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Department of Biochemistry, The Ohio State University, Columbus, Ohio
Correspondence: Address reprint requests to Elizabeth L. Gross, E-mail: gross.3{at}osu.edu.
| ABSTRACT |
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| INTRODUCTION |
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Electrostatic interactions have been shown to be very important for complex formation between cyt f and PC from higher plants using chemical modification (12
14
), cross-linking (15
17
), and mutagenesis techniques (18
21
). In contrast, mutagenesis studies of cyt f from the green alga Chlamydomonas demonstrated that electrostatic interactions were not important in Chlamydomonas in vivo (22
), although they were observed in vitro (20
).
Higher plant cyt fs have a positively-charged electrostatic field (23
) due to a series of highly conserved positively charged residues (K58, K65, K66, K187, and R209 in turnip cyt f) (24
26
), which interact with the negatively-charged electrostatic field on higher plant PCs (27
) caused by two clusters of anionic residues (7
,8
) on PC. In cyanobacterial cyt fs, such as that of Phormidium laminosum, the cationic residues are replaced by anionic residues (1
,28
) and the anionic patches on PC are replaced by cationic or neutral residues (Fig. 1) (29
35
). The net charge on cyanobacterial PCs varies over a wide range. Prochlorothrix hollandica and Nostoc sp. PCC7119 (formerly Anabaena variabilis) PCs have a net charge of 1.1 and 1.0 at pH 7.0, respectively, as calculated using the program MacroDox (36
). Positively-charged residues on these PC molecules, including R93 (consensus sequence; see Appendix), K11, and K35 surround the H92 ligand to the copper atom resulting in a positively-charged electrostatic field over the top of the molecule (Fig. 1 A). In contrast, Phormidium PC has a net charge of 2.3 at pH 7.0 and shows a much reduced positive patch surrounding H92 (Fig. 1 A). The PCs from Synechocystis sp. PCC6803 and Synechococcus sp. PCC7922, with a net charge of 1.8 and 4.5, respectively, have a negative electrostatic field except in the vicinity of H92 and R93 (Fig. 1 B).
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In this article, we will use Brownian dynamics (BD) simulations (35
,36
,39
) to examine the relationship between the net charge on five PC molecules from five different species of cyanobacteria (Prochlorothrix hollandica, Nostoc sp. PCC7119, Phormidium laminosum, Synechocystis sp. PCC6803, and Synechococcus sp. PCC7942) and their ability to form complexes with Phormidium laminosum cyt f. We show that electrostatic interactions between cyt f and PC depend on two factors: 1) the net charge on the PC molecule; and 2), the distribution of charged residues surrounding H92 on the surface of the PC molecule, which will, in turn, allow us to show that cyanobacterial PCs possess a common binding site for Phormidium cyt f.
BD simulations have been used to study the interaction of turnip cyt f with poplar (40
) and spinach PC (41
,42
); Chlamydomonas cyt f interacting with Chlamydomonas PC (43
,44
); and Phormidium cyt f interacting with Phormidium PC (35
). Brownian dynamics simulations of the interaction between Phormidium PC and Phormidium cyt f (35
) showed that fewer complexes were formed than for the green alga Chlamydomonas reinhardtii PC interacting with Chlamydomonas cyt f, unless the Zn2+ ion found in the crystal structure of Phormidium PC (31
) was included in the simulations. However, even in the absence of the Zn2+ ion, mutation of charged residues on Phormidium PC and cyt f affected the rate of complex formation in BD simulations.
| METHODS |
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Structures for mutant molecules were generated using the MacroDox program (36
,48
,49
). All mutant residues were kept in the same orientation as their wild-type counterparts (i.e., no energy minimization was performed on the mutants). Mutants were divided into different classes depending on their relative effects (See Tables 1 and 2).
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Brownian dynamics (BD) simulations
BD simulations were carried out using the program MacroDox v. 3.2.1 (http://gemini.tntech.edu/
s;/index.html), as described (35
,40
,43
,51
). In MacroDox simulations, target molecule (Molecule I, in our case, cyt f) is placed with its center of mass at the center of a sphere 87 Å in diameter (87 Å was chosen so that the initial electrostatic fields would be very small). Molecule II (in our case, PC) is placed randomly on the surface of the sphere. Molecule II is allowed to move in response to both electrostatic and random Brownian forces. After Molecule II has moved an incremental distance, the forces are recalculated. The steps form a trajectory which ends when Molecule II leaves a sphere of 200 Å in diameter, with its center at the center-of-mass of the target molecule.
MacroDox determines the closest approach of the two molecules for each trajectory based on a preselected reaction criterion. Closest metal-to-metal distance was chosen as the reaction criterion to select for electron-transfer-active complexes (52
,53
). The point of closest approach (smallest Cu-Fe distance) was recorded for each trajectory, permitting the calculation of the number of complexes formed as a function of minimal Cu-Fe distance (Fig. 2). Second-order rate constants for complex formation were calculated from the fraction of complexes observed at distances less than or equal to a preselected reaction criterion using equations derived by Northrup et al. (36
,48
) from the equations of Smoluchowski. If the reaction is diffusion-limited, as was suggested by Hart et al. (54
), the rate of complex formation (k2) should be equal to the rate constant for electron transfer (ket) However, this may not be true in this case (55
) (see Discussion). The number of complexes with a Cu-Fe distances of
20 Å was used to calculate the rate constants; 20 Å was sufficient to include essentially all of the electrostatic complexes formed while excluding those formed solely by random Brownian motion (Fig. 2). MacroDox provides the following information for each trajectory: The structure of the complex at minimum Cu-Fe distance, the 15 closest pairs of charged residues, and the electrostatic interaction energy.
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When using formal charges, noninteger values of the charge on PC and cyt f result from the ionization of histidine residues at pH 7. H25 on cyt f and H39 and H92 (see Appendix) on PC have a zero net charge because they are ligands to the metal centers. The sulfur atom of the Cys-89 ligand to the Cu on PC was given a net charge of 1 (27
), and the Cu atom was given a charge of +2. For cyt f, the charges on the heme were as follows: Fe (+2), two ring nitrogen atoms (1 each), and two propionic acid side chains (1 each). The pK values were calculated using a modified Tanford-Kirkwood pK algorithm (56
).
Electrostatic calculations were carried out using the Warwicker/Watson finite difference method (57
) for solving the linearized Poisson-Boltzmann equation. This algorithm is slightly different from that used in GRASP. The center-of-mass of each protein was placed at the center of a 61 x 61 x 61 grid. The electrostatic field was first iterated over a 3.6 Å grid followed by iteration over a smaller 1.2 Å grid for better accuracy. The choice of grid size has a small (<20%) effect on the rates, but no effect on the structure of the complexes formed (43
). Most importantly, the relative rates of electron transfer were not affected.
Forces, torques, and electrostatic interaction energies
Forces were calculated as described by Northrup et al. (36
). Molecule I (cyt f, the target molecule) was given a low internal dielectric constant of 4.0. However, because of computational complexities, Molecule II (PC) was treated as a set of point charges embedded in a medium of the same dielectric (48
,58
,59
) (S. Northrup, personal communication, 2002). Also, mutual desolvation effects (59
,60
) were neglected. These effects may cause an overestimation of the reaction rates by as much as 25%. However, desolvation effects are not significant in these simulations (35
). By neglecting these, neither the relative effects of the mutations nor the structures of the complexes formed should be affected (48
) (S. Northrup, personal communication, 2002). Also, hydrodynamic effects can be neglected due to the compact nature of the molecules (39
). Torques were calculated using dipoles for the moving protein as described by Northrup et al. (61
).
Calculation of hydrophobic and electrostatic free energies
Hydrophobic interaction free energies were determined as described by Gross and Pearson (43
). The residues at the complex interfaces were determined by selecting those residues on Phormidium cyt f within 8 Å of any residues on PC (10 Å for Phormidium PC), using an in-house program. Those residues on PC within 8 Å (10 Å for Phormidium PC) of any residue on cyt f were chosen using the same method. Ten representative complexes, with Cu-Fe distances less than or equal to those at maximum complex formation, were chosen for study (17 Å for Nostoc and Prochlorothrix Y12G PC, 18 Å for WT Prochlorothrix PC and 21 Å for Phormidium PC). A residue was considered to be part of the interface if it was observed in at least eight of the 10 complexes chosen (seven out of 10 complexes for Phormidium PC). The calculated interaction area is an underestimate, particularly in the case of Phormidium PC, because the two molecules are not as close as they will be in the final electron transfer active dock. The surface areas of the hydrophobic atoms of these residues on both PC and cyt f were calculated using the Richards (62
,63
) algorithm, which is part of the MacroDox software package. The total hydrophobic surface area was considered to be twice the smaller of the PC or cyt f hydrophobic surface area.
Reported values for hydrophobic interaction energies vary between 25 and 47 cal/Å2 (64
66
). Because of the wide variation, both 25 and 47 cal/Å2 were used for our calculations.
Electrostatic interactions were taken from the .rec files of the MacroDox output. In each case, all complexes formed with Cu-Fe values less than the values of maximal complex formation (see above) were included. Five sets of 1000 trajectories for Prochlorothrix and Nostoc and 5000 trajectories for Phormidium PC were averaged and included between 150 and 400 complexes per set.
| RESULTS |
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Fig. 2 A compares the results for Nostoc, Prochlorothrix, and Phormidium PC interacting with Phormidium cyt f, with those previously obtained for Chlamydomonas PC interacting with Chlamydomonas cyt f (43
). In the case of Nostoc PC, maximum complex formation occurred at a Cu-Fe distance of 17 Å compared to 15 Å for the Chlamydomonas system. However, for Prochlorothrix PC, the peak is shifted to 18 Å as a result of the presence of a tyrosine at position #12 in Prochlorothrix PC instead of the glycine found in PCs from all other species (8
). When Y12 is replaced by a glycine (Fig. 2 B), the peak is shifted back to 17 Å. The double mutant (Y12G + P14L) described by Crowley et al. (38
) showed nearly identical results to the single Y12G mutant. Both Nostoc and Prochlorothrix PC showed a greater number of complexes formed when interacting with Phormidium cyt f than did Chlamydomonas PC interacting with Chlamydomonas cyt f (Fig. 2 A).
When Phormidium PC interacted with Phormidium cyt f, peak complex formation was shifted to 20 Å (Fig. 2 D). Also, the number of complexes formed was only 20.4 ± 0.5 complexes/1000 trajectories compared to 341.2 ± 4.7 for Prochlorothrix PC under the same conditions. However, in the absence of the electrostatic field, the number of complexes formed were 2.0 ± 0.2 (35
) and 1.8 ± 0.8 (Table 1) for Phormidium and Prochlorothrix PC, respectively, indicating that the differences in complex formation reflect the differences in charge on the two PC proteins. Maximum complex formation was observed at a Cu-Fe distance of 22 Å (with a value of 33.7 ± 0.6 complexes/1000 trajectories) for Synechocystis PC (Fig. 2 D).
Interestingly, in the case of Synechococcus PC, fewer complexes were formed in the presence of the electrostatic field than in its absence (Fig. 2, C and D), indicating charge repulsion between Synechococcus PC and Phormidium cyt f. This is not surprising, since the net charge on Synechococcus PC is 4.5 compared to a net charge 14.0 Phormidium cyt f. This raises the questions as to whether Synechococcus PC would show greater complex formation when interacting with Synechococcus cyt f than with Phormidium cyt f. For this reason, Synechococcus cyt f was built by homology-modeling with SWISS MODEL ((67
) http://swiss-model.expasy.org), using turnip and Phormidium cyt f as templates. When Synechococcus PC interacted with Synechococcus cyt f, 17.1 ± 0.1 complexes with Cu-Fe distances
20 Å were formed per 1000 trajectories compared to 18.0 ± 0.1 for Phormidium cyt f under the same conditions. The rates of interaction were 4.9 ± 1.3 and 5.3 ± 1.0 x 107 M1 s1, respectively. These results are not surprising since the net charge on the Synechococcus cyt f molecule is 18.7 as calculated by MacroDox compared to 14.0 for Phormidium cyt f. Therefore, the poor performance of Synechococcus PC can not be attributed to using the "wrong" cyt f.
The effect of the net charge on the PC molecule on the number of complexes formed with Phormidium cyt f
One reason for the difference in the number of complexes formed for PCs from different species of cyanobacteria may be the difference in net charge on the various PC molecules. To test this hypothesis, two types of simulations were performed (Fig. 3). In the first experiment, indicated by the numbers 19 next to the data points in Fig. 3, the net charge on Prochlorothrix PC was varied between 2.0 and +3.0 by mutating charged residues to alanine. The results show that the number of complexes formed was a linear function of the net charge at values more positive than 1.0. The results for mutants of Phormidium PC also fall on the same line (68
). In the second set of simulations, the five cyanobacterial PCs shown in Figs. 1 and 2 were compared. These are indicated by letters AD and the number 5 on Fig. 3. It can be seen that few, if any, complexes were formed, due to electrostatic interactions alone, if the net charge on the PC molecule was more negative than 2, but that the data point for Nostoc PC falls on the same line as for the Prochlorothrix mutants. Thus, the number of complexes formed is a linear function of the net charge on the PC molecule for a net charge greater than 2. Note that, in both sets of experiments, hydrophobic interactions were not included in the simulations. If they had been, the number of complexes formed would have been greater and significant complex formation would have been observed for Synechocystis, Synechococcus, and Phormidium PC.
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20 Å was determined. A 20 Å reaction criterion was chosen under the assumption that once the metal centers of the two molecules approach to within that distance, hydrophobic interactions come into play. For comparison, the PC and cyt f touch each other at a Cu-Fe distance of 15 Å for Nostoc PC and 16 Å for Prochlorothrix and Phormidium PC. Changing the reaction criterion to 18 Å changes the number of complexes included but not the relative effects of the mutations (35For both Prochlorothrix and Nostoc PC, the mutants were divided into five classes:
130% of the WT values. These included D10A, E17A, and D44A for PCs from both species. In addition, E90A, which is not conserved, was also included in Class I for Nostoc PC.
D44A, D10A, and E17A also showed maximal stimulation of the interaction of Phormidium PC with Phormidium cyt f (35
), and D10A and E17A also showed significant stimulation for Synechocystis PC (not shown) interacting with Phormidium cyt f. K6A, K35A, K46A, K100A, and R93A also showed severe inhibition for Phormidium PC interacting with Phormidium cyt f (35
) as did mutants K6A, K35A, and R93A (consensus sequence) for Synechocystis PC (not shown). Thus, the same residues (especially D10, E17, D44, K35, R93, and possibly K6) are involved in complex formation in all four cyanobacterial PCs studied. K11 is also important for Prochlorothrix and Nostoc PC. S11K mutants of Phormidium and Synechocystis PC (not shown) stimulated complex formation to the same extent as the neighboring D10A mutants, indicating that a lysine at position 11, when present, also assists in complex formation. The locations of these important (Classes I, IV, and V) residues on the surface of Prochlorothrix, Nostoc, and Phormidium PC are shown in Fig. 5. Note that they all surround H93 (H87 in higher plant and algal PCs) on the top face of the PC molecule. Also, note the significant role of conserved charged residues in complex formation. Moreover, the location of these charged residues controls the location of binding site on PC for cyt f but the net charge on the PC molecule controls the strength of the electrostatic portion of the interaction.
Close electrostatic contacts
The output of the MacroDox program provides a list of the 15 closest electrostatic contacts for all complexes with reaction coordinate distances less than or equal to a preset value. For our studies of cyanobacterial PCs interacting with Phormidium cyt f, we chose a Cu-Fe distance less than or equal to that which gave the peak value for complex formation. This value was 20 Å for Phormidium PC, 17 Å for Nostoc PC, and 18 Å for Prochlorothrix PC, respectively. The results are presented in Table 3. A given residue was listed if it appeared as one of the 15 closest contacts in at least 50% of the complexes formed.
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The most prevalent electrostatic contacts for residues on Phormidium cyt f are listed in Table 4. A residue is listed if it showed at least an average of 0.5 contacts/complex for at least one of the PC species represented. The following residues show at least 0.9 contacts/complex for all three PCs: D63, E123, R157, E165, D188, and the heme. All of these residues surround the heme as shown in Fig. 6. E165 and D188 are located on the small domain whereas all of the other residues are located on the large domain of cyt f.
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| DISCUSSION |
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Agreement of BD simulations and experimental results
The question arises as to how well the BD results agree with experiments both with respect to rates of electron transfer, and the structure of the complexes formed.
With respect to the rates, three questions need to be answered:
With respect to the first question, Schlarb-Ridley et al. (55
) studied the effect of viscosity and temperature on electron transfer rates for Phormidium cyt f interacting with Phormidium PC. They concluded that the reaction is not diffusion-limited, but instead involves a rearrangement of the initial diffusion-controlled complex to bring PC to a position in which it can rapidly receive an electron from cyt f. Thus, the overall reaction is at least partially activation-limited.
The second question concerns whether the MacroDox complexes observed in our simulations are the result of diffusion or activation-limited processes. This depends on the reaction criterion used. If the reaction criterion used is best electrostatic interactions, then the complexes observed will be entirely electrostatically driven and diffusion-limited. On the other hand, the use of minimum Cu-Fe distance as the reaction criterion yields complexes as they would appear after a rearrangement with a small Cu-Fe distance allowing rapid electron transfer.
In the case of cyt f and PC, hydrophobic residues on both proteins would be brought together. Thus, although hydrophobic forces do not provide a driving force for complex formation, they are evident in the final complexes. However, the MacroDox complexes do not represent the final electron-transfer-active dock because many of them stop short of the final docked position (because of the random forces and the lack of an explicit inclusion of hydrophobic forces). This is the reason that hydrophobic interaction energies are underestimated.
With respect to question three, the magnitude of the rate constants determined by MacroDox simulations are always greater than the corresponding experimental values.
There are at least three reasons for the larger rate constants in MacroDox simulations. First, the rate constants for the simulations are overestimated due to the absence of a low internal dielectric constant for PC and the desolvation effects mentioned above. Second, no attempt was made to correct the BD reaction rates for attenuation due to the distance between the metal centers, which would decrease the measured electron transfer reaction rates (52
,53
). Third, the calculated rates are a function of the reaction coordinate cutoff distance. For these simulations, a 20 Å cutoff distance was chosen to include all possible complexes in which the Cu on PC might come close enough via electrostatic or hydrophobic interactions to receive an electron from cyt f. The 20 Å cutoff distance resulted in a calculated reaction rate (ka) of 360 x 10 6 M1 s1 (35
). Decreasing Cu-Fe reaction criterion distance to 18 Å (35
) decreased the calculated rate to 80 x 10 6 M1 s1, which is comparable to the experimental value of 47 x 10 6 M1 s1 (34
).
The most important point, however, is that the relative effects of the mutations are independent of the reaction coordinate cutoff distance and are in general agreement with experiments, not only for mutations of Phormidium PC (34
) but also for Chlamydomonas PC (44
) when compared to experimental mutations of higher plant PCs (19
,21
). Thus, MacroDox simulations can be used to predict the effects of PC mutations in systems for which there are no experimental data.
Overall, the structures of the BD complexes formed also agree with those determined by NMR. For example, the complex formed between Chlamydomonas PC and Chlamydomonas cyt f is very similar to that of spinach (69
), poplar (71
), and parsley (72
) PC. In all of these cases, H87 (H92 in the cyanobacteria) faces the heme on cyt f and the PC molecule is tilted toward the small subunit with the two acidic clusters on PC interacting with the cationic residues on cyt f.
In contrast, in the complexes formed between Phormidium cyt f and Phormidium PC (35
), Prochlorothrix PC (Figs. 7 and 8), and Nostoc PC (Fig. 7) PC, the PC molecules sits vertically on top of the cyt f with its long axis perpendicular to the long axis of cyt f. These results agree with the NMR results of Crowley et al. (37
,38
) for complexes formed between Phormidium cyt f and Phormidium and Prochlorothrix PC, respectively.
The role of electrostatic interactions in complexes formed between cytochrome f and PC in cyanobacteria
Electrostatic interactions between Phormidium cyt f and various cyanobacterial PCs depend on two factors: 1), the net charge on the PC molecule; and 2), the charge configuration around H92.
The effect of the net charge on the cyanobacterial PC molecule on complex formation
The results depicted in Fig. 3 show that the number of complexes formed in MacroDox simulations is a linear function of the net charge on the PC molecule whether the net charge on the PC molecule is altered by mutation or by using PCs from different species of cyanobacteria. Those species of cyanobacteria for which the net charge on PC at pH 7.0 is <1.0, such as Synechococcus, Synechocystis, and Phormidium, show few if any complexes due to weaker electrostatic interactions in the Brownian dynamics (BD) simulations (note that there may still be complex formation due to hydrophobic interactions). These results agree with the NMR studies of complex formation between Phormidium cyt f and Phormidium PC (37
), in which there was no effect of ionic strength on complex formation to indicate a paucity of electrostatic interactions. In contrast, cyanobacterial PCs having net charges more positive than 1.0, including WT Nostoc PC (net charge = +1.1) and Prochlorothrix PC (net charge = +1.0), showed a linear relationship between the number of complexes formed and the net charge on the PC molecule. This is true both for the Prochlorothrix mutants shown here and the Phormidium mutants described by Gross (68
). Also, NMR studies of complex formation between Phormidium cyt f and Prochlorothrix PC (38
) showed an ionic strength-dependence of complex formation indicating significant electrostatic interactions in agreement with the BD results described above. Note that a linear dependence of electron transfer rate on net charge was also observed for higher plants (19
).
The increase in the number of BD complexes formed as a function of increasing positive charge on the PC molecule parallels the increase in binding constants for Phormidium cyt f-cyanobacterial PC complexes determined by NMR spectroscopy. For example, the binding constant for Phormidium PC complexes was 0.3 mM1 PC (37
), 6 ± 2 mM1 for Prochlorothrix PC (38
), and 12 ± 1 mM1 for Nostoc PC (73
) interacting with Phormidium cyt f. The increase in both the number of BD complexes formed and the magnitude of the binding constants reflect the increase in electrostatic interactions.
Specific charge interactions between Phormidium cyt f and cyanobacterial PCs
There are also specific charge interactions that are superimposed upon the net charge effects and influence the structure of the complexes formed between Phormidium cyt f and cyanobacterial PCs. Mutation of R93 and K35 to alanine inhibits complex formation for Prochlorothrix PC (Table 1), Nostoc PC (Table 2), Phormidium PC (Table 2 from Gross (35
)), and Synechocystis PC (not shown). Mutant studies also show that K11 is important in Prochlorothrix and Nostoc PC as is K62 in Nostoc PC. K35, R93, and K11 (present only in Prochlorothrix and Nostoc PC) also showed more than one electrostatic contact per complex formed (3
). On the other hand, mutation of D10 and E17 stimulated complex formation in all four cyanobacteria. Removal of D44 in Prochlorothrix, Nostoc, and Phormidium PC and E56 in Synechocystis PC also stimulated complex formation. Additional residues that are involved include E90 in Nostoc PC, E70 in Synechocystis PC, and D45, D55, and E70 in Phormidium PC.
R93, K35, D10, E17, and a residue in the vicinity of D44 are highly conserved in cyanobacterial PCs. Moreover, all of these residues surround H92 on the top face of cyanobacterial PC molecules (Fig. 5) implying that this is the face presented to cyt f in agreement with the NMR results for Phormidium (37
) and Prochlorothrix (38
) PCs interacting with Phormidium cyt f. These results contrast with those obtained for higher plant and green algal PCs in both NMR (62
,64
,65
) and BD simulations (35
,40
,43
,44
), in which the anionic residues surrounding Y88 (Y83 in green plant numbering) provide the electrostatic interactions.
The role of hydrophobic interactions in complex formation between Phormidium cyt f and cyanobacterial PCs
The question arises as to the role of hydrophobic interactions in complex formation. This is particularly important for those PCs such as Synechococcus, Synechocystis, and Phormidium that show poor electrostatic interactions. All PCs including those from higher plants and green algae have a highly conserved hydrophobic patch surrounding H92 (H87 in higher plants and green algae) (8
), which includes the following amino acid residues: G8, G12 (Y in Prochlorothrix), L14 (P in Prochlorothrix), F16 (Y in Prochlorothrix), Residue 36 (hydrophobic in cyanobacteria and G in higher plants and algae), P38, L64 (Y in green algae and some higher plant PCs such as parsley), P91, G94, A95, and G96, plus some other residues in individual PCs. Thus, hydrophobic interactions appear to be ubiquitous.
One of the weaknesses of MacroDox is that it does not explicitly include hydrophobic interactions. What this means is that hydrophobic interactions are not included as a driving force for complex formation (i.e., the number of complexes formed and the corresponding reaction rates would be greater upon inclusion of hydrophobic forces. This is particularly important in the case of mutants R93A (Nostoc PC) and R86A (Prochlorothrix PC) as well as wild-type Phormidium, Synechocystis, and Synechococcus PC, which would have shown significant complex formation if hydrophobic interactions had been included.
However, even though it was not possible to include hydrophobic interactions as a driving force for complex formation, it was possible to estimate the hydrophobic interaction energies of the complexes formed. The strength of the hydrophobic interactions was estimated for Prochlorothrix, Nostoc, and Phormidium PC interacting with Phormidium cyt f (Table 5). The procedure involved determining the surface areas of those residues involved in hydrophobic interactions between PC and cyt f. The surface areas of individual residues and atoms thereof for both cyt f and PC were determined using the method of Richards (62
,63
). Of these, the residues involved in hydrophobic interactions and the sum of their surface areas were determined as described in Methods and in Gross and Pearson (42
). Two times the smaller of the two hydrophobic surface areas (PC or cyt f) was taken as the hydrophobic surface area given in Table 5.
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The second problem is that there are large uncertainties in the magnitude of the hydrophobic free energies with estimates varying from 25 to 47 cal/Å2 (64
66
), which is why we have used both values in our calculations (Table 5). Nonetheless, two conclusions can be drawn. First, the hydrophobic free energies are as large as, or larger than, the electrostatic free energies. For Prochlorothrix PC (Table 5), for example, the hydrophobic interaction energies using 25 cal/Å (64
) was 16.1 kcal-mol1 compared to 9.1 kcal-mol1 for the electrostatic interaction energies. Second, the hydrophobic interaction energies are larger for the cyanobacteria than for Chlamydomonas (7.5 kcal-mol1) (47
). The results agree with the experimental results of Schlarb-Ridley et al. (74
), who observed significant interactions between Phormidium PC and Phormidium cyt f even at infinite ionic strength. On the other hand, the magnitude of the electrostatic interactions was the same magnitude for Nostoc (8.5 ± 0.3 kcal-mol1) and Prochlorothrix PC (10.5 ± 0.4 kcal-mol1) as for Chlamydomonas PC (10.5 ± 1.5 kcal-mol1), although the charge configurations are different. Note that the electrostatic interaction energy for Phormidium PC (2.1 ± 0.4 kcal-mol1) was less, as expected, due to the lower net charge.
The structure of the complexes formed between Phormidium cyt f and cyanobacterial PCs
An examination of the residues involved in electrostatic contacts (Table 4, Fig. 6) shows that the binding site on cyt f for cyanobacterial PCs surrounds the heme with five of the most frequent electrostatic contacts (D63, E123, K157, and E165, in addition to the heme itself) residing on the large domain and only D188 being situated on the small domain. In addition, the long axis of PC is perpendicular to the long axis of cyt f as shown previously for Phormidium cyt f-Phormidium PC and Phormidium cyt f -Prochlorothrix PC complexes in NMR studies (37
,38
) and by Gross (35
) in BD simulations of Phormidium cyt f interacting with Phormidium PC. Thus, the structure of these complexes is different from those of higher plants and algae in which both NMR studies (69
72
,75
) and BD simulations (39
,42
,43
) in which PC leans toward the small domain, allowing the lower negative patch to interact with positively-charged residues on the small domain of cyt f (e.g., K187 and K188 in Chlamydomonas cyt f).
However, all three PCs examined (WT Prochlorothrix, Nostoc, and Phormidium) showed considerable heterogeneity in orientation around the long axis of PC. The results for Phormidium PC agree with the NMR results of Crowley et al. (37
), who also observed considerable heterogeneity of the complexes formed (See (35
) for a comparison of BD and NMR results). These results are different from those for both higher plants and green algae where both NMR results (69
) and BD simulations (43
) showed more complexes that are homogeneous. This may be attributed to the greater asymmetry in charge distribution on PC molecules from higher plants and green algae (i.e., most of the negatively-charged residues are located on one face of the PC molecule). If charge asymmetry is required for orientation of PC within the complexes, then the more uniform electrostatic field around cyanobacterial PCs would not be expected to promote a single orientation of PC within the complexes. Interestingly, mutating Y12 to G increased the homogeneity of the complexes formed (Fig. 7). If the only requirement for electron transfer is a close distance between Y1 on cyt f and H92 (H87 in higher plants and green algae) on PC, then the orientation of PC within the complex is not important and multiple orientations of the PC molecule (provided H92 is close to Y1) may actually increase the probability of electron transfer as suggested by Crowley and Ubbink (70
).
| CONCLUSIONS |
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The complexes formed for all three cyanobacterial PCs studied show heterogeneity in the orientation of the PC molecule on cyt f even in complexes where the H92 ligand to the Cu on PC is close to the Y1 ligand to the heme on cyt f. These results suggest that an exact orientation is not required for electron transfer.
| APPENDIX |
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Submitted on April 22, 2005; accepted for publication September 13, 2005.
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