Adrian W.
Hodel
abc,
Jesse A.
Rudd-Schmidt
ad,
Joseph A.
Trapani
de,
Ilia
Voskoboinik
*ad and
Bart W.
Hoogenboom
*bcf
aKiller Cell Biology Laboratory, Peter MacCallum Cancer Centre, 305 Grattan Street, Melbourne, VIC 3000, Australia. E-mail: ilia.voskoboinik@petermac.org
bLondon Centre for Nanotechnology, University College London, 19 Gordon Street, London WC1H 0AH, UK. E-mail: b.hoogenboom@ucl.ac.uk
cInstitute of Structural and Molecular Biology, University College London, Gower Street, London WC1E 6BT, UK
dSir Peter MacCallum Department of Oncology, University of Melbourne, Melbourne, VIC 3000, Australia
eCancer Cell Death Laboratory, Peter MacCallum Cancer Centre, 305 Grattan Street, Melbourne, VIC 3000, Australia
fDepartment of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, UK
First published on 13th August 2020
Perforin is a pore forming protein used by cytotoxic T lymphocytes to remove cancerous or virus-infected cells during the immune response. During the response, the lymphocyte membrane becomes refractory to perforin function by accumulating densely ordered lipid rafts and externalizing negatively charged lipid species. The dense membrane packing lowers the capacity of perforin to bind, and the negatively charged lipids scavenge any residual protein before pore formation. Using atomic force microscopy on model membrane systems, we here provide insight into the molecular basis of perforin lipid specificity.
Perforin membrane binding – the first step in pore formation – is calcium-dependent and is mediated by its C2 domain.5–9 It was initially thought that phosphocholine lipids were perforin receptors in the target membrane,10 but it was later shown – by a comparison of lipids well above and just below their gel transition temperature – that lipid order was a more important factor in determining membrane sensitivity to perforin.11 The relatively tight plasma membrane packing of CTLs thus served as an explanation of the resistance of CTLs to perforin lysis. In the context of unidirectional killing in the immune synapse however, this hypothesis failed to explain the capability of CTLs to target and kill other CTLs, nor did it explain the absence of a clear correlation between the membrane packing of target cells and their susceptibility to perforin lysis.12 Following up on these early studies and on observations of perforin on model membranes by atomic force microscopy (AFM),13 we have recently revealed a two-layered lipid-based mechanism that renders CTLs refractory to perforin pore formation:14 firstly, increased lipid order and packing in the CTL membrane reduces perforin binding to the membrane, and secondly, perforin is sequestered and irreversibly inactivated by binding to the negative charge of externalised phosphatidylserine (PS) at the CTL surface. Importantly, these membrane changes are enhanced in the area of the CTL plasma membrane that is associated with the immune synapse.
This lipid specificity can be regarded in the context of other pore forming proteins in general15 and of the membrane attack complex-perforin/cholesterol dependent cytolysin (MACPF/CDC) family of pore forming proteins, which perforin is part of.16–19 The bacterial CDCs use – as implied by their name – cholesterol as a receptor on the membrane and only form pores in membranes above a rather sharp threshold of cholesterol contents, typically above ∼25–35%.20–23 This cholesterol dependence defines the specificity of CDCs to eukaryotic target cells, as bacteria generally do not contain cholesterol in their membranes.24,25 The mushroom derived MACPF pleurotolysin B utilizes the partner proteins ostreolysin A or pleurotolysin A to specifically bind and form pores in membranes containing sphingomyelin and cholesterol26–28 or insect specific lipids.29 In vertebrates, the membrane attack complex (MAC) is an immune effector that kills pathogenic bacteria. The formation of the MAC is facilitated on membranes that contain negatively charged lipids and show increased membrane tension, mimicking the surface of Gram-negative bacteria.30 Other examples from the vertebrate immune system are the more recently discovered pore forming proteins of the gasdermin family, which share some structural elements with MACPF/CDCs and trigger cell death by perforating the membranes of infected cells from the inside out.31 Gasdermin pore formation is related to negatively charged lipids that are in the inner leaflets of eukaryotic plasma membranes and mitochondria.
Besides cell-based assays, the lipid specificity of pore formation can be most conveniently studied on model lipid bilayers since these can be prepared from a wide selection of lipid components and therewith offer the ability to selectively alter biophysical properties. As a reference lipid, we used the dioleoyl derivative of phosphatidylcholine (PC), DOPC, which has a low liquid–gel transition, or melting, temperature (Tm, ca. −17 °C (ref. 32)), and is therefore present in a liquid disordered (Ld) state at physiological temperatures (37 °C). PC lipids in the Ld state (sometimes supplemented with cholesterol) are the most common components of model membranes used to visualize perforin assemblies,7,13,14,33–35 and the addition of cholesterol to Ld membranes increases membrane order and, at sufficiently high concentrations, it can give rise to a liquid ordered (Lo) state.25 Below their melting temperature Tm, lipids exist in a solid ordered (So) gel state. Different lipids have different Tm, e.g., the dipalmitoyl derivative of PC, DPPC, has a Tm of ca. 41 °C (ref. 36) and is thus in the So state at physiological temperature. Over time, a membrane containing a mix of lipids can phase separate and display domains of different states of membrane order. Commonly used mixtures to mimic eukaryotic membranes use a low Tm lipid species like DOPC, cholesterol and high Tm sphingomyelin (SM), e.g., egg SM. In such mixtures, one readily observes phase separation into PC-rich Ld domains and SM/cholesterol-rich Lo domains.37,38 Similarly, mixtures of DOPC and excess DPPC can lead to Ld/So phase separation.39 The lipid phase state is an important factor to consider when mixing different types of lipids. Thus, to retain the Ld state of a reference DOPC bilayer, we can use the dioleoyl derivatives of phospholipids, e.g. dioleoyl phosphatidylserine (DOPS, Tmca. −11 °C (ref. 40)), ethanolamine (DOPE, Tmca. −8 °C (ref. 41)), or glycerol (DOPG, Tmca. −22 °C (ref. 42)).
Such model membranes can be prepared as supported lipid bilayers on a flat substrate, e.g., mica or silica, facilitating their characterisation by in-liquid atomic force microscopy (AFM) experiments. AFM has become a popular tool to study the mechanisms of pore forming proteins,43,44 in part because it allows a relatively straightforward distinction between prepore assemblies and membrane inserted pores. This can be achieved either by detecting a height change45,46 or by the loss of mobility once the protein contacts the underlying substrate.13,46 Another important feature of AFM is its ability to distinguish between different lipid domains via Ångström-sized differences in membrane thickness,47 which allows us to simultaneously detect lipid phase boundaries and protein pores.
Here we use AFM-based experiments to expand upon our recent work14 on establishing and elucidating how perforin function depends on the physicochemical properties of the target membranes. Noting that perforin binding – and thus pore formation – is reduced on tightly packed membranes, we study and compare the effects of several properties that modulate membrane packing. In contrast to its response to changes in membrane order/packing, the interaction of perforin with the negatively charged DOPS is fundamentally different. The initial binding of perforin appears to be unaffected, but pore formation is disrupted. On model membranes, this effect is proportional to the amount of DOPS they contain. We therefore investigate how perforin interacts with pure DOPS membranes in the pursuit of understanding how perforin is deactivated by this lipid. Lastly, we describe the interaction of perforin with DOPE, as PE lipids are another major constituent of the plasma membrane.
4–8 μL of the unilamellar vesicles (containing 4 μg of lipid) were added to a freshly cleaved, ∅ 10 mm mica disc (Agar Scientific, Stansted, UK) and topped up with 80 μL of adsorption buffer containing 150 mM NaCl, 25 mM Mg2+, 5 mM Ca2+, and 20 mM HEPES, pH 7.4. To form a pure DOPG bilayer, lower salt conditions were necessary51 and the buffer was thus adjusted, instead containing no Mg2+ and 10 mM Ca2+. The lipids were incubated for 30 minutes above the Tm of the constituent lipids to cover the mica substrate with an extended lipid bilayer. Excess vesicles were removed by washing the bilayer 6–12 times with 80 μL of the adsorption buffer.
Additional washes were applied to samples that contained DOPS, for which we found that Mg2+ in the buffer interfered with perforin binding, samples that contained DOPG to remove excess Ca2+, or to control samples that required the removal of Mg2+: these were washed an additional 6 times with 80 μL buffer containing 150 mM NaCl, 5 mM Ca2+, and 20 mM HEPES, pH 7.4.
Wild-type perforin (WT-PRF), disulphide-locked perforin (TMH1-PRF), C2 domain mutant perforin (D429A-PRF) and perfringolysin O (PFO) were diluted up to ca. ten-fold to a volume of 40 μL in 150 mM NaCl and 20 mM HEPES, pH 7.4, and injected onto the sample, to reach concentrations of 150 nM or, where noted, ca. 400 nM above the model membrane. The protein was incubated for 2 (where noted) or 5 min at 37 °C. To unlock TMH1-PRF after its binding to the membrane, the engineered disulphide bond was reduced by addition of 2 mM DTT (Sigma-Aldrich, St. Louis, MO, USA) and 10 min incubation at 37 °C. We previously verified that, once TMH1-PRF was bound to target membranes, the effect of DTT on its native disulphide bonds did not change the pore forming functionality.13 Mobile TMH1-PRF assemblies were fixed by addition of glutaraldehyde 8% EM grade (TAAB Laboratories, Aldermaston, UK) to a final concentration of 0.04% v/v, and 10 min incubation at room temperature. Fixed TMH1-PRF assemblies were removed from their DOPS membrane substrate by chelating calcium with EGTA. To this end, the samples were washed 6 times with 80 μL of buffer containing 150 mM NaCl, 20 mM HEPES, and 4 mM EGTA, pH 7.4. EGTA was immediately removed from the sample afterwards by 6 further washes with 80 μL buffer containing 150 mM NaCl, 5 mM Ca2+, and 20 mM HEPES, pH 7.4.
Raw AFM images were background subtracted with reference to the lipid surface, masking perforin and applying second-order flattening. Height values of perforin prepores/pores indicated in the manuscript are given with ±1 nm confidence intervals, with the uncertainty due to scanner calibration and possible sample deformation caused by the probe–sample interaction. The same colour/height scale was applied to all images (except for the insets in Fig. 2A and 4A as specified in their captions), spanning 25 nm and 9 nm below and 16 nm above the membrane surface (set to 0 nm). The colour scale is only depicted once, in Fig. 2. Values for perforin coverage were estimated either by the area above a height threshold located 6–8 nm above the membrane surface and adjusted to counteract tip broadening effects; or, when sufficient images at a higher pixel resolution were available, by tracing pore shapes with 3dmod 4.9.4 (BL3DEMC & Regents of the University of Colorado52). Perforin coverages obtained by both methods are normalized with respect to a 100% DOPC reference and given as values between 0 and 1. One-way analysis of variance (ANOVA) with Dunnett’s post-hoc analysis was performed in R-3.6.3 using the multcomp package.53
Using TMH1-PRF, we first verified the earlier observation11 that perforin does not bind to lipids that are below their gel-transition temperature, i.e., in the gel or So phase. This could be best articulated by visualizing the binding of perforin on phase separated bilayers that contained both Ld and So domains. To this end, we mixed high Tm DPPC and low Tm DOPC and verified the phase separation by AFM, with the So domains appearing ca. 1 nm higher than the Ld domains (see Fig. 2). Upon exposure to TMH1-PRF, the Ld domains showed extensive protein coverage by the appearance of diffuse plateaus with a height close to 10 nm above the membrane. As in previous work, we interpret these plateaus as membrane-bound but not inserted and, hence, highly mobile perforin prepores.13 After addition of DTT, the TMH1-PRF transitioned from the prepore to the membrane-inserted pore state, while remaining localized within Ld domains.
Fig. 2 Prepore-locked TMH1-PRF preferentially binding to Ld domains in a phase separated Ld/So membrane. (A) AFM images of a supported lipid bilayer composed of DOPC/DPPC mixed in a 1:7 molar ratio. The first panel (‘Lipid only’) shows the empty membrane, where the colour contrast has been enhanced in the inset (colour scale: 4 nm) to better visualize the lipid phase separation. The phase boundaries are outlined for the whole image by dashed white lines. Addition of TMH1-PRF (‘TMH1-PRF − DTT’) leads to the formation of a diffuse plateau limited to Ld domains. Similar plateaus were earlier interpreted as mobile prepore assemblies.13 After addition of DTT (‘TMH1-PRF + DTT’), the mobile assemblies insert into the membrane, and a dense layer of arc- and ring-shaped pores is formed (see inset), still confined to Ld domains. Size of the inset, 150 nm. (B) Height profiles extracted along the dashed coloured lines in (A). The profiles depict the 0.5–1 nm height change at the phase boundaries (i) (the boundaries are highlighted by arrows), and the ca. 7–11 nm tall prepore and pore layers (ii and iii). Dashed grey lines indicate the height of the Ld membrane (0 nm) and the height of a perforin monomer (11 nm (ref. 7)). Note that perforin features can appear compressed due to tip–sample interaction forces. The data was recorded at 37 °C. |
Besides bilayer-based experimental substrates, membrane strips blotted with different types of lipids have been used to characterize the lipid specificity of several pore forming proteins (e.g.ref. 29 and 54–56). We find that commercially available strips fail to detect perforin binding to, for example, PC (Fig. 3), in agreement with previous reports using lipid strips;†55 this is in apparent contradiction to the scientific literature spanning from the 1980s10 to today.14 This contradiction can be simply explained by noting that the blotted (phospho-) lipids have a high Tm and were not in an Ld state at the physiological/experimental temperature, and are thus likely to cause erroneous readings when lipid order is a factor of importance for protein binding (such as for perforin). Moreover, lipids that bound perforin on these lipid strips (Fig. 3B and C, ‘+Ca2+’ vs. ‘−Ca2+’) did so independently of the calcium that is required for perforin binding to target membranes; such interactions may therefore be artefacts due to defects in the lipid covered membrane surfaces.
Fig. 3 Binding of TMH1-GFP-PRF to lipid strips in the presence and absence of 2 mM Ca2+, visualized by fluorescence imaging.† (A) Schematic layout of the lipid strips, with spots of lipids blotted where indicated (xylene cyanol FF is a non-lipid control). (B) Detection of TMH1-GFP-PRF binding to lipid strips in the presence and absence of Ca2+ (‘+Ca2+’ and ‘−Ca2+’ respectively) immediately after washing. (C) The same lipid strips as in (B) after 4 days at 4 °C in blocking buffer. |
As reported previously14 and reiterated here for completion and for comparison with Fig. 2, we observe the same preference of perforin for Ld domains when adding TMH1-PRF to phase separated lipid membranes that contain both Ld and Lo domains,14 which is also in agreement with previous results using WT-PRF.13,14 As shown in Fig. 4, perforin again preferentially binds to and forms pores in Ld domains, albeit that some rare examples of perforin binding may be observed on Lo domains. This binding dependence on lipid order is also in agreement with the reduction of WT-PRF pore formation on highly ordered egg sphingomyelin membranes compared with Ld 18:1 sphingomyelin membranes.14
Fig. 4 TMH1-PRF preferentially binding to Ld domains in a phase separated Ld/Lo membrane, analogous to Fig. 2. (A) AFM images of an approximately equimolar DOPC/egg SM/cholesterol supported lipid bilayer. ‘Lipid only’ shows the empty membrane with the phase boundaries between Ld and Lo domains highlighted by the inset (with a 4 nm colour scale) and dashed white lines. TMH1-PRF exclusively binds Ld domains (‘TMH1-PRF − DTT’) and remains (mostly) confined there after addition of DTT (‘TMH1-PRF + DTT’) and the formation of transmembrane pores (see inset). Size of the inset, 150 nm. (B) Height profiles extracted along the dashed coloured lines in A. The profiles depict the 0.5–1 nm height change at the phase boundaries (i) (the boundaries are highlighted by arrows), and the ca. 7–11 nm tall prepore and pore layers (ii and iii). Dashed grey lines indicate the height of the Ld membrane (0 nm) and the height of a perforin monomer (11 nm (ref. 7)). Note that perforin features can appear compressed due to tip–sample interaction forces. The data was recorded at 37 °C. Figure reproduced from ref. 14, under a Creative Commons Attribution 4.0 International License (CC BY 4.0). |
In the experiments reported above, lipid order was varied by using lipids with identical headgroups but different hydrophobic tails. In addition, membrane order can be dependent on divalent ions that intercalate with lipid headgroups, modulating intermolecular attractions.57 In most of our AFM work on model membranes, we used up to 25 mM Mg2+ in our buffers to stabilize the supported lipid bilayers on the negatively charged mica substrate. This concentration is about one order of magnitude higher than blood levels.58 To test how the presence of Mg2+ affects perforin function, we designed experiments in which we washed samples to remove Mg2+ from the buffer before adding perforin (WT-PRF, at 37 °C as usual) onto model membranes in either the Ld (pure DOPC), Lo (DOPC/cholesterol or egg SM/cholesterol, both 47/53 molar ratio), or So (pure egg SM) state.37
By comparison with previously published data acquired in the presence of Mg2+, we found the differences between pore formation at high and low levels of Mg2+ to be mostly insignificant (see Fig. 5). However, for low levels of Mg2+, a significant but small increase in pore formation was found on the Lo membranes consisting of DOPC/cholesterol and egg SM/cholesterol. We did not note any phase separation in any of these lipid substrates at either level of Mg2+, suggesting that perforin binding was uniformly affected, if at all, in all samples. In summary, the suggested increase in membrane order due to Mg2+ may be present and affect perforin pore formation in membranes of intermediate order, but this effect is small compared to the effects on lipid order due to high amounts of cholesterol or introduction of gel-phase lipids as reported above.
Fig. 5 Perforin lipid specificity as a function of Mg2+ concentration. (A) Representative AFM images of WT-PRF pores incubated on magnesium-depleted (<1 mM Mg2+, see Experimental) membranes of different lipid compositions and at 25 mM Mg2+, as indicated. The data was recorded at 37 °C. (B) Average perforin pore formation on different lipid mixtures, at Mg2+ concentrations of 25 mM and <1 mM, normalized to the number of pores on DOPC-only membranes. Here, perforin was incubated for 2 min instead of 5 min (see Experimental) to match the experimental conditions of the two datasets. Error bars represent standard deviations. The statistical significance was assessed using ANOVA with Dunnett’s post-hoc analysis, where ‘ns’ is not significant, *p < 0.05, **p < 0.01. The data for 25 mM Mg2+ are reproduced from ref. 14. |
Perforin can bind to PS-rich membranes, but pore formation is decreased: instead of pores, perforin aggregates into dysfunctional plaques.14 PS lipids have a net negative charge at physiological pH, and we previously hypothesized that this negative charge is the underlying cause of perforin dysfunction. We therefore tested the effect of the negatively charged DOPG and cholesterol sulphate on perforin pore formation. As predicted, the decrease in perforin pore formation was proportional to the levels of negatively charged lipids in the membranes and, possibly, further affected by an ordering effect induced by cholesterol sulphate (Fig. 6 A and B). This leads us to conclude that it is a generic negative surface potential, rather than specific lipid headgroups, that prevent perforin pore formation here.
Fig. 6 WT-PRF pore formation on different substrates containing DOPC and varying levels of either DOPS, DOPG, or cholesterol sulphate (CS). (A) Representative AFM images of perforin pores and aggregations on the different substrates. For pure CS, no bilayer could be formed. All data was recorded at room temperature. (B) Quantification of pore formation (mean ± SD) in the samples shown in (A), relative to the 0% dopant/100% DOPC reference. (C) Height profiles extracted along the dashed lines in (A); the ‘DOPC’ reference profile was extracted from the first tile in (A). The different profiles show the membrane level adjusted to 0 nm and the height of perforin pores (ca. 11 nm) and aggregates (ca. 7 nm at 60% dopant levels, up to 15 nm at 100% dopant levels), as highlighted by horizontal dashed lines. The colour tone of the profiles is darker compared to the ‘DOPC’ reference, corresponding to the level of negative charge present in the membrane substrates. Panels (A) and (B) are reproduced from ref. 14, under a Creative Commons Attribution 4.0 International License (CC BY 4.0). |
On the membranes with higher negative charge, the decrease in WT-PRF pore formation was accompanied by an increase in the presence of plaques of protein aggregates. Perhaps the most striking feature of these plaques is their height. Perforin aggregations appear at ca. 7 nm in height when PC is doped with 30–60 mol% negatively charged lipids; of note, the actual proportion of negatively charged lipids in the outer layer of supported lipid bilayers is likely to be reduced by at least one half due to leaflet asymmetry in negatively charged supported lipid bilayers.49 However, on pure DOPS and DOPG membranes, the aggregations appear as plaques with a height of (up to) 15 nm above the membrane surface (Fig. 6C). This height is to be compared with the ca. 11 nm height of membrane-bound perforin prior to and after membrane insertion.13,14
Intriguingly, the observed 15 nm height above the membrane agrees with the full height of perforin pores including the hairpins that span the membrane.7 This suggests that the protein has initiated the transition from its prepore to pore state, yet while unfurling these hairpins, it has failed to insert into the membrane. Given this possible interpretation, we sought to first further verify the height measurements of perforin plaques on pure PS membranes, by including the cholesterol dependent cytolysin (CDC) perfringolysin O (PFO) as a height ruler in our experiments. Like other CDCs, PFO forms pores that protrude ca. 7 nm above cholesterol-containing membranes.45,46,59,60 To this end, we prepared 70:30 mol% DOPS/cholesterol membranes, on which perforin behaved similarly as on pure DOPS membranes (Fig. 7A) but which – by the inclusion of cholesterol – allowed CDC binding and pore formation too (Fig. 7B). By first incubating these membranes with perforin and next with the CDC PFO, we observed PFO pores in addition to perforin plaques (Fig. 7C and D), with the perforin plaques being approximately double the height above the membrane as the PFO pores, which were taken as a height reference of ca. 7 nm (Fig. 7E). This fully confirms the extraordinary height of perforin on DOPS-only bilayers.
Fig. 7 AFM images of WT-PRF and PFO on 70:30 mol% DOPS/cholesterol bilayers for height referencing. (A) WT-PRF forms protein plaques on the lipid bilayer. (B) Cholesterol dependent PFO pore formation, visible as arc- and ring-shaped assemblies. A small number of the assemblies appeared higher, probably due to incomplete membrane insertion: PFO collapses from ca. 10 nm to 7 nm height upon membrane insertion.45. (C and D) When the DOPS/cholesterol bilayers were incubated first with WT-PRF and next with PFO, perforin plaques were observed adjacent to PFO pores. We here show two samples incubated with different amounts of PFO, ca. 150 nM in (C) and ca. 450 nM in (D). Consequently, the membrane surface is still visible in (C), while in (D) the PFO pores cover most of the remaining membrane. (E) Height profiles extracted along the dashed lines in (A)–(D). Horizontal lines at 0, 7, and 15 nm highlight the membrane surface and the heights of PFO pores and perforin plaques, respectively. All AFM data were recorded at room temperature. |
The preconditions and structural changes necessary to form such perforin plaques are unknown. In our earlier studies with the non-functional TMH1-PRF on pure DOPS bilayers, it emerged that in the membrane-binding and early assembly stage, i.e., before pore insertion, the behaviour of perforin is similar to that observed on DOPC bilayers:13,14 TMH1-PRF on DOPS and DOPC (i) showed a similar distribution of subunits per assembly (quantification in ref. 14), (ii) was ca. 10 nm in height above the membrane (similar to the height of an upstanding perforin molecule), and (iii) diffused freely and could be removed from the membrane surface by chelation of Ca2+ (demonstrated by the removal of oligomers after chelating calcium from the buffer, see Fig. 8A). After adding DTT and thus unlocking TMH1-PRF, the short oligomers clustered together and increased their height to ca. 15 nm (Fig. 8B). Taken together, this supports the interpretation that the formation of plaques on PS is linked to the unfurling of the protein as it attempts – unsuccessfully – to insert into the membrane.
Fig. 8 Membrane binding to DOPS membranes prior to plaque formation, assessed with TMH1-PRF. (A) AFM images of locked and unlocked TMH1-PRF on DOPS membranes. To visualize initially mobile TMH1-PRF features (not shown here) in the AFM images, we fixed the protein by addition of glutaraldehyde (GA). The patches of crosslinked perforin (‘−DTT + GA’, ‘−EGTA’) are removed by washing the samples with the calcium-chelating agent EGTA (‘−DTT + GA’, ‘+EGTA’). If TMH1-PRF is unlocked by addition of DTT, perforin plaques are formed similarly to WT-PRF (‘+DTT − GA’, ‘−EGTA’). The plaques are not visibly affected by washing with EGTA (‘+DTT − GA’, ‘+EGTA’). (B) Height profiles of cross-linked (‘−DTT + GA’) and unlocked (‘+DTT − GA’) TMH1-PRF extracted from the panels in A, as indicated by dashed lines. All images were recorded at room temperature. The panels in (A) are reproduced from ref. 14, under a Creative Commons Attribution 4.0 International License (CC BY 4.0). |
To further investigate how this behaviour depends on electrostatic interactions, we varied the concentration of divalent ions in solution, thus changing the screening of surface charges. Firstly, when 5 mM Ca2+ and an excess concentration of Mg2+ (25 mM) were present in the buffer, perforin (WT-PRF) would not bind to or form plaques on a DOPS membrane, even at higher perforin concentrations (Fig. 9A and B). Secondly, in the absence of Mg2+, the appearance of the plaques was dependent on the Ca2+ concentration in the buffer: at higher concentrations of Ca2+, there was a decrease in the spread of plaques over the membrane surface (Fig. 9C and D). The dependence of perforin membrane binding on the concentration of divalent cations further confirms that the observed behaviour on DOPS is mediated by electrostatic interactions. These two observations are different from what we observe on DOPC membranes, where a similar increase in Ca2+ concentration produced no effect on the formation of arc- and ring-shaped pores.
Fig. 9 Interaction of WT-PRF with DOPS membranes at various levels of Ca2+ and Mg2+. (A) WT-PRF on DOPS membranes at low (<1 mM) and high (25 mM) Mg2+ levels in the buffer. Perforin only forms the ca. 15 nm high plaques at low Mg2+ levels, although some protein binds at a high Mg2+ level. Here, we used 400 nM WT-PRF (instead of the 150 nM used for other experiments, see Experimental) to test the effect at high perforin concentrations. (B) Analogous experiment to (A) on DOPC instead of DOPS membranes, as a control. At both low and high Mg2+ concentrations, arc- and ring-shaped perforin pores are visible.‡ (C) Perforin plaques formed on DOPS membranes at Ca2+ concentrations of 1, 5, and 30 mM Ca2+ (with no Mg2+). For larger Ca2+ concentrations, the plaques appear less dispersed. (D) For comparison, arc- and ring-shaped pores formed on DOPC at 30 mM Ca2+. All images were recorded at room temperature. |
For functional perforin, the initial membrane binding occurs through its C2 domain. By mutating this domain in D429A-PRF,5 we could also test whether the initial perforin binding depends on lipid composition: the mutation completely abrogated D429-PRF binding to DOPC bilayers, but on DOPS membranes the mutant still formed plaques with heights of mostly ca. 7 nm and up to 15 nm (Fig. 10), roughly consistent with the plaques formed by WT-PRF (Fig. 6).
Taken together, the experimental data indicate that negatively charged membranes disrupt perforin function due to electrostatic interactions, and that the disruptions are manifested at the stage of membrane insertion. The data in Fig. 8 and 9 show that the interaction of perforin with PS membranes depends on calcium, suggesting the involvement of calcium binding sites within the C2 domain.9 As illustrated by locked TMH1-PRF in Fig. 8, perforin initially binds to PS membranes in an upright orientation, further indicating that the C2 domain is facing the membrane surface (an alternative, but somewhat far-fetched hypothesis is that the protein is bound upside down). In contrast, the C2 domain mutant perforin shows different binding to PS membranes compared to PC membranes, i.e., binding is completely absent on PC membranes. To reconcile the seemingly contradictory data, we can imagine two scenarios: (I) disruption of perforin function is caused by small differences in the binding geometry between the C2 domain and charged lipid substrates,§ leading to protein misfolding and plaque formation; (II) only a (possibly small and imperceptible in AFM images) fraction of perforin is required to bind DOPS in a different fashion, possibly independent of the C2 domain, and this fraction disables otherwise correctly bound perforin when it attempts to insert into the membrane. Of note, a similar disruptive effect was observed when functional WT-PRF was co-incubated with excess non-functional TMH1-PRF,13 although in that case, the pore forming functionality could be fully restored by subsequent addition of DTT (unlocking the disulphide lock in TMH1-PRF).
To test how the addition of PE affects pore formation by perforin, we doped a DOPC bilayer with up to 60 mol% DOPE, and exposed the resulting membranes to WT-PRF. As shown in Fig. 11A and B, the addition of DOPE had no significant influence on the pore forming capacity of perforin per se. We also performed an alternative experiment in which we tested whether addition of 80 mol% DOPE would restore pore forming capacity in a DOPS host bilayer. A qualitative assessment of the AFM images indeed indicated that the inclusion of PE caused some restoration of pore formation on DOPS membranes (Fig. 11C). This preliminary result could be explained by presuming that perforin directly binds to PE lipid headgroups. However, it is also possible that PE, with its small headgroup, provides no direct perforin binding site and, instead, introduces membrane defects that expose areas otherwise buried underneath the membrane surface or generally acts as a spacer between DOPS molecules. As a result, perforin might access and bind the PS headgroup differently, thus (partially) restoring its functionality. Future experiments will need to determine if perforin can bind PE directly.
Compared with previous results, we have here (i) demonstrated the power of AFM and model membranes in investigating the lipid specificity of pore forming proteins and of perforin in particular; (ii) used AFM to demonstrate how membrane order in gel-phase lipids completely prevents perforin binding, as previously observed for liquid-ordered domains;14 (iii) demonstrated that this lipid specificity for liquid-disordered membranes is robust against variations in divalent ion concentration (Mg2+, and Ca2+ above the threshold needed to facilitate perforin binding to the membrane); (iv) verified the extraordinary height (ca. 15 nm above the membrane) of dysfunctional perforin aggregates observed on negatively charged membranes; (v) confirmed the electrostatic nature of how such membranes disable perforin; and (vi) showed that perforin pore formation is relatively insensitive to interfacial membrane tension, although it may play a role in restoring perforin functionality on PS-rich membranes.
To assess the physiological relevance of these findings, they need to be compared with cell-based assays, e.g., possible correlations of perforin lysis with lipid order in target cell membranes,12 which confirm that reduction of lipid order sensitizes CTL membranes to perforin and that non-lytic perforin is co-localized with externalized (non-apoptotic) PS on CTLs.14
Finally, it is noted that related pore forming proteins have been reported to show specificity for particular lipids, e.g., the membrane attack complex30 and gasdermin31 show specificity for negatively charged lipids, whereas bacterial CDCs prefer cholesterol-rich and hence liquid-ordered domains in phase separated membranes.46 These observations indicate a wide range of biomedically relevant processes in which the physical properties of membranes may be determinants of the function of pore forming proteins.
Footnotes |
† Some of the observed perforin–lipid binding was different from previously published results. Without investigating this further, we point out that we used a recombinant mouse perforin mutant (vs. native human perforin elsewhere) and detected fluorescence directly (vs. primary/secondary antibody detection elsewhere). Furthermore, we noted some perforin binding that exclusively occurred in the absence of Ca2+ and disappeared after prolonged incubation in the washing buffer. The reasons for this are unknown to us. |
‡ We note that in the images depicted here, the overall perforin coverage at high Mg2+ concentration appears lower (at 400 nM WT-PRF concentration). It is not clear if this difference is significant; to date, we do not have sufficient AFM data and repeats of this experiment to rigorously quantify the number of perforin pores at high versus low Mg2+ concentrations. |
§ D429A-PRF is distinct from WT in its dual effect on the C2 domain: it is unable to bind two out of five C2 domain Ca2+ ions,9 and it also fails to undergo the conformational change required for the reorientation of W427 and Y430 residues – a critical Ca2+-dependent step required for perforin binding to a membrane.8 The fact that D429A binds to PS, but not to PC, suggests that perforin binding to PS occurs through a non-canonical mechanism that is independent of the hydrophobic interactions of W427, Y430, Y486 and W488 with the membrane.8 |
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