Structural and Energetic Factors of the Increased Thermal Stability in a Genetically Engineered Escherichia coli Adenylate Kinase*

Simona Burlacu-Miron, Véronique PerrierDagger , Anne-Marie GillesDagger , Elisabeth PistotnikDagger , and Constantin T. Craescu§

From INSERM U350, Institut Curie-Recherche, 91405 Orsay Cedex, France and Dagger  Laboratoire de Chimie Structurale des Macromolécules (URA D1129), Institut Pasteur, 7524 Paris Cedex 15, France

    ABSTRACT
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Abstract
Introduction
Procedures
Results
Discussion
References

Several variants of Escherichia coli adenylate kinase, designed to bind a Zn2+ ion, were produced by site-directed mutagenesis. The metal binding and enzymatic properties of the engineered variants have been described (Perrier, V., Burlacu-Miron, S., Bourgeois, S., Surewicz, W. K., and Gilles, A.-M. (1998) J. Biol. Chem. 273, 19097-19101). Here we report the structural properties and stability changes in a 4-Cys variant which binds a Zn2+ ion and has an increased thermal stability. CD studies indicate a very similar secondary structure content in the wild type and the engineered variant. NMR analysis revealed that the topology of the parallel beta -sheet, belonging to the protein core, and of the peripheral antiparallel beta -sheet are also conserved. The small local changes observed in the neighborhood of the substitution sites reflect a more compact state of the metal-binding domain. The Zn2+-bound quadruple mutant shows an increased thermal stability, reflected in a 9 °C increase of the mid-temperature of the first cooperative unfolding step. Binding of a bisubstrate analog P1,P5-di(adenosine-5')-pentaphosphate increases, by about 7 °C, the midpoint of this transition in both wild type and modified variant. The NMR data suggest that the peripheral domains involved in substrate binding unfold during the first denaturation step. Urea denaturation experiments indicate an increased resistance against chemical unfolding of the Zn2+-binding variant. In contrast, the Gibbs free energy of unfolding (at physiologically relevant conditions) of the quadruple mutant is lower than that of the wild type.

    INTRODUCTION
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Abstract
Introduction
Procedures
Results
Discussion
References

Adenylate kinases (AKs)1 represent a class of small (20-26 kDa) and abundant phosphotransferases involved in the reversible transfer of the terminal phosphate group from ATP to AMP. They contribute to the maintenance of a constant level of cellular adenine nucleotides, necessary for energetic metabolism and nucleic acid synthesis. From the structural point of view (Fig. 1) AKs belong to the alpha /beta class (a five-stranded beta -sheet surrounded by several alpha -helices), characteristic for many nucleotide-binding proteins (1). In addition to this protein core, they contain generally two smaller domains involved in the substrate binding. One is composed by two helices (alpha 2 + alpha 3) and contributes to the mononucleotide binding, NMP domain closing over bound AMP (residues 30-59). The other is involved in binding of ATP and, due to its large movement, closing over the bound nucleotide, it was called LID domain. In the mitochondrial and most of the bacterial variants of AK, the LID domain has 38 residues (residues 122-159 in AKe) while smaller cytosolic enzymes have only an irregular loop of 11 residues (2, 3). In the AKe (a "long" kinase) the LID domain contains a small four-stranded antiparallel beta -sheet (4). X-ray structures of the enzyme in complex with various ligands revealed that this domain has significantly different positions relative to the protein core, depending on the nature and number of bound ligands. Therefore, it was inferred that complexation (particularly with ATP) induces a large scale rotation/translation movement from a remote position into a close contact with the main part of the protein (3-6). Solution studies, using resonance energy transfer measurements (7), confirmed the existence of such hinge motion of the LID domain upon binding of Ap5A, AMP, and ATP. Nevertheless, the short AKs conserve their catalytic activity despite the absence of the LID domain, but seems to loose the high specificity for ATP (8).


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Fig. 1.   Schematic representation of the global structure of Ake drawn with MOLSCRIPT software (22) and the atomic coordinates (4ake) determined by Müller et al. (4). Some of the side chains mentioned in the text are shown explicitly and labeled.

A screening of bacterial AKs has revealed that the enzymes from Gram-positive organisms bind a Zn2+ ion via coordinative bonds to four side chains (Cys and Asp) situated in the beta -hairpin loops of the LID domain (9). Based on sequence comparison with AK from the Gram-positive, thermophilic Bacillus stearothermophilus, we have designed several variants of the Escherichia coli enzyme involving three- or four-amino acid substitutions in the LID domain, at positions His126, Ser129, Asp146, and Thr149. In the companion study (10) we showed that some of these variants bind a Zn2+ ion and conserve the enzymatic activity. In this study we report the results of NMR and CD experiments aimed to characterize in more detail the structural consequences of the amino acid substitutions and zinc binding. The 4-Cys variant has an increased thermal and chemical (urea) stability, but the structural stability at physiologically relevant conditions is slightly reduced.

    EXPERIMENTAL PROCEDURES
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Abstract
Introduction
Procedures
Results
Discussion
References

All chemicals were of highest purity available. Protein design, expression, and purification were described in our companion study (10).

Circular Dichroism-- The far-UV CD spectra were recorded on a Jasco 700 spectropolarimeter in a 0.1-cm quartz cells. The spectra were obtained as an average of five runs and were corrected for the contribution of the buffer. For the thermal denaturation experiments we followed the ellipticity at 222 nm as a function of temperature, programmed to rise uniformly at 60 °C/h.

Urea denaturation was monitored by the changes in ellipticity at 222 nm. Aliquots of concentrated solutions of protein were added to urea solutions (0-8.8 M) and the samples were incubated until equilibrium was reached at the temperature chosen for determining the unfolding curve (20 °C). The Gibbs free energy of denaturation was estimated by Equation 1
&Dgr;G=<UP>−RT ln</UP> K (Eq. 1)
where K is the equilibrium constant of denaturation at a given reaction temperature (RT) and urea concentration. The measured free energy difference is considered (11) a linear function of the denaturant concentration
&Dgr;G=&Dgr;G<FENCE><UP>H<SUB>2</SUB>O</UP></FENCE>−m[<UP>urea</UP>] (Eq. 2)
where Delta G(H2O), the extrapolated value of Delta G at zero molar denaturant, represents the intrinsic stability of the protein in absence of urea.

NMR Methods-- Samples were prepared by dissolving the lyophilized protein in potassium phosphate buffer (50 mM) in 2H2O or in 1H2O containing 7% 2H2O at pH 6.5. NMR spectra were obtained on a Varian Unity 500 NMR spectrometer, using standard methods for pure absorption DQF-COSY (12), NOESY (13), and TOCSY experiments with 30-60-ms spin lock times (14). Proton chemical shifts were referenced relative to the water signal which, in our conditions, at 308 K resonates at 4.69 ppm from the sodium 2,2-dimethyl-2-silapentane sulfonate signal.

    RESULTS
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Abstract
Introduction
Procedures
Results
Discussion
References

Structure Characterization of the Engineered Variant-- CD spectroscopy in the far-UV region is a sensitive measure of the secondary structure content in polypeptides and is particularly useful in comparing the backbone structural differences between related proteins (15). The similarity between the CD spectra of the wild-type and mutated enzymes (data not shown) indicates that the two proteins have roughly the same secondary structure content.

NMR analysis of a protein such as AKe (23,587 Da, flexible domains, high alpha -helix content) is a difficult task. The proton resonance assignment was facilitated by the large spectral dispersion in the fingerprint region corresponding to beta -strand residues and by the strong sequential connectivities between Calpha Hi and NHi+1 in this type of secondary structure (16). Using several two-dimensional homonuclear NMR spectra (DQF-COSY, TOCSY, and NOESY) we assigned the majority of the resonances corresponding to the two beta -sheet domains in the AKe and AKC4. The quality of the two-dimensional spectra and some of the sequential NOE pathways of AKC4 are shown in Fig. 2. The chemical shift values for the assigned resonances in the proton spectra of AKC4 and AKe are available upon request from the authors.


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Fig. 2.   Portion of the NOESY spectrum of AKC4 illustrating the sequential connectivities used to assign the backbone protons in the beta -strands. The sample (1.5 mM) was dissolved in potassium phosphate buffer (50 mM), pH 6.5, containing 7% 2H2O for the lock. The squares indicate the cross-peaks corresponding to the intraresidue dipolar connectivities Calpha Hi/NHi and are labeled with residue name and number. In the beta -strands these interactions are weak but the position of the cross-peaks is confirmed from comparison with correlation spectra (DQF-COSY, TOCSY). Sequential and some of the long range connectivities are labeled with the numbers of the two interacting residues.

Resonance assignment enabled us to identify a large number of sequential and long range dipolar interactions between specific protons of the protein. Observation of strong sequential connectivities dalpha N(i, i + 1) indicates very short distances between the corresponding protons (Calpha Hi, NHi+1), as is the case for a backbone in an extended conformation. The local geometry was further characterized by the analysis of the chemical shift values. Indeed, statistical analysis of experimental NMR data on proteins, showed that the Calpha protons experience a mean upfield shift of 0.4 ppm if the residue belongs to an alpha -helix and almost the same downfield shift value in the beta -sheet or extended structures (17). Together, the sequential connectivities and the secondary shift of alpha  protons provided a reliable delineation of the beta -strands in AKe and AKC4.

In addition, analysis of long range NOEs between resonances corresponding to the backbone protons revealed the relative arrangement of the secondary structure elements. In particular, the presence of long range dalpha alpha (i, j) NOE cross-peaks is characteristic for antiparallel beta -sheets. The synthesis of the present NMR data is the global topology of the polypeptide chain in the two beta -sheet domains, as represented in Fig. 3 for AKC4. A number of other long range dipolar interactions involving all the protons support this topology. For instance, methyl protons of Leu153 give NOE connectivities with amide protons of Tyr133, Gly144, and Lys145 and with aromatic protons of Tyr133.


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Fig. 3.   Schematic representation of the global topology of the two beta -sheet domains in AKC4 as defined by the present NMR analysis. The amino acids shown are those for which at least the backbone protons were assigned. The strong sequential connectivities (dalpha N(i, i + 1)) within the strands and the dalpha alpha (i, j) and dNN(i, j) long range connectivities between Calpha protons on opposite strands are indicated by arrows.

The secondary and tertiary structure descriptions of AKC4, based on the present experimental data, are very similar to that obtained for the wild-type enzyme and are completely compatible with the crystallographic structure of AKe (4). However, a number of minor spectroscopic modifications were observed between the wild-type protein and AKC4 in the LID domain. Chemical shift changes (up to 0.45 ppm) were noted for residues adjacent to the substituted positions (Ala127, Val125, and Val148). Also, dipolar interactions between amide protons of Tyr133 and Thr154 and delta 1,2 methyl protons of Leu153 were observed in AKC4 but not in AKe. This suggests that Zn2+ binding in AKC4 brings closer the two loops containing the cysteine side chains, and the movement extends over the adjacent beta -strands, so that the methyl groups of Leu153 comes into NOE contact with the amide proton of Tyr133. In contrast, sequential dNN(i, i + 1) connectivities for the amide pairs 147/148 and 148/149 and the NOE between Calpha H(145) and NH(153) were observed in AKe but not in AKC4 spectra.

Investigation of the Thermal Stability-- The heat-induced denaturation curve in Fig. 4 was obtained by recording the ellipticity at 222 nm, which is the minimum in the far-UV CD spectrum for an alpha -helix. The two proteins show a similar profile including an initial slow phase followed by two cooperative transitions, separated by a clear plateau. As reflected in the relative ellipticity changes, a comparable amount of secondary structure is unfolded in each step. The Tm (the mid-temperature of the cooperative transition) for the first transition of the wild-type protein is 52.5 °C which is in good agreement with the previous data (18, 19) and close to the calorimetric value (10). The quadruple mutant shows a significantly increased mid-temperature (61.6 °C), close to the thermal transition (63 °C) observed by microcalorimetry (10). The apoAKC4 (the four Cys mutant in absence of Zn2+) has an intermediate thermal stability between the wild type and AKC4 (Table I). Dithiothreitol, an efficient sulfhydril reductant, at 1-10 mM has no significant effect on the denaturation transition points.


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Fig. 4.   Temperature unfolding of Ake and AKC4 monitored by the ellipticity at 222 nm as a function of temperature. Samples are about 10 µM in 10 mM Tris/HCl buffer, pH 7.2. The data represent wild-type AKe (continuous line) and the variant AKC4 (dotted line) in absence (A) and presence (B) of Ap5A.

                              
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Table I
Parameters of the thermal and urea unfolding for wild type and engineered adenylate kinases

The second transition, not observed in previous studies, is less cooperative and shows more similar Tm values for the two proteins (72.6 and 75.6 °C for AKe and AKC4, respectively). The unfolding process is entirely reversible for AKC4 and partially reversible (80%) for the wild-type protein when the temperature cycle is stopped after the first transition. When the unfolding cycle is continued over this temperature, the denaturation is irreversible.

Ap5A is a bisubstrate analog which binds simultaneously at the ATP and AMP sites of AKs, giving a more compact structure in which the LID domain is in close contact with the protein core (20). To quantify the effect of its binding on the structural stability we studied the denaturation process in the presence of an equimolar concentration of Ap5A. The first transition is significantly shifted toward higher temperatures for AKe, apoAKC4, and AKC4 by about 7 °C (Fig. 4 and Table I). In contrast, no effect was observed on the second transition. A similar thermal protection was observed for a fluorescent analog of Ap5A (19).

The temperature-induced unfolding of the wild type and two mutated variants was further studied by recording one-dimensional proton NMR spectra at different temperatures. The heating up to the first equilibrium intermediate state is accompanied by continuous, small changes of some resonances corresponding to nonexchangeable protons. Some of these peaks were identified in the NMR one-dimensional spectra and were assigned to precise protons of the protein (Fig. 5). One example corresponds to the aromatic protons of Tyr181: a second peak, slightly high field shifted and of increasing intensity is observed in all three samples. Similarly, resonances from imidazole protons of His172 undergo a small upfield shift while the high field peak from Leu213 methyl (chemical shift = -0.16 ppm) is unchanged. At the temperature where the first unfolding transition already took place, these resonances are probes for a folded structure as their chemical shift values are very different (from 0.36 to 0.94 ppm) from the random coil values (16). We note that Tyr181, Leu213, and His172 are located in helices, alpha 8, alpha 9, and C-end of alpha 7, respectively, within the protein core (Fig. 1). Their chemical shift values should be largely dominated by the ring current of neighboring aromatic side chains (Tyr182, Tyr105, and Tyr171, respectively). These observations reflect only small local conformational rearrangements of the side chains within a conserved secondary and tertiary structure. Compared with the wild type, the spectral changes in the two variants AKC4 and AKHC3 extend over larger temperature ranges, suggesting that the Zn2+ binding in the LID domain influences the local fluctuations in the central core.


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Fig. 5.   Temperature dependence of the one-dimensional NMR spectra of three AK variants. Samples are 0.5 mM in 50 mM phosphate buffer (pH 6.5) in 2H2O.

A large number of Calpha protons, resonating between 4.7 and 6.0 ppm, conserve their low field shift characteristic for beta -strand secondary structure. An example is the Calpha proton of Tyr193, a residue from the beta 5 strand of the parallel sheet, which is clearly identified in all one-dimensional spectra at 5.77 ppm (Fig. 5). In the case of AKC4, this observation is indicative of persistence of beta  secondary structure in the intermediate state of the denaturation process (at 70 °C). For AKe and AKHC3, the native Calpha H are conserved during the first thermal transition.

Coupled with the CD data, the temperature-dependent NMR observations suggest that the parallel beta -sheet and part of the surrounding alpha -helices are conserved in the intermediate state and denaturate only during the second thermal transition. Unfortunately, due to aggregation problems, the NMR study was limited to the first part of the denaturation process.

Chemical Denaturation-- The structural stability was further studied using urea as a chemical agent and CD spectroscopy. A single sigmoidal transition was observed for the two studied proteins (not shown). Curve fitting using a two-state model enabled us to calculate the thermodynamic parameters characterizing the structural stability of the proteins (Table I). The urea concentration at which half of the molecules are denatured (Cm) is significantly higher in AKC4 variant reflecting a better resistance to urea denaturation of this protein. The calculated Gibbs free energy of unfolding, extrapolated to zero urea concentration (Delta G(H2O)) is larger in the wild type relative to the engineered variant. Thus, despite an increased thermal stability and a higher resistance to chemical denaturation, the quadruple mutant has a lower structural stability in standard conditions (no denaturant, 20 °C). The coefficient of linear dependence of the Gibbs free energy of unfolding on the urea concentration (m) is considerably decreased in AKC4, indicating a decreased cooperativity of unfolding in the engineered protein.

    DISCUSSION
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Abstract
Introduction
Procedures
Results
Discussion
References

Structure/Function Relationships-- As indicated by the CD and NMR results, introduction of 4 Cys residues and zinc binding in the engineered variant AKC4 conserve the global fold of the polypeptide chain and induce only small structural changes in the LID domain. The Zn2+-binding loops come closer to each other and the domain becomes more compact. The fact that the catalytic properties are practically conserved suggests that the domain keeps its ability to move toward the ATP-binding site. This is further supported by the fact that Ap5A binding (which is known to favor this movement) increases the thermal unfolding mid-temperature (Tm) with similar extent in both wild type and AKC4 (Fig. 4).

Mechanism of the Thermal Unfolding-- The present experimental data provide a minimal structural basis for a basic description of the thermal unfolding process of AKe. The CD experiments indicate a complex thermal denaturation mechanism with two separated cooperative steps. Comparative analysis of the NMR and CD data suggests that the protein core, including the parallel beta -sheet and the surrounding helices (alpha 1, alpha 8, and alpha 9), is conserved in the equilibrium intermediate state and unfolds in the second step. This domain represents about 45% of the total regular secondary structure (alpha -helix and beta -sheet) contributing to the CD signal around 220 nm, in reasonable agreement with the relative extent of ellipticity change during the second unfolding transition (Fig. 4). In agreement with this hypothesis, Ap5A shifts significantly the Tm of the first transition but has only a minimal effect on the second one. Indeed, structural analysis of the bi-substrate binding (3) revealed that the most perturbed fragments are the connecting helices (alpha 6 and alpha 7) while the parallel beta -sheet is not affected. The present experiments provide no definite data on the role of the LID domain in the denaturation process. Recent 1H/2H exchange experiments on 15N-labeled Ake2 revealed that some amide protons in the antiparallel beta -sheet exchange more rapidly than in the protein core (parallel beta -sheet, alpha 1, alpha 8, and alpha 9) but more slowly than in the peripheral alpha -helices. This suggests that the LID domain exhibits a more fluctuating hydrogen bond network than the parallel beta -sheet and may unfold in early stages of denaturation. The large values of the temperature factors observed in x-ray studies in the LID domain of the unliganded AKe (4) support this hypothesis.

Interaction of AK with the bi-substrate Ap5A leads to a more symmetric and compact molecule and induces a structural stabilization of the nucleotide-closing domains (the antiparallel beta -sheet, helices alpha 2 and alpha 3) and of the connecting helices (alpha 6 and alpha 7). The total accessible surface of the protein decreases by about 13% (4) and the ligand forms tight contacts with several side chains in the active site (20). These factors should contribute to the Ap5A-induced delay of the first denaturation step of the two proteins described here.

Increased Thermal Stability of AKC4-- The experiments done on apoAKC4 indicate that the four side chain substitution and zinc binding have a cumulative effect in increasing the thermal stability. Analysis of the crystal structures suggests that the stability of the LID domain is mainly due to a network of hydrogen bond interactions between several side chains (including the 4 substituted residues, Arg131, Tyr133, and Glu151) keeping closer the two small beta -sheets. The 4 Cys residues (by their smaller size and polar character) are able to integrate into this network, increasing the global thermal stability of the protein. Zn2+ binding has an additional contribution in restraining the global flexibility of this solvent-exposed domain. This decreased flexibility is one of the factors shown to differentiate the thermostable proteins from their mesophilic counterparts (21). By an induced effect, the zinc finger domain may also stabilize the helices connecting the domain to the protein core (alpha 6 and alpha 7), preventing the fraying of peripheral structural elements. In contrast, it has no significant effect on the unfolding of the parallel beta -sheet which takes place at higher temperatures.

The Tm of the AK from the thermophilic B. stearothermophilus (74.5 °C) (9) is similar to that of the second unfolding transitions reported here for AKe and AKC4. This means that besides the contribution of the zinc binding region there are other contributions to the thermostability, especially related to the external helices. Indeed, when the metal ion is removed from the thermophilic enzyme, Tm decreases to 67 °C, a value which is still considerably higher than in AKe.

In contrast with the increased stability against thermal and chemical denaturation of AKC4, its structural stability in standard physicochemical conditions appears to be lower than that of the wild-type enzyme (Table I). The explanation of this observation requires a reliable thermodynamic characterization of the protein unfolding, based on combined variation of several physicochemical factors (temperature, pH, chemical denaturant, and so forth). Also, the complete NMR spectral assignment, the structure determination and characterization of the internal dynamics of the proteins will provide the necessary structural basis. These studies are currently in progress in our laboratory.

    Aknowledgments

We thank Joël Mispelter and Petya Christova for useful discussions.

    FOOTNOTES

* This work was supported in part by grants from the Institut National de la Santé et de la Recherche Médicale, the Centre National de la Recherche Scientifique, Institut Pasteur, and Institut Curie.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: INSERM U350, Institut Curie-Recherche, Centre Universitaire, Bât. 110-112, 91405 Orsay Cedex, France. Tel.: 33 1 69 86 31 63; Fax: 33 1 69 07 53 27; E-mail: craescu{at}curie.u-psud.fr.

1 The abbreviations used are: AK, adenylate kinase; Ap5A, P1,P5-di(adenosine-5')-pentaphosphate; AKe, wild-type E. coli adenylate kinase; AKC4, adenylate kinase variant with four amino acid substitutions (H126C, S129C, D146C, and T149C); AKHC3, three-substitution variant (S129C, D146C, and T149C); LID, domain closing over ATP of AKe (residues 122-159); DQF-COSY, double-quantum filtered correlation spectroscopy; NOE, nuclear Overhauser effect; NOESY, nuclear Overhauser enhancement two-dimensional spectroscopy; TOCSY, total correlation spectroscopy.

2 S. Burlacu-Miron and C. T. Craescu, unpublished results.

    REFERENCES
Top
Abstract
Introduction
Procedures
Results
Discussion
References

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