From: Chromosome–nuclear envelope attachments affect interphase chromosome territories and entanglement
Equations | Parameter | Value |
---|---|---|
\(\kappa\) | \(10K_{\text{b}} T\) (reduced to \(1K_{\text{b}} T\) for Topo II simulations) | |
\(\ell\) | .2 microns (twice the bead radius) | |
\(\sigma\) | \(\frac{\ell }{{2^{{{1 \mathord{\left/ {\vphantom {1 6}} \right. \kern-0pt} 6}}} }}\) where \(\ell = .2\) as in Eq. 1a | |
\(\varepsilon\) | \(3K_{\text{b}} T\) | |
\(\alpha\) | \(\pi \left[ {\left( {6^{{{1 \mathord{\left/ {\vphantom {1 6}} \right. \kern-0pt} 6}}} \sigma } \right)^{2} - \ell^{2} } \right]^{ - 1}\) | |
\(\beta\) | \(\pi - \ell^{2} \alpha\) | |
\(\xi\) | \(3K_{\text{b}} T\) | |
m | 77MDa (bead mass) | |
γ | \(\tau^{ - 1}\) where \(\tau = \sigma \sqrt {{m \mathord{\left/ {\vphantom {m \varepsilon }} \right. \kern-0pt} \varepsilon }}\) |