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-freezefracture 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.Mycoplasma gliding. Mycoplasmas are bacteria that lack a cell wall and are parasitic or commensal to many kinds of hosts, including humans, animals, and plants (25). Several mycoplasma species have a membrane protrusion at one end, called the "head-like protrusion," which creates the organism's characteristic flask-shaped cell morphology. These bacteria are capable of gliding motility, enabling them to translocate smoothly on solid surfaces, always in the direction of the headlike protrusion (3, 13). Although gliding motility of mycoplasmas is believed to be involved in pathogenicity, the mechanism of gliding motility has not been well investigated. Mycoplasmas do not have any homologs of genes that encode pili, flagella, genes related to other bacterial motility, or motor proteins that are common in eukaryotic motility, such as myosins (5,7,9,19). These facts suggest that mycoplasmas glide by an entirely unknown mechanism, but this mechanism has been difficult to isolate because many species of mycoplasma travel at low speed and with interrupted motility.The species Mycoplasma mobile provides an opportunity to study mycoplasma gliding motility, because this species is the fastest gliding and, unlike other species, glides without interruption (13-15, 20, 21, 27). At all stages of growth, M. mobile glides smoothly and continuously on glass at an average speed of 2.0 to 4.5 m/s, or about 3 to 7 times the length of the cell per s (27), exerting a force of up to 27 piconewtons (pN) (20,21). These distinct characteristics enabled detailed analyses of gliding (6,(20)(21)(22)(26)(27)(28) and isolation of gliding mutants that were characterized by reduced or deficient gliding or enhanced speed (23,28).