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The structure of and interactions between the normal and mutant espin-actin
complexes was systematically investigated using confocal microscopy and
synchrotron small angle x-ray scattering (SAXS) performed at BL4-2 of the
Stanford Synchrotron Radiation Laboratory and at the BESSRC-CAT (BL12-ID) at
the Advanced Photon Source. The SAXS data shows how interactions between
F-actin and different espin linkers are expressed in the system's
self-assembled structure and phase behavior.
The mixtures of normal espin and F-actin showed well defined actin bundles in
the confocal microscope images, which were found to be extremely well ordered
hexagonal bundle of twisted actin filaments when studied via SAXS (Fig. 1).
From the diffraction data we also measured the twisting of the helical F-actin
filaments and found that it was increased by -0.9 degrees from the native
helical twisting of F-actin. This suggests that the bundles of twisted
filaments are under constant strain, which acts to maintain the stability of
the bundle structure. From the large number of and narrow width of the
hexagonally coordinated peaks we determined that these bundles were well very
ordered and large. This corresponds to very rigid bundles; an important factor
for bundles which are typically used as mechanical sensors (levers) in living
cells.
Fig. 1(a)
Diffraction from partially oriented F-actin-espin bundles shows many
hexagonally coordinated peaks. The reconstructed 3D bundle structure is
approximated in (b). (c) Diffraction from F-actin complexed with mutant espin.
The diffraction pattern only shows a "bow-tie" pattern which is indicative of a
liquid crystalline nematic phase, like that shown in (d). The mutant espins
only weakly crosslink the actin filaments, but the normal espins arrange the
actin into tight crystalline bundles.
The structure of the bundles changes dramatically when normal espin is replaced
with espin mutants that cause deafness. The deafness mutants have damaged actin
binding sites and thus can be thought of as being less 'sticky' than the wild
type espins. With these deafness mutations we could then assess the
relationship between linker 'stickiness' and actin bundle formation. Damaging
the actin binding site impairs the ability to form thick ordered bundles. The
dominant deafness mutant (which has one good actin binding site, and one
partial binding site) bundles actin at high espin concentrations creating a
similar hexagonal structure to the normal espin-actin bundles but the
inter-actin spacing was larger and more variable. At low espin concentrations,
though, the hexagonal bundle peaks decreased in intensity and a new
nematic-like peak appeared which displays a characteristic "bow-tie" pattern in
2D (Fig. 1). This indicates that the rods spontaneously oriented along an axis
but they only had short-range positional ordering, not like the bundles which
have long range ordering (Fig. 1). This nematic ordering is in addition to weak
crosslinking which pulls the actin filaments close together, but not close
enough to form bundles. A stronger mutant espin (which has only one actin
binding site, the second being completely truncated by the mutation) was also
studied, and for this recessive mutation, bundles never form, only the weakly
crosslinked nematic phase is observed.
The observation of this crosslinked nematic-network phase was very exciting
from a physics standpoint as new theories have been recently developed to
explain physical relationship between the network and bundle phases of actin
observed in cells, and the multitude of crosslinking proteins. By changing the
preferred orientation of the crosslinking protein (does it like to form bundles
or perpendicular networks) a rich phase behavior can predicted. However, the
weakly crosslinked nematic phase observed with the deafness mutant espins,
which are "weakly sticky" but still want to orient the actin filaments in
bundles, has not yet been explored theoretically. This suggests that there is a
new axis yet to be explored in the theoretical phase diagram of filaments and
crosslinkers - the 'stickiness' axis.
The biological implications of a weakly crosslinked nematic phase in ear cell
stereocilia show up predominantly in the bending stiffness. A weakly
crosslinked nematic phase has a bending stiffness which is about a thousand
times floppier, than a rigid bundle. This is in fact consistent with the
observation that mutant espin cause malformed, floppy stereocilia. A thinner
diameter bundle (which occurs even when the deafness mutant espins do bundle)
also results in much floppier bundles. As a consequence the ear cannot respond
to sound in the same way. When mixing mutant espin and normal espin (as is
normally the case for the dominant mutant expression in humans), however, the
bundling ability of the espin can be restored, and the bundles get slightly
thicker. It is possible that this mechanism could be used to potentially
'rescue' this particular kind of pathology, particularly in the dominant mutant
case, where partial expression of the normal espin is already possible. If gene
expression could turn on the production of slightly more normal espin linkers,
a kind of rescue attempt at restoring hearing could, in principle, be made.
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Last Updated: | 30 July 2007 |
Content Owner: | K. Purdy and G. Wong |
Page Editor: | L. Dunn |