Rohith R Mohan1, Gary A Huber2, Dimitrios Morikis1. 1. Department of Bioengineering, University of California , Riverside, California 92521, United States. 2. Department of Chemistry and Biochemistry, University of California , San Diego, California 92093, United States.
Abstract
Electrostatic effects are ubiquitous in protein interactions and are found to be pervasive in the complement system as well. The interaction between complement fragment C3d and complement receptor 2 (CR2) has evolved to become a link between innate and adaptive immunity. Electrostatic interactions have been suggested to be the driving factor for the association of the C3d:CR2 complex. In this study, we investigate the effects of ionic strength and mutagenesis on the association of C3d:CR2 through Brownian dynamics simulations. We demonstrate that the formation of the C3d:CR2 complex is ionic strength-dependent, suggesting the presence of long-range electrostatic steering that accelerates the complex formation. Electrostatic steering occurs through the interaction of an acidic surface patch in C3d and the positively charged CR2 and is supported by the effects of mutations within the acidic patch of C3d that slow or diminish association. Our data are in agreement with previous experimental mutagenesis and binding studies and computational studies. Although the C3d acidic patch may be locally destabilizing because of unfavorable Coulombic interactions of like charges, it contributes to the acceleration of association. Therefore, acceleration of function through electrostatic steering takes precedence to stability. The site of interaction between C3d and CR2 has been the target for delivery of CR2-bound nanoparticle, antibody, and small molecule biomarkers, as well as potential therapeutics. A detailed knowledge of the physicochemical basis of C3d:CR2 association may be necessary to accelerate biomarker and drug discovery efforts.
Electrostatic effects are ubiquitous in protein interactions and are found to be pervasive in the complement system as well. The interaction between complement fragment C3d and complement receptor 2 (CR2) has evolved to become a link between innate and adaptive immunity. Electrostatic interactions have been suggested to be the driving factor for the association of the C3d:CR2 complex. In this study, we investigate the effects of ionic strength and mutagenesis on the association of C3d:CR2 through Brownian dynamics simulations. We demonstrate that the formation of the C3d:CR2 complex is ionic strength-dependent, suggesting the presence of long-range electrostatic steering that accelerates the complex formation. Electrostatic steering occurs through the interaction of an acidic surface patch in C3d and the positively charged CR2 and is supported by the effects of mutations within the acidic patch of C3d that slow or diminish association. Our data are in agreement with previous experimental mutagenesis and binding studies and computational studies. Although the C3d acidic patch may be locally destabilizing because of unfavorable Coulombic interactions of like charges, it contributes to the acceleration of association. Therefore, acceleration of function through electrostatic steering takes precedence to stability. The site of interaction between C3d and CR2 has been the target for delivery of CR2-bound nanoparticle, antibody, and small molecule biomarkers, as well as potential therapeutics. A detailed knowledge of the physicochemical basis of C3d:CR2 association may be necessary to accelerate biomarker and drug discovery efforts.
Electrostatics plays an important role
in accelerating biomolecular
reactions, such as diffusional encounters and catalytic processes.[1−5] Both long-range and short-range electrostatic interactions have
been shown to affect the protein–protein association rate[6−8] and have demonstrated important contributions to improving the efficiency
of enzymatic reactions, often by several orders of magnitude.[9,10] An area of research that has received significant attention in recent
computational studies is the role of electrostatics in the function
and regulation of the complement system, as well as the electrostatic
mechanisms that bacterial and viral proteins have evolved to infiltrate
host cells or evade the immune system.[11−20]The complement system is a vital component of innate immunity,
acting as a rapid-response surveillance system that identifies and
eliminates, or contributes to the elimination of foreign pathogens
through the processes of inflammation, opsonization, phagocytosis,
and direct cell lysis.[21] In addition, the
complement system contributes to clearance of apoptotic cells, damaged
cells and cellular debris, and immune complexes.[22−26] The complement system is tightly regulated to discriminate
self-from nonself,[27] and when such regulation
fails, the complement system contributes to autoimmune and inflammatory
diseases.[28−30] Overall, the complement system senses and responds
to danger signals, contributing to host homeostasis.[23,25]A direct result of complement activation is the role it plays
as
a link between innate and adaptive immunity, through the interaction
between complement fragment C3d and complement receptor 2 (CR2). This
is a property of mammals and higher species, because invertebrates
have complement immune response but lack adaptive immunity. The formation
of the C3d:CR2 complex contributes to the formation of the B cell
receptor–coreceptor complex and to the enhancement of B cell-mediated
antibody production by up to 3–4 orders of magnitude.[31−33] Due to the importance of the C3d:CR2 complex to the development
of autoantibodies, the C3d:CR2 interaction is also implicated in the
pathology of autoimmune and inflammatory diseases. Thus, a comprehensive
understanding of the nature of the C3d:CR2 interaction not only will
contribute to mechanistic knowledge of a fundamental immune response
process, but also can serve as the basis for improvements in therapeutic
development.Complement activation occurs through three different
pathways:
the classical, alternative, and lectin pathways. All three pathways
converge at complement component C3.[34] Complement
C3 undergoes a series of cleavage steps that activate, inactivate,
and redirect its activation. The first cleavage step produces the
opsonin fragment C3b that covalently (through a thioester bond) attaches
to pathogens and other surfaces, tagging them for recognition and
elimination by phagocytic cells, and the fragment C3a that contributes
to inflammatory response and phagocytosis. The second cleavage step
produces the so-called inactivated C3b, iC3b, which also contributes
to phagocytosis. The final cleavage steps produce C3c and C3dg, which
is immediately transformed to C3d. Although C3d is the final cleavage
product that remains on cell surfaces for the life of the cell, it
is not just a degradation product. Nature has evolved mechanisms that
utilize antigen-bound C3d and B cell expressed CR2 as a site of interaction
between innate and adaptive immunity. B cell expressed antibodies
also opsonize pathogens by binding to antigens on pathogen surfaces.
Thus, the combined function of B cell bound antibodies and the CR2-C3d
complex cross-link B cells to pathogens, forming the so-called B cell
receptor (antibody)–coreceptor (CR2) complex. This cross-linking
initiates a cascade of intracellular signaling reactions, involving
protein kinases.Several structural and computational studies
have proposed that
the interaction between C3d and CR2 is predominantly electrostatic
in nature,[35−39] occurring through a negatively charged patch on a concave surface
of C3d and the first two modules of CR2 that are positively charged
(Figure ). Experimental
studies involving mutagenesis, pH, and ionic strength effects are
in agreement with the dominant role of electrostatics in the association
between C3d and CR2.[35,36,40−42] Although there was ambiguity and controversy for
several years because of an older nonphysiological crystallographic
structure of the C3d:CR2 complex, this controversy is now resolved
with new crystallographic, mutagenesis and binding, and computational
data.[19,36,41,43] A recent study has evaluated the physicochemical
origins and strength of the C3d:CR2 interaction, using the physiological
and the controversial crystallographic structures, and has demonstrated
the electrostatic mechanism of binding.[19] This and earlier studies[37−39] have proposed a two-step model
for C3d:CR2 association, consisting of recognition and binding for
highly and oppositely charged proteins. This model was based on earlier
work on electrostatic steering in enzymatic reactions and protein
interactions by McCammon and co-workers.[1−10,44−46] During the
recognition step, long-range electrostatic interactions between protein
macrodipoles accelerate the formation of a transient encounter complex,
followed by the binding step, which is marked by the stabilization
of the bound complex through short-range, pairwise polar and nonpolar
interactions and entropic effects.
Figure 1
Electrostatic potentials mapped onto the
protein surfaces of C3d
and CR2 in open book representation. Electrostatic potentials were
calculated at ionic strength corresponding to 150 mM monovalent counterion
concentration. The color transitions from red to white to blue represent
electrostatic potential values of −5 kT/e to 0 kT/e to 5 kT/e.
Electrostatic potentials mapped onto the
protein surfaces of C3d
and CR2 in open book representation. Electrostatic potentials were
calculated at ionic strength corresponding to 150 mM monovalent counterion
concentration. The color transitions from red to white to blue represent
electrostatic potential values of −5 kT/e to 0 kT/e to 5 kT/e.Another recent study used the
concept of “electrostatic
hotspots” to evaluate the origin of the C3d–CR2 interaction
throughout evolution.[47] An “electrostatic
hotspot” was defined as a surface patch of like-charged residues
that is resistant to perturbation. Such hotspots contribute to the
formation of the encounter complex and rapid association. Because
of the high concentration of like charges, a hotspot forms an unfavorable
electrostatic environment, which is amenable to the formation of favorable
interactions with proteins that have areas with complementary charges
when such an encounter occurs. The study was performed using C3d sequences
from 24 species, homology modeling based on the most recent (physiological)
crystallographic structure, perturbations based on alanine scan of
ionizable residues and molecular dynamics simulations, Poisson–Boltzmann
electrostatic calculations, and electrostatic potential similarity
clustering. The study proposed that C3d has two “electrostatic
hotspots” located at opposite faces; one hotspot is predominantly
positively charged and contains the thioester bond that opsonizes
pathogen surfaces, and the other hotspot is predominantly negatively
charged and forms the concave surface that is the site of interaction
with CR2. The study concluded that the appearance of the negatively
charged hotspot coincides with the onset of adaptive immunity at the
level of jawless fish and beyond, and it is stronger in mammals, but
it is not present in invertebrates. Therefore, C3d evolved its electrostatic
properties to acquire the negatively charged hotspot to interact with
the positively charged CR2, resulting to enhancement of adaptive immunity.Given the large number of background studies on the electrostatic
character of the C3d-CR2 interaction, and that the formation of the
encounter complex is a diffusion-limited process,[48] we initiated a Brownian dynamics (BD) simulation study
to evaluate kon reaction rate constants
for C3d:CR2 complexes. We perform our study for native C3d and CR2,
as well as for a number of mutants with available experimental binding
data. We evaluate the ionic strength dependence of the C3d:CR2 interaction
to investigate the impact of salt concentration on electrostatic screening.
We utilize computational mutagenesis to elucidate the contributions
of specific mutants, with known experimental binding data, to the
association of the C3d:CR2 complex. We demonstrate the inverse relationship
between the association rate constant and ionic strength.We also find
that mutations of residues shown to enhance or hinder binding in experimental
binding data[35,40,41] result in slower or higher association rate constants, respectively.
The examined mutations involved ionizable residues at the binding
interface and were introduced to disrupt association. Our results
are in agreement with the experimental data, as well as with a previous
computational study,[19] and they indicate
that the electrostatic steering accelerates the interaction between
C3d and CR2.
Methods
Protein Structure Preparation
We utilized the more
recent crystallographic structure of the C3d:CR2 complex (Protein
Data Bank, PDB, code: 3OED)[36] in our study. From the
three-dimensional coordinates of this structure, we used chains A
and C, corresponding to C3d and CR2, respectively, as they had better
electron density and lower B-factor compared to chains B and D of
another complex present in the structure. It should be noted that
the structure of CR2 contains only the two modules that contact C3d,
SCR1, and SCR2, out of a total of 15 or 16 SCR modules. C3d consists
of 292 amino acids with a net charge of −1e while CR2 consists of 130 amino acids with a net charge of +8e. To alleviate crystal packing effects in the crystallographic
structure, 25 000 steps of conjugate-gradient energy minimization
were performed using NAMD.[49]Subsequent
to energy minimization, missing hydrogens, atomic radii, and partial
charges were added to the coordinates of the structure, using PDB2PQR
version 2.0[50] and the PARSE force field,[51] thus converting the PDB file to a PQR file.
No atypical protonation states were observed using PROPKA.[52,53] Histidine residues were neutral with a hydrogen attached to Nδ1 atom. Computational mutagenesis was performed on the
protein complex using the analysis of electrostatic similarities of
proteins (AESOP) computational framework.[15,39,54,55] Mutants were
chosen from prior literature that had reported experimental binding
data.[35,40,41] Electrostatic
potentials were calculated for the parent (wild-type) and mutated
protein complexes using the Adaptive Poisson–Boltzmann Solver
(APBS) version 1.4.[56] The number of grid
points was set to 129 × 161 × 161. Coarse and fine mesh
dimensions were set to 1000 Å × 1000 Å × 1000
and 150 Å × 150 Å × 150 Å, respectively,
as discussed previously.[54] Protein and
solvent dielectric values were set to 20 and 78.54, respectively.[54] Ionic strengths corresponding to monovalent
counterion concentrations of 50, 75, 100, 125, 150, 200, and 300 mM
were used for the evaluation of ionic strength dependence of parent
C3d:CR2 and the alanine scan mutants. An ionic concentration of 150
mM was used in the electrostatic analysis of the alanine scan mutants.
Brownian Dynamics Simulations
Brownian dynamics simulations
and the corresponding rate calculations were performed using the BrownDye
package,[57] according to the Northrup–Allison–McCammon
algorithm,[44] which is based on the original
Brownian dynamics algorithm by Ermak and McCammon.[58] The two molecules start separated at a center-to-center
radius (represented by the inner circle in Figure A), and the simulation progresses until termination
due to formation of the encounter complex or due to the molecule reaching
an escape radius (represented by the outer circle in Figure A). The center-to-center radius
is calculated by BrownDye for each system, and through an improvement
to the Northrup–Allison–McCammon algorithm, the escape
radius is no longer a necessary input.[59] Pairwise residue interactions with cutoff distances of 5.0 Å
were calculated from the PQR files generated as described above. Criteria
for a successful reaction required that at least two of the atom pairs
from the calculated list of pairwise interactions approach within
3.495 Å of each other (Figure B).
Figure 2
Schematic and molecular graphics illustrating the Brownian
dynamics
(BD) simulation of C3d:CR2 and the corresponding reaction criteria
with C3d and CR2 in blue and red, respectively. (A) At the beginning
of the BD simulation, CR2 starts at a center-to-center radius away
from C3d, as represented by the inner circle. The simulation terminates
when either the formation of the encounter complex occurs or if CR2
reaches an escape radius as represented by the outer circle. (B) The
concentric circles represent the reaction criteria for the C3d:CR2
BD simulations where 5 Å is the cutoff for determining potential
pairwise residue interactions between C3d and CR2. The circle with
radius 3.495 Å represents the distance within which at least
two atom pairs of the previously determined pairwise residue interactions
must occur for a successful reaction.
Schematic and molecular graphics illustrating the Brownian
dynamics
(BD) simulation of C3d:CR2 and the corresponding reaction criteria
with C3d and CR2 in blue and red, respectively. (A) At the beginning
of the BD simulation, CR2 starts at a center-to-center radius away
from C3d, as represented by the inner circle. The simulation terminates
when either the formation of the encounter complex occurs or if CR2
reaches an escape radius as represented by the outer circle. (B) The
concentric circles represent the reaction criteria for the C3d:CR2
BD simulations where 5 Å is the cutoff for determining potential
pairwise residue interactions between C3d and CR2. The circle with
radius 3.495 Å represents the distance within which at least
two atom pairs of the previously determined pairwise residue interactions
must occur for a successful reaction.Reaction criteria were selected to match known rate constants
of
C3d:CR2 association. Initially, the BrownDye program rates_of_distances
was utilized to generate a list of reaction constants corresponding
to minimum reaction distances. Then, the criteria were fine-tuned
to the known association rate constant at 125 mM NaCl from experimental
data.[40] There are two experimental association
rate constants, at 50 and 125 mM NaCl ionic strength, and we chose
for calibration the value at 125 mM because of its proximity to the
physiological ionic strength of 150 mM. Additional input files were
generated using the program bd_top. BD simulations were carried out
using the weighted-ensemble method to account for low probabilities
of reactions.[60] The association rate constant, kon, and corresponding reaction probabilities
were calculated using weighted-ensemble simulations carried out for
2 000 000 steps with 200 copies of each system to guarantee
convergence of the results. The acceleration of protein–protein
association, as well as enzymatic reactions, by electrostatic steering
has been explored previously, which suggested the feasibility of this
study.[61,62]
Results and Discussion
Ionic
Strength Dependence of Association
The weighted-ensemble
BD simulations of C3d:CR2 demonstrate that under constraints of reaction
criteria of 3.495 Å and at least two successful pairwise interactions,
the association rate constant decreases with increasing ionic strength
(Figure ), which is
expected when ionic screening of Coulombic interactions is present.
The experimental data utilized for calibration of the reaction criteria
is plotted in Figure as well. Additionally, Figure shows the ionic strength dependence of the Debye length,
suggesting the importance of ionic screening for association. Both
the ionic strength dependence and Debye length curves follow similar
trends.
Figure 3
Association rate constant of CR2 binding to C3d and the calculated
Debye length at varying ionic strengths. The mean association rate
constant is represented by a green circle with 95% confidence intervals
represented as error bars. The Debye length at each ionic strength
is represented as a purple square. Experimentally known association
rate constants at two ionic strengths, 50 mM and 125 mM NaCl, are
plotted and represented as orange triangles.[40] Note: the experimental data point at 125 mM was utilized for calibration
of the BD simulation reaction criteria.
Association rate constant of CR2 binding to C3d and the calculated
Debye length at varying ionic strengths. The mean association rate
constant is represented by a green circle with 95% confidence intervals
represented as error bars. The Debye length at each ionic strength
is represented as a purple square. Experimentally known association
rate constants at two ionic strengths, 50 mM and 125 mM NaCl, are
plotted and represented as orange triangles.[40] Note: the experimental data point at 125 mM was utilized for calibration
of the BD simulation reaction criteria.Because C3d and CR2 have surfaces that are both highly and
oppositely
charged (Figure ),
we expect that association follows the two-step model of recognition
(formation of the intermediate encounter complex) and binding (formation
of the final bound complex). This is demonstrated by the ionic strength
dependence of the association, which is possible if electrostatics
drives association. From our results, the acceleration of the interaction
through electrostatic steering underscores the plausibility of the
model. The kinetic rate constants acquired through these BD simulations
reflect the recognition step, given the calculation limitation, such
as the rigid body assumption of the protein structures and lack of
modeling of short-range interactions such as salt bridges, van der
Waals forces, and hydrogen bonding.[63] These
limitations may affect only the binding step of the aforementioned
two-step model of protein–protein association and may not be
necessary for the evaluation of electrostatic steering during the
diffusion-limited recognition step.[64]
Impact of Specific Residues on Electrostatic Steering
We
investigated the effects of electrostatic steering when various
C3d:CR2 residues are mutated. Computational mutations were chosen
from available experimental data and BD simulations were performed
for each mutant system. We observe that mutations of certain residues
result in a decrease in the association rate constant, or in other
words, the residue is significant to the formation of the encounter
complex of C3d:CR2 (Figure A,B). The reverse holds true as well where mutations of residues
resulting in an increase in the association rate constant signify
that the residue hinders the formation of the encounter complex. These
results are in line with a previous computational alanine scan and
electrostatic analysis study using AESOP[19] with a few small discrepancies such as K251A on C3d and R83A on
CR2, which are close to the threshold of the error. Thus, we establish
that the acceleration of the formation of the encounter complex due
to electrostatic steering is affected by individual charged residues
contributions as well.
Figure 4
Effects of mutagenesis on association rate constant and
ionic strength
dependence. (A, B) The mean association rate at 150 mM ionic strength
is plotted for each mutant for C3d and CR2 with 95% confidence intervals
represented as error bars. The shaded region represents the upper
and lower bound threshold of the association rate constant values
of the parent (C3d or CR2). Computational mutations were performed
based on previous experimentally generated mutants.[35,40,41] (C, D) Ionic strength dependence of selected
mutants demonstrating significant deviations from the wild type association
rate constant. The mutant notation denotes the residue number surrounded
by the replaced residue on the left and the replacing residue on the
right.
Effects of mutagenesis on association rate constant and
ionic strength
dependence. (A, B) The mean association rate at 150 mM ionic strength
is plotted for each mutant for C3d and CR2 with 95% confidence intervals
represented as error bars. The shaded region represents the upper
and lower bound threshold of the association rate constant values
of the parent (C3d or CR2). Computational mutations were performed
based on previous experimentally generated mutants.[35,40,41] (C, D) Ionic strength dependence of selected
mutants demonstrating significant deviations from the wild type association
rate constant. The mutant notation denotes the residue number surrounded
by the replaced residue on the left and the replacing residue on the
right.Mutants displaying significant
variance from the wild-type (outside
the shaded area of Figure A,B) were selected for ionic strength dependence analysis
(Figure C,D). We find
that the mutants exhibit ionic strength dependence as well, and the
trends are overall in line with what we would expect from the mutagenesis
analysis of Figure A,B. As expected from the mutagenesis analysis, certain mutants demonstrate
more drastic electrostatic steering, suggesting that they play a more
significant role in the formation of the encounter complex.
Comparison
with Prior Experimental and Computational Studies
A recent
computational study investigating the binding mode of
C3d:CR2 using molecular dynamics (MD) simulations (both explicit-solvent
and steered), including MM-GBSA analysis, and electrostatic calculations,
including AESOP alanine scan analysis, quantifies why the acidic patch
on C3d plays a key role in driving the C3d:CR2 interaction.[19] In particular, two clusters of C3d residues
(D36, E37, and E39; E160, K162, D163, E166, and E167) demonstrate
significant contributions to electrostatic interactions, intermolecular
interaction occupancies (hydrogen bonds, salt bridges, and nonpolar
interactions) and steered MD (SMD) simulations. The computational
study also emphasizes the importance of both the SCR1 and SCR2 domain
to the stability and energetics of the complex. This is supported
by the electrostatic and MD simulation analysis and also was strongly
suggested by the slow unbinding of the SCR1 domain in SMD simulations,
in contrast to the SCR2 domain.Our results are generally in
agreement with prior experimental and computational data. C3d residues
at the acidic patch such as D36, E37, and E39 (Figure ) were suggested to be important to binding
by a 2000 rosette immunological assay study[35] and a 2010 surface plasmon resonance study,[41] in addition to the AESOP analysis.[19] Our
BD results support the importance of D36, E37, and E39 in binding
as well. C3d residues E117, D122, D128, and D147, a cluster of residues
not located at the acidic patch, demonstrated minimal contributions
to electrostatic steering, in contrast to a mutagenesis study[40] performed by authors of the older crystallographic
C3d:CR2 structure.[65] This is in line with
the previous computational study[19] and
the 2000 and 2010 mutagenesis studies.[35,41]
Figure 5
Molecular graphic
of C3d:CR2 in open-book form and locations of
residues with significant contributions to electrostatic steering.
The surfaces of C3d and CR2 are rendered translucent and colored from
red to white to blue according to electrostatic potential values (calculated
at 150 mM ionic strength) from −5 kT/e to 0 kT/e to 5 kT/e.
Residues are displayed in ball-and-stick form with atoms colored according
to atom type (carbon in gray, oxygen in red, nitrogen in blue). Residues
found to demonstrate significant contributions to electrostatic steering
(falling outside the shaded area in Figure A,B) in this ionic strength dependence analysis
and significant contributions to electrostatic interactions (greater
or less than ±2.5 kJ/mol) in a previous AESOP computational alanine
scan study[19] are labeled with a solid black
box. Residues found to demonstrate significant contributions to electrostatic
steering in this ionic strength dependence analysis but less significant
interactions (within ±2.5 kJ/mol) in the AESOP computational
alanine scan study are labeled with a dashed black box. Additional
residues found to have significant contributions to electrostatic
interactions in the AESOP computational alanine scan study are labeled
without a box.
Molecular graphic
of C3d:CR2 in open-book form and locations of
residues with significant contributions to electrostatic steering.
The surfaces of C3d and CR2 are rendered translucent and colored from
red to white to blue according to electrostatic potential values (calculated
at 150 mM ionic strength) from −5 kT/e to 0 kT/e to 5 kT/e.
Residues are displayed in ball-and-stick form with atoms colored according
to atom type (carbon in gray, oxygen in red, nitrogen in blue). Residues
found to demonstrate significant contributions to electrostatic steering
(falling outside the shaded area in Figure A,B) in this ionic strength dependence analysis
and significant contributions to electrostatic interactions (greater
or less than ±2.5 kJ/mol) in a previous AESOP computational alanine
scan study[19] are labeled with a solid black
box. Residues found to demonstrate significant contributions to electrostatic
steering in this ionic strength dependence analysis but less significant
interactions (within ±2.5 kJ/mol) in the AESOP computational
alanine scan study are labeled with a dashed black box. Additional
residues found to have significant contributions to electrostatic
interactions in the AESOP computational alanine scan study are labeled
without a box.C3d residues at the other
acidic patch cluster (E160, D163, and
E166) demonstrated significant contributions to electrostatic steering,
in line with the previous computational study,[19] but are at odds with the 2000 mutagenesis study. However,
the influence of electrostatic steering of C3d residues K162 and E167
are in contrast to the previous computational study[19] and 2000 mutagenesis study.[35] Here, we found that removal of K162, which is located within the
acidic patch of C3d, did not affect the electrostatic steering of
the formation of the encounter complex as dramatically as it was suggested
by the results of the 2000 rosette study[35] and the previous AESOP study.[19] It is
likely that the role of K162 is to stabilize the negative surface
patch, and its removal produces local structural rearrangements to
optimize the remaining electrostatic interactions. Such structural
effects are not taken into account by the rigid model BD and AESOP
studies. We should keep in mind that the BD and AESOP analyses introduce
theoretical perturbation to assess the importance of each mutated
residue in binding of the parent proteins, and they do not aim to
model the structures of the mutated proteins.The importance
of the SCR1 domain of CR2, which was overlooked
by the original C3d:CR2 crystallographic structure, is further emphasized
in our BD results, as evidenced by the effects of mutagenesis and
electrostatic steering by CR2 residues R13, R36, and K41. This is
in line with the previous computational study where it was established
that the contributions of the SCR1 domain to the C3d:CR2 interface
are significant.[19]
Pharmacological Significance
Understanding the physicochemical
origins of the C3d:CR2 interaction is important for the design of
biomarkers and therapeutic interventions. Recent studies have utilized
information from the C3d–CR2 interaction to design C3d-binding
biomarkers for imaging of complement activation, such as fluorescently
labeled antibodies,[66] small fluorescent
molecules,[67] and CR2-bound iron nanoparticles.[68]The complement system has been a target
of inhibition in several studies, but only two anticomplement drugs
are currently in the clinic.[69] Although,
a lack of proper regulation of complement response has been implicated
in several autoimmune and inflammatory diseases, inhibiting complement
activation may reduce the efficacy of response to infection and injury.
Recent studies have demonstrated in animal models effective targeted
delivery of CR2-attached protein complement inhibitors, through the
CR2:C3d interaction, to sites of local inflammation, which are abundant
of C3d-opsonized tissues.[70−75] Such inhibitors included fragments of the alternative pathway regulator
Factor H, or the complement inhibitory protein Crry, but can also
be low-affinity C3d-bound or CR2-bound peptidic or nonpeptidic molecules.
Therefore, the C3d:CR2 interaction is an ideal target for therapeutic
development because it allows for inhibition of complement response
through the alternative pathway while retaining the ability to fight
infection through the lectin and classical pathways. The C3d:CR2 interaction
can also be a target for therapeutic intervention in cases of autoimmunity
because it allows for inhibition of complement-enhanced adaptive immune
response, through the inhibition of the formation of the B cell receptor–coreceptor
complex.
Conclusion
We have investigated
the role of electrostatic steering on the
C3d:CR2 interaction, using BD simulations. We demonstrate that the
predicted kon reaction rate constant depends
on ionic strength, which is possible only if electrostatics contributes
significantly to the C3d:CR2 interaction. We have also evaluated the
contributions of specific ionizable residues to the electrostatic
acceleration of the interaction through computational mutagenesis
and ionic strength dependence analysis. We demonstrate that computational
mutations of ionizable residues previously known from experimental
studies to be significant to the C3d:CR2 interaction result in a reduced kon rate constant. Therefore, the replaced (original)
residues contribute to the acceleration of the interaction in the
native complex. These results are in agreement with a previous computational
analysis, based on the calculation of electrostatic free energies
of association for a family of experimentally known mutants and an
alanine scan family of C3d:CR2 complexes.[19] Interestingly, acidic residues within an evolutionarily significant
“electrostatic hotspot” in C3d are the major contributors
to the complex formation. As was suggested in a previous work, this
acidic patch in the complement degradation product C3d may have evolved
to establish a link between innate immunity (complement system) and
adaptive immunity (B cell bound antibodies).[47] Although this C3d “electrostatic hotspot” may be destabilizing
local structure, it accelerates interaction with CR2 and function.
As was suggested by Professor J. Andrew McCammon in his 2009 “Darwinian
Biophysics” article, evolution favors speed and acceleration
of function;[76] and evolution favors function
over stability.[77]
Authors: Chris A Kieslich; Homero Vazquez; Gabrielle N Goodman; Aliana López de Victoria; Dimitrios Morikis Journal: J Mol Graph Model Date: 2011-05-06 Impact factor: 2.518
Authors: Natalie J Serkova; Brandon Renner; Brian A Larsen; Conrad R Stoldt; Kendra M Hasebroock; Erica L Bradshaw-Pierce; V Michael Holers; Joshua M Thurman Journal: Radiology Date: 2010-03-23 Impact factor: 11.105
Authors: Yogesh B Narkhede; Avneesh K Gautam; Rohaine V Hsu; Wilson Rodriguez; Nehemiah T Zewde; Reed E S Harrison; Pablo R Arantes; Zied Gaieb; Ronald D Gorham; Chris Kieslich; Dimitrios Morikis; Arvind Sahu; Giulia Palermo Journal: Front Mol Biosci Date: 2021-03-16