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« Fine Reading: Classics from the Archives of the Royal Society | Main | Fine Reading: Yet Another Reason to Appreciate Fungi »

January 25, 2010

Measuring the Strength and Speed of the Microbial Grappling Hook

by Amber Pollack-Berti

Ninjagrapplinghook

Source.

I’ll admit, I’ve been in love with the type IV pili (T4P) for a long time. After memorizing all those complex pathways for regulation and metabolism, there was something so refreshing and accessible about pili. These bacterial surface appendages are, by their nature, mechanical structures. They are easy to visualize. Their composition is simple: a Type IV pilus is a flexible filament made up of thousands of repeating pilin subunits. Bacteria employ this one structure for a variety of purposes: T4P play structural roles in motility and biofilm formation, and have also been implicated in DNA binding and uptake, in host cell signaling, and even in communication of electrical signals as ‘nanowires’.

T4P are long and thin and have great tensile strength. They are involved in bacterial motility using a special mechanism: the pili are retracted into the cell when the pilin subunits are removed at the pilus’ cell end by an ATPase, the protein PilT. This results in the ratcheting of the pilus back into the cell. When a pilus is attached by its distal end to a surface of agar, the retraction is so strong that the cell is pulled forward in a kind of movement called twitching motility. When a bacterium attaches via the pilus to the surface of a host cell, it retracts until the two come in contact. In these cases, the pilus acts as a grappling hook, pulling the cell along in short bursts of pili elongation, attachment, and retraction.

Clausen_Fig1

Experimental setup and force generation during T4P
retraction. (a) A cell is immobilized on a polystyrene-
coated cover slide. When a T4P bound to a bead in
the laser trap is retracted, it displaces the bead by
a distance d from the center of the trap. The force
feedback is triggered by moving the slide by a dis-
tance x to maintain d at a constant value. (b) Typical
deflection, d, of the bead during pilus retraction as a
function of time. F, force; t, time.
Source.

The force exerted in pilus retraction as well as its speed have been recently measured. Just how much force can be exerted during the retraction of one pilus? How fast can it retract? If you apply force to the pilus, does it change the speed of retraction? These are physics experiments, albeit at a microscopic scale. The authors used laser tweezers to measure the force and velocity of pilus retraction. The experimental setup consists of immobilizing a cell on a microscope slide and linking a bead to the end of a pilus. The bead can be localized via a laser trap, and the distance it travels recorded as a function of force and time.

Using this approach, they pitted two different microbes—Myxococcus xanthus and Neisseria gonorrhoeae—against one another in the equivalent of a bacterial tractor pull. They compared M. xanthus T4P to previously reported stats for N. gonorrhoeae. Could two distinct bacteria, living very different lifestyles and gazing at each other from far across the phylogenetic tree, pull their pili with similar force? Similar velocity?

Mattick

Model of type IV pili assembly and retraction. Prepilin
leader sequences are cleaved by PilD. Processed PilA is
assembled on a base of minor pilins (PilE, V, W, X, and
FimU) by the action of the cytoplasmic membrane protein
PilC and the NTP-binding protein PilB. The pilus is extrud-
ed through the outer membrane via a pore of PilQ multi-
mers. Pilus retraction is by the action of PilT. Source.

When it comes to stalling force (the force at which retraction drops by an order of magnitude), M. xanthus may be the winner, with a stalling force of ~150 pN. But N. gonorrhoeae is no slouch, with a previously reported force of ~110 pN. Whatever the details, the authors state: to our knowledge, the pilus motor is the strongest linear motor reported in the literature to date. By comparison, the stalling force of an actin filament is 7.7 pN per filament, that of myosin 2.5 pN. But while both N. gonorrhoeae and M. xanthus may retract their pili with the same general amount of force and at similar velocities, there was a striking difference: when force is applied to N. gonorrhoeae there is an increased likelihood of direction switching: the pilus stops retracting and begins to elongate. In contrast, applying force to a M. xanthus pilus does not increase the likelihood of elongation.

Similar values for retraction strength and velocity suggest common machinery at work in two very different bacteria. Does the difference in direction switching reflect the different lifestyles of a soil-dwelling microbe and a human pathogen? T4P systems are employed by a wide variety of bacterial species. Certainly studies that investigate this mechanism in other twitching bacteria will further expand our knowledge of T4P retraction across diverse bacterial lifestyles.

Pollack



Amber is a Graduate Research Assistant in the Ruby Lab at the University of Wisconsin, Madison, and the host of a blog that also features The Small Things: Tiny Topics.

Research Blogging Citation:

Clausen M, Jakovljevic V, Søgaard-Andersen L, & Maier B (2009). High-force generation is a conserved property of type IV pilus systems. Journal of bacteriology, 191 (14), 4633-8 PMID: 19429611

Comments

that was a outstanding article very informative i really enjoyed reading it thanks

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