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. 2006 Aug 4;91(11):4121–4132. doi: 10.1529/biophysj.106.082099

TABLE 2.

Comparison of the nucleosomal DNA bending energies predicted within the classical elastic rod theory with those observed in the simulations reported here

Arc length, φ, rad 2.0 π 3.7
End-to-end distance, Å 411 318 257
Classical Ebend, kcal/mol 2.3 5.8 8.0
E〉 of snapshots in Fig. 6, Kcal/mol −19.1 −12.8 −12.5

The classical values are computed assuming bending through perfectly circular arcs of specified end-to-end distance; Eq. 2 is used with the persistence length of Lp = 500 Å. Conformational energies are computed as averages over the following representative points in Fig. 6, as one moves along the horizontal axis: five rightmost points, five in the middle (interval [300, 325] Å), and five leftmost points. Their average energies 〈E〉 and end-to-end distances are reported. Note that each interval contains 500 of the original molecular dynamics conformations, 100 per each point. Since only the snapshots from the last 4 ns of the MD are included in the energy analysis, the energy of the initially fully stretched DNA conformation (end-to-end distance ∼500 Å, φ = 0) is not computed, and can be considered as an unknown constant offset.