The mobility of troponin C and troponin I in muscle

Constructing a structural model of troponin using site-directed spin labeling: EPR and PRE-NMR

The relative ease of introducing a paramagnetic species onto a protein, and advances in electron paramagnetic resonance (EPR) over the past two decades, have established spin labeling as a vital structural biology technique for revealing the functional workings of the troponin muscle regulatory complex-an ~80 kDa heterotrimeric protein switch for turning on striated muscle contraction. Through the site-directed spin labeling (SDSL) of cysteine residues at key sites in troponin, a molecular-level understanding of the troponin muscle regulatory system across all levels of structural hierarchy has been achieved. Through the application of EPR, mobility and accessibility trends in the EPR signals of the spin labels attached to consecutive residues can reveal the secondary structure of troponin elements and also help map the interaction between subunits. Distance restraints calculated from the interspin interactions between spin label pairs have helped with building a structural model of the troponin complex. Further, when SDSL is paired with NMR, paramagnetic relaxation enhancement (PRE)-NMR has been used to obtain high-resolution structural detail for both intra- and interdomain interactions in troponin and revealed details of protein conformational changes and dynamics accompanying troponin function. In this review, we provide an overview of the SDSL labeling methodology and its application towards building a dynamic structural model of the multi-subunit troponin complex which details the calcium-induced conformational changes intimately linked to muscle regulation. We also describe how the SDSL method, in conjunction with EPR or NMR, can be used to obtain insights into structural perturbations to troponin caused by disease-causing mutations.

Slowed Dynamics of Thin Filament Regulatory Units Reduces Ca2+-Sensitivity of Cardiac Biomechanical Function

Actomyosin kinetics in both skinned skeletal muscle fibers at maximum Ca²⁺-activation and unregulated in vitro motility assays are modulated by solvent microviscosity in a manner consistent with a diffusion limited process. Viscosity might also influence cardiac thin filament Ca²⁺-regulatory protein dynamics. In vitro motility assays were conducted using thin filaments reconstituted with recombinant human cardiac troponin and tropomyosin; solvent microviscosity was varied by addition of sucrose or glucose. At saturating Ca²⁺, filament sliding speed (s) was inversely proportional to viscosity. Ca²⁺-sensitivity (pCa₅₀ ) of s decreased markedly with elevated viscosity (η/η₀ ≥ ~1.3). For comparison with unloaded motility assays, steady-state isometric force (F) and kinetics of isometric tension redevelopment (k_TR ) were measured in single, permeabilized porcine cardiomyocytes when viscosity surrounding the myofilaments was altered. Maximum Ca²⁺-activated F changed little for sucrose ≤ 0.3 M (η/η₀ ~1.4) or glucose ≤ 0.875 M (η/η₀ ~1.66), but decreased at higher concentrations. Sucrose (0.3 M) or glucose (0.875 M) decreased pCa₅₀ for F. k_TR at saturating Ca²⁺ decreased steeply and monotonically with increased viscosity but there was little effect on k_TR at sub-maximum Ca²⁺. Modeling indicates that increased solutes affect dynamics of cardiac muscle Ca²⁺-regulatory proteins to a much greater extent than actomyosin cross-bridge cycling.

Calcium structural transition of troponin in the complexes, on the thin filament, and in muscle fibres, as studied by site-directed spin-labelling EPR

We have measured the intersite distance, side-chain mobility and orientation of specific site(s) of troponin (Tn) complex on the thin filaments or in muscle fibres as well as in solution by means of site-directed spin labeling electron paramagnetic resonance (SDSL-EPR). We have examined the Ca(2+)-induced movement of the B and C helices relative to the D helix in a human cardiac (hc)TnC monomer state and hcTnC-hcTnI binary complex. An interspin distance between G42C (B helix) and C84 (D helix) was 18.4 angstroms in the absence of Ca2+. The distance between Q58C (C helix) and C84 (D helix) was 18.3 angstroms. Distance changes were observed by the addition of Ca2+ and by the formation of a complex with TnI. Both Ca2+ and TnI are essential for the full opening -3 angstroms of the N-domain in cardiac TnC. We have determined the in situ distances between C35 and C84 by measuring pulsed electron-electron double resonance (PELDOR) spectroscopy. The distances were 26.0 and 27.2 A in the monomer state and in reconstituted fibres, respectively. The addition of Ca2+ decreased the distance to 23.2 angstroms in fibres but only slightly in the monomer state, indicating that Ca2+ binding to the N-lobe of hcTnC induced a larger structural change in muscle fibres than in the monomer state. We also succeeded in synthesizing a new bifunctional spin labels that is firmly fixed on a central E-helix (94C-101C) of skeletal(sk)TnC to examine its orientation in reconstituted muscle fibres. EPR spectrum showed that this helix is disordered with respect to the filament axis. We have studied the calcium structural transition in skTnI and tropomyosin on the filament by SDSL-EPR. The spin label at a TnI switch segment (C133) showed three motional states depending on Ca2+ and actin. The data suggested that the TnI switch segment binds to TnC N-lobe in +Ca2+ state, and that in -Ca2+ state it is free in TnC-I-T complex alone while fixed to actin in the reconstituted thin filaments. In contrast, the side chain spin labels along the entire tropomyosin molecule showed no Ca(2+)-induced mobility changes.

Regulatory and catalytic domain dynamics of smooth muscle myosin filaments

Domain dynamics of the chicken gizzard smooth muscle myosin catalytic domain (heavy chain Cys-717) and regulatory domain (regulatory light chain Cys-108) were determined in the absence of nucleotides using saturation-transfer electron paramagnetic resonance. In unphosphorylated synthetic filaments, the effective rotational correlation times, tau(r), were 24 +/- 6 micros and 441 +/- 79 micros for the catalytic and regulatory domains, respectively. The corresponding amplitudes of motion were 42 +/- 4 degrees and 24 +/- 9 degrees as determined from steady-state phosphorescence anisotropy. These results suggest that the two domains have independent mobility due to a hinge between the two domains. Although a similar hinge was observed for skeletal myosin (Adhikari and Fajer (1997) Proc. Natl. Acad. Sci. U.S.A. 94, 9643-9647. Brown et al. (2001) Biochemistry 40, 8283-8291), the latter displayed higher regulatory domain mobility, tau(r)= 40 +/- 3 micros, suggesting a smooth muscle specific mechanism of constraining regulatory domain dynamics. In the myosin monomers the correlation times for both domains were the same (approximately 4 micros) for both smooth and skeletal myosin, suggesting that the motional difference between the two isoforms in the filaments was not due to intrinsic variation of hinge stiffness. Heavy chain/regulatory light chain chimeras of smooth and skeletal myosin pinpointed the origin of the restriction to the heavy chain and established correlation between the regulatory domain dynamics with the ability of myosin to switch off but not to switch on the ATPase and the actin sliding velocity. Phosphorylation of smooth muscle myosin filaments caused a small increase in the amplitude of motion of the regulatory domain (from 24 +/- 4 degrees to 36 +/- 7 degrees ) but did not significantly affect the rotational correlation time of the regulatory domain (441 to 408 micros) or the catalytic domain (24 to 17 micros). These data are not consistent with a stable interaction between the two catalytic domains in unphosphorylated smooth muscle myosin filaments in the absence of nucleotides.

Calcium-dependent movement of troponin I between troponin C and actin as revealed by spin-labeling EPR

We measured EPR spectra from a spin label on the Cys133 residue of troponin I (TnI) to identify Ca(2+)-induced structural states, based on sensitivity of spin-label mobility to flexibility and tertiary contact of a polypeptide. Spectrum from Tn complexes in the -Ca(2+) state showed that Cys133 was located at a flexible polypeptide segment (rotational correlation time tau=1.9ns) that was free from TnC. Spectra of both Tn complexes alone and those reconstituted into the thin filaments in the +Ca(2+) state showed that Cys133 existed on a stable segment (tau=4.8ns) held by TnC. Spectra of reconstituted thin filaments (-Ca(2+) state) revealed that slow mobility (tau=45ns) was due to tertiary contact of Cys133 with actin, because the same slow mobility was found for TnI-actin and TnI-tropomyosin-actin filaments lacking TnC, T or tropomyosin. We propose that the Cys133 region dissociates from TnC and attaches to the actin surface on the thin filaments, causing muscle relaxation at low Ca(2+) concentrations.

Calcium Structural Transition of Human Cardiac Troponin C in Reconstituted Muscle Fibres as Studied by Site-directed Spin Labelling

The in situ structure of human cardiac troponin C (hcTnC) has been studied with site-directed, spin labelling, electron paramagnetic resonance (SDSL-EPR). Analysis of the in situ structures of hcTnC is essential for elucidating the molecular mechanism behind its Ca(2+)-sensitive regulation. We prepared two hcTnC mutants (C35S and C84S) containing one native cysteine residue (84 and 35, respectively) for spin labelling. The mutants were labelled with a methane thiosulfonate spin label (MTSSL) and the TnC was reconstituted into permeabilized muscle fibres. The mobility of Cys84-MTSSL changed markedly after addition of Ca2+, while that of the Cys35 residue did not change in the monomer state or in fibres. The rotational correlation time of Cys84-MTSSL decreased from 32ns to 13ns upon Ca(2+)-binding in the monomer state, whereas in fibres the spectrum of Cys84-MTSSL was resolved into mobile (16ns) and immobile (35ns) components and the addition of Ca2+ increased the immobile component. Moreover, the accessibility of Cys84-MTSSL to molecular oxygen increased slightly in the presence of Ca2+. These data suggest that Cys35 remains in the same location regardless of the addition of Ca2+, whereas Cys84 is located at the position that interacts with B and C helices of hcTnC and interacts with troponin I (TnI) at high concentrations of Ca2+. We determined the distances between Cys35 and Cys84 by measuring pulsed electron-electron double resonance spectra. The distances were 26.0 angstroms and 27.2 angstroms in the monomer state and in fibres, respectively, and the addition of Ca2+ decreased the distance to 23.2 angstroms in fibres but only slightly in the monomer state, showing that Ca2+ binding to the N-domain of hcTnC induced a larger structural change in muscle fibres than in the monomer state.

Correlation between normal modes in the 20-200 cm-1 frequency range and localized torsion motions related to certain collective motions in proteins

In certain biologically relevant collective motions, such as protein domain motions and sub-domain motions, large amplitude movements are localized in one or a few flexible regions consisting of a small number of residues. This paper explores the possible use of normal mode analysis in probing localized vibrational torsion motions in these flexible regions that may be related to certain collective motions. The normal modes of 10 structures of five proteins in different conformation (TRP repressor, calmodulin, calbindin D(9k), HIV-1 protease and troponin C), known to have shear or hinge domain or sub-domain motion, respectively, are analyzed. Our study identifies, for each structure, unique normal modes in the 20-200 cm-1 frequency range, whose corresponding motions are primarily concentrated in the region where large amplitude torsion movements of a known domain or sub-domain motion occur. This suggests possible correlation between normal modes at 20-200 cm-1 frequency range and initial fluctuational motions leading to localized collective motions in proteins, and thus the potential application of normal mode analysis in facilitating the study of biologically important localized motions in biomolecules.