Abstract
Due to the number of nucleotides in a typical system of interest, and the complexity of the interactions between them, it is impossible to find exact analytical expressions for the behaviour of a general coarse-grained model of DNA. Computer simulations can provide numerical information in the absence of any exact solutions, and guide the application of simpler, analytic descriptions.
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Notes
- 1.
To avoid confusion, I shall take the term microstate to be a given set of positions, orientations, velocities and angular velocities for the system in question. The configuration is defined by the positions and orientation of entities in the sysem. Finally, I shall use the term state more broadly, to apply to a set of microstates or configurations which are in some way similar (for instance, the ‘duplex state’ consists of all microstates in which the two strands are bound to each other.
- 2.
The algorithm used is actually the variant detailed in the appendix of Ref. [9].
- 3.
Here I consider only additive noise, and can therefore neglect the subtleties of the distinction between Ito and Stratonovich calculus [12].
- 4.
Despite this reduction in noise, dynamics are still highly damped. For example, a simulation of a 10 bp duplex at 300 K initiated with all 10 bp formed but far from an optimal configuration (with around 70 % of the typical binding energy and no kinetic energy) will reach states typical of equilibrium in around \(10\) units of reduced time. For comparison, diffusion over its own length is around 10–100 times slower for a 10 bp duplex.
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Ouldridge, T.E. (2012). Methods. In: Coarse-Grained Modelling of DNA and DNA Self-Assembly. Springer Theses. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-30517-7_3
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