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Copyright © 2013 American Scientific Publishers
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Printed in the United States of America
Journal of
Bioinformatics and Intelligent Control
Vol. 2, 316–320, 2013
polDNAmelt: Local Melting Within Polymeric DNA—An
Improved Method and Its Applications
Sankar Basu
1
and Dhananjay Bhattacharyya
2 ∗
1
Crystallography and Molecular Biology Division, Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Kolkata 700064, India
2
Computer Science Division, Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Kolkata 700064, India
Local pseudo-unimolecular partial melting in polymeric cellular DNA is very much different from
bimolecular comprehensive melting of short oligonucleotides in solutions. Several softwares esti-
mate the melting temperature pretty accurately for the latter case and are used routinely for primer
designing in PCR. However, the local partial melting in polymeric DNA involves the formation of
a short-lived interior bubble constrained by double helical DNA at both the ends and thus (i) the
melting-annealing transition becomes concentration independent and (ii) the fraying effect due to
dangling ends are ruled out. Based on these features, the current study appropriately modifies
the thermodynamic equations for calculation of local melting within polymeric DNA and incorpo-
rates them in a web-server (http://www.saha.ac.in/biop/www/db/local/nsdnamelt.html). Applications
of the method in validating annotated promoter sequences and origin of replication have also been
surveyed.
Keywords: T
m
, Local Pseudo-Unimolecular Partial Melting, Short-Lived Interior Bubble,
Concentration Independent Dna Melting, Fraying Effect.
We report the availability of a web-server, polDNAmelt
(http://www.saha.ac.in/biop/www/db/local/nsdnamelt.html)
to analyze local melting within polymeric DNA. Theoreti-
cal localization of melting nucleation sites distributed over
chromosomal double stranded DNA (ds-DNA) is crucial
to study since only the converted single stranded DNA is
active for most of the biochemical processes (e.g., repli-
cation, transcription, recombination, etc.). Local melting
within polymeric DNA with both the ends being held in
double helical conformation is significantly different from
melting of short oligonucleotides in solution. In either
case, the main forces stabilizing a ds-DNA are base pair-
ing and stacking interactions.
1
While there are two types
of Watson-Crick base pairs (bp) present in ds-DNA with
different hydrogen bonding strength, there are ten unique
stacking arrangements between any two consecutive base
pairs leading to ten different stacking energy increments.
Thus, different base pairing and stacking interaction ener-
gies across diverge sequences (of say, identical length)
require different amount of kinetic energies to transfer to
unstructured melted out conformations. These evolution-
arily conserved melting nucleation sites inhomogeneously
distributed throughout the genome, map to local minima
of stability with respect to their immediate neighboring
∗
Author to whom correspondence should be addressed.
sequences. Although one can determine T
m
considering
only Watson-Crick base pairing energy (i.e., GC con-
tent) in a sequence, inclusion of heterogeneous stacking
considerably improves agreements between theory and
experiment for long polymeric DNA.
2
Experimental char-
acterizations of duplex stability by (calorimetric and/or
spectroscopic) DNA-melting studies have worked out
several libraries of stacking-based melting thermodynamic
parameters.
2–11
Quite a few softwares and servers
12–16
are
available for prediction of melting temperature (T
m
of
short oligonucleotides using these libraries but their use to
determine sequence dependent local melting can be erro-
neous. The present study attempts to modify appropriate
thermodynamic equations for calculation of local melting
within long polymeric DNA and incorporates them in
polDNAmelt.
In a ds-DNA (devoid of mismatches), stacking occurs
between every two consecutive base pairs (Nearest Neigh-
bors: NN) once the Watson-Crick hydrogen bonding
donor–acceptor pairs are stereo-specifically positioned.
In the available libraries of stacking-based NN-step param-
eters (H
0
, S
0
, G
0
, the contribution of hydrogen bond-
ing is implicitly included. PolDNAmelt utilizes the library
derived by Santalucia
3
and adds these individual step
parameters (NN propagation energies) for each consecutive
NN-step along a polymeric DNA. This library is ‘a single
316 J. Bioinf. Intell. Control 2013, Vol. 2, No. 4 2326-7496/2013/2/316/005 doi:10.1166/jbic.2013.1058