Nobunori Kami-ike

Charged residues in the cytoplasmic loop of MotA are required for stator assembly into the bacterial flagellar motor

MotA and MotB form a transmembrane proton channel that acts as the stator of the bacterial flagellar motor to couple proton flow with torque generation. The C‐terminal periplasmic domain of MotB plays a role in anchoring the stators to the motor. However, it remains unclear where their initial binding sites are. Here, we constructed Salmonella strains expressing GFP‐MotB and MotA‐mCherry and investigated their subcellular localization by fluorescence microscopy. Neither the D33N and D33A mutations in MotB, which abolish the proton flow, nor depletion of proton motive force affected the assembly of GFP‐MotB into the motor, indicating that the proton translocation activity is not required for stator assembly. Overexpression of MotA markedly inhibited wild‐type motility, and it was due to the reduction in the number of functional stators. Consistently, MotA‐mCherry was observed to colocalize with GFP‐FliG even in the absence of MotB. These results suggest that MotA alone can be installed into the motor. The R90E and E98K mutations in the cytoplasmic loop of MotA (MotAC), which has been shown to abolish the interaction with FliG, significantly affected stator assembly, suggesting that the electrostatic interaction of MotAC with FliG is required for the efficient assembly of the stators around the rotor.

Roles of the extreme N-terminal region of FliH for efficient localization of the FliH-FliI complex to the bacterial flagellar type III export apparatus

Most bacterial flagellar proteins are exported by the flagellar type III protein export apparatus for their self‐assembly. FliI ATPase forms a complex with its regulator FliH and facilitates initial entry of export substrates to the export gate composed of six integral membrane proteins. The FliH–FliI complex also binds to the C ring of the basal body through a FliH–FliN interaction for efficient export. However, it remains unclear how these reactions proceed within the cell. Here, we analysed subcellular localization of FliI–YFP by fluorescence microscopy. FliI–YFP was localized to the flagellar base, and its localization required both FliH and the C ring. The ATPase activity of FliI was not required for its localization. FliI–YFP formed a complex with FliHΔ1 (missing residues 2–10) but the complex did not show any localization. FliHΔ1 did not interact with FliN, and alanine‐scanning mutagenesis revealed that only Trp‐7 and Trp‐10 of FliH are essential for the interaction with FliN. Overproduction of the FliH–FliI complex improved the export activity of the fliN mutant whereas neither of the FliH(W7A)‐FliI nor FliH(W10A)‐FliI complexes did, suggesting that Trp‐7 and Trp‐10 of FliH are also required for efficient localization of the FliH–FliI complex to the export gate.

Assembly and stoichiometry of FliF and FlhA in Salmonella flagellar basal body

The bacterial flagellar export apparatus is required for the construction of the bacterial flagella beyond the cytoplasmic membrane. The membrane‐embedded part of the export apparatus, which consists of FlhA, FlhB, FliO, FliP, FliQ and FliR, is located in the central pore of the MS ring formed by 26 copies of FliF. The C‐terminal cytoplasmic domain of FlhA is located in the centre of the cavity within the C ring made of FliG, FliM and FliN. FlhA interacts with FliF, but its assembly mechanism remains unclear. Here, we fused yellow fluorescent protein (YFP) and cyan fluorescent protein (CFP) to the C‐termini of FliF and FlhA and investigated their subcellular localization by fluorescence microscopy. The punctate pattern of FliF–YFP localization required FliG but neither FliM, FliN, FlhA, FlhB, FliO, FliP, FliQ nor FliR. In contrast, FlhA–CFP localization required FliF, FliG, FliO, FliP, FliQ and FliR. The number of FlhA–YFP molecules associated with the MS ring was estimated to be about nine. We suggest that FlhA assembles into the export gate along with other membrane components during the MS ring complex formation in a co‐ordinated manner.

Suppressor Analysis of the MotB(D33E) Mutation To Probe Bacterial Flagellar Motor Dynamics Coupled with Proton Translocation

MotA and MotB form the stator of the proton-driven bacterial flagellar motor, which conducts protons and couples proton flow with motor rotation. Asp-33 of Salmonella enterica serovar Typhimurium MotB, which is a putative proton-binding site, is critical for torque generation. However, the mechanism of energy coupling remains unknown. Here, we carried out genetic and motility analysis of a slowly motile motB(D33E) mutant and its pseudorevertants. We first confirmed that the poor motility of the motB(D33E) mutant is due to neither protein instability, mislocalization, nor impaired interaction with MotA. We isolated 17 pseudorevertants and identified the suppressor mutations in the transmembrane helices TM2 and TM3 of MotA and in TM and the periplasmic domain of MotB. The stall torque produced by the motB(D33E) mutant motor was about half of the wild-type level, while those for the pseudorevertants were recovered nearly to the wild-type levels. However, the high-speed rotations of the motors under low-load conditions were still significantly impaired, suggesting that the rate of proton translocation is still severely limited at high speed. These results suggest that the second-site mutations recover a torque generation step involving stator-rotor interactions coupled with protonation/deprotonation of Glu-33 but not maximum proton conductivity.

Evidence for symmetry in the elementary process of bidirectional torque generation by the bacterial flagellar motor

The bacterial flagellar motor can rotate in both counterclockwise (CCW) and clockwise (CW) directions. It has been shown that the sodium ion-driven chimeric flagellar motor rotates with 26 steps per revolution, which corresponds to the number of FliG subunits that form part of the rotor ring, but the size of the backward step is smaller than the forward one. Here we report that the proton-driven flagellar motor of Salmonella also rotates with 26 steps per revolution but symmetrical in both CCW and CW directions with occasional smaller backward steps in both directions. Occasional shift in the stepping positions is also observed, suggesting the frequent exchange of stators in one of the 11–12 possible anchoring positions around the rotor. These observations indicate that the elementary process of torque generation by the cyclic association/dissociation of the stator with every FliG subunit along the circumference of the rotor is symmetric in CCW and CW rotation even though the structure of FliG is highly asymmetric and suggests a 180° rotation of a FliG domain for the rotor-stator interaction to reverse the direction of rotation.

Assembly dynamics and the roles of FliI ATPase of the bacterial flagellar export apparatus

For construction of the bacterial flagellum, FliI ATPase forms the FliH2-FliI complex in the cytoplasm and localizes to the flagellar basal body (FBB) through the interaction of FliH with a C ring protein, FliN. FliI also assembles into a homo-hexamer to promote initial entry of export substrates into the export gate. The interaction of FliH with an export gate protein, FlhA, is required for stable anchoring of the FliI6 ring to the gate. Here we report the stoichiometry and assembly dynamics of FliI-YFP by fluorescence microscopy with single molecule precision. More than six FliI-YFP molecules were associated with the FBB through interactions of FliH with FliN and FlhA. Single FliI-YFP molecule exchanges between the FBB-localized and free-diffusing ones were observed several times per minute. Neither the number of FliI-YFP associated with the FBB nor FliI-YFP turnover rate were affected by catalytic mutations in FliI, indicating that ATP hydrolysis by FliI does not drive the assembly-disassembly cycle of FliI during flagellar assembly. We propose that the FliH2FliI complex and FliI6 ring function as a dynamic substrate carrier and a static substrate loader, respectively.

A kinetic analysis of the electrogenic pump of Chara corallina. I: Inhibition of the pump by DCCD

SummaryThe current-voltage curve of theChara membrane was obtained by applying a slow ramp depo- and hyperpolarization by use of voltage clamp. With the progress of poisoning by DCCD (dicyclohexylcarbodiimide) theI–V curve moved by about 50 mV (depolarization) along the voltage axis, reducing its slope, and finally converged to theid-V curve of the passive diffusion channel. Changes ofip-V curve of the electrogenic pump channel could be obtained by subtracting the latter from the former.The sigmoidalip-V curve could be simulated satisfactorily by adopting a simple reaction kinetic model. Kinetic parameters of the successive changes of state of the H+ ATPase could be evaluated. Changes of these kinetic parameters during inhibition gave useful information about the molecular mechanism of the electrogenic pump.Depolarization of the membrane potential, decrease of membrane conductance, and decrease of pump current during inhibition of the pump with DCCD are caused mainly by the decrease of conductance of the pump channel. The decrease of this pump conductance is caused principally by a marked decrease of the rate constant for releasing H+ to the outside.

Effect of intracellular pH on the torque-speed relationship of bacterial proton-driven flagellar motor.

Bacterial flagella responsible for motility are driven by rotary motors powered by the electrochemical potential difference of specific ions across the cytoplasmic membrane. The stator of proton-driven flagellar motor converts proton influx into mechanical work. However, the energy conversion mechanism remains unclear. Here, we show that the motor is sensitive to intracellular proton concentration for high-speed rotation at low load, which was considerably impaired by lowering intracellular pH, while zero-speed torque was not affected. The change in extracellular pH did not show any effect. These results suggest that a high intracellular proton concentration decreases the rate of proton translocation and therefore that of the mechanochemical reaction cycle of the motor but not the actual torque generation step within the cycle by the stator-rotor interactions.

Load‐sensitive coupling of proton translocation and torque generation in the bacterial flagellar motor

The Salmonella flagellar motor consists of a rotor and about a dozen stator elements. Each stator element, consisting of MotA and MotB, acts as a proton channel to couple proton flow with torque generation. A highly conserved Asp33 residue of MotB is directly involved in the energy coupling mechanism, but it remains unknown how it carries out this function. Here, we show that the MotB(D33E) mutation dramatically alters motor performance in response to changes in external load. Rotation speeds of the MotA/B(D33E) and MotA(V35F)/B(D33E) motors were markedly slower than the wild‐type motor and fluctuated considerably at low load but not at high load, whereas the rotation rate of the wild‐type motor was stable at any load. At low load, pausing events were frequently observed in both mutant motors. The proton conductivities of these mutant stator channels in their ‘unplugged’ forms were only half of the conductivity of the wild‐type channel. These results suggest that the D33E mutation induces a load‐dependent inactivation of the MotA/B complex. We propose that the stator element is a load‐sensitive proton channel that efficiently couples proton translocation with torque generation and that Asp33 of MotB is critical for this co‐ordinated proton translocation.

A kinetic analysis of the electrogenic pump ofChara corallina: III. Pump activity during action potential

SummaryThe current-voltage curve (I–V curve) of theChara membrane was obtained by applying a slow ramp hyper- and depolarization by use of voltage clamp. By inhibiting the electrogenic pump with 50μm DCCD (dicyclohexylcarbodiimide), theI–V curve approached a steadyI–V curve within two hours, which gave theid-V curve of the passive diffusion channel. Theip-V curve of the electrogenic pump channel was obtained by subtracting the latter from the former. The sigmoidalip-V curve could be simulated satisfactorily with a simple reaction kinetic model which assumes a stoichiometric ratio of 2. The emf of the pump (Ep) is given as the voltage at which the pump current changes its sign. The conductance of the pump (gp) can be calculated as the chord conductance from theip-V curve, which is highly voltage dependent having a peak at a definite voltage. The changes of emf and conductance during excitation were determined by use of the current clamp (I=0). Since theEp andgp(V) are known, the changes, during excitation, of emf (Ed) and conductance (gd) of the passive diffusion channel can be calculated. The marked increase of the membrane conductance and the large depolarization during the action potential are caused by the marked increase of the conductance of the passive diffusion channel and the large depolarization of its emf. The conductance of the electrogenic pump decreases to about half at the peak of action potential, while the pump current increases almost to a saturated level.