Self-assembly of protein monomers directed by metal ion coordination constitutes a promising strategy for designing supramolecular architectures complicated by the noncovalent interaction between monomers. Herein, two pulse dipolar electron paramagnetic resonance spectroscopy (PDS) techniques, pulse electron-electron double resonance and relaxation-induced dipolar modulation enhancement, were simultaneously employed to study the CuII-templated dimerization behavior of a model protein (Streptococcus sp. group G, protein G B1 domain) in both phosphate and Tris-HCl buffers. A cooperative binding model could simultaneously fit all data and demonstrate that the cooperativity of protein dimerization across α-helical double-histidine motifs in the presence of CuII is strongly modulated by the buffer, representing a platform for highly tunable buffer-switchable templated dimerization. Hence, PDS enriches the family of techniques for monitoring binding processes, supporting the development of novel strategies for bioengineering structures and stable architectures assembled by an initial metal-templated dimerization.
Self-assembly of protein monomers directed by metal ion coordination constitutes a promising strategy for designing supramolecular architectures complicated by the noncovalent interaction between monomers. Herein, two pulse dipolar electron paramagnetic resonance spectroscopy (PDS) techniques, pulse electron-electron double resonance and relaxation-induced dipolar modulation enhancement, were simultaneously employed to study the CuII-templated dimerization behavior of a model protein (Streptococcus sp. group G, protein G B1 domain) in both phosphate and Tris-HCl buffers. A cooperative binding model could simultaneously fit all data and demonstrate that the cooperativity of protein dimerization across α-helical double-histidine motifs in the presence of CuII is strongly modulated by the buffer, representing a platform for highly tunable buffer-switchable templated dimerization. Hence, PDS enriches the family of techniques for monitoring binding processes, supporting the development of novel strategies for bioengineering structures and stable architectures assembled by an initial metal-templated dimerization.
Self-assembly of protein monomeric
units is of great interest in supramolecular complex design,[1−3] but because of the noncovalency of quaternary structural interactions,
mimicking their functionality for the synthesis of new protein complexes
is demanding.[3] Metal coordination is used
as a driving force for the assembly of protein monomers, leading to
a degree of multimerization that depends on the metal ion coordination
geometry.[4−6] Different strategies employed the engineering of
chelating motifs of natural[7] and unnatural[8] amino acid residues, the incorporation of non-natural
ligands onto protein surfaces,[9,10] and the construction
of hybrid coordination motifs,[10] resulting
in metal-induced increased stability of the multimer due to higher
metal binding affinity. Protein–protein interfaces nucleated
by metal coordination have led to the formation of two- and three-dimensional
crystalline protein lattices[11,12] and novel functional
materials.[13] Of particular interest is
the formation of metal-bridged dimers because they are considered
to be the precursor of more complex assemblies.[3] Several techniques such as X-ray crystallography, nuclear
magnetic resonance (NMR), and sedimentation velocity have extensively
characterized these binding processes.[5,7,14] Pulse dipolar electron paramagnetic resonance spectroscopy
(PDS) has been employed to characterize metal motifs that induce polymerization[15] and the conformational flexibility of supramolecular
polymers.[16] Moreover, PDS has recently
emerged as an excellent complementary tool for studying metal ion
binding equilibria with submicromolar sensitivity.[17−21]The four-pulse DEER[22−24] (double electron–electron
resonance) and the
five-pulse RIDME[25,26] (relaxation-induced dipolar modulation
enhancement) experiments (for pulse sequences, see section 1.3 of the Supporting Information) allow detection
of the weak dipolar interaction between paramagnetic centers, which
is characterized by modulation with the dipolar frequency (ωAB) that encodes the interspin distance, rAB. The modulation depth (Δ) of these traces (i.e.,
the amplitude between the signal intensity at time zero and the time
when the signal is entirely damped in the limit of negligible intermolecular
decay) informs the number of coupled spins.[27] In previous studies, pulse electron–electron double resonance
(PELDOR, mainly in the form of the four-pulse DEER experiment) and
RIDME were employed individually to monitor the metal-templated dimerization
of a nitroxide-labeled terpyridine-based ligand model system using
different divalent metal ions as templates[19−21] and proved
the feasibility of monitoring binding events at cryogenic temperatures,
with the modulation depth informing on the degree of binding at a
given metal:ligand ratio.[20]Here,
PELDOR and RIDME were employed complementarily to study the
metal-templated dimerization of a protein model system, the B1 immunoglobulin-binding
domain of protein G of Streptococcus sp. group G
(GB1). Double-histidine (dHis) motifs are incorporated as artificial
metal-binding sites,[28] making this system
particularly suitable for this study. Previous works have used this
system as a biological model for PDS studies,[18,28−30] improving the precision and accuracy of distance
measurements due to the increased rigidity of CuII-chelate
spin-labels through bipedal attachment.[18,28] The I6R1/K28H/Q32H
and I6H/N8H/K28R1 constructs (Figure ) were selected for this work as they were used in
previous studies;[18,31,32] however, their propensity for metal-templated dimerization was unexplored.
Screening revealed that only the I6R1/K28H/Q32H construct gave an
appreciable PELDOR modulation depth when bound to CuII and
ZnII (see section 2.1 of the Supporting Information and dataset[45]), suggesting
that metal-templated dimerization may occur only across the α-helix
motif and not across the β-sheet motif. This disparity is potentially
explained by steric effects, as well as reduced apparent binding affinity
of CuII at the β-sheet motif. Additionally, the modulation
depth was maximized for the CuII series, which is not entirely
surprising because it is consistent with the finding of metal-induced
stabilization of the α-helix motif[33,34] via histidine residues and higher apparent affinity for CuII than for ZnII and other metal ions, per the Irving–Williams
series.[34]
Figure 1
Representations of (a) the nitroxide spin-label
MTSL conjugated
to a cysteine residue, resulting in the R1 side chain; of the monomers
for constructs (b) I6H/N8H/K28R1 and (c) I6R1/K28H/Q32H with CuII ions shown as bronze spheres and R1 side chains and dHis
motifs shown as sticks; and of (d) the putative metal-templated dimeric
structure. The axial solvent ligands are shown as red spheres.
Representations of (a) the nitroxide spin-label
MTSL conjugated
to a cysteine residue, resulting in the R1 side chain; of the monomers
for constructs (b) I6H/N8H/K28R1 and (c) I6R1/K28H/Q32H with CuII ions shown as bronze spheres and R1 side chains and dHis
motifs shown as sticks; and of (d) the putative metal-templated dimeric
structure. The axial solvent ligands are shown as red spheres.The PELDOR method measures the intermolecular nitroxide–nitroxide
(R1–R1) distances within the metal-templated dimer and therefore
provides direct information about dimer formation. The modulation
depth, ΔR1–R1, depends on the dipolar interaction
between nitroxide moieties of each GB1 monomer. The RIDME experiment
measures the intramolecular metal–nitroxide distances (M–R1)
and is a reporter of all metal-bound species. The modulation depth,
ΔM–R1 provides information about the formation
of dimers coordinated around the metal template and fractional saturation
of the metal-binding site, the dHis motif. To characterize these binding
equilibria, a cooperative binding model (see section 1.7 of the Supporting Information) was used to fit simultaneously
ΔR1–R1 and ΔM–R1 values.[35] This allows simultaneous characterization of
an apparent dissociation constant (KD)
for initial metal binding and an apparent cooperativity factor (α)
for the metal-templated dimerization event. Determination of the true
dissociation constant and cooperativity factor is obscured because
the precise CuII concentration available for binding cannot
be quantified, because of the competition with the buffer and unspecific
CuII binding at the protein surface. Such effects are not
treated by the binding model, and instead, apparent thermodynamic
parameters are extracted.First, measurements were performed
as a nine-point pseudotitration
series (where each data point was a discrete sample) for CuII, in the presence of phosphate buffer [150 mM NaCl, 42.4 mM Na2HPO4, and 7.6 mM KH2PO4 (pH
7.4)], having been used extensively for previous EPR methodological
work involving GB1 and CuII-NTA.[30−32]Figure shows the background-corrected
traces for RIDME and PELDOR measurements of the phosphate buffer series.
The corresponding validated distance distributions yielded significant
peaks (i.e., above the noise floor) at ∼2.5 and ∼5.0
nm, respectively (see section 2.3 of the Supporting Information).
Figure 2
In phosphate buffer, (a) deconvoluted RIDME and (b) PELDOR
background-corrected
traces with the modulation depth Δ indicated, (c) bivariate
fitted modulation depth profiles as a function of CuII concentration
for RIDME (blue scatter) and PELDOR (red scatter) data, and (d) the
corresponding error contour, for the phosphate buffer series. Data
in panels a and b are offset vertically to aid visualization, and
the direction of increasing CuII concentration is indicated
by the arrows. The 95% confidence intervals of RIDME and PELDOR modulation
depths in panel c are shown as the blue and red error bars, respectively.
The fitted apparent α and KD values
in panel d are indicated by the white dot.
In phosphate buffer, (a) deconvoluted RIDME and (b) PELDOR
background-corrected
traces with the modulation depth Δ indicated, (c) bivariate
fitted modulation depth profiles as a function of CuII concentration
for RIDME (blue scatter) and PELDOR (red scatter) data, and (d) the
corresponding error contour, for the phosphate buffer series. Data
in panels a and b are offset vertically to aid visualization, and
the direction of increasing CuII concentration is indicated
by the arrows. The 95% confidence intervals of RIDME and PELDOR modulation
depths in panel c are shown as the blue and red error bars, respectively.
The fitted apparent α and KD values
in panel d are indicated by the white dot.In Figure , the
ΔM–R1 behavior was consistent with a reduced
apparent binding affinity of CuII for the dHis motif in
phosphate buffer, with <80% occupancy at a metal:protein ratio
of 1:1. Indeed, ΔM–R1 was systematically lower
for the phosphate buffer series than for the Tris-HCl buffer series
(Supporting Information and vide
infra for details). Interestingly, the ΔR1–R1 behavior suggested that in phosphate buffer, metal-templated dimer
formation was optimized at a metal:protein ratio of 1:1 and persists
even above a stoichiometric CuII concentration. Replicate
measurements of the phosphate buffer series (see the Supporting Information) reproduced this observation, and the
fitted parameters (α = 2, and KD = 2.7 × 10–5) further supported the positive
cooperativity of dimerization. This affinity agrees with reported
literature values for the binding of CuII to histidine
residues on a solvent-exposed α-helix.[36,37]Aware of the possible precipitation of CuII in
the presence
of phosphate salts,[38] we chose a second
buffer by preparing a concentration series of CuCl2 in
Good’s buffers and examining which retained free CuII in solution under alkali conditions via CW-EPR measurements (see section 2.4 of the Supporting Information). CuCl2 precipitated in PBS and MOPS buffers, but Tris-HCl buffer
[150 mM NaCl and 20 mM Tris-HCl (pH 7.4)] retained CuII in solution. For this reason, Tris-HCl was adopted for this study.
Interestingly, CW-EPR data showed the phosphate buffer retained ∼15–60%
of CuII in solution when in the presence of 2 equiv of
imidazole or 0.5 equiv of K28H/Q32H GB1 (see the Supporting Information). Leaving a solution of CuCl2 in phosphate buffer to equilibrate led to negligible available CuII (i.e., subsequent incubation with protein yielded very poor
PELDOR modulation depths). From these observations, we hypothesized
that the changing availability of metal ions in solution would modify
the binding equilibria reflected by the modulation depths of our measurements.Measurements were then performed as an eight-point pseudotitration
series for CuII in the presence of Tris-HCl buffer. Figure shows the background-corrected
traces for RIDME and PELDOR measurements of the Tris-HCl buffer series.
Figure 3
In Tris-HCl
buffer, (a) deconvoluted RIDME and (b) PELDOR background-corrected
traces, (c) bivariate fitted modulation depth profiles as a function
of CuII concentration for RIDME (blue scatter) and PELDOR
(red scatter) data, and (d) the corresponding error contour, for the
Tris-HCl buffer series. Data in panels a and b are offset vertically
to aid visualization, and the direction of increasing CuII concentration is indicated by the arrows. The 95% confidence intervals
of RIDME and PELDOR modulation depths in panel c are shown as the
blue and red error bars, respectively. The fitted apparent α
and KD values in panel d are indicated
by the white dot.
In Tris-HCl
buffer, (a) deconvoluted RIDME and (b) PELDOR background-corrected
traces, (c) bivariate fitted modulation depth profiles as a function
of CuII concentration for RIDME (blue scatter) and PELDOR
(red scatter) data, and (d) the corresponding error contour, for the
Tris-HCl buffer series. Data in panels a and b are offset vertically
to aid visualization, and the direction of increasing CuII concentration is indicated by the arrows. The 95% confidence intervals
of RIDME and PELDOR modulation depths in panel c are shown as the
blue and red error bars, respectively. The fitted apparent α
and KD values in panel d are indicated
by the white dot.In Figure , the
ΔM–R1 behavior indicated a high binding affinity
of CuII for the dHis motif, with >90% occupancy at a
metal:protein
ratio of 1:1. The ΔR1–R1 behavior suggested
that metal-templated dimer formation was optimized at a metal:protein
ratio of 4:5, with a ΔR1–R1 marginally higher
than that at a metal:protein ratio of 1:2 (see the Supporting Information), but was abolished entirely above
stoichiometric ratios of CuII, where either (i) significant
cutting of data was required for processing or (ii) the detected echo
was free of dipolar modulation. Replicates of metal:protein ratios
of 3:5 and 4:5 (see the Supporting Information) showed optimized dimer formation at a metal:protein ratio of 3:5,
which is consistent with a negative cooperativity mode of templated
dimerization (i.e., the initial dHis motif binding event outcompetes
the formation of the dimer construct), and the global fitting of the KD and α parameters supports it further.
Exploratory simulations validated the robustness of the cooperative
binding model (see section 2.5 of the Supporting Information) and indicated a strongly negative cooperativity
parameter (α = 0.15) and a KD of
3.1 × 10–6.Despite the imperfect agreement
between the fitted KD and α parameters
and the phosphate series experimental
data manifest by CuII precipitating from solution, bivariate
fitting of repeat measurements (see the Supporting Information) indicated that the positive cooperativity and
reduced initial binding affinity compared to those of the Tris-HCl
buffer series were reproducible. Additionally, scaling the experimental
CuII concentration by 0.65 for the phosphate and 0.85 for
the Tris-HCl buffer series yielded global root-mean-square deviation
minima upon reprocessing (see the Supporting Information). This observation is consistent with the CW-EPR data (see the Supporting Information) for the phosphate buffer
series showing that only ∼60% of CuII is retained
in the solution, while for the Tris-HCl buffer series, scaling by
a factor of 0.85 corresponds to a shift in optimized dimer formation
from a metal:protein ratio of 3:5 to 1:2, as expected for negative
cooperativity.These observations can be rationalized by the
strong negative cooperativity
for the Tris-HCl buffer (the metal-templated dimer formation would
be disfavored, i.e., the initial metal binding event outcompetes the
formation of the templated dimer) by considering Tris-HCl interacts
strongly with CuII,[39] retaining
it in solution. This maximizes the effective CuII concentration
that can bind dHis motifs, and because for templated dimer formation,
one monomer must have an unoccupied dHis motif, Tris-HCl buffer disfavors
this. On the contrary, precipitation of CuII as Cu3(PO4)2 reduces the effective CuII concentration in solution.[38] The
lower availability of CuII reduces the apparent affinity
of dHis motifs; fewer dHis motifs are occupied, and metal-templated
dimer formation is favored.It is important to note that additional
low-affinity CuII-binding sites on the protein surface,
precipitation in alkaline
pH, and complexation by buffer components are all potentially limiting
the available CuII for ligation by one or two dHis motifs.
In this context, the study of, e.g., morpholine-based buffers effective
under mildly acidic conditions (such as MES) may be interesting for
maximizing the availability of CuII.Positive cooperativity
in metal-templated dimerization is considered
to be rare,[40] while negative cooperativity
characterizes many systems.[41−44] The potential utility of the α-helical dHis
motif for protein–protein interface nucleation by metal binding
is already well-known;[7,33,34] however, the observation that cooperativity of templated dimerization
is modulated by the buffer provides an additional handle for manipulation
of the binding equilibrium. We serendipitously observed that in the
presence of phosphate buffer, CuII-templated dimerization
demonstrated apparent positive cooperativity, while in Tris-HCl buffer,
this templated dimerization displayed strongly negative cooperativity
behavior.Additionally, to the best of our knowledge, this is
the first pulse
dipolar EPR methodology to extract apparent cooperativity and KD parameters by global fitting of nitroxide–nitroxide
PELDOR and CuII–nitroxide RIDME modulation depths.
The results also showcase the robustness and accuracy of PDS in monitoring
equilibrium processes and in detecting variations of cooperativity
mode while changing buffer conditions (J. L. Wort et al., manuscript
in preparation). Finally, this methodology can be easily complemented
by other PDS measurements (for instance, by CuII–CuII RIDME modulation depths or comparison of validated distance
distributions) to study the cooperativity behavior of more complex
systems with nonspecific binding contributions (i.e., of CuII binding away from the dHis motifs), which are notoriously difficult
to disentangle without overfitting by other techniques such as isothermal
titration calorimetry.
Authors: Timothy F Cunningham; Miriam R Putterman; Astha Desai; W Seth Horne; Sunil Saxena Journal: Angew Chem Int Ed Engl Date: 2015-03-27 Impact factor: 15.336
Authors: Maria Oranges; Joshua L Wort; Miki Fukushima; Edoardo Fusco; Katrin Ackermann; Bela E Bode Journal: J Phys Chem Lett Date: 2022-08-17 Impact factor: 6.888