
7.2. Variations on a Theme 215
It has also been suggested that longitudinal deformations of DNA might be
associated with many DNA/protein binding events, such as DNA binding to the
TATA-box binding protein TBP (where DNA is locally compressed, strongly bent,
and unwound) and DNA binding to nucleosomes [1050], where variable lengths
of DNA associated with nucleosome wrapping might accommodate sequence and
ionic variations [678].
More generally, single-molecule biochemistry experiments help investigate the
energetics and dynamics of folding and unfolding, the stability of various 2D and
3D intermediates, conformational landscapes, and folding pathways.
Box 7.2: Modeling Overstretched DNA
Results of modeling studies of overstretched DNA — by energy minimization or molec-
ular dynamics — are protocol dependent. For example, results and interpretations depend
on which end of the DNA is pulled, what minimization method is used, how minimization
is implemented (e.g., how fine the helical rise increments are), what force field is em-
ployed, and how solvent is treated.
The minimization work of Lavery and coworkers [711] suggested that the stretched con-
formation may be a flat, unwound duplex or a narrow fiber with substantial bp inclination
[711]. The molecular dynamics simulations of Konrad and Bolonick [671] reproduced the
helix to ladder transition and analyzed the geometric and energetic properties stabilizing
the S-ladder. The constrained minimization studies of Olson, Zhurkin and coworkers [678]
produced a wealth of structural analyses for both compressed and stretched DNA duplexes
(from 2 to 7
˚
A per bp) of poly(dA)·poly(dT) and poly(dG)·poly(dC) homopolymers under
high and low salt conditions. It was found that DNA can stretch to about double, and
compress to half, its length before the internal energy rises sharply. Energy profiles span-
ning four families of right-handed structures revealed that DNA extension/compression
deformations can be related to concerted changes in rise, twist, roll, and slide parameters.
The lowest energy configurations correspond to canonical A and B-DNA. These models
may be relevant to nucleoprotein filaments between bacterial Rec-A-like proteins and
overstretched, undertwisted DNA [349].
Such fascinating single-molecule biochemistry manipulations have also shown that un-
der much smaller forces (<3 pN), a new DNA phase is achieved, with about 2.6 bps/turn
and thus about 75% more extended than B-DNA [21]. This new DNA conformation,
termed P-DNA (for Pauling, see below), occurs at moderate positive supercoiling for
molecules that cannot relieve the torsional stress via writhing (nonplanar bending). (For
negative supercoiling, DNA denatures in this force range). Intriguingly, some modeling
suggests that such a structure is ‘inside-out’, with bases on the helical exterior and the
sugar/phosphate backbone at the center, as Linus Pauling once suggested for the structure
of the double helix based on a model with un-ionized bases [975]. Such a conformational
transition arrives from major rotation of torsion angles (notably α and γ,towardthetrans
conformation) and is compatible with both C2
-endo and C3
-endo sugar puckers. The
intrastrand P–P distances in P-DNA (around 7.5
˚
A) are larger than the corresponding
values in canonical A and B-DNA (5.8 and 6.6
˚
A, respectively). Evidence shows that this
P-DNA conformation is found in the packed DNA inside some virus complexes, where