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. 2011 Mar 9;133(9):2824-7.
doi: 10.1021/ja1099775. Epub 2011 Feb 14.

Helical hairpin structure of influenza hemagglutinin fusion peptide stabilized by charge-dipole interactions between the N-terminal amino group and the second helix

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Helical hairpin structure of influenza hemagglutinin fusion peptide stabilized by charge-dipole interactions between the N-terminal amino group and the second helix

Justin L Lorieau et al. J Am Chem Soc. .

Abstract

The fusion domain of the influenza coat protein hemagglutinin HA2, bound to dodecyl phosphocholine micelles, was recently shown to adopt a structure consisting of two antiparallel α-helices, packed in an exceptionally tight hairpin configuration. Four interhelical H(α) to C═O aliphatic H-bonds were identified as factors stabilizing this fold. Here, we report evidence for an additional stabilizing force: a strong charge-dipole interaction between the N-terminal Gly(1) amino group and the dipole moment of helix 2. pH titration of the amino-terminal (15)N resonance, using a methylene-TROSY-based 3D NMR experiment, and observation of Gly(1 13)C' show a strongly elevated pK = 8.8, considerably higher than expected for an N-terminal amino group in a lipophilic environment. Chemical shifts of three C-terminal carbonyl carbons of helix 2 titrate with the protonation state of Gly(1)-N, indicative of a close proximity between the N-terminal amino group and the axis of helix 2, providing an optimal charge-dipole stabilization of the antiparallel hairpin fold. pK values of the side-chain carboxylate groups of Glu(11) and Asp(19) are higher by about 1 and 0.5 unit, respectively, than commonly seen for solvent-exposed side chains in water-soluble proteins, indicative of dielectric constants of ε = ∼30 (Glu(11)) and ∼60 (Asp(19)), placing these groups in the headgroup region of the phospholipid micelle.

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Figures

Figure 1
Figure 1
pH titration of the N-terminal amino 15N resonance of Gly1 with the HACAN CH2-TROSY experiment. (A) Superimposed small regions of 1H/15N cross sections taken through the 3D CH2-TROSY HACAN spectrum of HAfp23, showing the correlation between the Gly1 1Hα2/1Hα3 and amino 15N chemical shifts. (B) The Gly1 backbone amino 15N (black) and 13Cα (red) chemical shift dependence on pH is shown. A non-linear least-squares regression was used to fit the Henderson-Hasselbalch equation to the titration curves. The fitted values are: pK = 8.73±0.07, 15N and 13Cα chemical shifts of 27.0±0.6. ppm and 44.3±0.1 ppm, respectively, for the protonated form (NH3+), and 13.6±0.4 ppm and 46.8±0.1 ppm, respectively, for the deprotonated form (NH2). The fitted pK value when measuring the Gly1 13C′ shift on a separate sample (Fig. 2) is 8.84±0.05.
Figure 2
Figure 2
Changes in the 13C′ chemical shifts on titrating the amino group of Gly1. (A) Superimposed small regions of cross-sections taken through the 3D HCACO spectra of HAfp23, recorded at pH values ranging from pH 7.09 to 9.62, with 13C′ chemical shift changes summarized in (C). The Gly8 13C′ chemical shifts could not be identified uniquely due to spectral congestion and are not reported. (B) pH dependence of Gly1 13C′ (green, right axis) and 13C′ chemical shifts of various residues near the end of helix 2. Reported chemical shift changes are relative to values measured at pH 7.09. Traces shown represent nonlinear regression fits to the Henderson-Hasselbalch equation, yielding: Δδ = 7.1±0.2 ppm and pK = 8.84±0.05 for Gly1; Δδ = −0.08±0.02 ppm and pK = 8.9±0.2 for Ile18; Δδ = −0.46±0.02 ppm and pK = 8.84±0.09 for Gly20; Δδ = −0.35±0.06 ppm and pK = 8.9±0.2 for Trp21; Δδ = +0.37±0.04 ppm and pK = 8.87 ±0.10 for Gly23.
Figure 3
Figure 3
Chemical shift titrations of the carboxylate groups of Glu11 and Asp19. (A) Superimposed small regions of cross sections taken through the 3D HCCO spectra taken over the range from pH 6.5 to 2.9, showing the correlation between the carboxylic acid 13C and its vicinal methylene 1H chemical shifts. Chemical shift versus pH for (B) the Glu11 side chain 13Cδ (black) and 13Cγ (red), and (C) the Asp19 side chain 13Cγ (black) and 13Cβ (red) are fit to the Henderson-Hasselbalch equation using non-linear least-squares regression. Fitted values for (B) are: pK = 5.31±0.01, with 13Cδ and 13Cγ chemical shift of 179.2 ppm and 33.0 ppm, respectively, for the protonated form (COOH), and a 13Cδ and 13Cγ chemical shift of 183.2 ppm and 36.3 ppm for the deprotonated form (COO). Fitted values for Asp19 are: pK = 4.35±0.02, with 13Cγ and 13Cβ chemical shift of 175.5 ppm and 37.1 ppm, respectively, for the protonated form, and 13Cγ and 13Cβ chemical shifts of 178.8 ppm and 40.3 ppm for the deprotonated form (COO).

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