Manoj
Mandal
*a,
Keisuke
Saito
bc and
Hiroshi
Ishikita
*bc
aDepartment of Chemical and Biological Sciences, S. N. Bose National Centre for Basic Sciences, Kolkata 700106, West Bengal, India. E-mail: mandalmanojcu@gmail.com
bResearch Center for Advanced Science and Technology, The University of Tokyo, 4-6-1 Komaba, Meguro-ku, Tokyo 153-8904, Japan. E-mail: hiro@appchem.t.u-tokyo.ac.jp
cDepartment of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8654, Japan
First published on 6th February 2023
Ca2+, which provides binding sites for ligand water molecules W3 and W4 in the Mn4CaO5 cluster, is a prerequisite for O2 evolution in photosystem II (PSII). We report structural changes in the H-bond network and the catalytic cluster itself upon the replacement of Ca2+ with other alkaline earth metals, using a quantum mechanical/molecular mechanical approach. The small radius of Mg2+ makes W3 donate an H-bond to D1-Glu189 in Mg2+-PSII. If an additional water molecule binds at the large surface of Ba2+, it donates H-bonds to D1-Glu189 and the ligand water molecule at the dangling Mn, altering the H-bond network. The potential energy profiles of the H-bond between D1-Tyr161 (TyrZ) and D1-His190 and the interconversion between the open- and closed-cubane S2 conformations remain substantially unaltered upon the replacement of Ca2+. Remarkably, the O5⋯Ca2+ distance is shortest among all O5⋯metal distances irrespective of the radius being larger than that of Mg2+. Furthermore, Ca2+ is the only alkaline earth metal that equalizes the O5⋯metal and O2⋯metal distances and facilitates the formation of the symmetric cubane structure.
The Mn4CaO5 cluster has four water molecules as ligands, W1 and W2 at the dangling Mn (Mn4) and W3 and W4 at Ca2+, which are also candidates for substrate water molecules (e.g.,11,12). Ca2+ has seven ligand groups (O1, O2, O5, D1-Asp170, D1-Ala344, W3, and W4).1 Ca2+ and Mg2+ are the most abundant alkaline earth metals in biological systems. In PSII, Ca2+ is a prerequisite for O2 evolution.13–19 Previously, it was speculated that Ca2+ was the origin of the distorted cubane structure (e.g.,20). However, the distortion of the Mn4CaO5 cluster remains even upon the removal of Ca2+.21–23 Indeed, not Ca2+ but dangling Mn4 is most responsible for the distortion of the cluster shape.23 The S2 to S3 transition is inhibited in Ca2+-depleted PSII.13,24–26 Ca2+ depletion not only causes the alteration of the H-bond network at the Mn4O5 and TyrZ moieties23 but also decreases the redox potential (Em) of TyrZ significantly due to reorientation of the water molecules in the H-bond network, making electron transfer from the Mn4CaO5 cluster to TyrZ uphill.27
Replacement of Ca2+ with any metals except Sr2+ inhibits O2 evolution,13–17 although the inhibition mechanism may depend on the metals. The geometry of the catalytic site in Sr2+-substituted PSII (Sr2+-PSII) resembles that of native PSII (Ca2+-PSII).28,29 The Em values for the artificial clusters with Sr2+ are also similar to those with Ca2+.30–32 The Em value for the Mn4BaO5 cluster in Ba2+-substituted PSII (Ba2+-PSII) is also considered to be similar to that for the Mn4CaO5 cluster in native PSII based on the observation of the normal thermoluminescence S2QA˙− band.33 Fourier transform infrared (FTIR) studies by Kimura et al. showed that the double difference S2/S1 spectrum was not affected significantly upon the substitution of Ca2+ with Mg2+ and Sr2+, whereas the vibrational modes of the carboxylate ligand residue disappeared upon substitution with Ba2+ in the PSII membrane from spinach.33 According to FTIR studies by Suzuki et al.,34 more than three carboxylate residues, except D1-Glu189 and the carboxyl terminus of the D1 protein, D1-Ala344, were perturbed upon Sr2+ substitution. FTIR studies by Strickler et al. also suggested that D1-Ala344 was not involved in the perturbation observed upon Sr2+ substitution.35
S2 can form in Mg2+-substituted PSII (Mg2+-PSII) but not in Ba2+-PSII.36 Vrettos et al. reported that Mg2+ and Ba2+ are unlikely to bind competitively with Ca2+.14 It was proposed that Ba2+ led to the deformation of the proton-conducting H-bond network.37,38 Although the radius of Ca2+ is one of the key factors,14,32 it remains unclear what property of Ca2+ is specifically required for O2-evolving activity among alkaline earth metals. Previous theoretical studies by Vogt et al. showed the detailed geometry of the Mn4SrO5 cluster in S1, S0, S–1, and S–2 in Sr2+-PSII.29 On the other hand, not only the geometry of the Mn4SrO5 cluster but also the energetics of the H-bond network in S2, in which the significance of Ca2+ is pronounced, remains unclear. FTIR studies suggested that the S2 to S3 transition involves the migration of the proton of a ligand water molecule toward D1-Asp61,39 which is in line with mutational studies (mutated to the other 19 residues).40 Theoretical studies also showed that a low-barrier H-bond forms between the ligand water molecule W1 and D1-Asp61 specifically in S2.41,42 The replacement of Ca2+ with the other redox-inactive divalent metals is unlikely to affect the H-bond between W1 and D1-Asp61, as the Ca2+ binding site is not directly involved in the W1⋯D1-Asp61 moiety. In contrast, the redox-active TyrZ⋯D1-His190 pair is directly involved in the H-bond network of the Ca2+ binding site.23 Because TyrZ forms a low-barrier H-bond with D1-His19043 and is directly involved in the H-bond network of the ligand water molecules (W3 and W4) at Ca2+,23,27 Ca2+-substitution may affect the low-barrier H-bond formation between TyrZ and D1-His190. However, to the best of our knowledge, the influence of Ca2+ on the TyrZ⋯D1-His190 H-bond has not been specifically reported.
To understand the specificity of Ca2+ in PSII, we investigated the local geometry of the metal-substituted Mn4MO5 cluster (M = Mg2+, Sr2+, and Ba2+) in S2 with Mn1(III)Mn2(IV)Mn3(IV)Mn4(IV) (open-cubane S2 conformation) by adopting a quantum mechanical/molecular mechanical (QM/MM) approach based on the native Ca2+-PSII crystal structure. As proton transfer occurs most effectively in the well-ordered H-bond network44,45 and the water molecules in the focusing H-bond network are less disordered in molecular dynamics simulations,46 comparisons of the H-bond networks among the metal-substituted PSIIs based on the QM/MM-optimized geometries are, therefore, the best starting point.
The Mn4CaO5 cluster was considered to be in the S2 states with antiferromagnetically coupled Mn ions; the resulting Mn oxidation states (Mn1, Mn2, Mn3, Mn4) and the total spin, S, were (III, IV, IV, IV) and S = 7/2 (↑↓↑↑) in S2, respectively. It should be noted that the difference in S (e.g., S = 1/2 in S2,60 high, low, ferromagnetic, and antiferromagnetic) did not affect the values; for example, (i) the resulting geometry61,62 and (ii) the potential-energy profile of proton transfer41 are not crucial to the spin configurations as far as the protein electrostatic environment is fully included.63
The initial-guess wavefunctions were obtained using ligand field theory64 implemented in the QSite program. For native PSII, the QM region was defined as the Mn4MO5 cluster (including the ligand side-chains of D1-Asp170, D1-Glu189, D1-His332, D1-Glu333, D1-Asp342, and CP43-Glu354; ligand carboxy-terminal group of D1-Ala344; and ligand water molecules, W1–W4), O4–water chain (W539, W538, and W393),45,65 Cl-1 binding site (Cl−, W442, W446, and the side-chains of D1-Asn181 and D2-Lys317), second-sphere ligands (side-chains of D1-Asp61 and CP43-Arg357), H-bond network of TyrZ (side-chains of D1-Tyr161, D1-His190, and D1-Asn298), including the diamond-shaped water cluster (W5, W6, and W7).43,66 The QM region defined in the present study is one of the largest among theoretical studies of PSII, which essentially covers the entire H-bond network of the ligand water molecules at the Ca2+ moiety (summarized in ref. 56).
To obtain the potential energy profiles of the O⋯H+⋯N bond for TyrZ⋯D1-His190, the QM/MM-optimized geometry was used as the initial geometry. The H atom under investigation was moved between the O and N moieties by 0.05 Å, after which the geometry was optimized by constraining the distance between O–H+ and H+–N, and the energy was calculated. This procedure was repeated until the H atom reached the O moieties. To obtain the potential energy profiles of the Mn1⋯O5 and O5⋯Mn4 bonds for the open- and closed-cubane S2 conformations, the QM/MM-optimized geometry of the open-cubane S2 conformation was used as the initial geometry. The O5 was moved toward the Mn4 moiety by 0.05 Å, after which the geometry was optimized by constraining the Mn1⋯O5 distance, and the energy was calculated.
Mg2+ | Ca2+ | Sr2+ | Ba2+ | Ba2+ + water | |
---|---|---|---|---|---|
a See ref. 67. b The surface area of Ca2+ is normalized to 1. | |||||
Ionic radiusa | 0.66 | 0.99 | 1.12 | 1.34 | 1.34 |
(Surface area ratiob) | (0.44) | (1) | (1.28) | (1.83) | (1.83) |
W3⋯M | 2.06 | 2.44 | 2.56 | 2.68 | 2.82 |
W4⋯M | 2.14 | 2.42 | 2.55 | 2.70 | 2.74 |
O1⋯M | 2.14 | 2.38 | 2.50 | 2.65 | 2.69 |
O2⋯M | 2.30 | 2.61 | 2.75 | 2.89 | 2.82 |
O5⋯M | 2.96 | 2.60 | 2.68 | 2.78 | 2.92 |
O5⋯Mn1 | 2.93 | 3.08 | 3.08 | 3.12 | 3.15 |
O5⋯Mn4 | 1.80 | 1.82 | 1.81 | 1.80 | 1.80 |
The small radius of Mg2+ shortens the Mg2+⋯W3 and Mg2+⋯W4 distances (to 2.06 and 2.14 Å, respectively) (Table 1). The small radius of Mg2+ also breaks the H-bond between W3⋯W7 (3.26 Å), which is energetically compensated for by the H-bond formation between W3 and D1-Glu189 (2.66 Å). Eventually, the alteration in the H-bond network occurs with respect to the Ca2+- and Sr2+-PSIIs (Fig. 1a), which may be associated with the inhibited O2-evolving activity in Mg2+-PSII. In contrast, the large radius of Ba2+ increases the Ba2+⋯W3 and Ba2+⋯W4 distances significantly (to 2.68–2.70 Å, Table 1). However, the H-bond pattern of the H-bond network essentially remains unchanged with respect to the Ca2+- and Sr2+-PSIIs (Fig. 1d). The surface area of Ba2+, which is 1.8 times larger than that of Ca2+, may allow the third water molecule (WBa) to bind at Ba2+ in addition to W3 and W4 (Table 1). To evaluate the existence of the extra water molecule, WBa is placed at the resulting cavity near Ba2+. QM/MM calculations show that WBa bridges the gap between D1-Glu189 and W2 via H-bonds (Fig. 1e). Thus, the alteration of the H-bond network is pronounced if the third water molecule is incorporated at the Ba2+ site. Note that no remarkable difference in the QM/MM-optimized geometry is observed when considering dispersion correction (Table S2, ESI†).
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Fig. 2 Potential-energy profile of the H-bond between TyrZ and D1-His190 in S2. (a) Mg2+-PSII. (b) Ca2+-PSII. (c) Sr2+-PSII. (d) Ba2+-PSII. |
The potential-energy profiles for the interconversion between the open- and closed-cubane S2 conformations, namely, the energy difference between the open- and closed-cubane S2 conformations, are similar in native Ca2+-PSII and metal-substituted PSIIs (Fig. 3), which suggests that the inhibition of the interconversion of the two S2 conformations is not responsible for the inhibition of O2 evolution upon replacement of Ca2+. Thus, the difference in the pKa value for ligand-water deprotonation between alkaline earth metals may still be one of the plausible hypotheses for the inhibition mechanism.14,76,77
The PSII crystal structure shows that Ca2+ has seven ligand groups (O1, O2, O5, D1-Asp170, D1-Ala344, W3, and W4).1 In particular, O1, O2, and O5 form the Ca2+ binding site of the Mn4CaO5 cluster. Most distances with M increase as the radius of the alkaline earth metal increases (Fig. 4a). However, the O5⋯M distance is exceptional. Intriguingly, the O5⋯M distance in Ca2+-PSII is the shortest among all metal-substituted PSIIs. Thus, Ca2+ is the alkaline earth metal that interacts most strongly with the Mn4O5 host region. The short O5⋯Ca2+ distance, even shorter than the O5⋯Mg2+ distance, suggests that Ca2+ may function most cooperatively with the Mn sites of the Mn4O5 cubane among all alkaline earth metals.
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Fig. 4 (a) Dependence of the distances with M on the radius in the open-cubane S2 conformation: O5⋯M (black solid line); W3⋯M (red dotted line); W4⋯M (blue dotted line); O1⋯M (green dotted line). (b) The open-cubane Mn4CaO5 structure and the [M (Ca2+)–O1–O3–Mn3] plane (sky blue square). See Table 1 for ionic radii. |
The O5⋯M and O2⋯M distances are identical (2.6 Å) only in Ca2+-PSII, which suggests that the shape of the open-cubane Mn3CaO4 region is most symmetric with respect to the [M (Ca2+)–O1–O3–Mn3] plane among all metal-substituted PSIIs (Fig. 4b). The result presented here indicates that the binding of Ca2+ is not the origin of the distorted cubane structure (e.g.,20), but it minimizes the distortion of the cluster with respect to other alkaline earth metals, leading to the symmetric shape of the open-cubane Mn3CaO4 region. The minimized distortion with Ca2+ may indicate that the Mn4CaO5 cluster is most stable among all alkaline earth metal clusters. Thus, Ca2+ may contribute to the remarkably large turnover number of 105 for the Mn4CaO5 cluster in native PSII.78
In summary, no significant difference is observed in the core structure or the characteristics of the H-bond between TyrZ and D1-His190 among the metal-substituted PSII (Fig. 2). This is consistent with the recent observations of synthetic Mn4Ca clusters, in which Ca2+ can be structurally and energetically replaced by other metal ions (e.g., Y and Gd).79
The characteristics of Sr2+-PSII are closest to those of Ca2+-PSII among Mg2+, Sr2+, and Ba2+-PSIIs (Fig. 3). The H-bond pattern of the H-bond network of only Sr2+-PSII is also consistent with that of Ca2+-PSII (Fig. 1). The calculated pKa value of a ligand water molecule at the Mn4MO5 cluster at the same level for Ca2+ and Sr2+ (∼13) in the absence of the PSII protein environment (i.e., gas phase).77 In contrast, the pKa value for the ligand water molecule differs by 2 units between Mg2+ and Ba2+,76 which largely originates from the difference in the radius. The difference in pKa alters the H-bond distances with the ligand water molecules, whereas the difference in the radius alters the distance between the metal center and the ligand water molecule. These differences are ultimately pronounced in the difference in the H-bond pattern of W3 in Mg2+-PSII. In Mg2+-PSII, W3 donates an H-bond to D1-Glu189, but the H-bond between W3 and W7 disappears, altering the H-bond network with respect to Ca2+- and Sr2+-PSIIs (Fig. 1a). In contrast, an increase in the radius compared to that of Ba2+ does not induce an alteration in the H-bond pattern of the H-bond network (Fig. 1d). Indeed, the difference in the pKa value for the ligand water molecule among Ca2+ (12.8), Sr2+ (13.2), and Ba2+ (13.4) is very small,76 which cannot explain the inactivity of Ba2+-PSII. Only if a water molecule additionally binds at Ba2+ as the third ligand water molecule does it donate H-bonds to D1-Glu189 and W2, altering the H-bond network (Fig. 1e). According to recent X-ray free electron laser (XFEL) structures, a water molecule (O6) was inserted between W2 and D1-Glu189 during the S2 to S3 transition.72,73 However, in Mg2+-PSII, W3 is closer to O5 and already donates an H-bond to D1-Glu189, which may inhibit O6 insertion (i.e., the S2 to S3 transition). In Ba2+-PSII, the binding site of the third ligand water molecule overlaps with the O6 binding site in the XFEL Ca2+-PSII structure. Thus, Ba2+ with a third ligand water molecule may restrict the insertion of an extra water molecule (e.g.,71,72) in the S2 to S3 transition. The low-barrier H-bond between TyrZ and D1-His190 remains unaffected even in the Mg2+- and Ba2+-PSIIs irrespective of the Ca2+/metal binding site being relatively close to TyrZ (Fig. 2). Although Mg2+ and Ba2+ may not bind competitively with Ca2+,14 the observed alteration in the “external” environment of the catalytic center (e.g., ligand structure and H-bond network) may be associated with the inhibition mechanism for O2 evolution if the metal-substituted PSIIs are properly assembled.
More importantly, Ca2+ exclusively minimizes the “internal” structure of the catalytic center. Ca2+ is the unique alkaline earth metal that (i) has the shortest O5⋯M distance (irrespective of the radius being larger than Mg2+) and interacts most strongly with the Mn4O5 host region and (ii) equalizes the O5⋯M and O2⋯M distances (2.6 Å) and facilitates the formation of the symmetric cubane structure (Fig. 4a). The resulting distortion-free Mn4CaO5 cluster is energetically advantageous with respect to the other metal-substituted clusters, which may contribute to the remarkably large turnover number of 105 in native PSII.78 This may be one of the reasons why Ca2+ is the preferred redox-inactive site in nature as the catalytic O2-evolving center.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2cp05036f |
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