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. 1. Department of Biochemistry, Medical College of Wisconsin, Milwaukee, Wisconsin 53226 United States. 2. Department of Bioengineering, University of California, Los Angeles, Los Angeles, California 90095, United States. 3. UCLA-Caltech Medical Scientist Training Program, David Geffen School of Medicine, University of California, Los Angeles, Los Angeles, California 90095, United States. 4. Department of Pediatrics, Medical College of Wisconsin, Milwaukee, Wisconsin 53226 United States.
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.
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.
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, XCL1R23A and XCL1R43A, 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). XCL1R23A 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.XCL1R23A and
XCL1R43A 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, XCL1R23A, XCL1R43A, 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, XCL1R23A also did not generate NGC
in these membranes (Figure B,D), deviating from its pattern of membrane-disruptive activity
with bacteria-like membranes. However, XCL1R43A 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 (XCL1V21CV59C), CC0 (XCL1 C11A C48A),
XCL1 1–72 (truncated at residue 72), XCL1R23A, XCL1R43A,
XCL1 W55D, and CC5 (XCL1A36CA49C). 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 (XCL1A36CA49C),
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 (XCL1V21CV59C), CC5 (XCL1A36CA49C),
CC0 (XCL1 C11A C48A), XCL1 1–72 (truncated at residue 72),
XCL1R23A, XCL1R43A, 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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