Literature DB >> 36043851

S2 Subunit of SARS-CoV-2 Spike Protein Induces Domain Fusion in Natural Pulmonary Surfactant Monolayers.

Xiaojie Xu1, Guangle Li1, Bingbing Sun2, Yi Y Zuo1,3.   

Abstract

Pulmonary surfactant has been attempted as a supportive therapy to treat COVID-19. Although it is mechanistically accepted that the fusion peptide in the S2 subunit of the S protein plays a predominant role in mediating viral fusion with the host cell membrane, it is still unknown how the S2 subunit interacts with the natural surfactant film. Using combined bio-physicochemical assays and atomic force microscopy imaging, it was found that the S2 subunit inhibited the biophysical properties of the surfactant and induced microdomain fusion in the surfactant monolayer. The surfactant inhibition has been attributed to membrane fluidization caused by insertion of the S2 subunit mediated by its fusion peptide. These findings may provide novel insight into the understanding of bio-physicochemical mechanisms responsible for surfactant interactions with SARS-CoV-2 and may have translational implications in the further development of surfactant replacement therapy for COVID-19 patients.

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Year:  2022        PMID: 36043851      PMCID: PMC9454269          DOI: 10.1021/acs.jpclett.2c01998

Source DB:  PubMed          Journal:  J Phys Chem Lett        ISSN: 1948-7185            Impact factor:   6.888


Severe acute respiratory syndrome coronavirus 2 (SARS-CoV-2), the virus responsible for coronavirus disease 2019 (COVID-19), is causing a global pandemic with millions of deaths. SARS-CoV-2 is an enveloped, positive-sense, single-stranded RNA virus with a genome size of ∼30 kb.[1] It consists of four structural proteins, namely, nucleocapsid (N), membrane (M), envelope (E), and spike (S).[1] Among these proteins, the S protein is the major mediator of cellular infection, which determines the attachment of SARS-CoV-2 onto the host cell membrane and the subsequent membrane fusion. During infection, the S protein recognizes and binds to angiotensin-converting enzyme 2 (ACE2) on the host cell membrane and thus mediates viral cellular entry.[2] The S protein is a heavily glycosylated, trimeric, type I membrane protein anchored on the exterior surface of the mature virion.[3] Each monomer of the trimeric S protein is about 180 kDa with 1273 amino acids. It is composed of a signal peptide (residues 1–13) and two functional subunits, that is, the S1 subunit (residues 14–685) responsible for binding to the host cell receptor and the S2 subunit (residues 686–1273) responsible for fusion of the viral and cellular membranes.[4] Once bound to the cell membrane, the S protein undergoes cleavage by proteases, such as furin, into the S1 and S2 subunits.[5] As illustrated in Figure A, the S1 subunit consists of an N-terminal domain and a receptor-binding domain that interacts with ACE2. The S2 subunit consists of a fusion peptide, central helix, connecting domain, heptad repeat 1 and 2, transmembrane domain, and cytoplasmic tail (Figure A,B). After S protein cleavage and membrane fusion, a fusion pore forms between viral and cellular membranes, which facilitates delivery of the viral genetic information into the host cell cytoplasm for further replication and transcription.
Figure 1

(A) Primary structure of the SARS-CoV-2 S protein. It is composed of the S1 and S2 subunits. The S1 subunit contains an N-terminal domain (NTD) and a receptor-binding domain (RBD). The S2 subunit consists of a fusion peptide (FP), central helix (CH), connecting domain (CD), heptad repeat 1 (HR1) and 2 (HR2), transmembrane (TM) domain, and cytoplasmic tail (CT). (B) Cryo-EM structures of the S2 subunit from the Protein Data Bank ID 6VXX. (C) Constrained drop surfactometry (CDS) for probing biophysical interactions between natural pulmonary surfactant and the S2 subunit.

(A) Primary structure of the SARS-CoV-2 S protein. It is composed of the S1 and S2 subunits. The S1 subunit contains an N-terminal domain (NTD) and a receptor-binding domain (RBD). The S2 subunit consists of a fusion peptide (FP), central helix (CH), connecting domain (CD), heptad repeat 1 (HR1) and 2 (HR2), transmembrane (TM) domain, and cytoplasmic tail (CT). (B) Cryo-EM structures of the S2 subunit from the Protein Data Bank ID 6VXX. (C) Constrained drop surfactometry (CDS) for probing biophysical interactions between natural pulmonary surfactant and the S2 subunit. In COVID-19-associated acute respiratory distress syndrome (ARDS),[6] SARS-CoV-2 attacks alveolar epithelial cells, where the ACE2 receptor is highly expressed.[7] Damage to type II alveolar epithelial cells could compromise the synthesis and function of the endogenous pulmonary surfactant (PS) that plays a crucial physiological role in host defense and alveolar surface tension reduction. The PS is composed of ∼80 wt % phospholipids, with dipalmitoylphosphatidylcholine (DPPC) being the major lipid species, ∼10 wt % cholesterol, and ∼10 wt % surfactant-associated proteins SP-A, -B, -C, and -D.[8] SP-A and SP-D, presenting in airways and the alveolar regions, were found to bind to the S protein, thus mitigating infection of the epithelial cells through viral neutralization, agglutination, and enhanced phagocytosis.[9,10] In addition, a recent clinical trial showed that the DPPC levels in the bronchoalveolar lavage fluids of COVID-19 patients were lower than those in healthy controls.[11] All this evidence justified the hypothesis that exogenous surfactant therapy, in which clinical surfactant preparations extracted from animals’ lungs are delivered to patients’ lungs, may be used as a supportive therapy to treat patients with COVID-19 and COVID-19-associated ARDS.[12−14] There have been multiple ongoing clinical trials in the past two years.[14] Although the verdict is still out, preliminary reports have demonstrated promise for the surfactant therapy in managing the progress of COVID-19.[15,16] Clinical application of the exogenous surfactant therapy in COVID-19 entails a biophysical understanding of specific interactions between the PS film and the functional group of SARS-CoV-2 responsible for mediating membrane fusion. It is mechanistically accepted that the fusion peptide (FP) in the S2 subunit of the S protein takes a central role in mediating the initial penetration of the virus into the host cell membrane.[5,17,18] There have been a few in silico studies based on molecular dynamics simulations that investigated the specific FP-lipid interactions in the initial stage of SARS-CoV-2 infection.[19,20] However, it is still unknown how the FP of the S2 subunit interacts with or adversely impacts the natural PS film. Here, we experimentally studied the specific biophysical interactions between the recombinant S2 subunit and an animal-derived clinical surfactant, that is, Infasurf, using constrained drop surfactometry (CDS) (Figure C).[21,22] With biophysical simulations using CDS and molecular visualization using atomic force microscopy (AFM), we found that the S2 subunit inhibited the biophysical properties of PS and, most importantly, directly induced fusion of phospholipid microdomains in the Infasurf monolayer. These results may provide novel insight into the understanding of biophysical mechanisms responsible for PS interactions with SARS-CoV-2 and may have translational implications in further developing the surfactant replacement therapy for COVID-19 patients. Figure shows the biophysical impact of the S2 subunit on the Infasurf film under physiologically relevant conditions. Reproducibility is demonstrated in Figure S1 of the Supporting Information. The surface area of the Infasurf film was oscillated with a 20% compression ratio (CR) and a highly dynamic rate of 3 s per compression–expansion cycle, to mimic breathing.[23]Figure A shows cycles of 1 mg/mL Infasurf with a low 0.15 mol % or a moderate 0.75 mol % S2 subunit. The minimum surface tension (γmin) of Infasurf is increased from 2.9 to 4.4 mN/m with 0.15% S2 subunit and to 6.5 mN/m with 0.75% S2 subunit, indicating significant surfactant inhibition (Figure B). The compressibility (κcomp) of the Infasurf film is increased from 0.64 to 0.71 m/mN with the addition of 0.15% S2 subunit and to 1.06 m/mN with 0.75% S2 subunit (Figure C). The film compressibility is a quantitative measure of the “softness” of the PS film.[8] The increase of film compressibility is an indication of the strong implication of biophysical inhibition of the PS, since more area reduction is needed to decrease the surface tension.
Figure 2

Effect of the S2 subunit (0.15 and 0.75 mol %) on the biophysical properties of 1 mg/mL Infasurf, with various compression ratios (CRs). (A–C) 20% CR, (D–F) 30% CR, and (G–I) 40% CR. (A, D, G) show the dynamic compression–expansion cycles of Infasurf with/without the S subunit. (B, E, H) show the statistical analysis of γmin and maximum surface tension (γmax). (C, F, I) show the analysis of κcomp and the compressibility for the expansion process (κexp). Results shown are the tenth cycle. *p < 0.05 suggests statistically significant differences in comparison to pure Infasurf film without the S2 subunit.

Effect of the S2 subunit (0.15 and 0.75 mol %) on the biophysical properties of 1 mg/mL Infasurf, with various compression ratios (CRs). (A–C) 20% CR, (D–F) 30% CR, and (G–I) 40% CR. (A, D, G) show the dynamic compression–expansion cycles of Infasurf with/without the S subunit. (B, E, H) show the statistical analysis of γmin and maximum surface tension (γmax). (C, F, I) show the analysis of κcomp and the compressibility for the expansion process (κexp). Results shown are the tenth cycle. *p < 0.05 suggests statistically significant differences in comparison to pure Infasurf film without the S2 subunit. Other than the physiologically relevant 20% CR, dynamic surface activities of the Infasurf film were also studied at supraphysiological levels of 30% and 40% CRs (Figure D–I). Similar to 20% CR, the addition of 0.75% S2 subunit more than doubles the corresponding γmin and κcomp of the Infasurf film, thus indicating significant biophysical inhibition of the PS function. Figure demonstrates the isothermal compression of Infasurf at a quasi-static rate of 0.1 cm2/min, with and without S2 subunit injected into the subphase, that is, the droplet, to a protein concentration of 0.05 mg/mL. The compression isotherms of the Infasurf monolayer with a faster compression of 0.3 cm2/min and with a higher S2 concentration of 0.1 mg/mL were also studied (Figure S2). It can be seen that, at two temperatures—20 and 37 °C—the S2 subunit injected into the subphase significantly increases the initial surface pressure prior to monolayer compression, to the surface pressure of ∼20 mN/m, corresponding to the S2 subunit’s equilibrium surface tension at 50 mN/m (see Figure S3 for adsorption kinetics of the S2 subunit). At both temperatures, the compression isotherms reach a plateau region at the equilibrium spreading pressure (πeq) of surfactant at 50 mN/m, where the PS monolayer is transformed into a multilayer.[24,25] While the Infasurf monolayer at 20 °C can be further compressed to a metastable supracompressed state above the πeq,[24,26] the Infasurf monolayer with the subphase-injected S2 subunit spontaneously collapses at πeq, thus indicating the S2 subunit-induced surfactant inhibition.
Figure 3

Effect of the S2 subunit on the quasi-static compression isotherms of spread Infasurf monolayers. Aqueous solution of the S2 subunit was subphase injected to a protein concentration of 0.05 mg/mL prior to monolayer compression. The Infasurf monolayer was quasi-statically compressed at a rate of 0.1 cm2/min, under two environmental temperatures of 20 and 37 °C.

Effect of the S2 subunit on the quasi-static compression isotherms of spread Infasurf monolayers. Aqueous solution of the S2 subunit was subphase injected to a protein concentration of 0.05 mg/mL prior to monolayer compression. The Infasurf monolayer was quasi-statically compressed at a rate of 0.1 cm2/min, under two environmental temperatures of 20 and 37 °C. Figure shows AFM topographic images of Infasurf at the characteristic surface pressure of 30 mN/m, with/without the S2 subunit under two environmental temperatures of 20 and 37 °C, respectively. Figures S4–S7 show the reproducibility of these images. At 20 °C (Figure A), the Infasurf monolayer shows microscale and nanoscale tilted-condensed (TC) domains that are approximately 0.8–1.0 nm higher than the liquid-expanded (LE) phase, which is mostly composed of fluid phospholipids. These TC domains mainly contain solid-like disaturated phospholipids, largely DPPC. These microdomains have a nearly circular shape with a diameter of 3–5 μm, in good agreement with our previous observations.[24]
Figure 4

AFM images of Infasurf with/without the addition of the S2 subunit, under two environmental temperatures of 20 and 37 °C, respectively. (A) Infasurf at 20 °C, (B) Infasurf with S2 at 20 °C, (C) Infasurf at 37 °C, and (D) Infasurf with S2 at 37 °C. All AFM images were obtained at the characteristic surface pressure of 30 mN/m. AFM images in the first row are 20 × 20 μm in the lateral dimension and 5 nm in the z range. Images in the middle row demonstrate the enlarged structures in the white boxes. The bottom row shows the 3D renderings of the topographic images shown in the middle row. White arrows point to designated lateral and altitudinal dimensions.

AFM images of Infasurf with/without the addition of the S2 subunit, under two environmental temperatures of 20 and 37 °C, respectively. (A) Infasurf at 20 °C, (B) Infasurf with S2 at 20 °C, (C) Infasurf at 37 °C, and (D) Infasurf with S2 at 37 °C. All AFM images were obtained at the characteristic surface pressure of 30 mN/m. AFM images in the first row are 20 × 20 μm in the lateral dimension and 5 nm in the z range. Images in the middle row demonstrate the enlarged structures in the white boxes. The bottom row shows the 3D renderings of the topographic images shown in the middle row. White arrows point to designated lateral and altitudinal dimensions. Addition of the S2 subunit completely alters the lateral structure of the Infasurf monolayer. The most striking change caused by the S2 subunit is the morphology of the microdomains. As shown in Figure B, the microdomains, ∼1 nm higher than the LE phase, mostly merge into an irregular wormlike shape. A small amount of isolated circular microdomains still appears in the monolayer but exists with a much smaller diameter than that of the Infasurf monolayer (1.5 vs 3.8 μm). A similar effect of the S2 subunit on the Infasurf monolayer is also found at 37 °C. As shown in Figure C, microdomains of the Infasurf monolayer at 37 °C are, in general, smaller than those at 20 °C (1.3 vs 3.8 μm). A subphase-injected S2 subunit also causes fusion of microdomains in the Infasurf monolayer at 37 °C (Figure D). Figure shows the quantified domain coverage of the Infasurf monolayer. In general, addition of the S2 subunit increases the area fraction of microdomains but decreases the area fraction of the nanodomains. However, the total area fraction of microdomains and nanodomains remains at around 25–30% and does not appear to change with the addition of the S2 subunit. Infasurf contains a total of approximately 40% disaturated phospholipids, mostly DPPC.[24] Therefore, it appears that the lipid composition of the Infasurf monolayer, with and without the S2 subunit, is close to that of Infasurf. Hence, the S2 subunit only varies the domain morphology by inducing domain fusion, instead of changing the lipid composition of the natural PS film.
Figure 5

Quantification results for the Infasurf monolayer coverage of TC microdomains and nanodomains at surface pressure 30 mN/m.

Quantification results for the Infasurf monolayer coverage of TC microdomains and nanodomains at surface pressure 30 mN/m. The equilibrium morphology of microdomains of phospholipid monolayers is controlled by competition of line tension at the domain boundaries and electrostatic repulsion between lipid headgroups in the domain.[8] A large line tension favors the formation of a small number of larger domains with a round shape, thus minimizing the total domain boundaries. This mechanism explains why the size of microdomains in the Infasurf monolayer at 37 °C is much smaller than that at 20 °C (Figure A vs C), because, in general, line tension decreases with temperature. The dramatic change of microdomain morphology with the addition of the S2 subunit (Figure A vs B and Figure C vs D) must be caused by a significantly reduced line tension at the domain boundary. It is not unexpected that the fusion peptide of the S2 subunit selectively partitions into the microdomain boundaries to reduce line tension. It has been proposed that line tension dominates the human immunodeficiency virus (HIV) FP-mediated fusion.[27] Since the solid-like domains mostly consist of ordered lipid phases, they are energetically unfavorable for membrane fusion when it comes to infection by enveloped viruses, such as HIV and influenza. It has been found that line tension induces HIV gp41-FP-mediated fusion.[27] Similarly, line tension was found to be a significant control factor for membrane fusion mediated by influenza hemagglutinin.[28] A critical stage of viral infection is the fusion between viral and host cell membranes. The FP of the S2 subunit is responsible for the initial penetration of the virus into the host cell membrane.[29] The FP is a relatively hydrophobic residue located at the N-terminus of the S2 subunit. Molecular dynamics simulations have shown that residues L821, L822, and F823 in the helical portion of the FP can deeply insert into the hydrophobic core of a model membrane, thus closely interacting with the membrane lipids.[19] Other hydrophobic residues of the FP may also contribute to binding to biomembrane, thus minimizing its exposure to water. Once bound to the membrane, a fully conserved disulfide bridge in the FP establishes the strong anchoring that is required for subsequent membrane fusion.[20] In comparison to extensive studies of the FP-mediated membrane fusion, it is still unknown how the FP of an enveloped virus affects the natural PS film. The endogenous PS film adsorbed at the alveolar surface is a lipid–protein biomembrane that consists of an interfacial monolayer with functionally attached multilayers composed of hundreds of fluid phospholipids.[22,30] In terms of membrane structures, the PS monolayer controlled at the surface pressure 30 mN/m can be loosely considered as a natural model mimicking a single leaflet of a biomembrane, since the lateral pressure of enclosed bilayers is largely conserved at 30 mN/m.[31] Using combined biophysical simulations with CDS and direct membrane imaging with AFM, we have established two experimental findings. First, the S2 subunit at a molar ratio of 0.75% with respect to phospholipids strongly inhibited the biophysical function of a natural PS (Figure ). Second, the S2 subunit subphase injected at a low concentration of 0.05 mg/mL induced significant domain fusion in the natural PS monolayer (Figure ). These two biophysical findings are interrelated, since the membrane fluidization caused by the penetration of the S2 subunit is most likely responsible for the surfactant inhibition as revealed by the increase of film compressibility. It has been shown that the FP of the S2 subunit transforms from an intrinsically disordered state in an aqueous solution into a wedge-shaped structure inserting into bilayered micelles, with the hydrophobic, narrow end of the wedge contacting the fatty acyl chains of the phospholipids and the polar end of the wedge interacting with the lipid head groups and binding calcium ions for membrane fusion.[32] A similar mechanism may be also responsible for the penetration of the S2 subunit into the natural PS film. Moreover, it has been reported that the FP-mediated fusion became more favorable for membranes containing cholesterol[33] and negatively charged phospholipids,[34] likely due to electrostatic interactions promoted by the positively charged FP. The natural PS contains 20% anionic phospholipids, including phosphatidylglycerol, phosphatidylinositol, and lysophosphatidic acid, and up to 10% cholesterol.[8] Hence, the FP-mediated fusion is expected to prevail in the natural PS film. Nevertheless, it should be noted that the surfactant preparation used in this study, that is, Infasurf, is devoid of the hydrophilic surfactant proteins SP-A and SP-D.[24] It is known that these immunological proteins, especially SP-D, modulate viral infection in the lung. It has been shown that a recombinant fragment of human SP-D inhibits replication and infection of SARS-CoV-2.[10] However, the molecular mechanism appears to be mostly related to the SP-D-mediated interaction between the S1 subunit of SARS-CoV-2 and the ACE2 receptor of the host cells.[10] Hence, lack of hydrophilic surfactant proteins in Infasurf does not likely vary our conclusions about the S2 subunit-mediated domain fusion found in natural PS films. Using combined biophysical simulations and AFM imaging, we have studied the biophysical impact of the S2 subunit on a natural PS film, Infasurf. We have concluded that the S2 subunit can inhibit the biophysical properties of the PS. We have provided direct experimental evidence for S2 subunit-induced microdomain fusion in the Infasurf monolayer. The surfactant inhibition has been attributed to the membrane fluidization caused by insertion of the S2 subunit mediated by its fusion peptide. These findings may provide novel insight into the understanding of biophysical mechanisms responsible for PS interactions with SARS-CoV-2 and may have translational implications in the further development of surfactant replacement therapy for COVID-19 patients.
  34 in total

1.  Relations among alveolar surface tension, surface area, volume, and recoil pressure.

Authors:  H Bachofen; S Schürch; M Urbinelli; E R Weibel
Journal:  J Appl Physiol (1985)       Date:  1987-05

2.  A modified squeeze-out mechanism for generating high surface pressures with pulmonary surfactant.

Authors:  Eleonora Keating; Yi Y Zuo; Seyed M Tadayyon; Nils O Petersen; Fred Possmayer; Ruud A W Veldhuizen
Journal:  Biochim Biophys Acta       Date:  2011-12-21

3.  Comparative study of clinical pulmonary surfactants using atomic force microscopy.

Authors:  Hong Zhang; Qihui Fan; Yi E Wang; Charles R Neal; Yi Y Zuo
Journal:  Biochim Biophys Acta       Date:  2011-03-23

Review 4.  Current perspectives in pulmonary surfactant--inhibition, enhancement and evaluation.

Authors:  Yi Y Zuo; Ruud A W Veldhuizen; A Wilhelm Neumann; Nils O Petersen; Fred Possmayer
Journal:  Biochim Biophys Acta       Date:  2008-04-08

5.  Molecular Architecture of the SARS-CoV-2 Virus.

Authors:  Hangping Yao; Yutong Song; Yong Chen; Nanping Wu; Jialu Xu; Chujie Sun; Jiaxing Zhang; Tianhao Weng; Zheyuan Zhang; Zhigang Wu; Linfang Cheng; Danrong Shi; Xiangyun Lu; Jianlin Lei; Max Crispin; Yigong Shi; Lanjuan Li; Sai Li
Journal:  Cell       Date:  2020-09-06       Impact factor: 41.582

6.  Surfactant for the Treatment of ARDS in a Patient With COVID-19.

Authors:  Moshe Heching; Shaul Lev; Dorit Shitenberg; Dror Dicker; Mordechai R Kramer
Journal:  Chest       Date:  2021-01-22       Impact factor: 9.410

7.  Reduced levels of pulmonary surfactant in COVID-19 ARDS.

Authors:  Peter Schousboe; Andreas Ronit; Henning B Nielsen; Thomas Benfield; Lothar Wiese; Nikolaos Scoutaris; Henrik Verder; Ronan M G Berg; Povl Verder; Ronni R Plovsing
Journal:  Sci Rep       Date:  2022-03-08       Impact factor: 4.379

Review 8.  Acute respiratory distress syndrome.

Authors:  Nuala J Meyer; Luciano Gattinoni; Carolyn S Calfee
Journal:  Lancet       Date:  2021-07-01       Impact factor: 79.321

9.  SARS-CoV-2 Cell Entry Depends on ACE2 and TMPRSS2 and Is Blocked by a Clinically Proven Protease Inhibitor.

Authors:  Markus Hoffmann; Hannah Kleine-Weber; Simon Schroeder; Nadine Krüger; Tanja Herrler; Sandra Erichsen; Tobias S Schiergens; Georg Herrler; Nai-Huei Wu; Andreas Nitsche; Marcel A Müller; Christian Drosten; Stefan Pöhlmann
Journal:  Cell       Date:  2020-03-05       Impact factor: 41.582

10.  Distinct conformational states of SARS-CoV-2 spike protein.

Authors:  Yongfei Cai; Jun Zhang; Tianshu Xiao; Hanqin Peng; Sarah M Sterling; Richard M Walsh; Shaun Rawson; Sophia Rits-Volloch; Bing Chen
Journal:  Science       Date:  2020-07-21       Impact factor: 47.728

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