actin (cofilins were excluded from cofilactin) structures and compared to monomeric G-actin. The results strongly suggest that C-actin, rather than F-ADP-actin, represented the favourable structure for binding preference of cofilin. High-speed atomic force microscopy explored that the shortened bare half helix adjacent to the cofilin clusters on the pointed end side included fewer actin protomers than normal helices. The mean axial distance (MAD) between two adjacent actin protomers along the same long-pitch strand within shortened bare half helices was longer (5.0-6.3 nm) than the MAD within typical helices (4.3-5.6 nm). The inhibition of torsional motion during helical twisting, achieved through stronger attachment to the lipid membrane, led to more pronounced inhibition of cofilin binding and cluster formation than the presence of inorganic phosphate (Pi) in solution. F-ADP-actin exhibited more naturally supertwisted half helices than F-ADP.Pi-actin, explaining how Pi inhibits cofilin binding to F-actin with variable helical twists. We propose that protomers within the shorter bare helical twists, either influenced by thermal fluctuation or induced allosterically by cofilin clusters, exhibit characteristics of C-actin-like structures with an elongated MAD, leading to preferential and cooperative binding of cofilin.

molecular biology↗

bioRxiv2023

Evolutionarily acquired activity-dependent transformation of the CaMKII holoenzyme

Ca2+/calmodulin-dependent protein kinase II (CaMKII) has long been central in synaptic plasticity research. CaMKII is a dodecameric serine/threonine kinase that has been essentially conserved across metazoans for over a million years. While the mechanisms of CaMKII activation are well studied, its "behavior" at the molecular level has remained unobserved. Here, high-speed atomic force microscopy was used to visualize the activity-dependent structural dynamics of rat/hydra/C. elegans CaMKII in various states at nanometer resolution. Among the species, rat CaMKII underwent internal kinase domain aggregation in an activity-dependent manner and showed a higher tolerance to dephosphorylation by phosphatase. Our findings suggest that mammalian CaMKII has evolutionarily acquired a new structural form and a tolerance to phosphatase to maintain robust CaMKII activity for proper neuronal function. One-Sentence SummaryHigh-speed atomic force microscopy reveals the activity-dependent structural dynamics of rat/hydra/C. elegans CaMKII

neuroscience↗

bioRxiv2022

Activity-dependent glassy cell mechanics : Mechanical properties measured with active microrheology

Active microrheology was conducted in living cells by applying an optical-trapping force to vigorously-fluctuating tracer beads with feedback-tracking technology. The complex shear viscoelastic modulus G({omega}) = G'({omega}) - iG''({omega}) was measured in HeLa cells in an epithelial-like confluent monolayer. We found that G({omega}) {propto} (-i{omega})1/2 over a wide range of frequencies (1 Hz <{omega} /2{pi}<10 kHz). Actin disruption and cell-cycle progression from G1 to S and G2 phases only had a limited effect on G({omega}) in living cells. On the other hand, G ({omega}) was found to be dependent on cell metabolism; ATP-depleted cells showed an increased elastic modulus G'({omega}) at low frequencies, giving rise to a constant plateau such that G({omega}) = G0 + A(-i{omega})1/2. Both the plateau and the additional frequency dependency {propto} (-i{omega})1/2 of ATP-depleted cells are consistent with a rheological response typical of colloidal jamming. On the other hand, the plateau G0 disappeared in ordinary metabolically active cells, implying that living cells fluidize their internal states such that they approach the critical jamming point. Statement of SignificanceIntracellular mechanical properties were measured using optical-trap-based microrheology. Despite expectations to the contrary, shear viscoelasticity was hardly affected by reorganization of cytoskeletal structures during cell-cycle progression (G1 to S and G2 phases), nor by artificial disruption of the actin cytoskeleton induced by chemical inhibitors. Rather, the mechanics of cell interiors is governed by the glassy cytoplasm. Cells depleted of ATP solidified, whereas living cells that maintained metabolic activities were more fluid-like. Instead of a completely fluid response, however, we observed a characteristic power-law viscoelasticity G({omega}) {propto} (-i{omega})1/2 over the whole range of frequencies measured. Based on our current understanding of jamming rheology, we discuss how cells fluidize their internal state in a way that pushes the system towards the critical jamming transition.

biophysics↗