| Literature DB >> 30689638 |
Daniel Havelka, Ondřej Kučera, Marco A Deriu, Michal Cifra.
Abstract
[This corrects the article DOI: 10.1371/journal.pone.0086501.].Entities:
Year: 2019 PMID: 30689638 PMCID: PMC6349308 DOI: 10.1371/journal.pone.0210897
Source DB: PubMed Journal: PLoS One ISSN: 1932-6203 Impact factor: 3.240
List of parameters.
| Symbol | Description | Value | Units |
|---|---|---|---|
| dipole moment of | 369 | D | |
| dipole moment of | 26 | D | |
| axial shift between protofilaments | 0.92 | nm | |
| diameter of MT rings | 10.76 | nm | |
| Ξ | leading angle of MT rings | 10.28 | degrees |
| major axis of ellipsoid cell | 10.32 | μm | |
| minor axis of ellipsoid cell | 5.28 | μm | |
| radius of non-dividing spherical cell | 3.3 | μm | |
| volume of spherical cell with radius | 150.5 | μm3 | |
| position of MTOC on the x-axis | 3.089 | μm | |
| diameter of MTOC | 200 | nm | |
| number of MTs | 300 | - | |
| number of nucleation centers, astral MTs, one MTOC | 50 | - | |
| number of nucleation centers, kinetochore MTs, one MTOC | 50 | - | |
| number of nucleation centers, polar MTs, one MTOC | 50 | - | |
equivalent number of nucleation centers | 120 | - | |
| Ω | spatial angle for division of MTOC, astral MTs | 2.8212 | sr |
| equivalent number of nucleation centers | 225 | - | |
| Ω | spatial angle for division of MTOC, polar and kinetochore MTs | 2.9154 | sr |
| arbitrary constant | 1 | - | |
| index of polar and kinetochore MTs | 1, 2, …, 200 | ||
| mathematical constant | 3.14159 | - | |
| index denoting | 1,2,…, | - | |
| Oscillating part of dipole moment of | (3.8)−1 | - | |
| oscillating part of dipole moment of | (3.8)−1 | - | |
| quality factor | 0.5 ÷ 100 | - | |
| coefficient of extrapolation | 2.5304 ⋅ 1012 | - | |
| radius of outer wall of MT | 12.5 | nm | |
| coefficient of extrapolation | 9.0966 ⋅ 108 | - | |
| length of tubulin heterodimer | 8 | nm |
The list of symbols (in the order of appearance) representing variables of the model and their values used for calculations.
Fig 10Electrical parameters of the cytosol.
We used homogeneous electrical properties of the surroundings of the MTs in our model. The figure shows frequency versus complex permittivity plot. The real part of the complex permittivity (up) represents the value of the relative electrical permittivity, and therefore energy stored in the material, and the imaginary part (down) corresponds to dielectric losses.