D. Porschke et al., STRUCTURE AND DYNAMICS OF CURVED DNA FRAGMENTS IN SOLUTION - EVIDENCEFOR SLOW MODES OF CONFIGURATIONAL TRANSITIONS, Biophysical chemistry, 47(2), 1993, pp. 179-191
DNA fragments with unusually low electrophoretic mobility due to intri
nsic curvature have been analyzed by comparison of electrooptical data
with results of hydrodynamic simulations. Electrooptical data have be
en collected for three fragments with 161, 196 and 399 base pairs deri
ved from the DNA of Chironomus thummi thummi as repetitive elements by
Alu I restriction. The dichroism decay time constants reflecting over
all rotational diffusion, the bending time constants and the bending a
mplitudes measured at low salt concentrations (2.4 mM Na+ and 100 muM
Mg2+) are rather close to those observed for standard DNA fragments. A
t high salt concentration (0.1 M Na+ and 10 mM Mg2+) the temperature d
ependence of the overall rotational time constants indicates a slightl
y increased degree of curvature at low temperature (2-degrees-C). The
experimental data are complemented by hydrodynamic simulations based o
n predictions of DNA trajectories given by Bolshoy et al. [Proc. Natl.
Acad. Sci. USA 88 (1991) 2312]. These trajectories are converted into
bead models, which are then subjected to thermal fluctuations using a
Monte Carlo procedure. For standard values of the persistence length
and the torsional flexibility, thermal fluctuations induce considerabl
e variations of the equilibrium curvature. As a first attempt to find
conditions where the predicted trajectories are consistent with our hy
drodynamic data, we tested a model with a high internal mobility, whic
h has been commonly applied for standard DNA fragments. However, the o
verall rotational time constants predicted for this case are clearly s
maller than the observed ones, even at high values of the persistence
length. Then, we simulated time constants in the limit of low internal
mobility by calculation of electrooptical transients for large number
s of individual configurations. The average of these transients could
be fitted by two exponentials at high accuracy, although the simulatio
ns led to broad distributions of configurations. In this respect the s
imulated curves are very similar to the experimental ones. For standar
d values of the persistence length and of the torsional flexibility, t
he large time constants tau2, reflecting overall rotational diffusion,
are still smaller than the experimental ones. Tau2-values simulated a
s a function of the persistence length p show a maximum, which appears
at p almost-equal-to 1000 angstrom for the Alu-fragments. The tau2-va
lues simulated at these maxima are consistent with the experimental on
es within the limits of accuracy. Thus, provided that the curvature ha
s been estimated correctly by the model based on gel mobilities and on
circularization experiments curved DNA fragments show a relatively lo
w rate of the internal dynamics and also appear to be less flexible th
an standard DNA's with respect to the dynamic persistence. The differe
nce in the dynamic persistence is negligible, however, if the apparent
persistence length of standard DNA has a major contribution from intr
insic curvature, corresponding to an average static persistence length
of about 800 angstrom. In summary, our results indicate that the ''de
viations from linearity'' of our curved fragments are not much differe
nt from those of standard DNA's; however, our results are consistent w
ith the view that curved DNA fragments are ''curved'' preferentially i
n one direction with relatively slow modes of configurational transiti
ons and with a relatively high rigidity, whereas standard DNA is subje
ct to bending by thermal motion in all directions with (almost) equal
probability.