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J Biol Chem, Vol. 274, Issue 47, 33601-33608, November 19, 1999
Interactions of the Major Cold Shock Protein of Bacillus
subtilis CspB with Single-stranded DNA Templates of Different
Base Composition*
Maria M.
Lopez ,
Katsuhide
Yutani§, and
George I.
Makhatadze ¶
From the Department of Chemistry and Biochemistry,
Texas Tech University, Lubbock, Texas 79409-1061 and the
§ Institute for Protein Research, Osaka University, 3-2 Yamadaoka, Suita, Osaka 565-0871, Japan
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ABSTRACT |
CspB is a small acidic protein of Bacillus
subtilis, the induction of which is increased dramatically in
response to cold shock. Although the exact functional role of CspB is
unknown, it has been demonstrated that this protein binds
single-stranded deoxynucleic acids (ssDNA). We addressed the question
of the effect of base composition on the CspB binding to ssDNA by
analyzing the thermodynamics of CspB interactions with model
oligodeoxynucleotides. Combinations of four different techniques,
fluorescence spectroscopy, gel shift mobility assays, isothermal
titration calorimetry, and analytical ultracentrifugation, allowed us
to show that: 1) CspB can preferentially bind poly-pyrimidine but not
poly-purine ssDNA templates; 2) binding to T-based ssDNA template
occurs with high affinity (Kd(25 °C) 42 nM) and is salt-independent, whereas binding of CspB
to C-based ssDNA template is strongly salt-dependent (no
binding is observed at 1 M NaCl), indicating large
electrostatic component involved in the interactions; 3) upon binding
each CspB covers a stretch of 6-7 thymine bases on T-based ssDNA; and
4) the binding of CspB to T-based ssDNA template is enthalpically
driven, indicating the possible involvement of interactions between
aromatic side chains on the protein with the thymine bases. The
significance of these results with respect to the functional role of
CspB in the bacterial cold shock response is discussed.
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INTRODUCTION |
An important characteristic of living cells is their ability to
survive under extreme conditions such as chemical stress and heat or
cold shock. Although much knowledge has accumulated on the mechanism of
the heat shock response, the cold shock response of living cells was
discovered only a decade ago (1-3). When the temperature is shifted
from 37 to 10 °C, bacterial cells express a specific subset of
proteins (2). This subset in Escherichia coli consists of
more than 14 different proteins involved in various cellular processes
and includes NusA, IF2, polynucleotide phosphorylase, RecA, H-NS, GyrA,
RbfA, and several other unidentified proteins (3, 4). The dominant
fraction of this subset is the so-called major cold shock protein CspA,
a protein of 70 amino acid residues (4). Its induction level increases
dramatically (5) even under conditions that completely block protein
synthesis (6). Using the cspA gene as a probe, several other
homologous genes named cspC, cspD,
cspE, cspF, cspG, cspH, and
cspI have been identified; however, only some of these genes
code for cold shock-inducible proteins (7-10). The set of cold shock
proteins first discovered in E. coli have been found in
other bacteria (3, 11, 12) and are highly homologous to the eukaryotic
Y-box transcription factors (13-15).
The cold shock response in Bacillus subtilis is also
accompanied by an increased levels in CspB, a small acidic protein
highly homologous to CspA of E. coli (16). The biological
function and induction mechanism of the CspB protein is not yet clear; however, preferential binding to particular single-stranded DNA (ssDNA)1 sequences has been
demonstrated (17). The structure of CspB has been determined both in
crystal (18) and in the solution (19) and consists of five -strands
organized into an antiparallel -barrel. Six aromatic residues
(Phe15, Phe17, Phe27,
Phe30, Phe38, and Trp8) and five
positively charged amino acid residues (His29,
Lys7, Lys13, Lys39, and
Arg56) are located on the same side of the CspB molecule.
Amino acid substitutions at these positions have pronounced effects on
CspB binding to ssDNA as measured in gel retardation experiments (17). The ssDNA binding activity of CspB has been tested exclusively in gel
retardation experiments. These results have established that there is
preferential binding of the protein to the ssDNA containing Y-box
sequence ATTGG (20). Subsequent experiments have shown that binding of
CspB to ssDNA is not limited to ATTGG; however, no unique recognition
sequences have been identified (17).
In this paper we studied the interactions of the B. subtilis
major cold shock protein CspB with ssDNA templates addressing the
question of whether these interactions depend on the base composition
of the template. Using a combination of four different techniques
(fluorescence spectroscopy, gel shift mobility assay, isothermal
titration calorimetry, and analytical ultracentrifugation) we show that
CspB has a preference for polypyrimidine ssDNA templates. CspB seems to
bind both C- and T-based ssDNA templates; however, the underlying
mechanisms of these interactions appear to be very different. Binding
of CspB to C-based ssDNA is strongly salt-dependent, indicating the involvement of a large electrostatic component in the
interactions. In contrast, interactions of CspB with T-based ssDNA
templates are independent of salt concentration and are characterized
by an apparent binding constant in the nanomolar range.
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EXPERIMENTAL PROCEDURES |
Purification of CspB and ssDNA Templates--
Protein
purification was modified from that described previously (21). Briefly,
CspB was purified from E. coli strain BL21 (DE3) (22), which
contained the overexpression plasmid pCSPB3 carrying the gene of CspB
under control of the T7 RNA polymerase promoter. Cells were grown to an
optical density ~0.8 optical units at 600 nm at 37 °C in 2× YT
medium containing 100 µg/ml ampicillin. CspB production was induced
by addition of isopropyl- -D-thiogalactopyranoside (final
concentration, 1 mM) and incubated for 5 h. Cells were harvested by centrifugation at 7,500 × g. The cell
pellet was resuspended in 20 mM Tris, pH 7.5, 1 mM EDTA, 2 mM dithiothreitol, and passed twice
through a French pressure cell. Cellular debris was removed by
centrifugation at 40,000 × g at 4 °C. The
supernatant was diluted with an equal volume of resuspension buffer and
applied on Fast Flow Q-Sepharose column (2 × 10 cm). After
washing, the bound protein was eluted in a linear salt gradient (0-0.5
M NaCl). The CspB-containing fractions were eluted at
~150 mM NaCl, dialyzed against water, and lyophilized.
Lyophilized protein was dissolved in 50 mM Tris-HCl, pH
7.5, 100 mM KCl and applied on a Sephadex G-50 column
(2.5 × 100 cm) equilibrated with the same buffer and eluted from
the column. The CspB containing fractions were dialyzed extensively
against water, lyophilized, and stored at 20 °C. The purity of the
protein was higher that 95% as judged from Coomassie staining of
SDS-polyacrylamide gels. The concentration of CspB was measured
spectrophotometrically using the extinction coefficient 280 = 5690 M 1
cm 1 (23). Corrections for light scattering were taken
into account as described (24).
Purification of ssDNA Templates--
The ssDNA
oligodeoxynucleotides were purchased from Biosynthesis Inc.
(Lewisville, TX) and purified on a Mono-Q column (HR 10/10, Amersham
Pharmacia Biotech) equilibrated in 10 mM Tris-HCl, pH 7.0, 1 mM EDTA, and 20% acetonitrile. The ssDNA bound to the column was eluted with a shallow salt gradient prepared from
equilibration buffer and equilibration buffer containing 1 M NaCl. The fractions of interest, eluted at ~0.5
M NaCl, were dialyzed against water and lyophilized.
Lyophilized ssDNA was dissolved in 50 mM Tris-HCl, pH 7.5, 0.2 mM EDTA, dialyzed against the same buffer, aliquoted in
small volumes, and stored at 20 °C. The ssDNA concentration was
calculated from the absorbance at 260 nm. The extinction coefficients for individual ssDNA were estimated using the following extinction coefficients for individual nucleotides (25): 8,400 M 1 cm 1 (dT), 12,010 M 1 cm 1 (dG), 7,050 M 1 cm 1 (dC), and 15,200 M 1 cm 1 (dA). Because
guanine-based oligodeoxynucleotides are known to form oligomers, only a
limited number of experiments were performed using 23G and 23pG templates.
Fluorescence Measurements--
Fluorescence intensity was
measured using a FluoroMax spectrofluorometer with DM3000F software.
Constant temperature during the experiments was maintained using a
thermostated cell holder connected to a circulated water bath. The CspB
concentration was 0.3 µM (equilibrium titrations) or 14 µM (stoichiometric titrations) in 50 mM
Tris-HCl pH 7.5 buffer, containing either 100 mM NaCl (normal experimental conditions) or 1 M NaCl (high salt
buffer). Tryptophan fluorescence was excited at 287 nm (under
equilibrium conditions) or 300 nm (under stoichiometric conditions),
and the emission was recorded at 349 nm. The experiments were performed at 25 °C (when not otherwise specified), and the initial volume in
the cuvette was 1.1 ml. The solution was gently stirred during the
titration, and the measured intensity values were corrected for sample
dilution. Inner filter effects were taken into account, and blanks were
subtracted. Because it is known that poly(dG) can form oligomers, the
control experiments at lower concentrations of G-based templates have
been performed, but no difference was found.
Gel Shift Assays--
150 pmol of ssDNA were 5' 32P
end-labeled by incubating templates with T4 polynucleotide kinase (3 µl), T4 polynucleotide kinase buffer (New England Biolabs), and 0.03 mCi of [ -32P]ATP (NEN Life Science Products) in a
total volume of 60 µl at 37 °C for 1 h. The reaction was
stopped by heat inactivation (30 min at 65 °C). Unincorporated
[ -32P]ATP was removed with QIAquick Nucleotide Removal
Kit (Qiagen). The binding reaction was routinely performed by
incubating 10 pmol of labeled ssDNA with different amounts of protein
(total volume, 25 µl) at room temperature for 25 min in binding
buffer (20 mM Tris, pH 8.6, 50 mM NaCl, and 5 mM MgCl2); however, incubation for shorter (10 min) or longer (60 min) periods of time did not produce appreciable
changed in the retardation patterns. 5 µl of dye solution (20%
glycerol, 0.034% bromphenol blue) were added to the samples prior to
gel electrophoresis. The electrophoresis was performed in TBE (89 mM Tris, 89 mM boric acid, 2 mM
EDTA, pH 8.0) buffer through a 22.5% acrylamide gel at 75 volts until the samples had entered the gel and then at 100 volts overnight. Autoradiograms were obtained by exposing gels to a Kodak MR-2 film for
0.5-2 h at room temperature.
Isothermal Titration Calorimetry--
ITC experiments were
performed using a titration microcalorimeter (MicroCal Inc.,
Northhampton, MA). Protein and ssDNA were dialyzed simultaneously in 50 mM Tris, pH 7.5, 100 mM NaCl buffer. The
protein concentration was 14 µM in a 1.34-ml cell volume, and 4 µl of ssDNA were sequentially injected into the protein solution until no further heat effects were observed. As a control, identical additions of ssDNA were injected into the buffer to measure
the heat of dilution. The heat of the reaction was obtained by
integrating the peak after each injection of ssDNA ligand using Origin
software provided by the manufacturer. Because the CspB-ssDNA binding
was stoichiometric under our experimental conditions, Hcal was calculated by summing individual
heat increments and dividing by the total number of moles of CspB
present in the solution. Thus Hcal is
expressed per mole of CspB molecules.
Analytical Centrifugation Experiments--
Analytical
centrifugation experiments were performed in a Beckman XL-A centrifuge.
For each run three cells were used: one containing ssDNA only (2 µM for 23pT or 2.5 µM 23pC), another with
CspB only (20-fold higher protein concentration than ssDNA), and a
third containing CspB-ssDNA complex with the same concentrations of
CspB and ssDNA as in the other cells. The CspB-ssDNA complex was formed
by incubating CspB and ssDNA at room temperature for 25 min prior to
each run. The runs were performed at 4 °C under different speed
(20,000 or 25,000 rpm) for 10 h. Absorbances were recorded
simultaneously at 260 and 280 nm during the runs. The partial molar
volumes for CspB, ssDNA (23pT and 23pC), CspB-23pT complex, and
CspB-23pC complex were 0.74, 0.55, 0.69, and 0.65 cm3/g,
respectively, calculated as described (26-28). Analysis of the data
was performed using the Beckman supplied script for Origin (MicroCal
Inc.) software.
Analysis of Binding Isotherms--
The binding isotherms
obtained by monitoring the changes in the fluorescence intensity upon
titration of CspB with ssDNA template was analyzed according to the
following classical binding equation (29).
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(Eq. 1)
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where A = [CspB]Total + np·[ssDNA]Total + 1/Kaind, Q is the
quenching effect of CspB Trp fluorescence intensity after each addition of ssDNA, Qmax is the maximum quenching obtained
upon complete saturation of the protein with ssDNA,
[CspB]Total and [ssDNA]Total are the total
concentrations of protein and ssDNA in solution, respectively,
Kaind is the equilibrium
association constant for the CspB-ssDNA interactions, and
np is the number of molecules of CspB bound per
molecule of ssDNA. One needs to keep in mind that for protein-DNA
interactions when more than one molecule of protein binds to DNA, the
Kaind obtained from Equation 1 represents an apparent equilibrium constant because this model does
not consider the degeneracy of the binding site on nucleic acid. In the
case of single binding site, this binding model is exact and has been
successfully used for the analysis of protein-ssDNA interactions
(30).
Data analysis was also performed according to the model originally
introduced by Epstein (31). This model is a particular case of the
model of McGhee and von Hippel (32) for the short templates and takes
into account the fact that for homogeneous template the binding site
can be formed by any continuous segment with a given number of bases.
According to Epstein (31), the fractional saturation of the lattice
( ) is defined as follows.
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(Eq. 2)
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where n is the binding site size, M is the
length of the ssDNA, and is the average number of
bound ligands expressed as follows.
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(Eq. 3)
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where k, g, and j represent the
number of ligands bound, the maximum number of ligands that can bind to
the lattice, and the number of adjacencies, respectively.
KaEps and are the
equilibrium association constant and the cooperativity parameter for
the interaction, respectively. Finally, PM is
the number of distinct ways that k n-site ligands
may bind to an M-site lattice with j adjacencies and is
calculated as follows.
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(Eq. 4)
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is related to the binding density of the ligand on the
lattice, (in mole of ligand per mole of nucleotide base), as shown in Equation 5 (33).
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(Eq. 5)
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where relates to the quenching as follows.
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(Eq. 6)
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Combining Equations 2, 5, and 6 we obtain
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(Eq. 7)
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where Q, [CspB]Total, and
[ssDNA]Total are experimentally attainable parameters.
Fit of the experimental data to Equation 7 was performed using a
nonlinear least square software package NLREG.
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RESULTS |
CspB-ssDNA Binding Monitored by the Trp Fluorescence
Quenching--
A number of aromatic (Trp8,
Phe17, Phe17, Phe27, and
Phe30) and basic (Lys7, Lys13, and
His29) residues of CspB have been proposed to be involved
in the interactions with the single-stranded DNA molecules (17, 34). Of
these, Trp8 presents a useful probe to monitor ssDNA-CspB
interactions by measuring the changes in the protein fluorescence
intensity as a function of ssDNA concentration. Fig.
1 presents changes in Trp fluorescence
intensity of CspB at 25 °C upon titration with three different
single-stranded oligodeoxynucleotides, 43YB+,
43YB , and 43NS (Table I).
These oligodeoxynucleotides represent shorter forms of the sequences
used previously in gel shift experiments (18-20). Based on these gel
shift mobility assays, it has been shown that CspB binds to ssDNA
containing the Y-box motif, with higher preference to the
(+)-strand-containing ATTGG core sequence than to the
(-)-strand-containing CCAAT core sequence or the "nonspecific" sequence that contains neither the ATTGG nor the CCAAT sequence. The
results presented in Fig. 1 agree with this conclusion, i.e. quenching CspB Trp fluorescence intensity occurs at lower
concentrations of 43YB+ than for 43YB or the
control nonspecific 43NS template. Nevertheless, all three single-stranded templates quench the CspB Trp fluorescence, thus indicating that CspB interacts with all three of them. This is in
agreement with the gel shift experiments in which just 2-3-fold higher
concentration of CspB was needed to observe complete retardation of the
YB and NS templates as compared with the YB+
template (18, 19).

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Fig. 1.
Changes in the fluorescence intensity of CspB
as a function of ssDNA template concentration. ,
43YB+; , 43YB ; , 43NS. A
shows the absolute values of the quenching of Trp fluorescence
intensity. B shows relative changes in the quenching of the
Trp fluorescence intensity. Solid lines drawn through the
points do not carry any meaning; they are intended to guide
the eye.
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To simplify the system, we synthesized four oligodeoxynucleotides in
which the core ATTGG sequence was positioned in the middle of a 23-mer
with nine flanking A, T, C, or G nucleotides on both sides,
i.e.
X9ATTGGX9, where
X = A, T, C, or G (see Table I for the nomenclature of
the oligodeoxynucleotides). The quenching effects on the CspB Trp
fluorescence intensity upon titration with 23T, 23G, 23C, or 23A at
25 °C are shown in Fig. 2A.
Surprisingly, under our experimental solvent conditions (50 mM Tris, 100 mM NaCl, pH 7.5) there is a
significant difference in the titration profiles. Changes in the
fluorescence quenching reach saturation at 0.2 µM of 23T
template. In the case of 23C ssDNA template saturation is reached at
>1 µM, whereas 23A and 23G templates do not produce changes in the fluorescence quenching of CspB (Fig. 2A). In
control experiments we measured the changes in the Trp fluorescence of CspB as a function of concentrations of A-, T-, G-, or C-based oligodeoxynucleotides that lacked the core ATTGG sequence,
i.e. 23pA, 23pT, 23pG, and 23pC (Table I). We observe that,
except for the 23C and 23pC, quenching of the protein Trp fluorescence is independent of the ATTGG core sequence (Fig. 2A).
Notably, the total quenching of CspB Trp fluorescence by 23T and 23pT
is much larger than for the other oligodeoxynucleotides and takes place
at very low ssDNA concentration. The lower quenching effect observed
for 23pC could be due to the stacking interactions of the C-bases at
the pH of our experiment (7.5) (35). However, fluorescence experiments
performed at pH 8.1, where no stacking is expected, did not differ from
the titration curve obtained at pH 7.5 (data not shown). The quenching
of fluorescence intensity of Trp8 does occur because of the
direct interactions of CspB with ssDNA templates. This can be
demonstrated by measuring the changes in the fluorescence intensity of
N-acetyl-tryptophan-amide upon addition of different amounts
of 23T, 23A, and 23C (up to 0.5, 0.9, and 1.4 µM,
respectively). Under the same experimental conditions titrations with
these ssDNA templates did not lead to appreciable quenching of
N-acetyl-tryptophan-amide fluorescence intensity (Fig.
2B). These results suggest that the quenching of the CspB intrinsic Trp fluorescence by ssDNA templates, as it was shown for
other protein-DNA complexes (36), is entirely due to direct interactions and does not have contribution from simple collision of
these molecules. Additional evidence for this conclusion follows from
the gel shift experiments.

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Fig. 2.
A, changes in the quenching of Trp
fluorescence intensity of CspB as a function of ssDNA template
concentration. , 23T; , 23pT; , 23C; , 23pC; , 23G; ,
23pG; , 23A; , 23pA. Template sequences are given in Table I.
B, changes in the quenching of Trp fluorescence of
N-acetyl-tryptophane-amide upon titration with ssDNA
templates 23T, 23C, and 23A. Symbols are the same as those
used in A. Solid lines drawn through the points
do not carry any meaning; they are intended to guide the eye.
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CspB-ssDNA Binding Monitored by Gel Shift
Electrophoresis--
Fig. 3 presents the
results of the mobility shift assay on nondenaturing polyacrylamide
gels for 23T, 23pT, and 23pC ssDNA templates. This assay allows
separation of free ssDNA from the CspB bound ssDNA by retardation of
electrophoretic mobility. CspB-ssDNA complexes were formed at varying
concentrations of CspB incubated with invariant amounts of 5'
32P-labeled ssDNA templates. Increase of the concentration
of CspB leads to appearance of the distinctly migrating band
corresponding to the CspB-ssDNA complex. It is evident that 23T and
23pT ssDNA templates behave almost identically (in agreement with the
fluorescence experiments; Fig. 2), and complete retardation is observed
at a CspB:ssDNA ratio of 8:1 (Fig. 3). On the other hand, when 23pC is
used as much as 200:1 ratio of CspB to ssDNA is required for complete
shift of the band corresponding to free ssDNA (Fig. 3). Similar
experiments using 23A as the template showed no appreciable ssDNA
retardation even at a 300:1 ratio (data not shown).

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Fig. 3.
Electrophoretic mobility shift assay.
Lane 1, CspB:23T = 2:1; lane 2,
CspB:23T = 8:1; lane 3, free 23T; lane 4,
CspB:23pT = 2:1; lane 5, CspB:23pT = 8:1;
lane 6, free 23pT; lane 7, CspB:23pC = 50:1;
lane 8, CspB:23pC = 200:1; lane 9, free
23pC. All lanes contained 10 pmol of 5' 32P-labeled 23pT,
23T, or 23pC template. Band B, CspB bound ssDNA; band
F, free ssDNA. See "Experimental Procedures" for
details.
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Comparison of the gel retardation experiments with the results of the
Trp fluorescence titration of CspB with ssDNA templates (Fig. 2) shows
that there is a clear correlation between these two data sets. The
degree of Trp quenching as a function of ssDNA concentrations
correlates well with the CspB-ssDNA ratio required for the complete
retardation in the gel shift assay, thus confirming that quenching of
the CspB intrinsic Trp fluorescence by ssDNA results from the direct
interactions of the ssDNA with the protein. It is also notable that the
T-based ssDNA templates 23T and 23pT behave similarly and seem to have
the highest affinity for CspB.
CspB-ssDNA Binding Monitored by ITC--
Further characterization
of the thermodynamics of formation CspB-ssDNA complexes was done using
ITC. This technique measures directly the heat of the interactions at a
given temperature. The change in the heat of the reaction as a function
of ligand concentration contains all the information on the
thermodynamic parameters of interactions in the system including the
stoichiometry and binding constant (67). Because in many cases the heat
of the reaction is relatively small, ITC experiments are generally performed at relatively high concentrations of protein or ligand. Fig.
4A presents the typical ITC
recording of 15 injections (4 µl each) of 23pT (220 µM)
into the cell containing 14 µM CspB at 25 °C. The
reaction is exothermic, and each addition of 23pT leads to a lower
amount of heat released until the reaction is saturated. After
integration of each peak and normalization for CspB concentration, the
heat of the reaction is plotted versus the ligand (ssDNA)
concentration (Fig. 4B). It is notable that in the case of
23pT the titration profile shown on Fig. 4B is very steep,
indicating that under these concentrations of CspB and 23pT binding is
stoichiometric (strong). This enables an estimate of the stoichiometry
of binding as the ssDNA to CspB ratio at which the break point on the
titration profile occurs. From the profile for 23pT-CspB shown on Fig.
4B, it appears that the break point occurs at the ration of
23pT to CspB of ~0.3, i.e. the stoichiometry of binding is
three molecules of CspB per one molecule of 23pT. This result was
corroborated by titration of the same concentrations CspB with 23pT
monitored by Trp fluorescence (Fig. 4C). The ITC and Trp
fluorescence titration profiles show perfect overlap if converted into
fractional saturation, indicating that both techniques follow the same
process and that the stoichiometry of 23pT-CspB interactions is indeed
three molecules of CspB bind one molecule of 23pT.

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Fig. 4.
Interactions of CspB with ssDNA templates as
monitored by ITC. A, typical titration data for 15 injections of 4 µl of 23pT (220 µM) into the cell with
14 µM CspB (line a) or without CspB
(line b). Buffer conditions 50 mM Tris, 100 mM NaCl, pH 7.5. B, enthalpy of CspB-23pT ( )
and CspB-23pC ( ) interactions as a function of ssDNA:CspB ratio.
C, comparison of fractions of CspB bound to ssDNA template
obtained with 14 µM CspB using ITC or fluorescence
spectroscopy. , 23pT; , 23pC; , 23pT; , 23pC.
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Additional evidence for a 3:1 stoichiometry of CspB-23T/23pT
interactions was obtained by analytical ultracentrifugation. The
analytical centrifugation experiments were performed simultaneously on
23pT template, CspB, and their mixture at a 20:1 ratio of CspB to 23pT
(Fig. 5). The average apparent molecular
mass of 23pT is 8.9 ± 0.5 kDa, which compares with the
theoretical molecular mass of 7.1 kDa. The average apparent molecular
mass for CspB under these conditions was found to be 8.8 ± 0.7 kDa, which is close to the expected molecular mass of 7.5 kDa
calculated from the amino acid composition. Under the same solvent
conditions (50 mM Tris, 100 mM NaCl, pH 7.5)
the average apparent molecular mass of the species formed in a solution
containing both CspB and 23pT was 37 ± 7 kDa. Using the average
apparent molecular masses of CspB and 23pT, this gives the
stoichiometry of the formed complex of 3.2 molecules of CspB per one
molecule of 23pT, identical to the results obtained by ITC and Trp
fluorescence spectroscopy. Considering the length of ssDNA template and
stoichiometry of binding, we can estimate the size of the CspB binding
site to be 6-7 T nucleotides.

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Fig. 5.
Interactions of CspB with ssDNA template as
monitored by analytical centrifugation on Beckman XL-A.
A shows representative data taken at 20,000 rpm. Different
symbols represent the data obtained simultaneously for CspB alone
( ), 23pT alone ( ), and for CspB-23pT mixture at a 20:1 ratio
( ). Solid lines represent the best fit of the data to the
following molecular masses: CspB, 8 700 Da; 23pT, 8 800 Da; CspB:23pT,
38,000 Da. Buffer conditions were 50 mM Tris, 100 mM NaCl, pH 7.5. B shows the residuals of the
fits shown in A using the same symbols.
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For comparison the ITC experiments were performed with 23pC template
(Fig. 4B). CspB binds 23pC and 23pT differently; the former
template produces a linear increase in the heat released upon binding
of CspB and possibly reaches saturation at a 23pC to CspB ratio above
2, whereas the latter template reaches saturation upon binding of CspB
at a 23pT to CspB ratio of 0.3. This result agrees with results of the
gel shift assays in which much higher amounts of protein were needed to
obtain complete retardation for 23pC compared with 23pT (Fig. 3). We
also observe that the total heat released upon binding of 23pC to the
protein is much lower than for 23pT, 25 kJ/mol for 23pC
versus 110 kJ/mol for 23pT.
The 23pC template also differs from 23pT in the stoichiometry of
binding to CspB. Analytical centrifugation experiments performed simultaneously on 23pC, CspB, and the 23pC-CspB complex show that under
our experimental conditions 23pC seems to form a 1:1 complex with CspB.
The average apparent molecular mass of 23pC from analytical centrifugation experiments was estimated to be 8.8 ± 0.7 kDa, which compares with the theoretical molecular mass of 6.8 kDa, keeping
in mind the possibility for this template to form sometimes oligomeric
structures (35). The average apparent molecular mass for CspB from this
set of experiments was found to be 7.9 ± 0.4 kDa. The average
apparent molecular mass of species formed in the solution containing
both CspB and 23pC was 17.6 ± 3 kDa, thus indicating that complex
consists of one molecule of CspB per one molecule of 23pC.
 |
DISCUSSION |
The use of spectroscopic methods for the analysis of protein-DNA
interactions requires the knowledge of the relationship between the
change in the spectroscopic signal and the extent of binding (36). In
many cases this information is not available and the model-independent
treatment of the data is required (36-38). Thus the relationship
between the change in the spectroscopic signal and the extent of
binding for CspB-ssDNA system must be established prior to the analysis
of such data. The fluorescence signal of quenching of Trp of CspB
appears at least in a first approximation to reflect the extent of
binding to ssDNA template. This can be expected because the
spectroscopic signal is originated from a single fluorophore,
Trp8 of CspB. However, the direct indication of this is an
overlap of the normalized signals obtained by two very different
methods: fluorescence spectroscopy and ITC (Fig. 4C). It is
notable that the overlap of the normalized signals obtained by the two
techniques is observed for both 23pT and 23pC ssDNA templates. For 23pT
there is higher degree of quenching observed, and correspondingly there is higher heat associated with the interaction as measured by ITC. For
23pC it is just opposite: there is less fluorescence quenching
observed, and the heat of the reaction is also lower. These
observations provide a background for the validity of the analysis of
the CspB-ssDNA interactions using fluorescence spectroscopy.
Thermodynamics of CspB Interactions with 23pT and
23pC--
Thermodynamics of CspB interactions with ssDNA templates was
assessed by fluorescence spectroscopy and by ITC. Because of the high
concentrations of CspB and 23T/23pT templates required for the ITC
experiment and the corresponding stoichiometric character of binding of
CspB to 23pT under these reaction conditions, only the enthalpy of
interactions and not the equilibrium constant could be obtained
directly. The calorimetric enthalpy of the interactions of one molecule
of CspB with 23pT at 25 °C is estimated to be 110 ± 7 kJ/mol
(Fig. 4).
An alternative way of determining the enthalpy of interactions is from
the temperature dependence of the equilibrium constant using the well
known van't Hoff relation shown in Equation 8.
|
(Eq. 8)
|
Temperature dependence of the equilibrium constant can be
estimated from the equilibrium binding isotherms obtained at different temperatures.
Fig. 6 shows the binding isotherms for
23pT and 23T with CspB as monitored by the quenching of CspB Trp
fluorescence intensity at four different temperatures: 25, 31, 37, and
42 °C. No significant difference in titration profiles was observed
for the 23pT or 23T templates at any temperature. Data were analyzed
according to the classical binding formalism (Equation 1) or Epstein
model (Equation 7), and the results of analysis are shown in Table
II. It is notable that the association
constants obtained from these two different models are comparable. This
is particularly due to the very moderate cooperativity of the
interactions, as measured by the parameter in the Equation 3 of
Epstein model. Increase in temperature has a profound effect on the
association constant leading to a decrease of this parameter (Table
II). The van't Hoff analysis (Equation 8 and Fig. 6B) for
the enthalpy of CspB-23pT interactions gives enthalpies ( 119 ± 6 kJ/mol using independent binding site model or 104 ± 10 kJ/mol using Epstein model) that are in an excellent agreement with the
calorimetrically determined binding enthalpy of 110 ± 7 kJ/mol.
Knowing the equilibrium constants and the enthalpy changes for
CspB-ssDNA interactions allow us to estimate the entropy changes in the
system (Table II). For 23pC the entropy change upon CspB-23pC
interactions is positive, indicating that complex formation is favored
both enthalpically and entropically. It is notable, however, that the
enthalpy and the entropy changes for 23pT template are both negative
(Table II), thus the favorable enthalpy change upon binding
overcompensates the unfavorable entropic
( T· S) term leading to an enthalpically driven association between CspB and the 23pT/23T templates.

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|
Fig. 6.
Analysis of the thermodynamics of Csp-23pT
interactions. A, changes in the fluorescence intensity
of CspB as a function of 23pT concentration (open symbols)
or 23T concentration (filled symbols) at different
temperatures. Circles, 25 °C; squares,
31 °C; triangles, 37 °C; inverted
triangles, 42 °C. The solid lines represent the fit
of experimental points to Equation 1, using the parameters listed in
Table II. B, the plot of the
R·ln(Ka) versus
1000/T using classical ( , Equation 1) or Epstein ( ,
Equation 7) models. Lines are linear fits of the data with
the slopes (which represent the van't Hoff enthalpy) of 119 ± 6 kJ/mol (solid line) and 104 ± 10 kJ/mol
(dotted line).
|
|
These enthalpically driven interactions might be rationalized in terms
of burial of aromatic side chains of CspB and of the pyrimidine ring of
thymine. Five aromatic residues of CspB (Trp8,
Phe17, Phe17, Phe27, and
Phe30) have been implicated in the binding to nucleic acids
(17), and our results suggest that these aromatic residues probably interact with 6-7 thymine bases. The estimates of the enthalpy changes
upon complex formation between the five aromatic groups of CspB and
6-7 pyrimidine groups of T-based ssDNA template can be made using
model compound data. One can imagine a two-step process: dehydration of
these ring structures followed by the formation of interactions between
them. The first step can be modeled as a transfer of a compound from
water into the gas phase and the second as a condensation process
(39-41). The enthalpy of transfer of benzene ring from the aqueous
phase to the gas phase (dehydration) at 25 °C is 29 kJ/mol (42),
somewhat close to the enthalpy of transfer for toluene (33 kJ/mol). So,
for the first step an enthalpy value of 32 kJ/mol can be a reasonable estimate. For the second step, the enthalpies of condensation of model
compounds such as benzene ( 42 kJ/mol), toluene ( 38 kJ/mol), or
pyrimidine ( 50 kJ/mol) suggest an average enthalpy on the order of
43 kJ/mol (43). Thus the net enthalpy changes for both steps can be
estimated at 11 kJ/mol. Using the calorimetric enthalpy of
interactions of CspB with 23pT ( 110 kJ/mol) and assuming that all
enthalpy change comes from the two-step transfer considered above, we
can estimate that ~10 (110 divided by 11) aromatic groups are
required to give the observed enthalpy changes. This estimate compares
favorably with our previous estimate of 11-12 groups (5 aromatic side
chains of the CspB and 6-7 pyrimidine rings of 23pT) being involved in
the interactions between CspB and T-based ssDNA template. An
independent indication for the validity of such analysis comes from the
results of thermodynamic studies of interactions between ssDNA
templates and Trp-containing oligolysine peptides (44, 45). The authors
found that a single Trp residue contributes 8-12 kJ/mol to the binding
enthalpy, a value in good agreement with our estimate based on the
thermodynamics of the two-step model compound transfer process.
Enthalpically driven protein-nucleic acid interactions have been
observed, for example, for the sequence specific interactions of cI
repressor with the bacteriophage lambda OR operator (46, 47) and in the formation of the MetJ-operator complex (48). However,
inspection of the crystal structure of the complexes (49, 50) does not
show stacking interactions between aromatic side chains of protein and
DNA bases but does bury a number of aromatic groups. Enthalpically
driven interactions between E. coli single-stranded binding
protein to different single-stranded nucleic acids have also been
demonstrated. For example, the enthalpy of interactions of
single-stranded binding tetramer with dT(pT)34 varies from
600 kJ/mol in 10 mM NaCl to 470 kJ/mol in 1 M NaCl (30, 51). These enthalpies, calculated per mole of
single-stranded binding monomer, are comparable with that obtained for
the CspB-23pT interactions (~110 kJ/mol).
Difference in the Mechanism of CspB Interactions with 23pT and
23pC--
Thus all four methods, analytical centrifugation, gel shift
assays, ITC, and Trp fluorescence spectroscopy, show that there are
significant differences in the interactions between CspB and the ssDNA
templates 23pC and 23pT. CspB binding to the T-based templates has four
distinctive features. First, the equilibrium dissociation constants for
T-based template are at least several times lower than those for CspB
binding to the 23pC template (Table II). Second, the stoichiometry of
binding of CspB is different for 23pT than for 23pC. Three molecules of
CspB bind to one molecule of 23pT, which indicates that about seven
nucleotides are involved in the interaction with one CspB molecule.
Geometrical considerations based on the structure of CspB (18, 19) and
on the length of the seven nucleotide long stretch of ssDNA are
consistent with this estimate. In contrast, only one molecule of CspB
binds to 23pC. Third, the enthalpy of interactions of CspB with 23pT is five times that observed for the interactions of CspB with 23pC ( 110
kJ/mol versus 25 kJ/mol). Fourth, the entropy of
interactions of CspB with 23pT is negative, whereas the entropy of
interactions of CspB with 23pC is positive. All these results suggest
that distinct mechanisms govern the interactions of CspB with 23pC and
23T/23pT templates.
Protein-DNA interactions in general and protein-ssDNA interactions in
particular can be mediated through the formation of contacts between
the basic side chains on a protein with the negatively changed
phosphodiester backbone of DNA and/or through the contacts between side
chains on a protein with the sugar moiety and base. In the first case,
the interactions will have a significant electrostatic component. In
the second case, other types of noncovalent forces such as hydrogen
bonding, van der Waals' interactions, and hydrophobic effect will be
involved. To distinguish between these two mechanisms of interactions
we analyzed the effect of ionic strength on the CspB-ssDNA binding
isotherms. Increased ionic strength weakens the charge-charge
interactions, thus making electrostatically formed complexes less
stable (52-54). Fig. 7 compares the
results CspB titration with T- and C-based oligodeoxynucleotides in the presence of 100 mM and 1 M NaCl monitored by
quenching of CspB Trp fluorescence. Addition of 1 M NaCl to
the solution did not affect the binding isotherm for T-based template.
The profiles in the presence of low (100 mM NaCl) and high
(1 M NaCl) salt are superimposable not only at 25 °C but
also at 37 °C, a condition of lower binding affinity. However, in
the presence of 1 M NaCl binding of CspB to the C-based
template is virtually abolished (Fig. 7). This provides an indication
that the interactions of CspB with C-based templates are mainly
mediated by electrostatic interactions of basic side chains on the
protein with the phosphodiester backbone of ssDNA template. On the
other hand interactions of CspB with the T-based template occur mainly
via the interactions of protein with the bases and to a lesser extent
with the phosphodiester backbone of ssDNA.

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Fig. 7.
Changes in the fluorescence intensity of CspB
as a function of concentration of ssDNA templates 23pC (25 °C,
circles) and 23pT (25 °C, squares
and 37 °C, triangles) in low (100 mM, open symbols) or high (1 M, filled symbols) concentrations of
NaCl. Solid lines drawn through the points do not carry
any meaning; they are intended to guide the eye.
|
|
Concluding Remarks--
The observation that CspB can bind
preferentially T-rich stretches of ssDNA with an affinity on the order
of 107 M 1 or higher at
temperatures below 25 °C might suggest a possible role for in
vivo function of CspB. There are two prevalent occurrences of
T-rich regions identified in DNA. First, T-rich sequences occur at
factor-independent transcription termination signals (see for reviews
Refs. 55-59). These sites are characterized by a GC-rich region of
dyad symmetry followed by a run of 6-8 T residues (59). The
possibility of CspB involvement in transcription termination at low
temperatures can be rationalized in the terms of possible CspB
interactions with the T-run on the coding strand of DNA, which will
force dissociation of RNA polymerase. Second, T-rich runs are
frequently located downstream from promoter sequences as part of the
sequences contained within the unusually long 5'-untranslated region of
cold shock proteins (17). The importance of these 5'-untranslated
region in stabilizing the mRNA of the the major cold shock proteins
of E. coli has been clearly demonstrated (60-65). Possible
role of the Csp family of proteins in the transcriptional initiation
was recently demonstrated for CspE. Using photocross-linking ribonucleotide analogs Hanna and Liu (66) showed that CspE (~66% sequence identity to CspB) is cross-linked to the nascent (but not
full-length) mRNA in an in vitro transcription reaction.
These possible functional roles for CspB follow directly from the
observed high binding affinity of this protein to the T-rich ssDNA
templates. Direct demonstration of the role of these in
vitro observed properties for the cellular function of Csp family
of proteins awaits experimental validation.
 |
ACKNOWLEDGEMENTS |
We thank Prof. Dr. Mohamed Marahiel for the
overexpression vector for CspB, Miyo Sakai for performing experiments
on Beckman XL-A, and Drs. James Harman and Michael Fried for fruitful
discussions. We also thank the anonymous reviewer for thoughtful
comments on the manuscript.
 |
FOOTNOTES |
*
This work was supported by Human Frontier in Science Program
Grant RPG-0036/1997M and by National Science Foundation Grant DBI
9604753 (to G. I. M.).The costs of publication of this
article were defrayed in part by the
payment of page charges. The article must therefore be hereby marked
"advertisement" in
accordance with 18 U.S.C. Section
1734 solely to indicate this fact.
¶
To whom correspondence should be addressed: Dept. of
Biochemistry and Molecular Biology, Penn State College of Medicine,
Hershey, PA 17033. Tel.: 717-531-0712; Fax: 717-531-7072; E-mail:
makhatadze@psu.edu.
 |
ABBREVIATIONS |
The abbreviations used are:
ss, single-stranded;
ITC, isothermal titration calorimetry.
 |
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