Active streaming in actomyosin solutions

Solutions of actomyosin, extracted from plasmodia of Physarum polycephalum or from rabbit's striated muscle, were introduced into microcapillaries in the presence of ATP. Vigorous and sometimes oscillatory streaming was observed which resembled in many respects cytoplasmatic streaming.     

Depletion of phosphate in active muscle fibers probes actomyosin states within the powerstroke.

Variation in the concentration of orthophosphate (Pi) in actively contracting, chemically skinned muscle fibers has proved to be a useful probe of actomyosin interaction. Previous studies have shown that isometric tension (Po) decreases linearly in the logarithm of [Pi] for [Pi] > or = 200 microM. This result can be explained in terms of cross-bridge models in which the release of Pi is involved in the transition from a weakly bound, low-force actin x myosin x ADP x Pi state to a strongly bound, high-force, actin x myosin x ADP state. The 200 microM minimum [Pi] examined results from an inability to buffer the intrafiber, diffusive buildup of Pi resulting from the fiber ATPase. In the present study, we overcome this limitation by employing the enzyme purine nucleoside phosphorylase with substrate 7-methylguanosine to reduce the calculated internal [Pi] in contracting rabbit psoas fibers to < 5 microM. At 10 degrees C we find that Po continues to increase as the [Pi] decreases for [Pi] > or = 100 microM. Below this [Pi], Po is approximately constant. These results indicate that the free energy drop in the cross-bridge powerstroke is approximately 9 kT. This value is shown to be consistent with observations of muscle efficiency at physiological temperatures.     

Contribution of the actomyosin motor to the temperature-dependent translational diffusion of water by cytoplasmic streaming in Elodea canadensis cells

Summary. The extent to which the actomyosin motor responsible for cytoplasmic streaming contributes to the translational diffusion of water in Elodea canadensis cells was studied by a nuclear magnetic resonance (NMR) spin-echo technique. The relative contribution of the actomyosin motor was determined from the corresponding apparent diffusion coefficient by the Einstein–Smolukhovsky relation. It is equal to the difference between the diffusional displacements of the cytoplasmic and the bulk water (X). The NMR data show that the temperature dependence of X is humpshaped, which is characteristic of enzyme reactions. At the same time, the apparent diffusion coefficient of cytoplasmic water increases with an increase in temperature. The most significant contribution of the actomyosin motor to X is observed at temperatures below 20°C. Within the temperature range of 20 to 33°C, X changes only slightly, and a further increase in temperature reduces X to zero.     

Study of cytoplasm streaming as a cytophysiological method in radiolabeled experiment

Estimation of influence of ionizing radiation, high-frequency electromagnetic radiation and their combined action on a higher water plant Elodea canadensis has been carried out using cytophysiological method of determination of the cytoplasm streaming rate. It was shown that low-intensive electromagnetic radiation modifies reaction of the differentiated cells on radiolesion. The rate of cytoplasm streaming can be used as an informative characteristic of plant cell state in radiobiological experiment.     

Theoretical investigation of aspects of single-molecule fluorescence detection in microcapillaries.

In the present report, the results of a theoretical investigation of two aspects of single-molecule detection by laser-induced fluorescence in microcapillaries are presented. The two issues studied are the scattering of the exciting laser beam on the microcapillary and the change of the fluorescence lifetime of the molecule due to the electrodynamic interaction between its fluorescence emission and the confining capillary. Numerical results for experimentally relevant conditions are provided.     

On the mechanical response of the actomyosin cortex during cell indentations

Biomechanics and Modeling in Mechanobiology - A mechanical model is presented to analyze the mechanics and dynamics of the cell cortex during indentation. We investigate the impact of active...     

Dinitrophenylation of rabbit skeletal actomyosin.

Dinitrophenylated reconstituted or natural actomyosin effected changes in the Ca2+ sensitivity which were dependent upon the ionic strength of the reaction medium. Dinitrophenylation of reconstituted actomyosin in 0.6 M KCl led to the incorporation of 2-6 mol of the reagent per 5-10(5) g of protein and it possessed considerable Ca2+ sensitivity. Dinitrophenylated natural actomyosin under the same conditions lost most of its Ca2+ sensitivity when 1.3-5.4 mol of the dinitrophenyl group were bound. The myosin from these modified actomyosins did not lose Ca2+ sensitivity and the myosin was labeled only with 0.4-1.7 mol of the dinitrophenyl group. Dinitrophenylation of both kinds of actomyosin in 0.06 M KCl abolished the Ca2+ sensitivity; the myosin from the modified actomyosins also lost Ca2+ sensitivity. Myosin alone was more susceptible to a loss of Ca2+ sensitivity than myosin in actomyosin. Actin protected the ability of myosin to sense Ca2+ regulated actin in modified actomyosin at 0.6 M KCl but not at 0.06 M KCl. Actomyosin dinitrophenylated in the presence of ATP lost Ca2+ sensitivity. However, the myosin from this actomyosin possessed Ca2+ sensitivity. Thiolysis of the dinitrophenylated actomyosin by 2-mercaptoethanol at low ionic strength did not restore the Ca2+ sensitivity of this actomyosin or its myosin although there was a significant loss of the dinitrophenyl group.     

Actin cross-linking and inhibition of the actomyosin motor.

Intrastrand cross-linking of actin filaments by ANP, N-(4-azido-2-nitrophenyl) putrescine, between Gln-41 in subdomain 2 and Cys-374 at the C-terminus, was shown to inhibit force generation with myosin in the in vitro motility assays [Kim et al. (1998) Biochemistry 37, 17801-17809]. To clarify the immobilization of which of these two sites inhibits the actomyosin motor, the properties of actins with partially overlapping cross-linked sites were examined. pPDM (N,N'-p-phenylenedimaleimide) and ABP [N-(4-azidobenzoyl) putrescine] were used to obtain actin filaments cross-linked ( approximately 50%) between Cys-374 and Lys-191 (interstrand) and Gln-41 and Lys-113 (intrastrand), respectively. ANP, ABP, and pPDM cross-linked filaments showed similar inhibition of their sliding speeds and force generation with myosin ( approximately 25%) in the in vitro motility assays. In analogy to ANP cross-linking of actin, pPDM and ABP cross-linkings did not change the strong S1 binding to actin and the V(max) and K(m) parameters of actomyosin ATPase. The similar effects of these three cross-linkings reveal the tight coupling between structural elements of the subdomain 2/subdomain 1 interface and show the importance of its dynamic flexibility to force generation with myosin. The possibility that actin cross-linkings inhibit rate-limiting steps in motion and force generation during myosin cross-bridge cycle was tested in stopped-flow experiments. Measurements of the rates of mantADP release from actoS1 and ATP-induced dissociation of actoS1 did not reveal any differences between un-cross-linked and ANP cross-linked actin in these complexes. These findings are discussed in terms of the uncoupling between force generation and other aspects of actomyosin interactions due to a constrained dynamic flexibility of the subdomain 2/subdomain 1 interface in cross-linked actin filaments.     

Mechanism of actomyosin adenosine triphosphatase. Evidence that adenosine 5'-triphosphate hydrolysis can occur without dissociation of the actomyosin complex.

We have investigated the steps in the actomyosin ATPase cycle that determine the maximum ATPase rate (Vmax) and the binding between myosin subfragment one (S-1) and actin which occurs when the ATPase activity is close to Vmax. We find that the forward rate constant of the initial ATP hydrolysis (initial Pi burst) is about 5 times faster than the maximum turnover rate of the actin S-1 ATPase. Thus, another step in the cycle must be considerably slower than the forward rate of the initial Pi burst. If this slower step occurs only when S-1 is complexed with actin, as originally predicted by the Lymn-Taylor model, the ATPase activity and the fraction of S-1 bound to actin in the steady state should increase almost in parallel as the actin concentration is increased. As measured by turbidity determined in the stopped-flow apparatus, the fraction of S-1 bound to actin, like the ATPase activity, shows a hyperbolic dependence on actin concentration, approaching 100% asymptotically. However, the actin concentration required so that 50% of the S-1 is bound to actin is about 4 times greater than the actin concentration required for half-maximal ATPase activity. Thus, as previously found at 0 degrees C, at 15 degrees C much of the S-1 is dissociated from actin when the ATPase is close to Vmax, showing that a slow first-order transition which follows the initial Pi burst (the transition from the refractory to the nonrefractory state) must be the slowest step in the ATPase cycle. Stopped-flow studies also reveal that the steady-state turbidity level is reached almost instantaneously after the S-1, actin, and ATP are mixed, regardless of the order of mixing. Thus, the binding between S-1 and actin which is observed in the steady state is due to a rapid equilibrium between S-1--ATP and acto--S-1--ATP which is shifted toward acto-S-1--ATP at high actin concentration. Furthermore, both S-1--ATP and S-1--ADP.Pi (the state occurring immediately after the initial Pi burst) appear to have the same binding constant to actin. Thus, at high actin concentration both S-1--ATP and S-1--ADP.Pi are in rapid equilibrium with their respective actin complexes. Although at very high actin concentration almost complete binding of S-1--ATP and S-1--ADP.Pi to actin occurs, there is no inhibition of the ATPase activity at high actin concentration. This strongly suggests that both the initial Pi burst and the slow rate-limiting transition which follows (the transition from the refractory to the nonrefractory state) occur at about the same rates whether the S-1 is bound to or dissociated from actin. We, therefore, conclude that S-1 does not have to dissociate from actin each time an ATP molecule is hydrolyzed.     

Calmodulin distribution and the actomyosin cytoskeleton in Toxoplasma gondii.

The gliding motility of the protozoan parasite Toxoplasma gondii and its invasion of cells are powered by an actin-myosin motor. We have studied the spatial distribution and relationship between these two cytoskeleton proteins and calmodulin (CaM), the Ca(2+)-dependent protein involved in invasion by T. gondii. A 3D reconstruction using labeling and tomographic studies showed that actin was present as a V-like structure in the conoidal part of the parasite. The myosin distribution overlapped that of actin, and CaM was concentrated at the center of the apical pole. We demonstrated that the actomyosin network, CaM, and myosin light-chain kinases are confined to the apical pole of the T. gondii tachyzoite. MLCK could act as an intermediate molecule between CaM and the cytoskeleton proteins. We have developed a model of the organization of the actomyosin-CaM complex and the steps of a signaling pathway for parasite motility.     

Intermediate states of actomyosin adenosine triphosphatase.

The early kinetic steps of actomyosin subfragment 1 (acto-S1) adenosine triphosphatase have been investigated by simultaneous monitoring of fluorescence and light scattering and also by observation of the time course of the production of phosphate. The results show that fluorescence enhancement occurs after the dissociation of actomyosin and that the rate of enhancement is similar to the maximum rate of enhancement for S1 alone, under similar conditions of pH and temperature. The maximum rate of the phosphate burst for acto S1 is also approximately the same as that for S1 alone. The maximum rates for fluorescence enhancement or phosphate formation are reached at much lower adenosine triphosphate concentrations for acto-S1 than for S1. An extension of the actomyosin scheme is presented which accounts for these results.