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3.3DNAunderMechanicalStress
number of water molecules, depending upon the length of DNA, were replaced
with sodiumcounterions toneutralize thenegatively chargedDNAbackbones.
ClassicalMDsimulationswereperformedwith theparm99/BSC0 force-field,[111–
113] and theparameterizationbyÅqvistwasapplied todescribe theNa+ counter-
ions.[114] The topologieswere createdwithAmberTools[115] andconverted to the
Gromacs formatwithAmbconv.[116]All simulationswereperformedwith a time
step of 2 fs with LINCS[117] to constrain the bonds involving hydrogen to their
reference lengths. Pilot calculations,performedonnucleobases in thegasphaseas
well as ona solvatedoligonucleotides, showed that these constraints affect neither
the ionization potentials of the nucleobases nor the electronic couplings between
them. The Lennard-Jones interactionswere cut off at 1 nm, and the electrostatics
were treatedwith theparticle–meshEwaldmethod [52].
The prepared systems were equilibrated in a multi-step procedure. First of all,
a steepest-descentsminimizationwas performed for 100 steps to removepossible
badcontacts. Subsequently, the initialvelocities forallatomswererandomlydrawn
from a Maxwell–Boltzmann distribution at 10K. The water was heated up first
in an NVT simulation of 20 ps length. Here the DNA was weakly coupled to a
bath at 10Kand the solvent coupled to a separate bath at 300K. The Berendsen
thermostat was used for this purpose.[57] After that, anotherNVT simulation of
20ps lengthwasused tobring the entire system to 300K,with a singleheat bath.
Finally, anNPT simulation at 300Kand 1barwasperformedover the interval of
0.5ns. TheNosé–Hoover extended-ensemble thermostatwith a characteristic time
of 0.5pswas used to keep the temperature of 300K.[58, 59] InNPT simulations,
the Parrinello–Rahman barostatwith characteristic time of 0.5ps and a reference
pressure of 1 barwas used.[60] The consecutive production simulationswere run
with the same parameters as the last equilibration step. The Gromacs package
(versions4.0and4.5)[118,119]wasused for all simulations.
3.3 DNAunderMechanicalStress
EachDNAspecieswas stretchedbypulling its3’-ends inoppositedirections. This
setupwas inspiredbytheexperimentswhere the3’-endsofdsDNAwerecontacted
to the electrodes. To do so, an additional force along the z-axis of the simulation
45
Charge Transport in DNA
Insights from Simulations
- Title
- Charge Transport in DNA
- Subtitle
- Insights from Simulations
- Author
- Mario Wolter
- Publisher
- KIT Scientific Publishing
- Date
- 2013
- Language
- English
- License
- CC BY-SA 3.0
- ISBN
- 978-3-7315-0082-7
- Size
- 17.0 x 24.0 cm
- Pages
- 156
- Keywords
- Charge Transport, Charge Transfer, DNA, Molecular Dynamics, Quantum Mechanics
- Categories
- Naturwissenschaften Chemie
Table of contents
- Zusammenfassung 1
- Summary 3
- 1 Introduction 5
- 2 TheoreticalBackground 11
- 3 SimulationSetup 39
- 4 DNAUnderExperimentalConditions 49
- 5 ChargeTransport inStretchedDNA 69
- 6 ChargeTransport inMicrohydratedDNA 79
- 7 AParametrizedModel toSimulateCT inDNA 89
- 8 Conclusion 105
- Appendix 111
- A DNAUnderExperimentalConditions 111
- B CTinMicrohydratedDNA 117
- List ofPublications 137