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Biologische Systeme und Medizin Poster: Mi., 14:00–16:30 M-P181<br />

Dynamic studies of an in situ molecular motor using synchrotron radiation<br />

Christopher Ashley 1 , Maria Bagni 2 , Giovanni Cecchi 2 , Barbara Colombini 2 ,<br />

Sergio Funari 3 , Peter Griffiths 1 , Radek Pelc 4<br />

1 Univ. Lab. of Physiology, Parks Road, Oxford OX1 3PT, U.K. – 2 Dpt. di Scienze<br />

Fisiol., Universita degli Studi di Firenze, Florence I-50134, Italy. – 3 Gebaeude 25F,<br />

Hasylab at DESY, Notkestrasse 85, Hamburg D-22603, Germany – 4 Dept. of Microbiology,<br />

Czech Academy of Sciences, 142 20 Prague 4-Krc, Czech Republic.<br />

In higher animals, mechanical work is performed by translational molecular motors<br />

(protein macromolecules which transduce the free energy of ATP hydrolysis into linear<br />

motion). The most ubiquitous motor, myosin, achieves this by a multi-stage catalysis<br />

of ATP hydrolysis, powering cardiac and smooth muscle, all voluntary movement,<br />

and also adjustment of visual and aural acuity and myriad processes in intracellular<br />

physiology. Myosins form a class of at least 17 different forms of translational motor<br />

[1] Myosin II, present in all muscle tissue, is unique in that it forms helically-based<br />

filamentous aggregates. In striated muscles, these are arranged in a quasi-crystalline<br />

array, per<strong>mit</strong>ting structural events in the motor to be investigated dynamically by<br />

time-resolved X-ray diffraction. The X-ray pattern from skeletal muscle contains a<br />

strong axial reflection (M3) at a spacing corresponding to the third harmonic of the<br />

pitch of the myosin helix, which is sensitive to changes in myosin molecular structure.<br />

Upon activation, it undergoes changes in both intensity (IM3) and in axial spacing<br />

(dM3) [2]. We have studied the changes in M3 which accompany the motor power<br />

stroke in the microsecond time domain, and have attempted to relate these changes to<br />

the crystallographic structure of the myosin molecule.<br />

IM3 changes reflect structural events in the S1 moiety of myosin, which projects from<br />

the surface of the myosin filament on a helical pitch and bears both the ATP catalytic<br />

site and the binding sites for the filamentous protein, actin (the ’track’ along which<br />

the myosin ’locomotive’ runs). Recent crystallographic work suggests that the motor<br />

mechanism is a tilting of the ’lever arm’ domain of S1, an a-helix chain of 9nm in length,<br />

linking the actin- and ATP-binding motor domain to the myosin filament backbone,<br />

producing 2-5 pN of force if isometric, or ca. 10 nm of translation if movement is<br />

per<strong>mit</strong>ted.<br />

dM3 increases by ca. 1.5 % upon activation. This change is not explicable by structural<br />

events in S1. Instead, it may indicate a change in the myosin filament backbone<br />

structure, or the formation of a new axial unit cell due to the mismatch of actin and<br />

myosin filament helices. Recently, we examined this phenomenon further [3]. Our<br />

findings question the origin of this spacing change, suggesting that dM3 is not an<br />

indicator of actin-S1 interaction, and allowing us to propose a new mechanism for dM3<br />

changes which could have important consequences for the prevailing models of the<br />

mechanism of contraction.<br />

[1] Sellers, J.R. Biochim. Biophys. Acta. 1496 (2000) 3. [2] Huxley, H.E.et al., J. Mol.<br />

Biol. 158 (1982) 63711. [3] Griffiths, P.J. et al., Biophys. J., 90 (2006) 975.

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