Volume 104, Issue 9, Pages (May 2013)

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Date of download: 7/10/2016 Copyright © ASME. All rights reserved. From: A Model for Highly Strained DNA Compressed Inside a Protein Cavity J. Comput.
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Volume 104, Issue 9, Pages 2058-2067 (May 2013) Structural Ensemble and Dynamics of Toroidal-like DNA Shapes in Bacteriophage ϕ29 Exit Cavity  Andrew D. Hirsh, Maryna Taranova, Troy A. Lionberger, Todd D. Lillian, Ioan Andricioaei, N.C. Perkins  Biophysical Journal  Volume 104, Issue 9, Pages 2058-2067 (May 2013) DOI: 10.1016/j.bpj.2013.03.032 Copyright © 2013 Biophysical Society Terms and Conditions

Figure 1 Cross section of the three-dimensional cryo-EM ϕ29 reconstruction (11). The virion map (purple, color online) is overlaid with the emptied map to highlight the genome. (Inset) Region to be simulated; the toroid constrained in the connector/lower collar cavity. Density maps generated with UCSF CHIMERA (36). Biophysical Journal 2013 104, 2058-2067DOI: (10.1016/j.bpj.2013.03.032) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 2 (A) Cross section of the connector/lower-collar cavity with toroidal DNA from Tang et al. (11). (B) Point-wise discretized constraint surface, derived from the protein cavity walls, specifies the location of computational grid points in the rod model or inert atoms in MD rigidly positioned on the cavity surface. (C) The atomic structure of DNA superimposed with an elastic rod with equivalent elastic properties. R→(s,t) defines the position of the helical axis as a function of contour length s and time t with respect to the inertial frame e. We also define a body-fixed reference frame a(s,t), which is also a function of s and t. The interaction forces are dependent on all pairwise vectors between rod grid points p and points q representing the cavity surface. Biophysical Journal 2013 104, 2058-2067DOI: (10.1016/j.bpj.2013.03.032) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 3 Rod model predicts toroid formation in the ϕ29 cavity. Snapshots of twist-free equilibrium conformations as a function of toroid size (basepairs). (Black stripe) Aid in visualizing the twist state of DNA. During supercoil formation, twist is relieved through the lower boundary. Biophysical Journal 2013 104, 2058-2067DOI: (10.1016/j.bpj.2013.03.032) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 4 Compressive force required to form a toroid is well within packing motor capabilities (25 pN for toroids >10 bp). Plotted are DNA internal (elastic strain) energy (gray squares) and compressive force (black circles) as a function of toroid size. DNA is initially nearly straight while the top boundary descends in the tube one basepair (3.4 Å) at a time. Biophysical Journal 2013 104, 2058-2067DOI: (10.1016/j.bpj.2013.03.032) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 5 Energy landscape of all possible DNA conformations over the two-parameter space of toroid size and registry. (A) Potential energy landscape and its (B) electrostatic, (C) bonded, and (D) van der Waals components for right-handed toroids. To highlight energetic differences between conformations, energy values are scaled relative to the minimum value in the corresponding landscape. Biophysical Journal 2013 104, 2058-2067DOI: (10.1016/j.bpj.2013.03.032) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 6 Molecular dynamics model of atomic DNA structure highly bent and under extreme compression. (A and B) Front and top views of all-atom initial condition of a 33-bp toroid with helical axis predicted by rod model inside the constraints of the cavity. The DNA sequence is the first 75 bps from the ϕ29 genome. (C and D) Same views of final conformations after MD equilibration within the constraints of the cavity show that basepairing is preserved. (Magenta) Hydrogen bonds. All atomistic DNA graphics generated with UCSF CHIMERA (36). Biophysical Journal 2013 104, 2058-2067DOI: (10.1016/j.bpj.2013.03.032) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 7 Predicted density maps compared side by side with experimental data. (A) Predicted maps for different-sized toroids. (B) Two orthogonal cross sections of the experimental cryo-EM density map (11). (Yellow and dark blue) Regions of highest and lowest intensity, respectively. Rotational averaging of the conformation was performed using UCSF CHIMERA (36). Consistent with the experimental results, the color scale is determined by scaling the highest intensity bin relative to the lowest intensity bin (see Methods). Biophysical Journal 2013 104, 2058-2067DOI: (10.1016/j.bpj.2013.03.032) Copyright © 2013 Biophysical Society Terms and Conditions

Figure 8 Rod model of toroid collapse predicts large reaction force/torque at the connector. (A) Snapshots show instantaneous conformations during ejection. (B) Axial reaction force and torque at the upper boundary as a function of reduced time t/τ, where τ is the time required for the toroid to fully straighten and can range from ∼τ = 6.8–68 μm (see text for discussion). Biophysical Journal 2013 104, 2058-2067DOI: (10.1016/j.bpj.2013.03.032) Copyright © 2013 Biophysical Society Terms and Conditions