Investigation of viral DNA packaging using molecular mechanics models
Introduction
Some bacteriophage have linear double-stranded DNA (ds-DNA) genomes that are tightly packaged into a roughly spherical volume inside the viral capsid [5]. The packaging of genomic DNA poses two problems for bacteriophage. First, a very high degree of condensation is required, with the final DNA concentration being on the order of 300 mg/ml [18]. This must be achieved without the benefit of higher order protein–DNA structures like those found in eukaryotic chromatin. Second, ejection of the DNA at the time of infection requires that the DNA not be knotted or entangled.
Diverse models have been proposed for the packaging of phage ds-DNA. The DNA might have local ordering but no long-range ordering, so that it is a liquid crystal [22]. Alternatively, there may be overall ordering into a fairly well-defined geometry. Among the latter possibilities are coaxial spooling [12], [31], spiral folding [6], folded coaxial spooling [38], and a folded toroid [17]. Recent cryo-electron microscopy experiments appear to be most consistent with coaxial spooling, at least for bacteriophage T7 [8].
The issue of viral packaging has received renewed importance because of the quality of data from cryo-electron microscopy, and because of other experimental developments. Single molecule measurements are now capable of measuring the forces and pressures generated during packaging [19], [40], and new 2D gel electrophoretic methods allow the quantitative determination of the relative frequencies of differently knotted conformers of closed circular DNAs like those found in bacteriophage P4 [47]. Furthermore, DNA packing in lipid complexes resembles packing in bacteriophage, with obvious implications for gene therapy [37]. Accurate modeling tools should assist in the interpretation of these and future experiments. Here we focus on the spooling model and its consequences, using P4 as a model.
Low resolution models for DNA can be used to examine issues of DNA packaging, supercoiling and knotting [26], [30]. A number of approaches have been used to model DNA molecules in the size range 1–30 kilobasepairs (kb). The molecules have been described mathematically using finite elements [2], [54], Fourier series [56], and B-splines [14], [35], [36]. DNA can also be treated as a segmented chain, using bead models (pseudoatom representations) suitable for hydrodynamic and molecular mechanics algorithms [20], [23], [27], [28], [43], [48], and that is the approach we use here.
Unlike traditional molecular mechanics models in which each atom is represented as a point mass [29], low resolution models use a reduced representation, with appropriate pseudoatoms representing pieces of the structure. Our original model [43] used three pseudoatoms to define the plane of each basepair. The potential energy function was parameterized so that the elastic moduli for stretching, bending and twisting deformations matched those for double helical DNA. The model is thus a discretized approximation to a continuum elastic model. It has been used to investigate a number of questions about the structure, topology and dynamics of small closed circular DNAs [41], [45], [46].
Here we investigate the packaging of molecules in the size range of genomic phage DNA inside viral capsids, approximating the icosahedron by a sphere. Since we are using the model to investigate questions of global organization rather than local structural details, we do not need atomic detail, or even to represent each basepair. ds-DNA in bacteriophage does not differ significantly from normal B-DNA [1] and does not interact strongly with the capsid [39], so we can use a very simple model with a single pseudoatom to represent one turn of the double helix. This reduces the computational requirements and permits rapid calculations on molecules in the size range 10–30 kb. A variety of traditional molecular mechanics algorithms (energy minimization; Monte Carlo; simulated annealing; molecular dynamics (MD); Brownian dynamics) can be used to refine static models, to sample conformational space, to estimate average properties of thermodynamic ensembles, and to investigate conformational transitions.
Section snippets
Methods
All modeling and data analysis were carried out with YAMMP [44], a molecular modeling package developed specifically for reduced representation models. See http://uracil.cmc.uab.edu/YammpWeb for more information on the YAMMP package.
The model uses one pseudoatom to represent ten basepairs (approximately one turn of the double helix). Successive pairs of pseudoatoms are held together by harmonic bonds with an ideal length of 34 Å, the pitch of the double helix. The bond stretching force constant
Random packing of a closed circular DNA molecule
The power of the method is illustrated by the compression of a relaxed closed circular DNA molecule into the volume corresponding to that of a small viral capsid (Fig. 1). With an exclusion diameter of 30 Å for the DNA, this model occupies over 90% of the available volume. A variety of starting conformations were generated, each corresponding to a typical structure for a relaxed closed circular 10 kb ds-DNA. The starting structures are quite extended, with radii of gyration on the order of 100
Discussion
Cryo-electron microscopy on oriented tailless T7 heads reveals a quasi-crystalline packing of the DNA into six coaxial shells, consistent with the coaxial spooling model [8], and it is likely that this motif occurs in some other viruses with ds-DNA genomes. Here we have described methods for modeling packaging in such systems, using energy minimization to generate idealized models for coaxially spooled DNA. When the packing density is high, we find that little reduction in energy is obtained by
Conclusions
Reduced representations like the one reported in the present work are potentially powerful tools for teasing out the interplay of the various energetic factors on the structural, kinetic and thermodynamic aspects of DNA packaging. It is already clear that the optimal structure will depend on the free volume within the capsid, and on whether or not attractive interactions are present. Little is presently known about the proper functional form for treating attractive interactions for DNA
Acknowledgements
J.A., M.V. and D.W.S. were partially supported through infrastructure grants to the Program in Mathematics and Molecular Biology from the National Science Foundation (NSF DMS-9406348) and the Burroughs Wellcome Fund Interfaces Program. This work also supported by NSF grant DMS 9971169 (J.A. and M.V.) and by a DGAPA graduate fellowship (M.V.). S.C.H. and R.K.Z.T. were supported by a grant from the National Institutes of Health (P41 RR12255, C.L. Brooks, III, Scripps Research Institute, PI).
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Present address: Department of Mathematics, University of California, Berkeley, CA, USA.