Dual-color fluorescence-burst analysis to study pore formation and protein-protein interactions

Dual-color fluorescence-burst analysis (DCBFA) enables to study leakage of fluorescently labeled (macro) molecules from liposomes that are labeled with a second, spectrally non-overlapping fluorophore. The fluorescent bursts that reside from the liposomes diffusing through the focal volume of a confocal microscope will coincide with those from the encapsulated size-marker molecules. The internal concentration of size-marker molecules can be quantitatively calculated from the fluorescence bursts at a single liposome level. DCFBA has been successfully used to study the effective pore-size of the mechanosensitive channel of large-conductance MscL and the pore-forming mechanism of the antimicrobial peptide melittin from bee venom. In addition, DCFBA can be used to quantitatively measure the binding of proteins to liposomes and to membrane proteins. In this paper, we provide an overview of the method and discuss the experimental details of DCFBA.     

Gating of the mechanosensitive channel protein MscL: the interplay of membrane and protein

The mechanosensitive channel of large conductance (MscL) belongs to a family of transmembrane channel proteins in bacteria and functions as a safety valve that relieves the turgor pressure produced by osmotic downshock. MscL gating can be triggered solely by stretching of the membrane. This work reports an effort to understand this mechanotransduction by means of molecular dynamics (MD) simulation on the MscL of mycobacterium tuberculosis embedded in a palmitoyloleoylphosphatidylethanolamine membrane. Equilibrium MD under zero membrane tension produced a more compact protein structure, as measured by its radii of gyration, compared to the crystal structure, in agreement with previous experimental findings. Even under a large applied tension up to 1000 dyn/cm, the MscL lateral dimension largely remained unchanged after up to 20 ns of simulation. A nonequilibrium MD simulation of 3% membrane expansion showed a significant increase in membrane rigidity upon MscL inclusion, which can contribute to efficient mechanotransduction. Direct observation of channel opening was possible only when an explicit lateral bias force was applied to each of the five subunits of MscL in the radially outward direction. Using this force, open structures with a large pore of radius 10 Å could be obtained. The channel opening takes place in a stepwise manner and concurrently with the water chain formation across the channel, which occurs without direct involvement of protein hydrophilic residues. The N-terminal S1 helices stabilize the open structure, and the membrane asymmetry (different lipid density on the two leaflets of membrane) promotes channel opening.     

Chemically charging the pore constriction opens the mechanosensitive channel MscL

MscL is a bacterial mechanosensitive channel that protects the cell from osmotic downshock. We have previously shown that substitution of a residue that resides within the channel pore constriction, MscL's Gly-22, with all other 19 amino acids affects channel gating according to the hydrophobicity of the substitution (). Here, we first make a mild substitution, G22C, and then attach methanethiosulfonate (MTS) reagents to the cysteine under patch clamp. Binding MTS reagents that are positively charged ([2-(trimethylammonium)ethyl] methanethiosulfonate and 2-aminoethyl methanethiosulfonate) or negatively charged (sodium (2-sulfonatoethyl)methanethiosulfonate) causes MscL to gate spontaneously, even when no tension is applied. In contrast, the polar 2-hydroxyethyl methanethiosulfonate halves the threshold, and the hydrophobic methyl methanethiolsulfonate increases the threshold. These observations indicate that residue 22 is in a hydrophobic environment before gating and in a hydrophilic environment during opening to a substate, a finding consistent with our previous study. In addition, we have found that cysteine 22 is accessible to reagents from the cytoplasmic side only when the channel is opened whereas it is accessible from the periplasmic side even in the closed state. These results support the view that exposure of hydrophobic surfaces to a hydrophilic environment during channel opening serves as the barrier to gating.     

Lactococcus lactis uses MscL as its principal mechanosensitive channel

The functions of the mechanosensitive channels from Lactococcus lactis were determined by biochemical, physiological, and electrophysiological methods. Patch-clamp studies showed that the genes yncB and mscL encode MscS and MscL-like channels, respectively, when expressed in Escherichia coli or if the gene products were purified and reconstituted in proteoliposomes. However, unless yncB was expressed in trans, wild type membranes of L. lactis displayed only MscL activity. Membranes prepared from an mscL disruption mutant did not show any mechanosensitive channel activity, irrespective of whether the cells had been grown on low or high osmolarity medium. In osmotic downshift assays, wild type cells survived and retained 20% of the glycine betaine internalized under external high salt conditions. On the other hand, the mscL disruption mutant retained 40% of internalized glycine betaine and was significantly compromised in its survival upon osmotic downshifts. The data strongly suggest that L. lactis uses MscL as the main mechanosensitive solute release system to protect the cells under conditions of osmotic downshift.     

Disulfide trapping the mechanosensitive channel MscL into a gating-transition state

The mechanosensitive channel of large conductance, MscL, serves as a biological emergency release valve protecting bacteria from acute osmotic downshock, and is to date the best characterized mechanosensitive channel. The N-terminal region of the protein has been shown to be critical for function by random, site-directed, and deletion mutagenesis, yet is structurally poorly understood. One model proposes that the extreme N-termini form a cluster of amphipathic helices that serves as a cytoplasmic second gate, separated from the pore-forming transmembrane domain by a "linker". Here, we have utilized cysteine trapping of single-cysteine mutated channels to determine the proximity, within the homopentameric complex, of residues within and just peripheral to this proposed linker. Our results indicate that all residues in this region can form disulfide bridges, and that the percentage of dimers increases when the channel is gated in vivo. Functional studies suggest that oxidation traps one of these mutated channels, N15C, into a gating-transition state that retains the capacity to obtain both fully open and closed states. The data are not easily explained by current models for the smooth transition from closed-to-open states, but predict that an asymmetric movement of one or more of the subunits commonly occurs upon gating.     

Loss-of-function mutations at the rim of the funnel of mechanosensitive channel MscL

MscL is a bacterial mechanosensitive channel that is activated directly by membrane stretch. Although the gene has been cloned and the crystal structure of the closed channel has been defined, how membrane tension causes conformational changes in MscL remains largely unknown. To identify the site where MscL senses membrane tension, we examined the function of the mutants generated by random and scanning mutagenesis. In vitro (patch-clamp) and in vivo (hypoosmotic-shock) experiments showed that when a hydrophilic amino acid replaces one of the hydrophobic residues that are thought to make contact with the membrane lipid near the periplasmic end of the M1 or M2 transmembrane domain, MscL loses the ability to open in response to membrane tension. Hydrophilic (asparagine) substitution of the other residues in the lipid-protein interface did not impair the channel's mechanosensitivity. These observations suggest that the disturbance of the hydrophobic interaction between the membrane lipid and the periplasmic rim of the channel's funnel impairs the function of MscL.     

Anionic phospholipids affect the rate and extent of flux through the mechanosensitive channel of large conductance MscL

The mechanosensitive channel of large conductance MscL from Escherichia coli has been reconstituted into sealed vesicles, and the effects of lipid structure on the flux of the fluorescent molecule calcein through the open channel have been studied. The channel was opened by reaction of the G22C mutant of MscL with the reagent [2-(triethylammonium)ethyl]methanethiosulfonate (MTSET) which introduces five positive charges within the pore constriction. Flux through the channel was small when the lipid was phosphatidylcholine, but addition of the anionic lipids phosphatidylglycerol, phosphatidic acid, or cardiolipin up to 50 mol % resulted in increases in the amplitudes and rates of release of calcein. Similar effects were seen when either wild-type MscL or the G22C mutant was opened by osmotic pressure difference; rates of release of calcein were very slow in the absence of anionic lipid but increased with increasing concentrations of phosphatidylglycerol to 50 mol %. The observed partial release of trapped calcein following activation of MscL was attributed to the formation of a long-lived subconductance state of MscL following channel opening. Effects of anionic lipid were attributed to an increase in the rate of the transition from closed to fully open state and to a decrease in the rate of the transition from the fully open state to the subconductance state. Higher concentrations of anionic lipid led to a decrease in the rate and amplitude of release of calcein, possibly due to a decreased rate of flux through the open channel. In mixtures with anionic lipids, phosphatidylethanolamine resulted in lower rates and amplitude of release than phosphatidylcholine.     

The mechanosensitive channel protein MscL is targeted by the SRP to the novel YidC membrane insertion pathway of Escherichia coli

The mechanosensitive channel MscL in the inner membrane of Escherichia coli is a homopentameric complex involved in homeostasis when cells are exposed to hypo-osmotic conditions. The E. coli MscL protein is synthesized as a polypeptide of 136 amino acid residues and uses the bacterial signal recognition particle (SRP) for membrane targeting. The protein is inserted into the membrane independently of the Sec translocon. Mutants affected in the Sec-components are competent for MscL assembly. Translocation of the periplasmic domain was detected using a membrane-impermeant, sulfhydryl-specific gel-shift reagent. The modification of a single cysteine residue at position 68 indicated its translocation across the inner membrane. From these in vivo experiments, it is concluded that the electrical chemical membrane potential is not necessary for membrane insertion of MscL. However, depletion of the membrane insertase YidC inhibits translocation of the protein across the membrane. We show here that YidC is essential for efficient membrane insertion of the MscL protein. YidC is a component of a recently identified membrane insertion pathway that is evolutionarily conserved in bacteria, mitochondria and chloroplasts.     

Intragenic suppression of gain-of-function mutations in the Escherichia coli mechanosensitive channel, MscL

Mechanosensitive channels play an important role in protecting bacterial cells from osmotic downshock by serving as biological 'pressure release valves'. One of these channels, MscL, is found throughout the bacterial kingdom, but has been most studied in Escherichia coli. The E. coli MscL is a 136-amino-acid protein organized as a homopentamer with each subunit containing two transmembrane segments. Previous studies have shown that several residues, including V23 and G26, are essential for normal function of MscL; very severe gain-of-function phenotypes in which cell growth slows or is arrested can result from residue substitutions at these positions. Through random mutagenesis and growth selection, we have generated intragenic suppressors of the V23A and G26S mutations. The suppressor mutants have been characterized by growth phenotype, Western blot and patch clamp. Most of the mutations that render phenotypic suppression are located in the transmembrane domains with additional sites lying in the periplasmic loop. In contrast, only one mutation is found in the amino-terminal S1 domain, and none is found within the carboxyl-terminal domain. Not only have these findings revealed functional domains and subdomains critical for MscL function, but they also predict a pair of residues that interact directly during channel opening.     

On the conformation of the COOH-terminal domain of the large mechanosensitive channel MscL

COOH-terminal (S3) domains are conserved within the MscL family of bacterial mechanosensitive channels, but their function remains unclear. The X-ray structure of MscL from Mycobacterium tuberculosis (TbMscL) revealed cytoplasmic domains forming a pentameric bundle (Chang, G., R.H. Spencer, A.T. Lee, M.T. Barclay, and D.C. Rees. 1998. SCIENCE: 282:2220-2226). The helices, however, have an unusual orientation in which hydrophobic sidechains face outside while charged residues face inside, possibly due to specific crystallization conditions. Based on the structure of pentameric cartilage protein, we modeled the COOH-terminal region of E. coli MscL to better satisfy the hydrophobicity criteria, with sidechains of conserved aliphatic residues all inside the bundle. Molecular dynamic simulations predicted higher stability for this conformation compared with one modeled after the crystal structure of TbMscL, and suggested distances for disulfide trapping experiments. The single cysteine mutants L121C and I125C formed dimers under ambient conditions and more so in the presence of an oxidant. The double-cysteine mutants, L121C/L122C and L128C/L129C, often cross-link into tetrameric and pentameric structures, consistent with the new model. Patch-clamp examination of these double mutants under moderately oxidizing or reducing conditions indicated that the bundle cross-linking neither prevents the channel from opening nor changes thermodynamic parameters of gating. Destabilization of the bundle by replacing conservative leucines with small polar residues, or complete removal of COOH-terminal domain (Delta110-136 mutation), increased the occupancy of subconducting states but did not change gating parameters substantially. The Delta110-136 truncation mutant was functional in in vivo osmotic shock assays; however, the amount of ATP released into the shock medium was considerably larger than in controls. The data strongly suggest that in contrast to previous gating models (Sukharev, S., M. Betanzos, C.S. Chiang, and H.R. Guy. 2001a. NATURE: 409:720-724.), S3 domains are stably associated in both closed and open conformations. The bundle-like assembly of cytoplasmic helices provides stability to the open conformation, and may function as a size-exclusion filter at the cytoplasmic entrance to the MscL pore, preventing loss of essential metabolites.     

Identification of the hydrophobic thickness of a membrane protein using fluorescence spectroscopy: studies with the mechanosensitive channel MscL

The hydrophobic thickness of a membrane protein is an important parameter, defining how the protein sits within the hydrocarbon core of the lipid bilayer that surrounds it in a membrane. Here we show that Trp scanning mutagenesis combined with fluorescence spectroscopy can be used to define the hydrophobic thickness of a membrane protein. The mechanosensitive channel of large conductance (MscL) contains two transmembrane alpha-helices, of which the second (TM2) is lipid-exposed. The region of TM2 that spans the hydrocarbon core of the bilayer when MscL is reconstituted into bilayers of dioleoylphosphatidylcholine runs from Leu-69 to Leu-92, giving a hydrophobic thickness of ca. 25 A. The results obtained using Trp scanning mutagenesis were confirmed using Cys residues labeled with the N-methyl-amino-7-nitroben-2-oxa-1,3-diazole [NBD] group; both fluorescence emission maxima and fluorescence lifetimes for the NBD group are sensitive to solvent dielectric constant over the range (2-40) thought to span the lipid headgroup region of a lipid bilayer. Changing phospholipid fatty acyl chain lengths from C14 and C24 results in no significant change for the fluorescence of the interfacial residues, suggesting very efficient hydrophobic matching between the protein and the surrounding lipid bilayer.     

Contributions of the different extramembranous domains of the mechanosensitive ion channel MscL to its response to membrane tension

MscL is a mechanosensitive channel that is gated by tension in the membrane bilayer alone. It is a homo-oligomer of a protein comprising two transmembrane segments connected by an external loop, with the NH(2) and COOH termini located in the cytoplasm. The contributions of the extramembranous domains of the channel to its activity were investigated by specific proteolysis during patch-clamp experiments. Limited proteolysis of the COOH terminus or the NH(2) terminus increased the mechanosensitivity of the channel without changing its conductance. Strikingly, after cleavage of the external loop of each monomer, the channel was still functional, and its mechanosensitivity was increased dramatically, indicating that the loop acts as a spring that resists the opening of the channel and promotes its closure when it is open. These results indicate that the integrity of most of the extramembranous domains is not essential for mechanosensitivity. They suggest that these domains counteract the movement of the transmembrane helices to which they are connected, thus setting the level of sensitivity of the channel to tension.     

Lipid-protein interactions studied by introduction of a tryptophan residue: the mechanosensitive channel MscL

Trp fluorescence spectroscopy is a powerful tool to study the structures of membrane proteins and their interactions with the surrounding lipid bilayer. Many membrane proteins contain more than one Trp residue, making analysis of the fluorescence data more complex. The mechanosensitive channels MscL's of Mycobacterium tuberculosis (TbMscL) and Escherichia coli (EcMscL) contain no Trp residues. We have therefore introduced single Trp residues into the transmembrane regions of TbMscL and EcMscL to give the Trp-containing mutants F80W-TbMscL and F93W-EcMscL, respectively, which we show are highly suitable for measurements of lipid binding constants. In vivo cell viability assays in E. coli show that introduction of the Trp residues does not block function of the channels. The Trp-containing mutants have been reconstituted into lipid bilayers by mixing in cholate followed by dilution to re-form membranes. Cross-linking experiments suggest that the proteins retain their pentameric structures in phosphatidylcholines with chain lengths between C14 and C24, phosphatidylserines, and phosphatidic acid. Quenching of Trp fluorescence by brominated phospholipids suggests that the Trp residue in F80W-TbMscL is more exposed to the lipid bilayer than the Trp residue in F93W-EcMscL. Binding constants for phosphatidylcholines change with changing fatty acyl chain length, the strongest interaction for both TbMscL and EcMscL being observed with a chain of length C16, corresponding to a bilayer of hydrophobic thickness ca. 24 A, compared to a hydrophobic thickness for TbMscL of about 26 A estimated from the crystal structure. Lipid binding constants change by only a factor of 1.5 in the chain length range from C12 to C24, much less than expected from theories of hydrophobic mismatch in which the protein is treated as a rigid body. It is concluded that MscL distorts to match changes in bilayer thickness. The binding constants for dioleoylphosphatidylethanolamine for both TbMscL and EcMscL relative to those for dioleoylphosphatidylcholine are close to 1. Quenching experiments suggest a single class of binding sites for phosphatidylserine, phosphatidylglycerol, and cardiolipin on TbMscL; binding constants are greater than those for phosphatidylcholine and decrease with increasing ionic strength, suggesting that charge interactions are important in binding these anionic phospholipids. Quenching experiments suggest two classes of lipid binding sites on TbMscL for phosphatidic acid, binding of phosphatidic acid being much less dependent on ionic strength than binding of phosphatidylserine.     

The gating mechanism of the bacterial mechanosensitive channel MscL revealed by molecular dynamics simulations

One of the ultimate goals of the study on mechanosensitive (MS) channels is to understand the biophysical mechanisms of how the MS channel protein senses forces and how the sensed force induces channel gating. The bacterial MS channel MscL is an ideal subject to reach this goal owing to its resolved 3D protein structure in the closed state on the atomic scale and large amounts of electrophysiological data on its gating kinetics. However, the structural basis of the dynamic process from the closed to open states in MscL is not fully understood. In this study, we performed molecular dynamics (MD) simulations on the initial process of MscL opening in response to a tension increase in the lipid bilayer. To identify the tension-sensing site(s) in the channel protein, we calculated interaction energy between membrane lipids and candidate amino acids (AAs) facing the lipids. We found that Phe78 has a conspicuous interaction with the lipids, suggesting that Phe78 is the primary tension sensor of MscL. Increased membrane tension by membrane stretch dragged radially the inner (TM1) and outer (TM2) helices of MscL at Phe78, and the force was transmitted to the pentagon-shaped gate that is formed by the crossing of the neighboring TM1 helices in the inner leaflet of the bilayer. The radial dragging force induced radial sliding of the crossing portions, leading to a gate expansion. Calculated energy for this expansion is comparable to an experimentally estimated energy difference between the closed and the first subconductance state, suggesting that our model simulates the initial step toward the full opening of MscL. The model also successfully mimicked the behaviors of a gain of function mutant (G22N) and a loss of function mutant (F78N), strongly supporting that our MD model did simulate some essential biophysical aspects of the mechano-gating in MscL.     

Importance of direct interactions with lipids for the function of the mechanosensitive channel MscL

We have studied the effects of lipid structure on the function of the mechanosensitive channel of large conductance (MscL) from Escherichia coli to determine whether effects follow from direct interaction between the lipids and protein or whether they follow indirectly from changes in the curvature stress in the membrane. The G22C mutant of MscL was reconstituted into sealed vesicles containing the fluorescent molecule calcein, and the release of calcein from the vesicles was measured following opening of the channel by reaction with [2-(triethylammonium)ethyl] methanethiosulfonate (MTSET), which introduces five positive charges into the region of the pore constriction. The presence of anionic lipids in the vesicle membrane changed the rates and amplitudes of calcein release, the effects not correlating with calculated changes in lipid spontaneous curvature. Mutation of charged residues in the Arg-104, Lys-105, Lys-106 cluster removed high-affinity binding of anionic lipids to MscL, and the presence of anionic lipid no longer affected calcein flux through MscL. Changing the zwitterionic lipid from phosphatidylcholine to phosphatidylethanolamine resulted in a large decrease in the rate of calcein release, the change in rate varying linearly with lipid composition, as expected if spontaneous curvature affected the rate of release. However, rates of release of calcein measured in the presence of phosphatidylethanolamine- N-methyl and phosphatidylethanolamine- N, N-dimethyl did not fit the correlation between rate and curvature established for the phosphatidylcholine/phosphatidylethanolamine mixtures. Rather, the effects of zwitterionic lipid headgroup on calcein flux suggested that what was important was the presence of a proton in the headgroup, able to take part in hydrogen bonding to MscL. We conclude that the function of MscL is likely to be modulated by direct interaction with the surrounding, annular phospholipids that contact the protein in the membrane.     

Functional and structural conservation in the mechanosensitive channel MscL implicates elements crucial for mechanosensation

mscL encodes a channel in Escherichia coli that is opened by membrane stretch force, probably serving as an osmotic gauge. Sequences more or less similar to mscL are found in other bacteria, but the degree of conserved function has been unclear. We subcloned and expressed these putative homologues in E . coli and examined their products under patch clamp. Here, we show that each indeed encodes a conserved mechanosensitive channel activity, consistent with the interpretation that this is an important and primary function of the protein in a wide range of bacteria. Although similar, channels of different bacteria differ in kinetics and their degree of mechanosensitivity. Comparison of the primary sequence of these proteins reveals two highly conserved regions, corresponding to domains previously shown to be important for the function of the wild-type E . coli channel, and a C-terminal region that is not conserved in all species. This structural conservation is providing insight into regions of this molecule that are vital to its role as a mechanosensitive channel and may have broader implications for the understanding of other mechanosensitive systems.     

Cysteine scanning of MscL transmembrane domains reveals residues critical for mechanosensitive channel gating

The mechanosensitive channel of large conductance (MscL), a bacterial channel, is perhaps the best characterized mechanosensitive protein. A structure of the Mycobacterium tuberculosis ortholog has been solved by x-ray crystallography, but details of how the channel gates remain obscure. Here, cysteine scanning was used to identify residues within the transmembrane domains of Escherichia coli MscL that are crucial for normal function. Utilizing genetic screens, we identified several mutations that induced gain-of-function or loss-of-function phenotypes in vivo. Mutants that exhibited the most severe phenotypes were further characterized using electrophysiological techniques and chemical modifications of the substituted cysteines. Our results verify the importance of residues in the putative primary gate in the first transmembrane domain, corroborate other residues previously noted as critical for normal function, and identify new ones. In addition, evaluation of disulfide bridging in native membranes suggests alterations of existing structural models for the “fully closed” state of the channel.     

Energetic and spatial parameters for gating of the bacterial large conductance mechanosensitive channel, MscL

MscL is multimeric protein that forms a large conductance mechanosensitive channel in the inner membrane of Escherichia coli. Since MscL is gated by tension transmitted through the lipid bilayer, we have been able to measure its gating parameters as a function of absolute tension. Using purified MscL reconstituted in liposomes, we recorded single channel currents and varied the pressure gradient (P) to vary the tension (T). The tension was calculated from P and the radius of curvature was obtained using video microscopy of the patch. The probability of being open (Po) has a steep sigmoidal dependence on T, with a midpoint (T1/2) of 11.8 dyn/cm. The maximal slope sensitivity of Po/Pc was 0.63 dyn/cm per e-fold. Assuming a Boltzmann distribution, the energy difference between the closed and fully open states in the unstressed membrane was DeltaE = 18.6 kBT. If the mechanosensitivity arises from tension acting on a change of in-plane area (DeltaA), the free energy, TDeltaA, would correspond to DeltaA = 6.5 nm2. MscL is not a binary channel, but has four conducting states and a closed state. Most transition rates are independent of tension, but the rate-limiting step to opening is the transition between the closed state and the lowest conductance substate. This transition thus involves the greatest DeltaA. When summed over all transitions, the in-plane area change from closed to fully open was 6 nm2, agreeing with the value obtained in the two-state analysis. Assuming a cylindrical channel, the dimensions of the (fully open) pore were comparable to DeltaA. Thus, the tension dependence of channel gating is primarily one of increasing the external channel area to accommodate the pore of the smallest conducting state. The higher conducting states appear to involve conformational changes internal to the channel that don't involve changes in area.     

The gating mechanism of the bacterial mechanosensitive channel MscL revealed by molecular dynamics simulations: From tension sensing to channel opening

One of the ultimate goals of the study on mechanosensitive (MS) channels is to understand the biophysical mechanisms of how the MS channel protein senses forces and how the sensed force induces channel gating. The bacterial MS channel MscL is an ideal subject to reach this goal owing to its resolved 3D protein structure in the closed state on the atomic scale and large amounts of electrophysiological data on its gating kinetics. However, the structural basis of the dynamic process from the closed to open states in MscL is not fully understood. In this study, we performed molecular dynamics (MD) simulations on the initial process of MscL opening in response to a tension increase in the lipid bilayer. To identify the tension-sensing site(s) in the channel protein, we calculated interaction energy between membrane lipids and candidate amino acids (AAs) facing the lipids. We found that Phe78 has a conspicuous interaction with the lipids, suggesting that Phe78 is the primary tension sensor of MscL. Increased membrane tension by membrane stretch dragged radially the inner (TM1) and outer (TM2) helices of MscL at Phe78, and the force was transmitted to the pentagon-shaped gate that is formed by the crossing of the neighboring TM1 helices in the inner leaflet of the bilayer. The radial dragging force induced radial sliding of the crossing portions, leading to a gate expansion. Calculated energy for this expansion is comparable to an experimentally estimated energy difference between the closed and the first subconductance state, suggesting that our model simulates the initial step toward the full opening of MscL. The model also successfully mimicked the behaviors of a gain of function mutant (G22N) and a loss of function mutant (F78N), strongly supporting that our MD model did simulate some essential biophysical aspects of the mechano-gating in MscL.     

Defining the physical gate of a mechanosensitive channel, MscL, by engineering metal-binding sites

The mechanosensitive channel of large conductance, MscL, of Escherichia coli is one of the best-studied mechanosensitive proteins. Although the structure of the closed or "nearly-closed" state of the Mycobacterium tuberculosis ortholog has been solved and mechanisms of gating have been proposed, the transition from the closed to the open states remains controversial. Here, we probe the relative position of specific residues predicted to line the pore of MscL in either the closed state or during the closed-to-open transition by engineering single-site histidine substitutions and assessing the ability of Ni2+, Cd2+ or Zn2+ ions to affect channel activity. All residues predicted to be within the pore led to a change in channel threshold pressure, although the direction and extent of this change were dependent upon the mutation and metal used. One of the MscL mutants, L19H, exhibited gating that was inhibited by Cd2+ but stimulated by Ni2+, suggesting that these metals bind to and influence different states of the channel. Together, the results derived from this study support the hypotheses that the crystal structure depicts a "nearly closed" rather than a "fully closed" state of MscL, and that a clockwise rotation of transmembrane domain 1 occurs early in the gating process.