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1 Department of Chemical Sciences, Tata Institute of Fundamental Research, Mumbai-400005 India
2 Centro Risonanze Magnetiche, University of Florence, Florence, Italy
Reprint requests to: K.V.R. Chary, Department of Chemical Sciences, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai-400005, India; e-mail: chary{at}tifr.res.in; fax: 0091 (22) 2152110.
(RECEIVED July 26, 2002; FINAL REVISION November 14, 2002; ACCEPTED November 18, 2002)
Article and publication are at http://www.proteinscience.org/cgi/doi/10.1110/ps.0225603.
| Abstract |
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Keywords: EF-hand protein; calmodulin; EhCaBP; pseudocontact shifts; chemical shifts; ytterbium
Abbreviations: NMR, nuclear magnetic resonance ITC, isothernmal calorimetry HSQC, heteronuclear single quantum coherence EhCaBP, Entamoeba histolytica calcium binding protein CaM, calmodulin TnC, Troponin C
| Introduction |
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Out of these, residues at 1, 3, 5, and 12 position coordinate directly to Ca2+ via their side-chain carboxylate groups, with position 1 and 12 being an invariant Asp and Glu, respectively (Strynadka and James 1989; Falke et al. 1994). Residue at position 7 coordinate to Ca2+ via its backbone carbonyl group, whereas residue at position 9 coordinates to Ca2+ indirectly through an intervening water molecule (Strynadka and James 1989).
In recent years, there has been a growing interest with regard to the factors that govern Ca2+-binding affinities in EF-hand proteins (Linse and Forsén 1995). This is primarily due to the fact that a wide range of Ca2+ binding affinities/specificities has been found among these proteins despite the strong conservation in their primary sequence of Ca2+-binding loops (Linse and Forsén 1995). Several studies (Moeschler et al. 1980; Imaizumi et al. 1990; Linse and Forsén 1995; Gopal et al. 1997; Gilli et al. 1998) have concentrated on understanding Ca2+ binding affinity/specificity in these proteins against Mg2+, which is the only other competitor for Ca2+ inside the living cell. Models based on the primary sequence of the Ca2+-binding loop have been proposed to explain the origin of differences in Ca2+ binding affinities/specificities (Mardsen et al. 1988; Waltersson et al. 1993; Wu and Reid 1997). For example, in one of the studies, the presence of neighboring Asp residues at either the +X and +Y, the +Y and +Z, or the +X, +Y and +Z metal ion coordinating positions have been shown to lower metal binding affinity due to dentatedentate repulsion (Mardsen et al. 1988). In another study, the side chain of the ligating residue at position +Y in the Ca2+-binding loop has been shown to be important (Waltersson et al. 1993). In yet another study, EF-helices that flank the Ca2+-binding loops have also been proposed to modulate the Ca2+-binding affinity in this class of proteins (Sharma et al. 1997).
In the majority of these studies, the target protein/peptide has been taken in the Ca2+-free (apo) form. Very few studies have focussed on the displacement of Ca2+ in a Ca2+-saturated (holo) protein by other metal ions. Such studies yield information on the relative specificity and strength with which Ca2+ is bound to the protein. Tri-positive lanthanide ions (Ln3+) serve as ideal candidates for the displacement of Ca2+ in a protein owing to their similar ionic radii as Ca2+ (Shannon 1976). Such a study yields valuable information on the relative binding affinities of Ca2+ and Ln3+ with the protein under investigation. Lanthanides such as Tb3+ and Eu3+ possess optical properties and facilitate structural studies in substituted proteins using fluorescence and UV-Vis absorption spectroscopy (Horrocks and Sudnick 1981; Wu et al. 1996). Another favorable property of paramagnetic Ln3+ is their large anisotropic magnetic susceptibility, which has been harnessed in NMR studies of Ln3+-substituted proteins (Bertini et al. 2001a). The large pseudocontact shifts, observed for residues as far as 40 Å from the metal center, have been used for 3D structure refinement from NMR data (Allegrozzi et al. 2000). On the other hand, residual dipolar couplings that arise due to the partial alignment of proteins containing Ln3+ in high magnetic field have been used as further refinement tool (Bertini et al. 2001b) and to assess domain alignment in multidomain EF-hand proteins such as calmodulin, or CaM (Biekotsky et al. 1999). However, there have been very few studies that have aimed at understanding the binding affinity/ specificity of Ln3+ to these proteins. To characterize the factors that govern binding of Ln3+ to EF-hand proteins and harness their favorable magnetic properties for structural studies by NMR, we have initiated Ln3+-substitution studies in an EF-hand Ca2+-binding protein from Entamoeba histolytica (hereafter referred to as EhCaBP). A high-resolution 3D structure of this protein in solution has been recently deposited in the Protein Data Bank (Atreya et al. 2001).
EhCaBP is a 15-kD (134 amino acid residues) monomeric protein containing four canonical EF-hand Ca2+binding loops. The overall structural topology of EhCaBP resembles that of CaM and Troponin C (TnC) with two globular domains (the N- and C-terminal) connected by a flexible eight amino acid linker (Sahu et al. 1999a; Atreya et al. 2001). In this article, we present the NMR and thermodynamics study of Ca2+ displacement by Yb3+ in EhCaBP. Yb3+ has been chosen as the paramagnetic probe owing to its large pseudocontact shift to Curie linebroadening ratio (Bertini et al. 2001d). We have used isothermal titration calorimetry (ITC) to obtain binding affinities and free energy changes upon substitution of Ca2+ by Yb3+. To the best of our knowledge, this is the first study involving a combined use of NMR and thermodynamics to characterize lanthanide binding in EF-hand proteins.
| Results |
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1025 Å of Yb3+, while it is expected to completely broaden out if it is located within10 Å of Yb3+ (Allegrozzi et al. 2000).
The amide (1HN) protons of Gly residues present at the sixth position of the four internally highly homologous Ca2+ binding polypeptide stretches in EhCaBP (Scheme 1
), exhibit a characteristic downfield shift in the Ca2+-bound state (holo) of the protein (Akerfeldt et al. 1996). This is the result of their involvement in hydrogen bonding with the side-chain carboxyl oxygen atom (C'O) of an invariant Asp at the first position of respective Ca2+ binding loops (shown as bold letters in Scheme 1
with numbering shown on top).
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1 = 108.00115.00 ppm and
2 = 9.5011.00 ppm), and hence, formed the best markers for each Ca2+-binding site during the course of titration. For the convenience of discussion, the four Ca2+-binding sites present in EhCaBP are identified as follows: (a) Site I (residues 132), (b) Site II (residues 3362), (c) Site III (residues 71103), and (d) Site IV (residues 104134).
Up to a Yb3+:EhCaBP ratio of 1.0
During the initial stages of titration, [Yb3+]/[EhCaBP] ratio of (hereafter referred to as the metal:protein ratio) of 0.01.0, the most important observation is the gradual disappearance of cross peaks belonging to Sites III and IV of EhCaBP and the gradual appearance of new pseudocontact shifted cross peaks, whereas cross peaks arising from residues at Sites I and II, are almost unaffected. As an illustrative example of this observation, Figures 1A and 1B, and 2![]()
show selected regions of the 2D [15N-1H] HSQC spectrum. Assignment of pseudocontact shifted peaks for residues in Site IV was obtained based on the combined use of the 2D [15N-1H] HSQC spectra recorded on both [u-15N] and [AKL]-15N EhCaBP samples as shown in Figure 3
. As evident from Figure 3A
, selective labeling of Ala, Leu, and Lys resulted in a dramatic simplification of the spectrum, which aided in unambiguous resonance assignments of the pseudocontact shifted peaks of residues belonging to Site IV. As an illustrative example, Figure 3B
shows the assignment of pseudocontact shifted cross peaks of I107 and L126. No pseudocontact shifted peaks were observed for any of the residues belonging to Site III. To have an insight of these observations more vividly, Figure 4
shows the normalized volumes of cross peaks plotted for a few amino acid residues (both original and pseudocontact shifted peaks) in all the four metal binding sites of EhCaBP. These plots indicate the percentage of various species present up to a metal:protein ratio of 1.0. These observations taken together reveal that Yb3+ ions bind first to the C-terminal domain and particularly to the Site III of EhCaBP, resulting in complete broadening of cross peaks for residues belonging to this site. Simultaneously, pseudocontact shifts are observed for residues in Site IV, which lie within 1025 Å of Site III. Thus, as the titration approaches a metal:protein ratio of 1.0, the third binding site is almost completely filled by the Yb3+ ions and a majority of (Ca2+)4-EhCaBP transforms into (Ca2+)(I)-(Ca2+)(II)-(Yb3+)(III)-(Ca2+)(IV)-EhCaBP.
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1 = 114.6 ppm,
2 = 8.90 ppm, which has been assigned as the pseudocontact shifted peak of G15. This observation is substantiated further from the observation of pseudocontact shifted cross peaks of several other residues belonging to the Site I. For example, see plots of cross peak volumes for residues G13 and G51 in Figure 5
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30%; Fig. 6
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30%, as the titration proceeds up to a metal:protein ratio of 4.0 (Fig. 6
ITC measurements
A typical calorimetric reaction of the addition of aliquots of Yb3+ ligand to EhCaBP is shown in Figure 7A
along with its
Q versus the metal:protein ratio in Figure 7B
. Analysis of the data using the ligand-binding model by Wisemen et al. (1989), carried out using ORIGIN software, was made assuming the presence of four binding sites for Yb3+ in the protein. The fitting reveals three sites of endothermic in nature, while one site exhibits an exothermic behavior for the Ca2+ displacement by Yb3+. By varying the initialization parameters used to begin the fitting procedure, it was determined that the fit was stable and no other parameter set could be found that provided a good fit to the data. Binding constants along with enthalpy, entropy, and free energy of binding are given in Table 1
. The endothermic nature of Ca2+ displacement by Yb3+ is obvious considering the fact that the hydration enthalpy of Yb3+ is higher than Ca2+ (Marcus 1985). This implies that energy released on Ca2+ hydration is not sufficient to break the Yb3+ hydration shell to bind to the protein, resulting in heat being absorbed from the solution. The binding constants represent the following displacement reaction:
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| Discussion |
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As evident from Scheme 1
, the third Ca2+-binding loop (Site III) in EhCaBP possesses four charged residues (D85, D87, D89, and E96) that coordinate to Ca2+ as opposed to only three in the other three loops (I, II, and IV). Hence, Site III is expected to be the most preferred site for tripositive Yb3+, in EhCaBP (Biekofsky et al. 1999). Also, out of the four Ca2+-binding loops present in EhCaBP, the third loop structurally diverges the most from the corresponding loops of its homologous proteins, CaM and TnC (Atreya et al. 2001; Fig. 8
). Such a divergence of the third Ca2+-binding loop of EhCaBP could be attributed to the presence of a Tyr residue at position -4 with respect to the third loop, instead of a highly conserved Phe (Atreya et al. 2001). Previously, it has been shown that, in a given domain containing a pair of EF-hands, Phe at -4 position with respect to the first EF-hand loop (F[-4]) interacts with yet another conserved Phe at the 13th position of the second EF-hand loop (F[13]), such that their respective aromatic rings are oriented perpendicular to each other (Rashidi et al. 1999; Fig. 9
). Such an orientation results in their C
-C
distance of 78 Å (Rashidi et al. 1999). Further, proteins that lack such Phe-Phe interactions due to the absence of F(-4) or/and F(13), are found to have lower affinity for Ca2+ (Chandra et al. 1994; Ohya and Botstein 1994). In both CaM and TnC and in the N-terminal domain of EhCaBP, the respective Phe aromatic rings are oriented perpendicular to each other, with their C
-C
distances in the range of 78 Å (Fig. 9
). However, in the C-terminal domain of EhCaBP, the aromatic ring of Tyr 81 faces that of Phe 129 almost in a parallel orientation, resulting in their C
-C
distance of 10.3 Å (Atreya et al. 2001). This causes the divergence of the third loop of EhCaBP compared to the corresponding loops of CaM and TnC (Fig. 8
). Thus, the preference for Yb3+ to Site III can be attributed to both its higher negative charge compared to the other Ca2+-binding loops in the protein and to the presence of a Tyr at -4 position in the loop. Such a hypothesis is consistent with the NMR data, which show a rapid decrease in intensity of G90 amide cross peak during the initial stages of titration when the metal:protein ratio is increased from 0 to 1. Simultaneously, the pseudocontact shifted peak of G122 (
1HN = 9.3 ppm) increases in its integral volume and reaches maximum at a little over metal:protein ratio of 1 (Figs. 1, 4, 6![]()
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). We can therefore conclude that Yb3+ first displaces Ca2+ from the Ca2+-binding Site III in EhCaBP, which results in a pseudocontact shift of residues belonging to Site IV.
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Further, the rate at which the pseudocontact shifted peaks of residues belonging to Site I increase in their integral volumes is relatively lower compared to the rate of decrease of the corresponding original peaks. This implies the coexistence of species (Yb3+)(I)-(Yb3+)(II)-(Yb3+) (III)-(Ca2+)(IV)-EhCaBP (species A) and species (Ca2+) (I)-(Yb3+)(II)-(Yb3+)(III)-(Ca2+)(IV)-EhCaBP (species B). Their relative populations can be determined from the knowledge of the ratio of integral volumes of cross peaks arising from the respective species.
Beyond a metal:protein ratio of 2.0, both the original and pseudocontact shifted cross peaks for residues in Site I show a decline in their integral volumes (Figs. 1, 5A![]()
). This implies the filling of Yb3+ in Site I only in the species wherein Site II is already filled with Yb3+. As observed, a net decrease in the pseudocontact shifted cross peak volumes implies that population of species B is relatively more compared to species A. Another important point to note is that, the reaction path that proceeds via the filling of Site I is completely ruled out in the present case, as we did not observe any pseudocontact shifted peaks for residues in Site II.
As far as the cooperativety is concerned, it is very well known that it exists between any two metal binding sites of adjacent EF-hands. Such cooperative binding of ions is the most important functional property of the calcium signaling pathways. So, it is not surprising that we also notice positive cooperativity during the process of our lanthanide titration discussed here. The most pertinent explanation for such cooperativity is that the binding of one metal facilitates the binding of the other metal ion, because the apo becomes half-holo, and causes the other site to loose its flexibility and become more structured. Such sitesite communication in the EF-hand calcium binding proteins has been reported earlier (Maler et al. 2000). However, in the present case it does not go from apo to half-holo to holo. Instead, it is a displacement of Ca2+ ions by Yb3+. To start with, both sites are already well structured and remain so even after the metal displacement. This observation, however, raises questions such as what is the origin of the positive cooperativity seen in the present case? And why should the second Yb3+ care to go to a site only when another Yb3+, and not a Ca2+, is in its neighboring site of a given pair of EF-hands? The answers to these questions lie in the difference in charges present in individual sites. When both sites are negatively charged there is an intrinsic repulsion between them, which is decreased when a metal ion binds to one of the sites, resulting in the formation of a short stretch of ß-sheet, which in turn, facilitates the entry of the second metal ion. If a domain with a pair of EF-hands is already occupied by two Ca2+ ions, as is the case now, there could still be a slight excess of negative charge. Substitution of one of them with a tripositive lanthanide ion could decrease even more, or perhaps abolish, the residual electrostatic repulsion between the two loops, facilitating the entry of the second tripositive lanthanide ion. This argument is in line with the works reported earlier on the N-terminal domain of calbindin (Maler et al. 2000; Bertini et al. 2001c), where strong cooperativity was observed. When cerium ions occupy both the sites of the domain, the intermetal distance is reported to be sizably shorter than that observed between the two Ca2+ ions in the native protein.
As mentioned earlier, EF-hand proteins maintain specificity for Ca2+ against its strong competitor Mg2+ inside the cell. Hence, it could also be the same case with tripositive lanthanide ions against Mg2+.
Coming to the ITC data, it yields four macroscopic binding constants, K1, K2, K3, and K4, as shown in Table 1
, which can be now assigned to the Ca2+ displacement by Yb3+ from the respective Ca2+-binding sites in EhCaBP.
Up to a metal:protein ratio of 1.0, Site III is predominantly filled with Yb3+, leaving Sites I, II, and IV with Ca2+. Thereafter, Sites I and II are filled completely at a metal: protein ratio slightly above 3.0. Further, it is interesting to note that, Site IV is left with 30% Ca2+ even when we go beyond a metal:protein ratio of 4.0. This implies that binding constants for Yb3+ in Sites III and IV of EhCaBP differ by a large factor, resulting in the sequential displacement of Ca2+ in the C-terminal domain. In the light of such observations, we can ascribe the highest binding constant (K1) obtained in ITC to the Ca2+ displacement by Yb3+ in Site III (kIII), while the lowest (K4) to the similar process in Site IV. It is important to note that K4 is the binding constant of Yb3+ for Site IV when Yb3+ is already bound to Site III (kIV,III). The assignment K4 to Site IV is in line with the thermodynamics study of Ca2+-binding in EhCaBP carried out earlier, which showed that Site IV has the highest affinity for Ca2+ in EhCaBP (Gopal et al. 1997). In the present study, the remaining two macroscopic binding constants, K2 and K3 obtained using ITC (Table 1
) can be assigned to the Ca2+ displacement by Yb3+ in Sites I and II in the N-terminal domain. As discussed above, during the course of titration wherein the metal:protein ratio is changed from 1 to 3, NMR studies indicate that Yb3+ preferentially displaces Ca2+ in Site II. Further, at a metal:protein ratio of 2.0, the population of species B is about 45% and that of species A is about 25% of the total species present. The presence of species B in excess to that of species A implies that kI,II > kII. Thus, out of K2 and K3, the smaller one (K3) can be assigned to the Ca2+ displacement by Yb3+ in Site II (kII); K2 then represents the equilibrium constant of Ca2+ displacement by Yb3+ in Site I, when Yb2+ is already bound in its neighboring Site II (kI,II).
To verify whether the above assignments of thermodynamic constants to the various reactions are correct, plots of normalized volumes of cross peaks (Figs. 2, 5, 6![]()
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) were back calculated using the equilibrium constants obtained from ITC (Table 1
, last column). The reactions considered in the simulations are given in the Electronic Supplemental Material.
The experimental and simulated plots of intensity profiles are shown in Figure 10
for the original and pseudocontact shifted cross peaks of G15 and G122. As evident from the figure, simulated plots (Fig. 10B
) obtained using the thermodynamic constants given in Table 1
(last column) are almost identical to the intensity profiles obtained for various species based on NMR titration data (Fig. 10A
). The values of the thermodynamic constants used in the simulation are same as the experimentally observed ones, except for K1, which is found to be three times higher). To verify the assignments of K2 and K3, simulated plots of intensity profiles were generated by interchanging the values of K2 and K3. This is shown in Figure 10C
. A lower value for K2 compared to K3 results in 40% population of the pseudocontact shifted cross peak of G15 at a metal:protein ratio 2. However, NMR data indicates about 25% population of this species at this metal:protein ratio (Fig. 5
). Thus, a higher value of K2 compared to K3 (as given in Table 1
) more appropriately describes the system.
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Finally, studies such as this will help in unraveling the number of Ca2+-binding sites in a protein. It assumes importance for EF-hand proteins such as neuronal Ca2+ sensor 1 (NCS-1), wherein an exact number of Ca2+-binding sites in the protein have not yet been resolved unambiguously (Cox et al. 1994; Ames et al. 2000). Moreover, in multidomain proteins, if we can observe pseudocontact shifts in one domain due to the filling of Ln3+ in the other, then such shifts help in fixing the interdomain orientations. Efforts are on in this direction to define the relative orientation of the two domains in EhCaBP.
| Materials and methods |
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12.5 mg of protein in 0.6 mL) by measuring the absorbance at 280 nm (
280 = 5120 M-1 cm-1) on a Varian Inc. Cary 50 scan spectrophotometer. NMR experiments were performed at 35°C on 0.6 mL of
1 mM protein samples (pH 6.0), in a mixed solvent of 90% H2O and 10% 2H2O.
Yb3+ titration of [u-15N] and [ALK]-15N-labeled (Ca2+)4-EhCaBP
NMR experiments on EhCaBP were carried out in the form of a titration. The displacement of Ca2+ in the protein by Yb3+ was achieved by adding small aliquots from a 20 mM stock solution of YbCl3 to the protein solution. To start with, an aliquot of YbCl3 from a 0.02 M stock solution corresponding to a metal:protein ratio of 0.1 was taken each time and added directly to the protein solution in the NMR sample tube. The sample was mixed thoroughly before transferring it to the 600/700 MHz magnet. As the metal: protein ratio reached 0.5, large changes were observed in the HSQC spectrum and, hence, further titration was carried out in smaller steps of 0.05 metal:protein ratios. From a metal:protein ratio of 2.0 to 4.6, titrations were carried out in larger step sizes (at a variable metal:protein ratio of 0.1, 0.2, and 0.4). This resulted in a total number of 47 titration points. The change in pH on addition of the lanthanide salt was found to be negligible.
NMR experiments
NMR experiments were recorded either on a Bruker Avance 700 MHz NMR spectrometer (CERM) or Varian Unity+ 600 MHZ NMR spectrometer (NFMR), both equipped with pulsed field gradient units and triple resonance probes with actively shielded Z-gradients. Sensitivity enhanced 2D [15N-1H] HSQC spectrum using pulsed field gradients for coherence selection (Kay et al. 1992) was acquired during each step of the titration. During the entire course of titration, the sample was found to be stable and soluble. 1H chemical shift calibrations were carried out with respect to the methyl signal (at 0.0 ppm) of 3-(trimethylsilyl)[3,3,2,2-2H] propionated4 (TSP), which has been used as an external reference. 15N chemical shifts were referenced with respect to an external standard of 15N-labeled ammonium chloride (2.9 M in 1 M HCl). The 1H and 15N chemical shifts published earlier (Sahu et al. 1999a, 1999b) were used to identify individual cross peaks in the 2D [15N-1H] HSQC spectrum of EhCaBP.
ITC measurements and analyses
ITC measurements were performed with a Microcal Omega titration calorimeter. Samples were centrifuged and degassed prior to the titration and examined for precipitation, if any, after the titration. A typical titration consisted of injecting 1.2 µL aliquots of 20 mM YbCl3 solution into 0.24 mM (1 mL) of the protein solution after every 3.5 min to ensure that the titration peak returned to the baseline prior to the next injection. A total of 31 injections were carried out. No precipitation was observed during the titration. Aliquots of more concentrated ligand solution were injected into the buffer solution (without the protein) in a separate ITC run, to subtract the heat of dilution. All experiments were repeated at least twice with different protein and ligand concentrations to establish reproducibility of the data. The ITC data were analyzed using the software ORIGIN (supplied with Omega Microcalorimeter). The amount of heat released per addition of the titrant was fitted to two/four or sequential/independent binding sites on the protein as given by Wisemen et al. (1989).
Considering a two-metal binding site system depicted in Scheme 3
(e.g., N- or C-terminal domain of EhCaBP), a situation can arise in which the values of the microscopic binding constants kI and kII for the two sites under consideration are widely different (one of them might be 1001000-fold larger than the other). In such a situation, the protein will exhibit a step-wise or sequential binding/displacement of Ca2+.
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ITC experiments yield only the values of the macroscopic binding constant K1 and K2. However, if kII >> kI, the reaction path shown as dashed lines in Scheme 3
is completely ruled out and the macroscopic binding constants K1 and K2 essentially coincide with the microscopic binding constants kII and kI,II. Further, the values of kII and kI,II are reflected in the relative populations of species A and B shown in Scheme 3
. If kII is much larger than kI,II (say 100-fold), then the population of species A will be largely predominant until all of the Site II is filled with the metal. On the other hand, if kII and kI,II are comparable, both species A and B coexist and their relative population can then be determined by the ratio: kII/kI,II.
| Electronic supplemental material |
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| Acknowledgments |
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The publication costs of this article were defrayed in part by payment of page charges. This article must therefore be hereby marked "advertisement" in accordance with 18 USC section 1734 solely to indicate this fact.
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