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M A Geeves

Publications and source records attributed to M A Geeves.

At least 19 recordsLinked to original sources

Molecular mechanism of actomyosin-based motility.

Sophisticated molecular genetic, biochemical and biophysical studies have been used to probe the molecular mechanism of actomyosin-based motility. Recent solution measurements, high-resolution structures of recombinant myosin motor domains, and lower resolution structures of the complex formed by filamentous actin and the myosin motor domain provide detailed insights into the mechanism of chemomechanical coupling in the actomyosin system. They show how small conformational changes are amplified by a lever-arm mechanism to a working stroke of several nanometres, explain the mechanism that governs the directionality of actin-based movement, and reveal a communication pathway between the nucleotide binding pocket and the actin-binding region that explains the reciprocal relationship between actin and nucleotide affinity. Here we focus on the interacting elements in the actomyosin system and the communication pathways in the myosin motor domain that respond to actin binding.

Actins↗

Cooperative regulation of myosin-actin interactions by a continuous flexible chain I: actin-tropomyosin systems.

We present a model for cooperative myosin binding to the regulated actin filament, where tropomyosins are treated as a weakly-confined continuous flexible chain covering myosin binding sites. Thermal fluctuations in chain orientation are initially required for myosin binding, leaving kinked regions under which subsequent myosins may bind without further distortion of the chain. Statistical mechanics predicts the fraction of sites with bound myosin-S1 as a function of their affinities. Published S1 binding curves to regulated filaments with different tropomyosin isoforms are fitted by varying the binding constant, chain persistence length nu (in actin monomers), and chain kink energy A from a single bound S1. With skeletal tropomyosin, we find an S1 actin-binding constant of 2.2 x 10(7) M(-1), A = 1.6 k(B)T and nu = 2.7. Similar persistence lengths are found with yeast tropomyosin. Larger values are found for tropomyosin-troponin in the presence of calcium (nu = 3.7) and tropomyosins from smooth muscle and fibroblasts (nu = 4.5). The relationship of these results to structural information and the rigid-unit model of McKillop and Geeves is discussed.

Actins↗

Cooperative regulation of myosin-actin interactions by a continuous flexible chain II: actin-tropomyosin-troponin and regulation by calcium.

The model of myosin regulation by a continuous tropomyosin chain is generalized to a chain of tropomyosin-troponin units. Myosin binding to regulated actin is cooperative and initially inhibited by the chain as before. In the absence of calcium, myosin is further inhibited by the binding of troponin-I to actin, which through the whole of troponin pins the tropomyosin chain in a blocking position; myosin and TnI compete for actin and induce oppositely-directed chain kinks. The model predicts equilibrium binding curves for myosin-S1 and TnI as a function of their first-order affinities K(S1) and L(TI). Myosin is detached by the actin binding of TnI, but TnI is more efficiently detached by myosin when the kink size (typically nine to ten actin sites) spans the seven-site spacing between adjacent TnI molecules. An allosteric mechanism is used for coupling the detachment of TnI to calcium binding by TnC. With thermally activated TnI kinks (kink energy B approximately k(B)T), TnI also binds cooperatively to actin, producing cooperative detachment of myosin and biphasic myosin-calcium Hill plots, with Hill coefficients of 2 at high calcium and 4-6 at low calcium as observed in striated muscle. The theory also predicts the cooperative effects observed in the calcium loading of TnC.

Actins↗

Ionic interactions play a role in the regulatory mechanism of scallop heavy meromyosin.

Heavy meromyosin from scallop (scHMM) striated muscle is regulated by calcium binding to the essential light chain. The regulation can be modeled with a calcium-dependent equilibrium between on and off scHMM conformations. The observed rate constant for mant-ADP dissociation from scHMM is calcium dependent, and we show here that it can be used to define the equilibrium constant (K(eq)) between on and off conformations. The data show that K(eq) is markedly ionic strength dependent, with high salt (>/=200 mM) abolishing the off state even in the absence of calcium and low salt (<50 mM) favoring the off state even in the presence of calcium. Debye-Huckel plots of the equilibrium constant (K(eq)) for the on and off forms gave parallel slopes (5.94 +/- 0.33 and 6.36 +/- 0.17 M(-0.5)) in the presence and absence of calcium. The presence of an equilibrium mixture of two conformations was confirmed by sedimentation data and the effects of ADP, calcium and ionic strength were in qualitative agreement. Thus scHMM exists in two conformations that can be distinguished in sedimentation profiles and by the rate of release of mant-ADP. Increasing salt concentrations biases the system toward the on state, suggesting a role for ionic interactions in stabilizing the off state.

Adenosine Diphosphate↗

Kinetic resolution of a conformational transition and the ATP hydrolysis step using relaxation methods with a Dictyostelium myosin II mutant containing a single tryptophan residue.

The fluorescence emission intensity from a conserved tryptophan residue (W501) located in the relay loop (F466 to L516) of the Dicytostelium discoideum myosin II motor domain is sensitive to ATP binding and hydrolysis. The initial binding process is accompanied by a small quench in fluorescence, and this is followed by a large enhancement that appears coincident with the hydrolysis step. Using temperature and pressure jump methods, we show that the enhancement process is kinetically distinct from but coupled to the hydrolysis step. The fluorescence enhancement corresponds to the open-closed transition (k(obs) approximately 1000 s(-1) at 20 degrees C). From the overall steady-state fluorescence signal and the presence or absence of a relaxation transient, we conclude that the ADP state is largely in the open state, while the ADP.AlF(4) state is largely closed. At 20 degrees C the open-closed equilibria for the AMP.PNP and ADP.BeF(x) complexes are close to unity and are readily perturbed by temperature and pressure. In the case of ATP, the equilibrium of this step slightly favors the open state, but coupling to the subsequent hydrolysis step gives rise to a predominantly closed state in the steady state. Pressure jump during steady-state ATP turnover reveals the distinct transients for the rapid open-closed transition and the slower hydrolysis step.

Adenosine Triphosphate↗

Differing ADP release rates from myosin heavy chain isoforms define the shortening velocity of skeletal muscle fibers.

To understand mammalian skeletal myosin isoform diversity, pure myosin isoforms of the four major skeletal muscle myosin types (myosin heavy chains I, IIA, IIX, and IIB) were extracted from single rat muscle fibers. The extracted myosin (1-2 microg/15-mm length) was sufficient to define the actomyosin dissociation reaction in flash photolysis using caged-ATP (Weiss, S., Chizhov, I., and Geeves, M. A. (2000) J. Muscle Res. Cell Motil. 21, 423-432). The ADP inhibition of the dissociation reaction was also studied to give the ADP affinity for actomyosin (K(AD)). The apparent second order rate constant of actomyosin dissociation gets faster (K(1)k(+2) = 0.17 -0.26 microm(-1) x s(-1)), whereas the affinity for ADP is weakened (250-930 microm) in the isoform order I, IIA, IIX, IIB. Both sets of values correlate well with the measured maximum shortening velocity (V(0)) of the parent fibers. If the value of K(AD) is controlled largely by the rate constant of ADP release (k(-AD)), then the estimated value of k(-AD) is sufficiently low to limit V(0). In contrast, [ATP]K(1)k(+2) at a physiological concentration of 5 mm ATP would be 2.5-6 times faster than k(-AD).

Adenosine Diphosphate↗

Regulatory properties of tropomyosin effects of length, isoform, and N-terminal sequence.

The regulatory properties of naturally occurring tropomyosins (Tms) of differing lengths have been examined. These Tms span from 4 to 7 actin subunits. Native proteins have been used to study the common 7 actin-spanning skeletal and smooth muscle variants and expressed recombinant proteins to study the shorter fibroblast 5a, 5b, yeast Tm1 and yeast Tm2 Tms (6, 6, 5, and 4 actin-spanning variants, respectively). The yTm2 has been overexpressed in Escherichia coli with N-terminal constructs equivalent to those previously used for yTm1 [Maytum, R., et al. (2000) Biochemistry 39, 11913]. The regulation of myosin subfragment 1 (S1) binding to actin by Tm has been assessed using a sensitive S1 binding titration. The equilibrium between closed and open (C to M states, KT = 0.1-0.14) was similar for all vertebrate Tms. Apart from skTm where the apparent cooperative unit size (n) is the same as the structural size (n = 7 actin sites), the other vertebrate Tms that were studied exhibited large n values (n = 12-14). The yeast Tms also exhibited large values of n (6-9) in comparison to their structural sizes (4-5). The determined value of KT depended on the N-terminal sequence (KT = 0.15-1). These results are compared with the effect of S1 upon Tm's affinity for actin. The yeast Tms have regulatory parameters similar to those of skTm, but unlike skTm, S1 has little effect upon their actin affinity. This shows that an actin state with a high affinity for S1 and Tm is not necessary for regulation, and the higher affinity of S1 for actin in the presence of vertebrate Tms is probably the result of a direct interaction of S1 with Tm.

Actins↗

ADP binding induces an asymmetry between the heads of unphosphorylated myosin.

Light chain phosphorylation is the key event that regulates smooth and non-muscle myosin II ATPase activity. Here we show that both heads of smooth muscle heavy meromyosin (HMM) bind tightly to actin in the absence of nucleotide, irrespective of the state of light chain phosphorylation. In striking contrast, only one of the two heads of unphosphorylated HMM binds to actin in the presence of ADP, and the heads have different affinities for ADP. This asymmetry suggests that phosphorylation alters the mechanical coupling between the heads of HMM. A model that incorporates strain between the two heads is proposed to explain the data, which have implications for how one head of a motor protein can gate the response of the other.

Actins↗

Overexpression of human cardiac troponin in Escherichia coli: its purification and characterization.

All three subunits of the human cardiac troponin complex (cTn), namely the major isoform of the tropomyosin binding subunit (hcTnT3), the inhibitory subunit (cTnI), and the calcium binding subunit (cTnC), have been coexpressed in Escherichia coli. The cDNAs of each subunit have been cloned into the pSBET vector and transformed into E. coli. The coexpressed subunits assembled within the bacterial cells to form the hcTn complex (hcTnT3.hcTnI.hcTnC). The complex was isolated and purified by three chromatographic steps. Per 6-L cell culture about 10 mg of a highly purified troponin complex showing the expected 1:1:1 molar ratio of hcTnT3:cTnI:cTnC was obtained. Upon phosphorylation by protein kinase A at Ser22 and Ser23 in cTnI, this recombinant troponin complex shows a nearly identical (31)P NMR spectrum to the native one isolated from bovine heart. By measuring the rate of myosin S1 binding to reconstituted thin filaments it was shown that the dependence of the regulation of S1 binding upon calcium concentration and bisphosphorylation was comparable to the native complex.

Amino Acid Sequence↗

Actomyosin regulatory properties of yeast tropomyosin are dependent upon N-terminal modification.

The yeast tropomyosin 1 gene (TPM1) encodes the major isoform of the two tropomyosins (Tm) found in yeast. The gene has been expressed in E. coli and the protein purified. The gene product (yTm1) is a 199-amino acid protein that has a low affinity for actin compared to the native yTm1 purified from yeast. Mass spectrometry shows that the native protein is acetylated while the recombinant protein is not. A series of yTm1 N-terminal constructs were made with either an Ala-Ser dipeptide extension previously shown to restore actin binding to skeletal muscle Tm or the natural extension found in fibroblast Tm 5a/b. All constructs bound actin tightly and showed similar CD spectra and thermal stability. All constructs induced cooperativity in the equilibrium binding of myosin subfragment 1, to actin but the binding curves differed significantly between the constructs. The apparent cooperative unit size (n) and closed/open equilibrium (K(T)) were determined using a fluorescence titration technique [Maytum et al. (1998) Biophys. J. 74, A347]. The data could be accounted for by changes in K(T) (0.1-1) with no change in n. Values of n were approximately twice the structural unit size (5 actin sites). The presence of yTm on actin had little effect upon the overall affinity of S1 for actin despite showing an ability to regulate the acto-myosin interaction. These results show that the short yTm can aid our understanding of actomyosin regulation and that the N-terminus of Tm has a major influence upon its regulatory properties.

Actomyosin↗

Stabilization of the actomyosin complex by negative charges on myosin.

Sequence comparisons of members of the myosin superfamily show a high degree of charge conservation in a surface exposed helix (Dictyostelium discoideum myosin II heavy chain residues S510 to K546). Most myosins display a triplet of acidic residues at the equivalent positions to D. discoideummyosin II residues D530, E531, and Q532. The high degree of charge conservation suggests strong evolutionary constrain and that this region is important for myosin function. Mutations at position E531 were shown to strongly affect actin binding [Giese, K. C., and Spudich, J. A. (1997) Biochemistry 36, 8465-8473]. Here, we used steady-state and transient kinetics to characterize the enzymatic competence of mutant constructs E531Q and Q532E, and their properties were compared with those of a loop 2 mutant with a 20 amino acid insertion containing 12 positive charges (20/+12) [Furch et al. (1998) Biochemistry 37, 6317-6326], double mutant Q532E(20/+12), and the native motor domain constructs. Our results confirm that charge changes at residues 531 and 532 primarily affect actin binding with little change being communicated to the nucleotide pocket. Mutation D531Q reduces actin affinity (K(A)) 10-fold, while Q532E leads to a 5-fold increase. The observed changes in K(A)() stem almost exclusively from variations in the dissociation rate constant (k(-A)), with the introduction of a single negative charge at position 532 having the same effect on k(-A) as the introduction of 12 positive charges in the loop 2 region.

Actins↗

Tropomyosin and actin isoforms modulate the localization of tropomyosin strands on actin filaments.

Tropomyosin is present in virtually all eucaryotic cells, where it functions to modulate actin-myosin interaction and to stabilize actin filament structure. In striated muscle, tropomyosin regulates contractility by sterically blocking myosin-binding sites on actin in the relaxed state. On activation, tropomyosin moves away from these sites in two steps, one induced by Ca(2+) binding to troponin and a second by the binding of myosin to actin. In smooth muscle and non-muscle cells, where troponin is absent, the precise role and structural dynamics of tropomyosin on actin are poorly understood. Here, the location of tropomyosin on F-actin filaments free of troponin and other actin-binding proteins was determined to better understand the structural basis of its functioning in muscle and non-muscle cells. Using electron microscopy and three-dimensional image reconstruction, the association of a diverse set of wild-type and mutant actin and tropomyosin isoforms, from both muscle and non-muscle sources, was investigated. Tropomyosin position on actin appeared to be defined by two sets of binding interactions and tropomyosin localized on either the inner or the outer domain of actin, depending on the specific actin or tropomyosin isoform examined. Since these equilibrium positions depended on minor amino acid sequence differences among isoforms, we conclude that the energy barrier between thin filament states is small. Our results imply that, in striated muscles, troponin and myosin serve to stabilize tropomyosin in inhibitory and activating states, respectively. In addition, they are consistent with tropomyosin-dependent cooperative switching on and off of actomyosin-based motility. Finally, the locations of tropomyosin that we have determined suggest the possibility of significant competition between tropomyosin and other cellular actin-binding proteins. Based on these results, we present a general framework for tropomyosin modulation of motility and cytoskeletal modelling.

Actin Cytoskeleton↗

Inhibition of actin-myosin subfragment 1 ATPase activity by troponin I and IC: relationship to the thin filament states of muscle.

Troponin I (TnI) is the component of the troponin complex that inhibits actomyosin ATPase activity, and Ca(2+) binding to the troponin C (TnC) component reverses the inhibition. Effects of the binding of TnI and the TnI-TnC (TnIC) complex to actin-tropomyosin (actinTm) on ATPase and on the binding kinetics of myosin subfragment 1 (S1) were studied to clarify the mechanism of the inhibition. TnI and TnIC in the absence of Ca(2+) bind to actinTm and inhibit ATPase to similar levels with a stoichiometry of one TnI or one TnIC per one Tm and seven actin subunits. TnI also binds to actinTmTn in the presence of Ca(2+) with a stoichiometry and inhibition constant similar to those for the binding to actinTm of TnI and Tn in the absence of Ca(2+). Thus, in the presence of Ca(2+), the intrinsic TnI which is released from its binding site on actinTm does not interfere with the binding of an extra molecule of TnI to actinTmTn. The rate of S1 binding to actinTmTnI and to actinTmTnTnI in the presence of Ca(2+) was inhibited to the same extent as upon removal of Ca(2+) from actinTmTn. These studies show that TnI inhibits ATPase by the same mechanism as Tn in the absence of Ca(2+), by shifting the thin filament equilibria from the open state to the closed and blocked states.

Actin Cytoskeleton↗

Kinetic analyses of a truncated mammalian myosin I suggest a novel isomerization event preceding nucleotide binding.

MI(1IQ) is a complex of calmodulin and an epitope-tagged 85-kDa fragment representing the amino-terminal catalytic motor domain and the first of 6 calmodulin-binding IQ domains of the mammalian myosin I gene, rat myr-1 (130-kDa myosin I or MI(130)). We have determined the transient kinetic parameters that dictate the ATP hydrolysis cycle of mammalian myosin I by examining the properties of MI(1IQ). Transient kinetics reveal that the affinity of MI(1IQ) for actin is 12 nm. The ATP-induced dissociation of actin-MI(1IQ) is biphasic. The fast phase is dependent upon [ATP], whereas the slow phase is not; both phases show a Ca(2+) sensitivity. The fast phase is eliminated by the addition of ADP, 10 micrometer being required for half-saturation of the effect in the presence of Ca(2+) and 3 micrometer ADP in the absence of Ca(2+). The slow phase shares the same rate constant as ADP release (8 and 3 s(-)(1) in the presence and absence of Ca(2+), respectively), but cannot be eliminated by decreasing [ADP]. We interpret these results to suggest that actin-myosin I exists in two forms in equilibrium, one of which is unable to bind nucleotide. These results also indicate that the absence of the COOH-terminal 5 calmodulin binding domains of myr-1 do not influence the kinetic properties of MI(130) and that the Ca(2+) sensitivity of the kinetics are in all likelihood due to Ca(2+) binding to the first IQ domain.

Actins↗

The structural basis of muscle contraction.

The myosin cross-bridge exists in two conformations, which differ in the orientation of a long lever arm. Since the lever arm undergoes a 60 degree rotation between the two conformations, which would lead to a displacement of the myosin filament of about 11 nm, the transition between these two states has been associated with the elementary 'power stroke' of muscle. Moreover, this rotation is coupled with changes in the active site (CLOSED to OPEN), which probably enable phosphate release. The transition CLOSED to OPEN appears to be brought about by actin binding. However, kinetics shows that the binding of myosin to actin is a two-step process which affects both ATP and ADP affinity and vice versa. The structural basis of these effects is only partially explained by the presently known conformers of myosin. Therefore, additional states of the myosin cross-bridge should exist. Indeed, cryoelectron microscopy has revealed other angles of the lever arm induced by ADP binding to a smooth muscle actin-myosin complex.

Actins↗

A flash photolysis fluorescence/light scattering apparatus for use with sub microgram quantities of muscle proteins.

Transient kinetic methods such as stopped flow and quenched flow have been used to elucidate many of the fundamental features of the molecular interactions which underlie muscle contraction. However, these methods traditionally require relatively large amounts of protein (10(-3) g) and so have been used most effectively for the proteins purified from bulk muscle tissue of large animals or where the proteins can be expressed in large amounts (e.g.. Dictyostelium). We have investigated the use of flash photolysis of an inert precursor of ATP (cATP) to initiate the dissociation of acto.S1 and acto.myosin and the subsequent ATP turnover reaction. Using a sample volume of 10 microl we show that a significant amount of information on the transient and steady-state kinetics of the system can be obtained from a sample containing just 50 nM of acto.myosin or acto.S1 complex in solution. Therefore in presence of excess of one protein component the measurements require only 250 ng myosin, 62 ng S1 or 25 ng actin. This is therefore the method of choice for kinetic analysis of acto.myosins which are only available in microgram quantities. We report for the first time the determination of the second order rate constant of ATP-induced dissociation of actin from the myosin extracted from a single fibre from a rabbit psoas muscle.

Actins↗

Actin residue glu(93) is identified as an amino acid affecting myosin binding.

Many mutants have been described that affect the function of the actin encoded by the Drosophila melanogaster indirect flight muscle-specific actin gene, Act88F. We describe the development of procedures for purification of this actin from the other isoforms expressed in the fly as well as in vitro motility, single molecule force/displacement measurements, and stop-flow solution kinetic studies of the wild-type actin and that of the E93K mutation of the Act88F gene. We show that this mutation affects in vitro motility of F-actin, in both the presence and absence of methylcellulose, and the ability of the ACT88F actin to bind the S1 fragment of rabbit skeletal myosin. However, optical tweezer measurements of the actomyosin working stroke and the force transmitted from the rabbit heavy meromyosin to and through F-actin are unchanged by the mutation. These results support the proposal (Holmes, K. C. (1995) Biophys J. 68, (suppl.) 2-7) that actin residue Glu(93) is part of the secondary myosin binding site and suggest that myosin binding occurs first at the primary myosin binding site and then at the secondary site.

Actins↗