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* Integrated Bioscience and Biomedical Engineering, Graduate School of Science and Engineering,
Department of Physics, Faculty of Science and Engineering, and
Advanced Research Institute for Science and Engineering, Waseda University, Shinjuku-ku, Tokyo, Japan;
Graduate School of Pharmaceutical Sciences, The University of Tokyo, Bunkyo-ku, Tokyo, Japan; and ¶ Core Research for Evolutional Science and Technology, Japan Science and Technology Agency, Saitama, Japan
Correspondence: Address reprint requests to Takashi Funatsu, Laboratory of Bio-Analytical Chemistry, Graduate School of Pharmaceutical Sciences, The University of Tokyo, 7-3-1, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan. Tel.: 81-3-5841-4760; Fax: 81-3-5802-3339; E-mail: funatsu{at}mail.ecc.u-tokyo.ac.jp.
Actin is a ubiquitous protein that is a major component of the cytoskeleton, playing an important role in muscle contraction and cell motility. At steady state, actin monomers and filaments (F-actin) coexist, and actin subunits continuously attach and detach at the filament ends. However, the size distribution of actin oligomers in F-actin solution has never been clarified. In this study, we investigated the size distribution of actin oligomers using photon-counting histograms. For this purpose, actin was labeled with a fluorescent dye, and the emitted photons were detected by confocal optics (the detection volume was of femtoliter (fL) order). Photon-counting histograms were analyzed to obtain the number distribution of actin oligomers in the detection area from their brightness, assuming that the brightness of an oligomer was proportional to the number of protomers. We found that the major populations at physiological ionic strength were 15mers. For data analysis, we successfully applied the theory of linear and helical aggregations of macromolecules. The model postulates three states of actin, i.e., monomers, linear polymers, and helical polymers. Here we obtained three parameters: the equilibrium constants for polymerization of linear polymers, Kl = (5.2 ± 1.1) x 106 M1, and helical polymers, Kh = (1.6 ± 0.5) x 107 M1; and the ratio of helical to linear trimers,
= (3.6 ± 2.3) x 102. The excess free energy of transforming a linear trimer to a helical trimer, which is assumed to be a nucleus for helical polymers, was calculated to be 2.0 kcal/mol. These analyses demonstrate that the oligomeric phase at steady state is predominantly composed of linear 15mers, and the transition from linear to helical polymers occurs on the level of 57mers.
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