Hamid Hadi-Alijanvand1, Maryam Rouhani1. 1. Department of Biological Sciences, Institute for Advanced Studies in Basic Sciences (IASBS), Zanjan, 45137-66731, Iran.
Abstract
A highly infectious coronavirus, SARS-CoV-2, has spread in many countries. This virus recognizes its receptor, angiotensin-converting enzyme 2 (ACE2), using the receptor binding domain of its spike protein subunit S1. Many missense mutations are reported in various human populations for the ACE2 gene. In the current study, we predict the affinity of many ACE2 variants for binding to S1 protein using different computational approaches. The dissociation process of S1 from some variants of ACE2 is studied in the current work by molecular dynamics approaches. We study the relation between structural dynamics of ACE2 in closed and open states and its affinity for S1 protein of SARS-CoV-2.
A highly infectiouscoronavirus, SARS-CoV-2, has spread in many countries. This virus recognizes its receptor, angiotensin-converting enzyme 2 (ACE2), using the receptor binding domain of its spike protein subunit S1. Many missense mutations are reported in various human populations for the ACE2 gene. In the current study, we predict the affinity of many ACE2 variants for binding to S1 protein using different computational approaches. The dissociation process of S1 from some variants of ACE2 is studied in the current work by molecular dynamics approaches. We study the relation between structural dynamics of ACE2 in closed and open states and its affinity for S1 protein of SARS-CoV-2.
Since
the outbreak of coronavirus disease (COVID-19) in December
2019 in Wuhan, China, more than 210 countries have become involved.
This highly infectious disease is caused by a coronavirus named severe
acute respiratory syndrome coronavirus 2 (SARS-CoV-2) by the International
Committee on Taxonomy of Viruses (ICTV).Coronaviruses are enveloped
RNA viruses. They can cause respiratory,
enteric, and nervous system diseases in birds and mammals.[1] SARS-CoV-2 is a β-coronavirus. Among four
genera of coronaviruses, β-coronaviruses contain species that
have caused serious humanrespiratory tract infections: severe acute
respiratory syndrome (SARS) with outbreaks in 2002–2004 and
Middle East respiratory syndrome (MERS) with outbreaks from 2012,
which were about 10% and 36% lethal, respectively.[2]The main structural proteins of coronaviruses located
in the viral
envelope are membrane (M), envelope (E), and spike (S) proteins. The
S proteins form homo-trimers on the virus surface and are necessary
for entrance of the virus into the host cell. They determine the host
range and tissue tropism and induce host immune response. Each S glycoprotein
consists of the ectodomain, transmembrane, and intracellular regions.
The ectodomain consists of S1 and S2 subunits used for attachment
to receptor proteins and fusion with the membrane of host cells, respectively.
The S1 subunit of the spike protein is composed of a C-terminal domain
(CTD) and N-terminal domain (NTD). CTD, which is important in binding
of S proteins to protein receptors, is composed of a core region and
a receptor binding domain (RBD).[2]The spike protein of SARS-CoV-2 virus attaches to human angiotensin-converting
enzyme 2 (hACE2),[3−6] which is also the target of SARS coronavirus (SARS-CoV).[7−9] ACE2 is expressed in different organs of the body including lungs,
intestines, heart, kidneys, and endothelium.[10−13] This protein is a zinc peptidase
involved in converting angiotensin I to angiotensin 1-9,[14,15] and angiotensin II to angiotensin 1-7.[11]The ectodomain of ACE2 is composed of a collectrin homology
domain
and a peptidase domain more distant from the cell membrane. The peptidase
domain contains subdomains I and II that contain N-terminal and C-terminal
regions of the active site cleft, respectively.[16] Virus-binding motifs of hACE2 are recognized on the outer
N-terminal surface away from the catalytic cleft.[17] Similar to that observed for SARS-CoV,[17,18] the concave RBD of SARS-CoV-2 interacts with the convex N-terminal
helix of hACE2 mainly through polar interactions.[19−21]Changes
in coronavirusspike proteins could alter their corresponding
host.[22−26] In the same manner, the affinity between SARS-CoVspike protein
and ACE2 in the first step of viral attachment was a determining factor
in viral infectivity and host susceptibility and transmissions.[27−35] A few variations in critical ACE2 residues caused a lower affinity
of SARS-CoV virus to mouse, rat, and Daubenton’s bat ACE2 than
to humanACE2.[17,27,35,36] Variations in critical amino acids of mammalian
ACE2s were predicted to decrease or increase SARS-CoV-2 recognition.[37] Therefore, it is possible that mutations in
hACE2 affect the affinity and infection severity of SARS-CoV-2 in
human hosts.Iran is one of the countries infected pandemically
with the virus.
Iranian people show a variety of genetic backgrounds throughout the
country.[38] Beside global mutation databases
such as ENSEMBL,[39] Iranome is a database
that contains genetic information on different ethnic groups in Iran.[40] On the basis of Iranome data, the hACE2 gene
shows different mutations in different ethnic groups.To find
out whether the hACE2 missense mutations observed in human
populations affect the affinity of this protein to SARS-CoV-2 protein,
we created the three-dimensional (3D) structures of the mutated hACE2
proteins and computed the affinity of these proteins to the SARS-CoV-2spikeS1 protein. The interaction between S1 and its receptor in human
cells is one of the interesting targets for drug design to fight the
virus in the earliest stages. It is believed that blocking the virus–host
interaction at the molecular level opens new windows toward therapy.
In the current study, we considered the effect of the reported mutations
in ACE2 on its binding affinity for the S1 protein using some computational
approaches. We studied the dissociation of S1 RBD of SARS-CoV-2 from
the extracellular domain of different mutants of the hACE2 protein
in silico. The described dissociation process sheds light on the association
of the SARS-CoV-2S1 subunit with the ACE2 protein. We studied the
dynamics and stability of some ACE2 variants using molecular dynamics
approaches. The possible relation between ACE2 dynamics and its affinity
for SARS-CoV-2S1 subunit is discussed in the current study.
Methods
3D Structures
The 3D structure of
RBD of SARS-CoV-2spike subunit 1 complexed with its receptor, humanACE2, was retrieved from the Protein Data Bank (PDBID 6VW1).[19] The reported structure is chimeric. Its receptor binding
motif (RBM) that interacts with ACE2 belongs to the SARS-CoV-2 virus.
The 3D structures of humanACE2 mutants in association with spike
RBD are generated using the FoldX suite.[41] The FoldX suite is also utilized to compute the folding stability
of ACE2 along dissociation simulations. To simulate the dissociation
process of S1 from wild type (WT) ACE2 in its closed state, we utilized
ACE2 bonded to an ACE2-specefic inhibitor, ORE-1001 (PDBID 1R4L).[16] Then, we superimpose and align the ACE2 structure in the
closed state on wild-type ACE2 in association with S1 to find the
primary position of S1 in association with the closed state of ACE2.
Missense Mutations
The position of
missense mutations in the hACE2 gene is derived from ENSEMBL release
99, January 2020 with accession code ENST00000427411.1.[39] This list covers the reported mutations in hACE2
for various human populations with different geographical distributions.
Also, some missense mutations of ACE2 specific for Iranian ethnic
groups are derived from the Iranome project public data[40] and ENSEMBL database.[39]
Prediction of ACE2 Affinity to S1 Protein
Using Fast Methods
We predicted the affinity of the ACE2
mutants to the RBD of S1 by PISA,[42] FoldX,[43] Prodigy,[44] SEPAS,[45] and SAAMBE-3D.[46] We
fed the noted tools with complexes whose ACE2 subunits are mutated.
PISA-Based Prediction of Complex Stability
PISA assigns
the dissociation free energy (ΔGdiss) to the dimers using the following equation:[47]The solv, rot, and trans subscripts
stand for solvation, rotation, and transition, respectively. Number
(N) of hydrogen bonds (hb), salt bridges (sb), and
disulfide bonds (db) are also considered in the PISA computation.
Nonbonded interaction energy is presented by E. Δσ
stands for the buried surface area during complex formation. F and C are fitting constants. The hydration
energy and other contact-dependent energies are implemented in ΔGint as the binding energy of subunits. Rigid
body entropy (ΔS) is considered for rotation
(rot) and translation (trans) terms. We recruit the command line version
of PISA modules implemented in the CCP4 suite.[48] In the current study, the input structures for PISA to
predict the dissociation free energy of the complex are FoldX-generated
mutant 3D structures of ACE2 in association with the RBD of the S1
protein. If the deviation of PISA-computed stability of a mutant form
of ACE2/S1 complex from the stability computed for WT ACE2/S1 was
more than 0.1 kcal/mol, we considered the mutation as one that changed
the free energy of ACE2/S1 dissociation.
FoldX-Based
Prediction of Complex Stability
FoldX computes the stability
of protein complexes considering monomer
and dimer stabilities. The computed complex stability denotes the
intersubunit affinity. The stability of each monomer is computed by
using the empirical terms:[41]This equation is a linear
combination of various terms with specific coefficients. The van der
Waals (VDW) term’s contribution to total energy, solvation
of hydrophobic and polar groups, water bridges, hydrogen bonds, electrostatic
interactions, and electrostatic interactions’ contribution
to association constant are abbreviated to vdw, solvH, solvP, wb,
hbond, el, and kon in subscripts of stability terms, respectively.
The translational source of entropy, main-chain-, and side-chain-defined
entropies are abbreviated to tr, mc, and sc in subscripts of ΔS, respectively. We utilize the stand-alone academic version
of FoldX. The input structures of FoldX to predict the intersubunit
affinity are FoldX-generated mutant 3D structures of ACE2 in association
with the RBD of the S1 subunit. If the deviation of FoldX-computed
stability of a mutant form of ACE2/S1 complex from the stability computed
for WT ACE2/S1 was more than 0.1 kcal/mol, we considered the mutation
as one that changed the affinity of ACE2 for the S1 protein.
Prodigy-Based Prediction of ACE2 Affinity
for RBD of S1 Subunit
Prodigy utilizes inter-residue contacts
between subunits and the noninterface surface to predict the binding
affinity between subunits using the following equation:[44]ICs stands
for inter-residue
contacts, and the subscripts indicate the type of contact or type
of noninteraction surface (NIS). In the current study, we used the
stand-alone version of Prodigy.[49] The FoldX-generated
3D structures of ACE2 mutants in complex with S1 are the inputs of
Prodigy. If the deviation of Prodigy-computed affinity of a mutant
form of ACE2 to S1 from the affinity of WT ACE2 to S1 was more than
0.1 kcal/mol, we considered the mutation as one that changed the intersubunit
affinity.
SAAMBE3D-Based Prediction
of Complex Stability
SAAMBE was introduced to predict the
effect of mutations on dimer
stability. It considers MM/PBSA and knowledge-based descriptors such
as amino-acid-specific dielectric constants to perform its predictions.
SAAMBE-3D is the next generation of the mentioned method that uses
a machine learning approach to compute affinity changes resulting
from mutations using many knowledge-based properties of residues including
volume, hydrophobicity, flexibility, polarity, distance-based metrics,
and many other descriptors. We utilized the stand-alone version of
the mentioned software.[46] The FoldX-constructed
3D structures of ACE2 mutants in complex with RBD of S1 are the inputs
of SAAMBE-3D in the current study. On the basis of the software criteria,
the positive binding energy of a mutant means that such a mutation
weakens the binding free energy. If the amount of changes in binding
energy was more than 0.1 kcal/mol, we considered the mutation as one
that changed the intersubunit affinity.
SEPAS-Based
Prediction of Complex Stability
The mentioned methods all
require the 3D structure of the protein
complex to predict affinity or changes in affinity between subunits.
SEPAS utilizes the 3D structure of one monomer to perform affinity
prediction using the mechanical softness of the protein binding patch
(PBP). It requires the 3D structure of a PBP region on one monomer
to predict the affinity between the introduced PBP and tentative partners
of the PBP. It predicts the softness of PBP using the following equation:[45,50]N represents
the count of residues in PBP, and Nn represents
number of unique intra-PBP native contacts. The cutoff distance for
defining the native contact is set at 7.5 Å. To create ensembles
of near-equilibrium structures for all 240 mutants of ACE2 reported
in ENSEMBL and Iranome that are considered in current study, we utilize
the anisotropic network model (ANM) of the complexes.[51,52] The ANM approach provides a pool of 1000 structures for each of
240 mutants of ACE2 bonded to the S1 protein. The SEPAS-assigned affinity
of ACE2 for S1 is the average of predicted affinities of 1000 samples
generated by ANM for each mutant structure. Mainly, SEPAS predicts
the stability in a classwise manner. It predicts four possibilities
for each PBP, i.e., how much the introduced PBP belongs to high-affinity,
high-medium, medium-low, and low-affinity classes. If a mutation in
ACE2 leads to a 5% or more change in distribution of the computed
possibilities among denoted classes with respect to WT, we count the
mutation as an effective one.
Adaptive
Tempering MD and MM-GBSA Approach
Free energy of ACE2 binding
to RBD of SARS-CoV-2spike protein
1 is also estimated in the current work by using MM-GBSA approach
for mutations in ACE2 that are reported for Iranian ethnic groups
by NAMD 2.13.[53,54] To perform MM-GBSA, we gradually
heat up the complex structures to 300 K in Generalized Born implicit
solvent (GBIS) after minimization steps. The ion concentration is
set at 0.3 molar. The hydrophobic energy contribution from implicit
solvent is considered in simulations. We use adaptive tempering molecular
dynamics simulation (AT-MD) to enhance the system sampling.[55] The adaptive tempering is a single copy version
of replica exchange MD. In the current work, we let the langevin thermostat
use the updated temperatures from adaptive tempering for 2 ×
106 steps. The resulted ensemble of structures was also
used to study the properties of SARS-CoV-2 RBD/ACE2 complex for WT
and ACE2 mutants. To estimate the binding energy using MM-GBSA, we
utilized the single-trajectory approach[56] by considering the next equation:We used run-time-analysis
feature of NAMD 2.13 to compute potential energy and its constituent
terms in GBIS condition for all frames of protein complex (ΔG(ACE2/S1)), separated S1 subunit (ΔG(S1)), and separated ACE2 (ΔG(ACE2)). The run-time analysis is performed for 1000 snapshots
derived from 2 × 106 steps of AT-MD simulation for
WT and mutant complexes. The presented MM-GBSA-predicted affinities
of ACE2 for S1 are the average values of the ensemble data.
Adaptive Biasing Force Approach
To
simulate the binding of SARS-CoV-2S1 protein to humanACE2 and to
predict the binding free energy with higher accuracy, we utilized
adaptive biasing force (ABF) for complexes between RBD of SARS-CoV-2S1 protein and reported mutants of ACE2.[57,58] In ABF, we gradually dissociated monomers of the complexes along
the z-axis of the complexes in a 4–18.5 ns
simulation under GBIS conditions using collective variable features
of NAMD 2.13. ABF is a history-dependent approach to compute free
energy profiles along predefined collective variables. During simulation
steps, the free energy surface is smoothed by the adaptive bias so
the system behaves along the defined collective variable, the z-axis of the bonded subunits, like when it is able to perform
diffusion there. In the current study, the bin size was set to 0.2
Å. We tested 0.2, 0.4, and 2 ps as the simulation time before
applying the biasing force by ABF in each bin. Because the standard
error of the computed forces and the computed potentials are not so
small in long than in short bin-scanning and systems experience some
binding/unbinding during some of simulations, here we set 0.2 ps as
the simulation time before applying the biasing force by the ABF algorithm
in each bine. We are interested in comparative rather than quantitative
affinities. The ABF simulation time varies from 4 to 18.5 ns depending
on the considered system. The total time of ABF simulations in the
current study reached 248 ns. The maximum standard error (SE) of the
ABF-computed free energy between two adjacent positions on the reaction
coordinate (points c and b) are computed by the following equation:[59,60]The variance of the ABF force
is defined by σ2; N denotes number
of points that are sampled to compute PMF; and κ presents the
correlation length of the calculated force. We compute the SEs for
ABF simulations in two scenarios: time-based and distance-based. For
computing the time-based SE, we split the ABF simulations into windows
with 20 ps length. Each window has a 0.2 ps overlap with its previous
window. For computing the distance-based SE, we split the distance
between two subunits into windows with 0.5 Å length. This covers
2.5 bins of the original ABF simulations.
Characterizing
Partially Melted Structures
The AT-MD-reported potential
energies are used to measure the progression
of systems along a partial unfolding path. The state that resides
in the most negative potential well is considered as the most stable
species. The reported potential energy and their corresponding temperature
are used to define the temperature of microtransition and the energy
barrier between folded and partially melted states of the protein
using the following equation:[55]P stands
for the normalized computed potential energy where 1 means folded
state and 0 represents melted state, w adjusts the
reported fraction of the melted state, T stands for
the transition temperature, β denotes the reduced dimension
of simulation temperature, and ΔE represents
the energy difference between folded and partially melted states.
We use Cα-based inter-residue distance root mean
square (dRMS) deviation as a structural descriptor of the folded state.[61,62]
Miscellaneous
Some structural features
like computation of dipole, salt-bridges, H-bonds, and ASA properties
were computed by house-made Tcl codes run under VMD 1.9.2.[63] All MD-based computations such as pair interaction
calculations, adaptive tempering, MM/GBSA, ABF, and other runtime
analyses were performed by using NAMD 2.13. The utilized force fields
for proteins are CHARMM 22 and 27.[64] In
all simulations, the time steps are set at 2 fs. The force filed parameter
for the drug molecule is utilized from SwissParam.[65] Prody is recruited to perform ANM and PRS computations.[52] The electrostatic potential surface for the
complexes was computed by PMEPOT plugin of VMD 1.9.2.
Results and Discussion
There are reports indicating
that SARS-CoV-2 utilizes ACE2 as its
receptor for attaching to human cells.[4,7] ACE2 is expressed
in a wide range of tissues such as heart, lungs, and intestines.[13] It is indicated that SARS-CoV-2 binds to its
receptor via the S1 subunit of its surface spike complex.[20] The affinity of S1 for its receptor affects
the virulence, its hosts, and the intensity of virus infection.[9] It is observed that in some populations the incidence
of COVID-19 is not similar between members. Beside variables such
as age, sex, and sanitary conditions, the effects of genetic variations
are not ignorable.[66,67] The consequence of some mutations
in ACE2 in its interaction with SARS-CoV or SARS-CoV-2 spikes was
studied by genetic approaches.[67,68] The effects of some
ACE2 mutations that reside in interface region of SARS-CoV-2spike/ACE2
complex were studied by bioinformatics tools.[69,70] Studies suggested that ACE2 mutants possibly related to COVID-19
incidence.[71] Here, we studied the effect
of ACE2 gene polymorphisms on its stability, dynamics, and binding
affinity for the S1 protein of SARS-CoV-2 using multiple computational
approaches. In the current study, we predict the effect of 240 widespread
missense mutations in the ACE2 gene reported for different human populations
and especially eight ones specific for Iranian ethnic populations
on the binding affinity between ACE2 and S1 RBD of SARS-CoV-2 with
different computational approaches from bioinformatic methods to a
thermodynamic integration procedure.There are many reported
SNPs for the ACE2 gene in different human
populations in the ENSEMBL database. We selected the missense SNPs
in the humanACE2 extracellular domain. Recently, the 3D structure
of RBD of the SARS-CoV-2S1 protein in association with ACE2 was reported.[19] Using the crystallized 3D structure, we introduced
the ENSEMBL-reported missense mutations in the ACE2 subunit of the
assembly utilizing the FoldX suite.[41] The
constructed mutated ACE2 subunits in association with S1 created the
building blocks for the next steps in the current study.
Predicting the Affinity of ACE2 Mutants to
SARS-CoV-2 S1 Protein Using Fast Methods
In this section,
we predicted the effect of the detected mutations in ACE2 on the affinity
of ACE2 variants to S1 by using different computational methods. There
are many bioinformatic methods to predict the stability of the protein
complex and the affinity between subunits by using various approaches.
We utilized PISA,[42] FoldX,[43] Prodigy,[44] SEPAS,[45] and SAAMBE-3D[46] for
predicting the intersubunit affinity of the ACE2/S1 complexes using
their 3D structures.In one category of structure-based affinity
predictors, the utilized algorithm considers all parts of the interested
3D structure to predict the stability of protein complexes using the
thermodynamic formulation of protein folding. PISA and FoldX are verified
examples of the mentioned class of affinity predictors. In brief,
PISA is an acceptable method to predict the biounit assembly of PDB-submitted
structures by using an empirical energy function that considers the
interaction energy and implicit representation of complex dissociation
entropy to compute dissociation free energy of the complex. FoldX
is a successful method in predicting the effect of mutations on protein
complex stability. It performs the computations using semiempirical
energy function that considers the stability of the monomers and the
complex to predict complex stability.Besides the introduced
thermodynamic-based methods, some other
structure-based methods use different structural aspects of the complex
or interface region to predict intersubunit affinity. Prodigy, SEPAS,
and SAMMB3D are examples of evaluated methods for this class of affinity/stability
predictors. Prodigy is a successful method for predicting the experimentally
measured binding affinities of protein subunits by counting the intersubunit
contacts. SEPAS is a monomer-based predictor of binding affinity of
protein binding patches to tentative partners that computes the mechanical
stiffness of the proposed interface region. SAMMBE3D is a feature-based
new generation of a trained version of adjusted GB/MM that is a predictor
of the effect of mutations on dimer stability.We report the
predicted affinities of 240 mutated versions of ACE2
to S1 of SARS-CoV-2 using the mentioned fast structure-based computational
methods in Figure . About 4.5% of the considered mutations reside in the ACE2–S1
interface region. Mutations in ACE2 that cause the ACE2/S1 complexes
become more stable than wild type ACE2/S1 complex are red, whereas
mutations that destabilize the ACE2/S1 complex are blue in Figure . If a method does
not predict a considerable difference between the affinities of mutated
and WT ACE2 for S1, the method is colored yellow for the considered
mutation in Figure . The criteria for assigning different mutations outcomes are presented
in methods sections –2.3.5. For three cases, three
methods out of five predictors predict that the related mutations
stabilize ACE2/S1 complex, and for two cases, 3/5 of the predictors
expect the mutations destabilize the complex between ACE2 and S1.
These methods are fast and utilize different approaches to perform
the prediction.
Figure 1
Predicted affinity of the mutant ACE2 for the S1 protein
is presented.
The position of each ENSEMBL-reported SNPs for ACE2 protein is presented
in the first row. The mutated residue and its corresponding WT residue
are presented in third and second rows, respectively. Rows four to
eight represent the effect of the ACE2 mutation on the stability of
the ACE2/S1 complex predicted by different predictors. If a mutation
is predicted as a stabilizer one, it is red, if the mutation leads
to a more unstable complex than WT ACE2/S1 complex, it is blue, and
if no change is predicted for stability, the color is yellow.
Predicted affinity of the mutant ACE2 for the S1 protein
is presented.
The position of each ENSEMBL-reported SNPs for ACE2 protein is presented
in the first row. The mutated residue and its corresponding WT residue
are presented in third and second rows, respectively. Rows four to
eight represent the effect of the ACE2 mutation on the stability of
the ACE2/S1 complex predicted by different predictors. If a mutation
is predicted as a stabilizer one, it is red, if the mutation leads
to a more unstable complex than WT ACE2/S1 complex, it is blue, and
if no change is predicted for stability, the color is yellow.As the recruited fast methods in this section consider
different
structural aspects of protein complexes, the observed inconsistency
in prediction seems natural. The utilized thermodynamic approaches
are sensitive to the quality of the interested 3D structure. However,
some of the other structure-based methods perform predictions by just
utilizing general structural features that show less sensitivity to
the global quality of the structure. The utilized methods in the presented
part consider the static structure of the ACE2/S1 complex for predicting
changes in affinity. Here, to alleviate this issue, we feed the SEPAS
algorithm with ANM-generated ensembles of structures for predicting
the affinity of each ACE2 mutant to the SARS-COV-2S1 protein. The
ANM-defined ensemble of structures lets us consider the effect of
mutations on all regions of ACE2 better than using a single snapshot
of the mutant structure.Another possible source of the variation
between the prediction
results of thermodynamic-based and other descriptor-based affinity
predictors is the interface issue. The correct 3D structure of the
interface region is more important for the methods that are trained
for the interface structural properties. Because the interface region
between ACE2 variants and the RBD of S1 is derived by superimposing
ACE2 of the WT complex and mutant ACE2, this approach possibly misses
structural changes in the interface region resulting from mutations
especially for mutations that do not occur at the interface region.
Besides, we set restrict criteria to accept the influence of mutations
on changes in the affinity between subunits. As the mentioned methods
have different intrinsic errors, we assume if the difference between
the predicted affinity of WT subunits and mutant ones is larger than
0.1 kcal/mol then it is a meaningful change in the affinity. If we
accept a large difference in the predicted affinities between mutants
and WT complexes, the amount of inconsistency will be decreased.Despite the contrary results of the mentioned methods in predicting
the effect of ACE2 mutations on their affinity for S1, the results
indicate that those mutations may change the affinity of ACE2 to S1.
It is a considerable result because if such predictions would be verified
by other methods, it may mean the populations have different intrinsic
susceptibility to COVID-19.
Adaptive Tempering Generated
Ensembles, MM/GBSA
Approach, and Dynamic Properties of ACE2/S1 Complexes
The
utilized bioinformatic methods in previous section are fast with acceptable
accuracy for prediction of the affinity between subunits but we need
more accurate methods to predict the effect of ACE2 mutations on its
affinity for S1 protein of SARS-CoV-2 that consider the dynamic features
of protein structures. Because molecular dynamics (MD)-based approaches
to compute the binding affinities are time-consuming, we decide to
limit the target population for studying the consequence of ACE2 mutations
on its affinity for S1 protein and computing the effects of mutations
on complex dynamics by MD-based approaches.We utilized MD-based
approaches to predict the affinity between ACE2 and the S1 protein
of SARS-CoV-2 for the mutations in the ACE2 gene that are reported
in the Iranome database for ethnic groups of the Iranian population
as SNPs.[40] We selected eight missense mutations
of ACE2 from the Iranome project whose positions are available in
the crystallized structure of WT ACE2. Four out of the eight SNPs
are also reported in ENSEMBL for other populations (Table ).
Table 1
Properties
of ACE2 Mutations in Iranian
Ethnic Groups Are Presenteda
dbSNP accession code
Iranian ethnic group
Polyphen2
Mutation Assessor Pred
MM/GBSA-based affinity (kcal/mol)
WT
–62 (9)
D225G
just in Iranome
Azeri
probably damaging
functional
–69 (8)
D494V
rs765152220
Persian Gulf
Islander
probably damaging
functional
–61 (7)
F452V
just in Iranome
Turkmen
probably
damaging
functional
–61 (8)
Q60R
rs759162332
Azeri
benign
nonfunctional
–63 (7)
Y199C
rs750145841
Turkmen
probably damaging
functional
–63 (7)
S331F
just in Iranome
Turkmen
probably damaging
functional
–62
(8)
T334M
just in Iranome
Azeri + Turkmen
benign
functional
–57 (8)
V485L
just in Iranome
Persian Gulf Islander
possibly damaging
functional
–63 (9)
Ethnic group, the predicted severity
of the mutation, predicted functionality, and predicted affinity of
the ACE2 variant to the S1 protein are presented in columns 2–5,
respectively. The standard deviations of the predicted affinities
are reported as parenthesized numbers in the last column. If the predicted
affinity for a mutant in comparison to the WT shows a significant
difference (p < 0.05), its value is in bold in
the last column.
Ethnic group, the predicted severity
of the mutation, predicted functionality, and predicted affinity of
the ACE2 variant to the S1 protein are presented in columns 2–5,
respectively. The standard deviations of the predicted affinities
are reported as parenthesized numbers in the last column. If the predicted
affinity for a mutant in comparison to the WT shows a significant
difference (p < 0.05), its value is in bold in
the last column.We used
MM/GBSA and adaptive biasing force (ABF), a thermodynamic
integration method, to compute the free energy of S1 binding to ACE2
for ACE2 mutants that are reported in Iranian ethnic groups.The FoldX-generated 3D structures of ACE2 mutants in association
with S1 were minimized and heated up gradually. To increase the sampling
efficiency, we used an accelerated method, adaptive tempering (AT-MD),
instead of common MD. AT-MD is a single copy version of the replica
exchange method that finds structures with minimum energy faster than
simple MD does.[55] After 2 × 106 steps of AT-MD simulation, we utilized a single-trajectory-based
version of MM/GBSA[54,56] to make the first MD-based estimation
of binding energy between varieties of ACE2 and the S1 protein of
SARS-CoV-2 (Table ). As it is indicated in Table , for example, some members of the Azeri ethnic group
that carry the DA225G mutation in their ACE2 have higher MM/GBSA-predicted
affinity for the S1 protein of SARS-CoV-2 than members with WT ACE2
do. It may suggest that the carriers of the noted mutation may be
predisposed to infection with the virus because their ACE2 protein
shows high affinity for binding to the S1 protein.The AT-MD-generated
ensembles of the complexes provide us with
rich pools of structures to study the structural properties of the
ACE2/S1 complexes in the bonded state. AT-MD lets the ACE2/S1 complex
sample the energy landscape with high efficiency. We report the AT-MD
potential of the system, a measure of the ACE2 subunit structural
stability in the presence of the S1 protein, as a function of the
MM/GBSA-predicted affinity of ACE2 for S1 in 2D density plots (Figure S1).We are interested to compute
the structural stability of ACE2 mutants
when they are in association with the RBD of the S1 protein. We propose
the changes in structural stability of ACE2 will affect its binding
site for S1. The structural stability of ACE2 mutants is much more
informative when mutations reside in regions far from the binding
site of the S1 protein.In the utilized AT-MD, the ground state
energy of the system is
tuned in a history-dependent manner to pass some energy barriers ahead
of the system in its energy landscape by thermostat-directed boosts.
Because we do not want to unfold the subunits completely, we set the
acceptable range of temperature between 300 and 320 K. In this range
of temperature, all atoms RMSD of the considered structures are smaller
than 5 Å. We detect faint two-state transitions in AT-MD simulations
of the complexes (see Methods). The microtransition
occurs in the WT complex or complexes of considered mutants within
the temperature range of 308–309 K. The observed transitions
are detected by considering the potential energies of complexes as
a function of the simulation temperature. The transition energy between
the folded state of the ACE2/S1 complexes and the locally melted state
of the complexes are reported in Figure . We decomposed the amount of complex partial
melting by computing the dRMS metric for ACE2 and RBD subunits during
AT-MD simulation for pretransition population, i.e., populated stable
species (Figure S2). To find which subunit
of the considered dimer is affected more by temperature, we calculated
the difference of dRMS between ACE2 and S1 in each simulation frame
as ΔdRMS. Defining the ΔdRMS metric let us determine which
subunit is affected more during AT-MD simulations. The 2D density
plots of AT-MD potential energy as a function of ΔdRMS for WT
ACE2 and mutant ACE2s in association with S1 are presented in Figure S3. We map 2D density plots presented in Figure S1 on their corresponding plots in Figure S3. It helps us to determine the ΔdRMS
value that corresponds to the highly populated stable complex that
has been used for determining the MM/GBSA-based affinity for the desired
subunit pair. The obtained ΔdRMS values define the relative
order of the ACE2 subunit structural stability when it is bonded to
the S1 subunit. The summary of the procedure and the obtained relative
order of ACE2 subunit structural stability are presented in Figure . These results indicate
that some mutations stabilize ACE2 monomer and some decrease the structural
stability of ACE2. In one subpopulation of Y199C mutant of ACE2, the
structural stability of ACE2 is decreased, whereas the affinity of
ACE2 for the S1 subunit is increased in that population. The ACE2
structural stability is decreased in Q60R mutation but its MM/GBSA-based
affinity for S1 does not change significantly. As the studied mutations
of ACE2 are far from the interface region, they modulate the affinity
between ACE2 and S1 using long-range allosteric mechanisms. Although
some of the mutations make ACE2 unstable in comparison to WT, they
prepare the binding site region for making a stable complex with the
SARS-CoV-2S1 protein. These observations mean it is not necessary
for an affinity modulator mutation to appear in the interface region
of the complex for exerting its effect. In next steps, we follow how
the considered mutations in ACE2 change its affinity to S1 over a
distance.
Figure 2
Different states of the ACE2/S1 complex observed in AT-MD and the
structural stabilities of ACE2 subunits of the stable complexes are
described. The ACE2/S1 complexes show two populations in AT-MD simulations.
The stable population, pretransition, transits to an unstable population
after passing some barriers. The lower panel represents the ΔE for complexes with mutant ACE2 between the two faint states
of complexes by fitting the computed data to the two-state model of
protein transition (eq ). In the scheme that represents two-state transition, the x-axis represents 1/(kT) and the amount
of melted structure is decreasing, while the metric presented in the
vertical axis is close to 1. The shared highly populated states in Figures S1 and S3 show distinct amounts of ΔdRMS.
We sort ACE2 subunits on the basis of the amount of ΔdRMS of
their corresponding stable complexes (upper panel). The bold values
of predicted affinities are meaningful at the p <
0.05 level for the t test compared to the affinity
of WT assembly.
Different states of the ACE2/S1 complex observed in AT-MD and the
structural stabilities of ACE2 subunits of the stable complexes are
described. The ACE2/S1 complexes show two populations in AT-MD simulations.
The stable population, pretransition, transits to an unstable population
after passing some barriers. The lower panel represents the ΔE for complexes with mutant ACE2 between the two faint states
of complexes by fitting the computed data to the two-state model of
protein transition (eq ). In the scheme that represents two-state transition, the x-axis represents 1/(kT) and the amount
of melted structure is decreasing, while the metric presented in the
vertical axis is close to 1. The shared highly populated states in Figures S1 and S3 show distinct amounts of ΔdRMS.
We sort ACE2 subunits on the basis of the amount of ΔdRMS of
their corresponding stable complexes (upper panel). The bold values
of predicted affinities are meaningful at the p <
0.05 level for the t test compared to the affinity
of WT assembly.Considering variations of ACE2
and S1 protein electrostatic potential
(EP) as averaged isopotential surfaces, we find that the large negative
electrostatic potential of ACE2 makes the protein an interesting target
for proteins with a positive accessible electrostatic potential like
S1. The mutations in ACE2 affect the size and integrity of the negative
EP in mutant versus WT ACE2 (Figure S4).
The changes in EP for mutations at positions 225 and 452 are considerable.
These mutations increase the affinity of ACE2 to S1 on the basis of
MM/GBSA-based-predicted affinities (Table ).The 3D structure of ACE2 indicates
that there is a long groove
in its structure. The noted groove is possibly developed for substrate
binding. The active site of the enzyme also resides in one side of
the groove. The accessibility of the groove to solvent is restricted
by two regions assumed as “Gate”. The halves of the
gate are interconnected in one side via a disordered region labeled
as the “Zip” region (Figure ). We study the dynamics of ACE2 mutants
and WT structures during AT-MD simulations by measuring the Euclidian
distance between the halves of the gate region and the length of the
zip structure. As indicated in Figure , the dynamics of the Gate and Zip regions are different
between wild type ACE2 and the mutants of ACE2 in their S1-bonded
states. A mutation at the position 452 causes an increment of ACE2
affinity to S1 and simultaneously closes the Gate region. Also, the
Zip segment becomes shorter there. The gate is more opened in the
T334M mutant of ACE2 in comparison to the WT subunit, whereas the
affinity of this mutant of ACE2 for the S1 protein is decreased. It
seems that the closed/open state of the ACE2 changes its affinity
for the S1 protein of SARS-CoV-2. This observation and the mentioned
hint may be an opportunity for drug discovery and finding a possible
therapy against COVID-19.
Figure 3
Dynamics of the ACE2 groove region is measured
for AT-MD-generated
ensembles of ACE2/S1 complexes. Left panel depicts the schematic position
of the Gate and Zip regions in the ACE2 structure. The length of the
zip region and the distance between halves of the gate region are
presented in middle and right panels, respectively, for different
ACE2 variants in association with the S1 protein. The horizontal axes
represent length in angstroms, and the vertical axes present population
density.
Dynamics of the ACE2 groove region is measured
for AT-MD-generated
ensembles of ACE2/S1 complexes. Left panel depicts the schematic position
of the Gate and Zip regions in the ACE2 structure. The length of the
zip region and the distance between halves of the gate region are
presented in middle and right panels, respectively, for different
ACE2 variants in association with the S1 protein. The horizontal axes
represent length in angstroms, and the vertical axes present population
density.The perturbation-response scanning
(PRS) approach provides the
possibility to mechanically perturb specific residues and then predict
its effects on the dynamics of other regions of the protein.[72,73] Because we believe that the considered mutations of ACE2 for Iranian
ethnic groups exert their effects on the binding affinity between
ACE2 and S1 over a distance, we recruit the PRS approach for ACE2/S1
complexes that contain the WT or a mutated version of ACE2.Anisotropic network model (ANM) is a coarse-grained description
of a protein in which the nonbonding interactions between residues
are represented by linear-elastic springs. This model lets us evaluate
the effects of an external-force-driven mechanical perturbation of
one node, residue, on other nodes of the network and vice versa. Here,
we perturb all residues and measure the sensitivity of the mutation
positions to the perturbation using the PRS method. It means how much
the mutated ACE2 residues sense the overall mechanical perturbation
in an ACE2/S1 complex.The presented amounts of the residue
sensitivity in vertical axis
of graphs in Figure indicate that the sensitivity of S1 in S1/ACE2 complex is high in
response to ACE2 perturbations. It means that S1 is affected by ACE2
dynamics more than the amount ACE2 is influenced by the S1 perturbation.
Figure 4
Average
sensitivity of residues or the sensitivity of a specific
residue to the perturbation of other residues is presented. In the
“All” panel, the average sensitivity of all protein
residues to the physical perturbation is presented. In other panels,
the sensitivity of a specific residue (panel name) to the perturbation
of other residues of the complex is presented. The positions of interfacial
residues are presented as black bars parallel to the x-axis of the “All” panel. Here, chain A represents
the ACE2 subunit, and chain E denotes the S1 subunit. The surface
representation of ACE2/S1 assembly in panel “225” is
colored in the following manner: the ACE2 chain is blue; the S1 subunit
is red; distal residues of S1 are depicted by a gray surface; and
S1 residues that reside in the interface region of S1 and ACE2 are
shown as a yellow surface.
Average
sensitivity of residues or the sensitivity of a specific
residue to the perturbation of other residues is presented. In the
“All” panel, the average sensitivity of all protein
residues to the physical perturbation is presented. In other panels,
the sensitivity of a specific residue (panel name) to the perturbation
of other residues of the complex is presented. The positions of interfacial
residues are presented as black bars parallel to the x-axis of the “All” panel. Here, chain A represents
the ACE2 subunit, and chain E denotes the S1 subunit. The surface
representation of ACE2/S1 assembly in panel “225” is
colored in the following manner: the ACE2 chain is blue; the S1 subunit
is red; distal residues of S1 are depicted by a gray surface; and
S1 residues that reside in the interface region of S1 and ACE2 are
shown as a yellow surface.The average sensitivity profile of each residue of the complex
in response to perturbation of other residues of the complex is presented
in panel “All” in Figure . Peaks in Figure indicate which residues are strongly coupled with
the sensor, mutated, residues. As it is presented in panel “All”
of Figure , some of
the S1 distal residues (resid: 334, 360–369, 388, 427–430,
518) are highly coupled with the other residues in the complex. This
region of S1 is close to recently discovered allosteric modulator
region of the S1 protein.[74] Residues at
positions 225, 452, and 485 of ACE2 protein are highly coupled with
the distal residues of the S1 protein dynamically. Therefore, the
mentioned positions of ACE2 play a critical role in information transfer
between ACE2 and S1 subunits of the complex. Position 60 of ACE2 shows
an odd pattern; this node has no significant coupling with other residues
of the complex. Among the ACE2 residue positions that we studied,
corresponding to the mutated residues in Iranian ethnic groups, just
positions 199 and 225, are strongly coupled with residues of the S1
subunit that are in contact with the ACE2 subunit; so, their perturbations
may affect the assembly more than other positions. This analysis indicates
that position 199 in ACE2 is also coupled with some residues of ACE2;
therefore, a mutation in that position possibly affects the ACE2 structure
and the ACE2/S1 interface simultaneously. Position 225 is just sensitive
to the signal arrived from the S1 contact site with the ACE2 subunit.
This observation may rationalize the higher affinity of ACE2 to S1
resulting from the D225G mutation in ACE2. In brief, perturbations
in positions 225, 452, and 485 of ACE2 in complex with S1 provoke
a high amount of perturbation in S1; this perturbation response is
especially observed for position 225 that is coupled with the interface region
of S1. Perturbations in some positions such as 199 induce dynamic
changes in both partners of the complex. The PRS-predicted dynamics
changes in the interface region of S1 and ACE2 may be another justification
for different affinities of ACE2 mutants to S1 of SARS-CoV-2.
Dissociation Process of ACE2/S1 Complexes
The structural
aspects of the complex derived from AT-MD simulations
and MM/GBSA-based predicted affinity of WT and mutant ACE2s for S1
provide us with some information about the possible mechanisms behind
the changes in the affinity of ACE2 to S1. We utilize another MD-based
method to improve the accuracy of the predicted affinity of ACE2 for
S1 protein and to simultaneously study the dynamics of the partners
during the dissociation/association process. Using the adaptive biasing
force (ABF) method,[57] we derive the potential
of mean force (PMF) for dissociation of S1 from ACE2 in complexes
that contain the WT or a mutant version of ACE2. Before performing
ABF simulations, the WT and mutant ACE2 monomers in association with
S1 protein pass 2 × 106 steps in AT-MD. Next, the
S1 subunit is dissociated from ACE2 slowly along the z-axis of the complex (Supplementary Movie). Considering the standard errors of the ABF-computed dissociation
free energies (Figure S5), we find that
the ABF-computed affinities between S1 and ACE2 are increased in many
of ACE2 mutations in Iranian ethnic groups in comparison to WT ACE2
(Figure ). It means
that for those mutations we need higher forces to dissociate the S1
subunit from the mutant ACE2 structures than for WT ACE2. Among the
considered mutations, the V485L mutant shows a lower affinity for
binding to the SARS-CoV-2S1 protein than WT shows. It may provide
an intrinsic resistance against COVID-19 to its carriers.
Figure 5
ABF-computed
dissociation free energies are presented. The relative
free energy of dissociation of S1 from ACE2, which is computed by
the ABF approach, is presented for different variants of ACE2 in Iranian
ethnic groups. The computed free energy is reported as a relative
value compared with the computed affinity for WT complex, 48 kcal/mol.
The horizontal axis represents the relative distance between S1 and
ACE2. A higher value in the x-axis denotes a higher
distance between two subunits of ACE2/S1 complex along the axis interconnecting
two subunits. Zero in the x-axis represents the bound
state, and 1 represents the state in which S1 is dissociated from
ACE2 completely.
ABF-computed
dissociation free energies are presented. The relative
free energy of dissociation of S1 from ACE2, which is computed by
the ABF approach, is presented for different variants of ACE2 in Iranian
ethnic groups. The computed free energy is reported as a relative
value compared with the computed affinity for WT complex, 48 kcal/mol.
The horizontal axis represents the relative distance between S1 and
ACE2. A higher value in the x-axis denotes a higher
distance between two subunits of ACE2/S1 complex along the axis interconnecting
two subunits. Zero in the x-axis represents the bound
state, and 1 represents the state in which S1 is dissociated from
ACE2 completely.The presented results
in section suggest
that the dynamics of the gate/zip
regions of ACE2 possibly affects the affinity of ACE2 for S1. To study
the effect of the ACE2 closed state on its affinity for S1, we perform
ABF simulations also for ACE2 bonded to the ORE-1001 ligand as an
investigational drug that converts the open state of ACE2 to its closed
state. Studies suggested that during binding of substrate/inhibitor
to the ACE2 groove it transits to the closed state.[16] Our computations indicate that the affinity between S1
protein of SARS-CoV-2 and ACE2 in the ORE-1001-induced closed state
is higher than that in the open conformation (Figure ). We should note that the drug also changes
the dynamics of dissociation process; therefore, we would not extrapolate
the same conclusion for all closed states of ACE2.Nowadays,
there are many reports about the effects of high blood
pressure (HBP) suppressor drugs, ACEi/ARBs, on the incidence of COVID-19.
There are some contradictory results in such reports about the effect
of such drugs on predisposition to COVID-19.[75,76] Many of the HPB suppressors affect ACE2 gene expression in a tissue-specific
manner.[77−79] To the best of our knowledge, no experimental result
has been published about the effect of ACE2-specific drugs on the
affinity of ACE2 for S1 of SARS-CoV-2. Some studies reported the effect
of binding of some molecules to ACE2 in the closed conformation on
the affinity of ACE2 for the SARS spike.[80,81] They proposed such drug–ACE2 interactions may decrease ACE2
affinity for the SARS spike. They also postulated the critical role
of the closed, substrate-bonded state of ACE2 in its binding to SARS
or the COVID-19 virusspike protein. Recently, researchers reported
that the activity of ACE2 increased up to 10 fold by binding to RBD
of the SARS-CoV-2S1 protein.[82] The authors
of the mentioned paper suggested that the RBD of the SARS-CoV-2S1
protein binds to the closed state of ACE2. We report the dynamics
of Gate and Zip regions of ACE2 for some ACE2 mutations (Figure ). Our computations
suggest that the closed and open states of ACE2 show a different affinity
for the RBD of the SARS-CoV-2S1 protein (Figure ). When ACE2 binds to ORE-1001, an ACE2-selective
inhibitor, it transits to the closed state. In that state, ACE2 shows
a higher affinity for the SARS-CoV-2S1 protein than in the open state.
These observations suggest that ACE2 possibly fluctuates between closed
and open states and the RBD of the SARS-COV-2S1 protein has a higher
affinity toward the closed population of the ACE2 protein. Therefore,
it may mean that if some compounds induce the closed state in ACE2,
S1 may bind to ACE2 with higher affinity.The dissociation of
S1 from ACE2 in ABF simulation sets indicates
that the diverse ACE2 mutants dissociate from S1 differently. In some
cases, aromatic–aromatic contacts between the partners are
disrupted quickly (mutations at 331, 199, 452, and 485; Figure S6). Considering the salt bridges between
the subunits of ACE2/S1 complexes, we find that the bridge between
residues 31 and 484 of ACE2 and S1, respectively (bridge 31–484)
and the bridge between residue 329 of ACE2 and residue 439 of S1 (bridge
329–439) are two common bridges in ACE2/S1 assembly (Figure ), which were described
in the crystal structure and simulations.[19,83] The second salt bridge was introduced unnaturally to stabilize the
complex during crystallization steps. The structural changes resulted
from the F452V and S331V mutations in the ACE2 force ACE2 to create
a new short-life salt bridge between residue 23 of ACE2 and 458 of
S1 (bridge 23–458). The intersubunit salt bridges and aromatic–aromatic
contacts indicate that the disruption of the 329–439 bridge
is concomitant with tearing aromatic contacts between S1 and ACE2.
It suggests that the bridge acts as a lock for disruption of intersubunit
hydrophobic contacts.
Figure 6
Intersubunit salt bridges along ABF simulations are presented.
Three types of salt bridges detected between the S1 protein and different
variants of ACE2. The X-axis represents the normalized
simulation time along ABF simulations. Zero in the x-axis represents the bound state, and 1 represents the state in which
S1 is dissociated from ACE2 completely. The vertical axis represents
the total number of inter-residue contacts if the involved residues
are closer than 4 Å.
Intersubunit salt bridges along ABF simulations are presented.
Three types of salt bridges detected between the S1 protein and different
variants of ACE2. The X-axis represents the normalized
simulation time along ABF simulations. Zero in the x-axis represents the bound state, and 1 represents the state in which
S1 is dissociated from ACE2 completely. The vertical axis represents
the total number of inter-residue contacts if the involved residues
are closer than 4 Å.In ABF-derived results, we considered the effect of eight mutations
of ACE2 observed in Iranian ethnic groups on the ACE2 affinity for
the S1 protein of SARS-CoV-2. We measured the distances between positions
of the eight mutated residues in ACE2 structures and the interface
region of ACE2 along dissociation simulations (Figure S7). These eight mutations are distributed in different
regions of ACE2, and their distances from the interface region vary
in different mutations. It means that not only the structure of the
interface region is affected during dissociation process but also
other regions of ACE2 that are far from the interface are also affected.
These observations suggest that the integrity of the ACE2 structure
in different mutants control the amount of forces required for dissociating
S1 from ACE2. Changes in the integrity of mutants and WT ACE2 structures
during the dissociation process of S1 are dynamic. To depict them,
we follow all salt bridges that appear in ACE2 subunits of the complexes
during the dissociation of S1 from ACE2. Then, we detect similar salt
bridges, with the same donor and acceptor of the bridge, in different
varieties of ACE2 along ABF simulations. We compute the similarity
between ACE2 varieties on the basis of the appearance of the same
salt bridges along ABF experiments (Figure ). For example, the salt bridges that appear
in the Q60RACE2 mutant are unique ones and show a low similarity
to salt bridges of other ACE2 mutants in the S1/ACE2 dissociation
experiment.
Figure 7
Diversity of salt bridges appearing in the ACE2 subunit during
ABF simulations is compared among variants of ACE2. The unique intra-ACE2
salt bridges are detected during ABF simulations. The color represents
how many of salt bridges in the ACE2 subunit are similar between different
types of ACE2 along simulation time. 0–10%: light-gray, 10–20%:
gray, 20–30%: dark blue, 30–40%: light blue, 40–50%:
orange, 50–60%: red.
Diversity of salt bridges appearing in the ACE2 subunit during
ABF simulations is compared among variants of ACE2. The unique intra-ACE2
salt bridges are detected during ABF simulations. The color represents
how many of salt bridges in the ACE2 subunit are similar between different
types of ACE2 along simulation time. 0–10%: light-gray, 10–20%:
gray, 20–30%: dark blue, 30–40%: light blue, 40–50%:
orange, 50–60%: red.Studying the changes in VDW and electrostatic terms of interaction
energy between S1 and ACE2 along the dissociation process indicates
that the electrostatic portion of the interaction energy between subunits
is lower for the V485L mutant than for WT (Figure
S8). This is a mutation with the lowest ABF-computed affinity
for S1 in the current study. On the other hand, for the most stable
ACE2/S1 complex in the current study, the F452VACE2 mutant, the VDW
interaction energy diminishes quickly.On the basis of our studies
on the process of S1 dissociation from
ACE2, we might divide the receptor binding motif (RBM) of the S1 protein
into two distinct sections “Fist” and “Forearm”.
These parts have different affinities to the ACE2. The ratio of hydrophobic
(or polar) contacts between fist and ACE2 and hydrophobic (or polar)
contacts between forehand and ACE2 is computed along dissociation
of S1 from ACE2 (Figure ). We find that the ratios change differentially among ACE2 mutants
along dissociation steps. The ratios indicate that the first segment
of S1 that dissociates from ACE2 is forehand, and in final steps,
when S1 protein struggles to dissociate completely from ACE2, the
fist segment (residues 470–490 in the S1 protein) will be detached
from ACE2. If we suppose in ideal state that the dissociation process
is similar to the association process but in reverse direction, we
may conclude that in the first stages of its binding, the S1 protein
docks its fist section into ACE2. This step lets the RBD of S1 find
the appropriate region on ACE2 for its complete binding via the forehand
segment.
Figure 8
Superiority of different parts of the S1 subunit in interaction
with ACE2 is traced along the dissociation simulations. The proposed
segments of the RBD of the S1 protein in the current work are depicted
in the right panel. The normalized number of contacts between hydrophobic
residues of ACE2 and the fist region of S1 divided by the sum of hydrophobic
contacts between ACE2 and fist and forearm regions of S1 is represented
as blue lines. Red lines represent polar contacts between ACE2 and
S1 segments. The vertical axis represents the normalized number of
contacts. The X-axes represent the normalized time
along dissociation experiments in ABF simulations. The contact criterion
is set at <10 Å for the interatom distance.
Superiority of different parts of the S1 subunit in interaction
with ACE2 is traced along the dissociation simulations. The proposed
segments of the RBD of the S1 protein in the current work are depicted
in the right panel. The normalized number of contacts between hydrophobic
residues of ACE2 and the fist region of S1 divided by the sum of hydrophobic
contacts between ACE2 and fist and forearm regions of S1 is represented
as blue lines. Red lines represent polar contacts between ACE2 and
S1 segments. The vertical axis represents the normalized number of
contacts. The X-axes represent the normalized time
along dissociation experiments in ABF simulations. The contact criterion
is set at <10 Å for the interatom distance.The dynamics of the denoted segments of S1 is affected by
dynamic
changes of intra-ACE2 interactions which may be translated as changes
in ACE2 stability along the dissociation process. Considering the
changes in folding stability of ACE2 subunit during the dissociation
of S1 from ACE2, we find that the structure of ACE2 becomes more stable
in some mutants (Figure ). The increased stability of ACE2 in the F452V mutant even causes
a resistance against dissociation of S1 from ACE2. The FoldX-defined
folding stability analysis also indicates that the electrostatic portion
of ACE2 stability is decreased in most ACE2 mutants. It possibly indicates
that the electrostatic interactions in the considered mutants are
not in the optimal state.
Figure 9
Folding stability of the ACE2 subunit of the
complex is computed
along the dissociation process. While the S1 subunit is slowly dissociated
from the ACE2 subunit, the stability of ACE2 is computed for every
frame of the ABF simulation (middle panel) by the FoldX approach.
Left and right panels represent the density plots for the amount of
electrostatic and vdw terms of the stability function for variants
of ACE2, respectively. Error bars represent the standard error of
computed values. For each variant, 100 samples are picked from AT-MDs
to evaluate the stability.
Folding stability of the ACE2 subunit of the
complex is computed
along the dissociation process. While the S1 subunit is slowly dissociated
from the ACE2 subunit, the stability of ACE2 is computed for every
frame of the ABF simulation (middle panel) by the FoldX approach.
Left and right panels represent the density plots for the amount of
electrostatic and vdw terms of the stability function for variants
of ACE2, respectively. Error bars represent the standard error of
computed values. For each variant, 100 samples are picked from AT-MDs
to evaluate the stability.
Conclusion
In the current study, we report the effect of ACE2 polymorphism
on its binding affinity for the S1 protein of SARS-CoV-2, especially
for the reported mutations in ACE2 of Iranian ethnic groups as mutations
that reside far from the S1 binding site. The dynamics and stability
of the ACE2 mutants are studied in our work. We demonstrate that the
considered mutations affect the affinity between ACE2 and S1 via long-range
mechanisms. Many of the considered mutations in the current study
enhance the affinity of ACE2 to S1 of SARS-CoV-2, and it may suggest
possible intrinsic susceptibility of carriers of such mutations to
COVID-19. On the other hand, we find one of ACE2 mutants has a lower
affinity for the S1 protein of SARS-CoV-2 than WT does, which possibly
suggests a type of immunity for its carriers. Our computations suggest
that the affinity of ACE2 for S1 in its closed state may be greater
than that in the open state of ACE2. We report the relation between
dynamics of ACE2 structure and its affinity to the S1 protein of SARS-CoV-2.
This information may be informative to design compounds that modulate
ACE2 dynamics and consequently decrease its affinity for the SARS-CoV-2S1 protein.
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