Literature DB >> 32243126

Switchable Membrane Remodeling and Antifungal Defense by Metamorphic Chemokine XCL1.

Acacia F Dishman1, Michelle W Lee2, Jaime de Anda2, Ernest Y Lee2,3, Jie He4, Anna R Huppler4, Gerard C L Wong2, Brian F Volkman1.   

Abstract

Antimicrobial peptides (AMPs) are a class of molecules which generally kill pathogens via preferential cell membrane disruption. Chemokines are a family of signaling proteins that direct immune cell migration and share a conserved α-β tertiary structure. Recently, it was found that a subset of chemokines can also function as AMPs, including CCL20, CXCL4, and XCL1. It is therefore surprising that machine learning based analysis predicts that CCL20 and CXCL4's α-helices are membrane disruptive, while XCL1's helix is not. XCL1, however, is the only chemokine known to be a metamorphic protein which can interconvert reversibly between two distinct native structures (a β-sheet dimer and the α-β chemokine structure). Here, we investigate XCL1's antimicrobial mechanism of action with a focus on the role of metamorphic folding. We demonstrate that XCL1 is a molecular "Swiss army knife" that can refold into different structures for distinct context-dependent functions: whereas the α-β chemokine structure controls cell migration by binding to G-Protein Coupled Receptors (GPCRs), we find using small angle X-ray scattering (SAXS) that only the β-sheet and unfolded XCL1 structures can induce negative Gaussian curvature (NGC) in membranes, the type of curvature topologically required for membrane permeation. Moreover, the membrane remodeling activity of XCL1's β-sheet structure is strongly dependent on membrane composition: XCL1 selectively remodels bacterial model membranes but not mammalian model membranes. Interestingly, XCL1 also permeates fungal model membranes and exhibits anti-Candida activity in vitro, in contrast to the usual mode of antifungal defense which requires Th17 mediated cell-based responses. These observations suggest that metamorphic XCL1 is capable of a versatile multimodal form of antimicrobial defense.

Entities:  

Keywords:  XCL1; antifungal; antimicrobial; chemokines; metamorphic proteins; small-angle X-ray scattering

Mesh:

Substances:

Year:  2020        PMID: 32243126      PMCID: PMC7258946          DOI: 10.1021/acsinfecdis.0c00011

Source DB:  PubMed          Journal:  ACS Infect Dis        ISSN: 2373-8227            Impact factor:   5.084


Antimicrobial peptides (AMPs) are innate immune molecules that often exhibit a common antimicrobial mechanism of disrupting pathogen membranes, which leads to depolarization, leakage, and eventual cell death.[1,2] Examples of AMPs include cathelicidins, defensins, bacteriocins, histatins, protegrins, and, more recently, an increasing number of chemokines, which are more commonly thought of as signaling molecules.[2−8] Among the human chemokines that exhibit antibacterial, antifungal, or antiviral properties are CCL20,[9] CXCL4,[10] CCL28,[11] CXCL17,[12] and XCL1.[13] Chemokines are a family of ∼50 small, secreted proteins that direct cellular migration by binding to glycosaminoglycans (GAGs) to form concentration gradients, and by binding to G-protein coupled receptors (GPCRs) to induce pro-migratory cellular changes. All members of the chemokine family share a conserved tertiary structure consisting of a three-stranded antiparallel β-sheet and C-terminal α-helix. XCL1 provides a unique opportunity to demonstrate in an unambiguous manner the relationship between sequence, secondary and tertiary structure, and distinct forms of immune activity in a chemokine. XCL1 is unique among chemokines because it is a metamorphic protein, meaning that it reversibly switches between two or more native structures.[14,15] Thus, by using XCL1 as a model system, it becomes possible to interrogate what happens to signaling activity or membrane remodeling activity when the organization of secondary structure changes without changing the amino acid content. While most chemokines bind to GAGs and GPCRs using a single structure, XCL1 partitions these roles between its native states, which are (1) the highly conserved chemokine fold that binds its target receptor XCR1 and (2) a novel four-stranded β-sheet dimer that binds to GAGs.[16,17] Of XCL1’s two native conformations, the alternative β-sheet structure displays strong antibacterial activity.[13] Here, we investigated XCL1’s ability to remodel membranes like AMPs as a function of its available conformational states, since previous work has attributed the bactericidal activity of XCL1 to its ability to permeabilize bacterial membranes.[13] We applied a recently developed machine learning classifier capable of reliably predicting membrane-active α-helical peptide sequences to several prototypical chemokines.[18] The classifier identified the α-helices of CCL20 and CXCL4 as motifs that impart membrane activity to these chemokines. Surprisingly, however, the cognate helix of XCL1 is not predicted to induce negative Gaussian curvature (NGC) in membranes. We used synchrotron small-angle X-ray scattering (SAXS) to measure membrane curvature deformations induced by XCL1 and a panel of XCL1 structural variants in membranes modeling Escherichia coli, Candida albicans, and mammalian cells. We found that XCL1 generates NGC in E. coli-like model membranes in a manner that depends on its metamorphic structural state: The β-sheet structure exhibits strong remodeling activity, while the α–β chemokine structure does not. Whereas antifungal defense usually requires clearance by Th17 mediated cell-based immune responses, we find that XCL1 induces NGC in Candida-like membranes via a structural motif distinct from classical α–β chemokines, and exhibits anti-Candida activity in vitro. This suggests the possibility of a versatile multimodal antifungal defense associated with this metamorphic chemokine.

Results and Discussion

The presence or absence of membrane activity in different folded states of XCL1 is central to the manner in which different immune functions are programmed into this metamorphic chemokine. A large body of work has found that specific physicochemical properties, including positive net charge and amphipathicity, of AMPs contribute to their bactericidal activity by facilitating electrostatic and hydrophobic interactions between the peptide and cell membranes.[19] These interactions result in membrane destabilization, which can manifest in pore formation,[20−23] blebbing,[24,25] and vesicle budding.[26] A topological requirement shared by many membrane-permeation processes is the induction of NGC in target membranes.[27] NGC, also known as saddle-splay curvature, can be seen in the hole of a transmembrane pore or the neck of a fusion pore: for a flat horizontal surface labeled by cardinal directions (north (N), east (E), south (S), west (S)), NGC can be generated by deforming the surface upward in the N and S directions and downward in the E and W directions. A broad range of studies identified a strong correlation between the ability of AMPs, AMP mutants, and synthetic AMP analogues to disrupt bacterial membranes and their capacity to generate NGC in membranes.[19,28−34]

XCL1 Lacks a Membrane Active α-Helix

Many antimicrobial peptides are thought to destabilize phospholipid bilayers by inducing NGC, a topological feature of membrane pores and blebs.[19,28−34] Previously, we developed a machine-learning support vector machine (SVM) classifier trained to identify α-helical peptide sequences with the ability to remodel membranes by generating NGC.[18] In recent work, we have shown that even though the SVM was trained on short α-helical peptide sequences, the classifier is able to identify the existence of membrane active segments within larger membrane active proteins.[35,36] This machine learning approach constitutes a new kind of bioinformatic analysis that is based on function rather than structural or sequence homology. We aimed to apply this approach to chemokines, by determining whether the ability to generate NGC can be found in the α-helical domain of the characteristic α–β chemokine fold. We assessed differences between the sequences of XCL1 and two other antimicrobial chemokines, CXCL4 and CCL20, using the SVM classifier to predict membrane active peptide subdomains.[18] This sequence-based approach allows us to score individual amino acid segments and identify α-helical (or disordered) regions that are potentially involved in membrane remodeling. We screened the chemokine sequences using a “moving window” scan to isolate individual segments of n amino acids. Each subsequence was scored by the SVM classifier with a σ-score corresponding to its probability to be membrane disruptive, P(+1). The mean σ-score for each amino acid position is an average of the scores for all the sequences in which that amino acid appears for a given window size n. A large positive σ-score (σ > 0.89) corresponds to a high probability of membrane activity (P(+1) > 0.95), while a negative σ-score (σ < 0) indicates a small probability of membrane activity (P(+1) < 0.50). The scores for each chemokine’s full sequence are visualized on a 2D probability map for different window sizes (Figure ). For CXCL4 and CCL20, only the α-helical C-terminal regions were predicted to have membrane remodeling ability. In contrast, the entire XCL1 sequence scored poorly for membrane activity (Figure ) even though XCL1 exhibits antimicrobial activity.[13] The individual α-helical sequence for CCL20 scored slightly higher than the CXCL4 α-helix (TWVKYIVRLLSK, σ = 1.0, P = 0.97; PLYKKIIKKLLE, σ = 0.72, P = 0.92, respectively), whereas the XCL1 α-helix scored significantly lower (TWVRDVVRSMDRK, σ = 0.13, P = 0.61). Although the tertiary α–β structure is similar between the three chemokines (Figure ), the machine-learning classifier approach was able to identify subtle differences in these sequences using its optimized physicochemical descriptors. The presence of a membrane active α-helix in CXCL4 and CCL20 is consistent with the antimicrobial character of these chemokines in their native α–β form and provides contrast to understand the minimal antimicrobial activity of XCL1 in its α–β conformation, with a membrane inactive α-helix. Given that the SVM classifier is optimized to predict membrane active α-helical sequences and no membrane activity is identified in the XCL1 α-helix cognate to the helices in the other α–β chemokines examined, we hypothesize that the membrane remodeling activity in XCL1 arises from its ability to switch into a β-sheet structure, since such membrane activity is not detectable by an α-helical classifier.
Figure 1

Machine learning based analysis indicates that XCL1’s α-helix has drastically reduced levels of membrane remodeling activity compared to those of antimicrobial chemokines CCL20 and CXCL4. At left, the mean σ-scores for a window size of 30 are projected on the 3D structures of CCL20, CXCL4, and XCL1. Sequences of the helices are shown below each cartoon. At right, each chemokine’s full sequence is visualized on a 2D probability map, with helices highlighted by a white box. X axis, amino acid sequence. Y axis, window size. Color, mean σ-score.

Machine learning based analysis indicates that XCL1’s α-helix has drastically reduced levels of membrane remodeling activity compared to those of antimicrobial chemokines CCL20 and CXCL4. At left, the mean σ-scores for a window size of 30 are projected on the 3D structures of CCL20, CXCL4, and XCL1. Sequences of the helices are shown below each cartoon. At right, each chemokine’s full sequence is visualized on a 2D probability map, with helices highlighted by a white box. X axis, amino acid sequence. Y axis, window size. Color, mean σ-score.

XCL1 Induces Negative Gaussian Curvature Necessary for Membrane Permeation in Membranes Modeling Bacterial, but Not Mammalian Cells

To understand the specific biophysical mechanisms driving XCL1’s ability to selectively kill bacteria, we employed synchrotron SAXS experiments to quantitatively characterize XCL1-induced curvature deformations in model cell membranes. Although AMPs can kill microbes via a range of mechanisms, it has been recently shown that what AMPs have in common is their ability to generate NGC in microbial membranes,[18] which is related to the ability to kill microbes through membrane disruptive modes such as pore formation and blebbing.[27,30,37,38] Since selectivity of AMP-induced killing is thought to arise in part from the ability to recognize differences in membrane lipid composition between microbes and host cells, we compared the curvature deformations induced by XCL1 in two different membranes: one modeling E. coli membranes and one modeling mammalian cell membranes. Small unilamellar vesicles (SUVs) with lipid compositions mimicking that of E. coli membranes and mammalian cell membranes were incubated with XCL1, and the resulting crystalline structures were characterized using SAXS. Bacterial membranes were modeled using a lipid composition of 1,2-dioleoyl-sn-glycero-3-[phospho-rac-(1-glycerol)]/1,2-dioleoyl-sn-glycero-3-phosphoethanolamine at a molar ratio of 20/80 (DOPG/DOPE 20/80). Mammalian cell membranes were modeled using a lipid composition of 1,2-dioleoyl-sn-glycero-3-phospho-l-serine/1,2-dioleoyl-sn-glycero-3-phosphoethanolamine/1,2-dioleoyl-sn-glycero-3-phosphocholine at a molar ratio of 20/40/40 (DOPS/DOPE/DOPC 20/40/40). XCL1 was incubated with the SUVs at protein/lipid charge ratios (P/L) of 1/2 and 1/1 (i.e., molar ratios of 1/85 and 2/85, respectively). XCL1 restructured E. coli-like membranes into phases rich in NGC (Figure A), while control samples of the SUVs alone displayed a broad characteristic feature consistent with the form factor expected for unilamellar vesicles (Supplemental Figure 1). SAXS spectra for SUVs with the E. coli-like membrane composition that were exposed to XCL1 exhibited correlation peaks with Q-ratios of √2:√3:√6:√8:√9 (for P/L = 1/2) and √2:√3:√4 (for P/L = 1/1), which index to Pn3m cubic phases with lattice parameters of 32.17 and 19.68 nm, respectively (Figure A,B). Bicontinuous lipidic cubic phases (QII), such as the Pn3m “double diamond” cubic lattice seen here, are also commonly formed by prototypical AMPs with model bacterial membranes.[19,28−32] A bicontinuous cubic phase consists of two non-intersecting aqueous regions that are separated by a lipid bilayer with NGC at every point on its surface. In a cubic phase, the average amount of Gaussian curvature, K, can be calculated using the equation ⟨K⟩ = (2πχ)/(A0a2), where the Euler characteristic, χ, and the surface area per unit cell, A0, are constants specific to each cubic phase, and a is the lattice parameter. For Pn3m, χ = −2 and A0 = 1.919.[39] With the E. coli model membrane, XCL1 generated Pn3m cubic phases with ⟨K⟩ of −6.33 × 10–3 nm–2 (for P/L = 1/2) and −1.69 × 10–2 nm–2 (for P/L = 1/1), which in fact are of similar magnitude to NGC generated by many AMPs.[30] In other words, our SAXS spectra indicate that XCL1 causes restructuring of model bacterial membranes into phases rich in NGC. Because this type of curvature is topologically required for membrane permeabilization mechanisms, these results suggest that XCL1 has the capacity to kill bacteria via direct, physical membrane disruption. In contrast, the SAXS profile of XCL1 mixed with SUVs mimicking mammalian cell membranes (P/L = 1/2) exhibited a set of correlation peaks with integral Q-ratios consistent with a lamellar (Lα) phase with a periodicity of 8.54 nm, indicating the formation of multilamellar membrane stacks without significant curvature generation (Figure C). Similar to the E. coli-like SUVs, the control samples of mammalian cell-like SUVs alone also exhibited the form factor expected of unilamellar vesicles.
Figure 2

XCL1 induces negative Gaussian curvature in model bacterial membranes, but not model mammalian membranes. (A) SAXS spectra for XCL1 incubated with SUVs that have bacteria-like membrane compositions (DOPG/DOPE 20/80) at a P/L ratio of 1/1 (light blue) and 1/2 (dark blue). To facilitate visualization, spectra have been manually offset in the vertical direction by scaling each trace by a multiplicative factor. Spectra show characteristic Q peaks of NGC-rich Pn3m cubic phases (dashed gray boxes), which are indexed in (B). (C) SAXS spectra for XCL1 incubated with model mammalian SUVs (DOPS/DOPE/DOPC 20/40/40) in a P/L ratio of 1/2 show no detectable Q peaks (dashed gray box).

XCL1 induces negative Gaussian curvature in model bacterial membranes, but not model mammalian membranes. (A) SAXS spectra for XCL1 incubated with SUVs that have bacteria-like membrane compositions (DOPG/DOPE 20/80) at a P/L ratio of 1/1 (light blue) and 1/2 (dark blue). To facilitate visualization, spectra have been manually offset in the vertical direction by scaling each trace by a multiplicative factor. Spectra show characteristic Q peaks of NGC-rich Pn3m cubic phases (dashed gray boxes), which are indexed in (B). (C) SAXS spectra for XCL1 incubated with model mammalian SUVs (DOPS/DOPE/DOPC 20/40/40) in a P/L ratio of 1/2 show no detectable Q peaks (dashed gray box). Together, these results indicate that XCL1 can selectively kill bacteria via membrane disruption in a manner cognate with other known AMPs. Moreover, our data suggest that XCL1’s selective antimicrobial activity arises from XCL1’s ability to recognize differences between the membrane compositions of mammalian cells and bacteria.

A Panel of Structural XCL1 Variants Display Differing Membrane-Disruptive Activities in E. coli-like Membranes

XCL1 has been well studied, and a number of variants have been engineered to stabilize XCL1 in its chemokine, all-β, and unfolded states.[40,41] These variants are named CC3, CC5, and CC0, respectively. Additionally, an XCL1 point mutant, XCL1 W55D, destabilizes the hydrophobic core of XCL1’s chemokine structure by replacing hydrophobic Trp55 with a negatively charged aspartate, and thus allows access to the all-β and unfolded states, but not the chemokine structure.[17] Two other point mutants, XCL1 R23A and XCL1 R43A, shift XCL1’s conformational equilibrium to favor its chemokine structure, in addition to dramatically diminishing XCL1’s affinity for GAGs.[42,43] Finally, a truncated version of XCL1 (XCL1 residues 1–72) is missing its extended C-terminal tail (residues 73−93), without alteration to the structural equilibrium. The structural behaviors of these variants are illustrated in Figure A, and the antimicrobial activities of select variants against E. coli as measured by a radial diffusion assay[13] are catalogued in Figure B.
Figure 3

Structural and functional features of XCL1 variants tested for membrane remodeling activity. (A) Panel of seven XCL1 variants tested in this study. WT XCL1 can access a β-sheet structure and chemokine-like α–β structure and is thought to interconvert between the two via complete unfolding. W55D can access the β-sheet and unfolded state, but not the chemokine structure. CC5 can access only the β-sheet structure. XCL1 1–72 is a truncated version of WT XCL1 lacking the extended C-terminal tail (residues 73–93). XCL1 R23A and R43A are variants of XCL1 with reduced affinity for glycosaminoglycans, which preferentially occupy the chemokine structure but can access the unfolded and all-β structures. CC0 can access only the unfolded state. CC3 can access only the chemokine structure. (B) Published values for WT XCL1 and select XCL1 structural variants’ minimum effective concentrations (MEC, μM) against E. coli BL21 cells.[13] CC3, an XCL1 structural variant locked in the chemokine structure, is notably less active.

Structural and functional features of XCL1 variants tested for membrane remodeling activity. (A) Panel of seven XCL1 variants tested in this study. WT XCL1 can access a β-sheet structure and chemokine-like α–β structure and is thought to interconvert between the two via complete unfolding. W55D can access the β-sheet and unfolded state, but not the chemokine structure. CC5 can access only the β-sheet structure. XCL1 1–72 is a truncated version of WT XCL1 lacking the extended C-terminal tail (residues 73–93). XCL1 R23A and R43A are variants of XCL1 with reduced affinity for glycosaminoglycans, which preferentially occupy the chemokine structure but can access the unfolded and all-β structures. CC0 can access only the unfolded state. CC3 can access only the chemokine structure. (B) Published values for WT XCL1 and select XCL1 structural variants’ minimum effective concentrations (MEC, μM) against E. coli BL21 cells.[13] CC3, an XCL1 structural variant locked in the chemokine structure, is notably less active. To determine which specific structural features are influential in XCL1’s antibacterial activity, we used synchrotron SAXS to systematically examine each of these seven variants’ membrane disruption capabilities in SUVs with lipid compositions that mimic those of E. coli and mammalian cell membranes. We found that CC5 (locked β-sheet structure), CC0 (unfolded variant), and W55D (accesses unfolded state and β-sheet structure) are all capable of generating NGC in E. coli-like membranes, in a manner similar to that of WT XCL1. The SAXS spectra of the SUVs after exposure to these proteins revealed the formation of NGC-rich cubic phases (Figure A). For W55D and CC5 at P/L = 1/2, correlation peaks indexed to a Pn3m phase with a lattice parameter of 25.16 and 24.57 nm, respectively (Figure B). For CC0 at P/L = 1/2, we observed a coexistence of Pn3m and Im3m cubic phases, the latter of which is defined by χ = −4 and A0 = 2.345.[39] The respective lattice parameters of these coexisting cubic phases were 20.07 and 25.45 nm, which had a ratio close to the Bonnet ratio of 1.279, indicating that the two cubic phases are near equilibrium with the amount of curvature being balanced across both.
Figure 4

XCL1 requires access to its unfolded state or β-sheet structure, but not its C-terminal tail, for membrane remodeling. (A) SAXS spectra for model bacterial membranes (DOPG/DOPE 20/80) incubated with XCL1 structural variants. To facilitate visualization, spectra have been manually offset in the vertical direction by scaling each trace by a multiplicative factor. All variants except CC3, which is locked into the chemokine fold, induce NGC in model bacterial membranes. (B) Indexation plots for all variants shown in (A) that induce NGC. Inset: isolated indexation plot for CC0 to provide additional clarity for the coexisting Pn3m and Im3m cubic phases. (C) Summary of NGC induction by each variant in model bacterial and mammalian membranes. Check marks indicate induction of NGC.

XCL1 requires access to its unfolded state or β-sheet structure, but not its C-terminal tail, for membrane remodeling. (A) SAXS spectra for model bacterial membranes (DOPG/DOPE 20/80) incubated with XCL1 structural variants. To facilitate visualization, spectra have been manually offset in the vertical direction by scaling each trace by a multiplicative factor. All variants except CC3, which is locked into the chemokine fold, induce NGC in model bacterial membranes. (B) Indexation plots for all variants shown in (A) that induce NGC. Inset: isolated indexation plot for CC0 to provide additional clarity for the coexisting Pn3m and Im3m cubic phases. (C) Summary of NGC induction by each variant in model bacterial and mammalian membranes. Check marks indicate induction of NGC. SAXS spectrum from exposure of CC3 to E. coli-like membranes (P/L = 1/2) showed a broad feature that is consistent with the form factor of unilamellar vesicles and resembled the spectrum of the control SUVs, indicating that NGC was not induced and that the chemokine conformation does not effectively disrupt membranes at this P/L ratio (Figure A). In other words, XCL1 requires access to its β-sheet structure or unfolded state in order to readily function as an antimicrobial agent with the mechanism of membrane permeation. XCL1 R23A and XCL1 R43A also restructured E. coli-like SUVs (P/L = 1/2) into Pn3m cubic phases, as shown in Figure A,B. This indicates that despite their loss of GAG-binding affinity, these variants retain the ability to induce membrane disruption in E. coli-like membranes, disentangling XCL1’s GAG-binding activity from its antimicrobial function. Compared with WT XCL1, the structural equilibria of these variants are shifted to favor the chemokine fold.[42,44] Nonetheless, they are still able to induce NGC in model bacterial membranes. In conjunction with the results from CC3, CC0, W55D, and CC5, this suggests that access to the unfolded and β-sheet structures is critical for membrane-disruptive function, and that proteins can remain highly effective as membrane disruptors even when these structures are less highly populated than in WT XCL1. XCL1 1–72 (tail-less variant) was also able to induce NGC in E. coli-like membranes, as demonstrated by the generation of a Pn3m phase at P/L = 1/2, indicating that XCL1’s extended C-terminal tail (residues 73–93) is not required for membrane-disruptive activity. No XCL1 variants induce NGC in mammalian cell-like membranes even when structural and GAG-binding profiles are altered (Supplemental Figure 3). The results described above indicate that XCL1 functions as a molecular “Swiss army knife” metamorph that partitions distinct, context-dependent functions into its different folded structures. While the α–β chemokine structure binds and activates its cognate GPCR XCR1, only the β-sheet and unfolded XCL1 structures can induce NGC in membranes. It is interesting to compare these structural tendencies of XCL1 to recently studied metaphilic peptides, which have an architecture that allows side chains to reorganize in response to different environments.[33,34] In the case of XCL1, such functional changes are made possible by changes in secondary structure.

SAXS Reveals XCL1’s Ability to Induce NGC in a Conformation-Dependent Dependent Manner in Candida-like Artificial Membrane Compositions

Since fungi are eukaryotes, fungal membranes are more similar to mammalian membranes than bacterial membranes, and discrimination is often a challenge. As the structural motif for generating NGC in XCL1 is different than that of other chemokines (β-sheet rather than the α–β fold) we investigated whether XCL1 is able to disrupt Candida-like membranes. SUVs with a Candida-like membrane composition, 1,2-dioleoyl-sn-glycero-3-phospho-l-serine/1,2-dioleoyl-sn-glycero-3-phosphoethanolamine in a molar ratio of 20/80 (DOPS/DOPE 20/80), were incubated with XCL1 and the resulting membrane structures were characterized using synchrotron SAXS. As with other lipid-only control samples, the SAXS profile from DOPS/DOPE 20/80 SUVs exhibited a form factor that is consistent with unilamellar vesicles (Supplemental Figure 1). However, the lipid vesicles restructured when exposed to XCL1 (P/L = 1/1), as indicated by correlation peaks with ratios √2:√3:√4 that index to a Pn3m cubic phase with a lattice parameter of 21.16 nm and ⟨K⟩ of −1.46 × 10–2 nm–2 (Figure A,C).
Figure 5

XCL1 induces NGC in model fungal membranes in a structurally dependent manner and can kill Candida in vitro. (A,B) SAXS spectra for model fungal membranes (DOPS/DOPE 20/80) incubated with XCL1 and the panel of XCL1 structural variants described in Figure . To facilitate visualization, spectra have been manually offset in the vertical direction by scaling each trace by a multiplicative factor. (C,D) Indexation plots for the spectra in A and B. (E) Summary of NGC induction by each XCL1 variant in model fungal membranes. (F) In vitro Candida killing assay data for XCL1 (blue) and CCL28 (positive control, gray).

XCL1 induces NGC in model fungal membranes in a structurally dependent manner and can kill Candida in vitro. (A,B) SAXS spectra for model fungal membranes (DOPS/DOPE 20/80) incubated with XCL1 and the panel of XCL1 structural variants described in Figure . To facilitate visualization, spectra have been manually offset in the vertical direction by scaling each trace by a multiplicative factor. (C,D) Indexation plots for the spectra in A and B. (E) Summary of NGC induction by each XCL1 variant in model fungal membranes. (F) In vitro Candida killing assay data for XCL1 (blue) and CCL28 (positive control, gray). The seven XCL1 structural variants described earlier (CC3, CC0, CC5, XCL1 W55D, XCL1 R23A, XCL1 R43A, and XCL1 1–72) were also each incubated with Candida-like membranes and characterized. We found that the structural dependence observed in bacteria-like membranes was also consistent in Candida-like membranes, in which variants that could access the unfolded or β-sheet structure were able to generate NGC. SAXS spectra for CC0, CC5, and W55D showed correlation peaks with Q-ratios indicative of the presence of Pn3m and Im3m cubic lattices rich in NGC (Figure B,D). As with E. coli-like membranes, CC3 was not able to generate NGC in Candida-like membranes. Interestingly, XCL1 R23A also did not generate NGC in these membranes (Figure B,D), deviating from its pattern of membrane-disruptive activity with bacteria-like membranes. However, XCL1 R43A and XCL1 1–72 both generated NGC in Candida-like SUVs, consistent with their activity with bacterial membranes (Figure B,D). Collectively, these data suggest that similar structure–function relationships hold for XCL1’s activity with candidal membranes as for bacterial membranes, with a slight nuance at GAG binding residue Arg23.

XCL1 Exhibits Antifungal Activity against Candida

Several human mucosal chemokines, including CCL28,[11,45] CXCL17,[12] and CCL20,[9] kill Candida, but it is not clear whether this is a general feature of chemokines. Moreover, given the metamorphic nature of XCL1, it is also not known whether antifungal activity can exist in a molecule whose structures are transiently occupied. Our SAXS data demonstrate that XCL1 induces the structural rearrangement necessary for membrane disruption in Candida-like membranes, suggesting that XCL1 should exhibit antifungal activity. To investigate this hypothesis, we performed in vitro killing assays against C. albicans and found XCL1 to be a potent anticandidal agent, similar to CCL28, which has known anticandidal activity[11] (Figure F). While CCL28 is a slightly more potent killer of C. albicans perhaps due to XCL1’s structural interconversion, both proteins achieve complete killing at concentrations of 1 μM. These findings are in agreement with the previously identified correlations between NGC generation and membrane-disruptive AMP activity,[28,30] including that of mammalian α-defensins, which also have β-sheet-rich secondary structures.[29] Moreover, antifungal defense in mammals usually requires clearance by Th17 mediated neutrophil-based responses: Surprisingly, we find that XCL1 induces membrane-permeating NGC in Candida-like membranes via a structural motif distinct from classical α–β chemokines. This suggests the possibility of a multilayered antifungal defense associated with this metamorphic chemokine. Interestingly, both XCL1 and IL-17A are produced by NKT cells[47,48] and are involved in antifungal defense,[49] suggesting a possible functional, synergistic relationship between the two molecules, as well as a possible mechanism by which NKT cells participate in host defense against fungi.

Conclusions

Many antimicrobial peptides, such as bacteriocins, defensins, histatins, protegrins, and chemokines,[2−6,12] kill microbes via membrane disruption, such as by forming pores or blebs. For example, the human chemokine CXCL17 has been shown to kill E. coli by inducing membrane disruption.[12] The generation of NGC in the target membrane is a topological requirement for the formation of these structures.[27,30,37,38] We and others have previously detected antimicrobial activity for the human chemokine XCL1, a metamorphic chemokine with two native structures.[13,46] In this work, we find that XCL1 can selectively, physically disrupt bacterial and fungal membranes, and that XCL1’s metamorphic folding allows for restriction of its membrane remodeling function to its β-sheet structure. Our results suggest that XCL1’s dynamic interconversion could provide the opportunity for switchable, context-dependent function. Because XCL1’s α–β chemokine structure cannot induce membrane disruption and XCL1’s β-sheet structure cannot bind to XCL1’s cognate GPCR, shifts in equilibrium could tune XCL1 toward either membrane disruptive activity or receptor-binding activity in different environments, allowing for synergistic, context-dependent tuning of function. In fact, XCL1’s structural equilibrium is known to shift to favor the β-sheet state in the presence of one of its binding partners, GAGs.[17] It is possible that the presence of microbial membranes can similarly shift XCL1’s equilibrium toward the β-sheet structure, a hypothesis which will be explored in future studies. In the present paradigm, proteins typically evolve to minimize structural frustration in the thermodynamically favored native state.[50−52] The structural and functional divergence observed for XCL1 has fundamental consequences for this classical picture of a folded protein: it is possible for the same sequence to encode different structures with distinct patterns of frustrations. We speculate that metamorphosis has evolved in XCL1 because it is associated with a gain of function that may enhance XCL1’s “fitness”.[53] Such a gain of function is discovered here: XCL1’s conformation-specific, physical disruption of bacterial and fungal membranes illustrates how protein metamorphosis can allow for adjustability of function via modulation of structural equilibria. The principles uncovered in this study can be extended to the design of tunable, multifunctional antimicrobial protein therapeutics.

Materials and Methods

Identification of Membrane-Active Sequences Using an SVM Classifier

The amino acid sequences of the human chemokines XCL1, CXCL4, and CCL20 were screened for membrane active domains using a previously validated support vector machine (SVM) classifier trained to recognize membrane permeable helical sequences.[18] We implemented a variable moving window along the full sequences of each protein to give individual segments a σ-score indicative of the degree of likelihood that the segment is a membrane active peptide. To visualize the localization of these scores along the main sequence, we created a probability map displaying the scores along the sequence for each window size used. For a given window size, the score given to each amino acid position was calculated by averaging the mean σ-score of all the segments in which that amino acid appears. The resulting probability map was plotted as a window size vs amino acid position heat map, in which the intensity values correspond to the mean σ-score, i.e., the probability that the segment can induce membrane permeability.

Mutagenesis, Expression, and Purification of Recombinant XCL1 Proteins

The QuikChange Site-directed mutagenesis kit (Stratagene) was used to perform site-directed mutagenesis on the XCL1 pET28a expression vector and the XCL1 pQE30 expression vector in order to create the following XCL1 variants: CC3 (XCL1 V21C V59C), CC0 (XCL1 C11A C48A), XCL1 1–72 (truncated at residue 72), XCL1 R23A, XCL1 R43A, XCL1 W55D, and CC5 (XCL1 A36C A49C). Each protein was then expressed and purified as previously described.[13,17,54] XCL1 and CCL28 were also produced and purified using this pipeline. In brief, each of these proteins was then expressed recombinantly in BL21 DE3 E. coli with pET28a or pQE30 expression vectors containing the sequence for His6-SUMO-XCL1 or XCL1 variant sequence, except CC5 (XCL1 A36C A49C), which contained a His8 affinity tag. Cultures were grown in terrific broth containing 50 lg/mL kanamycin to an optical density of 0.5–0.7 at 37 °C, at which point 1 mM isopropyl-b-d-thiogalactopyranoside (IPTG) was used to induce protein expression. After induction, cultures were grown for 5 h at 37 °C and cells were harvested by centrifugation and stored at −80 °C. Following expression and harvesting, proteins were purified. Cell pellets were resuspended in 50 mM sodium phosphate (pH 8.0), 300 mM sodium chloride, 10 mM imidazole, 0.1% (v/v) β-mercaptoethanol, and 1 mM phenylmethylsulfonyl fluoride (PMSF). Cells were then lysed by three passages through a French press and lysates were centrifuged at 12 000g for 20 min to collect inclusion bodies. Soluble fractions and resuspended inclusion bodies were incubated with Ni2+-NTA resin (Qiagen) for 1 h at room temperature. Columns were rinsed and proteins were eluted with 6 M guanidinium chloride, 50 mM sodium phosphate (pH 7.4), 300 mM NaCl, 500 mM imidazole, 0.2% sodium azide, and 0.1% (v/v) β-mercaptoethanol. Infinite dilution refolding in 20 mM Tris (pH 8.0), 200 mM NaCl, 10 mM cysteine, and 0.5 mM cystine was performed for eluted proteins, followed by incubation at room temperature overnight with gentle stirring. The refolded protein solutions were concentrated to ∼50 mL, and the fusion tag was removed by overnight cleavage with ULP1 protease (His6-SUMO tag) or TEV protease (His8 tag). The tag was separated from the protein of interest by either cation exchange chromatography on SP Sepharose Fast Flow resin (GE Healthcare UK Ltd.) or reverse nickel chromatography using Ni2+-NTA resin (Qiagen) as above. Lastly, proteins were purified by reverse-phase high-performance liquid chromatography with a C18 column. Protein samples were then frozen and lyophilized. Sample identities, purities, and homogeneities were confirmed by matrix-assisted laser desorption ionization time-of-flight (MALDI-TOF) spectroscopy. Note that because the TEV system was used for CC5, the N-terminus of this protein was non-native, missing the N-terminal Val1.

Liposome Preparation for SAXS Experiments

Liposomes were prepared for SAXS experiments as previously described.[19,34] In brief, lyophilized phospholipids DOPG (1,2-dioleoyl-sn-glycero-3-[phospho-rac-(1-glycerol)]), DOPE (1,2-dioleoyl-sn-glycero-3-phosphoethanolamine), DOPC (1,2-dioleoyl-sn-glycero-3-phosphocholine), and DOPS (1,2-dioleoyl-sn-glycero-3-phospho-l-serine) purchased from Avanti Polar Lipids were dissolved in chloroform at 20 mg/mL to produce individual lipid stock solutions. Model membrane lipid compositions were prepared from the lipid stock solutions as mixtures at specified molar ratios. Each lipid mixture was subsequently evaporated under nitrogen and then desiccated overnight under vacuum to form a dry lipid film, which was resuspended in aqueous 140 mM NaCl, 10 mM HEPES (pH 7.4) to a concentration of 20 mg/mL. Lipid suspensions were incubated overnight at 37 °C, sonicated until clear, and then extruded through a 0.2 μm pore size Anopore membrane filter (Whatman) to form SUVs.

SAXS Experiments with Model Membranes

Methods used for SAXS experiments and data fitting were based around those that have been previously described.[30,33,34,55] Lyophilized proteins (WT XCL1 and XCL1 variants, i.e., CC3 (XCL1 V21C V59C), CC5 (XCL1 A36C A49C), CC0 (XCL1 C11A C48A), XCL1 1–72 (truncated at residue 72), XCL1 R23A, XCL1 R43A, and XCL1 W55D) were solubilized in aqueous 140 mM NaCl, 10 mM HEPES (pH 7.4) and mixed with SUVs at P/L of 1/2 and 1/1. Samples were hermetically sealed into quartz capillaries (Hilgenberg GmbH, Mark-tubes) for SAXS measurements taken at the Stanford Synchrotron Radiation Lightsource (SSRL, beamline 4–2) using monochromatic X-rays with an energy of 9 keV. The scattered radiation was collected using a DECTRIS PILATUS3 X 1M detector (pixel size, 172 μm), and the resulting 2D SAXS powder patterns were integrated using the Nika 1.50[56] package for Igor Pro 6.31 and FIT2D.[57] Using Origin Lab software, the integrated scattering intensity I(Q) was plotted against Q. Ratios of the measured peak positions (Qmeasured) were compared with those of permitted reflections for different crystal phases to identify the phase(s) present in each sample. A linear regression through points corresponding to the peaks was used to calculate the lattice parameter, a, of each identified cubic phase. For a cubic phase, each peak is represented by a point with coordinates of the assigned reflection (in terms of Miller indices h, k, l) and Qmeasured. For a cubic phase, Q = (2π/a)√(h2 + k2 + l2). Therefore, the slope of the regression (m = 2π/a) of Qmeasured vs √(h2 + k2 + l2) can be used to calculate a. Similarly, for a lamellar phase, each peak is represented by a point with coordinates of the order of the reflection, n, and Qmeasured with the relation Q = 2πn/d. In this case, the slope (m = 2π/d) of the regression of Qmeasured vs n is used to determine the periodic spacing, d.

Candida Killing Assays

Candida killing assays were performed in a similar manner to that which has been previously described.[11,45] In brief, yeast peptone dextrose (YPD) medium was used to culture a single clone of C. albicans strain CAF2–1 for 16–20 h at 30 °C and 250 rpm. Candida cultures were washed twice with low-salt buffer, 1 mM potassium phosphate buffer (PPB). Washed cultures were diluted to 10 mL stock at final concentration of ∼5 × 104 cells/mL cell/μL in 1 mM PPB, pH 7.0, WT. XCL1 and positive control chemokine CCL28 in lyophilized powder form were resuspended to a final concentration of 400 μM in 1 mM PPB and stored at −20 °C in 50 μL aliquots. Proteins were serially diluted and mixed 1:1 with the Candida stock at ∼5 × 104 cells/mL to a total volume of 100 μL in a 96-well plate. We performed a negative control (no protein) with vehicle treatment. After incubation of the 96-well plates at room temperature for 2 h with gentle shaking, appropriate dilutions of the suspensions were plated on YPD agar plates and incubated at 30 °C for 48 h. Colonies were then counted, and viability was calculated as a percentage of the colony number of the no-protein control. Each protein condition was tested in triplicate, and assays were performed at least in duplicate.
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