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A Holtzer

Publications and source records attributed to A Holtzer.

At least 37 records · Page 2Linked to original sources
PubMed1992

Kinetics of folding of alpha alpha-tropomyosin subsequences.

The kinetics of folding random coils of alpha alpha-tropomyson (Tm) subsequences to two-chain coiled coils was studied by stopped-flow CD. Subsequences studied were those comprising residues 11-127 (11Tm127), 142-281 (142Tm281), 1-189 (1Tm189), and 190-284 (190Tm284) of the parent 284-residue alpha-tropomyosin chain. Unlike the parent, subsequences 1Tm189 and 11Tm127 fold within the dead time of the instrument (less than 0.04 s). Like the parent, subsequences 142Tm281 and 190Tm284 fold in two phases. In the fast phase, 45% and 32%, respectively, of the equilibrium helical content form. In the time-resolvable, first-order slow phase (k-1 = 2.7 s at 20 degrees C for 142Tm281 and k-1 = 2.0 s at 15 degrees C for 190Tm284), the remaining structure forms. Neither reduced 142Tm281 nor 190Tm284 show any dependence of the rate on concentration, so chain association occurs in the fast phase. Like the parent 142Tm281 forms more helical content in the fast phase when cross-linked at C-190, and the remaining structure forms slowly with rate parameters similar to those of the reduced species. Comparison of the folding behavior of C- and N-terminal subsequences with that of the parent protein suggests that the slow phase in the parent is caused by a folding bottleneck somewhere nearer the C-terminus. However, rapid association and partial folding near the N-terminus is not necessary for prompt folding, since even 190Tm284 chains associate and partially fold very rapidly (less than 0.04 s), and then complete the folding in seconds.

Animals↗
PubMed1992

Kinetics of folding and unfolding of beta beta-tropomyosin.

The kinetics of folding from random coils to two-chain coiled coils of beta beta-tropomyosin was studied by stopped-flow CD (SFCD) in the backbone region (222 nm). Two species were studied: the reduced form and the doubly disulfide cross-linked form. The proteins were totally unfolded in 6M urea-saline buffer, then refolded by tenfold dilution into benign buffer. In the refolding medium, they spontaneously recover the two-chain coiled-coil structure. Reduced beta beta refolds in at least two stages: one or more fast phases (< 0.04 s), in which an intermediate with 71% of the equilibrium ellipticity forms, followed by a slower time-resolvable phase that completes the folding. The slow phase is first order, signifying that dimerization occurs in the fast phase. The time constant of the slow phase is 2 s at 20 degrees C and requires activation parameters of delta S not equal to = -7 +/- 0.3 cal/mol.K, delta H not equal to = 15 +/- 1 kcal/mol. These results are very similar to those previously found for the reduced genetic variant alpha alpha-tropomyosin. In contrast, refolding of doubly disulfide cross-linked beta beta is complete within the dead time (< 0.04 s), whereas the singly cross-linked alpha alpha species also displays a slow phase. The opposite process, unfolding reduced beta beta from the coiled-coil state, is complete within the dead time, as in the alpha alpha variant.

Animals↗
PubMed1992

Alpha-helix to random coil transitions: determination of peptide concentration from the CD at the isodichroic point.

A method is presented for determining the concentrations of peptides and proteins having isodichroic points near 203 nm. The existence of an isodichroic point for a given substance indicates a local two-state (alpha-helix, random coil) population. The mean residue ellipticity at the isodichroic point, [theta lambda i], is, of course, independent of helix content. For a wide variety of synthetic and natural peptides, including both single helices and coiled coils, it is shown that [theta lambda i] is also essentially independent of substance and of whether the transition is induced by temperature, ionic strength, pH, chain length changes, amino acid substitution, or solvent perturbation. Averaging [theta lambda i] values culled from various laboratories gives -151 +/- 16 (SD, 7 sources) deg.cm2.mmol-1. In our laboratory, nonpolymerizable rabbit alpha-tropomyosin and two alpha-tropomyosin subsequences yield -135 +/- 10 (SD, 190 values) deg.cm2.mmol-1. Thus, given [theta lambda i] for a peptide of known concentration, it is possible to estimate the concentration of any other peptide provided that it has an isodichroic point at which the ellipticity is accurately measurable. It is then possible to calculate [theta lambda] at any other wavelength for which theta is known. It is advisable to determine [theta lambda i] for the best known peptide in one's own laboratory, since it depends on absolute instrument and cell calibrations and an absolute concentration determination.

Amino Acid Sequence↗
PubMed1992

Beta beta homodimers exist in native rabbit skeletal muscle tropomyosin and increase after denaturation-renaturation.

Native tropomyosin from rabbit skeletal muscle (RSTm) consists mainly of alpha alpha and alpha beta coiled coils (alpha/beta approximately 3-4/1). In some extant studies, no beta beta molecules have been found. In this study, RSTm from several different preparations was disulfide cross-linked, both preparation and cross-linking being done under nondenaturing conditions. The cross-linked product was assayed for the presence of beta beta molecules cross-linked at both C36 and C190 (beta = beta). In such cross-linked RSTm, 3-8% beta = beta is detected by sodium dodecyl sulfate polyacrylamide gel electrophoresis, C4 reversed-phase high-performance liquid chromatography, and a free-solution capillary electrophoresis experiment. This percentage becomes approximately 4-10% beta beta when corrected for incomplete double cross-linking and is independent of protein concentration (0.1-10.0 mg/mL), indicating that the observed beta beta species are not artifacts due to intermolecular cross-linking. Upon denaturation and subsequent renaturation either by heating to 55 degrees C or by incubating at 45 degrees C followed by quenching to room temperature, or by guanidine hydrochloride exposure followed by phased renaturation by dialysis, the fraction of beta beta increases, indicating that the reassociation favors homodimer formation somewhat over random association. This result differs from the random association observed when the sulfhydryl on one of the chains is carboxyamidomethylated (Holtzer, M.E., Breiner, T., & Holtzer, A., 1984, Biopolymers 23, 1811-1833), and from the overwhelming heterodimer preferences reported for tropomyosins from other organisms (Lehrer, S.S., Qian, Y., & Hvidt, S., 1989, Science 246, 926-928; Lehrer, S.S. & Qian, Y., 1990, J. Biol. Chem. 265, 1134-1138).

Animals↗
PubMed1991

Kinetics of folding and unfolding of alpha alpha-tropomyosin and of nonpolymerizable alpha alpha-tropomyosin.

Stopped flow CD (SFCD) kinetic studies of self-assembly of coiled coils of rabbit alpha alpha-tropomyosin and of nonpolymerizable alpha alpha-tropomyosin (NPTm) are reported. The protein was denatured in 6 M urea buffer, then renatured by 10-fold dilution into benign saline buffer. Folding was monitored by SFCD in the backbone region (222 nm). Protein chains are shown to be totally unfolded (and separated in the reduced species) in the initial denaturing medium and fully folded as two-chain coiled coils in the final benign medium. In all cases of folding in benign buffer of totally unfolded chains, two phases were found in the folding process: a fast phase (less than 0.04 s, the SFCD dead time), in which an intermediate state with about 70% of the equilibrium ellipticity forms; followed by a slower, observable phase that completes the folding. The slow phase is first order (k-1 = 1.6 s at 20 degrees C), signifying that chain association for reduced samples occurs in the fast phase. In contrast, folding in benign buffer from an initial state with 70% of the equilibrium ellipticity is all fast, suggesting that the folding intermediate is not an equilibrium species. Cross-linking at Cys-190 increases the helix content of the fast-formed intermediate state to about 85% of the equilibrium value, but leaves the rate constant of the slow phase unchanged. In NPTm, which does not form high aggregates at low ionic strength, the rate of the observable phase is almost independent of ionic strength in the range of approximately 0.15-0.6 M, but is reduced one to two orders of magnitude by further reduction to 0.026 M. In folding from totally unfolded chains, the rate is reduced less than one order of magnitude by changing the final state to about 50% folded. In contrast to folding, unfolding of alpha alpha-tropomyosin from the native state is all fast.

Animals↗
PubMed1991

Kinetics of self-assembly of alpha alpha-tropomyosin coiled coils from unfolded chains.

The two-chain coiled-coil structural motif is found in fibrous muscle proteins and leucine zippers. Unfolding/refolding studies abound, but none establishes the time scale or mechanism of structural assembly from separated, unfolded chains. Stopped-flow circular dichroism studies of such refolding of alpha-tropomyosin chains are reported here. The backbone spectral region (222 nm) reveals a fast phase (less than 0.04 s), yielding an intermediate possessing approximately 70% of the equilibrium helix content. A subsequent slow phase is first order [k-1 (20 degrees C) = 1.67 s, Ea = 12.7 kcal.mol-1 (1 kcal = 4.18 kJ)], so dimerization is fast. The same rate constant characterizes folding in the Cys-190 crosslinked chains, so the intermediate has parallel and nearly registered chains. The tyrosine spectral region (280 nm) reveals only a fast phase, so these six chain sites are native in the intermediate.

Animals↗
PubMed1991

A scanning calorimetric study of the thermally induced unfolding of various forms of tropomyosin.

The reversible thermally induced unfolding of various forms of tropomyosin, a two-chain alpha-helical coiled coil, has been studied by high-sensitivity differential scanning calorimetry (DSC). Included in the study are the reduced and oxidized (disulfide cross-linked) forms of alpha alpha- and beta beta-tropomyosin, and the forms of alpha alpha-tropomyosin in which all sulfhydryl groups have been blocked by carboxymethylation or carboxyamidomethylation. Oxidation or blocking of the sulfhydryl groups of tropomyosin strongly affect the thermotropic behavior of the protein in unpredictable ways. The empirical results presented here are in qualitative agreement with those from an earlier DSC study of the oxidized and carboxymethylated forms of alpha alpha-tropomyosin [S.A. Potekhin and P.L. Privalov (1982) Journal of Molecular Biology, Vol. 159, pp. 519-535], but we find that a different decomposition into subtransitions is possible. Comparison of the alpha alpha and beta beta species indicates, in agreement with extant CD studies, that the noncross-linked beta beta species is somewhat less stable than its alpha alpha counterpart, but that cross-linking enhances the stability of the beta beta doubly cross-linked species by a greater amount and does not lead to the small low-temperature transition ("pretransition") seen in the singly cross-linked alpha alpha species.

Calorimetry, Differential Scanning↗
PubMed1991

The kinetics of chain exchange in two-chain coiled coils: alpha alpha- and beta beta-tropomyosin.

Measurements are presented on the time course of chain exchange among two-chain alpha-helical coiled coils of rabbit tropomyosin. All experiments are in a regime (temperature, protein concentration) in which coiled-coil dimers are the predominant species. Self-exchange in alpha alpha-tropomyosin was investigated by mixing alpha alpha species with alpha* alpha*, the asterisk designating an alpha-chain whose lone sulfhydryl (C190) has been blocked by carboxyamidomethylation. The overall process alpha alpha + alpha* alpha* in equilibrium with 2 alpha alpha* is followed by measurement of the fraction (h) of alpha alpha* species as a function of time. Similarly, self-exchange in beta beta-tropomyosin is examined by measurements of the overall process: beta beta + beta* beta* in equilibrium with 2 beta beta*, in which beta* signifies a beta-chain blocked at both sulfhydryls (C36 and C190). The observed time course for both chains is well fit by the first-order equation: h (t) = h (infinity) (1-e-k1t), with h (infinity) congruent to 0.5. This long-time limit is as expected for self-exchange, and agrees with experiments that attain equilibrium after slow cooling of thermally dissociated and unfolded chains. The simplest consonant mechanism is chain exchange by rate-limiting dissociation of dimers followed by random reassociation. Kinetic analysis shows k1 to be the rate constant for the chain dissociation step, a quantity not previously measured for any coiled coil. This rate constant for beta beta species is about an order of magnitude greater than for alpha alpha. In both, the activation enthalpy and entropy are very large, suggesting that activation to an extensively (greater than 50%) unfolded species necessarily precedes dissociation. Experiments are also reported for overall processes: alpha alpha + beta* beta* in equilibrium with 2 alpha beta* and alpha* alpha* + beta beta in equilibrium with 2 alpha* beta. Results are independent of which chain is blocked. Again h (infinity) congruent to 0.5, in agreement with equilibrium experiments, and the time course is first order. The rate constants and activation parameters are intermediate between those for self-exchange.

Animals↗
PubMed1990

The effect of sulfhydryl blocking groups on the thermal unfolding of alpha alpha tropomyosin coiled coils.

Equilibrium thermal unfolding curves from circular dichroism are given for alpha alpha tropomyosin and for alpha alpha tropomyosin blocked at C190 by a) carboxyamidomethylation; b) carboxymethylation. Although commonly assumed to be benign, these blocks in fact produce some weakening. All three substances are virtually completely alpha-helical at low T. Fraction helix vs T for parent protein is apparently monophasic (single inflection point). The curve for carboxyamidomethylated protein is very close to that of the parent, but is biphasic, with a small "pretransition". The curve for carboxymethylated protein is prominently biphasic, with a much larger pretransition. Some implications for the molecular model of these equilibria are discussed.

Iodoacetamide↗
PubMed1990

The thermal denaturation of nonpolymerizable alpha alpha-tropomyosin and its segments as a function of ionic strength.

Nonpolymerizable tropomyosin (NPTm) is found to unfold thermally at high ionic strength almost exactly as the parent protein, but it does not aggregate at low ionic strength. Thus, NPTm can be used as a tropomyosin surrogate whose coiled-coil structural stability can be probed by varying the ionic strength. Studies of NPTm by CD show that increasing ionic strength stabilizes the coiled-coil structure. CD spectra over a wide range of helix content, obtained by varying either temperature or ionic strength, show an isodichroic point at 203 nm, suggesting a local, residue-level, two-state model. At given temperature, such a local helix in equilibrium random equilibrium suggests ln [phi h/(1-phi h)] = A1 + A2In, wherein phi h is the fraction helix, and A1, A2, and n are constants. In the low ionic strength region, theoretical limiting laws for ionic strength mediated charge-charge, dipole-dipole, and apolar-apolar (salting out) interactions give, respectively, n = 0.5, 1.0, and 1.0. Our experimental values for 40 degrees C, where the data span a wide range of helix content, show n = 1.0, suggesting that ionic strength stabilizes either by reducing dipole-dipole repulsions or by enhancing hydrophobic interactions, both probably interhelix in nature. Two segments of tropomyosin, 11Tm127 and 142Tm281, neither of which aggregate at low ionic strength, give results similar to those for NPTm, i.e., n = 0.96 and 0.84, respectively.

Osmolar Concentration↗
PubMed1990

Alpha-helix to random coil transitions of two-chain coiled coils: experiments on the thermal denaturation of isolated segments of alpha alpha-tropomyosin.

Circular dichroism (CD) experiments in the backbone (200-240 nm) region are reported for four isolated, excised two-chain, coiled-coil segments whose chains comprise, respectively, residues 11-127, 142-281, 1-189, and 190-284 of the rabbit alpha alpha-tropomyosin (Tm) sequence. The uv and CD spectra for the noncross-linked segments are very similar to those for parent Tm. At 3 degrees C, all have a helix content of 90% or more; moreover, all thermal denaturation curves depend on concentration, as required by mass action, and are completely reversible. At comparable concentrations, solutions show values of T1/2 (the temperature at which the helix content is 50%) following the order of 11Tm127 approximately 1Tm189 greater than 142Tm281 greater than 190Tm284. The thermal unfolding data for 11Tm127, 190Tm284, and 142Tm281 fall on apparently monophasic curves (single inflection point). However, curves for 1Tm189 show a heretofore unknown low temperature transition in which the helix content drops from approximately 90% at 2 degrees C to approximately 73% at 20 degrees C, indicating that this segment has one or more weak sections totaling approximately 50 residues per chain. Since thermal denaturation curves for noncross-linked 11Tm127, 142Tm281, and Tm have no such low temperature transition, i.e., the helix content is not additive, the weak region probably comprises the bulk of the residues between 127 and 189 in 1Tm189, but is somehow stabilized in 142Tm281 and in parent Tm.(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗
PubMed1990

Alpha-helix to random-coil transitions of two-chain coiled coils: the use of physical models in treating thermal denaturation equilibria of isolated subsequences of alpha alpha-tropomyosin.

Two extant models of thermal folding/unfolding equilibria in two-chain, alpha-helical coiled coils are tested by comparison with experimental results on excised, isolated subsequences of rabbit alpha alpha-tropomyosin (Tm). These substances are designated iTmj where i and j are, respectively, the residue numbers (in the 284-residue parent chain) of the N- and C-terminal residues of the subsequence. One model postulates that a coiled coil consists of segments, each denaturing in an all-or-none manner, like small globular proteins. Thus this model yields a small number of populated molecular species. In an extant calorimetry study of 11Tm127 and of 190Tm284, each required only two all-or-none-segments, and their enthalpies and transition temperatures were assigned. These assignments are shown here to yield the concentration of all molecular species, and therefore the helix content, as a function of temperature. Such calculations for 190Tm284 are in tolerable agreement with CD experiments, but those for 11Tm127 are in gross disagreement. Thus, either the model itself or the calorimetric assignment is faculty. In the second model, all conformational states are counted and weighted, as in the Zimm-Bragg theory for single-chain polypeptides. This theory has been extended (by Skolnick) to two-chain coiled coils and is here used to fit CD data for 11Tm127, 142Tm281, and 190Tm284. The fit is tolerable for 11Tm127, good for 142Tm281, and quantitative for 190Tm284. Thus this comparison does not falsify this second model. The helix-helix interaction free energy, obtainable from the fit, shows nonadditivity when isolated subsequences are compared with the parent. This suggests that removal of a region from a long coiled coil allows energetically substantial adjustments in side-chain packing in the helix-helix interface. Thus, the helix-helix interaction in long coiled coils is characteristic of a global free energy minimum and not just of the regional constellation of side chains.

Amino Acid Sequence↗
PubMed1989

The CD of two-chain coiled coils: experiments on tropomyosin and tropomyosin segments in the tyrosine/disulfide spectral region.

CD experiments are reported for several coiled-coil species in the tyrosine/disulfide (approximately 250-350-nm) region. Intact noncross-linked tropomyosin (approximately 3 degrees C) shows a negative nonsymmetric band maximal at 280 nm. This spectrum is the sum over six tyrosines/chain, and has conformational significance, since it disappears on denaturation. Experiments on an excised coiled-coil segment, each of whose chains comprise residues 11-127 of the tropomyosin sequence and only one tyrosine (Y60), reveal that not all tyrosines are alike. The spectrum at 3 degrees C shows a small negative maximum at approximately 285 nm and a substantial, hitherto unknown, positive band at approximately 270 nm, the latter masked in the parent protein by the negative contribution from the other tyrosines. A noncross-linked coiled-coil segment comprising residues 142-281, in which Y60 is absent, shows no such positive band. This peculiarity of Y60 is confirmed by absorbance spectra, with the extinction coefficient of Y60 larger in benign media than the average of the other tyrosines. Intact (3 degrees C) C190 cross-linked tropomyosin is known to yield, besides tyrosine contributions, a positive maximum at approximately 300 nm. Subtracting the corresponding data for noncross-linked tropomyosin shows that the disulfide spectrum itself actually has two equal, partly resolved bands at, respectively, 250 and 280 nm. The existence of a chiral disulfide argues for a relatively rigid, perhaps strained, local coiled coil. A C190 cross-linked segment comprising residues 142-281 shows a chiral disulfide spectrum like tropomyosin's, but another segment, comprising residues 168-284, shows none; thus removal of residues 142-167 causes loss of chirality at C190, over 20 residues away. These spectra thus contain important information on the subtle local differences in coiled-coil structures.

Animals↗
PubMed1986

A theoretical model simulating the anomalous concentration dependence of the equilibrium thermal unfolding curve of noncrosslinked tropomyosin.

Thermal unfolding curves of tropomyosin have so far been fit only semi-quantitatively by the statistical-mechanical theory of the helix-coil transition. The calculated values of helix content are a bit too small for the most dilute solutions and a bit too large for the most concentrated ones. The theory, as hitherto used, assumes a uniform helix-helix interaction, whereas evidence from studies on molecular segments suggests otherwise. A theoretical model incorporating such non-uniformity in helix-helix interaction is used to produce simulated thermal unfolding curves. These simulated curves, when fit to the theory using the assumption of uniformity, reveal precisely the same discrepancies seen with the experimental data. We conclude that non-uniformity in helix-helix interaction along the tropomyosin molecule is responsible for the small discrepancy between experimental data and the uniform-model theory previously employed.

Models, Theoretical↗