Identification of a 349-kilodalton protein (Gli349) responsible for cytadherence and glass binding during gliding of Mycoplasma mobile

Several mycoplasma species are known to glide in the direction of the membrane protrusion (head-like structure), but the mechanism underlying this movement is entirely unknown. To identify proteins involved in the gliding mechanism, protein fractions of Mycoplasma mobile were analyzed for 10 gliding mutants isolated previously. One large protein (Gli349) was observed to be missing in a mutant m13 deficient in hemadsorption and glass binding. The predicted amino acid sequence indicated a 348,758-Da protein that was truncated at amino acid residue 1257 in the mutant. Immunofluorescence microscopy with a monoclonal antibody showed that Gli349 is localized at the head-like protrusion's base, which we designated the cell neck, and immunoelectron microscopy established that the Gli349 molecules are distributed all around this neck. The number of Gli349 molecules on a cell was estimated by immunoblot analysis to be 450 +/- 200. The antibody inhibited both the hemadsorption and glass binding of M. mobile. When the antibody was used to treat gliding mycoplasmas, the gliding speed and the extent of glass binding were inhibited to similar extents depending on the concentration of the antibody. This suggested that the Gli349 molecule is involved not only in glass binding for gliding but also in movement. To explain the present results, a model for the mechanical cycle of gliding is discussed.     

Temporal sequence of the recovery of traits during phenotypic curing of a Cytophaga johnsonae motility mutant.

The lack of cell translocation and the resulting formation of nonspreading colonies of mutants of the gram-negative gliding bacterium Cytophaga johnsonae have been correlated with the loss of cell surface features of the organism. These cell surface traits include the ability to move polystyrene-latex beads over the cell surface and the ability to be infected by bacteriophages that infect the parent strain. In order to assess whether these traits reflect structures or functions that actually play a role in gliding, we studied a mutant (21A2I) selected for its inability to form spreading colonies; it is deficient in sulfonolipid, lacks bead movement ability, and is resistant to at least one bacteriophage. The provision of cysteate (a specific sulfonolipid precursor) restores lipid content and gliding to the mutant; hence, the lipids are necessary for motility. Growth with cysteate also restores bead movement and phage sensitivity. In order to determine the temporal relationship of these traits, we undertook a kinetic study of the appearance of them after addition of cysteate to the mutant. One predicts that appearance of a trait essential for cell translocation will either precede or accompany the appearance of this ability, while a nonessential trait need not do so. Sulfonolipid synthesis was the only trait that appeared before gliding; this is consistent with its established importance for motility. Bead movement and phage sensitivity first appeared only after gliding started, suggesting that the machinery involved in those processes is not necessary, at least for the initiation of gliding.     

Isolation of a motile mycoplasma from fish

For the first time a mycoplasma has been isolated from fish. The organism, designated strain 163K, was isolated on modified Hayflick medium under aerobic conditions at 25 degrees C from the gills of a tench (Tinca tinca L.). It showed the characteristic features of mycoplasmas. In addition it was flask-shaped with a distinct head-like structure and was able to attach to inert surfaces and living cells. The most interesting property of the organism was its ability to show fast gliding motion. Movement was only in the direction of the head-like structure and was not interrupted by resting periods.     

Spike Structure at the Interface between Gliding Mycoplasma mobile Cells and Glass Surfaces Visualized by Rapid-Freeze-and-Fracture Electron Microscopy

Mycoplasma mobile is a flask-shaped bacteria that binds to a substrate and glides towards its tapered end, the so-called "head-like protrusion," by an unknown mechanism. To search for cellular structures underlying this motility, the cell-substrate interface of actively gliding cells was visualized by rapid-freeze-and-freeze-fracture rotary-shadow electron microscopy. Novel structures, called "spikes," were observed to protrude from the cell membrane and attach to the glass surface at their distal end. The spikes were on average 50 nm in length and 4 nm in diameter, most abundant around the head, and not observed in a nonbinding mutant. The spikes may be involved in the mechanism of binding, gliding, or both.     

Kinesin velocity increases with the number of motors pulling against viscoelastic drag

Although the properties of single kinesin molecular motors are well understood, it is not clear whether multiple motors pulling a single vesicle in a cell cooperate or interfere with one another. To learn how small numbers of motors interact, microtubule gliding assays were carried out with full-length Drosophila kinesin in a novel motility medium containing xanthan, a stiff, water-soluble polysaccharide. At 2 mg/ml xanthan, the zero-shear viscosity of this medium is 1,000 times the viscosity of water, similar to cellular viscosity. To mimic the rheological drag force on the motors when attached to a vesicle in a cell, we attached a 2 μm bead to one end of the microtubule (MT). During gliding assays in our novel medium, the moving bead exerted a drag force of 4–15 pN on the kinesins pulling the MT. The velocity of MTs with an attached bead increased with MT length and with kinesin concentration. The increase with MT length arose because the number of motors is directly proportional to MT length. Our results show that small numbers of kinesins cooperate constructively when pulling against a viscoelastic drag. In the absence of a bead but still in the viscous medium, MT velocity was independent of MT length and kinesin concentration because the thin MT, like a snake moving through grass, was able to move between xanthan molecules with little resistance. A minimal shared-load model in which the number of motors is proportional to MT length fits the observed dependence of gliding velocity on MT length and kinesin concentration.     

Gliding movement in Peranema trichophorum is powered by flagellar surface motility

A colorless euglenoid flagellate Peranema trichophorum shows unique unidirectional gliding cell locomotion on the substratum at velocities up to 30 micro m/s by an as yet unexplained mechanism. In this study, we found that (1) treatment with NiCl(2) inhibited flagellar beating without any effect on gliding movement; (2) water currents applied to a gliding cell from opposite sides caused detachment of the cell body from the substratum. With only the anterior flagellum adhering to the substratum, gliding movement continued along the direction of the anterior flagellum; (3) gentle pipetting induced flagellar severance into various lengths. In these cells, gliding velocity was proportional to the flagellar length; and (4) Polystyrene beads were translocated along the surface of the anterior flagellum. All of these results indicate that a cell surface motility system is present on the anterior flagellum, which is responsible for cell gliding in P. trichophorum.     

Gliding motility of Cytophaga sp. strain U67.

Video techniques were used to analyze the motion of the gliding bacterium Cytophaga sp. strain U67. Cells moved singly on glass along the long axis at a speed of about 2 micrometers/s, advancing, retreating, stopping, pivoting about a pole, or flipping over. They did not flex or roll. Cells of different lengths moved at about the same speed. Cells sometimes spun continuously about a pole at a frequency of about 2 HZ, the body moving in a plane parallel to that of the glass or on the surface of a cone having either a large or a small solid angle. Polystyrene latex spheres moved to and fro on the surfaces of cells, also at a speed of about 2 micrometers/s. They moved in the same fashion whether a cell was in suspension, gliding, or at rest on the glass. Two spheres on the same cell often moved in opposite directions, passing by one another in close proximity. Small and large spheres and aggregates of spheres all moved at about the same speed. An aggregate moved down the side of a cell with a fixed orientation, even when only one sphere was in contact with the cell. Spheres occasionally left one cell and were picked up by another. Cell pretreated with small spheres did not adhere to glass. When the cells were deprived of oxygen, they stopped gliding, and the spheres stopped moving on their surfaces. The spheres became completely immobilized; they no longer moved from cell to cell or exhibited Brownian movement. Cytophaga spp. are known to have a typical gram-negative cell envelope: an inner (cytoplasmic) membrane, a thin peptidoglycan layer, and an outer (lipopolysaccharide) membrane. Our data are consistent with a model for gliding in which sites to which glass and polystyrene strongly adsorb move within the fluid outer membrane along tracks fixed to the rigid peptidoglycan framework.     

Gliding movements in Myxococcus xanthus.

Prokaryotic gliding motility is described as the movement of a cell on a solid surface in the direction of the cell's long axis, but its mechanics are unknown. To investigate the basis of gliding, movements of individual Myxococcus xanthus cells were monitored by employing a video microscopy method by which displacements as small as 0.03 micron could be detected and speeds as low as 1 micron/min could be resolved. Single cells were observed to glide with speeds varying between 1 and 20 microns/min. We found that speed variation was due to differences in distance between the moving cell and the nearest cell. Cells separated by less than one cell diameter (0.5 micron) moved with an average speed of 5.0 micron/min, whereas cells separated by more than 0.5 micron glided with an average speed of 3.8 microns/min. The power to glide was found to be carried separately at both ends of a cell.     

Force and velocity of mycoplasma mobile gliding

The effects of temperature and force on the gliding speed of Mycoplasma mobile were examined. Gliding speed increased linearly as a function of temperature from 0.46 microm/s at 11.5 degrees C to 4.0 microm/s at 36.5 degrees C. A polystyrene bead was attached to the tail of M. mobile using a polyclonal antibody raised against whole M. mobile cells. Cells attached to beads glided at the same speed as cells without beads. When liquid flow was applied in a flow chamber, cells reoriented and moved upstream with reduced speeds. Forces generated by cells at various gliding speeds were calculated by multiplying their estimated frictional drag coefficients with their velocities relative to the liquid. The gliding speed decreased linearly with force. At zero speed, the force measurements extrapolated to 26 pN at 22.5 and 27.5 degrees C. At zero force, the speed extrapolated to 2.3 and 3.3 microm/s at 22.5 and 27.5 degrees C, respectively--the same speeds as those observed for free gliding cells. Cells attached to beads were also trapped by an optical tweezer, and the stall force was measured to be 26 to 28 pN (17.5 to 27.5 degrees C). The gliding speed depended on temperature, but the maximum force did not, suggesting that the mechanism is composed of at least two steps, one that generates force and another that allows displacement. Other implications of these results are discussed.     

SprB is a cell surface component of the Flavobacterium johnsoniae gliding motility machinery

Cells of the gliding bacterium Flavobacterium johnsoniae move rapidly over surfaces by an unknown mechanism. Transposon insertions in sprB resulted in cells that were defective in gliding. SprB is a highly repetitive 669-kDa cell surface protein, and antibodies against SprB inhibited the motility of wild-type cells. Polystyrene microspheres coated with antibodies against SprB attached to and were rapidly propelled along the cell surface, suggesting that SprB is one of the outermost components of the motility machinery. The movement of SprB along the cell surface supports a model of gliding motility in which motors anchored to the cell wall rapidly propel cell surface adhesins.     

Cell surface interaction of the protozoan Gregarina with concanavalin A beads - implications for models of gregarine gliding

Con A Sepharose beads can be translocated over the surface of the protozoan Gregarina and in (forward) moving gregarines, the bead may be moved backwards relative to the substrate. The speed of bead movement is not constant over the surface of the cell, but has a maximum value in the central region of the deutomerite. The mass of the individual beads used in this study was about the same order of magnitude as the mass of a gregarine, i.e. considerable force must be generated at the gregarine cell surface. The implications of these experiments to models of gregarine locomotion are considered. The close similarities between this system and flagellar surface motility of Clamydomonas studied by particle movement and gliding motility are discussed.     

Cytoskeletal protein P41 is required to anchor the terminal organelle of the wall-less prokaryote Mycoplasma pneumoniae

The cell wall-less prokaryote Mycoplasma pneumoniae approaches the minimal requirements for a cell yet produces a complex terminal organelle that mediates cytadherence and gliding motility. Here we explored the molecular nature of the M. pneumoniae gliding machinery, utilizing fluorescent protein fusions and digital microcinematography to characterize gliding-altered mutants having transposon insertions in MPN311, encoding the cytoskeletal protein P41. Disruption of MPN311 resulted in loss of P41 and P24, the downstream gene product. Gliding ceases in wild-type M. pneumoniae during terminal organelle development, which occurs at the cell poles adjacent to an existing structure. In contrast, terminal organelle development in MPN311 mutants did not necessarily coincide with gliding cessation, and new terminal organelles frequently formed at lateral sites. Furthermore, new terminal organelles exhibited gliding capacity quickly, unlike wild-type M. pneumoniae. P41 and P24 localize at the base of the terminal organelle; in their absence this structure detached from the cell body of motile and dividing cells but retained gliding capacity and thus constitutes the gliding apparatus. Recombinant wild-type P41 restored cell integrity, establishing a role for this protein in anchoring the terminal organelle to the cell body.     

Motility of Plasmodium berghei ookinetes in vitro

Motility of Plasmodium berghei ookinetes, which developed in primary and established cell line cultures obtained from Anopheles stephensi mosquitoes, was studied by using still photomicrographs and normal speed cinephotomicrography. At 18–72 hr after inoculation of P. berghei infected blood from hamsters or mice, motile ookinetes were seen in both mosquito cell cultures; the most active specimens were observed at 24–30 hr. Ookinetes underwent a sporadic forward gliding movement, during which a variable degree of rotation of the body upon its longitudinal axis usually occurred. Some specimens rotated repeatedly upon their axes without any forward progression. The direction of the gliding movement always coincided with the curvature of the ookinete body. In those specimens in which no rotation of the body occurred, a circular course resulted. Ookinetes covered a distance of as much as 50 μm during a single gliding movement. A few ookinetes undergoing locomotion appeared to leave a path or trail on the substrate. Occasionally, an ookinete penetrated a red cell with its slender anterior projection, resulting in lysis of the cell. After red cells had been penetrated by ookinetes, the parasites already within these cells fused with each other to form larger spheroidal bodies. Penetration of cultured cells was not observed.     

Cell polarity, intercellular signalling and morphogenetic cell movements in Myxococcus xanthus

In Myxococcus xanthus morphogenetic cell movements constitute the basis for the formation of spreading vegetative colonies and fruiting bodies in starving cells. M. xanthus cells move by gliding and gliding motility depends on two polarly localized engines, type IV pili pull cells forward, and slime extruding nozzle-like structures appear to push cells forward. The motility behaviour of cells provides evidence that the two engines are localized to opposite poles and that they undergo polarity switching. Several proteins involved in regulating polarity switching have been identified. The cell surface-associated C-signal induces the directed movement of cells into nascent fruiting bodies. Recently, the molecular nature of the C-signal molecule was elucidated and the motility parameters regulated by the C-signal were identified. From the effect of the C-signal on cell behaviour it appears that the C-signal inhibits polarity switching of the two motility engines. This establishes a connection between cell polarity, signalling by an intercellular signal and morphogenetic cell movements during fruiting body formation.     

Purification and characterization of native conventional kinesin, HSET, and CENP-E from mitotic hela cells

We have developed a strategy for the purification of native microtubule motor proteins from mitotic HeLa cells and describe here the purification and characterization of human conventional kinesin and two human kinesin-related proteins, HSET and CENP-E. We found that the 120-kDa HeLa cell conventional kinesin is an active motor that induces microtubule gliding at approximately 30 microm/min at room temperature. This active form of HeLa cell kinesin does not contain light chains, although light chains were detected in other fractions. HSET, a member of the C-terminal kinesin subfamily, was also purified in native form for the first time, and the protein migrates as a single band at approximately 75 kDa. The purified HSET is an active motor that induces microtubule gliding at a rate of approximately 5 microm/min, and microtubules glide for an average of 3 microm before ceasing movement. Finally, we purified native CENP-E, a kinesin-related protein that has been implicated in chromosome congression during mitosis, and we found that this form of CENP-E does not induce microtubule gliding but is able to bind to microtubules.     

Mucilage secretion and the movements of blue-green algae

Summary Recent discoveries of ultrastructures which might be involved in the gliding movements of blue-green algae have been reviewed, and in the light of these discoveries the role of mucilage secretion in movement has been reconsidered. The formation and behaviour of mucilage rings in filaments ofAnabaena cylindrica is described. The behaviour of the mucilage rings indicates that each cell has an autonomous gliding mechanism which is capable of immediate reversal, and that the gliding mechanism is probably located over the whole surface, rather than at the ends, of the cells. It follows that if mucilage secretion is the cause of movement it must take place over the whole surface of the cell: but if the ends of the cell are the sites of mucilage secretion, as seems likely, then gliding movement must be performed by some other process.A rather remarkable clumping phenomenon is described which takes place in dense suspensions ofAnabaena. It results from the gliding movements of randomly orientated filaments made mutually adhesive by the mucilage which surrounds them.     

Time-lapse video microscopy of gliding motility in Toxoplasma gondii reveals a novel, biphasic mechanism of cell locomotion

Toxoplasma gondii is a member of the phylum Apicomplexa, a diverse group of intracellular parasites that share a unique form of gliding motility. Gliding is substrate dependent and occurs without apparent changes in cell shape and in the absence of traditional locomotory organelles. Here, we demonstrate that gliding is characterized by three distinct forms of motility: circular gliding, upright twirling, and helical rotation. Circular gliding commences while the crescent-shaped parasite lies on its right side, from where it moves in a counterclockwise manner at a rate of approximately 1.5 microm/s. Twirling occurs when the parasite rights itself vertically, remaining attached to the substrate by its posterior end and spinning clockwise. Helical gliding is similar to twirling except that it occurs while the parasite is positioned horizontally, resulting in forward movement that follows the path of a corkscrew. The parasite begins lying on its left side (where the convex side is defined as dorsal) and initiates a clockwise revolution along the long axis of the crescent-shaped body. Time-lapse video analyses indicated that helical gliding is a biphasic process. During the first 180(o) of the turn, the parasite moves forward one body length at a rate of approximately 1-3 microm/s. In the second phase, the parasite flips onto its left side, in the process undergoing little net forward motion. All three forms of motility were disrupted by inhibitors of actin filaments (cytochalasin D) and myosin ATPase (butanedione monoxime), indicating that they rely on an actinomyosin motor in the parasite. Gliding motility likely provides the force for active penetration of the host cell and may participate in dissemination within the host and thus is of both fundamental and practical interest.     

Intracellular, periodic structures in the gliding bacterium Myxococcus xanthus.

Electron microscopic observations of thin sections of Myxococcus xanthus vegetative cells revealed the presence of cytoplasmic bundles of 4- to 5-nm-diameter filaments running longtitudinally below the cell membrane and terminating in association with the envelope near one pole. Part of each bundle demonstrated a herringbone-like periodicity (approximately 12-nm spacing). This structure was observed in cells from shake cultures and in gliding cells fixed by several methods. It is proposed that the structure may be attached to the envelope near both poles in gliding cells and that the motive force for motility may be provided by its contraction and relaxation. In one of four nongliding mutants examined, the periodicity was indistinct or lacking. In this mutant another structure, comprised of linearly arrayed beads, was observed in association with the filamentous bundle. Another structure, characterized by major, transverse bands (approximately 34 nm apart), occurred in patches that may traverse the diameter of the wild-type cells in which the structure was observed.     

Photokinesis and Photophobic Responses in the Gliding Flagellate, Euglena mutabilis

A pronounced photokinesis (as indicated by increases in bothpercentage of motile cells and average speed of movement) aswell as step-up and step-down photophobic responses at light/darkboundaries in the gliding flagellate Euglena mutabilis was studiedusing time-lapse video-microscopy. The spectral sensitivitiesof all the observed lightdependent motor responses were similarto each other and showed an activity throughout the whole visiblespectrum with maximum peaks at about 410, 450, 470, 530, 580and 650 nm and a pronounced minimum at about 600 nm. Thus, thephotoreceptor pigments markedly differ from the closely relatedswimming flagellate Euglena gracilis in which a flavin typeblue light receptor is supposed to be responsible for the stimulusperception. Light microscopic studies of mucilage distributionand regeneration suggested that the gliding movements are effectedby parallel gliding of adjacent pellicular strips while themucilage produced on the cell surface and transported to therear end seems to be responsible for adhesion of the cell onthe substrate. (Received November 21, 1985; Accepted January 30, 1986)