SUMMARY Actomyosin contractility plays a central role in a wide range of cellular processes, including the establishment of cell polarity, cell migration, tissue integrity, and morphogenesis during development. The contractile response is variable and depends on actomyosin network architecture and biochemical composition. To determine how this coupling regulates actomyosin-driven contraction, we used a micropatterning method that enables the spatial control of actin assembly. We generated a variety of actin templates and measured how defined actin structures respond to myosin-induced forces. We found that the same actin filament crosslinkers either enhance or inhibit the contractility of a network, depending on the organization of actin within the network. Numerical simulations unified the roles of actin filament branching and crosslinking during actomyosin contraction. Specifically, we introduce the concept of “network connectivity” and show that the contractions of distinct actin architectures are described by the same master curve when considering their degree of connectivity. This makes it possible to predict the dynamic response of defined actin structures to transient changes in connectivity. We propose that, depending on the connectivity and the architecture, network contraction is dominated by either sarcomeric-like or buckling mechanisms. More generally, this study reveals how actin network contractility depends on its architecture under a defined set of biochemical conditions.

The organization of actin filaments into higher-ordered structures governs eukaryotic cell shape and movement. Global actin network size and architecture is maintained in a dynamic steady-state through regulated assembly and disassembly. Here, we used experimentally defined actin structures in vitro to investigate how the activity of myosin motors depends on network architecture. Direct visualization of filaments revealed myosin-induced actin network deformation. During this reorganization myosins selectively contracted and disassembled anti-parallel actin structures while parallel actin bundles remained unaffected. The local distribution of nucleation sites and the resulting orientation of actin filaments appeared to regulate the scalability of the contraction process. This “orientation selection” mechanism for selective contraction and disassembly suggests how the dynamics of the cellular actin cytoskeleton can be spatially controlled by actomyosin contractility.

SummaryDEAD-box proteins are ATPase enzymes that destabilize and unwind duplex RNA. Quantitative knowledge of the ATPase cycle parameters is critical for developing models of helicase activity. However, limited information regarding the rate and equilibrium constants defining the ATPase cycle of RNA helicases is available, including the distribution and flux of populated biochemical intermediates, the catalytic step(s) that limits the enzymatic reaction cycle, and how ATP utilization and RNA interactions are linked. We present a quantitative kinetic and equilibrium characterization of the rRNA-activated ATPase cycle mechanism of DbpA, a DEAD-box rRNA helicase implicated in ribosome biogenesis. rRNA activates the ATPase activity of DbpA by promoting a conformational change after ATP binding that is associated with hydrolysis. Chemical cleavage of bound ATP is reversible and occurs via a gamma phosphate attack mechanism. ADP-P i and RNA binding display strong thermodynamic coupling, which causes DbpA-ADP-P i to bind rRNA with > 10-fold higher affinity than with bound ATP, ADP or in the absence of nucleotide. The rRNA-activated steady-state ATPase cycle of DbpA is limited both by ATP hydrolysis and P i release, which occur with comparable rates. Consequently, the predominantly populated biochemical states during steady-state cycling are the ATP-and ADP-P i -bound intermediates. Thermodynamic linkage analysis of the ATPase cycle transitions favors models in which rRNA duplex destabilization is linked to strong rRNA and nucleotide binding. The presented analysis of the DbpA ATPase cycle reaction mechanism provides a rigorous kinetic and thermodynamic foundation for developing testable hypotheses regarding the functions and molecular mechanisms of DEAD-box helicases.

The actin regulatory protein, cofilin, increases the bending and twisting elasticity of actin filaments and severs them. It has been proposed that filaments partially decorated with cofilin accumulate stress from thermally driven shape fluctuations at bare (stiff) and decorated (compliant) boundaries, thereby promoting severing. This mechanics-based severing model predicts that changes in actin filament compliance due to cofilin binding affect severing activity. Here, we test this prediction by evaluating how the severing activities of vertebrate and yeast cofilactin scale with the flexural rigidities determined from analysis of shape fluctuations. Yeast actin filaments are more compliant in bending than vertebrate actin filaments. Severing activities of cofilactin isoforms correlate with changes in filament flexibility. Vertebrate cofilin binds but does not increase the yeast actin filament flexibility, and does not sever them. Imaging of filament thermal fluctuations reveals that severing events are associated with local bending and fragmentation when deformations attain a critical angle. The critical severing angle at boundaries between bare and cofilin-decorated segments is smaller than in bare or fully decorated filaments. These measurements support a cofilin-severing mechanism in which mechanical asymmetry promotes local stress accumulation and fragmentation at boundaries of bare and cofilin-decorated segments, analogous to failure of some nonprotein materials.

Ligand photolysis and subsequent electronic and structural relaxation, followed by ligand recombination, in ferrous cytochrome c (cyt c) have been studied using ultrafast laser spectroscopy. A broad-band white-light continuum, generated by amplified pulses from a Ti:sapphire laser, was used to monitor the transient absorption spectra of cyt c in the Soret and Q bands following 50-fs pulsed photoexcitation at 400 nm. The reconstructed photoproduct absorption spectrum is found to closely resemble that of a model pentacoordinate histidineligated complex, microperoxidase (MP-8), suggesting methionine photolysis. Vibrational modes at ∼40, ∼80, and ∼220 cm -1 are observed in femtosecond coherence spectroscopy (FCS) measurements, which also indicates photodissociation of the methionine ligand. The quantum yield of ligand photolysis is found to be g80%, which is consistent with the ultrafast photolysis time constant (e40 fs) needed to induce coherent oscillations in the FCS measurements. The combination of high quantum yield and short time constant helps to resolve the longstanding question of the origin of the short lifetime (τ e ) and large Soret-state electronic damping factor (Γ e ) previously found in cytochrome c. We propose a simple multilevel model to describe the observed experimental data. The global analysis of the measured kinetics leads to a characterization of the major kinetic rates, including the 6.2-ps geminate rebinding of methionine to the heme iron. † Part of the special issue "Thomas Spiro Festschrift".

Flash photolysis investigations of horse heart metmyoglobin bound with NO (Mb(3+)NO) reveal the kinetics of water entry and binding to the heme iron. Photodissociation of NO leaves the sample in the dehydrated Mb(3+) (5-coordinate) state. After NO photolysis and escape, a water molecule enters the heme pocket and binds to the heme iron, forming the 6-coordinate aquometMb state (Mb(3+)H2O). At longer times, NO displaces the H2O ligand to reestablish equilibrium. At 293 K, we determine a value k(w) approximately 5.7 x 10(6) s(-1) for the rate of H2O binding and estimate the H2O dissociation constant as 60 mM. The Arrhenius barrier height H(w) = 42 +/- 3 kJ/mol determined for H2O binding is identical to the barrier for CO escape after photolysis of Mb(2+)CO, within experimental uncertainty, consistent with a common mechanism for entry and exit of small molecules from the heme pocket. We propose that both processes are gated by displacement of His-64 from the heme pocket. We also observe that the bimolecular NO rebinding rate is enhanced by 3 orders of magnitude both for the H64L mutant, which does not bind water, and for the H64G mutant, where the bound water is no longer stabilized by hydrogen bonding with His-64. These results emphasize the importance of the hydrogen bond in stabilizing H2O binding and thus preventing NO scavenging by ferric heme proteins at physiological NO concentrations.

The [Mg(2+)] dependence of ADP binding to myosin V and actomyosin V was measured from the fluorescence of mantADP. Time courses of MgmantADP dissociation from myosin V and actomyosin V are biphasic with fast observed rate constants that depend on the [Mg(2+)] and slow observed rate constants that are [Mg(2+)]-independent. Two myosin V-MgADP states that are in reversible equilibrium, one that exchanges nucleotide and cation slowly (strong binding) and one that exchanges nucleotide and cation rapidly (weak binding), account for the data. The two myosin V-MgADP states are of comparable energies, as indicated by the relatively equimolar partitioning at saturating magnesium. Actin binding lowers the affinity for bound Mg(2+) 2-fold but shifts the isomerization equilibrium approximately 6-fold to the weak ADP binding state, lowering the affinity and accelerating the overall rate of MgADP release. Actin does not weaken the affinity or accelerate the release of cation-free ADP, indicating that actin and ADP binding linkage is magnesium-dependent. Myosin V and myosin V-ADP binding to actin was assayed from the quenching of pyrene actin fluorescence. Time courses of myosin V-ADP binding and release are biphasic, consistent with the existence of two (weak and strong) quenched pyrene actomyosin V-ADP conformations. We favor a sequential mechanism for actomyosin V dissociation with a transition from strong to weak actin-binding conformations preceding dissociation. The data provide evidence for multiple myosin-ADP and actomyosin-ADP states and establish a kinetic and thermodynamic framework for defining the magnesium-dependent coupling between the actin and nucleotide binding sites of myosin.

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