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Structure and Conformational Dynamics of Scaffolded DNA Origami Nanoparticles Keyao Pan1,†, William P

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Structure and Conformational Dynamics of Scaffolded DNA Origami Nanoparticles Keyao Pan1,†, William P 6284–6298 Nucleic Acids Research, 2017, Vol. 45, No. 11 Published online 8 May 2017 doi: 10.1093/nar/gkx378 Structure and conformational dynamics of scaffolded DNA origami nanoparticles Keyao Pan1,†, William P. Bricker1,†, Sakul Ratanalert1,2 and Mark Bathe1,* 1Department of Biological Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139, USA and 2Department of Chemical Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139, USA Received October 21, 2016; Revised April 04, 2017; Editorial Decision April 22, 2017; Accepted April 25, 2017 ABSTRACT rials science (1–3). Scaffolded DNA origami (4,5) employs a single-stranded DNA (ssDNA) scaffold strand that forms Synthetic DNA is a highly programmable nanoscale a template for shorter DNA substrands called staples, of- material that can be designed to self-assemble into fering near-quantitative yield over the final, self-assembled 3D structures that are fully determined by underlying product for DX-based wireframe scaffolded DNA origami Watson–Crick base pairing. The double crossover structures. Watson–Crick base pairing between the scaffold (DX) design motif has demonstrated versatility in strand and staple strands enables folding ssDNA into struc- synthesizing arbitrary DNA nanoparticles on the 5– tured DNA assemblies with diverse geometries, including 100 nm scale for diverse applications in biotechnol- wireframe structures (6–11), 2D surfaces (4,12–15), and 3D ogy. Prior computational investigations of these as- solids (16–20). Alternatively, structured DNA assemblies of semblies include all-atom and coarse-grained mod- these three types of geometries can be programmed without eling, but modeling their conformational dynamics scaffold strands (21–26). Integral to the effective design and synthesis of struc- remains challenging due to their long relaxation tured DNA assemblies is computer-aided design (CAD). times and associated computational cost. We ap- Manual software tools including caDNAno (27)andTia- ply all-atom molecular dynamics and coarse-grained mat (28) have been developed to aid in this process. More finite element modeling to DX-based nanoparticles recently, the top-down, geometry-based algorithms vHe- to elucidate their fine-scale and global conforma- lix (10) and DAEDALUS (11) have been developed to au- tional structure and dynamics. We use our coarse- tomate the design of nucleic acid sequences in near-fully grained model with a set of secondary structural and fully automated manners, respectively, for wireframe motifs to predict the equilibrium solution structures geometries. The finite element (FE) modeling approach of 45 DX-based DNA origami nanoparticles includ- CanDo is also routinely used to predict the 3D equilibrium ing a tetrahedron, octahedron, icosahedron, cuboc- conformation of programmed DNA assemblies based on tahedron and reinforced cube. Coarse-grained mod- a coarse-grained representation of B-form DNA (5,29,30). Because numerous applications of structured DNA assem- els are compared with 3D cryo-electron microscopy blies exploit control over the angstrom-level positioning of density maps for these five DNA nanoparticles and individual bases (20,31–33), computational investigation of with all-atom molecular dynamics simulations for the atomic-level structure together with automated tools that tetrahedron and octahedron. Our results elucidate predict non-intuitive equilibrium shapes are of great utility non-intuitive atomic-level structural details of DX- to the field of structural DNA nanotechnology. based DNA nanoparticles, and offer a general frame- While numerous computational tools are capable of pre- work for efficient computational prediction of global dicting equilibrium solution structures of nucleic acid as- and local structural and mechanical properties of DX- semblies, all-atom molecular dynamics (MD) simulations based assemblies that are inaccessible to all-atom (34) in principle represent the gold standard for 3D struc- based models alone. ture prediction (35,36). All-atom models are capable of capturing the detailed structural, mechanical, and physic- ochemical properties of DNA assemblies, albeit at signifi- INTRODUCTION cant computational cost that limits their application using Synthetic DNA nanotechnology leverages the secondary conventional computing resources to short time-scale sim- structure of DNA to reliably program 3D geometries for ulations and low molecular weight assemblies. Larger-scale diverse applications in biotechnology and nanoscale mate- assemblies can be simulated on limited time-scales of tens to *To whom correspondence should be addressed. Tel: +1 617 324 3685; Fax: +1 617 324 7554; Email: [email protected] †These authors contributed equally to this work as first authors. C The Author(s) 2017. Published by Oxford University Press on behalf of Nucleic Acids Research. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by-nc/4.0/), which permits non-commercial re-use, distribution, and reproduction in any medium, provided the original work is properly cited. For commercial re-use, please contact [email protected] Nucleic Acids Research, 2017, Vol. 45, No. 11 6285 hundreds of nanoseconds using high performance comput- lations of the bulge to determine its rotational stiffness coef- ing resources that are not broadly available (34). In contrast, ficients. Further, we apply all-atom MD to model the equi- coarse-grained models use united atom representations to librium geometry and mechanical properties of a limited set model clusters of atoms and their interactions, thereby re- of DX-based nanoparticles to compare predictions of our ducing the total number of degrees of freedom (DOF) and coarse-grained model with both experimental cryo-electron associated computational cost (37–49) at the expense of all- microscopy (cryo-EM) data and all-atom modeling. atom resolution. In order to maximize structural prediction accuracy while MATERIALS AND METHODS reducing computational cost, numerous coarse-grained Lattice-free finite element model of structured DNA assem- models for DNA have been developed (50–53). Nucleotide- blies level models represented in oxDNA2 (54), an enhanced ver- sion of oxDNA (55), treat each nucleotide as a rigid body The FE method was originally used to model four dis- that interacts with other nucleotides via an empirical poten- tinct topological motifs defined by the secondary structure tial. This coarse-grained model has been applied to simulate of programmed DNA assemblies, which included duplexes, hybridization kinetics (56), overstretching (57), equilibrium nicks, ssDNA, and double crossovers (5,29), where duplexes structures (58), and self-assembly (59) of DNA. An alter- were assumed to reside on a square or honeycomb lattice. native category of models, the 3-site-per-nucleotide (3SPN) Subsequently, the requirement that duplexes reside on such model (60,61), uses three interaction sites to simulate the lattices was removed and single crossovers were also incor- base, sugar, and phosphate group of a nucleotide, and has porated into the model to account for their higher confor- been used to predict DNA melting curves and persistence mational flexibility with respect to double-crossovers (30). lengths (62). In addition, chemical group-level models such Here, we additionally introduce a bulge model to facilitate as the MARTINI coarse-grained force field (63–65)have simulation of DX-based objects, and also differentiate be- been extended to model DNA by treating each nucleotide tween open and closed nicks due to their distinct mechan- as six or seven beads (66). These coarse-grained models ical properties associated with stacked versus non-stacked of DNA have been discussed in more detail in recent re- base pairs (Figure 1). Closed nicks are identified using the view articles (67–69). While useful for predicting conforma- four nucleotides denoted n1, n2, n3 and n4, in the CAD de- tional dynamics of DNA assemblies, particularly involving sign, where base pair n1–n2 stacks with base pair n3–n4 (Fig- duplex dissociation, large-scale equilibrium structural and ure 1B). Otherwise, the two base pairs are modeled as an mechanical properties of highly structured DNA assemblies open nick (Figure 1B). programmed using the principle of scaffolded DNA origami Each base pair in a DNA assembly is modeled as a FE remain challenging to predict using these models. node with three translational DOF and three rotational As an alternative, here we apply our FE modeling frame- DOF in a global 3D Cartesian coordinate system (Figure work CanDo to solve for the ground-state equilibrium 1A). Such a node is rigidly connected to a right-handed structure and mechanical properties of structured DNA orthonormal reference frame (e0, e1, e2, e3) with the center nanoparticles. Compared with the aforementioned compu- e0 located at the position of the node. The all-atom model tational tools, our FE model treats DNA duplexes as worm- of a DNA assembly determines the reference frames of all like chains from polymer physics (70) or elastic beams from nodes, and vice versa. From the all-atom base pair model, mechanical engineering (71) accounting for the full axial, the convention used by the software 3DNA (73) defines the torsional, and bending properties of duplex B-form DNA. origin of the reference frame and its three orthogonal di- Double and single-crossovers are treated explicitly by con- rections:
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