The binding of three closely related chelators: 5-hydroxy-2-methyl-4H-pyran-4-thione (allothiomaltol, ATM), 3-hydroxy-2-methyl-4H-pyran-4-thione (thiomaltol, TM), and 3-hydroxy-4H-pyran-4-thione (thiopyromeconic acid, TPMA) to the active site of human carbonic anhydrase II (hCAII) has been investigated. Two of these ligands display a monodentate mode of coordination to the active site Zn(2+) ion in hCAII that is not recapitulated in model complexes of the enzyme active site. This unprecedented binding mode in the hCAII-thiomaltol complex has been characterized by both X-ray crystallography and X-ray spectroscopy. In addition, the steric restrictions of the active site force the ligands into a 'flattened' mode of coordination compared with inorganic model complexes. This change in geometry has been shown by density functional computations to significantly decrease the strength of the metal-ligand binding. Collectively, these data demonstrate that the mode of binding by small metal-binding groups can be significantly influenced by the protein active site. Diminishing the strength of the metal-ligand bond results in unconventional modes of metal coordination not found in typical coordination compounds or even carefully engineered active site models, and understanding these effects is critical to the rational design of inhibitors that target clinically relevant metalloproteins.
The binding of three closely related chelators: 5-hydroxy-2-methyl-4H-pyran-4-thione (allothiomaltol, ATM), 3-hydroxy-2-methyl-4H-pyran-4-thione (thiomaltol, TM), and 3-hydroxy-4H-pyran-4-thione (thiopyromeconic acid, TPMA) to the active site of humancarbonic anhydrase II (hCAII) has been investigated. Two of these ligands display a monodentate mode of coordination to the active site Zn(2+) ion in hCAII that is not recapitulated in model complexes of the enzyme active site. This unprecedented binding mode in the hCAII-thiomaltolcomplex has been characterized by both X-ray crystallography and X-ray spectroscopy. In addition, the steric restrictions of the active site force the ligands into a 'flattened' mode of coordination compared with inorganic model complexes. This change in geometry has been shown by density functional computations to significantly decrease the strength of the metal-ligand binding. Collectively, these data demonstrate that the mode of binding by small metal-binding groups can be significantly influenced by the protein active site. Diminishing the strength of the metal-ligand bond results in unconventional modes of metalcoordination not found in typical coordination compounds or even carefully engineered active site models, and understanding these effects is critical to the rational design of inhibitors that target clinically relevant metalloproteins.
Metalloproteins represent
a significant fraction of the human proteome,
and many represent important therapeutic targets.[1] With respect to the latter, a large number of metalloprotein
inhibitors have been developed, with clinically approved inhibitors
available for the Zn2+-dependent histone deacetylases (HDACs),
angiotension converting enzyme (ACE), and carbonic anhydrase (CA),
among others.[2,3] In the majority of these examples,
the small molecule inhibitors possess functional groups that bind
to the active site metal ion of the enzyme;[4] a relatively small selection of such groups, including carboxylates,
phosphates, and hydroxamic acids, are commonly employed as the metal-binding
groups (MBGs) of choice.[5] Recently, a number
of efforts have focused on the development of alternative MBGs to
these commonly employed groups,[6] and indeed
some newer metalloprotein inhibitors, such as raltegravir and dolutegravir
that target HIV integrase (HIV1 IN, Mg2+-dependent), employ
more sophisticated heterocyclic MBGs.[7−9] These next-generation
MBGs have the potential to improve the potency, selectivity, and pharmacokinetics
of metalloprotein-targeted therapeutics.As is the case with
other forms of inhibitor and drug development,
the use of structure-aided design can be invaluable to metalloprotein
inhibitor design. In previous efforts, inorganic model compounds have
been utilized to predict the binding of ligands to metalloprotein
active sites.[10−16] Although this approach can be effective, the constrained interactions
and nuances of a metalloprotein active site cannot be readily recapitulated
in such model scaffolds. Several examples of metalloprotein active
sites influencing metal–ligand coordination have been reported.
Specifically, changes in coordination caused by interactions with
the surrounding active site have been observed with inhibitors of
carboxypeptidase A based on the N-hydroxyurea MBG
as well as inhibitors of thermolysin that utilize an α-mercaptoketone
MBG.[17,18] In both cases, the changes in metalcoordination
are the result of large aromatic groups on the inhibitor being positioned
to form significant interactions with hydrophobic regions of the active
site, and the coordination involved is relatively weak.Despite
being a poor MBG for most metalloproteins, the arylsulfonamide
MBG (acetazolamide, Figure 1) dominates the
design of inhibitors of carbonic anhydrases (CAs).[19] CA inhibitors are used in the treatment of glaucoma, epilepsy,
and altitude sickness.[3] The potency of
sulfonamides for CAs is attributed largely to optimized protein–MBG
interactions upon binding the catalyticZn2+ ion; the metal-bound
amine and one of the sulfonamideoxygen atoms both form strong hydrogen
bonds with nearby amino acid residues. In addition, the second sulfonamideoxygen and the aromatic ring are positioned to occupy the substrate
binding pocket of the enzyme active site.
Figure 1
Structures of ATM, TM, TPMA, and several previously reported
hCAII
inhibitors: acetazolamide, based on the arylsulfonamide MBG, 1,2-HOPTO,
2-mercaptophenol (2-MP) and its methylated analog thioguaiacol (TG).
In order to elucidate
the binding of MBGs to metalloproteins as
compared to model compounds, this report describes the binding of
a series of closely related heterocyclicchelators to the active site
of humancarbonic anhydrase II (hCAII) and an inorganic model complex.
Because it has many characteristics that make it a suitable model
system including its rigid structure and ease of crystallization,
hCAII has been widely used to examine protein–ligand interactions.[20,21] In the present study, the MBGs of interest are O,S-donor ligands
based on a hydroxythiopyrone scaffold. Specifically, the three ligands,
5-hydroxy-2-methyl-4H-pyran-4-thione (allothiomaltol,
ATM), 3-hydroxy-2-methyl-4H-pyran-4-thione (thiomaltol,
TM), and 3-hydroxy-4H-pyran-4-thione (thiopyromeconic
acid, TPMA), which differ only by the presence and/or position of
a single methyl group, are examined (Figure 1). In model complexes based on a tris(pyrazolyl)borate (Tp) platform,
these chelators bind in an identical, bidentate manner.[15] In contrast, in the active site of hCAII these
chelators display a variety of coordination modes with the active
site Zn2+ ion, including an unprecedented monodentate mode
of binding by thiomaltol. The results not only show the utility but
also the limitations of bioinorganic modeling while highlighting the
subtle influence of active site structure on metal–ligand bonding.
Such subtle effects on coordination chemistry are not readily predicted
by current paradigms in bioinorganicchemistry and, consequently,
are not implemented in standard drug design efforts directed at metalloproteins.
Taken together, the findings presented here demonstrate that metalcoordination by an exogenous ligand in a metalloprotein active site
is strongly influenced by the protein active site. Existing drug design
protocols for metalloproteins will need to be adapted to account for
these perturbations.Structures of ATM, TM, TPMA, and several previously reported
hCAII
inhibitors: acetazolamide, based on the arylsulfonamide MBG, 1,2-HOPTO,
2-mercaptophenol (2-MP) and its methylated analog thioguaiacol (TG).
Experimental Section
Synthesis
MBGs and TpPh,MeZn(ATM) (TpPh,Me = hydrotris(5,3-methylphenylpyrazolyl)borate)
were synthesized
using modified reported procedures.[15,22] Details can
be found in the Supporting Information.
hCAII Activity Assay
As previously reported,[23] hCAII was expressed and purified, and a detailed
procedure can be found in the Supporting Information. Assays were performed in 50 mM HEPES pH 8.0 containing Na2SO4 to an ionic strength of 100 mM. Enzyme (100 nM final
concentration) was incubated with varying concentrations of inhibitor
for 10 min at room temperature before the addition of substrate (p-nitrophenyl acetate, final concentration between 50 μM
and 10 mM). The reaction was monitored by the increase in absorbance
at 405 nm. Initial reaction rates vs substrate concentration were
plotted for three concentrations of inhibitor, and the curves simultaneously
fit for K using GraphPad
Prism. Representative examples of curve fitting are included in the Supporting Information.
hCAII Crystallization
Crystals of hCAII were obtained
by the sitting-drop or hanging-drop vapor diffusion method. The protein
solution consisted of 20 mg/mL hCAII and 1 mM p-chloromercuribenzoic
acid in 50 mM Tris-SO4, pH 8.0. The precipitant solution
contained 2.7–3.0 M (NH4)2SO4 in 50 mM Tris-SO4 pH 8.15. Drops consisted of 3 μL
of protein solution plus 2.5–4.0 μL of precipitant solution
and were equilibrated at 18 °C against 750 μL of precipitant
solution. Crystals roughly 0.3 × 0.3 × 0.3 mm in size appeared
after 2 days to 3 weeks. Once formed, crystals were transferred to
15 μL of soak solutions containing inhibitor (at saturation,
∼1 mM), 1.5 M sodium citrate, 50 mM HEPES pH 8.15, 5% glycerol,
and 2–5% DMSO. Crystals were taken directly from the soak solutions
for data collection. Due to potential interference from the high concentration
of DMSO necessary for ligand solubility, cocrystallization of the
ligands with hCAII was not attempted.
Crystal Structure Determination
X-ray diffraction studies
on hCAIIcrystals were carried out at 100 K with a Bruker D8 Smart
6000 CCD detector and utilizing Cu Kα radiation (λ = 1.5478
Å) from a Bruker-Nonius FR-591 rotating anode generator. The
data were integrated and scaled using the Bruker APEX software suite.
All crystals belonged to the monoclinic space group P21. The data were phased by molecular replacement using
a previously reported hCAII structure (PDB 3KS3)[24] with water
molecules removed. Models were built by alternating refinement using
REFMAC5[25] and manual visualization and
model building in Coot.[26] Ligand topologies
were generated using the PRODRG server.[27] The structures have been deposited in the Protein Data Bank (PDB
IDs 4MLX and 4MLT for ATM and TM,
respectively). Mercury salts are commonly used in hCAIIcrystallization
to increase crystal quality and size. Both structures contain p-mercuribenzoic acid bound to Cys206. Complete data collection
details and refinement statistics for the TpPh,MeZn(ATM)
and hCAIIcrystal structures can be found in the Supporting Information.
X-ray Absorption Spectroscopy
Samples for XAS (∼2
mM in protein) were prepared from lyophilized CA (Sigma Aldrich),
dissolved in 50 mM phosphate buffer (pH 7.5) that was dialyzed overnight
against the same buffer to remove salts and adventitious metals. MBG
complexes were prepared by addition of a buffered solution of the
MBG to the hCAII solution to a final concentration of 6 mM (3-fold
molar excess). All samples contained 20% (v/v) glycerol as a glassing
agent and were loaded in Lucite cuvettes with 6 μm polypropylene
windows before being frozen rapidly in liquid nitrogen. X-ray absorption
spectra were measured at the National Synchrotron Light Source (NSLS),
beamline X3B, with a Si (111) double-crystal monochromator; harmonic
rejection was accomplished using a Ni focusing mirror. Fluorescence
excitation spectra for all samples were measured with a 31-element
solid-state Ge detector array. Samples were held at ∼15 K in
a Displex cryostat. Detailed data collection and reduction procedures
can be found in the Supporting Information.
Density Functional Computations
All geometry optimizations
were performed using the Gaussian 09 suite of programs,[28] utilizing Becke’s three-parameter hybrid
method with the Lee, Yang, and Parr correlation functional (B3LYP)[29−32] with the 6-311+G(d,p) basis set and CPCM solvation (ε = 10).[33−35] The B3LYP functional has previously been used to successfully recapitulate
geometric parameters of model active sites for Zn2+metalloproteins[36] as well as free energies of water-chloride exchange
in zinc chloridecomplexes.[37] Additional
details and explanations can be found in the Supporting
Information. Linear transit calculations were performed with
the phenyl groups of TpPh,MeZn omitted; this modified system
is referred to as TpZn.
Results
hCAII Inhibition
Previously reported data from screening
a library of MBGs against hCAII revealed TM and TPMA as moderately
potent fragments.[3] Determination of K values for ATM, TM, and TPMA
reveals inhibition constants consistent with these early reports (Table 1). The effect of the inhibitors on the Km curve of hCAII-catalyzed hydrolysis of p-nitrophenyl acetate is consistent with competitive inhibition (Figure S1). While TM and TPMA have similar K values (1.4 ± 0.2 and
1.1 ± 0.2 mM, respectively), ATM is roughly 2-fold more potent
(0.65 ± 0.06 mM). When the hydroxyl group of ATM is methylated
(ATM-OMe, Figure 1), the molecule drops ∼10-fold
(K = 6.9 ± 1.0
mM) in potency. In contrast, methylation of TM (i.e., TM-OMe) results
in a complete loss of inhibitory activity against hCAII (K ≫ 50 mM).
Table 1
K Values (mM) of Compounds
Against hCAII
compound
Ki
compound
Ki
ATM
0.65 ± 0.06
ATM-OMe
6.9 ± 1.0
THM
1.4 ± 0.2
THM-OMe
>50
TPMA
1.1 ± 0.2
Binding Mode Analysis
In order to explain the variation
in inhibitory activity for this series of molecules, the X-ray crystal
structures of ATM and TM bound to TpPh,MeZn model compounds
and the hCAII active site were examined. The crystal structure of
TM bound to this model complex has been previously reported,[15,16] and ATM shows a very similar binding mode to the Zn2+ ion. The ligands bind in a bidentate fashion, resulting in trigonal
bipyramidal geometry around the Zn2+ ion (Figure S2). The S–Zn and O–Zn distances of TpPh,MeZn(ATM) (2.35 and 2.09 Å, respectively) are similar
to those in the complex with TM (2.34 and 2.06 Å). In both cases,
the oxygendonor atom occupies an axial coordination site, while the
sulfur atom is an equatorial donor. The two ligands coordinate the
Zn2+ with nearly ideal “head-on” binding;
the plane formed by the ligand atoms is essentially normal to the
plane formed by the three pyrazolenitrogendonors. This angle (ϕ,
Figure 2) will be quantified by the torsion
angle between the Zn2+ ion, the sulfurdonor, the oxygendonor, and the endocycliccarbon bound to the oxygen; these angles
show absolute values of 166° and 174° for the TpPh,Me complexes of ATM and TM, respectively. Given the similarity of the
TM and ATMcomplexes, it is expected that the TPMA structure would
show an identical coordination geometry.
Figure 2
For ATM, TM, and TPMA,
ϕ is defined as the Zn2+–S–O-C dihedral
angle (A, shown labeled on ATM with
red arrows). This parameter defines the angle between the planes formed
by the Zn–S–O and S–O–C atoms, representing
the tilt of the MBG. MBGs assume different binding modes in TpPh,MeZn (B, ϕModel) and hCAII (C, ϕProtein) complexes. |ϕModel| ranges from 166
to 174°, while |ϕProtein| ranges from 90 to
143° depending on the MBG.
For ATM, TM, and TPMA,
ϕ is defined as the Zn2+–S–O-C dihedral
angle (A, shown labeled on ATM with
red arrows). This parameter defines the angle between the planes formed
by the Zn–S–O and S–O–C atoms, representing
the tilt of the MBG. MBGs assume different binding modes in TpPh,MeZn (B, ϕModel) and hCAII (C, ϕProtein) complexes. |ϕModel| ranges from 166
to 174°, while |ϕProtein| ranges from 90 to
143° depending on the MBG.In the active site of hCAII, ATM adopts the expected bidentate
coordination mode to the Zn2+ ion of hCAII, resulting in
trigonal bipyramidal geometry around the metal (Figure 3). The S–Zn (2.57 Å) and O–Zn (2.28 Å)
bonds are both ∼0.2 Å longer than those in TpPh,MeZn(ATM). As predicted by the model complex, the oxygendonor occupies
an axial coordination site, while the sulfur is in an equatorial position.
The hydroxyl group of the ligand, in addition to binding the Zn2+ ion, is in close proximity to the hydroxyl groups of Thr199
(O–O distance of 3.51 Å) and Thr200 (O–O distance
of 3.71 Å), and the methyl group is positioned to interact with
the side chains of Val121 and Phe131 of the hydrophobic region of
the active site. Due to the steric restrictions of the hCAII active
site, the ligand cannot bind in the ideal head-on fashion (ϕ
= 180°); it is forced to tilt more than 20° relative to
that of the model complex (Figure 2, ϕ
= 143°).
Figure 3
Crystal structure of ATM bound in the active site of hCAII.
The
|Fobs| electron density map (gray) is
shown contoured at 1.5σ for protein residues, while the omit
|Fobs – Fcalc| map (red) is shown contoured at 3.0σ for ATM. A
schematic representation of the interactions between ATM and hCAII
can be found in Figure S12.
Crystal structure of ATM bound in the active site of hCAII.
The
|Fobs| electron density map (gray) is
shown contoured at 1.5σ for protein residues, while the omit
|Fobs – Fcalc| map (red) is shown contoured at 3.0σ for ATM. A
schematic representation of the interactions between ATM and hCAIIcan be found in Figure S12.The crystal structure of TM bound in the active
site of hCAII reveals
an unconventional coordination mode: the ligand acts as a monodentate
donor through the sulfur atom with a bond length of 2.4 Å, resulting
in a distorted tetrahedral geometry around the Zn2+ ion.
The ligand electron density is best fit as a combination of two binding
modes, both with 50% occupancy, in which the coordinated sulfur atoms
overlay (Figure 4). In one orientation, the
exocyclic hydroxyl and methyl groups are oriented toward the hydrophobic
wall of the active site formed by Val143, Leu141, Val121, and Phe131.
In the second conformation, the ligand is flipped so that the hydroxyl
group is directed toward hydrophilic residues of the active site,
allowing for a hydrogen bond with the side chain of Thr200 (O–O
distance of 2.85 Å). In this conformation the ring of TM is positioned
∼1.1 Å closer to the to the side chains of Val121 and
Val143, allowing for enhanced hydrophobiccontacts with these groups.
The average B factor of TM is significantly greater than that of ATM
(40.5 vs 21.5), consistent with its lower affinity and disordered
binding. Efforts to soak TPMA into hCAIIcrystals repeatedly resulted
in poorly defined electron density for the MBG that could not be suitably
modeled.
Figure 4
Crystal structure of TM bound in the active site of hCAII. The
ligand has two conformations, shown in green and cyan. Omit maps (|Fobs|, gray; |Fobs – Fcalc|, red) are shown contoured
at 1.5σ. A diagram of the interactions between THM and hCAII
can be found in Figure S12.
Crystal structure of TM bound in the active site of hCAII. The
ligand has two conformations, shown in green and cyan. Omit maps (|Fobs|, gray; |Fobs – Fcalc|, red) are shown contoured
at 1.5σ. A diagram of the interactions between THM and hCAIIcan be found in Figure S12.X-ray
absorption spectroscopy
(XAS) data suggest the binding modes observed in the crystal structures
are representative of those present in frozen solution. The data for
hCAII with and without the MBGs (ATM, TM, and TPMA) are shown in Figure 5. Detailed fitting results for each data set are
given in Figures S3–S6 and Tables S3–S6. Comparison of the Fourier transforms (FTs) in Figure 5A shows that each MBG (bold lines) leads to only minor overall
perturbations relative to the resting enzyme (thin lines). ATM provides
the most striking changes in the first shell, with both a shift to
higher R and narrowing of the main peak (chiefly
Zn–N/O scattering), together with increased amplitude at R + α ∼2.1 Å (chiefly Zn–S). The
TMcomplex shows similar, although more subtle, changes in the first
shell scattering and substantial changes in the outer shell scattering
pattern. The TPMAcomplex is most similar to the resting enzyme, with
only subtle changes in the first shell apparent in the extended X-ray
absorption fine structure (EXAFS) FTs. However, examination of the k-space EXAFS data (Figure 5B) reveals
that all three MBGs cause a similar shift in the third oscillation
of the EXAFS (k ∼7 – 9 Å–1). Comparison of the theoretical EXAFS for Zn–N and Zn–S
interactions shows this is where the two patterns are most likely
to show visible divergence (Figure S7),
suggesting that all three MBG complexes include a Zn–S scattering
interaction. Each MBG causes a similar shift in the shape of the Zn
X-ray absorption near edge structure (XANES, Figure
S8), also consistent with S-coordination.
Figure 5
Fourier transforms (A)
of the k3-weighted
EXAFS (B) of hCAII with ATM, TM, and TPMA. In each case, the data
for the resting enzyme are shown as a thin line overlay.
Fourier transforms (A)
of the k3-weighted
EXAFS (B) of hCAII with ATM, TM, and TPMA. In each case, the data
for the resting enzyme are shown as a thin line overlay.The curve fits are consistent with the qualitative
assessment given
above. The ATMcomplex with hCAII appears 5-coordinate, with the sulfur
of the MBG directly coordinated (fits that excluded the Zn–S
bond gave fit residuals that were 3-fold larger, Figure S4 and Table S4). The Zn–N/O distance is also
slightly longer than for the resting enzyme and the other two MBG
complexes, suggesting higher coordination in the ATMcomplex, and
it is this XANES spectrum that shows that largest energy shift. In
contrast, fits to the TMcomplex data suggest that the total coordination
number remains at four with the MBG coordinated through only the sulfur
atom (fits that excluded the Zn–S bond gave fit residuals that
were 2- to 3-fold larger, Figure S5 and Table
S5). This is consistent with the change in the outer shells,
where more linear MBG coordination could potentially amplify multiple-scattering
interactions, although a deeper analysis is outside the scope of the
present study. TM also produces a change in shape in the XANES but
a smaller energy shift than ATM. The TPMAcomplex is strikingly similar
to the resting enzyme with only the shift in principal frequency noted
above being readily apparent. Fits to these data also suggest retention
of a total coordination of four in the TPMAcomplex (as observed for
TM), with the MBG S-bound (fits that excluded the Zn–S bond
gave fit residuals that were approximately 2-fold larger, Figure S6 and Table S6). This is supported by
the XANES, which clearly show a change in shape on addition of TPMA.
Computational Analysis
To assess one possible cause
for the switch to monodentate coordination of TM and TPMA in the active
site of hCAII, linear transit computations employing density functional
theory (DFT) were conducted along ϕ from 180° to 90°
for TMcomplexed to the simplified TpZn scaffold. Near ϕ = 180°,
the plane formed by TM is perpendicular to the plane defined by the
three Zn2+-coordinating pyrazolenitrogens. Similar to
the TpPh,MeZn(TM) crystal structure, this computed structure
adopts a trigonal bipyramidal geometry with the hydroxyl group as
an axial donor and the sulfurdonorcoordinating equatorially. The
calculated O–Zn and S–Zn distances (2.08 and 2.45 Å,
respectively) are similar to those observed in the crystal structure
of TpPh,MeZn(TM) (Figure S9).As TM is tilted along ϕ, the Zndonor atom distances increase
gradually until ϕ reaches 120°, which is the last point
along the linear transit where the ligand coordination is bidentate
(Figure 6). For values of ϕ < 120°,
no stationary states corresponding to bidentate coordination of the
Zn2+ ion are obtained; monodentate coordination by the
thione becomes the favored binding mode. At these points, the O–Zn
distance is >3.4 Å, while the S–Zn bond length, having
a value of 2.30 – 2.32 Å, more closely resembles a thiolate–Zn2+ bond.[38] Similar trends in coordination
mode along the ϕ reaction coordinate are also present for TM
and TPMA (Figure 6).
Figure 6
Calculated O–Zn
distances (top) and relative binding energies
(bottom) as a function of ϕ from linear transit computations.
Calculated O–Zn
distances (top) and relative binding energies
(bottom) as a function of ϕ from linear transit computations.For all three MBGs, the lowest
energies are achieved at values
of ϕ near 180°, where the ligand assumes its ideal “head-on”
binding mode as observed in the model complexes. Distorting the ligand
coordination from ϕ = 180° leads to an increase in energy
relative to the head-on binding geometry, and the energy of the complex
appears to follow a parabolic path up to the point where the coordination
mode shifts from bidentate to monodentate (Figure 6). Shifting to monodentate coordination of Zn2+ through the sulfur atom causes the relative energy of the complex
to level out at ∼12–15 kcal/mol above the energy of
the “head-on” binding mode.
Discussion
Aside
from being tilted away from ideal “head-on”
binding, the coordination of ATM to the active site Zn2+ ion of hCAII is similar to that predicted by the TpPh,Me model complex (Figure S2). This bidentate
coordination mode has been previously reported for 2-mercaptopyridine-N-oxide (1,2-HOPTO), a similar MBG (Figure 7).[39] The previously reported Ki of 1,2-HOPTO against hCAII (0.85 mM) is close
to that of ATM and coincides with the similar binding mode.[3] Although the interaction between ATM and the
Zn2+ ion appears to be bidentate, the residual inhibitory
activity of ATM-OMe suggests that the electrostatic interaction between
the oxygendonor and the Zn2+ ion is not essential for
binding.
Figure 7
Overlay of the crystal structures of ATM and 1,2-HOPTO (PDB ID 3M1K, shown in yellow)
bound to hCAII. Although the donor atoms are positioned similarly
(left), a view along the plane of the ligands (right) reveals that
ATM is ∼10° closer to ideal “head-on” binding.
Overlay of the crystal structures of ATM and 1,2-HOPTO (PDB ID 3M1K, shown in yellow)
bound to hCAII. Although the donor atoms are positioned similarly
(left), a view along the plane of the ligands (right) reveals that
ATM is ∼10° closer to ideal “head-on” binding.The coordination mode of TM to
the active site Zn2+ ion
of hCAII demonstrates that a protein environment can strongly perturb
MBG coordination. The inhibitory activity of ATM-OMe suggests that
the interaction between the hydroxyl group and the Zn2+ ion is not essential for activity, and the monodentate binding of
TM further supports this. While the methyl group of ATM is ideally
positioned for hydrophobic interactions when the ligand adopts bidentate
coordination, this is not the case for TM. It appears that in order
to maximize other protein–ligand interactions, the O–Zn
binding interaction is sacrificed. The conformation in which the hydroxyl
and methyl groups are oriented toward the hydrophobic wall of the
active site is very similar to a previously reported structure of
2-mercaptophenol (2-MP) bound to hCAII (Figure 8).[40] Although both TM and 2-MP are monodentate
ligands in hCAII, only the TpPh,Me model complex of 2-MP
recapitulates this monodentate binding mode.[41] In contrast, the TpPh,MeZn(TM) complex shows strong bidentate
coordination from both the sulfur and oxygendonor atoms. This suggests
that while the monodentate binding of 2-MP to hCAII is driven largely
by the properties of the ligand itself, the monodentate binding mode
of TM is a direct result of interactions with the hCAII active site
environment.
Figure 8
Overlay of the crystal structure of TM and inhibitors that show
similar binding modes. Left: The conformation with
the hydroxyl group of TM facing the hydrophobic pocket occupies a
space similar to that of 2-mercaptophenol (PDB 2OSM, shown in green).
Right: When the hydroxyl group of TM is oriented toward the hydrophilic
side of the active site, the ring nearly overlays with that of 2-mercaptophenol.
In contrast to TM, which loses all inhibitory activity
when methylated
(TM-OMe), when the hydroxyl group of 2-MP is methylated (TG, Figure 1), the activity against hCAII is unaffected (K =3.2 ± 0.3 μM
for TG vs 3.0 ± 0.7 μM for 2-MP).[3] This suggests that the binding mode of TM that is relevant to inhibition
is the conformation in which the hydroxyl and methyl groups are oriented
toward the hydrophilic residues of the active site. The loss in potency
for TM-OMe is consistent with this binding mode, as the interaction
between TM and Thr200 would be diminished and the methoxy group would
likely have a stericclash with either neighboring protein residues
or well-ordered active site water molecules. With the hydroxyl group
oriented toward the hydrophilicside of the pocket, a hypothetical
bidentate coordination mode would position the methyl group of TM
very close to the hydrophilicside of the active site, where well-ordered
water molecules interact with protein residues. Consequently, TM rotates
toward a monodentate coordination of Zn2+ to preserve the
preexisting interactions in the pocket. The microscopic pKa values of TM in the active site of hCAII are computed
to be 4.1 and 7.2 when the hydroxyl group is oriented toward the hydrophilic
and hydrophobic pockets, respectively (Figure
S11).[42] Coupling these data with
the observation of the two conformations in a ∼1:1 ratio in
the crystal structure determined at pH 8 suggest that at low pH, the
predominant species of TM is protonated and oriented toward the hydrophobic
pocket (attempts to verify this crystallographically were unsuccessful);
at high pH (pH > 7.2), the deprotonated form of TM is dominant
with
the ligand hydroxyl group oriented in the hydrophilic pocket, which
is likely the conformation responsible for the observed inhibitory
activity.Overlay of the crystal structure of TM and inhibitors that show
similar binding modes. Left: The conformation with
the hydroxyl group of TM facing the hydrophobic pocket occupies a
spacesimilar to that of 2-mercaptophenol (PDB 2OSM, shown in green).
Right: When the hydroxyl group of TM is oriented toward the hydrophilicside of the active site, the ring nearly overlays with that of 2-mercaptophenol.From the structural data acquired
for TM, particularly when compared
to the analogous O,S-donorATM, it is evident that the Zn2+–MBG interaction is not the sole dictator of ligand binding.
Ligand acidity is likely not a major driving force in the change in
coordination, as ATM and TM have relatively close acidities (pKa = 7.64 and 8.06, respectively).[43] The DFT-derived geometric and energetic analyses
of TpZn(MBG) complexes show that over the ligand orientations available
to MBGs in hCAII (|ϕ| = 90–143°), there can be a
very small energy difference between monodentate and bidentate coordination
of Zn2+. For example, between ϕ = 125–115°,
bidentate and monodentate coordination modes for the ligands considered
in this study differ in energy by <5 kcal/mol. From this observation,
it is reasonable that the orientation of TMcan, in some circumstances,
be altered by interactions with the active site of hCAII. This finding
implies that de novo or fragment-based approaches to inhibitor development
must take care to elucidate circumstances where protein effects alter
the coordination mode of an MBG.
Conclusion
The
rational design of metalloprotein inhibitors requires knowledge
as to how those inhibitors coordinate the active site metal ion. While
small molecule model complexes have been used as proxies for coordination
in enzyme active sites, the results presented here demonstrate that
the active site environment can have a significant effect on the metal–ligand
interaction; in cases where structural data is not available, care
must be taken in the assumptions made about metal-inhibitor interaction.
In the case of hCAII, the steric restrictions of the active site force
ligands to bind in conformations far from ideal head-on binding, drastically
decreasing the strength of metalcoordination. Other interactions,
including hydrogen bonding and hydrophobiccontacts, can influence
the binding mode of the MBG, leading to coordination modes not observed
in conventional coordination chemistry. Studies are underway to further
understand the role of metalcoordination in the binding of metalloprotein
inhibitors and how binding is influenced by other interactions within
the active site.
Authors: David T Puerta; Julie R Schames; Richard H Henchman; J Andrew McCammon; Seth M Cohen Journal: Angew Chem Int Ed Engl Date: 2003-08-18 Impact factor: 15.336
Authors: Carlo Baggio; Linda Cerofolini; Marco Fragai; Claudio Luchinat; Maurizio Pellecchia Journal: ACS Med Chem Lett Date: 2018-01-17 Impact factor: 4.345
Authors: Madeline E Kavanagh; Anthony G Coyne; Kirsty J McLean; Guy G James; Colin W Levy; Leonardo B Marino; Luiz Pedro S de Carvalho; Daniel S H Chan; Sean A Hudson; Sachin Surade; David Leys; Andrew W Munro; Chris Abell Journal: J Med Chem Date: 2016-03-22 Impact factor: 7.446