Yifen
Tang
a,
Zhen
Cao
a,
Elsa
Livoti
b,
Ulrich
Krauss
c,
Karl-Erich
Jaeger
c,
Wolfgang
Gärtner
a and
Aba
Losi
*b
aMax-Planck-Institute for Bioinorganic Chemistry, Stifstrasse 34-36 45470, Mülheim, Germany
bDepartment of Physics, University of Parma, viale G.P. Usberti 7/A, 43100, Parma, Italy. E-mail: aba.losi@fis.unipr.it
cInstitute of Molecular Enzyme Technology, Heinrich-Heine-University Düsseldorf, Research Center Jülich, Stetternicher Forst, 52426, Jülich, Germany
First published on 30th November 2009
YtvA from Bacillus subtilis is a blue-light responsive, flavin-binding photoreceptor, built of a light-sensing LOV domain (aa 25-126) and an NTP (nucleoside triphosphate)-binding STAS domain (aa 147-261). The STAS domain is supposed to be the effector part of the protein or a secondary switch. Both domains are connected by a linker polypeptide. The active form of YtvA is generated upon light excitation, causing the formation of a covalent bond between a cysteine residue (Cys62) in the LOV domain and the position 4a of the flavin chromophore. This photoadduct formation within the LOV domain results in a conformational change of the NTP-binding cavity, evidencing intra-protein signal transmission. We have previously shown that Glu105, localized on the beta-scaffold of the LOV-core, is involved in this process. Here, we extend this work by the identification of further residues that upon mutation supress or strongly impair signal transmission by interfering with the communication between the two domains. These comprise L106 and D109 on the LOV domain; K130 and K134 on the linker region; D193, L194 and G196 within the DLSG GTP-binding motif (switch region) and N201 on the STAS domain. Furthermore in the mutated S195A and D193A proteins, GTP affinity is diminished. Other mutations investigated have little or no effect on signal transmission and GTP-binding affinity: R63K that was found to accelerate the thermal recovery of the parent state ca. ten-fold; K128A, Q129A and Y132A within the linker region, and S183A and S212A on the STAS domain. The results show a key role of the LOV domain beta-scaffold and of positively charged residues within the linker for intra-protein signal transmission. Furthermore they evidence the conformational switch function of a structurally conserved strand-loop-helix region (bearing the DLSG GTP-binding motif and N201) within the STAS domain that constitutes a novel GTP-binding fold.
Fig. 1 (top) Structure of YtvA-LOV + linker (PDB entry 2pr5, chain A; (bottom) model of YtvA-STAS. Mutated residues causing a negative effect on signal transmission or GTPTR-binding are shown in black. For the effects of Y132A and R63A see text. |
The LOV-based photochemistry has first been discovered in the plant blue-light receptors phototropins (phot), built of two LOV domains in tandem, LOV1 and LOV2, and a C-terminally located S/T-kinase domain.10,11 In phot, the activity of the effector S/T-kinase domain is enhanced after LOV photoactivation with blue-light, resulting in phot auto-phosphorylation,12-14 a key event in signaling.15 LOV proteins other than phot, including the steadily growing bacterial family, bear solely one LOV domain, and the effector module can be represented by several functional motifs, e.g., a histidine kinase, gene-expression regulators, phosphodiesterases, phosphatases).2,16,17 This poses the question whether LOV domains communicate with effector partners through the same or partially overlapping surfaces, such that the structural basis for light-to-signal transduction is basically the same in the different LOV proteins, with only few residues acting as specific signal transmitters within the different systems. There is increasing experimental evidence that this surface largely involves the β-scaffold of the LOV-core (Fig. 1) which on one side hosts residues directly interacting with the isoalloxazine ring of FMN18,19 and on the other side communicates with helical regions flanking the LOV-core.20,21 As an example, a conserved glutamine on strand Iβ (Gln513 in Avena sativa phot1-LOV2) participates in light-driven conformational changes of LOV2,22-26 and of the LOV protein VIVID21 and in the light-activation of phot self-phosphorylation.27 The latter process is triggered by the light-induced unfolding of the so called Jα-linker helix, that interacts in the dark with the β-scaffold of LOV2 and connects LOV2 to the kinase domain.28,29,30 Moreover, the β-scaffold is involved in LOV-LOV dimerization, with or without the assistance/competition of the helical flanking regions.31-33 In VIVID, light-activation induces dimerization through the helical N-cap, but cross-linking data suggest that dissociation or removal of the N-cap induces dimerization via a β-sheet−β-sheet contact.34 In YtvA, the β-scaffold of the LOV-core has been identified as a competitive interface for LOV-LOV dimerization and intraprotein domain interactions,31 and a recently crystallized structure confirms the β-sheet mediated contact within the YtvA-LOV dimer.32
Due to its prokaryotic origin and the relatively small size (261 aa), YtvA is readily expressed as a full length protein and thus offers the possibility to study light induced changes also in the effector/signalling STAS domain. However, no three-dimensional structure of full-length YtvA is yet available, leaving a discussion on residues that potentially enable communication between the LOV- and the STAS domain at a speculative level. A preliminary investigation revealed that glutamic acid 105, localized on strand Hβ, is involved in signal transmission from LOV- into STAS domain (STAS, Sulfate Transporter and Anti-sigma factor antagonist).35 Although its exact function is not yet known, the STAS domain is thought to be the effector module of the protein or a secondary switch. It has been shown to bind ATP (adenosine triphosphate) and GTP (guanosine triphosphate),36 in agreement with a proposed general role of STAS domains as NTP (Nucleotide triphosphate) binding folds.37 E105 should therefore be located at that surface of the LOV domain interacting with the linker region or/and the STAS domain.
Communication between the two domains of YtvA is readily monitored by the blue light-induced conformational changes of the NTP-binding cavity of the STAS domain, i.e. by recording the spectroscopical changes in case a fluorescent, red light absorbing GTP derivative is employed.36 Specifically, a BODIPY® TR GTP (GTPTR) compound was chosen whose absorption and fluorescence maxima (ca. 590 and 620 nm, respectively) do not interfere with those of FMN (ca. 450 and 500 nm).38 Upon binding to YtvA (dissociation constant KDca. 40 μM in the light-activated state), the fluorescence of GTPTR increases with a concomitant, few nanometers red-shift of the absorption maximum.36 The thermally driven recovery reaction results in a further increment of fluorescence and of the absorption red-shift, indicative of conformational changes in the GTPTR binding cavity.36 These light-dark differences are fully reversible in the wild-type protein, but are completely suppressed in the mutated YtvA-E105L protein, although binding of GTPTR is not impaired.35 E105 is conserved in all YtvA-like proteins in the Firmicutes, while in phot-LOV domains this position is invariably occupied by a hydrophobic amino acid (generally leucine).17 In phot1-LOV2 this residue, Leu493, makes van der Waals contact to Ile532 on the Jα-linker,20 and the Ile532E mutation disrupts the LOV2-Jα interaction, rendering the kinase domain constitutively active.29 For YtvA, there is no evidence that light activation implies unfolding of the J-linker,31 neither does the presence of the J-linker prevent YtvA-LOV dimerization.32,39 Dimerization via the LOV-domain is only impaired in the full-length protein, at least in diluted solution.31 It is therefore conceivable that the LOV-core directly interacts with the STAS domain through the β-scaffold, possibly with the participation of the J-linker and by employing specific residues devoted to signal transmission.
We here present an extended investigation on the signalling pathway in YtvA, employing a set of selectively designed mutations, and using the GTPTR-binding assay and the GTPTR-based LOV-STAS signal transmission detection. A similar set of mutations has been recently investigated to study their role in the physiological function of YtvA in B. subtilis, making use of a reporter-protein mediated assay.6
By means of a fast cycling mutated protein, YtvA-R63K, suitable for spectroscopical studies and here fully characterized, we demonstrate the tight coupling between the LOV domain and the GTPTR-binding cavity on the STAS domain, even for the case of a strongly accelerated thermal recovery reaction. We also highlight the functional role of a second acidic amino acid, D109, typical of the YtvA-family and of L106, both localized on strand Hβ. In addition, our data reveal the functional role of charged amino acids (K130 and K134) within the J-linker, and of the DLSG193-196 Walker B- (Switch II) motif40 on the STAS domain. As a whole, the results stress the importance of the LOV-core strand Hβ and of specific residues within the J-linker in inter-domain signal transmission and confirm that YtvA-STAS is a novel NTP-binding fold, showing a conformational change switched by light within its NTP-binding cavity, through its coupling to the LOV domain.
Primers used for the Quick Change method were:
R63K. Forward: 5′-GAAATTTTAGGAAAGAACTGTTTCTTACAGGGGAAACACAC-3′
Reverse: 5′-GTGTGTTTCCCCTGTAAGAAACAGTTCTTTCCTAAAATTTC-3′
L106F. Forward: 5′-GGAACGATGTTCTGGAATGAATTAATATTGATCCAATGGAAATAGAG-3′
Reverse: 5′-CTCTATTTCCATTGGATCAATATTAATTCATTCCAGAACATCGTTCC-3′
D109L. Forward: 5′-TGGAATGAATTAAATATTTCCAATGGAAATAGAGGATAAAACG-3′
Reverse: 5′-CGTTTTATCCTCTATTTCCATTGGAAATATTTAATTCATTCCA-3′
K128A. Forward: 5′TGATATCACCCAAAAAGAATATGAAAAGCTTCTCGAGGATTCCCTCACG-3′
Reverse: 5′-CGTGAGGGAATCCTCGAGAAGCTTTTCATATTCTTTTTGGGTGATATCA-3′
Q129A. Forward: 5′-CAGAATGATATCACCAAGAAAAGAATATGAAAAGC-3′
Reverse: 5′-GCTTTTCATATTCTTTTCTTGGTGATATCATTCTG-3′
K130A. Forward: 5′- GAATGATATCACCAAGCAAGAATATGAAAAGCTTCTCG-3′
Reverse: 5′-CGAGAAGCTTTTCATATTCTTGCTTGGTGATATCATTC-3′
Y132A. Forward: 5′- CCAAGCAAAAAGAAGAAAAGCTTCTCGAGGATTCCCTCACG-3′
Reverse: 5′-CGTGAGGGAATCCTCGAGAAGCTTTTCTTCTTTTTGCTTGG-3′
The remaining mutations had been performed by a two step protocol following the megaprimer approach by using a plasmid-specific universal reverse primer and a mutagenic forward primer in a first run and then continuing with the thus generated DNA duplex in a second PCR reaction.
Universal reverse primer: 5′-TTTTGGATCCTTACATAATCGGAAGCACTTTAAC-3′,
S183A 5′-TTGACGAATATCTTAACATCCAAAGATG-3′
D193A 5′-GATTATTTGATCATTTTATCCGGATTGG-3′
L194A 5′-TATTTGATCATTGATTCCGGATTGGCCC-3′
S195A 5′-TTGATCATTGATTTAGGATTGGCCCAAG-3′
G196A 5′-ATCATTGATTTATCCTTGGCCCAAGTGAAC-3′
N201A 5′-GATTGGCCCAAGTGGAACAAACGGCC-3′
S212A 5′-CAAATTTTCAAGCTGCATTTGCTGAAATTG-3′
For all mutagenesis experiments, the obtained PCR products were treated with the restriction enzyme DpnI (New England BioLabs). DpnI is specific for methylated and hemimethylated DNA (targeting sequence: 5′-Gm6ATC-3′) and is used to digest the parental DNA template in the PCR products. 0.5 μl DpnI (20000 U/ml) was added to each PCR product and the digestion reaction was carried out at 37 °C for 30 minutes. In all cases, mutations were confirmed by sequencing.
His-tagged, mutated proteins were obtained from expression in E. coli (BL21) (Stratagene, Amsterdam, The Netherlands) using IPTG- (BioMol, Hamburg, Germany) induction and employing the pET28a plasmid (Novagen-Merck, Darmstadt, Germany), as described.8 The proteins were purified by affinity chromatography on a Talon resin (Qiagen, Hilden, Germany) according to the standard given protocol and adding in each step 200 mM PEFABLOC and 0.8 mM mercaptoethanol; the Talon resin loaded with the cell extract, was washed 5 times with the protocol given washing buffer plus 10 mM imidazole. The protein was then eluted in one step with 130 mM imidazole. The protein was concentrated by centrifugation at 10 °C employing centrifuge tubes with 10,000 Da cutoff and a final, storage buffer composed of Na-phosphate 10 mM, NaCl 10 mM, pH = 8. Care was taken not to concentrate the protein above 170 μM during centrifugation, because this leads, in our experience, to irreversible aggregation and inhomogeneous oligomeric composition.
With the exception of YtvA-R63K, binding experiments for the determination of the dissociation constant, KD, were carried out with YtvA proteins in their blue-light activated state (i.e. FMN covalently bound to Cys 62), achieved by illuminating the sample with a blue-light emitting Led-Lenser ® V8 lamp (470 nm, Zweibrüder Optoelectronics, Solingen, Germany) as previously described.36 The blue-light was switched-off just prior recording of the absorption and fluorescence spectra, ensuring that at least 95% of the sample is present as FMN-Cys adduct, given the long lifetime for the recovery to the dark state (denoted as YtvA450 from the absorption maximum of the bound flavin), τrec > 3500 s at 20 °C.8,41,42 The fluorescence spectra were always recorded upon excitation at 590 nm (where solely GTPTR absorbs) and no energy transfer can occur from or to other fluorophores (e.g. FMN or aromatic amino acids).
The calculation of KD was carried out as previously described.36 We define α = ΔF/ΔFmax as the fraction of bound ligand, where ΔF is the variation of the normalized fluorescence of GTPTR in the presence of the protein with respect to free GTPTR; ΔFmax is the maximum fluorescence enhancement corresponding to αmax, i.e.α =1. The value of ΔFmax was determined by the non-linear fitting for one-site binding (eqn 1):
(1) |
Where [P]tot = total concentration of protein added (bound + free), in our cases ranging between ca. 8 and 80 μM. Assuming a 1:1 complex and with α = ΔF/ΔFmax we can fit αvs. the concentration of free protein, as detailed in (eqn 2), where αmax must extrapolate to 1 if the assumption is correct:
(2) |
In principle, KD in eqn 2 is different from K′D in eqn 1, but in our case the two values are very similar given that the association is weak and [P]tot≅ [P]free total. Given that binding of GTPTR to YtvA induces a red-shift in the absorption spectrum, we also evaluate KD by employing ΔAbs in place of ΔF in eqn 1.
prot/FMN | K Da,b/μM (ΔFluo) | K Da,b/μM (ΔAbs) | Dark-Light GTPTR Spectral Changes | |
---|---|---|---|---|
a K D = dissociation constants. b Errors derive from at least 2 sets of measurements for each sample and from errors reported by the fitting algorithm. | ||||
YtvA-WT | 1 | 38 ± 5 | 26 ± 5 | Yes |
YtvA-WT | 4 | 15 ± 7 | 8.5 ± 2 | Yes |
LOV domain mutations | ||||
R63K | 1 | 28 ± 11 | 16 ± 2 | Yes |
E105L | 1 | 43 ± 6 | 43 ± 10 | No |
L106F | 1 | 60 ±13 | 81 ± 23 | Minor |
D109L | 2 | 13 ± 3 | 11 ± 2 | No |
Linker | ||||
K128A | 1 | 26 ± 2 | 36 ± 4 | Yes |
Q129A | 1 | 20 ± 5 | 42 ± 11 | Yes |
K130A | 1 | 54 ± 9 | 92 ± 23 | Minor |
Y132A | 1 | 62 ± 7 | 79 ± 18 | Yes, > ΔF than WT |
K134A | 1 | 76 ± 20 | 19 ± 5 | No |
S139A | 1 | 19 ± 2 | 11 ± 2 | Yes |
STAS domain | ||||
D193A | 4 | 67 ± 23 | 61 ± 6 | No |
L194A | 1 | 84 ± 25 | 34 ± 5 | Minor |
S195A | 1 | 300 ± 70 | 120 ± 50 | Yes |
G196A | 2 | 10 ± 3 | 2 ± 1 | No |
N201A | 1 | 23 ± 5 | 52 ± 27 | Minor |
S183A | 1 | 76 ± 40 | 65 ± 19 | Yes |
S212A | 1 | 87 ± 10 | 84 ± 15 | Yes |
The effects of mutations were monitored by recording two distinct phenomena: 1) the protein binding capacity for GTPTR (dissociation constant KD, see eqn 1 and 2), determined by the change in its (normalized) fluorescence intensity and by the red-shift in the absorption maximum upon binding; 2) effects on LOV-STAS signal transmission, monitored by following the spectral changes of bound GTPTR after formation of the FMN-cysteine photoadduct. This effect had been described in YtvA-WT as a slight absorption blue-shift and fluorescence decrease that reverses in the dark.35 Throughout the text, α is defined as the fraction of bound ligand, as detailed in the material and methods section.
All the proteins investigated exhibited a photocycle similar to YtvA-WT, with a slow recovery (ca. 4000 ± 1000 s at 20 °C) to the parent state. The sole exception was YtvA- R63K (vide infra).
Fig. 2 Dark recovery of (a) FMN, (b): W103 (LOV core), and (c) GTPTR (STAS domain) fluorescence for YtvA-R63K. The excitation wavelengths were 305, 280 and 590 nm, respectively. Kinetics traces were recorded at 20 °C. The values of τrec obtained from a mono-exponential fitting were: (a) 485 s; (b) 365 s; (c) 511 s. |
The kinetic effects of this mutation are similar to those observed in the LOV1 from Chlamydomonas reinhardtii phot, where the corresponding mutation (R58K) accelerates the recovery time from 204 to 73 s at 20 °C.44 As for the GTP-binding capacity and signal transmission, YtvA-R63K behaves very similar to the WT protein, showing the previously characterized absorption blue-shift and fluorescence decrease of bound GTPTR upon formation of the photoadduct (Table 1).
YtvA-R63K is thus suitable for spectroscopic and functional studies, given its accelerated photocycle and the fact that the dark recovery of three different regions of the protein can be easily followed by monitoring the fluorescence of FMN (LOV core), GTPTR (STAS domain) and of W103 (Hβ strand of the LOV core). Observation of changes of W103 is very supportive, since it was previously demonstrated to be an independent marker for interdomain interactions.45 The resulting recovery lifetimes are τrec,F= 480 s, τrec,TR= 511 s and τrec,W= 365 s, respectively (20 °C), clearly demonstrating the tight coupling of the three protein regions (Fig. 2).
For monitoring the kinetics traces, excitation (λex) and emission (λem) wavelengths were selected as follows: for FMN λex = 305 nm and λem =500, for GTPTRλex = 590 nm and λem = 620 nm, for W103 λex = 280 nm and λem =340 nm. FMN was excited in a “valley” of the absorption spectrum, in the UVB region and not with blue-light, in order to minimize secondary photochemistry leading to formation of the photoproduct during recording of the traces. We have infact verified that this methodology gives identical results as tracing the recovery of absorption, whereas flavin excitation at 450 nm triggers photolysis during emission spectroscopy, leading to artifacts in the kinetics traces.39
Another strategically positioned amino acid of this region is L106. Its side chain points towards the chromophore cavity and comes into close contact with the isoalloxazine ring.32 The L106F mutation diminishes but not completely abolishes the light-induced changes of GTPTR (see Table 1). The affinity for GTP appears to be slightly lower than for YtvA-WT, but remains definitely within the same range; this latter effect might result from a perturbation of the overall protein tertiary structure due to the introduced change and is observed also for other mutations (Table 1). We note nevertheless that these three mutations do not affect either the oligomeric state of the protein, that remains mainly monomeric as shown by gel filtration experiments, or the secondary structure composition, as indicated by circular dichroism data.39,43
Fig. 3 Absorption and fluorescence spectra of GTPTR partially bound to (a) YtvA-K128A and (b)YtvA-K130A, in the dark (dashed lines) and light (solid lines) state. The value of α is ca. 0.5 for both proteins. The two proteins are examples for signal-transmission “innocent” (K128A) and “guilty” (K130A) mutations. |
The uncoupling between LOV domain and GTP-binding site on the STAS domain is best appreciated by observing the kinetics traces for the dark-recovery fluorescence of FMN and of GTPTR. For a signal-transmission “guilty” mutation (e.g. K130) the latter fluorescence does not change, whereas the recovery of FMN fluorescence follows the usual pattern (Fig. 4). For a signal-transmission “innocent” change (e.g. K128) the two traces follow instead a similar time-course.
Fig. 4 Time course for the dark-recovery of fluorescence for (a) YtvA-K128A and (b) YtvA-K130A at 20 °C. The GTPTR fluorescence (full lines) has been recorded at 620 nm after 590 nm excitation. FMN (dashed lines) was excited at 305 nm and fluorescence was recorded at 500 nm. Conditions as in Fig. 3. |
In the case of mutation Y132A, light induced absorption changes are similar to YtvA-WT (showing a shift of ca. 2.5 nm with α = 0.5), but the light-induced decrease of GTPTR fluorescence is larger (ca. 10% with α = 0.5, compared to 5% in YtvA-WT) (Table 1, Fig. 5), suggesting a larger conformational change in the nucleotide-binding cavity.
Fig. 5 Absorption and fluorescence spectra of GTPTR partially bound to YtvA-Y132A, in the dark (dashed lines) and light (solid lines) state. The value of α is ca. 0.5. The light-induced spectral changes in this protein are larger than in YtvA-WT. |
Fig. 6 Partial alignment of LOV proteins forming the YtvA-family in Firmicutes, highlighting the mutations studied in this work (with the exception of R63K, that solely accelerates the photocycle) and their conservation throughout the family (Glu in place of Asp109 has been held as conservative substitution). Accession numbers for the proteins are taken from the UniProt Knowledgebase (Swiss-Prot + TrEMBL) databank.50 Abbreviations: B. = Bacillus, O. = Oceanobacillus, L = Listeria. Residues whose mutation impairs light triggered conformational changes transmission from LOV domain to the GTP-binding cavity on STAS domain and/or GTP affinity, are highlighted in green. Y132, whose mutation in alanine increases the light triggered conformational changes is highlighted in light-blue. Residues whose mutations have negligible effects are in grey. Numbering is from YtvA. Published secondary structures for the LOV domain are shown on top (arrows = strand, cylinders = helices, lines = turns/coils),32 with the nomenclature used in this work. Our modelled secondary structure elements for the STAS domain are shown,36 with nomenclature as in Aravind and Koonin.37 |
An acidic amino acid corresponding to E105 is present solely in bacteria and a second acidic residue (aspartate or glutamate) at position 109 is exclusive for YtvA-like proteins in the Firmicutes.17 Both E105 and D109 are oriented towards the exterior of the FMN binding cavity and at the interface of the YtvA-LOV dimer.31,32 Here we have shown that both amino acids are key elements for LOV-to-STAS signal transmission, as detected by the light-induced conformational changes of the GTP-binding cavity. A careful inspection of the GTPTR absorption spectra when bound to YtvA-E105L suggests that this mutated protein is locked in a light-activated conformation,35 whereas the presence of apoprotein in the YtvA-D109L preparation does not allow a similarly strict conclusion. If the NTP-binding properties are linked to a physiological response, the E105L mutation should thus result in constitutive activity of YtvA, e.g. activation of σB, and in any case there should be no light influence for both E105L and D109L. We have now evidence, from comparative in vivo data, that this is indeed the case: in particular, the mutated YtvA-E105L protein constitutively up-regulates σB, whereas the contrary holds for YtvA-D109L.6
It is striking that E105 seems to have a similar role as the corresponding Leu493 in plant phot that makes contact to Ile532 on the Jα-linker.20 The disruption of this contact by the I532E mutation disrupts the LOV2-Jα interaction and renders the kinase domain constitutively active.29 In case of YtvA, nevertheless, we cannot extrapolate with certainty that E105 makes contact with the linker, given that in the dimeric YtvA-LOV this is definitely not the case (vide infra).32
Our results confirm a previous conformational analysis that proposed the β-scaffold as a competitive interface for LOV-LOV dimerization and intraprotein interactions. They further identify the two conserved negatively charged amino acids as essential for the LOV-to-STAS signal transfer.
A leucine or another small apolar amino acid in the position corresponding to L106, is typical for phot-LOV1 and is changed for phenylalanine in LOV2, where it has been suggested to be a key element during phototropin activation.46 In known LOV domain structures, FMN is sandwiched between this residue and the reactive cysteine.18-20,32 In neochrome1-LOV2 (neo1-LOV2),18 a substitution of the corresponding Phe1010 by a leucine renders LOV2 similar to LOV1 in terms of light-induced structural changes, i.e. they become smaller and temperature independent.46 The reported larger light-induced structural changes of LOV2 with respect to LOV1 are in part ascribed to this residue (F1010) due to its larger capacity to activate the kinase domain via perturbations that propagate from FMN to F1010 viaπ-π stacking interaction, and further to the Jα-helix facilitating its unfolding.46 On the contrary, the opposite substitution, L106F in YtvA-LOV impairs signal transmission to the STAS domain, instead of facilitating it (this work). We cannot compare this result with similar data for phot-LOV1 because, to our knowledge, a similar mutation has not been reported so far. It might be that in YtvA-LOV a phenylalanine in this position cannot assume the same conformation as in LOV2 (being stacked with the isoalloxazine ring of FMN), due to other and still undetermined factors. However, our data stress the importance of the amino acid that faces the flavin ring, opposite to the reactive cysteine, in conveying the signal to the partner domain.
We are aware that the oligomeric state of YtvA is subject of controversy. The crystal structure of the extended YtvA-LOV+J-linker domain is dimeric,32 and it was suggested that the J-linker forms a coiled-coil dimer that works as light-activated rotary switch during regulation of a fused kinase domain.47 Nevertheless we showed that the full-length protein is mostly monomeric, at least at μM concentrations (see also Materials and methods) and that the oligomeric state and secondary structure pattern of the protein is not altered by the present mutations of the Hβ-strand.39 This, together with the in vivo data, allows us to conclude that the said mutations are truly affecting light-to-signal-transmission and not the overall conformation of the protein.
Notwithstanding the similarity, it is quite improbable that YtvA-STAS binds NTPs with the same configuration as GTP-binding proteins, because the required P-loop structure (Walker A)40 is missing. An alternative way of NTP-binding to STAS domains has been suggested, resembling lipid association by Sec14 domains, which have a very similar folding as SPOIIAA but show a poor sequence similarity.37 The conserved loop would thus be involved in binding of the γ-phosphate group, resembling the role of DXXG in small GTP-binding proteins, whereas the β-scaffold and helix 1 and 2 might accommodate the rest of the nucleotide. Structures of Sec14 domains are available in the PDB databank (e.g.3B74),49 but their similarity with STAS domains, as for ligand binding, remains to be demonstrated. This hypothesis is nevertheless supported by the observation that in YtvA the N201A mutation impairs the light-switched conformational changes within the GTP-binding cavity, given that N201 is localized within the conserved loop at the N-terminal end of helix 2. The DXXG sequence is in the vicinity of the phospholipid end l in Sec14, in the same position as YtvA-STAS and GTP-binding proteins, although it is not directly involved in binding.49
Finally we have shown that an up-to-now putative GTP-binding/switch motif is indeed strongly involved both in binding and in switching the conformational changes of the nucleotide cavity on the STAS module upon light activation of the LOV domain. Only a few data are available to support a general NTP-binding role for the wide-spread STAS domains, but this functionality is likely to be relevant, as evidenced by the above discussed link with in vivo data.
ATP | adenosine triphosphate |
FMN | flavin mononucleotide |
GTP | guanosine triphosphate |
GTPTR | Guanosine 5′-triphosphate, BODIPY® TR 2′-(or-3′)-O-(N-(2-aminoethyl) urethane) |
LOV | Light, Oxygen and Voltage |
NTP | nucleotide triphosphate |
phot | phototropin |
STAS | domain found in Sulfate Transporters and Anti-Sigma factor antagonist |
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