Resolving the Structure of Viral Genomes with Atomic Resolution - - PowerPoint PPT Presentation
Resolving the Structure of Viral Genomes with Atomic Resolution - - PowerPoint PPT Presentation
Resolving the Structure of Viral Genomes with Atomic Resolution Aleksei Aksimentiev Department of Physics University of Illinois at Urbana-Champaign I use Blue Waters to understand molecular underpinnings of life build biologically
I use Blue Waters to …
… understand molecular underpinnings of life … build biologically inspired systems
DNA, the blueprint
Viral genome, the program of infection
Cryoem reconstruction with concentric rings (Evilevitch et al, UIUC)
http://darwin.bio.uci.edu/~faculty/wagner/hsv2f.html
Herpes virus (HSV)
Open questions:
- What is the 3D structure of the genome?
- How genome ejection is triggered and sustained?
- Can it be used as a drug target?
DNA is a highly charged polymer!
Same sign charges ….
- Same sign charges can
a0ract (in a medium) F F
- Same sign charges repel
(in vacuum) F F
DNA is surrounded by counter ions
+1e, sodium or potassium
+2e, magnesium or calcium +4e,spermine +3e,spermidine
EffecBve a0racBon between DNA is observed when counterions have charge ≥ 2e
All-Atom Molecular Dynamics Simulation of DNA Condensates
Classical Force Field
U(r) = X
bonds
kb(b − b0)2 + X
angles
kθ(θ − θ0)2 )2 + X
dihedrals
kφ(1 + cos(nφ − φ0)) # φ θ b
Bonded parameters from quantum mechanics
}
LJ parameters from experiments
+ X
non-bonded pairs i,j
4✏ij "✓ij rij ◆12 − ✓ij rij ◆6## + X
non-bonded pairs i,j
qiqj 4⇡✏0rij
}
Partial charges from quantum mechanics
Add 64 DNA helices Add polyamine cations (+4) Add 150 mM NaCl Add explicit water Solve the equation of motion (F= ma) under periodic boundary condition in all directions
DNA-confining wall of radius R
Apply a half-harmonic wall potential only to DNA
y (nm)
15-ns MD
Cross-sectional view of MD using CHARMM27
Na
Standard CHARMM & AMBER Force Fields Are Not Perfect for the Simulation of DNA Condensates
x (nm)
1
2 4 6
10
2 4 6
100 Pressure (bar) 30 25 DNA-DNA distance (Å) 1
2 4 6
10
2 4 6
100 Pressure (bar) 32 30 28 26 24 22 DNA-DNA distance (Å)
[Na] = 250 mM [Mg] = 20 mM
Rau et al. Rau et al.
CHARMM27 AMBER99 CHARMM27 AMBER99
Long-lasting contact ion pairs (CIP) between Na+ and phosphate stabilize contact DNA pairs.
2 4
1
2 4
10
2 4
100 Pressure (bar) 30 28 26 24 22 DNA-DNA distance (Å)
[spermine] = 2 mM
Todd et al.
C H A R M M 2 7 AMBER99
Due to excessive CIP formation, the simulations underestimate both inter-DNA distance and pressure in DNA array systems.
[Na] = 250 mM outside
Yoo & Aksimentiev, JPCL 2012
Harmonic wall
Rau et al, PNAS 1984 Todd et al, BJ 2008
Champaign-Urbana Non-Bonded FIX (CUFIX): Improved Lennard-Jones Parameters for CHARMM & AMBER
- “Much of what is known about association and
dissociation of solutes and ions comes from measurements of colligative properties” — Molecular driving forces by Dill & Bromberg.
- 4
- 2
2 4 1.2 1.0 0.8 0.6 0.4 0.2 0.0 Density (g/cm
3)
Na Acetate Water Total
Na
≈
Dimethylphosphate Acetate
Yoo & Aksimentiev, JPCL 2012 Yoo & Aksimentiev, JCTC 2016 Yoo, Wilson & Aksimentiev, Biopolymers 2016
200 150 100 50 OSM pressure (bar) 4 3 2 1 molal conc (m) 200 150 100 50 4 3 2 1
Murad & Powles, JCP 1993 Luo & Roux, JPCL 2010
0.20 0.15 0.10 0.05 0.00
- 0.05
- 0.10
ULJ (kcal/mol) 4.0 3.6 3.2 2.8 Na–O distance (Å) 0.20 0.15 0.10 0.05 0.00
- 0.05
- 0.10
4.0 3.6 3.2 2.8
Standard rmin = 3.11 Å rmin = 3.20 Å Standard NBFIX
CUFIX for CHARMM36 & AMBER99
Effectively infinite slab under PBC
- Exp. from Robinson 1959
http://bionano.physics.illinois.edu/CUFIX
Yoo & Aksimentiev, JPCL 2012
1
2 4 6
10
2 4 6
100 Pressure (bar) 32 30 28 26 24 22 DNA-DNA distance (Å) 1
2 4 6
10
2 4 6
100 Pressure (bar) 30 25 DNA-DNA distance (Å)
CUFIX Improves Simulations of DNA Condensates
- 120
- 80
- 40
40 80 120 y (Å)
- 120 -80
- 40
40 80 120 x (Å)
- 120
- 80
- 40
40 80 120 y (Å)
- 120 -80
- 40
40 80 120 x (Å)
- 120
- 80
- 40
40 80 120 y (Å)
- 120 -80
- 40
40 80 120 x (Å)
[Na] = 250 mM [Mg] = 20 mM [spermine] = 2 mM
AMBER99 AMBER99
2 4
1
2 4
10
2 4
100 Pressure (bar) 30 28 26 24 22 DNA-DNA distance (Å)
A M B E R 9 9
A M B E R 9 9 + C U F I X AMBER99 + CUFIX
Yoo & Aksimentiev, NAR 2016
A M B E R 9 9 + C U F I X ( M D i n c l u d e d 2 m M N a )
CHARMM27 CHARMM27 CHARMM27
DNA is packaged by a motor
At higher forces, DNA will deform Packaging process is slow (~min), all-atom simulation at physiological forces is not possible Can one simulate the process? Takes about 3 minutes to pack DNA 130 times longer than the capsid ! Max Force: 100pN Movie: Carlos Bustamante Lab
Strategy: change resolution for speed and detail
Strategy: change resolution for speed and detail
Strategy: change resolution for speed and detail
Strategy: change resolution for speed and detail
Strategy: change resolution for speed and detail
Strategy: change resolution for speed and detail
500 bp dsDNA fragment modeled at different resolutions
24 bp/2 beads 12 bp/2 beads 6 bp/2 beads 3 bp/2 beads 1 bp/2 beads All-atom, ~100 bp
Interactions in a simple coarse-grained DNA model
Interactions in a simple coarse-grained DNA model
Bond potential
r0 = nbp × 3.4 ˚ A f0 = 1000pN kspring = f0/r0 Elastic constant r0
Force Extension
http://www.phys.ens.fr/~cocco/Art/24physworld.pdf
Interactions in a simple coarse-grained DNA model
Angle potential
Persistence length s
Lp = 50 nm
e−s/Lp = ⟨cos θ⟩ = ∫𝕐 d𝕐 cos θ δ(θ′[𝕐] − θ)e−βU[𝕐] ∫𝕐 d𝕐 e−βU[𝕐] = ∫
π 0 sin θ dθ cos θe−β 1
2 kspringθ2
∫
π 0 sin θ dθ e−β 1
2 kspringθ2
Interactions in a simple coarse-grained DNA model
90°
φ
Dihedral angle potential
Twist persistence length Ltw = 90 nm hcos φi = es/Ltw Z π dφ cos φ e
kdihed(φ−φ0)2 2kBT
= es/Ltw φ0 = s ⇥ 10.14/˚ A
Interactions in a simple coarse-grained DNA model
4 nm cutoff
z Periodic in axial axis
Pr
Interactions in a simple coarse-grained DNA model
4 nm cutoff
80 80 4 bp/
Optimized to reproduce Rau & Parsegian pressure Half-harmonic wall to prevent strand crossing
Mapping between coarse-grained resolutions
For each helix, fit a 3D spline through bead coordinates at end of simulation
coordinate 1D spline
Fit a spline between quaternion representation of rotations
Packaging viruses with ARBD
ARBD: Atomic Resolution Brownian Dynamics (multi-resolution)
Package DNA (CG) with ARBD, into CryoEM reconstruction of a HK97 bacteriophage capsid. A cryoEM map of the portal is fitted into the original capsid reconstruction, and DNA is packaged through the portal.
Smooth, purely repulsive grid-based potential obtained by blurring cryoEM density and adding the portal
MulB-resoluBon packaging dsDNA viruses
Internal pressure during packaging
27
Pressure (atm) Percent of DNA
- utside capsid, %
Evilevitch et al, PNAS
Comparison to structural data
28
Simulation Experiment
- J. Mol. Biol. (2009) 391, 471-483, Hendrix et al
Cryo-electron microscopy q [Å−1]
experiment simulation
I(q) [a . u.] Small Angle X-ray Scattering
Experiment: Journal of molecular biology, 408: 541 (2011)
Simulation SAXS data were generated from CRYSOL, using an atomistic PDB of the protein coat and packaged DNA
Conclusions and outlook
29
Obtained first atomic-resolution structure of packaged viral particle Developed accurate multi-resolution representation of DNA—DNA and DNA—protein interactions To do: Extend the model to ssRNA and ssDNA viruses
Acknowledgements
- Funding through CPLC
- Computations
Jejoong Yoo David Winogradoff Chris Maffeo Kush Coshic