Parameters of Cell Death and Proliferation of Prostate Cancer Cells with Altered Expression of Myosin 1C Isoforms.

Myosin 1C is a monomeric myosin motor with a truncated tail domain. Such motors are referred as slow "tension sensors." Three isoforms of myosin 1C differ in short N-termed amino acid sequences, the functional differences between isoforms have not been elucidated. Myosin 1C isoform A was described as a diagnostic marker for prostate cancer, but its role in tumor transformation remains unknown. Based on data on the functions of myosin 1C, we hypothesized the potential role of myosin 1C isoforms in maintaining the tumor phenotype of prostate cancer cells. In our work, we showed that a decrease in the expression level of myosin 1C isoform C leads to an increase in the proliferative activity of prostate tumor cells.

Proliferative Activity of Colorectal Cancer Cells with Different Levels of CD133 Expression.

We studied proliferative activity of colorectal cancer cells with different expression level of CD133 molecule associated with cancer stem cells phenotype. Analysis of BrdU incorporation into Caco-2 and HT-29 cell lines showed that the percentage of cells in the DNA synthesis phase in the CD133+/high population is higher than in CD133-/low population. The expression of proliferation marker Ki-67 and the percentage of Ki-67+ cells were also higher in the CD133+/high population. Colorimetric analysis with crystal violet dye showed that the number of cells after 10-days culturing was higher in the CD133+/high population in both cell lines. These findings suggest that cells with high level of CD133 expression are characterized by higher proliferative activity, which can contribute to the tumor progression.

Fine structure and dynamics of EB3 binding zones on microtubules in fibroblast cells.

End-binding (EB) proteins associate with the growing tips of microtubules (MTs)and modulate their dynamics directly and indirectly, by recruiting essential factors to fine-tune MTs for their many essential roles in cells. Previously EB proteins have been shown to recognize a stabilizing GTP/GDP-Pi cap at the tip of growing MTs, but information about additional EB-binding zones on MTs has been limited. In this work, we studied fluorescence intensity profiles of one of the three mammalian EB-proteins, EB3, fused with red fluorescent protein (RFP). The distribution of EB3 on MTs in mouse fibroblasts frequently deviated from single exponential decay and exhibited secondary peaks. Those secondary peaks, which we refer to as EB3-islands, were detected on 56% comets of growing MTs and were encountered once per 44 s of EB3-RFP comet growth time with about 5 s half-lifetime. The majority of EB3-islands in the vicinity of MT tips was stationary and originated from EB3 comets moving with the growing MT tips. Computational modeling of the decoration of dynamic MT tips by EB3 suggested that the EB3-islands could not be explained simply by a stochastic first-order GTP hydrolysis/phosphate release. We speculate that additional protein factors contribute to EB3 residence time on MTs in cells, likely affecting MT dynamics.

[Microtubules suppress blebbing and stimulate lamellae extension in spreading fibroblasts].

We compared spreading of Vero fibroblasts when microtubules were depolymerized or stabilized. After initial attachment cells start blebbing that continues for different time and abruptly transfers into spreading. After spreading initiation, most cells spread in an anisotropic manner through stochastic formation of lamellipodia. A second mode was rapid, isotropic spreading via formation of circular lamellum that occurs in 15% of cells. The rate of spreading was maximal at the beginning and decreased during the first hour according to logarithmic law. After 60 min many cells formed stable efges and started migrating on the substrate. However, cell area slowly continued to increase. Actin bundles are formed 20 min after cell attachment and they first run along cell boundary. This system disassembles within 20-40 min and is substituted with stress fibers crossing the cell. In the isotropically spread cells no actin bunbles are seen. Microtubules in the spreading cells enter into large blebs and all nascent lamella and later form radial array. When MTs has been depolymerized or stabilized blebbing started before cells attached to the substrate and continue much longer than in control cells. In both cases the initial rate of spreading decrease several fold, and remains constant for many hours. After 24 h the mean area occupied by cells with altered MT system was the same as in control. Alteration of MT system had moderate effect on actin system--formation of actin cables started at the same time as in control (within 20 min upon cell attachment), however, they grew even in cells undergoing prolonged blebbing. Actin cables running along cell margin were similar to tat in control cells, but they did not disappear up to 1 h. When stabilized, microtubules form chaotic array: they do not enter blebs and in spread cells run parallel to the cell margin at a distance of 3-5 microm. We conclude that dynamic microtubules speed up completion of blebbing and promote early stages of fibroblasts spreading.

[Experimental visualization of chromoneme as one of the higher levels of chromatin compactization in the mitotic chromosome].

We succeeded to visualize the chromoneme or a filamentous chromatin structure, with the mean thickness 0.1-0.2 microm, as a higher level of chromatin compactization in animal and plant cells at different stages of chromosome condensation at mitotic prophase and during chromatid decondensation at telophase. Under the natural conditions, chromoneme elements are not detected in the most condensed chromatin of metaphase chromosomes on ultrathin sections. We studied the ultrastructure and behavior of the chromatin of mitotic chromosomes in situ in cultured mouse L-197 cells under the conditions selectively demonstrating the chromoeneme structure of the mitotic chromosomes in the presence of Ca2+. Loosely packaged dense chromatin bands, ca. 100 nm in diameter, chromonemes, were detected in chromosome arms in a solution containing 3 mM CaCl2. When transferred in a hypotonic solution containing 10 mM tris-HCl, these chromosome swelled, lost the chromoneme level of structure, and rapidly transformed in loose aggregates of elementary DNP fibrils, 30 nm in diameter. After this decondensation in the low ionic strength solution, the chromoneme structure of mitotic chromosomes was restored when they were transferred in a Ca2+ containing solution. The morphological characteristics of the chromoneme and pattern of its packaging in the chromosome were preserved. However, when the mitotic cells with chromosomes, in which the chromoneme structure was visualized with the help of 3 mM CaCl2, were treated with a photosensbilizer, ethidium bromide, and illuminate with a light with the wavelength 460 nm, chromatic decondensation under the hypotonic solution was not observed. The chromoneme elements in a stabilized chromatin of the mitotic chromosome preserved specific interconnection and their general pattern of packaging in in the chromatic was also preserved. The chromoneme elements in the chromosomes stabilized by light preserved their density and diameter even in a 0.6 M NaCl solution, which normally leads to chromoneme destruction. An even more rigid treatment of the stabilized chromosomes with a 2 M NaCl solution, which normally fully decondenses the chromosomes, made it possible to detect a 3D reticular skeleton devoid of any axial structures.