Mechanosensitive Channels

Microbial survival in dynamic environments requires the ability to successfully respond to abrupt changes in osmolarity. The mechanosensitive channel of large conductance (MscL) is a ubiquitous channel that facilitates the survival of bacteria and archaea under severe osmotic downshock conditions by relieving excess turgor pressure in response to increased membrane tension. A prominent structural feature of MscL, the cytoplasmic C-terminal domain, has been suggested to influence channel assembly and function. In this report, we describe the X-ray crystal structure and electrophysiological properties of a C-terminal domain truncation of the Mycobacterium tuberculosis MscL (MtMscLΔC). A crystal structure of MtMscLΔC solubilized in the detergent n-dodecyl-β-D-maltopyranoside reveals the pentameric, closed state-like architecture for the membrane spanning region observed in the previously solved full-length MtMscL. Electrophysiological characterization demonstrates that MtMscLΔC retains mechanosensitivity, but with conductance and tension sensitivity more closely resembling full length EcMscL than MtMscL. This study establishes that the C-terminal domain of MtMscL is not required for oligomerization of the full-length channel, but rather influences the tension sensitivity and conductance properties of the channel. The collective picture that emerges from these data is that each MscL channel structure has characteristic features, highlighting the importance of studying multiple homologs. Mechanosensitive (MS) channels transduce mechanical stimuli into a variety of cellular responses. MS channels are widely distributed through all kingdoms of life, including bacteria and archaea, where they play a prominent role in maintaining proper osmoregulation 1-5. Sudden changes in osmolarity, such as osmotic downshock during exposure to hypotonic conditions, increases turgor pressure across the cell membrane. This in turn increases the tension within the lipid bilayer and activates a network of MS channels which respond by opening typically nonselective pores in the membrane to release cell contents and alleviate the pressure 1,5-7. Bacterial MS channels are characterized by their relatively high and non-selective conductances, ranging from ~0.1 nS to ~3 nS under defined experimental conditions 6-8 , which is up to several orders of magnitude greater than typical for ion-selective channels 3,6,9. Of these channels, the mechanosensitive channel of large conductance (MscL) exhibits the largest conductance, with an estimated open state pore diameter of ~25-35 Å-large enough for the passage of molecules up to 9 kDa 4,7,10,11. In view of the high conductance yet small subunit size of MscL (Escherichia coli MscL (EcMscL) has 136 residues; Fig. 1), the oligomeric nature of this channel was appreciated from its initial discovery 11. Considerable efforts have been made to establish the molecular mechanism of MscL gating 3,12 , employing a variety of techniques including electrophysiology, biochemical and genetic studies, molecular dynamics

Mechanosensitive channels are integral components for the response of bacteria to osmotic shock. The mechanosensitive channel of large conductance (MscL) responds to extreme turgor pressure increase that would otherwise lyse the cellular membrane. MscL has been studied as a model mechanosensitive channel using both structural and functional approaches. We will summarize the structural data and discuss outstanding questions surrounding the gating mechanism of this homo-oligomeric channel that has~3 nS conductance. Specifically, we will explore the following: (1) the variability in oligomeric state that has been observed, (2) the open pore size measurements, and (3) the role of the C-terminal coiled coil domain for channel function. The oligo-meric state of MscL has been characterized using various techniques, with a pentamer being the predominant form; however, the presence of mixtures of oligomers in the membrane is still uncertain. In the absence of structural data for the open state of MscL, the diameter of the open state pore has been estimated by several different approaches, leading to a current estimate between 25 and 30 Å. While the C-terminal domain is highly conserved among MscL homologues, it is not required for activity in vivo or in vitro. This domain is likely to remain intact during the gating transition and perform a filtering function that retains valuable osmolytes in the cytosol. Overall, studies of MscL have provided significant insight to the field, and serve as a paradigm for the analysis of non-homologous, eukaryotic mechanosensitive channel proteins.

Log phase Bacillus subtilis cells lacking the mscL gene encoding the mechanosensitive (MS) channel of large conductance are sensitive to an osmotic downshock > or =0.5 M. However, B. subtilis mscL cells develop osmotic downshock resistance in late log and early stationary phase growth that is partially dependent on three likely MS channel proteins of small conductance (MscS), YfkC, YhdY, and YkuT. Bacillus subtilis MS proteins were fused with green fluorescent protein (GFP) at their C termini; at least the MscL-, YfkC-, and YkuT-GFP fusions were functional and overexpression of YkuT-GFP, or YkuT alone abolished log phase mscL cells' osmotic downshock sensitivity. Western blot analysis found high levels of MscL-GFP in early exponential phase cells with levels subsequently decreasing greatly. MscS-GFP proteins were present in exponential phase cells, but again disappeared almost completely in stationary phase cells and these proteins were not detected in spores. Western blot analyses further showed that MS-GFP proteins were associated with the plasma membrane, as expected. Fluorescence microscopy confirmed the localization of MscL-GFP and YhdY-GFP to the plasma membrane, with non-uniform distribution of these proteins along this membrane consistent with but by no means proving that these proteins are present in a helical array.

Hearing relies on the conversion of mechanical stimuli into electrical signals. In vertebrates, this process of mechano-electrical transduction (MET) is performed by specialized receptors of the inner ear, the hair cells. Each hair cell is crowned by a hair bundle, a cluster of microvilli that pivot in response to sound vibrations, causing the opening and closing of mechanosensitive ion channels. Mechanical forces are projected onto the channels by molecular springs called tip links. Each tip link is thought to connect to a small number of MET channels that gate cooperatively and operate as a single transduction unit. Pushing the hair bundle in the excitatory direction opens the channels, after which they rapidly reclose in a process called fast adaptation. It has been experimentally observed that the hair cell's biophysical properties mature gradually during postnatal development: the maximal transduction current increases, sensitivity sharpens, transduction occurs at smaller hair-bundle displacements, and adaptation becomes faster. Similar observations have been reported during tip-link regeneration after acoustic damage. Moreover, when measured at intermediate developmental stages, the kinetics of fast adaptation varies in a given cell depending on the magnitude of the imposed displacement. The mechanisms underlying these seemingly disparate observations have so far remained elusive. Here, we show that these phenomena can all be explained by the progressive addition of MET channels of constant properties, which populate the hair bundle first as isolated entities, then progressively as clusters of more sensitive, cooperative MET channels. As the proposed mechanism relies on the difference in biophysical properties between isolated and clustered channels, this work highlights the importance of cooperative interactions between mechanosensitive ion channels for hearing. SIGNIFICANCE Hair cells are the sensory receptors of the inner ear that convert mechanical stimuli into electrical signals transmitted to the brain. Sensitivity to mechanical stimuli and the kinetics of mechanotransduction currents change during hair-cell development. The same trend, albeit on a shorter timescale, is also observed during hair-cell recovery from acoustic trauma. Furthermore, the current kinetics in a given hair cell depends on the stimulus magnitude, and the degree of that dependence varies with development. These phenomena have so far remained unexplained. Here, we show that they can all be reproduced using a single unifying mechanism: the progressive formation of channel pairs, in which individual channels interact through the lipid bilayer and gate cooperatively.

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Parabens are alkyl esters of p-hydroxybenzoic acid used as preservatives in a wide range of food, pharmaceutical, and cosmetic products (Soni et al. Food Chem. Toxicol. 39:513–532, 2001). Despite their common use for over 50 years, their mechanism of action is still unclear. In this study we examined the effects of ethyl and propyl paraben, on gating of the E. coli mechanosensitive channel of large conductance (MscL) reconstituted into azolectin liposomes. We found that propyl and ethyl paraben spontaneously activate MscL. Moreover, the addition of propyl paraben caused an increase in MscL activity and the lowering of p 1/2, the pressure at which the MscL was opened 50% of the time, the ΔG o, the free energy required to open the MscL, and the parameter α, which describes the channel sensitivity to pressure. In addition, in silico studies showed that propyl paraben binds to the channel gate of the MscL. The mechanosensitive channel of small conductance was also found to be spontaneously activated by parabens. In summary, our study indicates that one of the previously unidentified mechanisms of action of parabens as antimicrobial agents is via an interaction with the mechanosensitive channels to upset the osmotic gradients in bacteria.

Neurons communicate via a traveling wave of electrical excitation that propagates down an axon at speeds in the range of 10–100 m/s. This electrical wave is triggered and regulated by opening and closing of voltage-gated ion channels. These channels have been traditionally believed to be sensitive to the local electrochemical environment. A growing number of experiments now conclusively show that lipid-associated mechanical stimuli can control the channel response. We develop a quantitative model to elucidate the mechanosensitivity exhibited by these channels. With the help of a single model, we are able able to consolidate the fi ndings of the various experimental studies that have investigated the effect of different mechanical stimuli.

Mechanoelectrical transduction in the inner ear is a biophysical process underlying the senses of hearing and balance. The key players involved in this process are mechanosensitive ion channels. They are located in the stereocilia of hair cells and opened by the tension in specialized molecular springs, the tip links, connecting adjacent stereocilia. When channels open, the tip links relax, reducing the hair-bundle stiffness. This gating compliance makes hair cells especially sensitive to small stimuli. The classical explanation for the gating compliance is that the conformational rearrangement of a single channel directly shortens the tip link. However, to reconcile theoretical models based on this mechanism with experimental data, an unrealistically large structural change of the channel is required. Experimental evidence indicates that each tip link is a dimeric molecule, associated on average with two channels at its lower end. It also indicates that the lipid bilayer modulates ...

Mechanoelectrical transduction in the inner ear is a biophysical process underlying the senses of hearing and balance. The key players involved in this process are mechanosensitive ion channels. They are located in the stereocilia of hair cells and opened by the tension in specialized molecular springs, the tip links, connecting adjacent stereocilia. When channels open, the tip links relax, reducing the hair-bundle stiffness. This gating compliance makes hair cells especially sensitive to small stimuli. The classical explanation for the gating compliance is that the conformational rearrangement of a single channel directly shortens the tip link. However, to reconcile theoretical models based on this mechanism with experimental data, an unrealistically large structural change of the channel is required. Experimental evidence indicates that each tip link is a dimeric molecule, associated on average with two channels at its lower end. It also indicates that the lipid bilayer modulates channel gating, although it is not clear how. Here, we design and analyze a model of mechan-otransduction where each tip link attaches to two channels, mobile within the membrane. Their states and positions are coupled by membrane-mediated elastic forces arising from the interaction between the channels' hydrophobic cores and that of the lipid bilayer. This coupling induces cooperative opening and closing of the channels. The model reproduces the main properties of hair-cell mechan-otransduction using only realistic parameters constrained by experimental evidence. This work provides an insight into the fundamental role that membrane-mediated ion-channel cooperativity can play in sensory physiology. auditory system | cooperativity | hair cell | lipid bilayer | mechanotrans-duction channels