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Journal of Bacteriology, November 1999, p. 6865-6875, Vol. 181, No. 22
Department of Physics, Dalhousie University,
Halifax, Nova Scotia, Canada B3H 4J11;
Department of Physics, St. Francis Xavier University,
Antigonish, Nova Scotia, Canada B2G 2W52; and
Department of Microbiology, College of Biological Science,
University of Guelph, Guelph, Ontario, Canada N1G 2W13
Received 28 June 1999/Accepted 7 September 1999
Atomic force microscopy was used to measure the thickness of
air-dried, collapsed murein sacculi from Escherichia coli
K-12 and Pseudomonas aeruginosa PAO1. Air-dried sacculi
from E. coli had a thickness of 3.0 nm, whereas those from
P. aeruginosa were 1.5 nm thick. When rehydrated, the
sacculi of both bacteria swelled to double their anhydrous thickness.
Computer simulation of a section of a model single-layer peptidoglycan
network in an aqueous solution with a Debye shielding length of 0.3 nm
gave a mass distribution full width at half height of 2.4 nm, in
essential agreement with these results. When E. coli
sacculi were suspended over a narrow groove that had been etched into a
silicon surface and the tip of the atomic force microscope used to
depress and stretch the peptidoglycan, an elastic modulus of 2.5 × 107 N/m2 was determined for hydrated
sacculi; they were perfectly elastic, springing back to their original
position when the tip was removed. Dried sacculi were more rigid with a
modulus of 3 × 108 to 4 × 108
N/m2 and at times could be broken by the atomic force
microscope tip. Sacculi aligned over the groove with their long axis at
right angles to the channel axis were more deformable than those with their long axis parallel to the groove axis, as would be expected if
the peptidoglycan strands in the sacculus were oriented at right angles
to the long cell axis of this gram-negative rod. Polar caps were not
found to be more rigid structures but collapsed to the same thickness
as the cylindrical portions of the sacculi. The elasticity of intact
E. coli sacculi is such that, if the peptidoglycan strands
are aligned in unison, the interstrand spacing should increase by 12%
with every 1 atm increase in (turgor) pressure. Assuming an unstressed
hydrated interstrand spacing of 1.3 nm (R. E. Burge, A. G. Fowler, and D. A. Reaveley, J. Mol. Biol. 117:927-953, 1977) and
an internal turgor pressure of 3 to 5 atm (or 304 to 507 kPa) (A. L. Koch, Adv. Microbial Physiol. 24:301-366, 1983), the natural
interstrand spacing in cells would be 1.6 to 2.0 nm. Clearly, if large
macromolecules of a diameter greater than these spacings are secreted
through this layer, the local ordering of the peptidoglycan must
somehow be disrupted.
0021-9193/99/$04.00+0
Copyright © 1999, American Society for Microbiology. All rights reserved.
Thickness and Elasticity of Gram-Negative Murein
Sacculi Measured by Atomic Force Microscopy
*
Corresponding author. Mailing address: Department of
Microbiology, College of Biological Science, University of Guelph,
Guelph, Ontario, Canada N1G 2W1. Phone: (519) 824-4120, ext. 3366. Fax: (519) 837-1802. E-mail: tjb{at}micro.uoguelph.ca.
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