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Algorithm
of Melting Temperature
The
melting temperature, Tm, is defined as the temperature at which half of the
strands are in the double-helical state and half are in the "random-coil" state.
The melting temperature of an oligonucleotide is its most critically important
value. The most reliable and accurate determination of melting temperature is
determined empirically. However, this is cumbersome and not usually necessary.
Several useful, handy formulas have been developed to provide the Tm for PCR,
Southern and Northern blots, and in situ hybridization.
The
main factors affecting Tm are salt concentration, strand concentration, and the
presence of denaturants. Other effects such as sequence, length, and
hybridization conditions can be important as well.
a)
Basic Calculation
The
simple estimation of Tm is based on the number of each nucleotide within the
sequence.
(Eq.1)
where
,
,
,
are the number
of the bases A, T(U), G, C in the sequence, respectively.
This
equation was developed for short DNA oligos of 14-20 base pairs hybridizing to
membrane bound DNA targets in 0.9M NaCl.
For
sequences longer than 14 nucleotides, the equation used is
(Eq.2)
b)
Algorithm with Salt Adjustment
The
equation for DNA oligo shorter than 14 bases is:
(Eq.3)
For
DNA oligos longer than 14 nucleotides and pH from 5 to 9, the following formula
turns out to be appropriate:
(Eq.4)
The
nearest-neighbor (NN) algorithm for nucleic acids assumes that the stability of
a given base pair depends on the identity and orientation of neighboring base
pairs. The application of the NN model to nucleic acids was pioneered by
Zimm [1] and by Tinoco and coworkers [2]. Subsequently, several
experimental and theoretical papers on DNA and RNA NN thermodynamics have
appeared [3-4]. There has been disagreement concerning a number of issues,
particularly differences between DNA polymer and oligonucleotide NN
thermodynamic trends and the salt dependence of nucleic acid denaturation. A
unified view of polymer, dumbbell, and oligonucleotide DNA nearest-neighbor
thermodynamics was shown by SantaLucia[5]. We adopt the algorithm and
parameters shown in SantaLucia 1998.
For
self-complementary oligonucleotide duplexes, the Tm is calculated from the
following thermodynamic equation:
(Eq.5)
where
(Kcal/mol) is the sum of the nearest neighbor enthalpy
changes for hybrids;
is the sum of the nearest neighbor entropy
changes(cal/k.mol); R is the Gas Constant (1.987 cal/K.mol); C is the parameter
associated with the total oligonucleotide strand concentration. If the strand is
self complementary,
(Eq.6)
where
is the total
molar concentration of strands.
The
basic calculation of
and
is based on NN
parameters [Table
1].
A
correction of entropy without modification of enthalpy was suggested in
SantaLucia 1998 as follows,
(Eq.7)
where
is the total
entropy with [Na+]=1M; N is the length of the duplex.
It is important to realize that the nearest-neightbor approach has been established on small oligonucleotides. Therefore the use of Eq.5-7 in the non-approximate mode is really accurate only for relatively short sequences (<60bs).
Table
1. Unified
oligonucleotide
H
and
S
NN parameters in 1 M NaCl
|
Sequence |
|
|
|
AA/TT |
|
|
|
AT/TA |
|
|
|
TA/AT |
|
|
|
CA/GT |
|
|
|
GT/CA |
|
|
|
CT/GA |
|
|
|
GA/CT |
|
|
|
CG/GC |
|
|
|
GC/CG |
|
|
|
GG/CC |
|
|
|
Init.
w/term. G·C |
0.1 |
|
|
Init.
w/term. A·T |
2.3 |
4.1 |
|
Symmetry
correction |
0 |
|
1. Crothers, D. M. & Zimm, B. H.
(1964). J. Mol. Biol. 9, 19.
2. Uhlenbeck, O. C., Borer, P. N.,
Dengler, B., & Tinoco, I., Jr. (1973). J. Mol. Biol. 73,
483-496.
3. Breslauer, K. J., Frank, R.,
Blocker, H., & Marky, L. A. (1986). Proc. Natl. Acad. Sci. USA 83,
3746-3750.
4. Sugimoto, N., Nakano, S., Yoneyama,
M., & Honda, K. (1996). Nucleic Acids Res. 24, 4501-4505.
5. John SantaLucia, JR.(1998).Proc.
Natl. Acad. Sci. USA 95 (4), 1460-1465.