Large-scale vortex lattice emerging from collectively moving microtubules.

Spontaneous collective motion, as in some flocks of bird and schools of fish, is an example of an emergent phenomenon. Such phenomena are at present of great interest and physicists have put forward a number of theoretical results that so far lack experimental verification. In animal behaviour studies, large-scale data collection is now technologically possible, but data are still scarce and arise from observations rather than controlled experiments. Multicellular biological systems, such as bacterial colonies or tissues, allow more control, but may have many hidden variables and interactions, hindering proper tests of theoretical ideas. However, in systems on the subcellular scale such tests may be possible, particularly in in vitro experiments with only few purified components. Motility assays, in which protein filaments are driven by molecular motors grafted to a substrate in the presence of ATP, can show collective motion for high densities of motors and attached filaments. This was demonstrated recently for the actomyosin system, but a complete understanding of the mechanisms at work is still lacking. Here we report experiments in which microtubules are propelled by surface-bound dyneins. In this system it is possible to study the local interaction: we find that colliding microtubules align with each other with high probability. At high densities, this alignment results in self-organization of the microtubules, which are on average 15 µm long, into vortices with diameters of around 400 µm. Inside the vortices, the microtubules circulate both clockwise and anticlockwise. On longer timescales, the vortices form a lattice structure. The emergence of these structures, as verified by a mathematical model, is the result of the smooth, reptation-like motion of single microtubules in combination with local interactions (the nematic alignment due to collisions)--there is no need for long-range interactions. Apart from its potential relevance to cortical arrays in plant cells and other biological situations, our study provides evidence for the existence of previously unsuspected universality classes of collective motion phenomena.

Calaxin drives sperm chemotaxis by Ca²âº-mediated direct modulation of a dynein motor.

Sperm chemotaxis occurs widely in animals and plants and plays an important role in the success of fertilization. Several studies have recently demonstrated that Ca(2+) influx through specific Ca(2+) channels is a prerequisite for sperm chemotactic movement. However, the regulator that modulates flagellar movement in response to Ca(2+) is unknown. Here we show that a neuronal calcium sensor, calaxin, directly acts on outer-arm dynein and regulates specific flagellar movement during sperm chemotaxis. Calaxin inhibition resulted in significant loss of sperm chemotactic movement, despite normal increases in intracellular calcium concentration. Using a demembranated sperm model, we demonstrate that calaxin is essential for generation and propagation of Ca(2+)-induced asymmetric flagellar bending. An in vitro motility assay revealed that calaxin directly suppressed the velocity of microtubule sliding by outer-arm dynein at high Ca(2+) concentrations. This study describes the missing link between chemoattractant-mediated Ca(2+) signaling and motor-driven microtubule sliding during sperm chemotaxis.

Fluorescence resonance energy transfer between points on actin and the C-terminal region of tropomyosin in skeletal muscle thin filaments.

Fluorescence resonance energy transfer between points on tropomyosin (positions 87 and 190) and actin (Gln-41, Lys-61, Cys-374, and the ATP-binding site) showed no positional change of tropomyosin relative to actin on the thin filament in response to changes in Ca2+ concentration (Miki et al. (1998) J. Biochem. 123, 1104-1111). This is consistent with recent electron cryo-microscopy analysis, which showed that the C-terminal one-third of tropomyosin shifted significantly towards the outer domain of actin, while the N-terminal half of tropomyosin shifted only a little (Narita et al. (2001) J. Mol. Biol. 308, 241-261). In order to detect any significant positional change of the C-terminal region of tropomyosin relative to actin, we generated mutant tropomyosin molecules with a unique cysteine residue at position 237, 245, 247, or 252 in the C-terminal region. The energy donor probe was attached to these positions on tropomyosin and the acceptor probe was attached to Cys-374 or Gln-41 of actin. These probe-labeled mutant tropomyosin molecules retain the ability to regulate the acto-S1 ATPase activity in conjunction with troponin and Ca2+. Fluorescence resonance energy transfer between these points of tropomyosin and actin showed a high transfer efficiency, which should be very sensitive to changes in distance between probes attached to actin and tropomyosin. However, the transfer efficiency did not change appreciably upon removal of Ca2+ ions, suggesting that the C-terminal region of tropomyosin did not shift significantly relative to actin on the reconstituted thin filament in response to the change of Ca2+ concentration.

The second half of the fourth period of tropomyosin is a key region for Ca(2+)-dependent regulation of striated muscle thin filaments.

Rabbit skeletal muscle alpha-tropomyosin (Tm), a 284-residue dimeric coiled-coil protein, spans seven actin monomers and contains seven quasiequivalent periods. X-ray analysis of cocrystals of Tm and troponin (Tn) placed the Tn core domain near residues 150-180 of Tm. To identify the Ca(2+)-sensitive Tn interaction site on Tm, we generated three Tm mutants to compare the consequences of sequence substitution inside and outside of the Tn core domain-binding region. Residues 152-165 and 156-162 in the second half of period 4 were replaced by corresponding residues 33-46 and 37-43 in the second half of period 1, respectively (termed mTm152-165 and mTm156-162, respectively), and residues 134-147 in the first half of period 4 were replaced with residues 15-28 in the first half of period 1 (mTm134-147). Recombinant Tms designed with an additional tripeptide, Ala-Ala-Ser, at the N-terminus were expressed in Escherichia coli. Both mTm152-165 and mTm156-162 suppressed the actin-activated myosin subfragment-1 Mg(2+)-ATPase rate regardless of whether Ca(2+) and Tn were present. On the other hand, mTm134-147 retained the normal Ca(2+)-sensitive regulation, although the actin binding of mTm alone was significantly impaired. Differential scanning calorimetry showed that the sequence substitution in the second half of period 4 affected the thermal stability of the complete Tm molecule and also the actin-induced stabilization. These results suggest that the second half of period 4 of Tm is a key region for inducing conformational changes of the regulated thin filament required for its fully activated state.

The rates of switching movement of troponin T between three states of skeletal muscle thin filaments determined by fluorescence resonance energy transfer.

Troponin (Tn) plays the key roles in the regulation of striated muscle contraction. Tn consists of three subunits (TnT, TnC, and TnI). In combination with the stopped-flow method, fluorescence resonance energy transfer between probes attached to Cys-60 or Cys-250 of TnT and Cys-374 of actin was measured to determine the rates of switching movement of the troponin tail domain (Cys-60) and of the TnT-TnI coiled-coil C terminus (Cys-250) between three states (relaxed, closed, and open) of the thin filament. When the free Ca(2+) concentration was rapidly changed, these domains moved with rates of approximately 450 and approximately 85 s(-1) at pH 7.0 on Ca(2+) up and down, respectively. When myosin subfragment 1 (S1) was dissociated from thin filaments by rapid mixing with ATP, these domains moved with a single rate constant of approximately 400 s(-1) in the presence and absence of Ca(2+). The light scattering measurements showed that ATP-induced S1 dissociation occurred with a rate constant >800 s(-1). When S1 was rapidly mixed with the thin filament, these domains moved with almost the same or slightly faster rates than those of S1 binding measured by light scattering. In most but not all aspects, the rates of movement of the troponin tail domain and of the TnT-TnI coiled-coil C terminus were very similar to those of certain TnI sites (N terminus, Cys-133, and C terminus) previously characterized (Shitaka, Y., Kimura, C., Iio, T., and Miki, M. (2004) Biochemistry 43, 10739-10747), suggesting that a series of conformational changes in the Tn complex during switching on or off process occurs synchronously.

Kinetics of the structural transition of muscle thin filaments observed by fluorescence resonance energy transfer.

Fluorescence resonance energy transfer showed that troponin-I changes the position on an actin filament corresponding to three states (relaxed, closed, and open) of the thin filament (Hai et al. (2002) J. Biochem. 131, 407-418). In combination with the stopped-flow method, fluorescence resonance energy transfer between probes attached to position 1, 133, or 181 of troponin-I and Cys-374 of actin on reconstituted thin filaments was measured to follow the transition between three states of the thin filament. When the free Ca(2+) concentration was increased, the transition from relaxed to closed states occurred with a rate constant of approximately 500 s(-1). For the reverse transition, the rate constant was approximately 60 s(-1). When myosin subfragment-1 was dissociated from thin filaments in the presence of Ca(2+) by rapid mixing with ATP, the transition from open to closed states occurred with a single rate constant of approximately 300 s(-1). Light-scattering measurements showed that the ATP-induced myosin subfragment-1 dissociation occurred with a rate constant of approximately 900 s(-1). In the absence of Ca(2+), the transition from open to relaxed states occurred with two rate constants of approximately 400 and approximately 80 s(-1). These transition rates are fast enough to allow the spatial rearrangement of thin filaments to be involved in the regulation mechanism of muscle contraction.