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______________________________________________________________________ Introduction<br />

1.2.1 DNA in solution<br />

DNA is a highly charged polymer with charge density equal to two elementary charges per base<br />

pair. Therefore, in solution DNA interacts strongly with surrounding ions that counterbalance<br />

its charge. These ions can be grouped into different zones 31 . In the region closest to the DNA<br />

there are so called site-bound or inner-sphere ions that share water molecules with the DNA. In<br />

the following zone are outer-sphere ions (territorial ions) that keep their inner hydration layer<br />

and are free to move along the DNA molecule but are kept close to it due to the electrostatic<br />

field. And in the last zone are free ions that form an ionic cloud around the DNA 3 .<br />

The two most known approaches employed to investigate the extent of DNA-ion interaction are<br />

the Manning-Oosawa (MO) counterion condensation theory 32 and the Poisson-Boltzmann (PB)<br />

equation. MO theory addresses the DNA charge compensation by focusing on the counterions<br />

that form a so-called condensed layer around the DNA (outer-sphere ions) in order to reduce<br />

the charge density below a certain critical value 33 . According to the theory, counterion<br />

accumulation at the DNA surface forming a condensed layer occurs under the condition that<br />

the charge density parameter η is > 1:<br />

η = zl B<br />

b<br />

(1.4)<br />

where z is the valence of counterions, lB is the Bjerrum length and b is the charge separation.<br />

The Bjerrum length represents the distance between charges at which their electrostatic<br />

interaction energy equals the thermal energy and is defined as:<br />

l B =<br />

e 2<br />

4πεε 0 kT<br />

(1.5)<br />

where e is the elementary charge, ε is the dielectric constant of the solvent, ε0 is the vacuum<br />

permeability and kT is thermal energy scale. This means that the counterion condensation (for<br />

monovalent ions) occurs when the charge separation b is smaller than the Bjerrum length, which<br />

is true for both ss- and dsDNA. Namely, lB = 0.71 nm in aqueous solutions, while the charge<br />

separation is 0.43 nm in ssDNA and 0.34 nm in dsDNA 31 . According to the theory, condensed<br />

counterions are still assumed to be mobile 34 .<br />

1.2 DNA 9

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