No abstract

The giant muscle protein titin, also called connectin, is responsible for the elasticity of relaxed striated muscle, as well as acting as the molecular scaffold for thick-filament formation. The titin molecule consists largely of tandem domains of the immunoglobulin and fibronectin-III types, together with specialized binding regions and a putative elastic region, the PEVK domain. We have done mechanical experiments on single molecules of titin to determine their visco-elastic properties, using an optical-tweezers technique. On a fast (0.1s) timescale titin is elastic and force-extension data can be fitted with standard random-coil polymer models, showing that there are two main sources of elasticity: one deriving from the entropy of straightening the molecule; the other consistent with extension of the polypeptide chain in the PEVK region. On a slower timescale and above a certain force threshold, the molecule displays stress-relaxation, which occurs in rapid steps of a few piconewtons, corresponding to yielding of internal structures by about 20 nm. This stress-relaxation probably derives from unfolding of immunoglobulin and fibronectin domains.

Myosins are motor proteins in cells. They move along actin by changing shape after making stereospecific interactions with the actin subunits. As these are arranged helically, a succession of steps will follow a helical path. However, if the myosin heads are long enough to span the actin helical repeat (approximately 36 nm), linear motion is possible. Muscle myosin (myosin II) heads are about 16 nm long, which is insufficient to span the repeat. Myosin V, however, has heads of about 31 nm that could span 36 nm and thus allow single two-headed molecules to transport cargo by walking straight. Here we use electron microscopy to show that while working, myosin V spans the helical repeat. The heads are mostly 13 actin subunits apart, with values of 11 or 15 also found. Typically the structure is polar and one head is curved, the other straighter. Single particle processing reveals the polarity of the underlying actin filament, showing that the curved head is the leading one. The shape of the leading head may correspond to the beginning of the working stroke of the motor. We also observe molecules attached by one head in this conformation.

In striated muscles, the rapid production of macroscopic levels of force and displacement stems directly from highly ordered and hierarchical protein organization, with the sarcomere as the elemental contractile unit. There is now a wealth of evidence indicating that the giant elastic protein titin has important roles in controlling the structure and extensibility of vertebrate muscle sarcomeres.

Titin is at present the largest known protein (M(r) 3000 kDa) and its expression is restricted to vertebrate striated muscle. Single molecules span from M‐ to Z‐lines and therefore over 1 micron. We have isolated cDNAs encoding five distant titin A‐band epitopes, extended their sequences and determined 30 kb (1000 kDa) of the primary structure of titin. Sequences near the M‐line encode a kinase domain and are closely related to the C‐terminus of twitchin from Caenorhabditis elegans. This suggests that the function of this region in the titin/twitchin family is conserved throughout the animal kingdom. All other A‐band sequences consist of 100 amino acid (aa) repeats predicting immunoglobulin‐C2 and fibronectin type III globular domains. These domains are arranged into highly ordered 11 domain super‐repeat patterns likely to match the myosin helix repeat in the thick filament. Expressed titin fragments bind to the LMM part of myosin and C‐protein. Binding strength increases with the number of domains involved, indicating a cumulative effect of multiple binding sites for myosin along the titin molecule. We conclude that A‐band titin is likely to be involved in the ordered assembly of the vertebrate thick filament.

Myosin VI is involved in a wide variety of intracellular processes such as endocytosis, secretion and cell migration. Unlike almost all other myosins so far studied, it moves towards the minus end of actin filaments and is therefore likely to have unique cellular properties. However, its mechanism of force production and movement is not understood. Under our experimental conditions, both expressed full-length and native myosin VI are monomeric. Electron microscopy using negative staining revealed that the addition of ATP induces a large conformational change in the neck/tail region of the expressed molecule. Using an optical tweezers-based force transducer we found that expressed myosin VI is nonprocessive and produces a large working stroke of 18 nm. Since the neck region of myosin VI is short (it contains only a single IQ motif), it is difficult to reconcile the 18 nm working stroke with the classical 'lever arm mechanism', unless other structures in the molecule contribute to the effective lever. A possible model to explain the large working stroke of myosin VI is presented.

Partial amino acid sequence was obtained from the massive myofibrillar protein nebulin. This consists of repeating motifs of about 35 residues and super‐repeats of 7 × 35 = 245 residues. The repeat‐motifs are likely to be largely α‐helical and to interact with both actin and tropomyosin in thin filaments. Nebulin from different species was found to vary in size in proportion to filament length. The data are consistent with the proposal that nebulin acts as a protein‐ruler to regulate precise thin filament assembly.

It is still unclear whether mechanical unfolding probes the same pathways as chemical denaturation. To address this point, we have constructed a concatamer of five mutant I27 domains (denoted (I27)(5)*) and used it for mechanical unfolding studies. This protein consists of four copies of the mutant C47S, C63S I27 and a single copy of C63S I27. These mutations severely destabilize I27 (DeltaDeltaG(UN) = 8.7 and 17.9 kJ mol(-1) for C63S I27 and C47S, C63S I27, respectively). Both mutations maintain the hydrogen bond network between the A' and G strands postulated to be the major region of mechanical resistance for I27. Measuring the speed dependence of the force required to unfold (I27)(5)* in triplicate using the atomic force microscope allowed a reliable assessment of the intrinsic unfolding rate constant of the protein to be obtained (2.0 x 10(-3) s(-1)). The rate constant of unfolding measured by chemical denaturation is over fivefold faster (1.1 x 10(-2) s(-1)), suggesting that these techniques probe different unfolding pathways. Also, by comparing the parameters obtained from the mechanical unfolding of a wild-type I27 concatamer with that of (I27)(5)*, we show that although the observed forces are considerably lower, core destabilization has little effect on determining the mechanical sensitivity of this domain.