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1 Amgen, Inc., Thousand Oaks, California 91320, USA
2 Instituto di Biofisica, C.N.R., 56010 Pisa, Italy
Reprint requests to: Bruce A. Kerwin, Ph.D., Amgen, Inc., One Amgen Center Drive, Mail Stop 21-A, Thousand Oaks, CA 91320; e-mail: bkerwin{at}amgen.com; fax: (805) 375-5794.
(RECEIVED March 29, 2002; FINAL REVISION April 22, 2002; ACCEPTED April 22, 2002)
Article and publication are at http://www.proteinscience.org/cgi/doi/10.1110/ps.0208102.
| Abstract |
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Keywords: PEG; polyethylene glycol; soluble tumor necrosis factor receptor; phosphorescence; viscosity
Abbreviations: sTNF-RI, soluble tumor necrosis factor receptor PEG, polyethylene glycol MPEG, methoxypolyethylene glycol NATA, N-acetyltryptophanamide EDC, ethylenediamine carbodiimide HPLC, high pressure liquid chromatography
| Introduction |
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Despite its numerous applications, the molecular bases for its action are not always understood and, therefore, its behavior on individual protein systems is largely unpredictable. According to solution studies on model proteins, the polymer, owing to its size, tends to be excluded from the protein surface (Lee and Lee 1981; Bhat and Timasheff 1992), a process known as preferential exclusion. The addition of PEG to protein solutions then will increase the free energy of the system causing the polypeptide to adopt a more compact globular shape that minimizes the surface area exposed to the solvent (Lee and Lee 1981; Bhat and Timasheff 1992). This effect of molecular crowding by the polymer is expected to prompt polypeptides to fold and associate, the latter reaction leading eventually to phase separations in which proteins either precipitate (Atha and Ingham 1981) or crystallize (McPherson 1976) out of the solution.
For any given protein, however, the degree of preferential exclusion will be influenced also by the balance between repulsive interactions with surface charges and attractive interactions with hydrophobic, nonpolar patches. The latter clusters have been found to be composed of the side-chains of Trp, Phe, and Leu (Sasahara and Uedaira 1993) and the methylene backbones of ionizable amino acids such as Asp, Arg, and Lys (Furness et al. 1998). In general, PEG binding is weak (e.g., Kd = 76 mM, between PEG and Trp-62 of lysozyme (Furness et al. 1998) but can become stronger following large structural changes exposing previously buried hydrophobic residues, such as in the case with the molten globule state (Cleland and Randolph 1992) or denatured proteins (Lee and Lee 1987).
Beyond these broad considerations, our understanding of the molecular details governing protein-PEG interactions or the polymer influence on the conformation of the macromolecule is still inadequate. In particular, little is known about the factors that preside over PEG binding to specific protein sites and, more generally, on the effects that free or covalently bound PEG may have on the structure of folded proteins. Perturbations of the native fold may arise from proximity or direct contact with the polymer, replacing or altering the aqueous interface, as well as from PEG conjugation to specific, Cys (Kuan et al. 1994), or N terminus (Kinstler et al. 1996) protein sites. A largely unanswered question in the field of protein PEGylation is to what extent altered immunogenic response or macromolecular recognition is the result of modifications of the native protein conformation. The fact that PEG-induced structural changes have not been detected by common spectroscopic methods, which are mostly sensitive to changes in secondary structure, suggests that any perturbation is probably subtle and limited to the tertiary and quaternary structure.
This report attempts to address these issues by employing sTNF-RI as a model protein system. The full length polypeptide is composed of 162 amino acids arranged as an elongated (2.5 nm x 7.5 nm) ß-sheet, cross-linked by 10 disulfide bonds spread along the length of the macromolecule (Rodseth et al. 1994; Naismith et al. 1996) (Fig. 1
). The macromolecule contains a single, partially exposed Trp residue at position 107 that, together with nearby Phe-115, Tyr-106, and Leu-111, forms a hydrophobic/aromatic cluster with PEG-binding propensity. In this paper, we report that free PEG binds specifically to a truncated form of sTNF-RI. The interaction, which is absent in the full length protein, 4D sTNF-RI (Solorzano et al. 1998), was found to be sharply modulated by pH and to be for the most part attenuated when PEG was conjugated to the N terminus, a site far removed from the putative binding site. Taking advantage of the fine sensitivity of Trp phosphorescence to the nature and to the dynamic features of the Trp environment (Gonnelli and Strambini 1995; Strambini and Gonelli 1995; Cioni and Strambini 1998), it was found that an increased plasticity of the local structure plays an important role in conferring PEG-binding selectivity to the truncated protein. Most significantly, while protonation of a nearby His apparently is responsible for pH modulation of the binding interaction, an attenuated affinity for the free polymer following conjugation with PEG at the far N terminus was associated to subtle changes in conformation about the aromatic cluster.
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| Results |
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The phosphorescence spectrum obtained in low-temperature (140 K) glasses is related to the polarity of the Trp environment, while the bandwidth of the 0,0 vibronic band reports on its structural homogeneity. The spectral energy of Trp-107 (Fig. 4
) was indicative of a polar matrix similar to the aqueous solvent. However, the emission bandwidth of the 0,0 vibronic band was significantly smaller (5.4 nm) than for fully solvent-exposed residues (8.5 nm). Likewise, spectral invariance with respect to the excitation wavelength indicates homogeneity in ground-state energy and again excludes substantial solvation of the indole ring. Overall, the spectrum indicated that Trp-107 is located in a relatively polar but conformationally restricted environment. These spectral features were common to 2.6D and full-length sTNF-RI, and were invariant to PEGylation or pH from 4.510.
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1.3 nm, and again independent of truncation, pH, or PEGylation. From the correlation between spectral shift and degree of solvent exposure, it was estimated that
80% of the indole ring surface was not in contact with the mobile solvent. That is in fair agreement with the crystallographic structure of full-length sTNF-RI, in which only the carbon atoms CE3, CZ3, CH2, and CE2 of the indole ring can contact the solvent with the remainder of the structure being inaccessible (Naismith et al. 1996).
The static accessibility of Trp-107 to the aqueous solvent can be inferred from the decrease in phosphorescence lifetime caused by heavy-atoms species, like I-, relegated to the aqueous medium (Li et al. 1989). In glasses, the phosphorescence lifetime of Trp-107 was 6.4 sec. This value is typical of Trp residues not perturbed by the proximity of disulfides, which are numerous in sTNF-RI. In the presence of I-, the emission is considerably shorter-lived and heterogeneous (Fig. 5
), the multiplicity in phosphorescence lifetimes reflecting the random, static distribution of Trp-107-iodide distances. The accessibility of the indole ring to I- was estimated from the reduction in the average lifetime of Trp-107 relative to that of NATA free in solution (Table 1
). For the 4D sTNF-RI, the phosphorescence lifetime was about 2.3 times greater, at both pH 4.5 and 7.4, than for the free chromophore confirming substantial shielding of the aromatic ring from the solvent. The I-effect for truncated 2.6D sTNF-RI was similar to 4D sTNF-RI at acidic pH, but increased significantly on raising the pH to neutrality. PEGylation enhanced the interaction with I-, the effect increased with the molecular weight of PEG. In this case, the I- effect was similar at both acidic and neutral pH. The increased I- accessibility of the 2.6D sTNF-RI observed on raising the pH or subsequent to PEGylation reports subtle variations in the environment of Trp-107. These changes are consistent with either an increased exposure of the indole ring to the solvent and/or a more positive (attractive for I-) surface potential.
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= 1/
0 + kq[acrylamide],
0 the unperturbed lifetime) (Cioni and Strambini 1998). For the 2.6D sTNF-RI, a magnitude of kq = 9.6 ± 0.5 x 108 M-1s-1, similar to that for free Trp (kq = 1.3 x 109 M-1s-1), confirmed the superficial location of the aromatic ring, if not its partial exposure to the aqueous solvent. Relative to the 2.6D sTNF-RI, acrylamide quenching decreased nearly twofold in the 4D sTNF-RI. This implies that following truncation of the polypeptide, Trp-107 becomes more accessible to solvent-mediated interactions through either a better exposure of the aromatic ring to the solvent or increased mobility of the local protein structure. Interestingly, PEGylation of 2.6D sTNF-RI, with 2 kD, 5 kD, and 20 kD PEG offered little protection (a 10% reduction of kq) against quenching. This suggests that the greater iodide effect induced by PEGylation is likely because of an increased polarity of the region rather than a greater exposure of the indole ring to the solvent.
In fluid-aqueous solutions, the phosphorescence lifetime of Trp (
0) is drastically reduced by the motional freedom of the protein-solvent matrix surrounding the chromophore (Strambini and Gonelli 1995). Beyond this effect of matrix dynamics,
0 can be decreased further by internal quenching interactions with Cys, His, and Tyr side-chains coming in contact with the chromophore (Gonnelli and Strambini 1995). For all sTNF-RI forms, the phosphorescence decay in buffer at neutral pH was short-lived and remarkably nonuniform (Fig. 6
). The magnitude of phosphorescence lifetimes,
i, amplitudes,
i, and the average phosphorescence lifetime,
av = 
i
i, are reported in Table 2
. For the 2.6D sTNF-RI, a major fraction (84%) of the sample has a
shorter than that exhibited by highly flexible, unstructured peptides (
= 200250 µs) (Gonnelli and Strambini 1995). This demonstrates that in sTNF-RI,
is largely dominated by intramolecular quenching reactions. The X-ray structure points out that the imidazole of His-105 is perpendicular to and within interaction range (3.6 Å) of the indole ring of Trp-107 (Fig. 1
). His quenching can be discriminated from other reactions by the pH dependence of
in that its protonation is known to enhance up to 50-fold its quenching efficiency (Gonnelli and Strambini 1995). The lifetime pH profile of 2.6D sTNF-RI (Fig. 7
) confirmed a sharp decrease of
av at acid pH, the transition midpoint being around the expected pKa (66.5) of His. Both the acid transition and the pKa value strongly indicate proximal His-105 as the quencher of phosphorescence.
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av is largely independent of pH (Fig. 7
av (Table 2| Discussion |
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As in the 4D protein, the indole ring of 2.6D sTNF-RI is not fully available for an interaction with the polymer (being still largely shielded from the aqueous phase); the conformational plasticity of the local structure is probably crucial to permit, through an induced-fit type mechanism, a strong association between aromatic ring and polymer. The crystallographic structure of the 4D sTNF-RI (Naismith et al. 1996) predicts an indole ring with a restricted mobility and moderate exposure to the aqueous solvent. The relatively high phosphorescence spectral resolution (BW), ground-state homogeneity, and limited spectral relaxation agree with an ordered, rigid local structure where the indole ring is largely shielded from the solvent. Truncation of the C-terminal part of the polypeptide affects neither the side-chain configuration about Trp-107 nor the secondary and tertiary structures of the remaining 2.6D portion (FT-Raman and FTIR data not shown).
The main effects of truncation are an increased fluidity of the Trp environment with greater accessibility of the indole ring to solvent-mediated interactions and pronounced intramolecular phosphorescence quenching at acidic pH. A greater flexibility of the 2.6D fragment, relative to the parent macromolecule, is inferred from both a shorter phosphorescence lifetime (Table 2
) and the twofold increase in the acrylamide-quenching constant. On the other hand, the acid transition in the lifetime pH profile of 2.6D sTNF-RI emphasizes efficient quenching by neighboring His-105 in the protonated state, as the pH profile is similar to that observed for His titration (pKa = 6.6) (McNutt et al. 1990). It is significant that the acid transition is practically abolished in the full-length protein as it suggests that effective indole-imidazole quenching geometries are not attained in this case, presumably through restricted mobility of the side-chains. We note that the direct interaction between PEG and Trp-107 also provides a simple switch mechanism for the pH modulation of PEG binding. When His-105 is protonated, the imidazole ring can form a strong complex with indole (Loewenthal et al. 1992) and lead to partial withdrawal of the ring from the aqueous phase at acidic pH. A greater accessibility of Trp to the solvent at neutral/alkaline pH also is consistent with a larger I-effect (Table 1
).
Effects of PEGylation on protein structure
Covalently bound PEG at the N terminus reduces the interaction with the free polymer as it largely abolishes the viscosity enhancement. This occurs without changes to the secondary structure of the protein, as generally observed with other PEGylated proteins (Tuma et al. 1995; Kinstler et al. 1996). In principle, the decreased affinity for free PEG could be ascribed to subtle alterations of the protein conformation at the binding site, or to steric hindrance by bound PEG either shielding the binding site from the solvent or preventing a close approach of the polymer to the protein. Phosphorescence data show that in the conjugated protein, the chromophore is not screened from the solvent as the accessibility of acrylamide is practically unaltered and that of iodide is actually increased. The phosphorescence lifetime and the iodide accessibility of Trp-107 report that PEG conjugated to the N terminus induces a more rigid and polar configuration about the aromatic residue in the far C-terminal region. Thus, both an electrostatic repulsion to PEG as a result of the increased local charge and/or a more rigid local structure (as in the case of the full-length protein) could lead to a decreased affinity for the free polymer.
Steric hindrance by the bulky polymer also may be important. In general, its contribution is difficult to assess because, although it is assumed that covalently bound PEG surrounds the polypeptide, the area occupied by it in relation to the protein is unknown. Assuming a random coil configuration for PEG, the Flory radius estimates that 2 kD, 5 kD, and 20 kD PEGs occupy spheres with diameters of 35, 70, and 153 Å, respectively (Jeppesen et al. 2001). Because the length of 2.6D sTNF-RI is
35 Å, this rough calculation shows that steric interference by attached PEG can play a role in decreasing the interaction between sTNF-RI and free PEG, especially for the larger polymers. However, it may be significant in this respect that steric hindrance does not inhibit the association of PEGylated sTNF-RI to TNF-
(Edwards 1999), although its binding site is close to the N terminus (Banner et al. 1993). Furthermore, the smallest 2 kD PEG is even more effective in inhibiting the interaction with the free polymer than the 10 times bulkier 20 kD PEG.
In the absence of detectable changes in protein structure, steric effects often have been invoked to explain the decreased immunogenicity of some PEGylated proteins (Moreland et al. 2000; Reddy 2000). However, the results with sTNF-RI emphasize the ability of bound PEG to induce subtle changes in the conformation of surface residues in regions remote from the site of PEGylation, effects that may have important consequences for macromolecular recognition and the immunogenic response. Overall, the outcome of the present investigation emphasizes the importance of specific side-chains, surface charges, and structural plasticity in determining the binding affinity between proteins and PEG. Additionally, it demonstrates the ability of conjugated PEG to alter the surface structure of proteins and their interaction with other macromolecules such as may occur with the immune system. The ability to modify localized protein conformation away from the site of PEGylation expands the realm of possibilities for preventing unwanted macromolecular interactions. This will become increasingly important as, with the availability of the human genome, more proteins are brought forth as potential drugs.
| Materials and methods |
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The 2.6D and 4D sTNF-RI were produced at Amgen, Inc. as previously described (Solorzano et al. 1998) and provided by Dr. Jim Seely. PEGylation and purification of the 2.6D sTNF-RI with 2 kD PEG-aldehyde, 5 kD PEG-aldehyde, and 20 kD PEG-aldehyde was achieved through reductive alkylation as previously described (Kinstler et al. 1996).
The viscosity was measured at 26°C using a Haake fallingball micro viscometer. All proteins were fully equilibrated with 20 mM sodium acetate at pH 5.6. The protein concentration was 20 mg/mL for 2.6 D sTNF-RI, 2 kD PEGylated sTNF-RI, 5 kD PEGylated sTNF-RI, and 20 kD PEGylated sTNF-RI. The concentration was increased to 26 mg/mL for 4D sTNF-RI to maintain a constant protein/polymer molar ratio. Solid 20 kD MPEG was added to a final concentration of 50 mg/mL. Measurements were recorded after the system reached equilibrium as judged by a constant viscosity for more than three consecutive measurements. The values are the average of three measurements. Standard deviations were <5% of the value.
Chemical crosslinking was achieved using the following procedure. 2.6D sTNF-RI was equilibrated in 50 mM 2(N-morpholino) ethane sulfonic acid (MES) and diluted to a final concentration of 1 mg/mL. Ethylendiamine carbodiimide (EDC) was added at an EDC to protein ratio of 2:1 and reacted for 4 h at room temperature. Samples were diluted 20-fold with buffer equilibrated at 4°C to stop the reaction. Reaction mixtures were separated using reverse-phase HPLC. An aliquot, 15 µL, of the quenched samples were loaded on a 2.1 x 300 mm Phenomenex Jupiter C4 column equilibrated with 18% acetonitrile/0.1% trifluoroacetic acid at a flow rate of 0.2 mL/min. Protein was eluted with a 1%/min gradient of 90% acetonitrile/0.1% trifluoroacetic acid. The uncrosslinked and crosslinked sTNF-RI was quantified from the A215 of the chromatograms.
Tryptophan phosphorescence was measured on thoroughly deoxygenated samples using a procedure and instrumentation previously described (Strambini and Gonelli 1995). Low-temperature phosphorescence emission spectra were measured in a propylene glycol/buffer (50:50, V:V), at 140 K. The excitation wavelength was 295 nm and the bandwidth was 6 and 1 nm for excitation and emission, respectively. In these glasses, the sTNF-RI concentration was typically 20 µM, in 20 mM sodium phosphate, 100 mM sodium chloride, at the specified pH. Phosphorescence decays in buffer, above freezing temperatures, were obtained using pulsed excitation at 292 nm while the emission was collected through a filter combination transmitting between 410440 nm. All proteins were dissolved at a concentration of 810 µM in a buffer composed of equimolar (2 mM) sodium acetate, sodium phosphate, and sodium carbonate plus 100 mM sodium chloride. The presence of various buffering salts allowed pH variations between 4 and 11. All phosphorescence decays were analyzed in terms of a sum of exponential components by a nonlinear least-squaresfitting algorithm (Global Unlimited, LFD, University of Illinois). The reported lifetime data are averages of two or more independent measurements. The reproducibility of phosphorescence lifetimes was typically better than 5%. Acrylamide-quenching experiments were carried out as described (Cioni and Strambini 1998). The phosphorescence emission of sTNF-RI is intrinsically heterogeneous and remains so even when the average phosphorescence lifetime is considerably reduced by acrylamide. For convenience, lifetime Stern-Volmer plots were all constructed from the average lifetime,
av = 
i
I, obtained in general from a biexponential fit of phosphorescence decays. Consequently, the value of the bimolecular quenching rate kq derived from these plots is an averaged quantity.
| 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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