Open Access Article
Alexandra A.
Kuznetsova
a,
Danila A.
Iakovlev
a,
Inna V.
Misovets
b,
Alexander A.
Ishchenko
c,
Murat K.
Saparbaev
c,
Nikita A.
Kuznetsov
*ab and
Olga S.
Fedorova
*ab
aInstitute of Chemical Biology and Fundamental Medicine (ICBFM), Siberian Branch of Russian Academy of Sciences, 8 Lavrentyev Ave., Novosibirsk 630090, Russia. E-mail: fedorova@niboch.nsc.ru; nikita.kuznetsov@niboch.nsc.ru; Fax: +7 383-3635153; Fax: +7 383-3635153; Tel: +7 383-3635175 Tel: +7 383-3635174
bDepartment of Natural Sciences, Novosibirsk State University (NSU), 2 Pirogova St., Novosibirsk 630090, Russia
cGroupe “Réparation de l’ADN”, Université Paris-Sud XI, UMR8200 CNRS, Institute Gustave Roussy, Villejuif Cedex F-94805, France
First published on 11th October 2017
In all organisms, DNA glycosylases initiate base excision repair pathways resulting in removal of aberrant bases from DNA. Human SMUG1 belongs to the superfamily of uracil-DNA glycosylases catalyzing the hydrolysis of the N-glycosidic bond of uridine and uridine lesions bearing oxidized groups at C5: 5-hydroxymethyluridine (5hmU), 5-formyluridine (5fU), and 5-hydroxyuridine (5hoU). An apurinic/apyrimidinic (AP) site formed as the product of an N-glycosylase reaction is tightly bound to hSMUG1, thus inhibiting the downstream action of AP-endonuclease APE1. The steady-state kinetic parameters (kcat and KM; obtained from the literature) correspond to the enzyme turnover process limited by the release of hSMUG1 from the complex with the AP-site. In the present study, our objective was to carry out a stopped-flow fluorescence analysis of the interaction of hSMUG1 with a DNA substrate containing a dU:dG base pair to follow the pre-steady-state kinetics of conformational changes in both molecules. A comparison of kinetic data obtained by means of Trp and 2-aminopurine fluorescence and Förster resonance energy transfer (FRET) detection allowed us to elucidate the stages of specific and nonspecific DNA binding, to propose the mechanism of damaged base recognition by hSMUG1, and to determine the true rate of the catalytic step. Our results shed light on the kinetic mechanism underlying the initiation of base excision repair by hSMUG1 using the “wedge” strategy for DNA lesion search.
The superfamily of UDGs is classified into six families by substrate specificity, sequence homology, and structural similarity.11–13 Alignment of major motifs and structural organization of hSMUG1 and UDGs from other structural families revealed that the C-terminal motif of hSMUG1 contains the conserved histidine residue of UNG family 1. On the other hand, the N-terminal catalytic motif of hSMUG1 contains the asparagine that is found in MUG family 2. Therefore, hSMUG1 is a member of structural family 3, which represents the hybrid type of the active site.12
Mutational and structural analysis together with steady-state kinetic studies have revealed that in hSMUG1 Asn85 and His239 catalyze the cleavage of the N-glycosidic bond. Asn163 and Phe98 discriminate pyrimidine bases through π–π stacking with Phe98 and specific hydrogen bonding to the Asn163. The Gly87–Met91 region recognizes the C5 substituent through water-bridged (uracil) or direct (hoU, hmU, and fU) hydrogen bonds.14 In hSMUG1, the 239–249 sequence serves as a “wedge” penetrating the DNA double helix in the region of a specific site.5,14–18 Formation of the catalytic complex leads to the dissociative SN1-like cleavage of the N-glycosidic bond of an everted damaged base placed in the active site.14,19 AP-sites formed as products of the N-glycosylase reaction are tightly bound to hSMUG1 thereby inhibiting their cleavage by AP-endonucleases.15 The same mechanism may be responsible for the catalytic efficiency of hSMUG1 as determined by enzyme turnover. The steady-state kinetic parameters kcat and KM have been identified for dU:dA (0.05–0.07 s−1 and 4.0–11.3 μM),4,15 dU:dG (0.03–0.05 s−1 and 0.5–1.3 μM)4,15 and single stranded U (0.21–0.29 s−1 and 1.7–3.0 μM) oligonucleotide substrates.4,15 For DNA-substrates containing dU:dG base pairs alternatively it was obtained that the values of kcat and KM were equal to 0.014 s−1 and 2.2 nM, respectively.14 Nevertheless, steady-state studies have been unable to characterize the real catalytic power of hSMUG1 and to obtain the values of microscopic rate constants for the separate steps in the reaction pathway from recognition of specific sites to the formation of the final products.
To gain a deeper insight into the damage recognition mechanism, we performed a pre-steady-state kinetic analysis of conformational transitions of hSMUG1 and DNA in the course of the catalytic cycle under conditions when there is no large excess of enzyme or substrate. The conformational dynamics were directly recorded by the stopped-flow technique combined with fluorescence detection. Conformational changes in the protein were monitored by changes in Trp fluorescence intensity. To examine the conformational dynamics of DNA, the fluorescent base 2-aminopurine (aPu) and dye–quencher pair FAM/BHQ1 were incorporated into DNA. A DNA duplex containing the dU:dG base pair served as a “full enzymatic cycle” DNA substrate; this cycle includes DNA binding and N-glycosidic bond cleavage. A DNA duplex containing an uncleavable analog of the natural AP-site (3-hydroxytetrahydrofuran-2-yl)methyl phosphate (F-site) instead of dU was used as a DNA product. The DNA duplex containing dC:dG enabled us to follow the conformational changes in the enzyme and DNA during the formation of the nonspecific complex. A comparison of fluorescence kinetic data obtained by Trp, aPu, and FRET detection allowed us to elucidate the stages of specific and nonspecific DNA binding and to propose the mechanism of damaged-base recognition by hSMUG1.
bp. The PCR products were separated on 1.0% agarose/TAE gels, excised and purified using a QIAquick PCR purification kit (Qiagen, Hilden, Germany). Finally, the gene of hSMUG1 was cloned into the pET28c expression vector using NdeI and BamHI restriction sites and sequenced.
000 rpm, 10 min). A cell suspension was prepared in 30 mL of buffer I (20 mM HEPES-NaOH, pH 7.8) containing 100 mM NaCl and a protease inhibitor cocktail (Complete, Germany). The cells were lysed using a Thermo French Pressure Cell Press. All the subsequent procedures were conducted at 4 °C. The cell lysate was centrifuged (30
000 rpm, 40 min), and the supernatant was loaded onto column I (Q-Sepharose Fast Flow, Amersham Biosciences, Sweden) with subsequent washing with buffer solution I (20 mM HEPES-NaOH, pH 7.8) containing 100 mM NaCl. Fractions containing the protein were collected and loaded onto column II (HiTrap-Helating™, Amersham Biosciences, Sweden) in buffer solution II (20 mM HEPES-NaOH, pH 7.8) containing 500 mM NaCl and 20 mM imidazole. Chromatography was run in buffer solution II and a linear gradient of 20 → 500 mM imidazole. The solution's absorbance was detected at a wavelength of 280 nm. The protein purity was determined by gel electrophoresis. Fractions containing the hSMUG1 protein were dialyzed against a buffer (20 mM HEPES-NaOH, pH 7.5, 1 mM EDTA, 1 mM dithiothreitol, 250 mM NaCl, 50% glycerol) and stored at −20 °C. The protein concentration was calculated based on the optical density of the protein solution at 280 nm and a molar extinction coefficient of 28
460 M−1 cm−1.20
All the experiments on the enzymatic reaction were conducted in a buffer consisting of 50 mM Tris–HCl pH 7.5, 50 mM KCl, 1 mM EDTA, 1 mM dithiothreitol, and 7% glycerol at 25 °C.
:
1 molar ratio in a buffer consisting of 50 mM Tris–HCl pH 7.5, 50 mM KCl, 1 mM EDTA, 1 mM dithiothreitol, and 7% glycerol.
| Shorthand | Sequence |
|---|---|
| a aPu is 2-aminopurine, FAM is 6-carboxyfluorescein, BHQ1 is black hole quencher. | |
| X-substrate, X = U | 5′-GCTCAXGTACAGAGCTG-3′ |
| X-ligand, X = F-site and C | 3′-CGAGTGCATGTCTCGAC-5′ |
| X-aPu-substrate, X = U | 5′-GCTCAX(aPu)TACAGAGCTG-3′ |
| X-aPu-ligand, X = F-site | 3′-CGAGTGCATGTCTCGAC-5′ |
| X-FRET-substrate, X = U | 5′-FAM-GCTCAXGTACAGAGCTG-3′ |
| X-FRET-ligand, X = F-site and C | 3′-CGAGTGCATGTCTCGAC-BHQ1-5′ |
In a standard procedure, the solution of hSMUG1 was placed in one instrument's syringe and rapidly mixed in the reaction chamber with the substrate from another syringe. The reported concentrations of reactants are those in the reaction chamber after mixing. Typically, each trace shown in the figures is the average of four or more fluorescence traces recorded in individual experiments. In the figures, if necessary for better presentation, the curves were manually moved apart. This procedure does not affect the results of fitting because the background fluorescence is fitted separately for each curve.
![]() | (1) |
| Fi(t) = fi × [Ei(t)], | (2) |
The software performs numerical integration of a system of ordinary differential equations with subsequent nonlinear least-squares regression analysis. In the fits, we optimized all relevant rate constants for the forward and reverse reactions as well as the specific molar response factors for all the intermediate complexes. During the data processing, the kinetic information was obtained from temporal behavior of the fluorescence intensity, not from the amplitudes of the specific signal contributions. The response factors for different conformers resulting from the fits were not used for determination of the equilibrium constants but rather provided additional information on the fluorescence intensity variations in different complexes and conformers.
The hSMUG1 molecule contains four Trp residues: Trp62, Trp107, Trp142, and Trp251. Because no structure of hSMUG1 is available, we used the high sequence homology among hSMUG1, xSMUG1, and GmeSMUG1 (Fig. 1A) to obtain a structure of the hSMUG1–DNA complex by homology modelling. It follows from the structures of the xSMUG1–DNA complex5 that the enzyme bound the ends of the DNA duplex. Therefore, these data do not elucidate the lesion recognition state of the enzyme and DNA. Nevertheless crystal-soak experiments with free Ura bases indicate the possible position of the damaged base in the active site of the enzyme. Structural superposition of the noncovalent complex of xSMUG1 with a Ura base (Protein Data Bank code 1OE5)5 and the model structure of hSMUG1 revealed that Trp62, Trp107, and Trp142 are located inside the protein globule and far away (at least 11.9 Å between the N1 atom of uracil and the Cα atom of the Trp142 residue) from the damaged-base-binding pocket of the enzyme (Fig. 1B). Only Trp251 is located in close proximity to the intercalating loop of the enzyme (amino acids 239–249), and therefore this residue most likely can be sensitive to DNA binding.
![]() | ||
| Fig. 1 (A) An alignment of sequences of hSMUG1, xSMUG1, and GmeSMUG1. Motifs responsible for lesion binding (red), recognition using the intercalating loop (brown), and catalysis (green) of damaged-base processing are indicated with colors. Trp residues of hSMUG are colored blue. Asterisks indicate identical residues, colons denote conserved residues; dots are residues with at least some physicochemical properties conserved. (B) Structural superposition of the noncovalent complexes of xSMUG1 with a Ura base (Protein Data Bank code 1OE5)5 and model structure of hSMUG1. | ||
To study the conformational transitions in DNA substrates, two approaches were employed. First, the fluorescent analog of DNA base aPu was incorporated on the 3′-side of a damaged nucleotide in DNA substrates as a reporter group of the conformational transitions in the damaged DNA strand near the damaged nucleotide. The aPu residue has a high quantum yield of fluorescence in an aqueous solution, but it is highly quenched when aPu is incorporated into DNA or transferred into a nonpolar environment.38–40 Accordingly, aPu is highly sensitive to the local melting of DNA strands around the damaged nucleotide, to nucleotide flipping out, and to insertion of an enzyme's amino acids into DNA.41–43 Second, Förster resonance energy transfer (FRET) DNA substrates modified at their 5′ termini with the dye–quencher pair FAM/BHQ1 were used for FRET measurements. FRET analysis revealed changes in the distance between the dye and quencher in the processes of DNA helix distortion during the formation of the complex between hSMUG1 and DNA.
In the kinetic curves obtained during the interaction of hSMUG1 with the undamaged C-ligand, a fast single phase of an increase in the Trp fluorescence intensity up to 5 ms is seen (Fig. 2A). When hSMUG1 interacts with the C-FRET-ligand (Fig. 2B), a fast increase in the FRET signal is observed. These data most likely correspond to collisional nonspecific binding of the enzyme to DNA, resulting in the movement of the intercalating loop (239–249) with a change of the Trp251 environment and shielding of FAM fluorescence from the quenching with BHQ1. Both types of data were fitted to a kinetic mechanism consisting of a one-step equilibrium (Scheme 1). The rate constants obtained by the fitting procedure are presented in Table 2.
| Constants | Trp | FRET |
|---|---|---|
| K i = ki/k−i, i is the number of a step. | ||
| k 1, M−1 s−1 | (170 ± 60) × 106 | (120 ± 50) × 106 |
| k −1, s−1 | 1260 ± 460 | 850 ± 170 |
| K 1, M−1 | 0.13 × 106 | 0.14 × 106 |
As shown in Table 2, the values of k1 in both cases are in agreement with the typical rate constants of diffusion-controlled DNA–protein bindings.44–48 The rate constant of DNA–protein dissociation was found to be ∼1000 s−1, and a close to analogous value was obtained previously for DNA–glycosylase Fpg. from E. coli (2700 s−1).47 Thus, the human DNA–glycosylase SMUG1 is bound to DNA in a diffusion-controlled process and forms a nonspecific complex, probably by intercalation of the loop (positions 239–249) into the DNA helix.
The nature of these specific interactions was elucidated by analysis of aPu fluorescence because of high sensitivity of an aPu residue to the microenvironment. Mixing of an F-aPu-ligand with hSMUG1 led to a biphasic change in the aPu fluorescence intensity (Fig. 3B) represented by a humped curve. The initial fast increase in the aPu fluorescence intensity up to 5 ms reveals the increase of hydrophilicity of the aPu environment and correlates with the first phase in Trp fluorescence and FRET time courses. In general, these data support the notion about the nature of this phase as the initial DNA binding: movement of the intercalating loop inducing local melting of the DNA helix in the vicinity of the F-site. Our previous data on structurally unrelated DNA glycosylases hOGG152 and Fpg53 have revealed that the fast initial increase in the aPu fluorescence is caused by eversion of the damaged base from the DNA helix. Therefore, we propose that during this time interval, the F-site can also be flipped out from DNA.
The next phase is characterized by a decrease in the fluorescence intensity within 0.1 s. It is likely that this phase is associated with the insertion of intercalating amino acids into the void in the DNA helix formed by an F-site. The void-filling process leads to transition of the aPu base into a more hydrophobic environment leading to a decrease in the aPu fluorescence intensity within 0.1 s. The kinetic curves obtained for both Trp and aPu fluorescence data were fitted to a two-step equilibrium mechanism (Scheme 2) resulting in calculation of rate and equilibrium constants (Table 3).
| Constants | Trp | aPu | FRET |
|---|---|---|---|
| K i = ki/k−i, i is the number of a step. | |||
| k 1, M−1 s−1 | (120 ± 30) × 106 | (130 ± 10) × 106 | (200 ± 50) × 106 |
| k −1, s−1 | 1000 ± 250 | 490 ± 60 | 650 ± 70 |
| K 1, M−1 | 0.12 × 106 | 0.26 × 106 | 0.31 × 106 |
| k 2, s−1 | 60 ± 23 | 25 ± 16 | 7.7 ± 3.5 |
| k −2, s−1 | 24 ± 7 | 55 ± 21 | 18.4 ± 0.9 |
| K 2 | 2.5 ± 1.7 | 0.45 ± 0.46 | 0.42 ± 0.21 |
| K 1 × K2, M−1 | 0.3 × 106 | 0.12 × 106 | 0.13 × 106 |
| k 3, s−1 | 0.13 ± 0.02 | ||
| k −3, s−1 | 0.067 ± 0.004 | ||
| K 3 | 1.9 ± 0.4 | ||
| K 1 × K2 × K3, M−1 | 0.25 × 106 | ||
The time course of a FRET signal obtained during the interaction of hSMUG1 with the F-FRET-ligand has three visible phases: a fast increase followed by a biphasic decrease (Fig. 3C). The fast initial phase (up to 5 ms) represents DNA binding, which likely involves the movement of the intercalating loop of the enzyme and local melting of the DNA duplex, and induces an increase in the FRET signal owing to shielding of the FAM emitter from the BHQ1 quencher. The decrease in the FRET signal at the next steps reflects a decrease in the distance between the FAM and BHQ1 residues, probably, due to DNA bending. This DNA bending proceeds simultaneously with insertion into DNA of the void-filling amino acids, as detected by means of Trp and aPu fluorescence behavior. Moreover, the second decrease phase of the FRET signal proceeding slowly in a time range of 1–100 s reveals an additional conformational adjustment of DNA in complex with the enzyme. FRET kinetic curves were fitted to Scheme 3, which contains three equilibrium steps of the FRET-F-ligand binding by hSMUG1 (Table 3).
The rate constants of the formation and dissociation of a primary complex (E·F)1, k1 and k−1, are close (the difference is within the experimental error) and have values similar to those obtained for nonspecific C- and C-FRET-ligands (Table 2). Therefore, the first step is nonspecific binding resulting in local DNA melting and intercalating-loop movement. The second step where Trp and aPu fluorescence intensities as well as the FRET signal decrease can be attributed to the formation of a tight protein–DNA complex, void-filling, and DNA helix bending. The third step observed for the F-FRET-ligand at long periods (>10 s) means a slow process of DNA conformational change in complex with hSMUG1.
The minimal kinetic mechanism describing these fluorescence changes consists of two reversible binding steps and one irreversible step of catalysis (Scheme 4). Given that hSMUG1 binds tightly to product AP-sites, we hypothesized that the dissociation of the enzyme–product complex does not occur during the registration time (10 s), and product P stays tightly associated with the enzyme in this period. The rate and equilibrium constants obtained by Trp fluorescence trace fitting are shown in Table 4.
| Constants | Trp | aPu | FRET |
|---|---|---|---|
| K i = ki/k−i, i is the number of a step. | |||
| k 1, M−1 s−1 | (115 ± 20) × 106 | (130 ± 60) × 106 | (140 ± 20) × 106 |
| k −1, s−1 | 760 ± 90 | 240 ± 30 | 410 ± 20 |
| K 1, M−1 | 0.15 × 106 | 0.54 × 106 | 0.34 × 106 |
| k 2, s−1 | 30 ± 8 | 15 ± 8 | 3.6 ± 0.8 |
| k −2, s−1 | 11.5 ± 0.8 | 25 ± 6 | 9.7 ± 0.2 |
| K 2 | 2.6 | 0.6 | 0.37 |
| K 1 × K2, M−1 | 0.3 × 106 | 0.32 × 106 | 0.13 × 106 |
| k 3, s−1 | 1.7 ± 0.2 | 0.6 ± 0.1 | |
| k −3, s−1 | 0.11 ± 0.02 | ||
| K 3 | 5.4 | ||
| K 1 × K2 × K3, M−1 | 0.68 × 106 | ||
PAGE analysis of the reaction product formation (Fig. 4B) showed that in the initial region of the kinetic curves (up to 10 s), a burst is observed. This type of curve indicates the presence of a rate-limiting step after the catalytic reaction. Indeed, hSMUG1 binds tightly to product AP-sites, and steady-state rate constant kcat, which was found to be 0.014–0.05 s−1 as determined elsewhere,4,14,15 is much less than rate constant k3, which characterizes the catalytic step in Scheme 4. Therefore, we believe that changes in Trp fluorescence allow us to determine the “true” value of the catalytic rate constant.
The shape of the kinetic curves recorded by means of aPu fluorescence (Fig. 4C) and FRET (Fig. 4D) for U-aPu and U-FRET substrates, respectively, was similar to the shapes obtained for DNA containing an F-site. The similarity of kinetic curves obtained for cleavable (U-substrates) and uncleavable (F-ligands) DNAs supports the idea that catalytic reaction of N-glycosidic bond hydrolysis does not require additional conformational changes of DNA. The minimal kinetic schemes describing the observed changes in aPu fluorescence intensity (Scheme 5) and in the FRET signal (Scheme 6) were identical to those proposed for DNA containing an F-site (Table 4). It should be noted that the initial increase phase of the FRET signal is not well fitted to the kinetic scheme due to the fact that the registered process is very fast. Indeed, the dead time of the device is 1.4 ms, while the end of the growth phase occurs up to 4 ms. Therefore, this phase on the kinetic curves reflects only the end of the ongoing process. Nevertheless, the proposed mechanism allowed estimation of the values of the rate constants of this phase.
It should be noted that hSMUG1 removes uracil from both ssDNA and dsDNA. Control experiments with ssDNA were performed to verify the possibility of the influence of enzyme binding to ssDNA on the kinetics of interaction with dsDNA (ESI,† Fig. S1). The obtained data support the conclusion that interaction of hSMUG1 with ssDNA cannot be detected using Trp and aPu fluorescence. In the first case complex formation between hSMUG1 and ssU oligonucleotides does not provide enough quenching of Trp fluorescence by nucleic bases, probably, due to different modes of interaction with ssDNA and dsDNA. In the case of ssUaPu oligonucleotides, the aPu base is located in the aqueous polar environment and has a high level of fluorescence intensity, which does not allow the process of Ura base eversion to be registered as in the case of a double stranded U-aPu/G-substrate. Control experiments with the FAM-U/G duplex without BHQ1 were also carried out. As shown in the ESI,† Fig. S1, changes of FAM fluorescence without the BHQ1 quencher are barely noticeable in comparison with the case of the presence of the quencher.
A comparison of the rate constants obtained for DNA duplexes containing a Ura base or F-site (Tables 3 and 4) revealed that the formation of the first enzyme–substrate complex proceeds at a similar rate constant k1. By contrast, association constant K1 is slightly higher for uracil-containing DNA duplexes, thus indicating tighter binding with a specific substrate. Therefore, these data suggest that the initial DNA binding proceeds more efficiently in the case of a DNA duplex containing a Ura base. The second detected step, which consists of insertion of void-filling amino acids into DNA, has rate constant k2 that is twofold lower for DNA duplexes containing a Ura base in comparison with an F-site. These data allow us to suppose that the void-filling process depends on the nature of the damaged nucleotide, and the formation of additional contacts with the Ura base in the active site of the enzyme led to a decrease in the rate of catalytic-complex formation. The product accumulation curve detected by PAGE analysis revealed the burst phase already in the first time point up to 10 s. Although time resolution of the burst phase does not allow at what time a burst occurs before 10 s to be determined, a comparison of PAGE analysis with the Trp fluorescence data revealed increase of fluorescence also up to 10 s. Therefore a suggestion was made that the phase of the increase in Trp fluorescence reflects a catalytic process and allows a true value of the rate constant of the catalytic reaction to be calculated.
| SMUG1 | Human single-stranded selective monofunctional uracil-DNA glycosylase |
| AP-site | Apurinic/apyrimidinic site |
| F-site | (3-Hydroxytetrahydrofuran-2-yl)methyl phosphate |
| ODN | Oligodeoxyribonucleotide |
| PAGE | Polyacrylamide gel electrophoresis |
| BER | Base excision repair |
| FRET | Förster resonance energy transfer. |
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c7mb00457e |
| This journal is © The Royal Society of Chemistry 2017 |