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. 2024 Mar 21;33(4):e4951. doi: 10.1002/pro.4951

Liquid–liquid phase separation of α‐synuclein is highly sensitive to sequence complexity

Anindita Mahapatra 1,, Robert W Newberry 1,
PMCID: PMC10955625  PMID: 38511533

Abstract

The Parkinson's‐associated protein α‐synuclein (α‐syn) can undergo liquid–liquid phase separation (LLPS), which typically leads to the formation of amyloid fibrils. The coincidence of LLPS and amyloid formation has complicated the identification of the molecular determinants unique to LLPS of α‐syn. Moreover, the lack of strategies to selectively perturb LLPS makes it difficult to dissect the biological roles specific to α‐syn LLPS, independent of fibrillation. Herein, using a combination of subtle missense mutations, we show that LLPS of α‐syn is highly sensitive to its sequence complexity. In fact, we find that even a highly conservative mutation (V16I) that increases sequence complexity without perturbing physicochemical and structural properties, is sufficient to reduce LLPS by 75%; this effect can be reversed by an adjacent V‐to‐I mutation (V15I) that restores the original sequence complexity. A18T, a complexity‐enhancing PD‐associated mutation, was likewise found to reduce LLPS, implicating sequence complexity in α‐syn pathogenicity. Furthermore, leveraging the differences in LLPS propensities among different α‐syn variants, we demonstrate that fibrillation of α‐syn does not necessarily correlate with its LLPS. In fact, we identify mutations that selectively perturb LLPS or fibrillation of α‐syn, unlike previously studied mutations. The variants and design principles reported herein should therefore empower future studies to disentangle these two phenomena and distinguish their (patho)biological roles.

Keywords: aggregation, alpha‐synuclein, phase separation, sequence complexity

1. INTRODUCTION

Liquid–liquid phase separation (LLPS) is the metastable assembly of macromolecules into liquid‐like droplets, which enables spatiotemporal regulation of cellular functions (Hyman et al., 2014). Fibrillation, on the other hand, is the aberrant self‐assembly of functional proteins into amyloid fibrils, which is a pathological hallmark of various neurodegenerative disorders (Dobson, 2017; Eisenberg & Jucker, 2012). Recently, LLPS has been implicated as a regulator of pathological fibrillation (Zbinden et al., 2020; Babinchak & Surewicz, 2020), primarily because several amyloid‐forming proteins have been found capable of undergoing LLPS in physiological conditions (Lin et al., 2015; Molliex et al., 2015; Murakami et al., 2015; Patel et al., 2015; Wegmann et al., 2018; Ray et al., 2020), and disease‐associated mutations that affect fibrillation of these proteins have been found to affect their LLPS as well (Ray et al., 2020; Johnson et al., 2009; Conicella et al., 2016; Zhou et al., 2022). Prominent examples include hnRNPA1 (Lin et al., 2015; Molliex et al., 2015), TDP‐43 (Molliex et al., 2015), and FUS (Murakami et al., 2015; Patel et al., 2015)—associated with amyotrophic lateral sclerosis (Zhao et al., 2018); and tau (Wegmann et al., 2018)—associated with Alzheimer's disease (Grundke‐Iqbal et al., 1986). A relatively new inclusion in this group is α‐synuclein (α‐syn) (Ray et al., 2020)—associated with Parkinson's disease (PD) (Spillantini et al., 1997; Lee et al., 2004), which has only recently been found to undergo LLPS in vitro (Huang et al., 2022b; Nelson et al., 2023; Ray et al., 2020, 2023), in human cell lines (Ray et al., 2020), and in C. elegans (Hardenberg et al., 2021).

α‐Syn is an intrinsically disordered, presynaptic protein, the fibrillation of which is implicated in the pathogenesis of PD and other synucleinopathies (Spillantini et al., 1997; Goedert, 2001). Native α‐syn is involved in the trafficking of synaptic vesicles via membrane binding (Mahapatra et al., 2021; Fusco et al., 2018), and why and how it converts to pathogenic amyloid fibrils is still not clearly understood. In vitro studies have established that the process involves structural conversion of the soluble monomer into a fibrillation‐competent nucleus, which goes through oligomeric and pre‐fibrillar intermediates to eventually form insoluble fibrillar aggregates (Fink, 2006). The rate of α‐syn fibrillation is known to be influenced by environmental triggers (Goldman, 2014), as well as various missense mutations in the amino acid sequence of α‐syn that have been directly linked to the onset/progression of familial and sporadic PD (Mukherjee et al., 2023; Kumar et al., 2018). The recent discovery of α‐syn's ability to undergo LLPS, followed by a gradual liquid‐to‐solid transition into amyloid‐like fibrillar aggregates (Ray et al., 2020), has complicated matters further and led to significant interest in the potential role of α‐syn LLPS in fibrillation. Several studies have investigated LLPS of α‐syn in presence of extrinsic factors that affect its fibrillation, such as pH (Sawner et al., 2021), metal ions (Ray et al., 2020; Xu et al., 2022b; Huang et al., 2022a), and natural products (Xu et al., 2022a). However, the intrinsic drivers of α‐syn LLPS are still largely unclear. Reports to date have implicated all three domains of the protein (i.e., N‐terminal, non‐amyloid‐β component or NAC, and C‐terminal) to be involved in mediating its LLPS, either by electrostatic or hydrophobic interactions (Ray et al., 2020; Huang et al., 2022b); but more specific, residue‐level determinants of α‐syn LLPS remain unknown, making it difficult to ascertain its biological significance. Moreover, the coincidence of α‐syn LLPS and fibrillation complicates the dissection of their individual roles in disease.

Although α‐syn is structurally and functionally distinct from other phase‐separating, amyloidogenic proteins like hnRNPA1, TDP‐43, FUS and tau, they all share at least one notable similarity: the presence of low‐complexity domains (LCDs) in their primary structure. LCDs are segments within proteins that have low compositional (or sequence) complexity, that is, they are composed of relatively few distinct amino acids. LCDs are widely implicated as the key drivers of protein phase separation. They have been found sufficient for LLPS of hnRNPA1 (Molliex et al., 2015), TDP‐43 (Conicella et al., 2016), and FUS (Burke et al., 2015); and are generally believed to mediate LLPS through transient multivalent interactions between specific types of amino acids that are prevalent within them, mostly aromatic and/or polar residues (Zbinden et al., 2020; Vernon et al., 2018; Fung et al., 2018). For example, LLPS of FUS is mediated by tyrosine and glutamine residues in its LCD (Murthy et al., 2019; Qamar et al., 2018), and LLPS of TDP‐43 is mediated by arginine and regularly spaced aromatic residues in its LCD (Li et al., 2018a, 2018b; Schmidt et al., 2019). The role of LCDs in protein LLPS has therefore largely been ascribed to the physicochemical properties, and often identities, of their constituent amino acids (Zbinden et al., 2020). However, given the diversity of composition between different LCDs, we wondered if their complexity itself might be a key determinant of LLPS, and sought to test this hypothesis in α‐syn, which is predicted to contain two LCDs (Ray et al., 2020).

Some previous studies examined the roles of LCDs in protein LLPS by deleting parts or whole of the LCDs from the respective proteins (Lin et al., 2015; Li et al., 2018b); although informative, this approach can significantly alter one or more fundamental physicochemical properties of the protein, including its size, hydrophobicity, and charge. Because we wanted to specifically investigate the impact of sequence complexity on α‐syn LLPS, we took a different experimental approach that would largely preserve the fundamental physicochemical properties of the protein while only modifying the complexity of its two LCDs. To achieve this, we employed the Simple Modular Architecture Research Tool (SMART) – a computational tool that engages the SEG algorithm to identify LCDs in protein sequences (Letunic & Bork, 2018). The SEG algorithm (Wootton & Federhen, 1993; Wootton, 1994; Wootton & Federhen, 1996) classifies a protein segment as LCD based solely on its compositional complexity, which is determined by the count of unique amino acids in the given segment, independent of sequence patterns or repetition (Wootton & Federhen, 1996). Mathematically, compositional complexity of a protein segment of length L is defined by K=1Llog20L!i=120ni!, where ni is the number of occurrences of each of the 20 different amino acids in the given segment, with 0niL and i=120ni=L (Wootton, 1994). For the purpose of our study, we defined sequence complexity of α‐syn as the cumulative compositional complexity of the two segments corresponding to its two LCDs; and by careful design, introduced chemically subtle missense mutations in one or both of these segments, so that only sequence complexity of α‐syn is altered without affecting its structural and physicochemical properties. By comparing the propensity of the resulting variants to phase separate relative to the WT, we demonstrated that LLPS of α‐syn decreases dramatically with increasing sequence complexity. We also showed that our designed mutations have no consistent effect on α‐syn fibrillation in the absence of LLPS; in doing so, we identified mutations that selectively perturb either LLPS or fibrillation of the protein, providing new tools for studying the behavior of α‐syn.

2. RESULTS

2.1. Designing mutations to test the role of sequence complexity in LLPS of α‐syn

α‐Syn contains two low‐complexity domains (LCDs) in its primary structure, as predicted by SMART (Letunic & Bork, 2018) (Figure 1, WT). To test the role of sequence complexity in α‐syn LLPS, we designed subtle missense mutations in these two LCDs (LCD1 and LCD2), such that they increase sequence complexity of the protein while minimally perturbing its structural and physicochemical properties (see Sections 4.2 and 4.3 for detailed explanation of our design strategy and quantification of sequence complexity). After examining the sequence of LCD1 (residues 10–23), we identified a single valine‐to‐isoleucine mutation (V16I) that would be sufficient to increase the sequence complexity of this region above the threshold for identification as a LCD by SMART (Figure 1, variant −LCD1). Owing to the chemical subtlety of this mutation (a single methyl group on a single hydrophobic residue in a 140‐residue protein), computational analyses predicted minimal changes to the protein's charge and hydrophobicity (Table S1), as well as its propensity for disordered or helical structure (Figure S1a,c). Furthermore, to test if restoring the original sequence complexity can rescue LLPS behavior of the WT protein, we designed another variant in which the disruption of LCD1 by the V16I mutation was rescued by introducing a second V‐to‐I mutation (V15I) adjacent to the V16I (Figure 1, variant LCD1*). As a result, this variant had the same sequence complexity as the WT protein, albeit having a slightly different amino acid sequence (with two isoleucine residues instead of two valine residues at positions 15 and 16). SMART analysis predicted that introducing a single V‐to‐I mutation in LCD2 (residues 63–78), would not sufficiently increase sequence complexity to disrupt this LCD. We therefore paired a V‐to‐I mutation (V70I) with a glycine‐to‐proline mutation (G68P), which together raised sequence complexity of this region above the threshold for detection as a LCD by SMART (Figure 1, variant –LCD2). We also combined the –LCD1 and –LCD2 substitutions to make a variant with no predicted LCDs (Figure 1, variant –LCD1&2). Like the –LCD1 variant, the LCD1*, –LCD2 and –LCD1&2 variants were all predicted to retain the physicochemical properties and structural propensities of the WT protein, due to the chemical subtlety of the introduced mutations (Table S1, Figure S1a,c). We therefore expected our designed LCD variants to test the role of sequence complexity in LLPS of α‐syn.

FIGURE 1.

FIGURE 1

In silico analyses of amino acid sequences of α‐syn variants using SMART, showing their respective LCDs and calculated sequence complexities. The calculation of sequence complexity is described in detail in Section 4.3.

Curious to see if any of the known PD‐associated mutations of α‐syn affect any of its LCDs, we ran SMART prediction on the amino acid sequences of all known patient variants. Interestingly, only the sporadic PD‐associated mutation A18T (Kumar et al., 2018) (located within the LCD1 region of α‐syn) was found to sufficiently increase compositional complexity of this region so that it was no longer predicted as a LCD by SMART (similar to V16I). The familial PD mutation E83Q (Kumar et al., 2022) (lying slightly outside the LCD2 region of the WT protein) was predicted by SMART to slightly increase the length of this region (Figure 1, variant E83Q vs. WT). Although the E83Q mutation slightly lowered sequence complexity relative to WT α‐syn, it did not change the number of predicted LCDs of α‐syn, and may therefore be expected to behave similar to the WT protein. Interestingly, both E83Q and A18T, are known to promote fibrillation of α‐syn in vitro (Kumar et al., 2018, 2022). Though the patient variants did not have the same charge, hydrophobicity and helical propensity as the WT protein, unlike our carefully designed synthetic LCD variants, they might be useful for exploring the role of sequence complexity and/or LLPS in PD pathogenesis.

2.2. LLPS of α‐syn decreases with increasing sequence complexity

To compare the propensity of droplet formation among α‐syn variants with different sequence complexities, we induced in vitro LLPS of all seven variants (including WT) by introducing a widely used molecular crowder (PEG 8000, 20% w/v) under physiological salt and pH conditions (PBS, pH 7). Consistent with previous observations under similar conditions (Sawner et al., 2021), droplets of the WT protein started forming almost immediately (Figure S2). However, as the nascent (0‐h) droplets were too mobile to be focused under the fluorescence microscope for imaging, LLPS samples of all variants were allowed to mature for up to 4 h at 37°C prior to imaging and quantification. Quantification of the area covered by droplets revealed a marked decrease in droplet formation of α‐syn upon decreasing the number of LCDs by increasing sequence complexity of the protein (Figure 2). A similar correlation between sequence complexity and phase separation was observed when droplets were quantified by turbidity (Figure S3).

FIGURE 2.

FIGURE 2

(a) Quantification of droplet formation for all LLPS variants of α‐syn at pH 7, showing decrease in amount of droplet formation with decreasing number of LCDs in the protein. Images over each column show representative high magnification (126×) confocal microscopic images of individual droplets of respective LLPS variants. Scale bar = 10 μm. (b) Plot of droplet area vs. change in sequence complexity (relative to WT α‐syn), showing a decrease in LLPS propensity with increase in sequence complexity of α‐syn. Data represent mean ± standard deviation (SD) for n = 2 independent experiments. Statistical significances are indicated by *p ≤ 0.05, **p ≤ 0.01, ***p ≤ 0.001, ****p ≤ 0.0001.

Even a single V‐to‐I mutation in the first LCD (V16I), leading to disruption of this LCD due to increased sequence complexity, was sufficient to reduce droplet formation by a dramatic 75%, despite its minimal effects on the protein's physicochemical and structural properties (variant –LCD1). Remarkably, the reduction in α‐syn LLPS by the V16I mutation was reversed by a second adjacent V‐to‐I mutation (V15I), which restores the original sequence complexity and hence LCDs of the WT protein (variant LCD1*). The complete rescue of α‐syn LLPS upon introducing this second V‐to‐I mutation shows that V‐to‐I mutations do not inherently decrease LLPS of α‐syn; rather the overall sequence complexity of the protein appears to govern its propensity to phase separate.

Disrupting the second LCD (LCD2) of α‐syn by sufficiently increasing sequence complexity through the G68P and V70I mutations, was also found to drastically reduce LLPS relative to the WT (variant –LCD2). In contrast, a mutation in the LCD2 region that does not disrupt this LCD (such as V70I) could not reduce LLPS relative to WT α‐syn (Figure S4). The drastic reduction in LLPS propensity of the –LCD2 variant is consistent with previous observations by Ray et al. indicating the importance of the NAC domain (residues 61–95, containing the LCD2 region) in facilitating α‐syn LLPS (Ray et al., 2020). For the –LCD1&2 variant, with highest sequence complexity relative to the WT and no predicted LCDs, LLPS propensity was reduced to such an extent that we were unable to detect any droplets, even at reduced pH where LLPS is more abundant (Figures S5–S9). For all the other variants, LLPS was more abundant at reduced pH, as expected.

Changes in LLPS propensity due to the patient mutations E83Q and A18T could likewise be rationalized by their effects on sequence complexity. Upon induction of LLPS in vitro, the E83Q mutation did not affect droplet formation significantly when compared to WT (Figure 2), consistent with its minimal effect on sequence complexity. In contrast, the A18T mutation significantly reduced LLPS relative to WT (Figure 2), similar to the effect of V16I. However, V16I had a stronger effect on LLPS compared to A18T, despite having the same sequence complexity (of 0.912), which indicates that residue‐specific factors such as physicochemical properties and/or structural propensities also contribute to LLPS, in addition to sequence complexity. Nevertheless, the significant reduction of α‐syn LLPS by the complexity‐enhancing PD‐associated mutation A18T implicates sequence complexity in the pathogenicity of α‐syn.

We did not observe any changes in droplet appearance for any of the α‐syn variants, on imaging at longer (than 4 h) timepoints (Figure S11a). This is consistent with the fact that α‐syn droplets forming under our experimental conditions mature very quickly (Figure S2). However, there was a steady increase in turbidity of all LLPS variants over time (Figure S11b), which can be attributed to the ongoing fibril formation that is known to follow phase separation of α‐syn (Ray et al., 2020; Hardenberg et al., 2021; Sawner et al., 2021).

Therefore, by making subtle complexity‐enhancing changes to the sequence of α‐syn, we were able to control its LLPS over a wider dynamic range than possible with previously studied variants (i.e., E46K and A53T (Ray et al., 2020), neither of which affects sequence complexity). We next sought to use our designed (and patient) variants to investigate the relationship between LLPS and fibril formation of α‐syn.

2.3. Relationship between LLPS and fibrillation of α‐syn

LLPS of α‐syn is followed by a liquid‐to‐solid transition that includes the formation of amyloid fibrils (fibrillation), which can be monitored by the thioflavin T (ThT)‐binding assay (Ray et al., 2020; Hardenberg et al., 2021; Sawner et al., 2021). When we monitored the increase in ThT fluorescence over time following LLPS of each variant at neutral pH (Figure S12), we found that the variants with greater propensity to phase separate formed fibrils faster, as indicated by their shorter half‐times of fibrillation (Figure 3). The positive correlation between rate of fibrillation and propensity to phase separate suggests that LLPS can be a key determinant of amyloid formation under conditions promoting phase separation (i.e., in presence of PEG, ‘LLPS conditions’). This correlation was robust to changes in pH (Figure S13), further supporting the capacity of LLPS to promote fibrillation. Interestingly, despite exhibiting no measurable LLPS at any pH, the –LCD1&2 variant eventually formed fibrils in the presence of PEG, which demonstrates that LLPS is not required for fibrillation of α‐syn even under conditions that promote phase separation.

FIGURE 3.

FIGURE 3

(a) Fibrillation half‐times of different α‐syn variants subjected to aggregation under LLPS conditions. (b) The same plotted against droplet forming propensity of the variants, showing a negative correlation between the two—variants forming more droplets forms fibrils faster (shorter half‐times). Numbers in brackets represent number of LCDs. Dotted lines represent 95% confidence interval for linear regression. Data represent mean ± standard deviation (SD) for n = 3 independent experiments. Statistical significances are indicated by *p ≤ 0.05, **p ≤ 0.01, ***p ≤ 0.001, ****p ≤ 0.0001.

We next asked if mutations designed to selectively perturb LLPS also affect its fibrillation in conditions that do not promote phase separation. We therefore monitored the fibrillation kinetics of each α‐syn variant in the absence of PEG, where fibrillation was induced by the conventional method of continuous shaking (‘non‐LLPS conditions’). From the corresponding ThT‐binding profiles (Figure S14) and calculated half‐times of fibrillation (Figure 4a), we observed no correlation between the rate of fibrillation and either LLPS propensity (Figure 4b) or sequence complexity (Figure S15b). For example, whereas WT and LCD1* (with the same sequence complexity) have similar propensities to phase separate, they differ dramatically in rate of fibril formation. In contrast, whereas WT and –LCD2 have very different sequence complexities and propensities to phase separate, they form fibrils at similar rates. Therefore, by modifying sequence complexity, we could identify mutations that selectively perturb LLPS or fibrillation of α‐syn, which might allow dissection of their individual roles in vivo. Interestingly, the sporadic PD variant A18T (and designed variant –LCD1) accelerated α‐syn fibrillation, despite significantly reducing droplet formation. Also, the variant lacking both LCDs, despite being unable to phase separate, did form fibrils, albeit slower than the WT protein. These results indicate that the intrinsic determinants of α‐syn LLPS and fibrillation are different—while LLPS is highly sensitive to the sequence complexity of the protein, fibrillation is not.

FIGURE 4.

FIGURE 4

(a) Fibrillation half‐times of different LLPS variants subjected to aggregation under non‐LLPS conditions. (b) The same plotted against droplet forming propensity of the LLPS variants, showing a lack of correlation between the two. Numbers in brackets represent number of LCDs. The continuous box encloses variants that have similar fibrillation propensities despite drastically different phase‐separating tendencies, while the box with broken lines highlights variants with different fibrillation propensities despite similar phase‐separating tendencies. Data represent mean ± standard deviation (SD) for n = 3 independent experiments. Statistical significances are indicated by *p ≤ 0.05, **p ≤ 0.01, ***p ≤ 0.001, ****p ≤ 0.0001.

2.4. LLPS‐dependent vs. ‐independent fibrillation of α‐syn

Recent reviews have suggested that LLPS‐induced fibrillation of α‐syn is an alternate mode of amyloidogenesis, which might lead to fibrillar strains that are distinct from those formed in the absence of LLPS (Mukherjee et al., 2023; Mehra et al., 2021). We provide direct evidence for this divergence by comparing the morphology and proteolytic fingerprints of WT α‐syn fibrils obtained under LLPS and non‐LLPS conditions, which differ only in the presence of PEG (Figure 5). Not only did the two types of fibrils exhibit distinct morphologies (Figure 5a), they also produced different proteolytic fingerprints upon digestion with proteinase K (Figure 5b). Amyloids produced following LLPS were also significantly less resistant to digestion, indicating a more solvent‐exposed structure. The formation of structurally distinct amyloids in the presence versus absence of LLPS would require distinct assembly mechanisms, which is consistent with the lack of correlation between the rates of fibrillation via these two pathways (Figures 3 and 4). The significant molecular differences between LLPS and fibrillation further motivate efforts to dissect their individual roles in disease.

FIGURE 5.

FIGURE 5

(a) TEM images and (b) proteolytic fingerprints, of WT α‐syn fibrils produced under LLPS and non‐LLPS conditions. Scale bar = 100 nm.

3. DISCUSSION

LLPS, which involves the metastable de‐mixing of macromolecules into liquid‐like droplets, has recently been implicated as a regulator of fibril formation of amyloidogenic proteins associated with disease (Zbinden et al., 2020). α‐Syn is an amyloidogenic protein whose fibril formation is known to contribute to the pathology of PD and other synucleinopathies. Therefore, since the discovery of its propensity to undergo LLPS (Ray et al., 2020; Hardenberg et al., 2021), there has been significant interest in addressing the potential role of α‐syn LLPS in fibrillation. A gradual liquid‐to‐solid transition into fibrillar aggregates has been shown to follow α‐syn LLPS, and a variety of perturbations have been found to simultaneously enhance fibrillation and LLPS of α‐syn—suggesting LLPS to be an alternate nucleation mechanism in the fibrillation pathway (Mukherjee et al., 2023). However, the intrinsic drivers of LLPS itself remain largely unknown, without which it is difficult to ascertain its biological significance. Moreover, the lack of strategies to selectively perturb α‐syn LLPS complicates dissection of the individual roles of LLPS and fibrillation in disease.

In this paper, using a combination of carefully designed mutations that target the two LCDs of α‐syn, we demonstrate that low sequence complexity is one key intrinsic driver of α‐syn LLPS. To test the role of sequence complexity in α‐syn LLPS, we introduced chemically subtle, complexity‐enhancing point mutations in the two LCDs of α‐syn (to make the protein sequence progressively more complex without altering its physicochemical or structural properties), and studied the ability of the resulting variants to phase separate relative to the WT. We found that α‐syn's propensity to phase separate decreases with increasing sequence complexity, which was also reflected in relevant patient mutations (Figure 2). Note that the dramatic reduction in α‐syn LLPS by the extremely subtle, complexity‐enhancing V16I mutation (in variant –LCD1), and its reversal by another adjacent V15I mutation (in variant LCD1*), underscores the exquisite sensitivity of α‐syn phase separation to sequence complexity. Although the role of LCDs in protein LLPS has typically been attributed to their unique amino acid compositions (Zbinden et al., 2020), our results demonstrate that the low sequence complexity of the LCDs can itself be a driver of LLPS.

Furthermore, leveraging the differences in LLPS propensities among different α‐syn variants, we demonstrate that fibrillation of α‐syn does not necessarily correlate with its propensity to phase separate (Figure 4b). In doing so, we identify mutations that selectively perturb α‐syn LLPS (–LCD2) or fibrillation (LCD1*), which should allow dissection of their individual roles in vivo. It is interesting to note that previously studied fibrillation‐promoting patient mutations of α‐syn (i.e., E46K and A53T), were both found to increase LLPS (Ray et al., 2020), suggesting a pathological role of α‐syn LLPS in PD. However, in this work, we identified two patient variants—E83Q and A18T, which do not increase LLPS despite accelerating fibrillation; in fact, A18T reduces LLPS. This indicates that the role of LLPS in pathological fibrillation of α‐syn, and hence in PD, might be more complex than previously appreciated.

Overall, our results establish that low sequence complexity is a key driver of α‐syn phase separation but not necessarily fibrillation. We speculate that low sequence complexity contributes to LLPS by enabling a variety of distinct intermolecular contacts with similar energy, promoting dynamic self‐association and preventing the rapid adoption of a unique and stable conformational state. Similar phenomena have been implicated in molten globule proteins that likewise involve protein condensation without the formation of a unique structure (Ptitsyn, 1995). Conversely, increasing sequence complexity might reduce the number of intermolecular contacts that have similar energy, preventing the coexistence of many conformational states, which might be required for dynamic self‐assembly. Regardless of the molecular mechanism, our results highlight actionable design principles for controlling LLPS using sequence complexity, which can also be applied to decouple LLPS and fibrillation. We therefore believe that the variants we generated by these principles will enable future studies to distinguish the cellular/in vivo effects of α‐syn LLPS from those of its amyloid formation, and can also form the basis for disentangling LLPS and amyloid formation of other phase‐separating amyloidogenic proteins similar to α‐syn.

4. MATERIALS AND METHODS

4.1. Computational tools used in the study

To design mutations in the low‐complexity domains (LCDs) of α‐syn that would not alter physicochemical or structural properties of the protein, we selected substituent amino acids that have the same charge as the ones being replaced (neutral), and ensured that their hydrophobicity and α‐helix preferences were as close as possible to the ones being replaced. The overall hydrophobicity and charge of each resulting variant were calculated using the GRAVY (www.gravy-calculator.de) and Prot pi (www.protpi.ch/Calculator/ProteinTool) online calculators respectively. The helix‐forming propensity was obtained from the α‐helix calculator by Deleage and Roux (1987) in ProtScale (web.expasy.org/protscale), and disorder was calculated using IUPred2A (Mészáros et al., 2018) (iupred2a.elte.hu). After ensuring that the introduced mutations did not significantly alter any of these properties of the protein, their effects on sequence complexity were checked using the SMART prediction tool (Letunic & Bork, 2018) (smart.embl-heidelberg.de). Disease mutations were also similarly analyzed.

4.2. Design strategy of LLPS variants using SMART

SMART (Simple Modular Architecture Research Tool) is a freely available software that engages the well‐known SEG algorithm (Wootton, 1994; Wootton & Federhen, 1993, 1996) to predict LCDs in protein sequences. The SEG algorithm classifies protein segments as LCDs based solely on their compositional complexity. Compositional complexity of a protein segment is determined by the count of unique amino acids in that specific segment, irrespective of sequence patterns or repetition (Wootton & Federhen, 1996). Mathematically, compositional complexity of a subsequence of length L, is defined by K=1Llog20L!i=120ni!, where ni is the number of occurrences of each of the 20 different amino acids in the given segment, with 0niL and i=120ni=L (Wootton, 1994). As the number of distinct amino acids in a given segment of length L increases, one or more ni values decrease, resulting in a smaller denominator within the logarithmic term in K. Consequently, the logarithmic term, and hence the compositional complexity of the segment, increases with an increasing number of distinct amino acids in that segment. Importantly, the compositional complexity of a given segment remains the same for the same set of ni values (representing the count of different amino acids) regardless of the specific identities of the amino acids (i).

To test the role of sequence complexity in α‐syn LLPS, we designed subtle missense mutations in the two LCDs of the protein (LCD1 and LCD2), such that they increase sequence complexity of the protein while minimally perturbing its structural and physicochemical properties. The LCD1 region of WT α‐syn (residues 10–23) is composed of six different amino acids—four Ks, four As, two Es, two Vs, one G, and one T. Accordingly, K for this region is K1=114log2014!4!.4!.2!.2!.1!.1! Replacing one of the six different amino acids in LCD1 with an amino acid that doesn't exist in this segment is expected to increase compositional complexity of the segment by increasing the number of distinct constituent amino acids (and consequently lowering the value of the denominator within the logarithmic term in K 1). Accordingly, we introduced a single V‐to‐I (valine‐to‐isoleucine) mutation in this region (V16I); and found it sufficient to increase sequence complexity of this region above the threshold for identification as a LCD by SMART (Figure 1, variant –LCD1). We chose a V‐to‐I mutation in particular as it introduces an extremely subtle change in the protein (adds a single methyl group on a single hydrophobic residue in a 140‐residue protein), which should minimally perturb the structural and physicochemical properties of the protein. This was confirmed from computational analyses, which predicted minimal changes to the protein's charge and hydrophobicity (Table S1), as well as its propensity for disordered and helical structures (Figure S1a,c). Note that changing one of the two valines in LCD1 to isoleucine (in case of V16I) increases K 1 by lowering the denominator within the logarithm; however, changing both of the two valines to isoleucines in this region would restore the original value of the denominator and consequently K 1 (same set of n i values as for the WT protein). Therefore, to test if restoring the original sequence complexity can rescue LLPS behavior of the WT protein, we designed another variant in which the increased local complexity of the LCD1 region by the V16I mutation was reversed by introducing another V‐to‐I mutation at position 15 (Figure 1, variant LCD1*). As a result, this variant had the same sequence complexity as the WT protein, but a slightly different amino acid sequence (with two Is instead of two Vs at positions 15 and 16 within the LCD1 region).

The LCD2 region of WT α‐syn (residues 63–78) has five different amino acids: six Vs, three As, three Gs, three Ts, and one N. Accordingly, K for this region is: K2=116log2016!6!.3!.3!.3!.1! Following the same principle as that used for designing the –LCD1 variant, we first introduced a single V‐to‐I mutation at position 70, to increase complexity of this region (by lowering the value of the denominator within the logarithmic term in K 2). However, a single substitution was not sufficient to increase complexity of this relatively longer LCD above the threshold for detection as a LCD by SMART. Therefore, we paired another G‐to‐P mutation at position 68 to lower K 2 further. The combined changes (G68P and V70I) were sufficient to increase complexity of the LCD2 region above the threshold for identification as a LCD by SMART (Figure 1, variant –LCD2). Then we combined the –LCD1 and –LCD2 substitutions to make a variant with no predicted LCDs (Figure 1, variant –LCD1&2).

4.3. Quantification of sequence complexity of LLPS variants

For the purpose of our study, we defined sequence complexity of α‐syn (S) as the sum of the local compositional complexities of the two segments corresponding to its two LCDs. Therefore S = K 1 + K 2. Note that for the E83Q variant of α‐syn used in our study, the second LCD spans residue 63–83 instead of 63–78 as for the WT (see Figure 1). Hence, for the sake of maintaining uniformity in our quantification parameter, we used the local compositional complexity of this stretch (K2 ' ) in place of K 2 in the expression of S.

Therefore S = K 1 + K 2 ' , where K 1 and K 2 ' are the local compositional complexities of segments 10–23 and 63–83 in each of the α‐syn variants used in our study.

Accordingly, the calculations of sequence complexities for the variants used in our study, have been tabulated below:

Mutation/name of variant Compositions of segments 10–23 and 63–83 K 1 (of segment 10–23) K 2′ (of segment 63–83) S = K 1 + K 2
E83Q

10–23: 4K, 4A, 2E, 2V, 1G, 1T

63–83: 7V, 4T, 3A, 3G, 2Q, 1N, 1K

114log2014!4!.4!.2!.2!.1!.1!=0.416
121log2021!7!.4!.3!.3!.2!.1!.1!=0.467
0.883
None/WT

10–23: 4K, 4A, 2E, 2V, 1G, 1T

63–83: 7V, 4T, 3A, 3G, 1Q, 1N, 1K, 1E

114log2014!4!.4!.2!.2!.1!.1!=0.416
121log2021!7!.4!.3!.3!.1!.1!.1!.1!=0.479
0.895
V15I, V16I/LCD1*

10–23: 4K, 4A, 2E, 2I, 1G, 1T

63–83: 7V, 4T, 3A, 3G, 1Q, 1N, 1K, 1E

114log2014!4!.4!.2!.2!.1!.1!=0.416
121log2021!7!.4!.3!.3!.1!.1!.1!.1!=0.479
0.895
A18T

10–23: 4K, 3A, 2T, 2E, 2V, 1G

63–83: 7V, 4T, 3A, 3G, 1Q, 1N, 1K, 1E

114log2014!4!.3!.2!.2!.2!.1!=0.433
121log2021!7!.4!.3!.3!.2!.1!.1!.1!=0.479
0.912
V16I/−LCD1

10–23: 4K, 4A, 2E, 1V, 1G, 1T, 1I

63–83: 7V, 4T, 3A, 3G, 1Q, 1N, 1K, 1E

114log2014!4!.4!.2!.1!.1!.1!.1!=0.433
121log2021!7!.4!.3!.3!.2!.1!.1!.1!=0.479
0.912
G68P, V70I/−LCD2

10–23: 4K, 4A, 2E, 2V, 1G, 1T

63–83: 6V, 3A, 4T, 2G, 1N, 1P, 1I, 1K, 1Q, 1E

114log2014!4!.4!.2!.2!.1!.1!=0.416
121log2021!6!.3!.4!.2!.1!.1!.1!.1!.1!.1!=0.527
0.943
V16I, G68P, V70I/−LCD1&2

10–23: 4K, 4A, 2E, 1V, 1G, 1T, 1I

63–83: 6V, 3A, 4T, 2G, 1N, 1P, 1I, 1K, 1Q, 1E

114log2014!4!.4!.2!.1!.1!.1!.1!=0.433
121log2021!6!.3!.4!.2!.1!.1!.1!.1!.1!.1!=0.527
0.960

4.4. Site‐directed mutagenesis

The recombinant bacterial plasmid pET‐28a, containing a kanamycin resistant gene and the gene for α‐syn, was used as a template for site‐directed mutagenesis (SDM) to produce all the mutants apart from –LCD1&2, which was obtained from Twist Bioscience (USA). For every other mutant, mutagenic primers were designed (see below) and the mutagenesis was done using either the Phusion High‐Fidelity PCR Kit (ThermoFisher Scientific, USA) or the QuikChange Lightning Site‐Directed Mutagenesis Kit (Agilent Technologies, USA), following respective manufacturers' protocols. The Simply Amp Thermal Cycler (ThermoFisher Scientific, USA) was used to carry out all PCR. When using the Phusion kit, DpnI digestion of the PCR product was done using 1 μL of DpnI added to 50 μL reaction mixture and incubating for 1 h at 37°C. This was followed by PCR clean‐up using the GeneJet PCR Purification Kit (ThermoFisher Scientific, USA), following manufacturer's protocol. The resulting DNA was then transformed into competent DH5‐alpha cells, which were plated on kanamycin selective LB‐agar plates and incubated overnight for growth of colonies containing the desired mutation. For PCR using the Agilent kit, DpnI digestion and subsequent transformation into XL 10‐Gold Ultracompetent Cells was done using reagents provided in the kit, following manufacturer's protocol. Single colonies resulting from successful PCR and transformations were grown overnight in 5 mL cultures, and DNA from them were extracted using the GeneJET Plasmid Miniprep kit following manufacturer's protocol. The resulting mutations were confirmed by Sanger sequencing of the extracted DNA samples (through Eton Bioscience).

The primers used for the SDM reactions are as follows:

Mutant Forward/reverse primers Kit used
A18T GCCAAGGAGGGAGTTGTGGCTACTGCTGAGAAAACCAAACAGGGTG/ Phusion
CACCCTGTTTGGTTTTCTCAGCAGTAGCCACAACTCCCTCCTTGGC
V16I (−LCD1) GGACTTTCAAAGGCCAAGGAGGGAGTTATCGCTGCTGCTGAGAAAACCAAACAGGG/ Phusion
CCCTGTTTGGTTTTCTCAGCAGCAGCGATAACTCCCTCCTTGGCCTTTGAAAGTCC
G68P, V70I (−LCD2) CCAAAGAGCAAGTGACAAATGTTGGACCAGCAATCGTGACGGGTGTGACAGCAGTAG/ Phusion
CTACTGCTGTCACACCCGTCACGATTGCTGGTCCAACATTTGTCACTTGCTCTTTGG
V15I, V16I (LCD1*) TTCTCAGCAGCAGCTATAATTCCCTCCTTGGCCTTTGAAAGTCCT/ Agilent
AGGACTTTCAAAGGCCAAGGAGGGAATTATAGCTGCTGCTGAGAA
E83Q GTAGCCCAGAAGACAGTGCAGGGAGCAGGGAGCATT/ Agilent
AATGCTCCCTGCTCCCTGCACTGTCTTCTGGGCTAC

4.5. Expression and purification of α‐syn variants

Recombinant WT α‐syn and its mutants were individually expressed in the Escherichia coli BL21 (DE3) cells transformed with the respective plasmids. Expression was induced using 1 mM of isopropyl β‐d‐1‐thiogalactopyranoside (IPTG) at an OD of 0.5–0.6. The cultures were incubated at 37°C with shaking at 225 rpm for 4 h after addition of IPTG. Cells were then harvested by centrifugation, and stored at −80°C until purification of α‐syn by a previously reported non‐chromatographic method (Mahapatra et al., 2021; Shaltiel‐Karyo et al., 2013). Briefly, the cell pellets were resuspended in Tris buffer (50 mM Tris, 10 mM EDTA and 150 mM NaCl, pH 8) and boiled for 10 min, after adding 100 mM phenylmethylsulfonyl fluoride (PMSF). Lysed cells were then centrifuged and the supernatant was removed into a fresh tube. Streptomycin sulfate (136 μL of 10% solution per mL supernatant) and glacial acetic acid (228 μL per mL supernatant) were added to it, followed by additional centrifugation at 12,000 g for 5 min at 4°C. The supernatant was removed again and then precipitated with solid ammonium sulfate (up to 50% saturation, as calculated using the online Ammonium Sulfate Calculator from EnCor Biotechnology Inc.) at 4°C. The precipitated protein was collected by centrifugation for 30 min at 12,000 g, and the pellet was washed once with 50% ammonium sulfate solution. The washed pellet was re‐suspended in minimum volume of 100 mM ammonium acetate (to form a cloudy solution) and precipitated by adding an equal volume of 100% ethanol at room temperature. Ethanol precipitation was repeated once more, followed by freezing of the obtained pellet, and subsequent lyophilization using a FreeZone lyophilizer by Labconco (USA).

4.6. Preparation of low molecular weight forms of α‐syn variants

Low molecular weight (LMW) forms of all variants were prepared using a previously published protocol (Ray et al., 2020), with slight modifications. Lyophilized protein was dissolved in 20 mM sodium phosphate buffer (NaP) at pH 7, at 10‐12 mg/mL. If required, the protein was solubilized by the addition of a few drops of 0.2 N NaOH and the final pH was adjusted to 7 using 2 M HCl. The protein solution was then centrifuged at 15,000 rpm for 30 min at 4°C to remove insoluble aggregates. Thereafter, the supernatant was passed through a pre‐washed 100 kDa cut‐off filter (Amicon Ultra‐0.5 Centrifugal Filter Unit) to remove any high‐order aggregates. The flow‐through that is, the LMW fraction constituting majorly of monomeric α‐syn was collected, and the concentration was estimated by measuring the absorbance at 280 nm. The molar extinction coefficient (ε) used for calculating concentrations of all variants was 5960 M−1 cm−1 (obtained using Prot pi).

4.7. Protein labeling with NHS‐rhodamine

For the purpose of fluorescence microscopy, all samples were doped with 1% (v/v) of the respective rhodamine‐labeled proteins. To obtain the labeled proteins, purified variants of α‐syn were labeled with NHS‐rhodamine dye (ThermoFisher Scientific, USA) following the manufacturer's protocol. Briefly, 10× molar excess of dye (dissolved in DMSO) was added to the LMW protein, and the reaction was allowed to proceed at room temperature for 2 h in the dark. Excess unreacted dye was removed by dialysis against NaP (pH 7) at 4°C for 48 h, with 3–4 changes of buffer.

4.8. In vitro liquid–liquid phase separation

To induce liquid–liquid phase separation (LLPS), WT α‐syn and its variants, at a concentration of 100 μM, were suspended in NaP in presence of 150 mM NaCl (PBS), 1 mM sodium azide and 20% PEG 8000, at pH 7, 6 and 5. Reaction mixtures prepared under these conditions (LLPS conditions) were added to the wells of half‐area 96‐well plates in triplicates, and incubated in a moist chamber at 37°C. For droplet imaging and quantification, samples were prepared with 1% (v/v) of labeled proteins, and incubated for up to 4 hours. For monitoring fibril formation by the thioflavin T (ThT)‐binding assay (see Appendix S1.9), samples without labeled proteins were incubated in presence of 25 μM ThT under the same conditions.

4.9. Fluorescence microscopy and image quantification

Droplet formation by LLPS variants of α‐syn was visualized under a ‘EVOS FL Auto 2’ fluorescence microscope (ThermoFisher Scientific, USA), in the fluorescence mode, using the EVOS™ Light Cube, RFP 2.0 (excitation: 542/20, emission: 593/40). Appropriate buffer controls for each experiment were kept for baseline fluorescence settings, and all the images were obtained at a resolution of 2080 × 1552 pixels at 32‐bit depth. Samples were either viewed through the LWD EVOS™ 10× Objective (fluorite, NA = 0.3, WD = 7.13 mm) or the LWD EVOS™ 60× Objective (fluorite, NA = 0.75, WD = 2.2 mm), for capturing low and high magnification images respectively.

Quantification of droplet formation was done from the low magnification (10×) images of 4‐h samples, using Fiji (ImageJ). For every image, at first the scale was set for particle size measurements using the scale bar from the microscope. Then the image was converted to an 8‐bit image, followed by thresholding to include only droplets in the particle size measurements. The sizes (areas) of all highlighted droplets in the field of view were then measured, using the ‘Analyze particles’ module, setting the lower limit of size at 3.14 μm2 (radius = 1 μm) and keeping circularity within 0–1. Individual areas thus obtained were used to estimate diameters of the droplets and plot the corresponding size distributions. Fractional area covered by droplets and number of droplets were also obtained from the analyses, which were multiplied to obtain the percentage of total area covered by droplets in each of the samples.

4.10. Confocal microscopy and fluorescence recovery after photobleaching

Fluorescence recovery after Photobleaching (FRAP) studies were performed using a laser scanning confocal microscope (Zeiss LSM 710, inverted) equipped with a Plan‐Apochromat 63X/1.4 NA oil immersion objective (WD = 0.19 mm). After 1 h of incubation of all α‐syn variants under LLPS conditions, droplet formation was first confirmed by fluorescence microscopy (EVOS FL Auto 2), and then the wells containing droplets were subjected to FRAP experiments in the confocal microscope. Intensity was recorded from three different region of interests (ROIs) of constant radii—actual bleaching region (ROI‐1), reference region on same/neighboring droplet (ROI‐2) at a different location to correct for passive bleaching during laser exposure, and a region outside the droplet in the dark (ROI‐3) to correct for background fluorescence intensity. The selected ROI‐1 was then bleached with 50% laser power, using a 561 nm DPSS 561‐10 laser and emission intensities from all ROIs were recorded for 100 s (when fluorescence emission from ROI‐1 reached a plateau for the WT variant). All measurements were performed at room temperature.

FRAP data analyses were performed according to previous studies (Ray et al., 2020; Taylor et al., 2019). First, all fluorescence recovery curves were constructed from the total intensity values in the ROI for each frame corrected for the background and passive bleaching. To calculate corrected and normalized fluorescence intensity, I(n), Equation (1) was used:

In=ItIbr (1)

where, I(t) = fluorescence intensity at time t, I(b) = background fluorescence intensity, and rate of photo‐bleaching (r) = Ic/Ic0 [Ic0 = fluorescence intensity of the ROI‐2 before photo‐bleaching; Ic = fluorescence intensity of the ROI‐2 after photo‐bleaching].

The normalized and background corrected fluorescence recovery curves thereby obtained were fitted using the following single exponential recovery function (Equation (2)) in the OriginPro8.5 software (OriginLab, USA):

It=A1exptτ+C (2)

where, τ is the fluorescence recovery time constant, ‘A’ corresponds to the mobile fraction of the fluorescent probe and ‘C’ is the y‐intercept of the recovery curve. Note that mobile fraction (MF) is depicted by: MF=IIcIc0Ic.

4.11. Thioflavin T‐binding assay

ThT‐binding assay was used for monitoring the fibrillation of all variants of α‐syn in the presence and absence of LLPS. For fibrillation under LLPS conditions, all variants at a concentration of 100 μM, were suspended in NaP in presence of 150 mM NaCl, 1 mM sodium azide, 25 μM ThT and 20% PEG 8000, at pH 7, 6 and 5. Samples were prepared and loaded in triplicates into half‐area 96‐well plates, and incubated under quiescent conditions in a moist chamber at 37°C. For fibrillation under non‐LLPS conditions, all variants at a concentration of 100 μM, were suspended in NaP in presence of 150 mM NaCl and 25 μM ThT, at pH 7. Samples were prepared and loaded in triplicates into half‐area 96‐well plates, and shaken continuously at 800 rpm at 37°C in a ThermoMixer C (Eppendorf, Germany). At regular time intervals, the plates were read using a Synergy H1 microplate reader from BioTek (USA), to monitor the changes in ThT fluorescence over time, usually for up to a month. Since all replicates of the −LCD1&2 variant under LLPS conditions did not show saturation of ThT signal within a month, they were monitored for an additional 2 weeks until saturation. The steady state fluorescence of ThT was measured using excitation at 440 nm and emission at 485 nm. The resulting ThT‐binding profiles were then fit into the Boltzmann equation (Equation (3)) as follows:

y=y0+A1+exptt1/2dx (3)

where y 0 is the signal baseline at the beginning, A is the total increase in fluorescence signal, (1/dx) is the growth rate constant, and t12 is the mid‐point of the transition, that is, half‐time of fibrillation.

Curve fitting was done in the OriginPro8.5 software (OriginLab, USA), and corresponding half‐times were calculated for further analyses.

4.12. Preparation of pre‐formed fibrils of α‐syn

To prepare WT α‐syn fibrils under LLPS conditions, the un‐labeled LMW protein was incubated at a concentration of 100 μM in NaP at pH 7, in presence of 150 mM NaCl, 1 mM sodium azide and 20% PEG 8000, under quiescent conditions for a month. To prepare WT α‐syn fibrils under non‐LLPS conditions, the un‐labeled LMW protein was incubated at a concentration of 100 μM in NaP at pH 7, in presence of 150 mM NaCl, under constant agitation at 800 rpm in a ThermoMixer C (Eppendorf, Germany), for a month. Fibril formation in the resulting turbid solutions was checked by ThT‐binding fluorescence, and samples were centrifuged at 15,000 rpm for 30 min to pellet down fibrils. Clear supernatants from the top were carefully removed and their volumes determined. For the non‐LLPS fibril sample, protein concentration of the supernatant was measured by recording absorbance at 280 nm (OD280); and quantity of fibrils formed was determined (in micrograms) by subtracting the amount of protein left in the supernatant (volume times concentration) from the initial amount of protein. The pellet was then resuspended in required volume of NaP (pH 7) to obtain a final concentration of 1 mg/mL protein. For the fibril sample produced under LLPS conditions, determining protein concentration by OD280 measurement was not feasible due to absorption of PEG at 280 nm. Therefore, fibril pellet was resuspended in a volume of NaP (pH 7) that was equal to the supernatant volume, so as to obtain ≤1.4 mg/mL (100 μM) of LLPS fibrils. Both LLPS and non‐LLPS fibril samples were aliquoted and stored at −80°C until further use.

4.13. Transmission electron microscopy

Five microliters of pre‐formed fibril (PFF) solution (~1 mg/mL) was spotted on a freshly glow‐discharged 300‐mesh carbon coated formvar grid (Electron Microscopy Sciences, USA) and incubated for 3 min. Excess solution was soaked off using a filter paper, and the grid was then washed twice Milli‐Q water. Five microliters of 1% (w/v) uranyl acetate solution was added onto the grid and allowed to sit for 2 min before soaking off excess with a filter paper. All grids were air‐dried, and imaged using a Tecnai Biotwin Spirit Transmission Electron Microscope (TEM), operated at 80 kV. Images were captured using an AMT 1k × 1k camera at 43,000× and 135,000× magnifications, using the TIA imaging system provided with the instrument.

4.14. Preparing LLPS fibrils for proteolytic fingerprinting

Proteolytic fingerprinting of fibrils involves subjecting fibril samples to limited proteolysis by proteinase K (or PK) followed by running a SDS‐PAGE with digested samples to identify the characteristic band patterns (position and relative intensity) obtained on digestion. As presence of PEG in LLPS fibril samples interferes with running of the protein gel and creates smeared bands (data not shown), these particular fibril samples were subjected to an additional wash step prior to being used for proteolytic fingerprinting experiments. After isolating the LLPS fibrils as pellets using high‐speed centrifugation, the obtained pellet was resuspended in 500 μL of NaP buffer, and passed through a pre‐washed 100 kDa cut‐off spin column (Amicon Ultra‐0.5 Centrifugal Filter Unit). The residual volume of sample retained in the spin column, containing fibrillar aggregates (>100 kDa), was then washed twice more with 500 μL of buffer. Finally, the fibrillar aggregates retained in the spin column, free of most of the PEG contamination after three wash steps, were recovered by inverting the spin column and centrifuging it once more. The sample thus obtained was then subjected to proteolytic fingerprinting experiments (see below).

4.15. Limited proteolysis using proteinase K

Limited proteolysis of protein samples with PK generates distinct peptide fragments depending on which epitopes of the protein are accessible to the enzyme. Suitable amounts of WT α‐syn PFFs formed under LLPS and non‐LLPS conditions were mixed with 0, 0.01, 0.1 and 1 μg/mL of PK (20 mg/mL) in NaP to a final volume of 12 μL, and incubated at 37°C for 10 min. PK digestion was stopped with 1 mM PMSF. Reaction samples were then boiled with equal volumes of Novex™ Tricine SDS sample buffer (2×) at 85°C for 2 min, and then centrifuged at high speed for 5 min. Samples were then run and resolved on Novex™ 16% Tricine gels (1.0 mm, Mini Protein Gels) supplied by Invitrogen, to obtain respective proteolytic fingerprints.

4.16. Data plotting and statistical data analyses

All experimental data were plotted and fit using OriginPro 8.5 or GraphPad Prism 9 software. All statistical data analyses were performed using one‐way ANOVA (Tukey's post hoc) in the GraphPad Prism 9 software, where ns: nonsignificant, *p ≤ 0.05, **p ≤ 0.01, ***p ≤ 0.001, and ****p ≤ 0.0001.

AUTHOR CONTRIBUTIONS

Robert Newberry: Funding acquisition; writing – review and editing; methodology; formal analysis; project administration; supervision; resources; data curation. Anindita Mahapatra: Conceptualization; writing – original draft; writing – review and editing; investigation; methodology; formal analysis; project administration; data curation.

CONFLICT OF INTEREST STATEMENT

There are no conflicts to declare.

Supporting information

Appendix S1: Supporting Information

PRO-33-e4951-s001.pdf (1.2MB, pdf)

ACKNOWLEDGMENTS

This work was supported by grants from the NIH (R00‐NS116679) and the Welch Foundation (F‐2116‐20220331). Transmission electron microscopy and confocal microscopy were performed at the Center for Biomedical Research Support (CBRS) Microscopy and Imaging Facility at UT Austin (RRID:SCR_021756).

Mahapatra A, Newberry RW. Liquid–liquid phase separation of α‐synuclein is highly sensitive to sequence complexity. Protein Science. 2024;33(4):e4951. 10.1002/pro.4951

Review Editor: Jean Baum

Contributor Information

Anindita Mahapatra, Email: anindita.sphs@utexas.edu, Email: rnewberry@utexas.edu.

Robert W. Newberry, Email: rnewberry@utexas.edu.

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Supplementary Materials

Appendix S1: Supporting Information

PRO-33-e4951-s001.pdf (1.2MB, pdf)

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