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1 Department of Biochemistry and Molecular Biology, University of Parma, 43100 Parma, Italy
2 Department of Physics, University of Parma, 43100 Parma, Italy
3 Italian National Institute for the Physics of Matter, University of Parma, 43100 Parma, Italy
Reprint requests to: Andrea Mozzarelli, Department of Biochemistry and Molecular Biology, University of Parma, 43100 Parma, Italy; e-mail: biochim{at}unipr.it; fax: 39-0521-905151.
(RECEIVED May 31, 2001; FINAL REVISION August 7, 2001; ACCEPTED August 20, 2001)
Article and publication are at http://www.proteinscience.org/cgi/doi/10.1101/ps.20501.
| Abstract |
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- and ß-hemes. Significantly, hemoglobin encapsulated in the presence of the weak effector phosphate led to gels that show intermediate oxygen affinity and Hill coefficients of 0.7 to 0.8. The heterogeneous oxygen binding results from the presence of a mixture of the high and low oxygen-affinity T states. The Bohr effect was measured for hemoglobin gels containing the pure conformations and found to be more pronounced for the high-affinity T state and almost absent for the low-affinity T state. These findings indicate that the functional properties of the T quaternary state result from the contribution of two distinct, interconverting conformations, characterized by a 10-fold difference in oxygen affinity and a different extent of tertiary Bohr effect. The very small degree of T-state cooperativity observed in solution and in the crystalline state might arise from a ligand-induced perturbation of the distribution between the high- and low-affinity T-state conformations. | Introduction |
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2ß2-tetramer that binds ligands cooperatively via the modulation of equilibria between tertiary and quaternary conformations. X-ray crystallographic studies have shown that hemoglobin exists in two quaternary states, T and R, characterized by the presence and absence of salt bridges, respectively, and by a different pattern of
1ß2- and
2ß1-interactions (Perutz 1970; Baldwin and Chothia 1979). Binding of ligands triggers a series of tertiary conformational changes that break salt bridges, destabilizing the T state and leading to the liganded R state (Perutz 1970; Antonini and Brunori 1971; Perutz et al. 1998). Oxygen binding curves have been extremely useful in evaluating the effect of allosteric effectors on the functional properties of quaternary states (Imai 1982). In particular, the oxygen affinity and the degree of cooperativity of T-state hemoglobin have been investigated on mixed metal hybrids, for which iron at either the
- or ß-heme was substituted with metals that do not bind oxygen (Shibayama et al. 1986; Miyazaki et al. 1999), and on T-state hemoglobin crystals grown from polyethylene glycol solutions (Mozzarelli et al. 1991, 1997; Rivetti et al. 1993a, b; Bettati et al. 1997, 1998; Bruno et al. 2000). These new experiments were required to discriminate among the models proposed to explain cooperative ligand binding and functional modulation brought about by allosteric effectors. A critical difference among models concerns the predicted cooperative properties of the T state. The Monod, Wyman, and Changuex (MWC) model predicts noncooperative ligand binding (Monod et al. 1965), whereas the Koshland, Nemethy and Filmer model (Koshland et al. 1966), the "Monland" model of Perutz (1998), and the Symmetry Rule of Ackers (Ackers et al. 1992, 2000) predict cooperative ligand binding. A particularly powerful approach to dissect tertiary and quaternary contributions to cooperativity is the encapsulation of hemoglobin in silica gels, which stabilizes the protein either in the T or in the R state (Shibayama and Saigo 1995Shibayama and Saigo 1999Shibayama and Saigo 2001; Bettati and Mozzarelli 1997; Das et al. 1999; Juszczak and Friedman 1999; Shibayama 1999; Khan et al. 2000). The quaternary transition is not prevented but is dramatically slowed down with respect to solution, the rate of the process being strongly dependent on temperature (Das et al. 1999; Shibayama and Saigo 1999). This behavior allows the detection of tertiary conformational properties de-coupled from the quaternary transition. Even the rates of tertiary transitions of hemoglobin in silica gels are decreased by several orders of magnitude (Juszczak and Friedman 1999; Shibayama 1999; Shibayama and Saigo 2001). Despite these restraints on dynamic properties, spectroscopic markers (Das et al. 1999; Juszczak and Friedman 1999; Khan et al. 2000), oxygen affinity (Shibayama and Saigo 1995Shibayama and Saigo 2001; Bettati and Mozzarelli 1997), and the Bohr effect (Bettati and Mozzarelli 1997) were found to be similar to those observed in solution, indicating that hemoglobin encapsulated in silica gels retains its functional and structural properties. One intriguing result was that the oxygen binding curves of hemoglobin gels showed Hill coefficients significantly lower than unity (Shibayama and Saigo 1995Shibayama and Saigo 2001; Bettati and Mozzarelli 1997), indicating conformational heterogeneity, possibly originated by the presence of noninterconverting states with different oxygen affinities (Bettati and Mozzarelli 1997). This heterogeneity was also present in the T-state hemoglobin gels recently investigated (Shibayama and Saigo 2001), the Hill coefficient varying between 0.5 and 0.7. Based on the extrapolation of the oxygen binding curves at very high and very low oxygen saturations, Shibayama and Saigo (2001) proposed the presence of a high oxygen-affinity state with p50 of 1 to 2 torr and a low oxygen-affinity state with p50 of 64 to 100 torr. These values are five- and twofold lower than those observed in solution for the binding of the first oxygen to T-state hemoglobin in the absence and presence of allosteric effectors, respectively (Poyart et al. 1978; Imai 1982).
In the present work, we have addressed the question whether the functional properties of the T-state hemoglobin in solution are generated by a continuous population of tertiary conformational states or by a distribution of two or more discrete interconverting states, modulated by allosteric effectors and characterized by distinct ligand affinities, as originally proposed by Rivetti et al. (1993a) and Bettati and Mozzarelli (1997). Deoxy-hemoglobin was encapsulated in silica gels in the absence and presence of different allosteric effectors with the aim to isolate distinct tertiary T-state conformations and to accurately characterize oxygen binding and allosteric modulation. Results add further information to the ongoing investigation on the distribution of tertiary and quaternary conformations as a function of ligand saturation and on the degree of cooperativity within the T-state hemoglobin (Perutz et al. 1998; Eaton et al. 1999; Perrella 1999; Ackers et al. 2000; Russo et al. 2001).
| Results |
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- and ß-hemes (Lindstrom and Ho 1972; Shibayama et al. 1986; Bettati et al. 1996; Mozzarelli et al. 1997; Bruno et al. 2000). In fact, a two- and fourfold higher affinity of
-hemes with respect to ß-hemes would result in a Hill coefficient of 0.97 and 0.91, respectively. The calculated p50s, that is, the value of oxygen pressure at half saturation, are 12.4 ± 0.2 and 139 ± 4 torr, for hemoglobin gels obtained in the absence and presence of allosteric effectors, respectively. These values are compared in Table 1
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- to ß-heme inequivalence. The observed binding curves were fitted assuming the presence of a mixture of two noninteracting and noninterconverting sites. The analysis indicates that the binding curves result from an almost equal contribution from two sites characterized by
10-fold difference in oxygen affinity (Fig. 3a
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| Discussion |
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Encapsulation of hemoglobin in wet, porous silica gels has been used as an alternative method for trapping quaternary states (Shibayama and Saigo 1995Shibayama and Saigo 2001; Bettati and Mozzarelli 1997; Das et al. 1999; Juszczak and Friedman 1999; Khan et al. 2000). Oxygen binding curves to both the R and T states of hemoglobin were measured (Shibayama and Saigo 1995Shibayama and Saigo 2001; Bettati and Mozzarelli 1997). In contrast to hemoglobin in the crystal, the oxygen affinity of T-state hemoglobin in silica gels is modulated by IHP, bezafibrate, chloride, and pH (Bettati and Mozzarelli 1997), as in solution (Poyart et al. 1978; Imai 1982; Lee et al. 1988; Marden et al. 1990), indicating that the protein molecule in the gel retains a significant degree of flexibility. However, oxygen binding curves were characterized by a Hill coefficient significantly lower than unity (Shibayama and Saigo 1995Shibayama and Saigo 2001; Bettati and Mozzarelli 1997), consistent with the presence of a distribution of noninterconverting tertiary conformations (Bettati and Mozzarelli 1997). A recent study has supported this hypothesis, showing that high and low oxygen-affinity tertiary states are simultaneously pres-ent when T-state hemoglobin is encapsulated in silica gels (Shibayama and Saigo 2001). The oxygen binding curves showed a Hill coefficient of 0.5 to 0.7 and asymptotically extrapolated to two discrete components characterized by a Hill coefficient of one and a p50 of 1.1 to 2.2 and 64 to 101 torr at 20°C. The values of oxygen affinity for both the high- and low-affinity states are lower than the values of K1 reported for hemoglobin in solution under similar experimental conditions (Poyart et al. 1978; Imai 1982; Marden et al. 1990) and might result from the formation of a mixture of T and R states during the titration, as indicated by the nonperfect reversibility of the reported binding curves (Shibayama and Saigo 2001). To achieve a detailed functional characterization of the high and low oxygen-affinity T-state conformations, we have designed experimental conditions of hemoglobin encapsulation to isolate the distinct tertiary conformations of hemoglobin. The results indicate that hemoglobin silica gels fully populated with either high or low oxygen-affinity tertiary conformations have been obtained. These tertiary T states are characterized by a 10-fold difference in oxygen affinity. The observed affinities are very close to those determined in solution when the first oxygen binds to hemoglobin in the absence and presence of allosteric effectors (Poyart et al. 1978). Interestingly, the low oxygen-affinity state binds oxygen with the same affinity as hemoglobin crystals (Rivetti et al. 1993a; Mozzarelli et al. 1997). These conclusions are based on the assumption that a homogeneous population of conformations shows a Hill coefficient of one as postulated by the Monod, Wyman and Changeux model for noninteracting binding sites (Monod et al. 1965). Other models predict Hill coefficients up to 1.3 for T-state oxygen binding (Ackers et al. 2000). However, under any assumption, the hemoglobin gels that we have prepared are much more homogeneous that those previously investigated (Bettati and Mozzarelli 1997; Shibayama and Saigo 2001), opening the way to further functional and structural investigations. Furthermore, our findings indicate that the small degree of cooperativity observed within the T state in solution (Ackers et al. 2000) and in the crystalline state (Rivetti et al. 1993a; Mozzarelli et al. 1997; Eaton et al. 1999) might arise from a ligand-induced alteration of the distribution between the high and low oxygen-affinity T states.
An interesting result of the present study is the measurement of the effect of the binding of IHP and bezafibrate on the oxygen affinity of isolated tertiary T states of hemoglobin. Binding of allosteric effectors to the high-affinity state decreases the oxygen affinity by fourfold, whereas removal of the allosteric effectors from the low-affinity state increases the oxygen affinity by 1.3-fold. Remarkably, the oxygen binding curves still showed a Hill coefficient close to unity, indicating that tertiary states do not interconvert within the gel matrix. Thus, the influence on the oxygen affinity is solely due to the interaction of the allosteric effectors with a defined tertiary state of the protein. In solution, this effect is masked by the redistribution between high and low oxygen-affinity tertiary T states induced by ligand binding.
A model proposed by Rivetti et al. (1993a) suggests that T-state tertiary conformations endowed with different oxygen affinities might be associated to the presence or absence of salt bridges. The results here reported show that the extent of Bohr effect is higher for the high-affinity tertiary T- state and almost absent for the low-affinity tertiary T-state. This indicates that oxygenation causes more Bohr effectlinked salt bridges to be broken in the high-affinity than in the low-affinity T-state. Moreover, the salt bridges that constrain the low-affinity T-state do not appear to be involved in the Bohr effect. Absence of Bohr effect was also observed for the T-state conformation of hemoglobin in the crystal (Rivetti et al. 1993a), in keeping with the crystallographic evidence of intact salt bridges even in a fully liganded state (Arnone et al. 1986; Luisi and Shibayama 1989; Luisi et al. 1990; Abraham et al. 1992; Liddington et al. 1992; Paoli et al. 1996). In solution, the K1 in the absence and presence of allosteric effectors at pH 7.6 and 7.0, respectively (Poyart et al. 1978), differs by a factor of 13. The same value is found comparing the p50 for the high-affinity state of hemoglobin gels at pH 7.6 with the p50 for the low-affinity state at pH 7.0. We propose that the tertiary Bohr effect in solution is caused by the sum of two contributions: the pH-dependent interconversion of the low- and high-affinity states, accounting for a 10-fold difference of p50, and the intrinsic tertiary Bohr effect of the high and low oxygen-affinity states, accounting for a 1.3-fold difference (Poyart et al. 1978).
When encapsulation is performed under conditions that do not lead to the predominant accumulation of either one or the other tertiary conformation, as in the presence of the weak allosteric effector phosphate, a mixture of high- and low-affinity T-states is fixed, leading to binding curves that show Hill coefficients much lower than unity and a Bohr effect that is the result of the Bohr effect of the individual components scaled by their relative distribution.
Our study shows the existence of two discrete conformations within the T quaternary state of hemoglobin and provides the experimental procedure to isolate them. Spectroscopic studies, such as ultraviolet resonance raman of hemoglobin gels (Das et al. 1999; Juczczak and Friedman 1999), will be performed to characterize the low- and high-affinity states of hemoglobin and to determine the structural changes responsible for the 10-fold difference of oxygen affinity.
| Materials and methods |
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Hemoglobin purification and encapsulation
Human hemoglobin was purified as previously described (Rivetti et al. 1993a). Encapsulation of deoxy-hemoglobin in silica gels was performed using the following protocols.
Protocol 1
A solution containing 10 mM HEPES and 1 mM EDTA (pH 6.2) was added to an equal volume of tetramethyl orthosilicate and vortexed for a few minutes. The mixture was then deoxygenated by bubbling nitrogen for 20 min. A solution containing 2.7% (w/v) deoxy-hemoglobin A, 50 mM HEPES, and 1 mM EDTA (pH 6.2) was added. Gelification occurs in
1 h at room temperature. When the gel was formed, a solution containing 100 mM HEPES, 30 mM sodium dithionite, and 1 mM EDTA (pH 7.0) was layered on it.
Protocol 2
The encapsulation was performed following the procedure of Bettati and Mozzarelli (1997) with some modifications. A solution containing tetramethyl orthosilicate, water, and hydrochloric acid was sonicated for 20 min. An equal volume of a deoxygenated solution containing 10 mM potassium phosphate and 1 mM EDTA and the allosteric effectors 2 mM IHP (pH 6) was then added. The mixture was deoxygenated by bubbling nitrogen for 30 min. Finally, a solution containing 2.7% (w/v) deoxy-hemoglobin A, 50 mM potassium phosphate, 30 mM sodium dithionite, 1 mM EDTA, 2 mM IHP, and 2 mM bezafibrate (pH 7.2) was anaerobically added to the mixture. The gelification occured in a few minutes at 4°C. When the gel was formed, a solution containing 100 mM phosphate, 30 mM sodium dithionite, 1 mM EDTA, 2 mM IHP, and 2 mM bezafibrate (pH 7.0) was layered on it.
Protocol 3
The procedure is the same as protocol 2. The only difference is that none of the solutions contained the allosteric effectors IHP and bezafibrate.
Oxygen binding measurements
Before measurements, silica gels were washed under anaerobic conditions once with the storing buffer containing 30 mM dithionite (pH 7) and six times with a deoxygenated buffer solution at a defined pH between 6.5 and 7.8. Exposure of gels to higher pHs leads to slow hemoglobin release. Gels were anaerobically loaded in a Dvorak-Stotler flow cell (Dvorak and Stotler 1971) covered with a gas-permeable silicon copolymer membrane. The flow cell was mounted on the thermostated stage of a Zeiss MPM03 microspectrophotometer (Rivetti et al. 1993a; Bettati and Mozzarelli 1997). Silica gels are optically isotropic and transparent. Unpolarized light was used, and the absorbtion was measured through the gel and the surrounding solution. Spectra were recorded in the wavelength range 450 to 700 nm at 1-nm intervals using gels that absorb usually less than one optical density unit.
Oxygen pressures between 0 and 760 torr were prepared by mixing oxygen and helium with a gas mixture generator (Environics, series 200). The gas mixture, humidified by bubbling through a solution containing 100 mM phosphate buffer, was flowed into the sample cell and then to a polarographic oxygen meter. The oxygen electrode was calibrated with three ceied oxygen gas mixtures1%, 5%, and 21%and pure oxygen. Experiments were performed by first exposing hemoglobin gels to helium and then to a defined oxygen pressure. Spectra were recorded for several hours to monitor both the equilibration with oxygen, which is usually complete within 30 min, and a very slow successive process that has been attributed to the T-to-R quaternary transition (Bettati and Mozzarelli 1997). To minimize the formation of oxidized hemoglobin and the T-to-R transition, measurements were performed at 15°C and on a new sample at each oxygen pressure. Under these conditions, <5% hemes are oxidized and the quaternary transition shows a lifetime of >10 h (C. Viappiani, G. Abbruzzetti, S. Bruno, and A. Mozzarelli, unpubl.).
Data analysis
Fractional saturation with oxygen and fractional concentration of oxidized hemes were determined by fitting each individual spectrum to a linear combination of deoxy, oxy, and oxidized hemoglobin spectra (reference spectra; Rivetti et al. 1993a; Bettati and Mozzarelli 1997), recorded in solution, plus a baseline and a slope to take into account the nonperfect optical quality of the gel surface. This procedure provides a more precise determination of the binding curve with respect to single wavelength measurements.
| 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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A. G. Salvay, J. R. Grigera, and M. F. Colombo The Role of Hydration on the Mechanism of Allosteric Regulation: In Situ Measurements of the Oxygen-Linked Kinetics of Water Binding to Hemoglobin Biophys. J., January 1, 2003; 84(1): 564 - 570. [Abstract] [Full Text] [PDF] |
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U. Samuni, D. Dantsker, I. Khan, A. J. Friedman, E. Peterson, and J. M. Friedman Spectroscopically and Kinetically Distinct Conformational Populations of Sol-Gel-encapsulated Carbonmonoxy Myoglobin. A COMPARISON WITH HEMOGLOBIN J. Biol. Chem., July 5, 2002; 277(28): 25783 - 25790. [Abstract] [Full Text] [PDF] |
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R. W. Noble, L. D. Kwiatkowski, H. L. Hui, S. Bruno, S. Bettati, and A. Mozzarelli Correlation of protein functional properties in the crystal and in solution: The case study of T-state hemoglobin Protein Sci., July 1, 2002; 11(7): 1845 - 1849. [Abstract] [Full Text] [PDF] |
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G. Chirico, F. Cannone, S. Beretta, A. Diaspro, B. Campanini, S. Bettati, R. Ruotolo, and A. Mozzarelli Dynamics of green fluorescent protein mutant2 in solution, on spin-coated glasses, and encapsulated in wet silica gels Protein Sci., May 1, 2002; 11(5): 1152 - 1161. [Abstract] [Full Text] [PDF] |
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