Two-state equilibria of myosin subfragment 1 and its complexes with ADP and actin

Kinetic and spectroscopic evidence for three actomyosin:ADP states in smooth muscle

Smooth muscle myosin II undergoes an additional movement of the regulatory domain with ADP release that is not seen with fast skeletal muscle myosin II. In this study, we have examined the interactions of smooth muscle myosin subfragment 1 with ADP to see if this additional movement corresponds to an identifiable state change. These studies indicate that for this myosin:ADP, both the catalytic site and the actin-binding site can each assume one of two conformations. Relatively loose coupling between these two binding sites leads to three discrete actin-associated ADP states. Following an initial, weakly bound state, binding of myosin:ADP to actin shifts the equilibrium toward a mixture of two states that each bind actin strongly but differ in the conformation of their catalytic sites. By contrast, fast myosins, including Dictyostelium myosin II, have reciprocal coupling between the actin- and ADP-binding sites, so that either actin or nucleotide, but not both, can be tightly bound. This uncoupling, which generates a second strongly bound actomyosin ADP state in smooth muscle, would prolong the fraction of the ATPase cycle time that this actomyosin spends in a force-generating conformation and may be central to explaining the physiologic differences between this and other myosins.

Osmotic pressure probe of actin-myosin hydration changes during ATP hydrolysis

Osmotic stress in the 0.5-5 x 10(6) dyne/cm2 range was used to perturb the hydration of actin-myosin-ATP intermediates during steady-state hydrolysis. Polyethylene glycol (PEG) (1000 to 4000 Da), in the 1 to 10 wt% range, which does not cause protein precipitation, did not significantly affect the apparent KM or the Vmax for MgATP hydrolysis by myosin subfragment 1 (S1) alone, nor did it affect the value for the phosphate burst. Consistent with the kinetic data, osmotic stress did not affect nucleotide-induced changes in the fluorescence intensities of S1 tryptophans or of fluorescein attached to Cys-707. The accessibility of the fluorescent ATP analog, epsilon ADP, to acrylamide quenching was also unchanged. These data suggest that none of the steps in the ATP hydrolysis cycle involve substantial hydration changes, which might occur for the opening or closing of the ATP site or of other crevices in the S1 structure. In contrast, KM for the interaction of S1.MgADP.Pi with actin decreased tenfold in this range of osmotic pressure, suggesting that formation of actin.S1.MgADP.Pi involves net dehydration of the proteins. The dehydration volume increases as the size of the PEG is increased, as expected for a surface-excluded osmolyte. The measured dehydration volume for the formation of actin.S1.MgADP.Pi was used to estimate the surface area of the binding interface. This estimate was consistent with the area determined from the atomic structures of actin and myosin, indicating that osmotic stress is a reliable probe of actin.myosin.ATP interactions. The approach developed here should be useful for determining osmotic stress and excluded volume effects in situ, which are much larger than those of typical in vitro conditions.

Structural characteristics of the nucleotide-binding site of Escherichia coli primary replicative helicase DnaB protein. Studies with ribose and base-modified fluorescent nucleotide analogs

Structural characteristics of the base- and ribose-binding regions of the high-affinity noninteracting nucleotide-binding site of Escherichia coli primary replicative helicase DnaB protein have been studied, using the base-modified fluorescent nucleotide analog 1, N6-ethenoadenosine diphosphate (epsilon ADP) and the ribose-modified fluorescent analogs 3'(2')-O-(N-methylantraniloyl)adenosine 5'-diphosphate (MANT-ADP), 3'-O-(N-methylantraniloyl)deoxyadenosine 5'-diphosphate (MANT-dADP), 3'-O-(N-methylantraniloyl)-deoxyadenosine 5'-triphosphate (MANT-dATP), and 2'(3')-O-(2,4,6-trinitrophenyl)adenosine 5'-diphosphate (TNP-ADP). The obtained data indicate contrasting differences between these two regions. Binding of epsilon ADP to the DnaB helicase causes only approximately 21% increase of the nucleotide fluorescence intensity and no shift of the emission spectrum maximum. The fluorescence of bound epsilon ADP is characterized by a single lifetime of 24.2 +/- 0.6 ns, only slightly shorter than the fluorescent lifetime of the free epsilon ADP in solution (25.5 +/- 0.6 ns). Solute-quenching studies of bound epsilon ADP, using different quenchers, acrylamide, I-, and Tl+, indicate limited accessibility of ethenoadenosine to the solvent. These results strongly suggest that the base-binding region of the DnaB nucleotide-binding site is located in the polar cleft on the enzyme's surface. Moreover, the limiting emission anisotropy of bound epsilon ADP is 0.21 +/- 0.02, compared to the anisotropy of 0.3 of completely immobilized epsilon ADP at the same excitation wavelength (lambda ex = 325 nm, lambda em = 410 nm), indicating that the adenine preserves substantial mobility when bound in the base-binding site. In contrast, fluorescence intensity at the emission maximum of TNP-ADP and MANT-ADP, which has modifying groups attached to the 2' and/or 3' oxygens of the ribose, increases upon binding to DnaB by factors of approximately 4.7 (lambda ex = 408 nm) and approximately 2.6 (lambda ex = 356 nm), respectively. Moreover, the maximum of emission spectrum of bound TNP-ADP is blue-shifted by approximately 11 nm and that of MANT-ADP by approximately 12 nm. Comparisons between spectral properties of TNP-ADP and MANT-ADP bound to DnaB and in different solvents suggest that the ribose-binding region of the DnaB nucleotide-binding site has relatively low polarity. Solute quenching studies of MANT-ADP fluorescence, using acrylamide, I-, and Tl+, indicate that the MANT group has very little accessibility to the solvent when bound to DnaB. Taken together, these results suggest that the ribose-binding region constitutes a hydrophobic cleft, or pocket, with very limited, if any, contact with the solvent.(ABSTRACT TRUNCATED AT 400 WORDS)

Transient kinetics of the interaction of actin with myosin subfragment-1 in the absence of nucleotide

The kinetics of the association of actin with myosin subfragment-1 (S1) has been studied by using S1 labeled at the sulfhydryl group SH1 with 5-(iodoacetamido)fluorescein (S1-AF). Upon rapid mixing in a stopped-flow apparatus, the fluorescence intensity of the fluorescein moiety increased by 50%, followed by a slower increase that was well resolved. This slow phase of the fluorescence change could not be fitted to either a monoexponential or a biexponential function, but it could be fitted to a sum of three exponential terms yielding three observed first-order rate constants (lambda i). The dissociation of acto.-(S1-AF) was studied by displacement of S1-AF from the complex with native S1. The dissociation kinetics was characterized by a single rate constant (approximately 0.012 s-1 at 20 degrees C), and this constant was independent of S1 concentration. Together with previous equilibrium data that were obtained under identified conditions for formation of acto-subfragment-1 (Lin, S.-H., and H. C. Cheung. 1991. Biochemistry. 30:4317-4323), a six-state two-pathway model is proposed as a minimum kinetic scheme for formation of rigor acto.S1. In this model, unbound subfragment-1 exists in two conformational states (S1' and S1) which are in equilibrium with each other, one corresponding to the previously established low-temperature state and the other to the high-temperature state. Each subfragment-1 state can interact with actin to form a collision complex, followed by two isomerizations to form two acto-subfragment-1 states (A.S1' and A.S1). Both isomerizations were visible in stopped-flow experiments. Two special cases of the model were considered: 1) a rapid pre-equilibration of the initial collision complex with actin and S1, and 2) trace accumulation of the collision complex. The first case required that the three combinations of the three observed rate constants be independent of actin concentration. The data were incompatible with this approximation. The other special case required that the sum of the lambda i vary linearly with actin concentration and the other two combinations of lambda i vary with actin concentration in a quadratic fashion. The present data were in agreement with the second case. At 20 degrees C and in 60 mM KCl, 2 mM MgCl2, 30 mM 2-([-hydroxy-1,1-bis(hydroxymethyl)ethyl]amino)ethanesulfonic acid, and pH 7.5, the biomolecular association rate constants for the interaction of actin with S1' and S1 were 8.58 x 10(5) and 1.11 x 10(6) M-1 s-1, respectively.

[2-3H]ATP synthesis and 3H NMR spectroscopy of enzyme-nucleotide complexes: ADP and ADP.Vi bound to myosin subfragment 1

The synthesis of [2-3H]ATP with specific activity high enough to use for 3H NMR spectroscopy at micromolar concentrations was accomplished by tritiodehalogenation of 2-Br-ATP. ATP with greater than 80% substitution at the 2-position and negligible tritium levels at other positions had a single 3H NMR peak at 8.20 ppm in 1D spectra obtained at 533 MHz. This result enables the application of tritium NMR spectroscopy to ATP utilizing enzymes. The proteolytic fragment of skeletal muscle myosin, called S1, consists of a heavy chain (95 kDa) and one alkali light chain (16 or 21 kDa) complex that retains myosin ATPase activity. In the presence of Mg2+, S1 converts [2-3H]ATP to [2-3H]ADP and the complex S1.Mg[2-3H]ADP has ADP bound in the active site. At 0 degrees C, 1D 3H NMR spectra of S1.Mg[2-3H]ADP have two broadened peaks shifted 0.55 and 0.90 ppm upfield from the peak due to free [2-3H]ADP. Spectra with good signal-to-noise for 0.10 mM S1.Mg[2-3H]ADP were obtained in 180 min. The magnitude of the chemical shift caused by binding is consistent with the presence of an aromatic side chain being in the active site. Spectra were the same for S1 with either of the alkali light chains present, suggesting that the alkali light chains do not interact differently with the active site. The two broad peaks appear to be due to the two conformations of S1 that have been observed previously by other techniques. Raising the temperature to 20 degrees C causes small changes in the chemical shifts, narrows the peak widths from 150 to 80 Hz, and increases the relative area under the more upfield peak. Addition of orthovanadate (Vi) to produce S1.Mg[2-2H]ADP.Vi shifts both peaks slightly more upfield without changing their widths or relative areas.

Molecular movements in the actomyosin complex: F-actin-promoted internal cross-linking of the 25- and 20-kDa heavy chain fragments of skeletal myosin subfragment

We describe, for the first time, the F-actin-promoted changes in the spatial relationship of strands in the NH2-terminal 25-kDa and COOH-terminal 20-kDa heavy chain fragments of the skeletal myosin subfragment 1 (S-1), detected by their exclusive chemical cross-linking in the rigor F-actin-S-1 complex with m-maleimidobenzoic acid N-hydroxysuccinimide ester (MBS). Quantitative electrophoretic analysis of the reaction products showed extensive conversion of the 95-kDa heavy chain of the actin-bound S-1 into a new species with an apparent mass of 135 kDa (yield = 50-60%), whereas the heavy chain mobility remained unaffected when actin was omitted. The 135-kDa entity retained the fluorescence of AEDANS-S-1 but not of AEDANS-actin, indicating that it was not a cross-linked acto-heavy chain adduct. Its extent of production depended markedly on the S-1: actin molar ratio and was maximum near a ratio of 1:4. The MBS treatment of acto-S-1 led also to some covalent actin-actin oligomers which could be suppressed by using trypsin-truncated F-actin lacking Cys-374, without altering the generation of the 135-kDa heavy chain derivative.(ABSTRACT TRUNCATED AT 250 WORDS)

Nucleotide- and temperature-induced changes in myosin subfragment-1 structure

The effects of nucleotide binding and temperature on the internal structural dynamics of myosin subfragment 1 (S1) were monitored by intrinsic tryptophan phosphorescence lifetime and fluorescence anisotropy measurements. Changes in the global conformation of S1 were monitored by measuring its rate of rotational diffusion using transient electric birefringence techniques. At 5 degrees C, the binding of MgADP, MgADP,P and MgADP,V (vanadate) progressively reduce the rotational freedom of S1 tryptophans, producing what appear to be increasingly more rigidified S1-nucleotide structures. The changes in the luminescence properties of the tryptophans suggest that at least one is located at the interface of two S1 subdomains. Increasing the temperature from 0 to 25 degrees C increases the apparent internal mobility of S1 tryptophans in all cases and, in addition, a reversible temperature-dependent transition centered near 15 degrees C was observed for S1, S1-MgADP and S1-MgADP,P, but not for S1-MgADP,V. The rotational diffusion constants of S1 and S1-MgADP were measured at temperatures between 0 and 25 degrees C. After adjusting for the temperature and viscosity of the solvent, the data indicate that the thermally induced transition at 15 degrees C comprises local conformational changes, but no global conformational change. Structural features of S1-MgADP,P, which may relate to its role in force generation while bound to actin, are presented.

The kinetics of a two-state transition of myosin subfragment 1. A temperature-jump relaxation study

Temperature-jump measurements were carried out on myosin subfragment 1 (S1) labeled at Cys-707 with 5-(iodoacetamido)fluorescein (S1-AF). The relaxation was monitored by following the increase in the fluorescence intensity of the attached probe after a jump of 5.8 degrees C. A single relaxation process was observed over a range of final temperatures, and the relaxation time decreased from 16.69 ms at 15 degrees C to 3.91 ms at 27 degrees C. The relaxation results are interpreted in terms of a two-state transition: (S1-AF)L K+ in equilibrium with K- (S1-AF)H, and the observed single relaxation time (tau) equals l/(k(+) + k-). The individual first-order rate constants, k+ and k-, were calculated from tau and the equilibrium constant previously determined. The activation energy was 21.9 kcal/mol for the forward reaction and 9.3 kcal/mol for the reverse reaction, corresponding to an enthalpy value of 12.6 kcal/mol for the two-state transition. The results provide, for the first time, direct kinetic evidence of a two-state transition of S1 in the absence of bound nucleotide, and support a two-state model of unliganded myosin subfragment 1.

Actin mediated regulation of muscle contraction

Striated and smooth muscles have different mechanisms of regulation of contraction which can be the basis for selective pharmacological alteration of the contractility of these muscle types. The progression in our understanding of the tropomyosin-troponin regulatory system of striated muscle from the early 1970s through the early 1990s is described along with key concepts required for understanding this complex system. This review also examines the recent history of the putative contractile regulatory proteins of smooth muscle, caldesmon and calponin. A contrast is made between the actin linked regulatory systems of striated and smooth muscle.