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* Laboratoire de Dynamique, Interactions et Réactivité, CNRS-Université Paris VI, Thais, France;
Max-Planck Institut für Strahlenchemie, Mülheim, Germany;
Paul Scherrer Institut, Life Sciences, Structural Biology, OSRA/008, Villigen, Switzerland; and
URA 2096, CEA-CNRS, DBJC/SBFM CEA-Saclay, Gif/Yvette, France
Correspondence: Address reprint requests to Dr. Sophie Lecomte, Laboratoire de Dynamique, Interactions et Réactivité, UMR-7075, CNRS-Université Paris VI, 2 Rue Henri Dunant, F-94320 Thais, France. Tel.: 33-1-4978-1113; Fax: 33-1-4978-1118; E-mail: sophie.lecomte{at}glvt-cnrs.fr.
| ABSTRACT |
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| INTRODUCTION |
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The lysine cluster (Lys-72, Lys-86, and Lys-87) close to the exposed heme edge was believed to be a structural template common to all soluble c-type cytochromes. But it was shown recently that cytochrome c552 (cyt-c552), an electron carrier in the respiratory chain of Thermus thermophilus, lacks this lysine-rich domain. The region around the exposed heme edge is shielded by an additional nonpolar peptide segment that is believed to increase the thermostability of the protein (Than et al., 1997
). This property of cyt-c552 raises fundamental questions about how electron transfer occurs to its membrane bound reaction partner, as well as its own interaction with membrane. The ba3-oxidase specifically recognizes the cytochrome c552 as electron donor (Than et al., 1997
) and there is no cross reactivity with the horse heart cytochrome c. This is due to differences in the properties of the protein surfaces interacting to form the electron transfer complex. The area around the solvent-exposed heme edge of cytochrome c552 as well as the surface near the CuA site of the ba3-oxidase are almost uncharged. (Soulimane et al., 2000
) The crystal structure of ba3-oxidase shows no negatively charged residues on the putative substrate binding site, resulting in uncommon electrochemical and spectroscopic properties of the ba3-oxidase (Hellwig et al., 1999
). Thus the mechanism of electron transfer for cyt-c552/ba3-oxidase is different from that of cyt-c/cyt-c oxidase. Some studies have demonstrated that the main interaction between cytochrome c552 and ba3-oxidase is hydrophobic and that heterogeneous electron transfer in cyt-c552 does not depend on a change in the heme conformation, as in horse heart cyt-c (Lecomte et al., 1998
, 1999
; Bernad et al., 2003). There is no published information on the binding of cyt-c552 to membranes or liposomes.
We therefore investigated the influence of the structure of T. thermophilus cyt-c552 on its interaction with liposomes, as model membranes. We examined the binding of cyt-c552 and cyt-c to DOPG vesicles to determine the similarities and differences in their behaviors. Turbidity measurements were used to evaluate the aggregation of liposomes incubated with the cytochromes. Fourier transform infrared (FTIR) spectroscopy was used to detect any changes in the secondary and tertiary structures of both proteins as they interacted with the DOPG liposomes. We also used Fourier transform infrared-attenuated total reflection (FTIR-ATR) to monitor the interaction of both proteins with a silicon surface coated with octadecyltrichlorosilane to estimate the influence of a pure hydrophobic environment on the secondary and tertiary structures of the two proteins.
| MATERIALS AND METHODS |
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Vesicle preparation
DOPG was purchased from Sigma. Dry films of 10 mg lipid were prepared from a stock solution in chloroform evaporated under a stream of nitrogen and left under vacuum for at least 8 h to remove all traces of the organic solvent. The lipid films were suspended in 5 mM HEPES/EDTA, pH 7.5, or 10 mM Tris/HCl, pH 7.5, buffer and gently vortexed for a few minutes. DOPG vesicles were then prepared by sequential extrusion through polycarbonate membranes (Osmonics) of decreasing pore size (from 0.8 µm to 0.05 µm). The size of DOPG vesicles, measured by dynamic light scattering (submicron particle analyzer model N4MD, Coulter Electronics, Hialeah, FL), was
110 nm. The DOPG vesicles used for FTIR experiments were prepared in deuterated buffer.
Turbidity experiments
The change in the turbidity at 650 nm of the suspension of liposomes while cyt-c or cyt-c552 were continuously added was recorded on a Perkin-Elmer (Foster City, CA) Lambda2 double beam spectrophotometer equipped with a temperature regulation system (Pott et al., 1998
). The wavelength used was far from any electronic transition of the cytochromes. The temperature was 25°C ±0.05°C. A paddle cuvette stirrer was placed in the quartz cuvette containing the liposome suspension. The cytochrome solution was slowly and continuously injected into the cuvette through a thin tube connected to a thermostated precision glass syringe (Hamilton, Reno, NV) driven by a syringe pump (Model VI, B. Braun, Melsungen, Germany). To ensure equilibrium conditions, cyt-c and cyt-c552 were injected very slowly (1.4 µL/min for 3 h) into 1.5 mL solutions with DOPG concentrations from 25 µM to 200 µM. The path length of the measuring cell was 10 mm for all experiments.
The concentration of cyt-c in the cuvette was deduced from the concentration of cyt-c in the syringe ([cyt-c]syringe), the initial volume of the liposome suspension (v0) and the added volume (va) using the equation:
![]() | (1) |
![]() | (2) |
The lipid in the cuvette ([lip]cuvette) was diluted; the concentration was calculated using the following equation:
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FTIR spectroscopic measurements
Deuterated buffer solutions were prepared with K22HPO4 (0.05 mol L1) obtained by repeated crystallization of K2HPO4 from 2H2O. The p2H of all samples was adjusted by adding 2HCl to obtain a value similar to pH 7.6. Lyophilized cyt-c and cyt-c552 were dissolved in deuterated buffer to a final concentration of 4 mg/ml (0.32 mM for cyt-c and 0.28 mM for cyt-c552). DOPG/cyt-c mixtures were prepared by adding DOPG vesicles in deuterated buffer to the cyt-c or cyt-c552 solution. The [cyt-c]/[DOPG] ratio used for the FTIR experiment was selected based on the turbidity results. These experiments determined the characteristic breakpoints on the turbidity curves and thus the relationship between lipid and cytochrome concentrations. We used this relationship to set the lipid and cytochrome concentrations for the infrared experiments. The lipid-protein complexes were separated from the small amount of unbound protein by centrifugation (Beckman Coulter, Fullerton, CA) for 4 h at 4°C at 30,000 rpm (32 x g). The concentration of unbound protein in the supernatant was determined spectrophotometrically at 410 nm. No more than 5% of the initial protein remained in the supernatant. Control experiments with rhodamine (R6G)-labeled vesicles showed that there were no DOPG vesicles in the supernatant. Fluorescence experiments after centrifugation confirmed that there were no vesicles in the supernatant. Thus, the FTIR spectra recorded were due solely to the cytochrome/DOPG complex. The [cytochrome]/[DOPG] ratios were 0.67:10 and 1.11:10 for cyt-c and 0.07:10 for cyt-c552. Protein/DOPG solutions were analyzed between two CaF2 plates of 25 µm thickness. FTIR transmission spectra were recorded with a Perkin-Elmer 1720 spectrometer (4 scans; 4 cm1 resolution). A Balston air dryer (Maidstone, UK) was used to reduce the water vapor content in the spectrometer. The FTIR spectra were recorded from 10 min to 5 h after sample preparation. The addition of buffer to the dry protein and protein/DOPG mixture was taken as the starting point of the processes under investigation. The FTIR spectra measured after 5 h were taken as the reference for equilibrium conditions.
FTIR-ATR experiment
The ATR crystal was cut at 45° from monocrystalline silicon Si(100) covered with a layer of native silica. The hydrophobic silanized surface was prepared by immersing the cleaned ATR crystal in a solution of octadecyltrichlorosilane (OTS) (Roth, Strasbourg, France) as described by Wasserman et al. (1989)
. Briefly, the concentration of OTS was 1 mM in carbon tetrachloride/hexadecane (30:70, v/v). The wettability of the grafted self-assembled monolayers was checked by contact angle measurements using water drops. The value for OTS was 110° (Nuzzo et al., 1990
). FTIR-ATR spectra were recorded on a Nicolet 850 spectrometer (Dongen, The Netherlands) with Boxcar apodization and a resolution of 4 cm1. The sample compartment was continuously purged with dried air. The internal reflection element was placed in an ATR liquid cell and allowed 75 internal reflections at the liquid/crystal interface (Noinville et al., 2002
). An infrared spectrum of the deuterated buffer was recorded as reference. The cell was emptied and refilled with 100 µg/mL cyt-c or cyt-c552 (around 8 µM) in deuterated buffer and interferograms were recorded from 8 min to 5 h.
Analysis of the FTIR and FTIR-ATR spectra
The spectral contributions of the buffer and adsorbents were subtracted from the measured spectra. The resulting spectra were analyzed with an algorithm based on a second derivative function and self-deconvolution procedures to determine the number and the wavenumber of individual bands within the spectral range 15001750 cm1 (Fig. 1; see also Boulkanz et al., 1997
; Lecomte et al., 2001
). The relative contributions of the various bands were obtained by a band-fitting procedure, keeping the wavenumbers, half widths at half heights (1420 cm1), and band profiles (75% Gaussian and 25% Lorentzian) constant and allowing only the intensities to vary. All spectra could be fitted by seven amide I' and two amide II components along with a few bands assigned to amino acid side chains. The content of the various secondary-structure elements was estimated by dividing the integral intensity of one amide I' band component by the total intensity of all amide I' band components. The amount of each secondary-structure element is given as a percentage. The surface of the amide I' band was considered to be due only to the amide I' band of the polypeptide backbone, neglecting the amide groups of the Gln and Asp side chains. The T. thermophilus cyt-c552 contains 3 Asn and 10 Gln residues, whereas horse heart cyt-c has only five Asn and three Gln. All are exposed to the solvent, so the amide I' wave numbers should be 1650 for Asn and 1635 cm1 for Gln residues (Chirgadze et al., 1975
; Sukhishvili and Granick, 1999
), with molar extinction coefficients comparable to those of the polypeptide backbone (Chirgadze et al., 1975
). These bands were not included in the band-fitting analysis, so that the relative contributions of the amide I' band components indicating peptide bonds in random-coil domains (1638 cm1) and ß-strands or turns (1630 cm1) and in the
-helix (1660 and 1646 cm1) were overestimated. The contribution of the Asn/Gln side chains to the amide I' band was constant in all spectra recorded; thus, the error of the secondary-structure determination is constant and systematic. The intensity redistribution among the amide I' bands can be quantified in terms of secondary-structure changes, allowing for the numbers of peptide bonds in cyt-c (Buschnell et al., 1990
) and cyt-c552 (Than et al., 1997
). Thus, a 2% increase or decrease in amide I' integrated absorbance is due to 23 peptide bonds. The integral amide II band intensities were normalized in the same way. The amide II/amide I' integrated absorbance ratio was used to assess the degree of H/2H exchange using a reference value of 0.5 for totally hydrogenated proteins in the solid state, according to studies of various globular proteins in solid state.
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| RESULTS |
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The effect of cyt-c552 binding to DOPG vesicles is quite different, as revealed by the shape of the turbidity curve and by the different R* values at flocculation. We again estimated the surface area ratio cyt-c552/DOPG at the flocculation point, assuming that the available surface area of one cyt-c552 molecule was 1400 Å2 (Than et al., 1997
) and found 0.145, which was very low, and indicated that aggregation takes place when the liposome surface is far from covered by absorbed protein. Cyt-c552 is also positively charged at physiological pH, but the distribution of the charge is quite different from that for the eukaryote cytochrome c.
FTIR-experiments on cyt-c and cyt-c552 in deuterated buffer
The 16001700 cm1 spectral region is dominated by the amide I' mode of the polypeptide backbone of cytochrome. A large number of experimental data enabled us to assign the individual amide I' band components to various elements of proteins secondary structure (Byler and Susi, 1986
; Surewicz and Mantsch, 1988
). Table 2 summarizes the assignment of the components of the amide I' band of both cytochromes. The assignment of the amide I' band of the T. thermophilus cyt-c552 has been already described and discussed (Lecomte et al., 2001
). Several assignments have been reported for horse heart cyt-c (Byler and Susi, 1986
; Lo and Rahman, 1998
; Paquet et al., 2001
). Except for the assignment of the band at 1660 cm1, described by Heimburg and Marsh (1993)
and Lo and Rahman (1998)
as a contribution to the amide I' group involved in ß-turns, the assignment in Table 2 is in a good agreement with those of other authors (Goormaghtigh et al., 1990
; Dong et al., 1992
). However, the difference may arise because the authors (Heimburg and Marsh, 1993
; Lo and Rahman, 1998
) used only six bands for the self-decomposition of the amide I' bands and because the half-width of the band associated with an
-helix is large. From their analysis the calculated percentage of
-helix is very different from the value determined by x-ray crystallography. The crystal structures of cyt-c and cyt-c552 show that
45% and 49% of the amino acids are involved in an
-helix (Buschnell et al., 1990
; Than et al., 1997
), which is in good agreement with the relative contributions (%) of each secondary structure element determined by our analysis of the FTIR spectra (see Tables 3 and 4). The profiles of the amide I' bands in the two cytochromes were different, in agreement with their structures. Cyt-c552, which is more compact and more hydrophobic than cyt-c, has 16% fewer residues involved in the hydrated random domain than cyt-c) and more residues in internal or hydrophobic
-helices (+6%) or ß-turn structures (+6%). The analysis of the FTIR spectra of both cytochromes at different times after dissolution gave similar results for the secondary-structure elements (result not shown).
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Binding of cyt-c and cyt-c552 to DOPG vesicles
The components used for the spectral analysis of the FTIR spectra of the cytochrome/DOPG mixtures were identical to those for cyt-c and cyt-c552 in solution; only the integrated absorbance of the band was varied. The diagram in Fig. 5 A shows the percentages of amide groups involved in secondary structure elements in cyt-c in solution and cyt-c bound to DOPG vesicles at a [cyt-c]/[DOPG] ratio of 1.1:10 (after breakpoint 2). The values in Table 3 show the result for a [cyt-c]/[DOPG] ratio of 0.66:10 (before breakpoint 1). The secondary structure elements underwent only small changes when the protein was bound to DOPG vesicles at all the [cyt-c]/[DOPG] ratios used. This is in agreement with published data (Choi and Swanson, 1995
; Heimburg and Marsh, 1993
). There is only a small decrease (2%) in the 1660 cm1 component that is assigned to peptide bonds in an internal
-helix, with an increase (+2%) in the amide I' involved in the external
-helix, but a 2% change is close to the repeatability error of the experiment (Lecomte et al., 2001
). On the other hand, the adsorption of cyt-c on DOPG vesicles increased the H/2H exchange, since 92% of the NH groups of cyt-c bound to DOPG vesicles were exchanged after 5 h.
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Binding of cyt-c and cyt-c552 to a hydrophobic surface
cyt-c was deposited on self-assembled monolayers of alkylsilanes on silicon to determine the change in cyt-c structure that occurred when it was adsorbed onto a pure hydrophobic surface. Fig. 6 A shows the difference between the secondary structure of a monolayer of cyt-c adsorbed onto the hydrophobic OTS surface and that of cyt-c in solution. The changes were much greater than those involved in binding to DOPG vesicles (see Table 3). The adsorption onto an alkyl chain drastically modified the amide groups involved in
-helix structures. Forty-four percent of the amide groups in solvated cyt-c were involved in internal or external
-helix structures, but only 32% of them were involved in
-helices when the protein was adsorbed onto OTS, with more amino acids implicated in ß-turns (+4%) or in protein self association (+5%) and in random domains (+2%). These changes involved at least 12% of the backbone, corresponding to 1012 residues. The percentage of residual NH of cyt-c adsorbed onto the OTS surface after 5 h was also very small (3%) compared to 15% of residual NH for cyt-c in solution. Most of the amide groups were exchanged by 2H2O, indicating a large change in the tertiary structure of the protein. Thus the adsorption of cyt-c onto alkyl chains modifies its secondary and tertiary structures, resulting in the spreading of cyt-c adsorbed onto the hydrophobic surface because of unfolding of the protein and increased self-association.
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2030%, whereas the band intensities at 1660 cm1 and 1638 cm1 decreased to 6%. At least 15% of the peptide backbone of cyt-c552 was modified by adsorption onto OTS. These changes can be attributed to the formation of ß-strand/turn structures, unfolding of part of the
-helix structure and a loss of hydrated random-coil domains. Analysis of the amide II bands indicated that the tertiary structure of the cyt-c552 was greatly altered when it was adsorbed onto alkyl chains. The adsorption allows the diffusion of 2H2O into buried domains, as reflected by the low final percentage of residual NH (8%). | DISCUSSION |
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The nature of the interactions between eukaryotic c-type cytochrome and DOPG vesicles has been described by several authors (De Meulenaer et al., 1997
; Heimburg and Marsh, 1993
; Morse and Deamer, 1973
; Muga et al., 1991
; Quinn and Dawson, 1969
). The forces driving the interaction of the eukaryotic cyt-c and negatively charged lipid are mainly electrostatic (Kostrzewa et al., 2000
; Muga et al., 1991
; Salamon and Tollin, 1996a
). Such an electrostatic interaction between the positively charged residues and the negatively charged headgroups of DOPG explains the strong binding of cyt-c to DOPG. The horse heart cyt-c has the typical positively charged front surface, in which a cluster of lysine residues surround the exposed heme edge (Buschnell et al., 1990
) (see Fig. 7 A). Cytochrome c seems to bind to the DOPG vesicles via the heme side of the protein. A recent paper has demonstrated that Lys-86, Lys-87, and Lys-72 are involved in the cyt c-membrane (DOPG) interaction (Kostrzewa et al., 2000
). However, some authors have reported that cytochrome c can also become inserted into the lipid bilayer of DOPG vesicles (Cortese et al., 1998
; Pinheiro and Watt, 1994
; Zuckermann and Heimburg, 2001
). The FTIR-ATR experiments were performed to determine how the secondary structures of the two cytochromes interact with a hydrophobic solid surface. The secondary structure of horse heart cytochrome c changes greatly, mainly due to unfolding of
-helix to form hydrated ß-strands or turns associated with the high degree of NH/N2H exchange. The rate of cyt-c adsorption onto the OTS surface reveals that a compact monolayer of cyt-c molecules is formed (results not shown). The protein also aggregates, as revealed by the increase in the band at 1616 cm1. All of these modifications are corroborated by the high degree of NH/N2H exchange and indicate considerable denaturation of the cyt-c adsorbed onto the hydrophobic surface. Although it is quite difficult to define a specific binding domain on the original structure, two external
-helices (Val-3 and Gly-6; Phe-10 and Lys-13) containing hydrophobic residues could be implicated in the interaction with the hydrophobic surface. The orientation of these two fragments toward the absorbent surface causes a loss of
-helix. The extensive unfolding of cyt-c adsorbed onto the hydrophobic surface is consistent with a majority of a nonnative forms (5cHS) of the heme detected by surface-enhanced resonance Raman spectroscopy (Rivas et al., 2002
).
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Cyt-c552 also has a strong affinity for DOPG vesicles, but the structure of this protein differs from that of eukaryotic cytochrome c. Cyt-c552 has only uncharged residues around the exposed heme edge, unlike a typical c-type cytochrome (Than et al., 1997
) (see Fig. 7 B). The lysine and arginine residues are located on the back side of the heme, where several carbonyl side chains are also situated, creating negative potential at the center, top, and bottom of the back side. The binding of cyt-c552 on DOPG vesicles can be also explained by electrostatic interaction between the lysine residues and the negatively charged headgroups of the lipid. The exposed heme edge is surrounded by many hydrophobic residues and this part of the protein is almost totally uncharged (Fig. 7 B). The adsorption of cyt-c552 onto a purely hydrophobic surface also results in major changes in its secondary structure, but they are different from the changes undergone by cyt-c. The global content of structured regular domains is increased by 4% with the formation of ß-structures. The secondary structure of cyt-c552 adsorbed onto talc undergoes similar changes (Lecomte et al., 2001
). The specific orientation of the cyt-c552 adsorbed onto hydrophobic surfaces occurs without the protein spreading. This is consistent with the low content of self-associated domains (band at 1616 cm1; Table 4); they are quite similar in cyt-c552 in solution and the protein adsorbed onto DOPG vesicles or the OTS. The domains that are modified by the hydrophobic surface are different from those involved in horse heart cyt-c. The crystal structure of cyt-c552 reveals two hydrophobic regions on the front surface close to the heme (Than et al., 1997
). These are both candidates for the interaction with OTS surface. One domain involves the hydrophobic ß-strands (Gly-19Pro-27) close to the enlarged ß-strands (Met-63Leu-75) and the second is the N-terminal helix (Ala-2Ala-9). This terminal peptide segment includes several alanine and isoleucine residues which can easily be oriented toward the hydrophobic OTS surface. The N-terminal segment is close to the reserved Met-63Leu-75 ß-strand and includes an
-helical portion which, if it changed to a ß-sheet, would contribute to the formation of a more extended ß-sheet domain. These changes in secondary structure could account for the increase in ß-sheet at the expense of
-helical structure that occurs when the protein binds to the OTS surface. The opening of the ß-strand could also explain the large exchange of NH/N2H. The secondary structure of cyt-c552 bound to DOPG vesicles does not seem to change much, according to the FTIR experiments. The change is much less than that occurring when the protein is bound to a pure hydrophobic surface. However, a purely electrostatic interaction with DOPG vesicles cannot explain the great aggregation that occurs at a low L/P ratio. This could imply that cyt-c552 also becomes inserted into bilayers via hydrophobic interactions. The hydrophobic ß-sheet surrounding the heme may act as an anchor in the vesicle. This local interaction involving a few amino acid residues would not be detected by the global FTIR analysis. The very small changes occurring when cyt-c552 is adsorbed onto DOPG vesicles are at the limit of the accuracy of our method. The positively charged residues can still interact with the negatively charged phosphatidyl headgroups via electrostatic interaction. The coexistence of electrostatic and hydrophobic interactions could explain the low cyt-c552/DOPG ratio at which flocculation occurs. Cyt-c552 could form bridges between DOPG vesicles.
| CONCLUSION |
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However, the turbidity experiments detected differences in their behavior when binding to DOPG vesicles; the cytochrome c formed multilayers on the surface of the DOPG vesicles, whereas the cyt-c552 caused the DOPG vesicles to aggregate even when their surfaces were not completely covered by protein. These features show the different stabilities of the two cytochromes in their interactions with DOPG vesicles. The binding of cyt-c to DOPG vesicles involves mainly electrostatic interactions. Cyt-c is greatly unfolded when it is adsorbed onto a purely hydrophobic surface, so there are hydrophobic interactions or cyt-c becomes inserted into the liposome. In contrast, the binding of cyt-c552 to DOPG vesicles is more complex. Electrostatic interactions cannot solely explain the extensive aggregation of DOPG vesicles covered by only a few molecules of protein. However, a purely hydrophobic interaction during cyt-c552 binding should cause more folding in a ß-structure. The spectral features of cyt-c552 adsorbed onto DOPG vesicles are similar to those seen when it is adsorbed onto hydrophobic surface, but this does not exclude hydrophobic interactions or maintain their prevailing with respect to electrostatic ones. The interactions of cytochrome c and cytochrome c552 with charged lipid membranes and hydrophobic surfaces are different, raising the question of how the functions of the two proteins differ.
| FOOTNOTES |
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Submitted on March 11, 2003; accepted for publication February 20, 2004.
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