Bálint Kiss1, Zoltán Kis2,3, Bernadett Pályi2, Miklós S Z Kellermayer1,4. 1. Department of Biophysics and Radiation Biology, Semmelweis University, Tűzoltó str. 37-47, Budapest H-1094, Hungary. 2. National Biosafety Laboratory, National Public Health Center, Albert Flórián Rd 2-6, Budapest H-1097, Hungary. 3. Department of Medical Microbiology, Semmelweis University, Nagyvárad Sq. 4, Budapest H-1089, Hungary. 4. Hungarian Centre of Excellence for Molecular Medicine (HCEMM), In Vivo Imaging Advanced Core Facility, Budapest H-1094, Hungary.
Abstract
SARS-CoV-2, the virus responsible for the current COVID-19 pandemic, displays a corona-shaped layer of spikes which play a fundamental role in the infection process. Recent structural data suggest that the spikes possess orientational freedom and the ribonucleoproteins segregate into basketlike structures. How these structural features regulate the dynamic and mechanical behavior of the native virion are yet unknown. By imaging and mechanically manipulating individual, native SARS-CoV-2 virions with atomic force microscopy, here, we show that their surface displays a dynamic brush owing to the flexibility and rapid motion of the spikes. The virions are highly compliant and able to recover from drastic mechanical perturbations. Their global structure is remarkably temperature resistant, but the virion surface becomes progressively denuded of spikes upon thermal exposure. The dynamics and the mechanics of SARS-CoV-2 are likely to affect its stability and interactions.
SARS-CoV-2, the virus responsible for the current COVID-19 pandemic, displays a corona-shaped layer of spikes which play a fundamental role in the infection process. Recent structural data suggest that the spikes possess orientational freedom and the ribonucleoproteins segregate into basketlike structures. How these structural features regulate the dynamic and mechanical behavior of the native virion are yet unknown. By imaging and mechanically manipulating individual, native SARS-CoV-2 virions with atomic force microscopy, here, we show that their surface displays a dynamic brush owing to the flexibility and rapid motion of the spikes. The virions are highly compliant and able to recover from drastic mechanical perturbations. Their global structure is remarkably temperature resistant, but the virion surface becomes progressively denuded of spikes upon thermal exposure. The dynamics and the mechanics of SARS-CoV-2 are likely to affect its stability and interactions.
Entities:
Keywords:
COVID-19; atomic force microscopy; force spectroscopy; mechanical resilience; nanoindentation; thermal stability
Severe acute respiratory syndrome
coronavirus 2 (SARS-CoV-2), the infective agent behind the current
coronavirus disease (COVID-19) pandemic,[1,2] is an enveloped
ssRNA virus with a corona-shaped surface layer of spikes that are
thought to play an important role in the infection mechanism.[3−7] Structural information about the spike protein has been acquired
either on crystals of purified protein[5,8−10] or on fixed and frozen virus particles.[11−13] It has been
suggested that the spike hinges provide structural flexibility.[11,12] High-resolution cryoelectron tomography observations indicate that
the ribonucleoprotein (RNP) of SARS-CoV-2 is partitioned into spherical,
basketlike structures.[13] However, the surface
dynamics and mechanical properties of native virions remain to be
understood. Here, we employed atomic force microscopy (AFM) and molecular
force spectroscopy[14−16] to investigate the topographical and nanomechanical
properties of native SARS-CoV-2 virions immobilized on an anti-spike-protein-functionalized
substrate surface. The unique single-particle approach revealed that
the surface layer of spikes on SARS-CoV-2 is highly dynamic; the virion
is unusually compliant and resilient, and it displays an unexpected
global thermal stability.The topographical structure of individual
SARS-CoV-2 virus particles
bound to the substrate surface was imaged using AFM (Figure a). To increase the efficiency
and specificity of binding, we employed a monoclonal anti-spike-protein
antibody, which resulted in a nearly 100-fold enhancement in the density
of substrate-bound virions (Figure S1).
AFM images of glutaraldehyde-fixed SARS-CoV-2 revealed virions (Figure b) with somewhat
variable dimensions (Table S1) and a rugged
surface (Figure c).
The mean central height of the virions (Figure S2), the structural parameter least sensitive to AFM tip convolution,
was 62 nm (±8 nm, standard deviation (SD)) The height was smaller
than the virion diameter measured in cryo-electron microscopic images,[11−13] suggesting that the virus particles were partially flattened on
the substrate. The 3D-rendered AFM image (Figure d) supported this interpretation and revealed
that the rugged surface is due to the presence of protrusions which
we identify as the spikes (S protein trimers) based on earlier topographical
results on SARS-CoV[17,18] and more recent cryo-electron
microscopic[11,12] data on the whole SARS-CoV-2
virion. In high-resolution (pixel size 5 Å) AFM images (Figure e and Figure S4a–d), individual S trimers could
sometimes be resolved based on the characteristic triangular appearance.
Visual inspection of the S trimers pointed at their positional (Figure S3c), flexural (Figure S3d), and rotational (Figure S4e) disorder in the viral envelope. The mean nearest-neighbor distance
between the S trimers and their topographical height were 21 nm (±6
nm, SD) and 13 nm (±5 nm, SD), respectively (Figure S3 and Table S2). From the mean nearest-neighbor distance
and the virion dimensions, and presuming that the spikes remain evenly
distributed over the virus surface during sample preparation, we calculated
that an average of 61 spikes cover the SARS-CoV-2 virus particle surface.
This number exceeds those reported recently (24,[11] 26,[13] and 40[12]), suggesting that the spike number is highly variable and
may be regulated during virus assembly and maturation in the host
cell.[19] The flexural disorder observed
here supports the interpretation of cryo-electron microscopic data,[11−13] revealing a high degree of spike flexibility. We propose that the
positional and rotational disorder of S trimers is due to their mobility
in the virus envelope.
Figure 1
Topographical structure of SARS-CoV-2 virions treated
with 5% glutaraldehyde.
(a) Schematics of scanning substrate-surface-bound virions with the
AFM tip. PLL: poly-l-lysine. (b) AFM image of an overview
(1.5 × 1.5 μm) sample area. (c) Zoomed-in AFM image of
SARS-CoV-2 virions. The virion surfaces are covered with protrusions
that correspond to spikes (S protein trimers). Inset: Topographical
profile plot measured along the center of one of the virions (dotted
line). The profile plot reveals a rugged surface. (d) 3D-rendered
image of a SARS-CoV-2 virion. A partially flattened virus particle
is observed, pointing at a global flexibility of the virion. (e) High-resolution
AFM image of a SARS-CoV-2 virion displaying axial view of S trimers.
(i) AFM image of the entire virion. (ii) Enlarged and contrast-enhanced
image of the rectangular area. (iii) Same AFM image with overlaid
triangles indicating S trimer orientation. The spikes apparently display
translational, rotational, and flexural disorder owing to their flexibility.
Topographical structure of SARS-CoV-2 virions treated
with 5% glutaraldehyde.
(a) Schematics of scanning substrate-surface-bound virions with the
AFM tip. PLL: poly-l-lysine. (b) AFM image of an overview
(1.5 × 1.5 μm) sample area. (c) Zoomed-in AFM image of
SARS-CoV-2 virions. The virion surfaces are covered with protrusions
that correspond to spikes (S protein trimers). Inset: Topographical
profile plot measured along the center of one of the virions (dotted
line). The profile plot reveals a rugged surface. (d) 3D-rendered
image of a SARS-CoV-2 virion. A partially flattened virus particle
is observed, pointing at a global flexibility of the virion. (e) High-resolution
AFM image of a SARS-CoV-2 virion displaying axial view of S trimers.
(i) AFM image of the entire virion. (ii) Enlarged and contrast-enhanced
image of the rectangular area. (iii) Same AFM image with overlaid
triangles indicating S trimer orientation. The spikes apparently display
translational, rotational, and flexural disorder owing to their flexibility.To circumvent the effects caused by chemical fixation
and to uncover
the spike dynamics in situ, we investigated the topography of unfixed,
native SARS-CoV-2 virions (Figure ). Unexpectedly, we were unable to resolve S trimers
on the virion surface at any of the investigated scanning strengths
(Figure S5); rather, the virus particles
displayed a blurred, smooth surface (Figure a). The mean central height of the native
virions was 83 nm (±7 nm, SD), which is significantly greater
than that observed for the fixed one (Figure b). We interpret the blurring of virion topography
as the result of aperture error caused by time averaging of spike
movement within the sampling region of each image pixel, hence the
increase in virion height is caused by the AFM tip scanning an apparent
dynamic surface (Figure c). Most plausibly, spike motion is dictated by the Brownian dynamics
of the receptor-binding-domain (RBD) trimer, which may then be thought
of as a tethered particle. Spike mobility in the virus envelope may
contribute further to the observed dynamics. An alternative explanation
for the observed blurred virion surface is that the spikes evade the
moving AFM cantilever tip, which then scans the envelope surface.
However, while it relies on a similarly dynamic spike behavior, a
reduced virion height should have been observed. We speculate that
the rapid spike motion revealed by these experiments may contribute
to an efficient dynamic search by the virion on the surface of the
targeted host cell, which explains why SARS-CoV-2 is at least as infective
as the influenza virus[20] in spite of its
fewer spikes (up to ∼60 in SARS-CoV-2 versus up to ∼350
in influenza A[21]).
Figure 2
Topographical analysis
of native, unfixed SARS-CoV-2 virions. (a.i)
AFM image of an overview (0.8 × 1 μm) sample area. Inset:
Topographical profile plot measured along the horizontal diameter
of one of the virions (dotted line), revealing a smooth surface. (a.ii,iii)
Magnified image of a fixed and native virion, respectively, for better
comparison. Surface protrusions are not resolved in the native virus
particle, but a blurred, smooth topography is observed. (b) Distribution
of the topographical maximal central height of fixed and unfixed SARS-CoV-2
virions obtained from particle analysis (see Figure S2). The bimodal distribution seen in both histograms may be
associated with spike position. Mean particle height (±SD) of
fixed and unfixed virions are 62 ± 8 and 83 ± 7 nm, respectively.
Unfixed virions have a particle height significantly larger than that
of the fixed ones. (c) Schematics explaining the dynamically enhanced
height of the unfixed virion.
Topographical analysis
of native, unfixed SARS-CoV-2 virions. (a.i)
AFM image of an overview (0.8 × 1 μm) sample area. Inset:
Topographical profile plot measured along the horizontal diameter
of one of the virions (dotted line), revealing a smooth surface. (a.ii,iii)
Magnified image of a fixed and native virion, respectively, for better
comparison. Surface protrusions are not resolved in the native virus
particle, but a blurred, smooth topography is observed. (b) Distribution
of the topographical maximal central height of fixed and unfixed SARS-CoV-2
virions obtained from particle analysis (see Figure S2). The bimodal distribution seen in both histograms may be
associated with spike position. Mean particle height (±SD) of
fixed and unfixed virions are 62 ± 8 and 83 ± 7 nm, respectively.
Unfixed virions have a particle height significantly larger than that
of the fixed ones. (c) Schematics explaining the dynamically enhanced
height of the unfixed virion.We investigated the mechanical properties of SARS-CoV-2 by lowering
the cantilever tip on the vertex of individual virions selected on
the AFM image (Figure a). The virion was indented by pressing the tip downward (Figure b) with constant
velocity (typically 0.5 μm/s) until a preset maximum force,
measured by the cantilever deflection, was reached (typically 2–3
nN). Such a nanomechanical manipulation did not result in permanent
topographical changes (Figure c and Figure S6) in spite of completely
compressing the virion so that the tip reached all the way to the
substrate, resulting in a wall-to-wall deformation (Figure d). In the initial stage of
indentation, immediately following the landing of the tip on the virion,
we observed a linear force response devoid of discrete mechanical
events (Figure S7), which allowed us to
measure virion stiffness (Table S3). Mean
stiffness was 13 pN/nm (±5 pN/nm, SD), which makes SARS-CoV-2
the most compliant virus investigated so far.[22,23] Virion stiffness is somewhat lower than that measured for the influenza
virus lipid envelope,[24] suggesting that
the elasticity of SARS-CoV-2 is dominated by its envelope, and the
RNP contributes little to the overall viral mechanics. The elastic
regime was followed by a yield point marking the deviation from the
linear force response and the onset of force-induced structural transitions
which continued to take place until total compression. Unlike in other
viruses,[14,25] force did not drop to near zero values following
mechanical yield, indicating that virion collapse or breakage was
not evoked in spite of the drastic mechanical perturbation. Conceivably,
the mechanical yield is made possible by the force-induced rearrangement
of the basketlike structures of the RNPs.[13] Subsequent to indentation, we retracted the cantilever. Remarkably,
the virion generated forces up to several hundred pN during retraction,
suggesting that structural recovery was taking place, possibly driven
by the restitution of the initial RNP arrangement. The process continued
until the initial virion height was re-established. The mean force–spectroscopic
height was 94 nm (±10 nm, SD), which is comparable to that obtained
from topographical data. The differences between the indentation and
retraction force traces revealed a force hysteresis indicating that
part of the mechanical energy invested in distorting the virion was
dissipated as heat (Figure S8). We were
able to continue the indentation–retraction cycles up to 100
times, but the virions never broke or collapsed (Figure e,f). Rather, both the indentation
and retraction force traces relaxed after about 10 mechanical cycles,
resulting in a minimized force hysteresis corresponding to a dissipated
heat of ∼25 aJ. The force response may potentially be explained
by two other mechanisms alternative to virion compression. The first
one is the force-induced virion rolling on the substrate. We exclude
this possibility because, due to the presence of anti-spike-protein
antibodies on the surrounding surface, the process is expected to
be completely irreversible. The second is the sideways slippage of
the cantilever tip off the virion surface. We exclude this possibility
based on a calibration of the cantilever’s lateral torsion
(Figure S9) and because this process is
expected to be completely reversible. We can only speculate about
the mechanisms behind the persistent structural self-healing of SARS-CoV-2.
Conceivably, the process involves the dynamic interaction between
the RNA, protein, and lipid components. Notably, in some (∼1%)
of the retraction traces, we observed sawtooth-shaped force responses,
the peak forces of which fall between ∼210 and 330 pN (Figure f). The most plausible
explanation is that the force peaks correspond to the mechanically
driven unfolding of S protein domains, which is supported by the similar
unfolding forces calculated with molecular dynamics simulation.[26] Altogether, the SARS-CoV-2 virion is a mechanically
stable, remarkably compliant and surprisingly resilient nanoparticle.
Figure 3
Single-particle
force spectroscopy of SARS-CoV-2 virions. (a) AFM
image of an overview (1 × 1 μm) sample area prior to nanomechanical
manipulation. Asterisk shows the virion selected for nanomechanical
manipulation. (b) Schematics of the force spectroscopy experiment.
The virion is indented with the AFM tip until a preset force (typically
2–3 nN) is reached. (c) AFM image of the same overview sample
area following nanomechanical manipulation. We could not detect any
topographical sign of permanent structural change. (d) Example of
a force versus distance curve obtained during a single indentation–retraction
cycle. From the slope of the indentation curve (gray dotted line)
and the distance between the landing point and substrate limit of
the trace, we obtained the stiffness and the force–spectroscopic
height of the virions, respectively. Red and blue dotted lines indicate
indentation and retraction data, respectively, obtained in the 100th
nanomechanical cycle. (e) Force versus distance curves obtained during
repeated indentation of a single SARS-CoV-2 virion. (f) Matching force
versus distance curves obtained during retraction. In some traces,
force sawteeth (red trace) correspond to the unfolding of domains
in a surface protein, plausibly within the S trimer.
Single-particle
force spectroscopy of SARS-CoV-2 virions. (a) AFM
image of an overview (1 × 1 μm) sample area prior to nanomechanical
manipulation. Asterisk shows the virion selected for nanomechanical
manipulation. (b) Schematics of the force spectroscopy experiment.
The virion is indented with the AFM tip until a preset force (typically
2–3 nN) is reached. (c) AFM image of the same overview sample
area following nanomechanical manipulation. We could not detect any
topographical sign of permanent structural change. (d) Example of
a force versus distance curve obtained during a single indentation–retraction
cycle. From the slope of the indentation curve (gray dotted line)
and the distance between the landing point and substrate limit of
the trace, we obtained the stiffness and the force–spectroscopic
height of the virions, respectively. Red and blue dotted lines indicate
indentation and retraction data, respectively, obtained in the 100th
nanomechanical cycle. (e) Force versus distance curves obtained during
repeated indentation of a single SARS-CoV-2 virion. (f) Matching force
versus distance curves obtained during retraction. In some traces,
force sawteeth (red trace) correspond to the unfolding of domains
in a surface protein, plausibly within the S trimer.To assess the thermal stability of SARS-CoV-2, we explored
the
topographical changes of virions exposed to high-temperature treatment
(Figure ). The sample
was exposed to temperatures of 60 (Figure a), 80 (Figure b), and 90 °C (Figure c) for 10 min then cooled to 20 °C for
AFM imaging. Remarkably, although virion density dropped from 22 (at
60 °C) to 18 virions/μm2 (at 90 °C), the
virus particles remained on the substrate surface and their global
appearance was only slightly altered. The mean peak height of the
viral particles increased slightly (83 ± 12, 88 ± 11, and
90 ± 9 nm at 60, 80, and 90 °C, respectively), and virion
topography became somewhat faceted, but the particles retained their
blurred, smooth surface. To test whether spikes were still present
following thermal exposure, we fixed the sample with 5% glutaraldehyde
(Figure d). Although
the rugged topography, seen in chemically fixed SARS-CoV-2 virions
(Figure c), was partially
restored, the spikes were much fewer and less distinct, and their
trigonal shape (Figure e) could not be resolved (Figure e), suggesting they became thermally denatured. Furthermore,
the smooth areas interspersed between rugged regions indicate that
thermal treatment resulted in a progressive dissociation of the S
trimers from the virion surface. Thus, the SARS-CoV-2 virion displays
an unexpected global thermal stability, which is likely related to
their aerosol and surface stabilities.[27] However, the conformational response of the spike proteins observed
here eventually leads to the heat-induced inactivation of SARS-CoV-2.
Figure 4
Effect
of temperature change on the topographical structure of
SARS-CoV-2. The sample was heated for 10 min at 60 (a), 80 (b), and
90 °C (c) then cooled back to 20 °C prior to AFM imaging.
The virions persist on the substrate surface with their global structure
nearly intact, but the topography becomes progressively more rugged,
pointing at the gradual disappearance of the dynamic surface smoothing
hence reduction of spike dynamics. (d) AFM image of an overview (1
× 1 μm) sample area following thermal treatment (90 °C
for 10 min) and glutaraldehyde (5%) fixation. Inset: Topographical
profile plot measured along the center of one of the virions (dotted
line). The rugged surface topography is partially restored, but large
areas on the virions are devoid of spikes. (e) High-resolution AFM
image of a heat-exposed (90 °C for 10 min) and fixed (5% glutaraldehyde)
SARS-CoV-2 virion. Shallow surface protrusions are present.
Effect
of temperature change on the topographical structure of
SARS-CoV-2. The sample was heated for 10 min at 60 (a), 80 (b), and
90 °C (c) then cooled back to 20 °C prior to AFM imaging.
The virions persist on the substrate surface with their global structure
nearly intact, but the topography becomes progressively more rugged,
pointing at the gradual disappearance of the dynamic surface smoothing
hence reduction of spike dynamics. (d) AFM image of an overview (1
× 1 μm) sample area following thermal treatment (90 °C
for 10 min) and glutaraldehyde (5%) fixation. Inset: Topographical
profile plot measured along the center of one of the virions (dotted
line). The rugged surface topography is partially restored, but large
areas on the virions are devoid of spikes. (e) High-resolution AFM
image of a heat-exposed (90 °C for 10 min) and fixed (5% glutaraldehyde)
SARS-CoV-2 virion. Shallow surface protrusions are present.In conclusion, the atomic force microscopic imaging
and nanomechanical
measurements revealed that the SARS-CoV-2 virion is highly dynamic,
compliant, and resilient, and it displays remarkable mechanical and
global thermal stabilities. While the dynamics of the surface spikes
may play an important role in the unusually high infectivity of the
virus, its mechanical and self-healing properties may also ensure
adaptation to a wide range of environmental circumstances. Considering
its capability of exploring viruses under native conditions, the single-particle
approaches[16] employed here may be important
in uncovering not only the mechanistic details behind viral infection
but also the viral response to potential therapies.
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