
Conformational stability of the RNP domain controls fibril formation of PABPN1
Jens Liebold
1Department of Protein Biochemistry, Institute of Biochemistry and Biotechnology, Martin Luther University, Halle Wittenberg, 06120, Halle, Germany
Reno Winter
1Department of Protein Biochemistry, Institute of Biochemistry and Biotechnology, Martin Luther University, Halle Wittenberg, 06120, Halle, Germany
Ralph Golbik
2Department of Virology, Institute of Biochemistry and Biotechnology, Martin Luther University, Halle Wittenberg, 06120, Halle, Germany
Gerd Hause
3Biocenter, Martin Luther University, Halle Wittenberg, 06120, Halle, Germany
Christoph Parthier
4Department of Physical Biotechnology, Institute of Biochemistry and Biotechnology, Martin Luther University, Halle Wittenberg, 06120, Halle, Germany
Elisabeth Schwarz
1Department of Protein Biochemistry, Institute of Biochemistry and Biotechnology, Martin Luther University, Halle Wittenberg, 06120, Halle, Germany
Associated Data
Abstract
The disease oculopharyngeal muscular dystrophy is caused by alanine codon trinucleotide expansions in the N-terminal segment of the nuclear poly(A) binding protein PABPN1. As histochemical features of the disease, intranuclear inclusions of PABPN1 have been reported. Whereas the purified N-terminal domain of PABPN1 forms fibrils in an alanine-dependent way, fibril formation of the full-length protein occurs also in the absence of alanines. Here, we addressed the question whether the stability of the RNP domain or domain swapping within the RNP domain may add to fibril formation. A variant of full-length PABPN1 with a stabilizing disulfide bond at position 185/201 in the RNP domain fibrillized in a redox-sensitive manner suggesting that the integrity of the RNP domain may contribute to fibril formation. Thermodynamic analysis of the isolated wild-type and the disulfide-linked RNP domain showed two state unfolding/refolding characteristics without detectable intermediates. Quantification of the thermodynamic stability of the mutant RNP domain pointed to an inverse correlation between fibril formation of full-length PABPN1 and the stability of the RNP domain.
Introduction
Oculopharyngeal muscular dystrophy (OPMD) is a late onset disease affecting facial muscle functions. The congenital disorder is caused by trinucleotide expansions leading to additional alanines in the N-terminal segment of the nuclear poly(A) binding protein (PABPN1).1 The protein harbors a central RNP (ribonucleoprotein) type RNA binding domain, followed by a 60 residues comprising C-terminal segment that adds to the affinity of PABPN1 for RNA. PABPN1 is an important component during polyadenylation of newly synthesized transcripts and controls processivity of the poly(A) polymerase.2–5
In contrast to CAG (glutamine) trinucleotide expansions with up to 200 glutamines in a row, alanine segments in PABPN1 reported for OPMD patients do not exceed 17 consecutive alanines. The wild-type segment comprises 10 alanines following the start methionine [Fig. 1(A)]. The N-terminal domain fibrillizes in vitro in an alanine-dependent manner.6 These fibrils exhibited an unusual high resistance against solubilization with denaturing agents and showed all features of typical amyloid-like structures. Moreover, fibrils built by the N-terminal domain with the extension of seven additional alanines were even more stable than those derived from the wild-type domain.7 In contrast to the fibrils of the N-terminal domains, fibrils of the full-length protein possessed unrelated properties: in this case, fibril formation was independent of the alanine segment, kinetics of unseeded fibril formation showed nonsigmoidal time courses, fibril formation was not seedable, and finally, the resistance against solubilization with denaturants was not comparable to the high resistance of fibrils from the N-terminal domains,8 for review see Ref.9. From these apparently hardly reconcilable datasets, it was concluded that fibril formation of PABPN1 may occur by two different pathways, an alanine-dependent process triggered by the N-terminal domain and an alanine-independent process which requires further segments of the full-length protein.8

Scheme of the PABPN1 domain contributions and structure of the RNP domain. (A) Constructs described in this publication. The top bar shows the domain structure of PABPN1. Numbers are given for start and end amino acid of structural regions. Thick, colored bars show protein constructs described in this publication. Alanine stretch (dark gray), N-terminal domain (gray), α-helical region (white), RNP domain (green), and C-terminal domain (blue). (B) Ribbon structure model of the WT-RNP domain based on the published crystal structure (PDB: 3B4D).13 Helices are shown in green, β-sheets and loops in yellow. Helix α1 and strand β2 are marked. Both wild-type cysteines, which had been replaced by serines to create ΔCys-RNP, are highlighted in blue. Alanine 185 and Valine 201 which were exchanged to cysteines are shown in red. The disulfide bond is indicated by a red dotted line.
Two potential oligomerization segments were identified via mutagenesis in PABPN1.10 One of these oligomerization segments covers residues 155–294 and thus the complete RNP domain [Fig. 1(A)]. It is currently unknown whether the RNP domain undergoes a structural change during association to higher oligomeric states. In general, conformational transitions during or before fibril formation have been postulated.11,12 The RNP domain of human PABPN1 has been crystallized and a structure model is available.13 A corresponding domain of Xenopus laevis embryonic poly(A)-binding protein 2 exhibited a very similar architecture.14 The RNP domain from Xenopus dimerized in the absence of poly(A) RNA.14 Dimerization was also observed during crystallization studies with the RNP domain from human PABPN1.13
To explore whether domain swapping would be involved in fibril formation of PABPN1, a disulfide bond was introduced into the RNP domain on the basis of in silico evaluation of interactions in a potential dimer.13 According to the model, a disulfide linkage between positions 185 and 201 should stabilize the association of strand β2 and helix α1 [Fig. 1(B)]. The effect of the disulfide bond on the thermodynamic stability was evaluated in the context of the RNP domain. We demonstrate that the disulfide linkage stabilizes the mutant RNP domain compared to the reduced form and retards fibrillation kinetics in the context of full-length PABPN1. Our data implicate that the stability of the RNP domain plays a role during fibril formation of PABPN1.
Results
The RNP domain and its mutant variants show reversible unfolding transitions
In contrast to the N-terminal domain of PABPN1 which fibrillizes only in the presence of the N-terminal alanine-segment,6,7 the full-length protein forms fibrils also in the absence of the N-terminal alanine stretch. The mechanism leading to fibril formation of the full-length protein is currently not clear. For both, the RNP domain from Xenopus and that from man, dimerization has been discussed.13,14 Dimer formation could be caused by domain swapping and initiate fibril formation.15,16 To impair such a potential domain swapping, disulfide bonds were modeled into the domain with the help of the programme MODIP17 using the crystal structure of the human RNP domain as a template.13 To prevent during disulfide bond formation the interference with the natural cysteines at positions 195 and 205, a cysteine-free variant, ΔCys-PABPN1 was produced via replacement of the natural cysteines by serines. Out of four tested disulfide-linked mutants of full-length PABPN1, only the variant with exchanges of A185C/V201C showed redox sensitive fibril formation (see data below). In this variant, linkage of helix α1 to strand β2 would impair the separation of strand β2 in a potential domain swapping [Fig. 1(B)].13 Based on the crystal structure, these two secondary structure elements have been suggested to form hydrogen bond interactions in a potential dimeric state.13 However, a domain swapping mechanism has not been mentioned by the authors.
The effect of the disulfide bridge should initially be investigated in the context of the RNP domain because thermodynamic parameters of the full-length protein could not be deduced due to irreversible aggregation during unfolding.6 To this end, first biophysical characteristics of the wild-type RNP domain were established with the purified protein derived from recombinant expression in E. coli cells. The success of the purification was controlled by SDS-PAGE [Fig. 2(A)]. Far- and near-UV CD spectroscopy and fluorescence measurements [Fig. 2(B–D)] confirmed the presence of a folded structure. The CD spectrum of the RNP domain indicated secondary structural elements mainly dominated by α-helical and β-sheet contributions, a result that was expected from the structure of the domain published by Ge et al.13 To learn whether the domain was suitable for thermodynamic analyses, chemical unfolding/refolding with urea as a denaturant was performed. A transition midpoint, D1/2 = 2.8M urea was observed. From the data, an m-value of 3.8 ± 0.3 kJ mol−1 M−1 and a ΔGD = 10.7 ± 0.9 kJ mol−1 were calculated (Fig. 3, TableTable1).1). These results show that the domain possesses a moderate thermodynamic stability. During purification of the wild-type RNP domain, however, no evidence for dimeric species was obtained. Analytical ultracentrifugation of all RNP domain variants pointed to monomeric species (data not shown). Yet, domain swapping may be a rare event and could occur rather frequently at elevated protein concentrations that might exist locally within cells, especially, in case of PABPN1, close to transcript polyadenylation.

Biophysical characterization of the RNP domain variants. (A) Coomassie-stained gel of purified RNP domain variants. Samples of WT-, ΔCys-, and dS-RNP were loaded under nonreducing conditions. Sample buffer of SH-RNP contained 100 mM DTT. (B) Far-UV CD spectrum of native (solid line) and denatured (dashed line) RNP domain variants. (C) Near-UV CD spectrum of native RNP domain variants. (D) Fluorescence spectrum of 10 µM RNP domain variants shown for the native (solid line) and denatured protein (dashed line). WT-RNP, black; ΔCys-RNP, blue; dS-RNP, red; SH-RNP, green.

Urea-induced unfolding transitions of RNP domain variants. WT-RNP black circles, black line; ΔCys-RNP light gray circles, light gray line; dS-RNP dark gray circles, dark gray line. For thermodynamic data, see Table I.
Table 1
Thermodynamic and kinetic parameters of RNP domain variants
| Thermodynamic parameters obtained from urea-induced unfolding transitions | |||||||||
|---|---|---|---|---|---|---|---|---|---|
| ΔGD (kJ mol−1) | m (kJ mol−1 M−1) | D1/2 (M) | Tm (app) (°C) | ||||||
| WT-RNP | 10.7 ± 0.9 | 3.8 ± 0.3 | 2.8 ± 0.5 | 55.6 ± 0.4 | |||||
| ΔCys-RNP | 2.4 ± 1.6a | n.d. | n.d. | 37.8 ± 0.8 | |||||
| dS-RNP | 8.1 ± 1.5 | 3.6 ± 0.4 | 2.3 ± 0.7 | 54.1 ± 0.5 | |||||
| SH-RNP | −2.5 ± 0.9a(app) | n.d. | n.d. | n.d. | |||||
| Kinetic parameters obtained from stopped-flow measurements | |||||||||
| ΔGD (kJ mol−1) | D1/2 (M) | ![]() | ![]() | mf (M−1) | mu (M−1) | ||||
| WT-RNP | 12.3 ± 2.8 | 2.9 ± 1.0 | 20.91 ± 1.99 | 0.13 ± 0.02 | 1.44 ± 0.06 | 0.31 ± 0.02 | |||
| dS-RNP | 8.7 ± 1.2 | 2.2 ± 0.5 | 45.66 ± 3.14 | 1.29 ± 0.09 | 1.27 ± 0.05 | 0.36 ± 0.01 | |||
Conditions are detailed in Material and Methods section.
(app): apparent values (incomplete reversibility).
Expression of the cysteine-free variant of the RNP domain, ΔCys-RNP, in E. coli resulted in soluble protein. Variant A185C/V201C-RNP, in contrast, was found aggregated after cell disruption. Hence the insoluble protein was solubilized with guanidinium chloride and separately refolded to either the disulfide linked (dS-RNP) or reduced species (SH-RNP). The presence of the disulfide bond was controlled by SDS-PAGE under reducing and nonreducing conditions. dS-RNP migrated at a lower apparent molecular weight unless it had been reduced with 100 mM dithiotreitol (DTT) [Fig. 2(A)]. Analysis of the mutant proteins via far- and near-UV CD spectroscopy indicated that amino acid replacements did not perturb the overall structure of the RNP domain, despite in ΔCys-RNP and SH-RNP, the random coil contributions appeared to be increased [Fig. 2(B)]. Near-UV CD spectra indicated that the aromatic residues of ΔCys-RNP and SH-RNP are very likely located in a similar chemical environment as in the wild-type structure. The increase in signal intensity for dS-RNP is probably caused by the disulfide bond.18,19 The intrinsic tyrosine fluorescence showed a clear difference under native and denatured conditions for WT-RNP, ΔCys-RNP, and dS-RNP, a result that points to a folded structure under native conditions [Fig. 2(D)]. The smaller difference in amplitudes of SH-RNP under native and denaturing conditions implies that the tyrosine residues in this variant might be more solvent-exposed.
Via equilibrium unfolding studies the influence of the amino acid replacements on the stability of the domain was studied. Urea-induced unfolding transitions indicated a ΔGD = 8.1 ± 1.5 kJ mol−1 for dS-RNP. For ΔCys-RNP, a plateau of natively folded species could not be observed at room temperature (Fig. 3). In the case of SH-RNP, only a baseline related to unfolded species was detected (not shown), indicating a severely reduced stability caused by the exchanges. Quantification of thermodynamic parameters for ΔCys-RNP and SH-RNP could be performed using the stabilizing Hofmeister salt (NH4)2SO4 during urea-induced unfolding and the extrapolation of the free energy of unfolding to 0M (NH4)2SO4, as described earlier for a different metastable protein domain20 (Supporting Information Fig. S1). This way, for ΔCys-RNP, a value of ΔGD = 2.4 ± 1.6 kJ mol−1 was obtained (Table(Table1).1). Whereas the unfolding of all other variants was completely reversible, refolding of SH-RNP occurred with only 80–90% of the species. Nevertheless, an apparent ΔGD = −2.5 ± 0.9 kJ mol−1 was calculated for SH-RNP (Table(Table1).1). The negative ΔGD value suggests that the unfolded state of the variant is thermodynamically favored. The numbers show also a significant stabilization resulting from the disulfide linkage in dS-RNP compared to its reduced form SH-RNP and the cysteine-free control ΔCys-RNP (Table(Table1).1). Despite a distinct stabilization by the disulfide bond was observed, dS-RNP exhibited a slightly lower stability than WT-RNP (Table(Table11).
In addition to chemical unfolding, thermal stabilities were examined for WT-RNP, ΔCys-RNP, and dS-RNP (Fig. 4). Despite optimizations such as modified buffer systems and heating/cooling rates, only 80% of the initial signal amplitudes were reached in the refolding experiments. Nevertheless, apparent parameters were determined (Table(Table1).1). Because of the limited reversibility of the more stable variants, thermal unfolding of SH-RNP was omitted. Melting temperatures, Tm, confirmed a notably increased thermal stability of dS-RNP compared to ΔCys-RNP, but a slightly decreased stability in comparison to the wild-type (Table(Table11).

Temperature-induced unfolding transitions of RNP domain variants. Monitoring of unfolding was performed by far-UV CD spectroscopy through detection at 208 nm. WT-RNP, black circles and black line; ΔCys-RNP, light gray circles and light gray line; dS-RNP, dark gray circles and dark gray line. Calculated thermodynamic parameters are summarized in Table I.
Stopped-flow kinetics support a two-state folding mechanism of the RNP domain
Unfolding of the RNP domain variants under equilibrium appeared to proceed without stable intermediates. Additional unfolding transitions for WT-RNP and dS-RNP by near-UV CD spectroscopy were monitored to follow unfolding of the secondary structures. Unexpectedly, the transition midpoints detected by CD spectroscopy were shifted to higher urea concentrations than those detected by fluorescence (Supporting Information Fig. S2). This non-coincidence of CD and fluorescence signals is presumably caused by the surface-exposed position of the tyrosine residues (Supporting Information Fig. S3). Consequently, unfolding transitions were repeated in the presence of 0.1M acrylamide as a fluorescence quencher. Under these conditions, transition midpoints were shifted to even lower urea concentrations (Supporting Information Fig. S2). The result confirmed the assumption that low urea conditions are sufficient to increase the solvent exposure of the tyrosine residues.
To elucidate the folding pathway of the RNP domain in more detail, folding kinetics of WT-RNP and dS-RNP were analyzed by stopped-flow measurements (Fig. 5). A coincidence of fluorescence and CD signals during folding and unfolding was observed, supporting the assumption of a two-state folding mechanism. Neither in the folding nor in the unfolding branch, any significant deviations from linearity were detectable. Since stopped-flow kinetics present a robust assay for assessing if structure formation occurs via a two-state pathway,21 these results were considered as an additional proof for the absence of stable intermediates. Moreover, the ΔGD values of the equilibrium studies agreed with the kinetic data for both proteins (Table(Table11).

Chevron plots for the unfolding and refolding of RNP domain variants. (A) WT-RNP and (B) dS-RNP. Measurements were performed using fluorescence (circles) or CD measurements (squares). Data obtained from unfolding experiments are shown as black symbols and from refolding experiments as open symbols. The fits were calculated from the fluorescence data. Thermodynamic values are listed in Table I.
Notably, the folding rate,
of dS-RNP was increased by factor two, while the unfolding rate,
showed a 10-fold acceleration when compared to the wild-type domain (Table(Table1).1). The faster folding rate is likely to be caused by the artificial disulfide bond, which may add to early contacts of native structures. Residues that form interactions in the native or transition state upon folding maybe constrained in close proximity, leading to faster folding. The accelerated unfolding rate could be caused by the replacement of both cysteines in WT-RNP by serines which probably lead to the faster disintegration of the native structure. Considering the low stability of ΔCys-RNP and SH-RNP and the need to add stabilizing salts during equilibrium measurements at room temperature, folding kinetics of these variants were not carried out. In summary, in the case of ΔCys-RNP and SH-RNP, a two-state folding process could not be deduced.
The disulfide bond in the RNP domain of PABPN1 retards fibril formation
Next, the effect of the disulfide bridge on the protein stability was investigated in the context of full-length PABPN1. Far- and near-UV CD spectra confirmed that the amino acid substitutions in ΔCys-PABPN1 and dS-PABPN1 did not significantly change the secondary or tertiary structures (Supporting Information Fig. S4). The functional integrity of the mutant PABPN1 variants was confirmed using RNA binding assays (data not shown).
To explore whether the disulfide bond may alter the thermal stability of the protein, heat-induced aggregation was followed by light scattering. Clearly, the onset of light scattering correlated with the stability of the corresponding RNP domain (Supporting Information Fig. S5). Thus, the stability differences of the RNP domain variants were detectable in full-length PABPN1.
Fibril formation was tested under reducing and nonreducing conditions via ThT fluorescence [Fig. 6(A)]. As expected, no significant influence of DTT on the fibrillation of WT-PABPN1 and ΔCys-PABPN1 was observed. A striking difference was detected during fibrillation of dS-PABPN1 under reducing and nonreducing conditions. Under nonreducing conditions dS-PABPN1 fluorescence signals turned into a plateau after about 300 h of incubation [Fig. 6(A)]. When dS-PABPN1 was reduced with 10 mM DTT, 50% of the species became reduced to SH-PABPN1, as determined by SDS-PAGE (Supporting Information Fig. S6). Fibrillation kinetics under these conditions showed a plateau of ThT fluorescence intensity after ca. 50 h (data not shown). An overnight incubation in the presence of 100 mM DTT resulted in 90% of the reduced form SH-PABPN1 (Supporting Information Fig. S6). In this case, fibril formation was further accelerated and fluorescence signals reached a plateau already after 5 h [Fig. 6(A)]. Thus, the elevated DTT concentrations that were required for efficient cleavage of the disulfide bond in dS-PABPN1 enabled also the fast fibrillation of SH-PABPN1. The presence of fibrillar structures was confirmed for all variants by electron microscopy [Fig. 6(B)]. Fibrils exhibited similar resistances against solubilization as fibrils obtained from wild-type PABPN1 (data not shown).

Fibril formation of full-length PABPN1 variants. (A) ThT fluorescence signals were detected at 482 nm. Black symbols represent reducing conditions, open symbols nonreducing conditions. WT-PABPN1, circles; ΔCys-PABPN1, squares; dS-PABPN1 and SH-PABPN1, triangles. Fibrillation reactions were performed at a protein concentration of 60 µM at 20°C. (B) Electron micrographs of fibrillar species. Samples were incubated either under reducing conditions (+) or nonreducing conditions (−).
The results clearly reveal a retardation of fibril formation in the presence of the disulfide bridge in the RNP domain. Notably, all PABPN1 variants showed faster fibril formation kinetics than wild-type PABPN1 which could be related to the lower thermodynamic stability of the RNP domains caused by the exchanges. To correlate fibrillation kinetics of full-length PABPN1 with the stabilities of the RNP domains, a hyperbolic fit of the ThT signals was used to determine fibrillation rate constants, k [Fig. 7(A)]. The natural logarithm of the fibrillation rate constant was plotted against ΔGD values. The resulting graphs reveal that fibrillation rate constants correlate inversely with the decreasing thermodynamic stability of the RNP domain [Fig. 7(B)]. Comparable results were obtained when the fibrillation rates at initial time points were investigated (data not shown). Thus, the disulfide bond in dS-PABPN1, although not fully impairing fibril formation, clearly retards fibrillation compared to reduced SH-PABPN1. We conclude from these data, that (partial) unfolding of PABPN1 or the RNP domain is rate-limiting for the conversion from soluble proteins to fibrils.

Kinetics of PABPN1 fibril formation. (A) Fibrillation kinetics of full-length PABPN1 were fitted using the exponential equation y = y0+a·exp(−k·x) as described in Material and Methods section. The fibrillation rate constant k quantifies conversion of monomeric protein into fibrils. WT-PABPN1, open circles, dotted line; ΔCys-PABPN1, open squares, dashed-dotted line; dS-PABPN1, open triangles, dashed line; SH-PABPN1, black triangles, solid line. (B) Plot of the natural logarithm of the fibrillation rate constant k against ΔGD of the corresponding RNP domain. The line shows a linear correlation between the plotted data.
Discussion
It is still unclear why in vitro, full-length PABPN1 forms fibrils in an alanine-independent process, while fibrillation of the N-terminal domain clearly depended on the presence and length of the alanine stretch.6–8 In muscle biopsies from OPMD patients, typical tubular filaments were found, closer analysis of the fibrils revealed that they contained predominantly PABPN1.22,23 The pathological relevance of the fibrils remains obscure because intranuclear inclusions consisting of PABPN1 have also been detected in neurons of wild-type rats.24 Apart from the biological aspects, the biochemical question remains as to why PABPN1 aggregates.
Presently, folding/unfolding studies cannot be performed with full-length PABPN1, because of its tendency to form amorphous aggregates. Structural analysis of the separate RNP domain had pointed to a dimerization,13,14 which could represent a starting point during fibrillation. In this work, an attempt has been made to explore the influence of the RNP domain on the fibril forming tendency of PABPN1, and together with a previous study, a complete picture of domain contributions during fibril formation of PABPN1 should be obtained.8
To clarify a potential role of the RNP domain in fibrillation, we aimed to create a stabilized variant of the RNP domain via introduction of a disulfide bond. Artificial disulfide linkages have been demonstrated as valuable tools to increase the conformational stabilities.25–28 The effect of such a covalent bond on the conformational stability can be quantified, based on the decrease of conformational entropy of the unfolded state with the following equation29:

where n is the number of residues between cysteines forming a disulfide bond.
According to the equation, for dS-RNP, ΔS = −12.7 kJ mol−1 at 20°C was calculated. This means, that the disulfide bond in dS-RNP should contribute additional 12.7 kJ mol−1 to the conformational stability compared to reduced SH-RNP. The theoretical contribution of the disulfide bond was compared to the measured difference between the ΔGD values of the oxidized and reduced forms: ΔΔG = ΔGD(ox) − ΔGD(red) = 10.6 kJ mol−1. The slight discrepancy of theoretical and calculated values might be caused by the conformational strain induced by the disulfide bond. Nevertheless, the disulfide bond significantly increased the conformational stability of dS-RNP compared to reduced SH-RNP. However, it did not exceed the more stable variant WT-RNP. As it becomes evident from TableTable1,1, the replacement of both natural cysteines by serines considerably reduced the thermodynamic stability of ΔCys-RNP, which very likely results from altered secondary and tertiary contacts. Evidence for structural changes in ΔCys-RNP were obtained from CD spectroscopy. Consequently, the artificial disulfide bond appeared to partially compensate for the introduced exchanges in ΔCys-RNP.
In the context of the full-length PABPN1, fibril formation of oxidized dS-PABPN1 was severely retarded compared to the reduced species SH-PABPN1 or the cysteine-free variant ΔCys-PABPN1. Hence, the disulfide bond in the RNP domain slowed fibril formation. Yet, fibrillation was not completely blocked in dS-PABPN1. Similarly, in cystatin C mutants, artificial disulfide bonds led to reduction of fibrillary species by only 80%.16 Studies on prion protein conformational transitions, revealed the reorganization of intramolecular disulfide bonds towards a disulfide-linked domain swapped dimer, which had been suggested to present a precursor during the oligomerization process.15,30 Interestingly, directional tethering of secondary structure elements with additional artificial disulfide bonds inhibited the conversion of soluble prion protein into fibrils.31
Despite the data presented here do not exclude a domain swapping mechanism that precedes PABPN1 fibril formation, we assume that rather by restricting a conformational transition or the dissociation of secondary structure elements, the artificial disulfide bond retards fibrillation via to its effect on the conformational stability. Similar correlations between stability of the flanking fold and induction of fibrillation by glutamine stretches have been reported upon integration of glutamines into a folded or unfolded host protein.32 In addition, comprehensive studies on the conversion of ataxin-3 revealed that fibril formation of ataxin-3 can be influenced by the stability of the neighboring Josephin domain and not only by the glutamine segment.33–35 Whether fibril formation of PABPN1 in mammalian tissue follows a two-stage mechanism and if an unfolding process precedes fibrillation presents a future experimental challenge.
Materials and Methods
Modelling
Disulfide-linked RNP domain variants were modeled with the program MODIP.17 The crystal structure of the RNP domain of human PABPN1 (PDB ID: 3B4D),13 served as the template for MODIP-assisted identification of suitable positions for double cysteine exchanges to allow formation of an intramolecular disulfide bond. In total, 19 potential variants were found. From four experimentally tested variants, mutant A185C/V201C-PABN1 showed redox-dependent fibril formation in the context of the full-length protein.
DNA technology for expression of mutant constructs
Mutations were introduced into a previously described expression construct8 for WT-PABPN1 in pET11a (Novagen) using the QuickChange II Site-Directed Mutagenesis Kit (Agilent Technologies). As a basis for disulfide-linked PABPN1 variants, the two existing cysteines of WT-PABPN1 were replaced by serines resulting in ΔCys-PABPN1. Forward primers for the replacement of cysteines 195 and 205 were 5′ G CTA GAA GCA CAC TTT CAT GGC AGT GGT TCA GTC AAC C 3′ and 5′ GC GTA ACT ATA CTC AGT GAC AAA TTT AGT GG 3′, respectively, and the corresponding complementary reverse primers. Based on ΔCys-PABPN1, codons for variant A185C/V201C-PABPN1 were introduced. Primers for A185C were 5′ GGC AAT GTG GAC TAT GGT GCA ACA TGT GA A GAG CTA GAA GC 3′ and for V201C, 5′ GGT TCA GTC AAC CGC TGT ACT ATA CTC TGT GAC AAA TTT AGT GGC C3′ including the complementary oligonucleotides. The RNP domain and mutant variants encompassing residues 167–25413 were amplified by PCR (Eppendorf Mastercycler Gradient) with Pwo polymerase from peqGOLD. Forward primer was 5′ TAT GTG CAT ATG GAG GCT GAT GCC C 3′ and reverse primer 5′ AT TAT GGA TCC TTA TTA GAT GCC TGG TCT GTT GG 3′. The PCR products were inserted into pET11a (Novagen) via NdeI and BamHI restriction sites.
Recombinant protein production and purification
PABPN1 and RNP domain variants were produced in E. coli BL21 (DE3) Rosetta 2 pLysS cells in the presence of chloramphenicol and carbenicillin (Applichem). Full-length PABPN1 was produced in complex medium in a 10 L bioreactor (Biostat C-DCU; Sartorius Stedim) according to an established protocol36 with minor modifications: The feeding solution contained glycerol instead of glucose. Before induction with 1 mM isopropyl 1-thio-β-d-galactopyranoside (IPTG), the cultivation temperature was reduced to 30°C to minimize protein aggregation. Recombinant gene expression was continued for 3 h. Purification of PABPN1 was performed as described.8,37 Buffers for ΔCys-PABPN1 lacked DTT. For the production of A185C/V201C-PABPN1, the wet cell pellet before cell disruption was resuspended in buffer containing 1 mM DTT. The elution buffer from the Blue Sepharose column contained 5 mM oxidized glutathione to trigger the formation of the intramolecular disulfide bond. From this oxidized form, referred to as dS-PABPN1, the reduced species SH-PABPN1 was obtained by overnight reduction on ice with 100 mM DTT.
For recombinant production of the RNP domain, cells were grown at 37°C in terrific broth (TB) in shake flasks. Induction with IPTG was done at OD600 = 0.4–0.5 and cultivation continued for 3 h. All buffers for preparation of WT-RNP except the final storage buffer contained 1 mM DTT. For production of ΔCys-RNP and oxidized species of A185C/V201C-RNP, DTT was omitted. The reduced form of A185C/V201C-RNP was maintained by the presence of 5 mM Tris-(2-carboxyethyl)-phosphine hydrochloride (TECP).
Per gram wet cell pellet, 4 mL 50 mM Tris/Cl pH 8.0, 5 mM EDTA supplemented with complete Mini EDTA-free protease inhibitor (Roche) and 0.1 mg mL−1 lysozyme (Applichem) was added. Cell disruption was performed by high-pressure homogenization. Subsequently, 10 U Benzonase (Novagen) per gram cells and MgCl2 to a final concentration of 8 mM were added. Cell extracts containing WT-RNP and ΔCys-RNP were subjected to a HiPrep Q XL 16/10 (GE Healthcare). The flow-through was collected, and (NH4)2SO4 was adjusted to a final concentration of 1.2M. After 1 h incubation at 4°C, precipitates were removed by centrifugation. The supernatant was loaded on a HiPrep Phenyl HP 16/10 column (GE Healthcare). Elution was achieved by a linear gradient from 1.2M to 0M (NH4)2SO4 in 50 mM Tris/HCl pH 8.0, 5 mM EDTA. RNP domain containing fractions were dialyzed against 20 mM MOPS pH 6.5, loaded on a HiPrep SP FF 16/10 column (GE Healthcare) and eluted by a gradient from 0M to 1.5M NaCl. Fractions containing pure protein were applied to a HiLoadSuperdex 75 prep grade 16/60.
For production of A185C/V201C-RNP which accumulated in the insoluble fraction after cell lysis, per gram wet pellet, 5 mL solubilization buffer containing 100 mM Tris/Cl pH 8.0, 6M GdmCl, 5 mM EDTA, 100 mM DTT was added. Thereafter, dialysis against 10 mM Na-acetate, pH 4.0, 5M GdmCl was performed. Renaturation at a final protein concentration of 0.2 mg mL−1 was performed by rapid dilution in 100 mM Tris/Cl pH 8.5, 1M l-arginine, 5 mM EDTA. To obtain oxidized species A185C/V201C-RNP, 5 mM oxidized and 2 mM reduced glutathione were added to the renaturation buffer. Reduced species was produced by renaturation in the presence of 10 mM DTT. Final purification procedures, including HiPrep SP FF 16/10 and size exclusion chromatography were done as described above. Protein purity was evaluated via SDS-PAGE and UV absorption. Finally, the RNP domains were dialysed against storage buffer (20 mM Tris/HCl pH 7.5) and kept at −70°C.
Circular dichroism and fluorescence spectroscopy
Circular dichroism (CD) spectra were recorded using a Jasco J810 spectropolarimeter and 0.1 mm cuvettes at 20°C. Protein concentration was between 0.5 and 1.0 mg mL−1. Spectra were buffer-corrected. Fluorescence spectra were measured on a Jobin Yvon Fluoromax-3 in 1 cm cuvettes at 20°C. The protein concentration was 10 µM. Excitation wavelength was 274 nm and the bandwidth was 5 nm. Emission bandwidth was 8 nm and spectra were accumulated 10 times, averaged and buffer corrected. Native protein was buffered in 20 mM Tris/HCl pH 7.5. For denaturation, 6M guanidinium chloride was added to the buffer.
Denaturant- and heat-induced unfolding transitions
For urea-induced unfolding, RNP domain variants at a concentration of 2.5 µM were incubated in the presence of varying urea concentrations in 20 mM Tris/HCl pH 7.5 overnight. Urea-induced unfolding was monitored by fluorescence measurements on a Jobin Yvon Fluoromax-3 at 20°C in 1 cm cuvettes. Since no tryptophans are present in the RNP domain, emission at 307 nm was averaged over 30 s upon excitation of tyrosines at 274 nm. Excitation and emission band widths were 5 nm and 8 nm, respectively. Unfolding transitions were evaluated assuming a two-state model by nonlinear least-squares fitting.38 Heat-induced unfolding/refolding signal changes were monitored by CD at 208 nm using a Jasco J810 spectropolarimeter and 1 mm cuvettes. Protein concentration was 24.5 µM in 20 mM KH2PO4, pH 7.5. The heating rate was 1 K min−1. For calculation of Tm, CD signals were fitted according to a published method.39
Stopped-flow measurements
Folding and unfolding rates were followed by fluorescence and CD spectroscopy at 20°C. In both methods 20 mM Tris/HCl, pH 7.5 was used as a buffer. Stock solutions with native (0M urea) or denatured (8M urea) protein were mixed before measurement at a ratio of 1 + 10 in buffer containing different urea concentrations to observe folding/unfolding kinetics. Fluorescence data were collected with an Applied Photophysics SX20 stopped-flow fluorimeter at a protein concentration of 5 µM. Excitation was set at 280 nm, emission was recorded above 305 nm using a cut-off filter. CD experiments were performed using an Applied Photophysics Pi-Star-180 spectrometer. Signals were detected at 235 nm with a slit width of 1 nm. The final protein concentration was 25 µM. Data were fitted as published previously.21
Miscellaneous
Fibril formation was recorded by the ThT fluorescence intensity at 482 nm. Samples from a fibrillation reaction were diluted to a final concentration of 2 µM protein and 50 µM ThT.8 Electron microscopy was carried out as described earlier.7 To ensure reducing conditions, 10 mM DTT was added each day. As SH-PABPN1 fibrillized after reduction with 100 mM DTT within 5 h, no further DTT was added. Fibrillation rate constants were calculated from ThT signals according to y = y0+a·exp(−k · x). The parameter k represents the fibrillation rate constant.
Acknowledgments
Valuable advice on the RNP domain purification was provided by Till Scheuermann. The assistance of Franziska Schikora and Victoria Junghans is gratefully acknowledged. We also thank Cordelia Schiene-Fischer for providing CD stopped-flow equipment.
Supporting Information
Additional Supporting Information may be found in the online version of this article.
Supporting Information
References
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