research communications
Solution NMR structures of oxidized and reduced Ehrlichia chaffeensis thioredoxin: NMR-invisible structure owing to backbone dynamics
aSeattle Structural Genomics Center for Infectious Disease, USA, bEarth and Biological Sciences Directorate, Pacific Northwest National Laboratory, Richland, Washington, USA, cSchool of Molecular Biosciences, Washington State University, Pullman, Washington, USA, dDepartment of Medicine, Division of Allergy and Infectious Disease, University of Washington, Seattle, Washington, USA, eDepartment of Global Health, University of Washington, Seattle, Washington, USA, fDepartment of Microbiology, University of Washington, Seattle, Washington, USA, gCenter for Infectious Disease Research, Seattle, Washington, USA, and hDepartment of Biomedical Informatics and Health Education, University of Washington, Seattle, Washington, USA
*Correspondence e-mail: garry.buchko@pnnl.gov
Thioredoxins are small ubiquitous proteins that participate in a diverse variety of redox reactions via the reversible oxidation of two cysteine thiol groups in a structurally conserved active site. Here, the NMR solution structures of a reduced and oxidized thioredoxin from Ehrlichia chaffeensis (Ec-Trx, ECH_0218), the etiological agent responsible for human monocytic ehrlichiosis, are described. The overall topology of the calculated structures is similar in both redox states and is similar to those of other thioredoxins: a five-stranded, mixed β-sheet (β1–β3–β2–β4–β5) surrounded by four α-helices. Unlike other thioredoxins studied by NMR in both redox states, the 1H–15N HSQC spectrum of reduced Ec-Trx was missing eight additional amide cross peaks relative to the spectrum of oxidized Ec-Trx. These missing correspond to residues Cys35–Glu39 in the active-site-containing helix (α2) and Ser72–Ile75 in a loop near the active site, and suggest a change in backbone dynamics on the millisecond-to-microsecond timescale associated with the breakage of an intramolecular Cys32–Cys35 disulfide bond in a thioredoxin. A consequence of the missing amide resonances is the absence of observable or unambiguous NOEs to provide the distance restraints necessary to define the N-terminal end of the α-helix containing the CPGC active site in the reduced state. This region adopts a well defined α-helical structure in other reported reduced thioredoxin structures, is mostly helical in oxidized Ec-Trx and CD studies of Ec-Trx in both redox states suggests there is no significant difference in the secondary structure of the protein. The NMR solution structure of reduced Ec-Trx illustrates that the absence of canonical structure in a region of a protein may be owing to unfavorable dynamics prohibiting NOE observations or unambiguous NOE assignments.
Keywords: human monocytic ehrlichiosis; infectious diseases; thioredoxin; reactive oxygen species; structural biology; molecular dynamics; Ehrlichia chaffeensis; NMR.
PDB references: oxidized Ec-Trx, 6ali; reduced Ec-Trx, 6amr
1. Introduction
Thioredoxins are small proteins of approximately 100 residues that are found in organisms ranging from archaea to mammals and participate in a diverse variety of redox reactions via the reversible oxidation of two cysteine thiol groups to a disulfide (Holmgren, 1985, 1995). In the reducing environment inside the cell the primary function of Trxs is to prevent the formation of unwanted disulfide bonds (Collet & Messens, 2010), especially in metabolically essential enzymes such as ribonucleotide reductase (Laurent et al., 1964). Thioredoxins protect proteins from oxidative aggregation and inactivation (Holmgren, 1985, 1995), are a critical component of cellular antioxidant defense strategies against reactive oxygen and nitrogen species (Lu & Holmgren, 2014), play a role in regulation of apoptosis (Ravi et al., 2005), act as growth factors and modulate inflammatory responses (Powis et al., 2000). Once oxidized, Trxs are reduced by thioredoxin reductase via an NADPH-dependent reaction to reactivate the Trxs (Mustacich & Powis, 2000).
Human monocytic ehrlichiosis is an important emerging infectious disease in the United States (Paddock & Childs, 2003). The pathogen responsible, Ehrlichia chaffeensis, is an obligate intracelluar bacterium in the Anaplasmataceae family (Rikihisa, 2010) that is transmitted between mammals by the blood-sucking arthropod Amblyomma americanum (also known as the lone star tick; Ewing et al., 1995). Clinical symptoms of human monocytic ehrlichiosis include headache, fever, myalgia, anorexia and chills. While the severity of the disease may be limited to asymptomatic seroconversion, because E. chaffeensis replicates inside mammalian monocyte and macrophage cells, infection may lead to leukopenia and life-threatening complications such as kidney or respiratory failure. Consequently, human monocytic ehrlichiosis may represent the most prevalent life-threatening tick-borne infection in the United States (Olano & Walker, 2002). No vaccines against human monocytic ehrlichiosis exist and the choice of antibiotics available to treat infection is currently limited to doxycycline and rifampin, with the effectiveness of these treatments reduced if initiation of treatment is delayed. Since reactive oxygen species are abundantly produced by host monocytes and macrophages, it is expected that a robust Trx system is vital for intracellular survival of E. chaffeensis (Lu & Holmgren, 2014), and thus Trx inhibition may represent an intervention strategy for human monocytic ehrlichiosis. The 107-residue protein ECH_0218 (Ec-Trx) has been identified as a Trx in E. chaffeensis. To assist structure-based drug design (Staker et al., 2015) targeting Ec-Trx and to better understand cellular redox mechanisms, we describe the NMR solution structure and backbone dynamic features of Ec-Trx in the oxidized and reduced states.
2. Materials and methods
2.1. Cloning, expression and purification
The Ec-Trx gene (ECH_0218, YP_507041.1) was PCR-amplified using the genomic DNA of E. chaffeensis (strain Arkansas) and the oligonucleotide primers 5′-GGGTCCTGGTTCGATGATTGAGCAAATTGGAGACAGTG-3′ (forward) and 5′-CTTGTTCGTGCTGTTTATTAGTTTATATTGTTATTTATTTCACTAATTAT-3′ (reverse) (Invitrogen, Carlsbad, California, USA) containing LIC primers (bold). To enable protein purification by metal-chelation (Choi et al., 2011), the amplified Ec-Trx gene was inserted into the NruI/PmeI-digested expression vector AVA0421 by ligation-independent cloning such that the N-terminus of the expressed gene product contained a 21-residue extension: MAHHHHHHMGTLEAQTGPGS–. A heat-shock method was then used to transform the recombinant plasmid into Escherichia coli BL21(DE3)-R3-pRARE2 cells (a gift from SGC Toronto, Ontario, Canada). 750 ml of minimal medium (Miller) containing 15NH4Cl (1 mg ml−1), D-[13C6]-glucose (2.0 mg ml−1), NaCl (50 µg ml−1), MgSO4 (120 µg ml−1), CaCl2 (11 µg ml−1), Fe2Cl3 (10 ng ml−1) chloramphenicol (35 µg ml−1) and ampicillin (100 µg ml−1) was used to obtain uniformly 15N,13C-labeled Ec-Trx. The transformed cells were grown at 37°C to an OD600 of ∼0.8, transferred to a 25°C incubator and protein expression was induced with isopropyl β-D-1-thiogalactopyranoside (0.026 µg ml−1). Approximately 4 h later the cell culture was harvested by mild centrifugation and frozen (−80°C). Ec-Trx was purified from the thawed pellet using a conventional two-step protocol: metal-chelate on a 20 ml Ni-Agarose 6 FastFlow column (GE Healthcare, Piscataway, New Jersey, USA) followed by gel-filtration on a Superdex 75 HiLoad 26/60 column (GE Healthcare). The only difference between the protocols used to prepare oxidized and reduced Ec-Trx was the addition of 1 mM dithiothreitol (DTT) to the gel-filtration buffer (100 mM NaCl, 20 mM Tris pH 7.1) to obtain the reduced state.
2.2. spectroscopy
An Aviv Model 410 spectropolarimeter (Lakewood, New Jersey, USA) was used to collect M Ec-Trx in a quartz cell of 0.1 cm path length. A steady-state wavelength spectrum was first collected for oxidized Ec-Trx at 20°C in buffer containing no DTT (100 mM NaCl, 20 mM Tris pH 7.0). The same sample was then made 1.0 mM in DTT and the spectrum of reduced Ec-Trx was recorded 1 h later. Thermal curves were obtained for Ec-Trx in both states by recording the ellipticity at 220 nm in 2.0°C intervals from 10 to 90°C. The reported steady-state wavelength spectrum is the average of two consecutive scans, collected with a bandwidth of 1.0 nm and a time constant of 1.0 s, processed by subtracting a blank spectrum from the protein spectrum and automatic line smoothing using the AVIV software.
data from a 400 µl sample of ∼0.07 m2.3. Nuclear magnetic resonance spectroscopy
All NMR data were collected from double-labeled (13C,15N) samples of Ec-Trx (∼1.0 mM) using Agilent spectrometers operating at 1H resonance field strengths of approximately 600, 750 or 800 MHz. All spectrometers were equipped with an HCN probe, pulse-field gradients and Varian Biopack software. Because the 1H–15N HSQC spectrum of reduced Ec-Trx contained the best amide cross peak line shape and dispersion at 20°C, NMR data for both Ec-Trx redox states were collected at this temperature. For reduced Ec-Trx, the 1H, 13C and 15N chemical shifts of the backbone and side-chain resonances were assigned from analysis of two-dimensional 1H–15N HSQC, 1H–13C HSQC, HBCBCGCDHD and HBCBCGCDCHE spectra and three-dimensional HNCACB, CBCA(CO)NH, HCC-TOCSY-NNH, CC-TOCSY-NNH and HNCO spectra. Because the 1H–15N HSQC spectrum of oxidized Ec-Trx was similar to the 1H–15N HSQC spectrum of reduced Ec-Trx, fewer NMR experiments were required to assign the 1H, 13C and 15N chemical shifts for oxidized Ec-Trx: two-dimensional 1H-15N HSQC and 1H–13C HSQC spectra and three-dimensional CC-TOCSY-NNH and HNCO spectra. For samples in both redox states, three-dimensional 15N-edited NOESY-HSQC and 13C-edited NOESY-HSQC (aliphatic and aromatic) spectra, collected with a mixing time of 85 ms, were analyzed to obtain the side-chain 1H assignments and the NOE-based distance restraints required for the structure calculations. Slowly exchanging were identified by lyophilizing the double-labeled (13C,15N) samples, re-dissolving them in 99.8% D2O and immediately collecting a 1H–15N HSQC spectrum (∼10 min later). Steady-state {1H}–15N heteronuclear NOE values (NOE = Isat/Iunsat) were measured (20°C, 600 MHz 1H resonance field strength) in triplicate by taking the ratio of 1H–15N HSQC cross-peak heights in spectra recorded in the presence (Isat) and absence (Iunsat) of 3.0 s of proton presaturation prior to the 15N excitation pulse (Farrow et al., 1994). Felix2007 (MSI, San Diego, California, USA) and Sparky (v.3.115) were used to process and analyze, respectively, all of the NMR data. The 1H, 13C and 15N chemical shifts were referenced using indirect methods (DSS = 0 p.p.m.) and deposited in the Biological Magnetic Resonance Bank database (https://www.bmrb.wisc.edu) under accession numbers BMRB-19452 and BRMB-19938 for reduced and oxidized Ec-Trx, respectively.
2.4. Structure calculations
Using the 1H, 13C and 15N assignments and peak-picked NOESY data as initial experimental inputs, solution structures for Ec-Trx in the oxidized and reduced states were determined with the programs CYANA (v.2.1) and CNS (v.1.1) following previously described protocols (Buchko et al., 2015; Buchko, Hewitt et al., 2013). On the basis of preliminary structure calculations and trends, six restraints between the side-chain S atoms of Cys32 and Cys35 (2.0–2.1, 3.0–3.1 and 3.0–3.1 Å for the Sγ—Sγ, Sγ—Cβ and Cβ—Sγ distances, respectively) were introduced into the structure calculations to fix this disulfide bond in oxidized Ec-Trx (Sagaram et al., 2013). It was not possible to assign the side-chain atoms (13C and 1H) of the third conserved proline, Pro76, in Ec-Trx and unambiguously identify the conformational state of Pro76 based on the intra-residue NOE pattern between proline side-chain protons. In all reported Trx structures the third conserved proline residue is exclusively observed in the cis conformation (Collet & Messens, 2010), and therefore, this assumption was made in our structure calculations and Pro76 was constrained to the cis conformation in the structure calculations. The final ensemble of 20 CYANA-derived structures was refined with explicit waters with CNS (v.1.1) using the PARAM19 force field and of 500, 500 and 1000 kcal for the NOE, hydrogen-bond and dihedral restraints, respectively. For these water calculations, the upper boundary of the CYANA distance restraints was increased by 10% for reduced Ec-Trx and 5% for oxidized Ec-Trx, with the lower boundary set to the van der Waals limit for both. Structure quality was assessed with the online Protein Structure Validation Suite (PSVS v.1.5; Bhattacharya et al., 2007) and these values are included in the summary of structure statistics in Table 1. Atomic coordinates for the final ensemble of 20 structures for reduced and oxidized Ec-Trx were deposited in the Research Collaboratory for Structural Bioinformatics (RCSB) Protein Data Bank (PDB) under PDB codes 6amr and 6ali, respectively. Note that while the protein sequence in the BMRB and PDB is numbered continuously, Met1–Asn107, here the first native residue (Met22 in the BMRB and PDB sequence) is numbered Met1.
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3. Results and discussion
3.1. Solution structure of reduced and oxidized Ec-Trx
Fig. 1 shows a superposition of the ordered regions of the ensemble structure closest to the average for reduced (PDB entry 6amr, purple) and oxidized (PDB entry 6ali, wheat) Ec-Trx generated using the program SuperPose (Maiti et al., 2004). As observed in both NMR and X-ray crystallographic structures of other oxidized and reduced Trxs (Holmgren, 1985, 1995; Jeng et al., 1994; Amorim et al., 2007; Olson et al., 2013; Peterson et al., 2005; Qin et al., 1994; Stefanková et al., 2005; Collet & Messens, 2010), Ec-Trx is composed of a five-stranded, twisted, mixed β-sheet (↑↑↑↓↑; β1–β3–β2–β4–β5) surrounded by four α-helices. Helices α1 and α3 are located on one face of the β-sheet and helices α2 and α4 on the opposite face, with α3 approximately perpendicular to α2 and α4. The catalytic CGPC motif, Cys32–Cys35, is located at the N-terminal end of α2, exposed to the surface of the protein. The reduced and oxidized structures are generally similar, with a backbone r.m.s.d. of 2.0 Å between ordered regions. The most significant difference between the two structures obtained from the available NMR data is the length of α2, which extends between residues Pro34 and Tyr49 in the oxidized state but only between residues Gln41 and Glu51 in the reduced state (Fig. 1b). This difference appears to contrast with the crystal and NMR structures of other Trxs in both redox states, where no such dramatic change in α2 was observed (Holmgren, 1985, 1995; Jeng et al., 1994; Olson et al., 2013; Peterson et al., 2005; Qin et al., 1994; Stefanková et al., 2005; Collet & Messens, 2010). For example, in the NMR solution structures of human Trx and Mycobacterium tuberculosis TrxC in both redox states, the backbones of the region containing the active-site cysteine residues form part of an α-helix and superimpose well (Qin et al., 1994; Olson et al., 2013), with only the side-chain S–S distance increasing (1–1.5 Å) on going from the oxidized to the reduced state. Was the difference observed between the two NMR-based structures of Ec-Trx real or a consequence of the available NMR data for the structure calculations?
3.2. verification of cysteine oxidation states
Foremost in assessing the NMR structural differences in α2 is to ascertain the and disulfide-bond pairings of the cysteine residues under both conditions used in the structure calculations. The two cysteine residues in the active-site CGPC motif are conserved in all Trxs and are essential for (Collet & Messens, 2010). In addition to the two cysteine residues, Cys32 and Cys35, in the CGPC motif of Ec-Trx, a third cysteine, Cys17, is also present in the primary amino-acid sequence of Ec-Trx. Because the of the cysteine Cβ atom is sensitive to the redox state of the cysteine Sγ atom, it can be used to infer the redox states of cysteine residues in a protein (Sharma & Rajarathnam, 2000). Generally, the cysteine 13Cβ in the reduced state is <32 p.p.m. and increases to >35 p.p.m. in the oxidized state. The Cys17 13Cβ changes little in the presence (27.8 p.p.m.) and absence (27.9 p.p.m.) of the reductant DTT, unambiguously verifying that Cys17 in Ec-Trx is a free thiol under both conditions. While this is expected in the presence of DTT, in the absence of DTT this observation indicates that Cys17 is not forming intermolecular or intramolecular disulfide bonds. On the other hand, out of the two remaining cysteine residues, only the 13Cβ for Cys35 in the absence of DTT could be assigned because it was the only other cysteine amide that was detected in the 1H–15N HSQC spectrum under both conditions (Fig. 1b). At 35.7 p.p.m., the Cys35 13Cβ is consistent with the formation of an oxidized cysteine participating in a disulfide bond. The possibility of Cys35–Cys35 intermolecular disulfide-bond formation is excluded as both oxidized and reduced Ec-Trx eluted from a size-exclusion column with a characteristic of a monomer (data not shown). Because the 13Cβ for Cys17 is characteristic of a reduced cysteine, by elimination Cys35 must be forming a disulfide bond with Cys32. As described in §2.4, these trends, along with proximity in preliminary structure calculations, were used to justify the introduction of six restraints between the side-chain S atoms of Cys32 and Cys35 in the structure calculations.
3.3. Data and structure quality
The 1H–15N HSQC spectrum for reduced Ec-Trx shown in Fig. 2(a) contains amide cross peaks with good dispersion in both the 1H and 15N dimensions characteristic of a structured protein (Yee et al., 2002). In the absence of the reductant DTT the 1H–15N HSQC spectrum for oxidized Ec-Trx, shown in Fig. 2(b), was generally similar to the spectrum for reduced Ec-Trx except for the appearance of eight amide cross peaks (circled in orange in Fig. 2b) and more uniform amide cross-peak intensities. Cross peaks were also missing for ten backbone in Ec-Trx in both redox states. Missing amide resonances in 1H–15N HSQC spectra of Trxs appear to be uncommon in either redox state. One missing amide resonance at the second cysteine in the CGPC motif was reported in the 1H–15N HSQC spectrum of reduced Saccharomyces cerevisiae Trx2 (Amorim et al., 2007). Instead of disappearing amide resonances in 1H–15N HSQC spectra, a subset of amide cross peaks are usually observed to shift markedly in 1H–15N HSQC spectra of reduced and oxidized Trxs, as shown for human (Qin et al., 1994), E. coli (Jeng et al., 1994), Arabidopsis thaliana (Peterson et al., 2005) and M. tuberculosis (Olson et al., 2013) Trxs. In these examples, the overall backbone of solution structures for α2 determined in both redox states was similar except for slight differences in the region of the active site corresponding to with the observed perturbations. Missing amide resonances have been observed at a dimer interface (Buchko et al., 2017); however, size exclusion showed that Ec-Trx was monomeric in both redox states (§3.2) as is common for Trxs (Eklund et al., 1991). Missing or non-uniform amide resonances may also be indicative of transient association (Buchko, Lin et al., 2013); however, no significant changes in the 1H–15N HSQC spectra were observed following a tenfold dilution of the NMR samples used in our studies (data not shown). Instead, the missing amide cross peaks in the 1H–15N HSQC spectrum of reduced Ec-Trx observed here are likely to signify that this region of the protein is undergoing chemical exchange on an intermediate timescale (milliseconds to microseconds; Buchko et al., 1999; Ådén et al., 2011). For example, amide resonances in 1H–15N HSQC spectra have been observed to disappear in peroxiredoxins as a function of the redox state of a single pair of intramolecular cysteine residues, with the disappearance attributed to substantial changes in backbone dynamics (Ådén et al., 2011; Buchko et al., 2016). Here, the eight additional amide residues that are missing cross peaks in reduced Ec-Trx, Cys35–Glu39 and Ser73–Ile75, are at the N-terminal end of a helix containing the active site and a loop near this site, respectively. Note that in S. cerevisiae Trx2 the residues equivalent to Ec-Trx residues Ser73–Ile75 were reported to be considerably line-broadened in the reduced state (Amorim et al., 2007), indicating that this region in S. cerevisiae Trx2 was likely to be undergoing chemical exchange on a nearly similar intermediate timescale (milliseconds to microseconds). The amide resonances that are missing in both Ec-Trx redox states are for residues N-terminal to the residues that disappear in reduced Ec-Trx (Phe27–Gly33) and in a loop connecting β3 and α3 that is also near the active site (Ile58–Glu61; Fig. 1b). As illustrated in Fig. 3, all the missing amide resonances in both redox states (blue) or for reduced Ec-Trx (cyan) are clustered at or near the active site of the CGPC motif, implying intermediate timescale (milliseconds to microseconds) dynamics that expand upon breaking the Cys32–Cys35 disulfide bond.
Owing to the eight fewer amide cross peaks in the 1H–15N HSQC spectrum of reduced Ec-Trx, only 69% of the backbone and side-chain 1H, 13C and 15N chemical shifts were assigned for reduced Ec-Trx, compared with the 79% assigned for oxidized Ec-Trx (excluding the N-terminal tag). One consequence of this assignment difference, as summarized in the structure statistics in Table 1, was 270 fewer NOEs and 12 fewer hydrogen bonds in the structure calculations for reduced Ec-Trx. Despite these differences in restraints, the ordered regions, as defined by the PSVS program, of the final ensembles of 20 structures both converged well on the average structure, with backbone (N—Cα—C=O) and all-heavy-atom r.m.s.d.s of less than 0.8 and 1.2 Å, respectively. On the other hand, when using the complete native sequence (residues Met1–Asn107) for the r.m.s.d. calculations, the convergence is poorer for reduced Ec-Trx (1.5 and 2.1 Å) than for oxidized Ec-Trx (0.8 and 1.3 Å), reflecting the fewer restraints in the former calculations. The good convergence of the ordered regions of both structures is visually apparent in Figs. 4(a) and 4(b), which show a superposition of the ordered regions of the final ensemble of 20 structures upon the average structure. In both structure ensembles the region with the least convergence is also the region where the missing in the 1H–15N HSQC spectra cluster (Fig. 3): around the CGPC active site. Ensemble analysis with the PSVS validation software package further confirmed a quality set of final structures (Bhattacharya et al., 2007). The Ramachandran statistics for the φ/ψ pairs of all of the residues in both ensembles were overwhelmingly in acceptable space (>95.8% in most favored regions and >3.1% in additionally allowed regions) and all of the structure-quality Z-scores were acceptable (>−2). Hence, given the available NMR data as input for the structure calculations, the final ensemble of calculated structures meets the generally accepted criteria for acceptable solution structures.
Amide cross peaks were not observed for residues Cys35–Glu39 in the reduced state of Ec-Trx owing to chemical exchange on the intermediate timescale (milliseconds to microseconds) that broadens these resonances beyond detection (Ådén et al., 2011; Buchko et al., 2016). Consequently, the difference in the length of α2 in the calculated NMR structure for reduced Ec-Trx is likely to be owing to the absence of NOEs and backbone hydrogen bonds to define the structure in this region of the protein and does not represent the complete unfolding of approximately half an α-helix. This conclusion is supported by the steady-state wavelength CD spectra for reduced (purple) and oxidized (red) Ec-Trx shown in Fig. 5(a). The data were obtained by first measuring the CD spectrum of oxidizing Ec-Trx, making the sample in the CD cell 1 mM in DTT using a 1 M stock solution and collecting a spectrum for reduced Ec-Trx 1 h later. The spectra superimpose well and are characterized by a single minimum at ∼218 nm and an extrapolated maximum of >200 nm, which are features of a structured protein with a mixture of α-helical and β-strand components (Holzwarth & Doty, 1965). The superimposed CD profiles suggest that the structures of reduced and oxidized Ec-Trx are similar, and this is corroborated by similar (<1% difference) deconvolution values calculated using the AVIV software. More significantly, the absence of an increase in the ellipticity of the ∼218 nm CD band upon the addition of DTT to oxidized Ec-Trx suggests that half an α-helix does not disappear in reduced Ec-Trx. More likely, the full α-helix is still largely present out to Pro34, but only the backbone dynamics of the helix around the active site have changed to make it invisible in the 1H–15N HSQC spectrum. This illustrates that care should be taken when viewing `disordered' regions in ensembles of NMR-based structures because the absence of canonical secondary-structure elements may be a result of the absence of NOEs owing to intermediate (millisecond to microsecond) backbone dynamics that make structure in these regions NMR-invisible.
3.4. Steady-state {1H}–15N heteronuclear NOEs
The missing and broadened amide resonances in the 1H–15N HSQC spectra of Ec-Trx are likely to be the result of intermediate (millisecond to microsecond) backbone dynamics in the protein backbone localized around the active site, as summarized in Fig. 3. This active site is localized on the surface of the protein to facilitate interaction with substrate (binding and reduction; Gleason & Holmgren, 1988; Collet & Messens, 2010). Localized protein dynamics are known to play a role in the binding and catalysis properties at, and around, active sites (Ishima & Torchia, 2000) and have been proposed to play a role in the activity of Trxs (Stefanková et al., 2005; Amorim et al., 2007). To further probe the backbone dynamics of Ec-Trx, this time on the fast picosecond-to-nanosecond timescale, steady-state {1H}–15N heteronuclear NOE ratios were collected in triplicate for Ec-Trx and the mean results are presented in Fig. 6. In both redox states most of the ratios are above 0.8, an approximate value typical of well structured residues. The few exceptions are the termini, where ratios below 0.8 are often observed (Peterson et al., 2005), and a few isolated residues located at, or next to, loops between regions of ordered secondary structure. While these exceptions indicate localized points of thermal motion on the picosecond-to-nanosecond timescale and have been proposed to possibly play a role in switching between Trx redox states (Amorim et al., 2007), the near-uniform distribution of the steady-state {1H}–15N heteronuclear NOE ratios above 0.8 suggest that the Ec-Trx structure is otherwise relatively rigid in both redox states (Peterson et al., 2005).
3.5. Ec-Trx and conserved proline residues in the Trx scaffold
Highly conserved residues have been identified in Trxs, as illustrated for Ec-Trx and six other thioredoxins in Fig. 7. However, these conserved residues are all not essential for but instead play roles in dictating the structure, dynamics and redox properties of the protein (Collet & Messens, 2010). Included in this group of conserved residues that are not essential for catalysis are three proline residues. In Ec-Trx, the first conserved proline is Pro34 located in the CGPC motif that plays a large role in determining the reducing power of Trxs (Collet & Messens, 2010). The second proline, Pro40, is six residues away from the first and serves to introduce a kink into α2 that isolates the CGPC motif from the rest of the helix (Collet & Messens, 2010), as shown here for oxidized Ec-Trx (Figs. 1 and 4). Proline residues in the middle of α-helices are known to introduce a kink into the helix (Woolfson & Williams, 1990). In reduced Ec-Trx Pro40 separates α2 into regions with amide cross peaks that are absent or present in the 1H–15N HSQC spectrum. As illustrated in Fig. 7, the four amino acids between the conserved last cysteine in the CGPC motif and the conserved proline appear to be semi-conserved (similar) in Trxs. However, in Ec-Trx only two of these four residues are semi-conserved. It may be that the SM and AE differences at the second and fourth positions, respectively, in Ec-Trx destabilize the N-terminus of α2 enough to introduce backbone dynamics on the millisecond-to-microsecond timescale after breaking the intramolecular Cys32–Cys35 disulfide bond. The third conserved proline residue, Pro76, is located just before β4. As described in §2.4, this proline is always observed in the cis conformation (Collet & Messens, 2010), and therefore, was constrained to the cis conformation in our structure calculations. This proline is in a loop spatially near the CGPC motif, and amide cross peaks for the three residues N-terminal to Pro76, Ser73–Ile75, are not observed in the 1H–15N HSQC spectrum of reduced Ec-Trx (Figs. 1 and 3), suggesting that the dynamics of this proximal region are also affected by the reduction of the Cys32–Cys35 disulfide bond.
3.6. Thermal stability
As described earlier, the major negative CD band for reduced and oxidized Ec-Trx with a minimum at ∼218 nm is a spectral feature of a structured protein with a mixture of α-helical and β-strand components (Fig. 5a). The thermal stability of Ec-Trx in both redox states can be assessed by measuring the ellipticity at 218 nm at 2.0°C intervals between 10 and 90°C. In this spectral region, an increase in ellipticity with increasing temperature is generally associated with the transition from a structured to a denatured state (Karantzeni et al., 2003). As shown in Fig. 5(b), the ellipticity for oxidized Ec-Trx (red) largely increases in a regular fashion from 10 to 88°C. On the other hand, the ellipticity for reduced Ec-Trx (purple) essentially follows the profile for oxidized Ec-Trx (red) until ∼80°C and then increases rapidly, with precipitate observable after cooling (irreversible denaturation). This difference suggests that in the presence of an intramolecular disulfide bond the temperature of thermal increases, making the oxidized protein more stable. In general, oxidized Trxs are more stable than the reduced form, with this difference in stability being a driving force for the catalytic reaction (Collet & Messens, 2010). For example, a 12°C increase in thermal stability was observed for E. coli Trx between the reduced and oxidized states (Jeng et al., 1994; Qin et al., 1994). Because the small structural changes observed between E. coli Trx in the reduced and oxidized states cannot account for the significant thermal and chemical stability differences between the two redox states, it was proposed that these stability differences may be owing, at least in part, to changes in the dynamic properties of E. coli Trx in the reduced and oxidized states (Stefanková et al., 2005). The dynamic differences implied by the disappearance of eight amide cross peaks in the 1H–15N HSQC spectrum of reduced Ec-Trx (Fig. 2) may play a role in the decreased thermal stability of reduced Ec-Trx despite the general similarities of the structures in both redox states (Fig. 1).
4. Conclusions
The overall topology of the solution structures determined for Ec-Trx in the oxidized and reduced states is similar to the topology reported in other thioredoxin structures. Using the available NMR data, the length of the α-helix containing the CGPC active site (α2) was observed to extend between residues Gly33 and Tyr49 in the oxidized state but only between residues Gln40 and Gln48 in the reduced state. However, these structural differences in the catalytic helix are very likely to be owing to the absence of proton–proton NOEs that are essential to define this region during the structure calculations, making the structure NMR-invisible in this region. These NOEs are missing because eight amide cross peaks are absent in the 1H–15N HSQC spectrum of reduced Ec-Trx relative to that of oxidized Ec-Trx. While the absence of these cross peaks is detrimental to the structure calculations, they do identify a change in the backbone dynamics on the intermediate millisecond-to-microsecond timescale associated with the breakage of an intramolecular Cys32–Cys35 disulfide bond. Dynamics have been suggested to play a contributing role in the catalytic function of thioredoxins and their roles in the thioredoxin system. If the dynamics observed here for Ec-Trx are unique to the intracellular bacterium E. chaffeenis, this may represent a potential pathway for new intervention strategies for human monocytic ehrlichiosis.
Acknowledgements
The internal SSGCID ID for Ec-Trx is EhchA.00546.a. Battelle operates PNNL for the US Department of Energy.
Funding information
This research was supported by the National Institute of Allergy and Infectious Diseases (NIAID) through Federal Contract Nos. HHSN2722001200025C and HHSN272200700057C. Most of this research was performed at the W. R. Wiley Environmental Molecular Sciences Laboratory (EMSL), a national scientific user facility located on the Pacific Northwest National Laboratory (PNNL) campus and sponsored by the US Department of Energy's Office of Biological and Environmental Research Program.
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