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1 Graduate Program in Biophysics, University of Wisconsin, Madison, Wisconsin 53706, USA
2 Department of Chemistry, University of Wisconsin, Madison, Wisconsin 53706, USA
Reprint requests to: S.H. Gellman, Department of Chemistry, University of Wisconsin, 1101 University Avenue, Madison, WI 53706, USA; e-mail: gellman{at}chem.wisc.edu; fax: (608) 265-4534.
(RECEIVED September 9, 2003; FINAL REVISION November 21, 2002; ACCEPTED November 22, 2002)
Article and publication are at http://www.proteinscience.org/cgi/doi/10.1110/ps.0232103.
| Abstract |
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1 nM). This dimerization was proposed to occur via antiparallel ß-sheet formation between the Lys7-Phe11 segments in each HA molecule. We conducted biophysical studies on synthetic HA in order to gain insight into its structure and aggregation tendencies. We found by analytical ultracentrifugation that HA is monomeric at low millimolar concentrations. Studies by 1H-NMR revealed that HA did not adopt any significant secondary structure in solution. We found no NOEs that would support the proposed dimer structure. We probed the propensity of the Lys7-Phe11 fragment to form antiparallel ß-sheet by designing peptides in which two such fragments are joined by a two-residue linker. These peptides were intended to form stable ß-hairpin structures with cross-strand interactions that mimic those of the proposed HA dimer interface. We found that the HA-derived fragments may be induced to form intramolecular ß-sheet, albeit only weakly, when linked by the highly ß-hairpin-promoting D-Pro-Gly turn, but not when linked by the more flexible Gly-Gly unit. These findings suggest that the postulated mode of HA dimerization and the proposed propensity of the molecule to form discrete aggregates with high affinity are incorrect. Keywords: Neuropeptide Head Activator; ß-sheet; ß-hairpin; equilibrium analytical ultracentrifugation
| Introduction |
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1 nM; Bodenmuller et al. 1986), which led to the hypothesis that inactivation at higher concentrations is due to self-association.
Previous attempts at conformational characterization of HA suggested that the molecule contains considerable ß-sheet structure (Bodenmuller et al. 1986; Saffrich et al. 1989; Fuentes et al. 1994). This hypothesis is unusual given that small linear peptides are generally too flexible to adopt well defined conformations in aqueous solution (Wright et al. 1988; Creighton 1996). Bodenmuller et al. (1986) proposed that homodimerization of the peptide occurs via an antiparallel sheet-like interaction. At the proposed dimer interface, residues Lys7 through Phe11 of one HA molecule are postulated to form an extended antiparallel ß-sheet with the same residues of a second HA molecule (Fig. 1A
). The dimerization is supposedly driven by intermolecular hydrophobic interactions between sidechains on opposing strands and by a symmetrical pair of salt bridges between Lys7 of one HA molecule and the C-terminal carboxylate of the other.
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| Results and Discussion |
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Figure 1A
shows the postulated mode of dimerization in which residues Lys7 though Phe11 of one HA molecule form an antiparallel two-stranded ß-sheet with the same residues of another HA molecule. We hypothesized that these interactions could be mimicked in an intramolecular fashion (Fig. 1B
), and the validity of the proposed dimer interface could be tested by probing the propensity of the resulting peptide to form a ß-hairpin. This configuration could be achieved by linking two segments corresponding to the C-terminal five residues of HA with a dipeptide loop. The propensity of the resulting peptides to form ß-hairpins is easily evaluated using biophysical techniques and provides a strategy to detect interactions without complications due to nonspecific aggregation. Peptides (HA-f)2-GG and (HA-f)2-pG were designed in this fashion. Fragments of HA were linked with either a flexible Gly-Gly loop [(HA-f)2-GG has the sequence +NH3-RRGSKVILF-GG-KVILF-CO2-], or a ß-hairpin-promoting D-Pro-Gly loop [(HA-f)2-pG has the sequence +NH3-RRGSKVILF-pG-KVILF-CO2-, where the lowercase letter denotes D absolute configuration]. An Arg-Arg-Gly-Ser segment was included at the N-termini of these peptides to improve solubility and discourage aggregation. The C-termini were left free to allow a potential electrostatic interaction between the carboxy group and the Lys5 sidechain on the opposing strand. A similar interaction is postulated to be important for HA dimerization (Bodenmuller et al. 1986).
A ß-hairpin with specific residue interactions mimicking those of the proposed interface could be envisioned if the Gly-Gly linker region and flanking residues of (HA-f)2-GG adopted a 2:2 ß-hairpin loop (see Fig. 1
; Sibanda et al. 1989). ß-Hairpin formation with this type of loop, in which the two loop residues correspond to residues i+1 and i+2 of a ß-turn, would maintain the registry of the hydrogen bond network of the postulated intermolecular HA dimer interface and would allow the same specific interactions that are proposed to stabilize the HA dimer. Peptide (HA-f)2-pG is very similar to (HA-f)2-GG, but the flexible Gly-Gly linker has been replaced by the highly hairpin-promoting D-Pro-Gly linker. The D-Pro-Gly segment strongly favors formation of type I and type II ß-turns (as residues i+1 and i+2). These unusual types of ß-turn are commonly observed at the loops of 2:2 ß-hairpins in proteins (Wilmot and Thornton 1988). The D-Pro-Gly segment has been shown to promote ß-hairpin formation in several short designed peptides (Haque et al. 1996; Haque and Gellman 1997; Stanger and Gellman 1998; Das et al. 2001). Furthermore, the incorporation of D-Pro into reverse turns has also been employed in several instances to stabilize antiparallel ß-sheet interactions between short strand segments derived from natural proteins outside the context of the natural tertiary structure (Struthers et al. 1996; Haque and Gellman 1997; Espinosa and Gellman 2000; Kaul et al. 2001). The Gly-Gly segment in (HA-f)2-GG endows the linker with high flexibility, and any ß-hairpin structure observed for (HA-f)2-GG would be attributable largely to the propensity of the strand segments to form cross-strand contacts that mimic those of the postulated HA dimer interface. In contrast, the D-Pro-Gly segment of (HA-f)2-pG strongly promotes formation of the ß-hairpin by enforcing an appropriate reverse turn. In this case, even modest interstrand contacts should be sufficient to induce folding. The ß-hairpin configurations of the designed peptides that would mimic the proposed HA dimer interface are presented in Figure 1B
.
Aggregational and conformational tendencies of HA and HA-f
Equilibrium analytical ultracentrifugation (AU) at concentrations of 1.0 mM and 1.3 mM in aqueous 50 mM acetic acid, pH 5.0, revealed that HA was predominantly monomeric under these conditions (Fig. 2
). The observation that HA is monomeric at low millimolar concentrations contradicts earlier conclusions based on molecular sieve chromatography, in which HA was thought to elute predominantly as a dimer at concentrations as low as 10-11 M (Bodenmuller et al. 1986). In these initial studies, the dimer was thought to be stable under aqueous buffering conditions such as 0.01 M to 0.1 M Tris (pH 7.5) containing 0.1 M NaCl [the authors reported that extremely harsh conditions such as 1 M (NH4)SO4 or boiling the peptide in 0.1 M HCl were required to obtain exclusively monomeric HA]. Although our analysis of HA was performed at pH 5.0, we conclude that there are no differences in conformation or aggregation state between our sample and that previously analyzed by NMR at pH 7.2 by Saffrich et al. (1989) because the chemical shifts are identical (discussed below). From our AU studies, we observe no traces of a discrete HA dimer with high association affinity.
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The 1H-NMR spectra for HA were well resolved, and full TOCSY (Bax and Davis 1985) spin-system assignments were achieved using NOESY (Jeener et al. 1979) and ROESY (Bothner-By et al. 1984) experiments (complete chemical shift assignments are found in the Supplemental Material). The observed 1H chemical shifts for HA were in excellent agreement with previous NMR analysis of HA (Saffrich et al. 1989). The maximum chemical shift differences were 0.01 ppm, that is, within experimental uncertainty, for all amide protons and
-protons [these types of protons are highly sensitive to secondary structure (Wishart et al. 1991Wishart et al. 1992)]. The similarities in chemical shifts observed for HA with previously reported values for HA suggest that there are no conformational differences between our sample and that analyzed previously in unbuffered aqueous solutions (Saffrich et al. 1989).
Chemical shifts for
-protons of residues in a ß-sheet conformation are generally shifted downfield relative to
-protons of residues in the random coil state, while
H chemical shifts of residues in
-helical conformations are shifted upfield relative to random coil (Wishart et al. 1991Wishart et al. 1992). Three consecutive residues with consistent deviations from random coil larger than 0.1 ppm are considered evidence of secondary structure formation (Wishart et al. 1992). Figure 3A
shows the deviation of observed
-proton chemical shifts from published random coil values [
H(observed) - 
H(random coil); random coil values from Wuthrich 1986] for HA. These data suggest that HA is predominantly in a random coil state under these conditions, a finding that contradicts secondary structural predictions that HA forms 62%67% ß-sheet conformation (Bodenmuller et al. 1986; Fuentes et al. 1994).
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-protons of residues in nonhydrogen-bonded positions on opposite strands (e.g., Val8
H to Leu10
H in Fig. 1A
1 mM), it is unlikely that these NOEs are due to self-association. If these NOEs were due to intramolecular contacts, these data would suggest partial folding of the peptide to a conformation with specific interactions. However, the paucity and low intensity of the nonsequential NOEs suggests that the conformation giving rise to these NOEs is very sparsely populated. These NOE data suggest that the postulated head-to-tail mode of HA dimerization is incorrect.
Evaluation of the proposed HA dimer interface via structural analysis of (HA-f)2-GG and (HA-f)2-pG
Our 1H-NMR analysis provides no indication of significant ß-hairpin formation by (HA-f)2-GG in solution. As shown in Figure 3B
, no systematic deviation of
-proton chemical shifts from random coil values was observed for any region of the peptide. Furthermore, no nonsequential NOEs were observed for (HA-f)2-GG. Geminal
-proton splitting for glycine residues in ß-turns has been used as an indication of ß-hairpin formation (Searle et al. 1999; Griffith-Jones and Searle 2000). For (HA-f)2-GG, the Gly9 protons were split very slightly (36 Hz), and chemical shifts for geminal protons of Gly10 were only moderately different (by 96 Hz). Vicinal 3J
N proton couplings are also frequently used as indicators of secondary structure for proteins and peptides (Serrano 1995; Smith et al. 1996; Griffiths-Jones et al. 1998). Large values (> 8.0 Hz) are indicative of ß-sheet structure, whereas smaller values (< 6.0 Hz) signify helical conformation. Most of the 3J
N could not be determined from the proton 1D-spectrum of (HA-f)2-GG due to poor dispersion; however, of the four values that could be extracted, none was above 8.0 Hz (Ser4, 6.8 Hz; Leu8, 7.7 Hz; Lys12, 7.0 Hz; Phe16, 7.9 Hz). Taken together, these data indicate that (HA-f)2-GG does not adopt the ß-hairpin conformation depicted in Figure 1B
.
NMR evidence suggests that peptide (HA-f)2-pG is at least partially folded into a ß-hairpin, in contrast to (HA-f)2-GG. Several of the
-proton chemical shifts for residues near the turn (Val6Phe9 and Leu12Val13) are suggestive of ß-sheet conformation (Fig. 3B
). In addition, several NOEs consistent with ß-hairpin formation were observed (Fig. 4
), including a long-range interaction between the
-protons of Leu8 and Val13. An additional
-proton-to-
-proton NOE was detected, but this signal could not be assigned unambiguously due to spectral overlap (Leu15
H to either Val6
H or Ile7
H). Two turn-defining NH-to-NH NOEs were also observed, one between the amide protons of Phe9 and Lys12, and another between Gly11 and Lys12. The amide 1H signals were well dispersed, and the majority of the 3J
N that could be resolved were indicative of significant ß-sheet population (Lys5, 7.2 Hz; Ile7, 9.2 Hz; Leu8, 9.1 Hz; Phe9, 7.0 Hz; Lys12, 8.1 Hz; Val13, 7.1 Hz; Ile14, 9.2 Hz; Phe16, 8.0 Hz). The turn glycine geminal
-proton signals were split by 150 Hz. These data suggest that (HA-f)2-pG is at least partially folded in the intended ß-hairpin conformation, particularly in the turn region. This observation implies that the linked HA fragments may be induced to associate in a ß-sheet mode if they are connected by a linker with a high turn propensity. However, this effect results in a ß-hairpin that is only moderately stable, indicating that the cross-strand interactions are relatively weak. Based on the behavior of (HA-f)2-GG and (HA-f)2-pG, we conclude that the potential for interaction between the two HA-derived fragments exists, but that this interaction would not be adequate to drive dimerization at low concentration. Furthermore, we conclude that the postulated mode of HA dimerization and the strength of the aggregation as earlier reported are incorrect.
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| Materials and methods |
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Equilibrium analytical ultracentrifugation (AU)
Samples were prepared by dissolving the pure lyophilized peptides, isolated as the TFA salt, to the appropriate concentration in aqueous 50 mM acetic acid, pH 5.0. Equilibrium ultracentrifugation studies were conducted on a Beckman XLA ultracentrifuge at 297 K. Cells with 1.2 cm pathlengths were used, and the absorbance was monitored at 257 nm. Analysis was performed at several rotor speeds ranging from 40 to 60 krpm. Data were acquired with a 0.001 cm step size at each speed every 4 h until three consecutive spectra were identical. Linear least-squares fitting was performed in accordance with the equation d (ln c)/d r2 = M(1-
)
2/2RT, where d (ln c)/d r2 is the slope of a ln(Absorbance) versus (Radial Distance)2 plot,
is the partial specific volume,
is the solvent density,
is the rotor speed, R is the gas constant, and T is temperature (Cantor and Schimmel 1980; Schuster and Laue 1994). Molecular weight estimates were determined from the parameter M. A partial specific volume of 0.786 mL g-1 for HA was calculated by the method of Durchschlag and Zipper (1994). A solvent density of 0.99885 g mL-1 was determined at 297 K using an Anton Parr DMA 5000 density meter.
Nuclear magnetic resonance (NMR)
NMR samples were prepared by dissolving the lyophilized peptides to
1 to 2 mM in 10% D2O/90% H2O or pure D2O, containing 100mM acetic acid-d6, pH 5.0 (uncorrected). Spectra were acquired on a Varian INOVA 600 MHz spectrometer at probe temperatures ranging from 277 K to 303 K as necessary to resolve resonance overlap. A 7000 Hz spectral window was used for all acquisitions, with 80 msec, 200 msec, and 200 msec mix times for TOCSY (Bax and Davis 1985), ROESY (Bothner-By et al. 1984), and NOESY (Jeener et al. 1979) experiments, respectively. Solvent suppression in the TOCSY and ROESY spectra was achieved using a selective presaturation pulse, and in NOESY with the WET method (Ogg et al. 1994; Smallcombe et al. 1995). Typical data sets consisted of 500 to 600 free-induction decay increments of 16 to 24 transients each (corresponding to 2048 to 4096 points in f2). All spectra were processed in standard Varian software, and referenced to internal 4,4-dimethyl-4-silapentane-1-sulfonic acid (DSS) standard. Although analytical ultracentrifugation was not performed on (HA-f)2-GG or (HA-f)2-pG, we assume that NMR studies on these peptides were conducted under nonaggregating conditions, because a 10-fold dilution of the NMR samples yielded identical one-dimensional spectra. It is unlikely that these peptides would aggregate below this concentration range (0.1 to 0.2 mM) due to their high charge density (overall charge at pH 5.0 should be +4).
| 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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