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R Censullo

Publications and source records attributed to R Censullo.

3 recordsLinked to original sources

Tropomyosin length and two-stranded F-actin flexibility in the thin filament.

In muscle thin filaments, each tropomyosin molecule is considered to be a rope-like structure that winds along the filament in contact with seven consecutive actin monomers on the same strand of the two-stranded actin helix. Taking into account the head-to-tail overlap of the tropomyosin molecule, the effective length of this "rope" is about 405 angstrum, which is believed to be conserved. Tropomyosin appears to be neither extensible nor compressible in its axial direction, although it may possess much flexibility in the transverse direction. During the "maximally on" state, characterized by the presence of Ca2+ and the strong binding between actin and myosin subfragment 1, the following conditions are thought to occur: the motion and associated flexibility of tropomyosin are reduced; the actin filament flexibility increases; a maximum number of equivalent tropomyosin binding sites on actin are concurrently saturated; and the tropomyosin molecule maintains an average thin filament radius of 38 to 40 angstrum. Under these potentiated conditions, the length of tropomyosin can be used to determine the limits on the underlying "cumulative angular disorder" of the actin filament with which it interacts. Our calculations show that only a small amount (approximately 1 to 3 degrees) of this type of actin monomer rotational disorder is possible at this stage of the contractile cycle, unless the length of the tropomyosin molecule is increased substantially between the head-to-tail joints. However, if the dominant type of F-actin rotational flexibility is between two relatively rigid actin strands (the lateral slipping/rotational offset model), all of the above actin-tropomyosin interactions can be completely and easily accommodated. We also discuss the implications of an interdomain hinge in G-actin and the possibility that there may be fewer than seven equivalent sites on actin that are saturated by tropomyosin concurrently.

Actin Cytoskeleton↗

A rotational offset model for two-stranded F-actin.

We propose the following "rotational offset" model for two independent strands of F-actin to account for the observation that it is possible, at times, for the crossover repeat to either alternate between long and short periods or remain constant (Bremer et al., 1991. J. Cell Biol. 115, 689-703). Rotational offset is the manifestation of the angular component of "lateral slipping" between the two long-pitch, right-handed strands comprising the actin filament. The present model is based on the premise that the longitudinal bond connecting the subunits along a single long-pitch strand is substantially stronger than the diagonal bond that connects interstrand subunits. We pose that, over fairly long stretches, the backbones of the two right-handed strands are individually close to being ideal helices, and that it is possible for the backbone of one strand to "roll across" the other. The rotational offset angle (epsilon 0) is the amount that one helical strand is angularly displaced relative to the position that otherwise would allow the two strands to be described as an ideal single genetic helix. Such an independent movement of the two strands is shown to shift the monomers that are involved in crossover points and produce the different patterns in crossover periods which have been observed from electron micrographs analysis. We specifically demonstrate that for a constant nonzero rotational offset the length of the crossover periods alternates, whereas for a constant offset of zero the crossover period remains constant. We also show that changes in the rotational offset angle along the filament can account for variable (random) crossover periods.

Actins↗