Lamya H Al-Wahaibi1, Sekar Karthikeyan2, Olivier Blacque3, Amal A El-Masry4, Hanan M Hassan5, M Judith Percino6, Ali A El-Emam4, Subbiah Thamotharan2. 1. Department of Chemistry, College of Sciences, Princess Nourah bint Abdulrahman University, Riyadh 11671, Saudi Arabia. 2. Biomolecular Crystallography Laboratory, Department of Bioinformatics, School of Chemical and Biotechnology, SASTRA Deemed University, Thanjavur 613 401, India. 3. Department of Chemistry, University of Zurich, Winterthurerstrasse 190, Zurich 8057, Switzerland. 4. Department of Medicinal Chemistry, Faculty of Pharmacy, Mansoura University, Mansoura 35516, Egypt. 5. Department of Pharmacology and Biochemistry, Faculty of Pharmacy, Delta University for Science and Technology, International Costal Road, Gamasa City, Mansoura 11152, Egypt. 6. Unidad de Polímeros y Electrónica Orgánica, Instituto de Ciencias, Benemérita Universidad Autónoma de Puebla, Val3-Ecocampus Valsequillo, Independencia O2 Sur 50, San Pedro Zacachimalpa, Puebla-C.P. 72960, Mexico.
Abstract
Two 3,6-disubstituted-[1,2,4]triazolo[3,4-b][1,3,4]thiadiazole derivatives, namely, 3-(adamantan-1-yl)-6-(2-chloro-6-fluorophenyl)-[1,2,4]triazolo[3,4-b][1,3,4]thiadiazole 1 and 6-(2-chloro-6-fluorophenyl)-3-phenyl-[1,2,4]triazolo[3,4-b][1,3,4]thiadiazole 2, were prepared, and the detailed analysis of the weak intermolecular interactions responsible for the supramolecular self-assembly was performed using X-ray diffraction and theoretical tools. Analyses of Hirshfeld surface and 2D fingerprint plot demonstrated the effect of adamant-1-yl/phenyl moieties on intermolecular interactions in solid-state structures. The effect of these substituents on H···H/Cl/N contacts was more specific. The CLP-PIXEL and density functional theory methods provide information on the energetics of molecular dimers observed in these compounds. The crystal structure of compound 1 stabilizes with a variety of weak intermolecular interactions, including C-H···N, C-H···π, and C-H···Cl hydrogen bonds, a directional C-S···π chalcogen bond, and unconventional short F···C/N contacts. The crystal structure of compound 2 is stabilized by π-stacking interactions, C-H···N, C-H···π, and C-H···Cl hydrogen bonds, and highly directional attractive σ-hole interactions such as the C-Cl···N halogen bond and the C-S···N chalcogen bond. In addition, S(lp)···C(π) and short N···N contacts play a supportive role in the stabilization of certain molecular dimers. The final supramolecular architectures resulting from the combination of different intermolecular interactions are observed in both the crystal packing. The molecular electrostatic potential map reveals complementary electrostatic potentials of the interacting atoms. The quantum theory of atoms in molecules approach was used to delineate the nature and strength of different intermolecular interactions present in different dimers of compounds 1 and 2. The in vitro experiments suggest that both compounds showed selectivity against COX-2 targets rather than COX-1. Molecular docking analysis showed the binding pose of the compounds at the active sites of COX-1/2 enzymes.
Two 3,6-disubstituted-[1,2,4]triazolo[3,4-b][1,3,4]thiadiazole derivatives, namely, 3-(adamantan-1-yl)-6-(2-chloro-6-fluorophenyl)-[1,2,4]triazolo[3,4-b][1,3,4]thiadiazole 1 and 6-(2-chloro-6-fluorophenyl)-3-phenyl-[1,2,4]triazolo[3,4-b][1,3,4]thiadiazole 2, were prepared, and the detailed analysis of the weak intermolecular interactions responsible for the supramolecular self-assembly was performed using X-ray diffraction and theoretical tools. Analyses of Hirshfeld surface and 2D fingerprint plot demonstrated the effect of adamant-1-yl/phenyl moieties on intermolecular interactions in solid-state structures. The effect of these substituents on H···H/Cl/N contacts was more specific. The CLP-PIXEL and density functional theory methods provide information on the energetics of molecular dimers observed in these compounds. The crystal structure of compound 1 stabilizes with a variety of weak intermolecular interactions, including C-H···N, C-H···π, and C-H···Cl hydrogen bonds, a directional C-S···π chalcogen bond, and unconventional short F···C/N contacts. The crystal structure of compound 2 is stabilized by π-stacking interactions, C-H···N, C-H···π, and C-H···Cl hydrogen bonds, and highly directional attractive σ-hole interactions such as the C-Cl···N halogen bond and the C-S···N chalcogen bond. In addition, S(lp)···C(π) and short N···N contacts play a supportive role in the stabilization of certain molecular dimers. The final supramolecular architectures resulting from the combination of different intermolecular interactions are observed in both the crystal packing. The molecular electrostatic potential map reveals complementary electrostatic potentials of the interacting atoms. The quantum theory of atoms in molecules approach was used to delineate the nature and strength of different intermolecular interactions present in different dimers of compounds 1 and 2. The in vitro experiments suggest that both compounds showed selectivity against COX-2 targets rather than COX-1. Molecular docking analysis showed the binding pose of the compounds at the active sites of COX-1/2 enzymes.
In recent years, 1,2,4-triazoles
and their fused heterocyclic derivatives
received considerable attention owing to their diverse biological
activities.[1,2] Several 1,2,4-triazoles were reported to
possess potent anti-inflammatory,[3−9] antifungal,[10,11] antibacterial,[12,13] and anticancer activities.[14−16] On the other hand, the 1,3,4-thiadiazole
heterocycle was early recognized as the core pharmacophore of numerous
bioactive agents,[17−20] possessing marked anti-inflammatory[21−23] and anticancer activities.[24,25] Moreover, the hybrid triazole-thiadiazole derivative, 1,2,4-triazolo[3,4-b][1,3,4]thiadiazole, was recently reported to possess marked
anticancer[26−29] and antibacterial activities[30,31] in addition to anti-inflammatory
activity via selective inhibition of the cyclooxygenase COX-2 isoform.[32−34]In continuation of our ongoing studies on the inhibitory selectivity
of COX-1/2 of 1,2,4-triazoles[35] and 1,2,4-triazolo[3,4-b][1,3,4]thiadiazoles,[36] we report
herein the synthesis, structural analysis, and COX-1/2 inhibitory
activity of two 1,2,4-triazolo[3,4-b][1,3,4]thiadiazole
derivatives. Khan et al. synthesized libraries of triazolothiadiazole
and triazolothiadiazine derivatives, which displayed remarkable cholinesterase
and monoamine oxidase inhibitory properties.[37] In their study, the crystal structure of one of the triazolothiadiazole
derivatives, 3-(3-bromophenyl)-6-(o-tolyloxymethyl)-[1,2,4]triazolo[3,4-b][1,3,4]thiadiazole, was reported as the first 1,2,4-triazolo[3,4-b][1,3,4]thiadiazole structure that exhibits a short chalcogen
bond [C=S···N: 2.795 (2) Å and 163.9 (2)°].
At that time, a Cambridge Structural Database (CSD) search revealed
that no structure with a triazolothiadiazole ring system contained
a short contact between the S atoms and N donors in the crystal structure,
which was significantly shorter than 3.0 Å. In addition to this
chalcogen bond, the π-stacking interaction formed between the
planar aryl-substituted triazolothiadiazole moieties and the C–H···π
interaction also involved in the stabilization of the crystal structure.
In another study,[38] the authors evaluated
the S···N chalcogen bond and the short N···N
contact found in the same centrosymmetric dimer using a 3D-deformation
density map, an electrostatic potential map, and quantum theory of
atoms in molecules (QTAIM) parameters.In the present investigation,
we describe the molecular conformation
and the role of noncovalent interactions in the crystal packing of
two closely related 1,2,4-triazolo[3,4-b][1,3,4]thiadiazole
derivatives, namely, 3-(adamantan-1-yl)-6-(2-chloro-6-fluorophenyl)-[1,2,4]triazolo[3,4-b][1,3,4]thiadiazole 1 and 6-(2-chloro-6-fluorophenyl)-3-phenyl-[1,2,4]triazolo[3,4-b][1,3,4]thiadiazole 2, in which adamantane
and phenyl substituents are introduced in the core skeleton. The effect
of adamantane and phenyl substituents has been characterized employing
different computational tools, including the Hirshfeld surface (HS),
molecular electrostatic potential (MESP) map, Bader’s QTAIM,
and noncovalent interaction plot (NCIPlot). The PIXEL energy calculation
helps identify energetically potential dimers within crystal structures.
The crystal structure of 1 is primarily stabilized by
intermolecular C–H···N, C–H···Cl,
and C–H··· π hydrogen bonds and a highly
directional σ–hole (chalcogen bond) C–S···C(π)
interaction in addition to unconventional F···C/N contacts.
Similarly, the crystal structure of 2 is stabilized by
intermolecular C–H···N, C–H···Cl,
C–H···π, and C–H···F
hydrogen bonds, weak π···π stacking interactions,
and directional σ–hole interactions, including a C–S···N
chalcogen bond and a Cl···N halogen bond. In addition,
an unconventional lp··· π contact is also observed
in one of the dimers of 2. These noncovalent interactions
play a critical role in the synthesis and stabilization of supramolecular
architectures of numerous organic and inorganic compounds relevant
to medicine, materials science, and catalysis.[39]It is known that two cyclooxygenase (COX-1 and COX-2)
enzymes have
been involved in the inflammatory cell signaling pathway in an arachidonic
acid-dependent manner. Selective inhibition of COX-2 can reduce the
adverse reactions, including ulcerogenic effects of non-steroidal
anti-inflammatory drugs such as acetylsalicylic acid and ibuprofen.[40] In the present investigation, we demonstrated
the effect of the adamantane moiety on the anti-inflammation potential
using two closely related derivatives of triazolothiadiazole. Further,
we described the observed bioactivity of the title compounds using
an in vitro COX-1/2 assay, molecular docking, and molecular mechanics
with generalized Born and surface area solvation (MM-GBSA) analyses.
Results and Discussion
The purpose
of this study is to investigate the effect of the adamantane
and phenyl groups introduced in the core skeleton of the triazolothiadiazole
ring on crystal packing and intermolecular interactions using various
computational approaches. With the support of the in vitro data from
the COX-1/2 assay, in silico molecular docking and free energy calculation,
we describe the effect of the adamantane group on the observed biological
activity.
Chemical Synthesis
The investigated
compounds 1 and 2 were prepared using the
following reaction sequences outlined in Scheme . The corresponding carboxylic acid hydrazide A was treated with carbon disulfide in an ethanolic potassium
hydroxide solution to yield the corresponding potassium dithiocarbazate
intermediates B, which were subsequently reacted with
hydrazine to produce the corresponding 4-amino-5-substituted-4H-1,2,4-triazole-3-thiols C.[41,42] Compounds C were then reacted with 2-chloro-6-fluorobenzoic
acid and phosphorous oxychloride by heating under reflux for 2 hours
to produce target compounds 1 and 2 in yields
of 84 and 72%, respectively.
Scheme 1
Synthetic Pathway for the Title Compounds 1 and 2
Description of Molecular and Crystal Structures
For the two closely related triazolothiadiazoles, a low-temperature
(160 K) single-crystal structure determination has been performed
to delineate the effect of adamantan-1-yl (compound 1) and phenyl (compound 2) moieties attached at position
3 (C9) carbon of the triazolothiadiazole ring on molecular conformation,
crystal packing, and intermolecular interactions. Both compounds have
a 2-chloro-6-fluorophenyl substituent at position 6 (C7) to study
their role in crystal packing and intermolecular interactions. The
X-ray analysis revealed that both compounds crystallize in the monoclinic
system, and one molecule is present in the respective asymmetric unit.
In compound 1, the 2-chloro-6-fluorophenyl ring was disordered
over two orientations with the site occupation factors of 0.7764(19)
for the major disordered component. This major disordered component
was used for all analyses reported in this work. Crystallographic
data and refinement parameters for compounds 1 and 2 are presented in Table , and their thermal ellipsoid representations are shown
in Figure .
Table 1
Crystal Data and Structure Refinement
Parameters for Compounds 1 and 2
compound 1
compound 2
empirical formula
C19H18ClFN4S
C15H8ClFN4S
formula weight
388.88
330.76
crystal
system
monoclinic
monoclinic
space group
P21/n
P21/c
a/Å
13.0790(2)
11.1796(3)
b/Å
11.69139(17)
15.4566(5)
c/Å
13.3373(2)
8.3228(2)
α/°
90
90
β/°
117.769(2)
93.499(2)
γ/°
90
90
volume/Å3
1804.55(6)
1435.49(7)
Z
4
4
ρcalc g/cm3
1.431
1.530
μ/mm–1
3.130
3.832
F(000)
808.0
672.0
crystal size/mm3
0.25 × 0.21 × 0.14
0.32 × 0.2 × 0.02
radiation
Cu Kα (λ = 1.54184)
2Θ range for data collection/°
7.82 to 148.9
7.924 to 148.986
index ranges
–11 ≤ h ≤ 16, –14 ≤ k ≤ 14, –16 ≤ l ≤ 13
–13 ≤ h ≤ 12, –15 ≤ k ≤ 19, –9 ≤ l ≤ 10
reflections
collected
18687
11943
crystal size/mm3
0.25 × 0.21 × 0.14
0.32 × 0.2 × 0.02
independent reflections
3685
[Rint = 0.0176, Rsigma = 0.0088]
2923 [Rint = 0.0336, Rsigma = 0.0284]
data/restraints/parameters
3685/501/297
2923/0/199
goodness-of-fit on F2
1.061
1.073
final R indexes [I ≥ 2σ (I)]
R1 = 0.0436, wR2 = 0.1144
R1 = 0.0432, wR2 = 0.1145
final R indexes [all data]
R1 = 0.0441, wR2 = 0.1149
R1 = 0.0598, wR2 = 0.1252
largest diff. peak/hole/e Å–3
0.69/–0.33
0.69/–0.72
CCDC no.
2122999
2123000
Figure 1
Thermal ellipsoid
plots of compounds (a) 1 (major
disordered component), (b) 1 (minor disordered component),
and (c) 2 drawn at the 50% probability level. (d) Structural
superimposition of structures 1 (major disordered component:
orange) and 2 (gray).
Thermal ellipsoid
plots of compounds (a) 1 (major
disordered component), (b) 1 (minor disordered component),
and (c) 2 drawn at the 50% probability level. (d) Structural
superimposition of structures 1 (major disordered component:
orange) and 2 (gray).The central triazolothiadiazole unit makes a right
angle (86.6°)
with the mean plane of the adamantane cage in compound 1, whereas the unsubstituted phenyl ring is nearly coplanar (3.4°)
with the central triazolothiadiazole moiety in compound 2. We note that the orientation of the 2-chloro-6-fluorophenyl ring
is nearly perpendicular to the mean plane of the central unit in both
structures (75.4° in 1 and 83.0° in 2). The Mogul geometry check suggests that both structures do not
show unusual bond lengths or angles. However, it should be mentioned
that the C7–S1 bond [1.761(1) Å in compound 1 and 1.757(1) Å in 2] exhibits bond lengthening
compared to the C8–S1 bond [1.738(1) Å in 1 and 1.728(1) Å in 2]. A similar feature has been
observed in related structures deposited in the CSD (version 5.42,
November 2020).[43] This bond lengthening
could be due to the formation of a σ–hole interaction
(chalcogen bond). Furthermore, the CSD search detected 51 hits containing
different substituents attached to atom C9 of the triazole ring and
atom C7 of the thiadiazole ring. Five of these compounds have an adamantane
cage attached to a thiadiazole ring (CSD refcodes: BOTYEP, UPAVIR,
VUNLUM, VUNMAT, and WADHIU).[44−47] Unlike compound 1, which has an adamantane
cage attached to a triazole ring, we identified eight structures containing
monosubstituted (CSD refcodes: NITSIV, ILETOK, LEPQED, QEMMUR, and
SAPRAD, UXIPOI),[36,48−52] disubstituted (CSD refcode: XOYWOZ),[53] and trisubstituted (csd refocde: GAJCUS)[38] halophenyl groups. The halogen atoms are either Cl or F
or both present at different positions of the phenyl ring. Contrary
to compounds 1 and 2, the substituted phenyl
ring in these structures is coplanar with the central triazolothiadiazole
ring. This planarity could be maintained due to the formation of intramolecular
S···X (X = Cl or F) contact in all structures mentioned
above except in 6-(4-chlorophenyl)-3-(thiophen-2-yl)-[1,2,4]triazolo[3,4-b][1,3,4]-thiadiazole (UXIPOI).[52] In this structure, Cl was substituted in the para position of the
phenyl ring and does not participate in the S···Cl
contact.For a deeper understanding of why title compounds 1 and 2 do not exhibit either S···Cl
or
S···F intramolecular contact (or why disubstituted
phenyl adopts non-coplanar with central unit?), as well as to uncover
the energy barriers associated with it, we performed a relaxed potential
surface scan around the C7–C1 bond in compound 2 at the B3LYP/6-31G+(d) level of theory (Figure ). The result suggests that the conformer
“a” is the least energy conformer for
the S1–C7–C1–C6 torsion angle of ±90°,
which is very similar to that of the X-ray conformer (−97.08°).
In the second least energy conformer “b”,
S and F atoms are displaced on the same side, whereas in the high
energy conformer “c”, S and Cl atoms
are oriented on the same side. The energy difference between the conformers
“a” and “b”
is 2.8 kcal mol–1, while the corresponding energy
difference for the conformers “b” and
“c” is only 1.3 kcal mol–1 (4.0 kcal mol–1 for the conformers “a” and “c”). This
analysis demonstrates that the twisted orientation of the disubstituted
phenyl ring has minimum energy on its potential energy surface, and
a molecular conformation with S···F/Cl contact has
a higher energy range from 2.8 to 4.0 kcal mol–1 concerning the minimum energy conformer.
Figure 2
Calculated potential
energy for rotation around the C7–C1
bond in structure 2.
Calculated potential
energy for rotation around the C7–C1
bond in structure 2.As shown in Figure S1, the molecular
conformation of compound 1 is stabilized by two intramolecular
C–H···N interactions. Similarly, compound 2 has an intramolecular C–H···N interaction.
The topological analysis confirms the existence of these interactions
(Table S1). Some of the related structures
are also stabilized by an intramolecular C–H···N
interaction as observed in compounds 1 and 2 (CSD refcodes for these structures are given in Supporting Information:
see Table S2).[36−38,44,48,49,52−63] Due to the existence of this intramolecular interaction, the central
triazolothiadiazole moiety becomes coplanar with the substituent group
attached to the triazole ring at atom C9 (corresponding atom in the
related structures). In other structures, the substituent group on
the triazole ring is slightly twisted to the mean plane of the central
unit due to the lack of an intramolecular C–H···N
interaction.
Hirshfeld Surface Analysis and 2D Fingerprint
Plots
Hirshfeld surface (HS) analysis has been widely used
to qualitatively determine the intermolecular contacts within crystal
structures. HS and decomposed 2D fingerprint (FP) plots reveal the
effect of the phenyl and adamantane moieties on the intermolecular
interactions. Figure a shows the HS over the dnorm values
for compounds 1 and 2. In compound 1, the intense red spots are shown for the intermolecular
C–H···N hydrogen bond and an attractive σ–hole
interaction such as a chalcogen bond of type S···C(π)
and an unorthodox bifurcated fluorine bond of type F···C/N
contacts.
Figure 3
HSs show red spots corresponding to the close intercontacts observed
in structures (a) 1 and (b) 2 in two different
orientations.
HSs show red spots corresponding to the close intercontacts observed
in structures (a) 1 and (b) 2 in two different
orientations.In compound 2, the S···N
chalcogen
bond shows intense and broad red surfaces, and a short N···N
contact also shows an intense spot near the chalcogen interacting
region (Figure b).
This feature suggests that the chalcogen bond along with a short N···N
contact plays a significant role in the stabilization of the crystal
structure. The relatively less intense spots were observed for C–H···N,
C–H···Cl, and Cl···N interactions.
Over the five-membered ring, we observed less intense red spots due
to the π-stacking interaction. We also observed tiny red spots
for the S(lp)···C(π) contact in the same π-stacking
dimer, which might provide additional stabilization to this dimer.The 2D-FP plots show distinct distribution patterns for intercontacts
in 1 and 2 (Figures , S2 and S3, Supporting
Information). The intermolecular H···H interactions
occupy most of the HS area toward the crystal packing of these structures.
Due to the adamantane cage in compound 1, the H···H
contacts increase (38.6%) and those in compound 2 decrease
(19.7%) due to the phenyl ring. The next significant contribution
comes from H···N contacts (14.3% in 1 and
13.1% in 2), and the contribution of these contacts is
comparable. Furthermore, this contact shows double spikes on the 2D-FP
and the tip distance is at 2.3 Å in compound 1,
whereas the corresponding contact beyond 2.5 Å in compound 2 indicates a relatively weak nature. The contributions of
other inter-contacts such as H···C (11% in 1 and 13.9% in 2) and H···S (6.3% in 1 and 7.2% in 2) interactions are comparable.
We note that the shortest di + de distance for H···C contacts
is very similar in these structures and located around 2.8 Å.
The inter-H···S contacts are located beyond 3.0 Å,
which is longer than the sum of the vdW radii, and these contacts
may not have a significant role in stabilizing crystal structures.
It is observed that the H···Cl contacts influence the
crystal packing, and the relative contribution of this contact is
higher in compound 1 (12.5%) than in compound 2 (7.2%). The shortest di + de distance is located for this contact at 2.8 Å in
compound 2 and 3.0 Å in compound 1,
suggesting that the short H···Cl contact plays a significant
role in the stabilization of the crystal structure of compound 2.
Figure 4
2D-fingerprint plots for selected intercontacts were observed in
crystal structures of compounds 1 and 2.
The shape index diagram (on the last column) shows red and blue triangles
(dot circled) over the phenyl and triazole rings, indicating the presence
of π-stacking interaction in compound 2.
2D-fingerprint plots for selected intercontacts were observed in
crystal structures of compounds 1 and 2.
The shape index diagram (on the last column) shows red and blue triangles
(dot circled) over the phenyl and triazole rings, indicating the presence
of π-stacking interaction in compound 2.In contrast to the H···Cl contact,
the contribution
of H···F contact is higher in compound 2 (9.2%) than in compound 1 (3.3%). The shortest di + de distance
appears more extended than the sum of the vdW radii of H and F atoms
suggesting that the H···F contact plays a minor role
in stabilization. Additionally, the inter-C···C contacts,
which represent π-stacking interactions, contribute about 4.9%
to compound 2, and the corresponding contact contributes
only 0.3%, indicating its absence in the crystal structure of compound 1. The shape index plot shows the presence or absence of π-stacking
in compounds 2 and 1, respectively (Figure ).In addition
to the intermolecular interaction mentioned above,
the contribution of some inter-contacts is relatively less compared
to other contacts. For instance, F···C and F···N
contacts contribute each about 1.9% and a highly directional S···C(π)
chalcogen bond contributes only 2.0% to the crystal packing of compound 1 yet plays a significant role in stabilizing the crystal
structure.
Crystal Packing
Crystal Packing of Compound 1
In the solid state, the molecules of compound 1 are packed in a columnar way along the crystallographic ac plane (Figure a). CLP-PIXEL energy analysis revealed six dimers (D1–D6; Figure a–e) in the
crystal structure of compound 1, and the intermolecular
interaction energies for these dimers range from −12.7 to −3.8
kcal mol–1. These energies for most dimers are comparable
to those calculated by the density functional theory (DFT) method
with the B97D3/def2-TZVP level of approximation. As shown in Figure a, the primary structural
motif (dimer D3) is stabilized by an intermolecular C–H···C(π)
interaction between the adamantyl moiety and the phenyl ring. This
interaction links the neighboring molecules into a C(10) chain that
runs parallel to the crystallographic b axis (Figure S4). Furthermore, the D3 dimer is stabilized
with an 80% dispersion energy component. The most stable dimer D1
stabilizes with the three centered F1A···C8/N2 contacts.
The stabilization of dimer D1 is further supported by an intermolecular
C–H···N interaction, which makes a R22(18) motif. Furthermore,
the dispersion and electrostatic energy components contribute 59 and
41%, respectively, toward the stabilization of dimer D1. As shown
in Figure a, the primary
structural motifs in the adjacent columns are interconnected by dimeric
motif D1.
Figure 5
(a) Columnar arrangement of the molecule of compound 1 in the solid state; basic structural motifs are boxed (dimers D1
and D3). (b–e) Other molecular dimers (D2, D4, D5, and D6)
formed in the crystal structure of 1 by different non-covalent
interactions.
(a) Columnar arrangement of the molecule of compound 1 in the solid state; basic structural motifs are boxed (dimers D1
and D3). (b–e) Other molecular dimers (D2, D4, D5, and D6)
formed in the crystal structure of 1 by different non-covalent
interactions.The second most stable dimer D2 is formed by two
intermolecular
C–H···π interactions involving H atoms
of the adamantane and triazolothiadiazole core, with a dispersion
energy contribution of approximately 74% for stabilization. These
C–H···π interactions interconnect the
neighboring molecules into a chain which runs parallel to the crystallographic a axis (Figure S5). Dimer D4
is formed by a highly directional chalcogen bond of type C–S···C(π)
interaction, which links the adjacent molecules into a C(6) chain
that runs parallel to the crystallographic b axis
(Figure S6). The electrostatic (51%) and
dispersion (49%) energy components are nearly equal to the stabilization
of this dimer.Dimer D5 is stabilized by an intermolecular C–H···N
interaction, and this interaction links neighboring molecules into
a C(10) chain that runs parallel to the crystallographic b axis. Moreover, the electrostatic energy contributes about 65% toward
the stabilization of this dimer. The least stable cyclic dimer [D6;
R22(22) motif]
is formed by intermolecular C–H···Cl interactions.
The H···Cl contact distance is slightly longer (by
0.06 Å) than the sum of the vdW radii of H and Cl atoms and Cl
atoms. For stabilization, the dispersion energy contributes about
79%.In addition, different intermolecular interactions observed
in 1 are combined to form a supramolecular self-association
in
the solid state. The basic structural motif D3 and the dimeric motif
D5 combined to assemble a molecular ribbon that runs parallel to the b axis. Further, three molecules of 1 generate
a loop utilizing two D3 and a D5 motifs (Figure a). As shown in Figure b, two intermolecular C–H···N
interactions (dimers D1 and D5) and a weak C–H···Cl
(dimer D6) interaction collectively generate a supramolecular sheet.
The adjacent loops formed by this weak C–H···Cl
interaction interlinked by C–H···N interactions
in both the directions. As mentioned above, the chalcogen bonding
(dimer D4) interaction alone generates a molecular chain and forms
a molecular ribbon when the chalcogen bond is combined to C–H···N
interactions (dimer D5) and this molecular ribbon runs parallel to
the b axis (Figure S7).
Figure 6
Supramolecular
self-assembly built by (a) motifs D3 and D5 and
(b) motifs D1, D5, and D6.
Supramolecular
self-assembly built by (a) motifs D3 and D5 and
(b) motifs D1, D5, and D6.Furthermore, we calculated the MESP map for compound 1 to understand the molecule’s charge distribution
and gain
further insights into the observed intermolecular interactions in
the solid states (Figure ). On the MESP map, we can see that the protons of the di-substituted
phenyl ring had the most positive electrostatic potentials (Vs,max) compared to the H atoms of the adamantane
moiety. The most negative electrostatic potentials (Vs,min) are observed for atoms N4 (−45.9 kcal mol–1) and N3 (−45.8 kcal mol–1) of the triazole ring. Atoms H4A (Vs,max: 30.0 kcal mol–1) and H5A (Vs,max: 29.7 kcal mol–1) have participated
as donors for the intermolecular C–H···N interactions
with triazole N4 atoms having the most negative electrostatic potential.
The lone pair of F1A atom with a Vs,min value of −10.4 kcal mol–1 is likely to
make F···π contact (dimer D1) with the π-hole
over the surface of C8–N2 bond with a Vs,max value of 10.1 kcal mol–1. The MESP
map also reveals the σ–hole for the S atom with the positive
electrostatic potential at the tip of the C7– S1 bond with
a Vs,max value of 14.3 kcal mol–1 and this atom forms a directional chalcogen bond (C–S···π
type) with atom C4A(π). On the MESP map, we observed a negative
electrostatic potential with a Vs,min value
of 3.8 kcal mol–1 near the C4A atom. From the calculated
MESP map, we can also see the σ–hole for the Cl atom
with a Vs,max value of 15.2 kcal mol–1 at the tip of the C–Cl bond and the negative
belt around Cl atom corresponds to lone pairs. It is interesting to
note that there is no σ–hole interaction involving the
Cl atom. However, the lone pair of the Cl atom makes a weak C–H···Cl
hydrogen bond (dimer D6) with the H atom of the adamantane moiety.
Figure 7
MESPs
for the structure of compound 1 and the electron
density surface drawn at 0.001 au contour. Color scales (in kcal mol–1): red: >15; yellow: 15 to 0, green: 0 to −25;
and blue: >−25. The small hemispheres indicate the positive
(Vs,max; black) and negative (Vs,min; blue) electrostatic potentials for selected
atoms along with their values. The close-up view shows σ–holes
for the Cl atom and a characteristic negative belt.
MESPs
for the structure of compound 1 and the electron
density surface drawn at 0.001 au contour. Color scales (in kcal mol–1): red: >15; yellow: 15 to 0, green: 0 to −25;
and blue: >−25. The small hemispheres indicate the positive
(Vs,max; black) and negative (Vs,min; blue) electrostatic potentials for selected
atoms along with their values. The close-up view shows σ–holes
for the Cl atom and a characteristic negative belt.
Crystal Packing of Compound 2
In the solid state, the molecules of compound 2 are also columnar packed in the crystallographic bc plane, but somewhat different from the crystal packing of molecule 1 (Figure ). CLP-PIXEL energy analysis identifies four dimers (D1–D4)
with significant intermolecular interaction energies (Etot) observed in this structure (Table ). These energies range from −11.1
to −6.3 kcal mol–1. The energy values are
comparable to those calculated by the DFT method with the B97D3/def2-TZVP
level of theory. The basic structural motif (dimer D1) consists of
inversion-related molecules stabilized by π-stacking interactions
between phenyl and triazole rings (Figure a). The π-stacked dimer D1 is further
strengthened by weak lp···π (involving atoms
S1 and C14) and C–H···F interactions. The latter
hydrogen bond is established slightly longer than the sum of the vdW
radii of the H and F atoms and makes an R22(20) ring motif.
Figure 8
(a) Crystal packing of
compound 2 and its basic structural
motif (D1) is highlighted. (b–d) Molecular pairs (D2–D4)
of compound 2 held together by different types of non-covalent
interactions. (e) Formation of a supramolecular ribbon by alternate
dimers of D3 and D1. (f) Herringbone-like supramolecular architecture
built by alternate dimers of D3 and D2.
Table 2
Intermolecular Interaction Energies
(in kcal mol–1) for Different Dimers Observed in
the Crystal Structures of Compounds 1 and 2
PIXEL/MP2/6-31G**
dimer
CD
symmetry
important interactions
geometry H···A (Å), ∠D–H···A (°)a
ECoul
Epol
Edisp
Erep
Etot
ΔEcp/B97D3/def2-tzvp
compound 1 (major disordered component)
D1
5.897
–x + 1, –y + 1, –z + 1
C5–H5A···N4
2.74, 137
–6.4
–1.7
–11.6
7.0
–12.7
–12.8
F1A···C8
2.920 (1)
F1A···N2
2.939 (1)
D2
8.124
x – 1/2, –y + 3/2, z – 1/2
C19–H19B···Cg1
2.63, 151
–2.6
–1.5
–11.5
7.7
–7.9
–8.4
C17–H17···Cg2
2.84, 125
D3
8.708
–x + 1/2, y – 1/2, –z + 3/2
C13A–H13A···C1A(π)
2.89, 145
–1.6
–0.9
–10.0
6.0
–6.5
–8.0
D4
9.185
–x + 1/2, y – 1/2, –z + 1/2
C7–S1···C4A(π)
3.186 (1), 170.5 (1)
–4.3
–2.9
–6.9
8.4
–5.7
–6.7
D5
11.691
x, y – 1, z
C4A–H4A···N4
2.27, 161
–5.9
–2.3
–4.4
7.0
–5.7
–5.2
D6
7.605
–x, –y + 1, –z + 1
C12–H12···Cl1A
3.01, 133
–0.9
–0.3
–4.4
1.8
–3.8
–4.1
compound 2
D1
6.491
–x + 1, –y + 1, –z + 1
Cg1···Cg2
3.509 (1)
–4.8
–3.3
–19.1
16.1
–11.1
–13.5
S1(lp)···C14(π)
3.475 (1)
C15–H15···F1
2.67, 125
D2
8.039
–x + 1, –y + 1, –z + 2
C7–S1···N3
2.803 (1), 164.8 (1)
–18.5
–9.1
–8.1
26.4
–9.3
–10.4
N3···N3
2.886 (1)
D3
5.834
x, –y + 1/2, z + 1/2
C11–H11···Cl1
2.79, 152
–2.4
–1.7
–13.2
9.1
–8.4
–9.4
C2–Cl1···N1
3.223 (1), 170.0 (1)
C13–H13···Cg2
2.85, 145
D4
11.180
x – 1, y, z
C4–H4···N4
2.50, 128
–4.4
–1.6
–3.9
3.6
–6.3
–5.4
C5–H5···N4
2.74, 117
Neutron values are given for all
D–H···A interactions. CD: distance between geometrical
centers of molecules. In compound 1: Cg1: S1–C7–N1–N2–C8; Cg2: N2–C8–N3–N4–C9. In compound 2: Cg1: N2–C8–N3–N4–C9; Cg2: C10–C15; Cg3: C1–C6.
(a) Crystal packing of
compound 2 and its basic structural
motif (D1) is highlighted. (b–d) Molecular pairs (D2–D4)
of compound 2 held together by different types of non-covalent
interactions. (e) Formation of a supramolecular ribbon by alternate
dimers of D3 and D1. (f) Herringbone-like supramolecular architecture
built by alternate dimers of D3 and D2.Neutron values are given for all
D–H···A interactions. CD: distance between geometrical
centers of molecules. In compound 1: Cg1: S1–C7–N1–N2–C8; Cg2: N2–C8–N3–N4–C9. In compound 2: Cg1: N2–C8–N3–N4–C9; Cg2: C10–C15; Cg3: C1–C6.The second strong dimer (D2) is also formed between
inversion-related
molecules and stabilized by C7–S1···N3 chalcogen
bonds and further reinforced by a short N···N (triazole···triazole)
contact with a distance of 2.89 Å (Figure b). It is important to note that the electrostatic
energy contributes 77% toward stabilizing dimer D2. The NCI (non-covalent
interaction index) analysis was performed to visualize the nature
of the interactions formed in this dimer based on electron density
(ρ) and its reduced density gradient (s). The
NCI plot shows a strong attractive nature of a chalcogen bond compared
to the N···N contact formed in the same dimer. A similar
feature has been observed in the related structure reported in the
literature.[38]Dimer D3 stabilizes
with intermolecular C–H···π
interactions and three centered interactions. The Cl atom acts as
an acceptor for C–H···Cl interactions and as
a donor for a halogen bond of type C–Cl···N
interactions. For stabilization of this dimer, the dispersion energy
contributes about 76% (Figure c). The least stable dimer (D4) in this structure is stabilized
by the three-centered C–H···N interaction (R21(5)ring motif)
in which one of the triazole nitrogens (atom N4) acts as an acceptor
(Figure d). This interaction
links the molecules into a chain that runs parallel to the crystallographic a axis. The electrostatic energy contributes about 61% toward
the stabilization of this dimer. It is observed that the adjacent
dimers of D1 are interlinked by D3 dimer runs that alternately form
a molecular ribbon (Figure e). We also observed that adjacent dimers of D2 are interconnected
by dimer D3 that forms a herringbone-like supramolecular architecture
(Figure f).Furthermore, the deformation density map was calculated for dimers
D2 and D3 to visualize σ–hole interactions (chalcogen
and halogen bonds). Figure a shows the deformation density map displaying the charge
concentration region (blue) near the N3 atom and charge depletion
region (red) closer to the S1 atom. These features suggest the existence
of the S···N chalcogen bond in dimer D2 (Figure a). Similarly, the charge concentration
region is located near the N1 atom and the charge depletion region
around the Cl1 atom, suggesting the presence of a highly directional
Cl···N halogen bond (Figure b).
Figure 9
Deformation density maps for dimers (a) D2 and
(b) D3 in 2 reveal the chalcogen and halogen bonds, respectively.
(c)
MESPs for structure 2 and the electron density surface
drawn at 0.001 au contour. Color scales (in kcal mol–1): red: >15; yellow: 15 to 0, green: 0 to −25; and blue:
>−25.
The small hemispheres indicate the selected positive (Vs,max; black) and negative (Vs,min; blue) electrostatic potentials along with their values.
Deformation density maps for dimers (a) D2 and
(b) D3 in 2 reveal the chalcogen and halogen bonds, respectively.
(c)
MESPs for structure 2 and the electron density surface
drawn at 0.001 au contour. Color scales (in kcal mol–1): red: >15; yellow: 15 to 0, green: 0 to −25; and blue:
>−25.
The small hemispheres indicate the selected positive (Vs,max; black) and negative (Vs,min; blue) electrostatic potentials along with their values.To further understand the formed interactions in
compound 2, MESP map was computed. The MESP map of compound 2 shows that the most positive electrostatic potentials (Vs,max) are observed for protons of the di-substituted
phenyl ring, which are higher than H atoms of the phenyl ring. This
feature is very similar to that of compound 1. The H
atoms of the di-substituted phenyl ring act as donors for intermolecular
C–H···N interactions with atom N4 (Vs,min: −41.7 kcal mol–1). The
most positive electrostatic potential surface near atoms H4 (Vs,max: 31.3 kcal mol–1) and
H5 (Vs,max: 31.0 kcal mol–1). Complementary electrostatic potentials facilitate the formation
of C–H···N interactions. The MESP map also reveals
the σ–hole at the tip of the C–Cl bond with a Vs,max value of 15.8 kcal mol–1 and a characteristic negative belt around the Cl atom (Vs,min: −4.0 to −0.2 kcal mol–1). The Cl makes an attractive σ–hole halogen bond (C–Cl···N)
with the lone pair of N1 atom having a negative electrostatic potential
value of −9.4 kcal mol–1. As observed in 1, the S1 atom shows σ–hole (17.6 kcal mol–1) and makes an attractive chalcogen bond (C–S···N)
with atom N3 having the negative electrostatic potential value of
−43.0 kcal mol–1. Atom H11 with a positive
ESP value of 10.2 kcal mol–1 is likely to participate
in a weak intermolecular C–H···Cl hydrogen bond
with the negative belt of the Cl atom.
Topological Analysis of Intermolecular Interactions
in Compounds 1 and 2
The intermolecular
interactions observed in various dimers of compounds 1 and 2 were characterized using the topological properties.
The topological properties for the selected interactions in these
dimers are summarized in Table . The molecular graphs showing the intermolecular interactions
at the bond critical points in different dimers of compounds 1 and 2 are illustrated in Figures S8 and S9. The positive values of Laplacian of the
electron density (∇2ρ(r) > 0) and total
electronic
energy density (H(r) > 0) and |−V(r)/G(r)| < 1 indicate all the observed
intermolecular
interactions in compounds 1 and 2 are closed-shell
in nature. In compound 1, the dissociation energy values
(De) suggest that the C–H···N
(dimer D4) interaction is found to be more assertive with a value
of 2.9 kcal mol–1, compared to other interactions.
The next strongest interaction is the F···N contact
with a De value of 1.9 kcal mol–1. The chalcogen bond of type S···π showed a
similar strength with that of F···N contact. The other
two interactions, C–H···N (dimer D1) and C–H···Cl
(dimer D6) showed similar strength.
Table 3
Topological Parameters for Selected
Intermolecular Interactions in Different Dimers of Compounds 1 and 2a
interaction
Rij
ρ(r)
∇2ρ(r)
V(r)
G(r)
H(r)
|−V(r)/G(r)|
De
compound 1
D1
H5A···N4
2.779
0.040
0.475
–7.8
10.4
2.6
0.75
0.9
F1A···N2
3.345
0.056
0.979
–15.6
21.1
5.5
0.74
1.9
D4
S1···C4A
3.340
0.071
0.774
–15.2
18.2
2.9
0.84
1.8
D5
H4A···N4
2.283
0.106
1.279
–23.9
29.4
5.4
0.81
2.9
D6
H12···Cl1A
3.050
0.031
0.393
–6.0
8.4
2.3
0.72
0.7
compound 2
D2
S1···N3
2.808
0.132
1.525
–35.4
38.5
3.1
0.92
4.2
N3···N3
2.908
0.078
1.141
–22.5
26.8
4.3
0.84
2.7
D3
H11···Cl1
2.819
0.046
0.562
–9.2
12.3
3.0
0.75
1.1
Cl1···N1
3.231
0.050
0.696
–10.8
14.9
4.1
0.73
1.3
D4
H4···N4
2.548
0.069
0.825
–15.4
19.0
3.5
0.81
1.8
H5···N4
2.812
0.048
0.593
–10.4
13.3
2.9
0.78
1.2
Rij,
bond path (Å); ρ(r), electron density (e Å–3); ∇2ρ(r), Laplacian of electron density
(e Å–5); V(r), potential electron
density (kJ mol–1 br–3); G(r), kinetic electron density (kJ mol–1 br–3); H(r), total electronic
energy density (kJ mol–1 br–3);
and De, dissociation energy (kcal mol–1).
Rij,
bond path (Å); ρ(r), electron density (e Å–3); ∇2ρ(r), Laplacian of electron density
(e Å–5); V(r), potential electron
density (kJ mol–1 br–3); G(r), kinetic electron density (kJ mol–1 br–3); H(r), total electronic
energy density (kJ mol–1 br–3);
and De, dissociation energy (kcal mol–1).In compound 2, the chalcogen bond (S···N, De = 4.2 kcal mol–1) and N···N
contact (De = 2.7 kcal mol–1) in dimer D1 showed significant strength compared to other interactions.
The topological parameters for these contacts are comparable with
the same contacts observed in the triazolothiadiazole derivatives
reported earlier.[38] We also note that the
strength of Cl···N halogen bond (dimer D3) is comparable
with the strength of one of the C–H···N interactions
observed in dimer D4. As expected, the intermolecular C–H···Cl
bond is slightly weaker than C–H···N interactions.
In Vitro COX Inhibition Assay and Molecular
Docking Analysis
The synthesized compounds in this study
were subjected to evaluate the anti-inflammation potentials against
two important enzymes (COX-1 and COX-2) involved in the inflammatory
cell signaling pathway. The in vitro inhibitory activity of compounds 1 and 2 against these enzymes and the selectivity
index (SI) are summarized in Table . The inhibition concentration (IC50) values
for control drugs, namely, celecoxib (selective COX-2 inhibitor) and
diclofenac (non-selective COX inhibitor) are compared to assess the
activity of compounds 1 and 2. The in vitro
data reveals that the binding affinity of compound 2 is
nearly in 3-fold excess that of compound 1 toward the
COX-1 enzyme. In contrast, the binding affinity of compound 1 is in 2-fold excess that of compound 2 toward
the COX-2 enzyme. The assay results also indicate that molecule 1 with an adamantane moiety showed marked COX inhibitory activity
with 10-fold selectivity toward COX-2 (SI = 9.82) compared to molecule 2 with a phenyl ring in the place of adamantane cage. The
result reveals the effect of the substituents (adamantane and phenyl)
on the observed COX inhibition activity. Molecules containing 1,2,4-triazole
have been reported to exhibit anti-inflammatory potential, and in
our earlier reports we described the selective inhibitory potential
of 4-(4-chlorophenyl)-3-[(4-fluorobenzyl)sulfanyl]-5-(thiophen-2-yl)-4H-1,2,4-triazole with a COX-2 SI of 1.89.[35]
Table 4
In vitro COX-1 and COX-2 Inhibitory
Activity and COX-2 Selectivity Index of Compounds 1 and 2, Celecoxib, and Diclofenac
IC50 (μM)a
COX-1
COX-2
SIb
compound 1
26.12
2.66
9.82
compound 2
8.50
5.44
1.56
celecoxib
21.60
0.07
308.57
diclofenac
2.72
3.02
0.90
IC50 value is the compound
concentration required to produce 50% inhibition of COX-1 or COX-2
for means of three separate determinations.
SI (IC50 COX-1/IC50 COX-2).
IC50 value is the compound
concentration required to produce 50% inhibition of COX-1 or COX-2
for means of three separate determinations.SI (IC50 COX-1/IC50 COX-2).To corroborate in vitro data, we performed an in silico
molecular
docking analysis for the title compounds and two known drugs (diclofenac
and celecoxib) with COX-1/2 enzymes. The GOLD docking program offered
a better performing ChemPLP fitness score for pose prediction,[64] which can be used to assess the binding potential
of the compound, and a higher fitness score can be considered to be
a better docking pose at the active site. Table summarizes the ChemPLP fitness score for
compounds 1 and 2 and two known COX inhibitors.
The scores obtained agree well with the in vitro data. The relative
affinity (ΔGbind) of the COX-1/2-ligand
(title compounds) was obtained using the MM-GBSA calculation. From
ΔGbind values, one can observe that
compound 2 shows higher affinity toward COX-1 compared
to COX-2, whereas both compounds display nearly equal affinity toward
the COX-2 enzyme (Table ). Overall, the molecule with an adamantane moiety shows relatively
higher binding potential with the active site of the COX-2 compared
to COX-1, which is in good agreement with the in vitro data.
Table 5
ChemPLP Fitness Scoring Calculated
Using the GOLD Molecular Docking Program
COX-1
COX-2
ChemPLP score
MM-GBSA ΔGbind
ChemPLP score
MM-GBSA ΔGbind
compound 1
66.0
–53.8
65.4
–58.4
compound 2
60.3
–70.5
62.1
–59.8
celecoxib
80.0
65.4
diclofenac
51.4
63.4
To understand the nature of noncovalent interaction
formed between
title compounds and COX enzymes, we analyzed the docked complexes
(refined models using the MM-GBSA approach) using a PLIP Web server,
as mentioned in the experimental section. Compound 1 establishes
only hydrophobic interactions with the active site residues (Arg 120,
Leu 352, Leu 359, Trp 387, Tyr 385, and Leu 531) of COX-1 (Figure a). It is noted
that the di-substituted phenyl and adamantane moieties are involved
in the hydrophobic interactions. As can be seen in Figure b, there is a relatively higher
number of interactions (residues involved are as follows: Arg 120,
Tyr 355, Leu 359, Phe 381, leu 384, Tyr 385, Trp 387, Leu 531, and
Ala 527) established between compound 1 and the COX-2
enzyme compared to the corresponding COX-1 complex. This could a possible
reason for the higher selectivity of compound 2 toward
COX-2 enzymes.
Figure 10
Active site residues of COX-1 and COX-2 establish noncovalent
interactions
with compounds 1 [(a) COX-1 and (b) COX-2] and 2 [(c) COX-1 and (d) COX-2].
Active site residues of COX-1 and COX-2 establish noncovalent
interactions
with compounds 1 [(a) COX-1 and (b) COX-2] and 2 [(c) COX-1 and (d) COX-2].Compound 2 showed relatively higher
affinity compared
to compound 1 for COX-1 according to the calculation
of the MM-GBSA and the in vitro assay. It can be seen in Figure c, in addition
to the higher number of hydrophobic interactions, the T-shaped π-stacking
interaction between the di-substituted phenyl ring of 1 and a conserved Tyr 385 residue of COX-1 and a short F···O
contact (backbone O atoms of the backbone of Met 522 and Ile 523 are
involved). The unsubstituted phenyl ring also establishes hydrophobic
interactions with the key residues. In the COX-2-compound 2 complex, both di-substituted and unsubstituted phenyl rings participate
in hydrophobic interactions with the active site residues of COX-2
(Figure d). In addition,
a hydrogen bond (O–H···N) formed between the
central triazole ring and the Tyr 355 residue.
Conclusions
The present study demonstrated
the interplay of hydrogen, halogen,
and chalcogen bonding in addition to π-stacking interactions
in two compounds containing a [1,2,4]triazolo[3,4-b][1,3,4]thiadiazole scaffold with adamantane and phenyl substituents.
The X-ray structures and various theoretical tools were used to characterize
the noncovalent interactions. Molecular conformation is locked by
weak intramolecular C–H···N interactions in
both compounds and one of the N atoms of the thiadiazole ring was
involved as an acceptor. In related reported structures, the di-substituted
ring was coplanar with the central triazolothiadiazole ring. The potential
energy surface analysis revealed the preferred orientation of the
di-substituted phenyl ring, which is in good agreement with the X-ray
conformation of the investigated compounds. Through the crystal packing
of compounds 1 and 2 are very similar (columnar
packing mode), their basic structural motifs are different. The basic
structural motif observed in 1 is stabilized by C–H···C(π),
whereas the π-stacking interaction generates the basic structural
motif in compound 2. The solid-state structure of 1 was also stabilized by C–H···N, C–H···π,
and C–H···Cl hydrogen bonds and a directional
C–S···π chalcogen bond and unconventional
short F···C/N contacts. Similarly, the solid-state
structure of 2 was also stabilized by C–H···N,
C–H···π, and C–H···Cl
hydrogen bonds and directional attractive σ–hole interactions
such as the C–Cl···N halogen bond and C–S···N
chalcogen bond. In compound 2, S(lp) ···C(π)
and a short N···N contacts play a supporting role in
the stabilization of certain molecular dimers. The electrostatic potential
surface map and the deformation density map revealed the characteristic
features of σ–hole interactions. The contribution of
H···H/Cl/N contacts was significantly varied due to
the effect of phenyl/adamantane substituents, as evident from the
HS analysis. The topological analysis suggested that the C–H···N
interaction was found to be stronger in 1, whereas C–S···N
chalcogen bond was stronger in compound 2. In vitro assay
and in silico molecular coupling and subsequent calculation of MM-GBSA
free energy supported that the compound with an adamantane scaffold
was 10-fold more selective against the COX-2 enzyme compared to compound
1. This study identified that terminal groups (di-substituted and
phenyl/adamantane moieties) are important in establishing noncovalent
interactions with the active site residues of the COX-1/2 enzymes.
In the future, these groups could be altered to improve the affinity
and selectivity against these enzymes.
Materials and Methods
Chemicals and Instruments
Melting
points (°C, uncorrected) were measured in open glass capillaries
using a Stuart SMP30 electro-thermal melting point apparatus. NMR
spectra were obtained on a Bruker 400 Avance III at 400.20 MHz for 1H and 100.63 MHz for 13C using DMSO-d6 as a solvent. Electrospray ionization mass spectroscopy
(ESI-MS) was performed on an Agilent 6410 triple quad tandem mass
spectrometer at 4.0 kV for positive ions. All chemical and solvents
(HPLC grade) were purchased from commercial suppliers and were used
without further purification. Monitoring the reactions and checking
the purity of the final products were carried out by thin-layer chromatography
using silica gel pre-coated aluminum sheets (60 F254, Merck)
and visualization was done with ultraviolet light (UV) at 365 and
254 nm.
Synthesis and Crystallization
A mixture
of the corresponding 4-amino-5-substituted-4H-1,2,4-triazole-3-thiol
(C)[41,42] (5.0 mmol), 2-chloro-6-fluorobenzoic
acid (873 mg, 5.0 mmol), and phosphorous oxychloride (5 mL) was heated
under reflux with stirring for 2 hours. On cooling, the reaction mixture
was cautiously poured onto crushed ice (50 g) and the separated crude
products were filtered, washed with saturated sodium hydrogen carbonate
solution, and then with water, dried, and crystallized from EtOH/CHCl3 to yield target compounds 1 and 2.
Single-crystal X-ray diffraction data were collected for crystals
of compounds 1 and 2 at 160 (1) K on a Rigaku
OD SuperNova/Atlas area-detector diffractometer using Cu Kα
radiation (λ = 1.54184 Å) from a micro-focus X-ray source
and an Oxford Instruments Cryojet XL cooler. The selected suitable
single crystals were mounted using polybutene oil on a flexible loop
fixed on a goniometer head and immediately transferred to the diffractometer.
Pre-experiment, data collection, data reduction, and analytical absorption
correction[65] were performed with the program
suite CrysAlisPro, version 1.171.40.68a (Rigaku Oxford Diffraction,
England, 2019). Using Olex2,[66] the structure
was solved with the SHELXT[67] small-molecule
structure solution program, and it was refined with the SHELXL2018/3
program package[68] by full-matrix least-squares
minimization on F2. In compound 1, the substituted benzene was disordered over two sets of
positions (labeled A and B) with site-occupancy factors of 0.7764(19)
and 0.2236(19). All H atoms were placed in calculated positions (C–H
= 0.95–0.99 Å) and were constrained to ride on their parent
atoms, with Uiso(H) = 1.2Ueq(C). The PLATON program was used to check the results
of the X-ray analysis.[69] Crystal packing
and molecular dimers were produced using the MERCURY program.[70]
Theoretical Calculations
For all
calculations, we used the crystal structure geometry with the normalized
H positions (C–H = 1.083 Å). Energy framework analysis[71,72] was performed on the CrystalExplorer-17.5 program[73] using the B3LYP/6-31G(d,p) level of approximation. The
HS[74] and 2D-FP plots[75] were obtained from the CrystalExplorer-17.5 program. The
deformation density was calculated for selected dimers at the HF/6-311G
level using the CrystalExplorer program. We calculated the intermolecular
interaction energies (Etot) between molecular
pairs using the CLP-PIXEL program.[76,77] For this computation,
the electron density was obtained with the Gaussian 09 program[78] using MP2/6-31G** levels of theory. Furthermore,
the accurate complexation energies of molecular pairs identified from
the CLP-PIXEL energy calculation were calculated using the B97D3/def2-TZVP
level of theory, and then, these complexation energies were corrected
(ΔEcp) for the basis set superposition
error using the counterpoise method.[79] The
topological analysis of the selected dimers was performed within the
framework of Bader’s QTAIM approach using the AIMALL program.[80] The wave functions were calculated at the M062X-D3/def2-TZVP
level of theory for topological analysis. The NCIplot index was also
used to characterize the nature of noncovalent interactions.[81] The MESP surfaces have been constructed using
the 0.001 a.u. isosurface with the program WFA-SAS.[82]
In Vitro COX Inhibition Assay
The
in vitro inhibitory activity of compounds 1 and 2 against cyclooxygenases COX-1 and COX-2 was evaluated using
an enzyme immunoassay kit of Cayman Chemical, Ann Arbor, MI, USA (catalog
no. 560131). The preparation of the reagents and the testing procedure
was performed according to the manufacturer recommendations using
various concentrations (0.01–100 μM) of compounds 1 and 2, celecoxib (selective COX-2 inhibitor),
and diclofenac (nonselective COX inhibitor) in dimethylsulfoxide (DMSO).
The concentration that causes 50% enzyme inhibition (IC50) was calculated from the concentration inhibition response curve
and the SI was calculated by dividing IC50 COX-1 by IC50 COX-2.
Molecular Docking and Protein–Ligand
Interaction Analysis
Docking studies were performed for compounds 1 and 2 and two control inhibitors, namely, celecoxib
and diclofenac, using GOLD software.[64] Crystallographic
structures of COX-1 (PDB ID: 3KK6; Ovis aries cyclooxygenase-1
complexed with celecoxib) and COX-2 (PDB ID: 5IKR; human cyclooxygenase-2
complexed with mefenamic acid) were obtained from Protein Data Bank
(www.rcsb.org). Prior to docking
simulations, the water molecules and cocrystallized ligands except
celecoxib and mefenamic acid inhibitors were removed. All protein
atoms within 6.0 Å of celecoxib and mefenamic acid inhibitors
were used for the binding site definition.The highest scoring
poses (ChemPLP) of compounds 1 and 2 were
also subjected to the MM-GBSA method to calculate the free energy
(ΔGbind) of the binding of ligands
to target proteins using the Schrödinger suite (Schrodinger
Release 2022-2, Schrödinger, LLC, New York, NY, 2021). In this
calculation, the title compounds and active residues within 6 Å
from the ligands were treated to be flexible and the remaining protein
residues were kept frozen. Protein–ligand interactions for
the docked complexes were analyzed using the PLIP Web server (protein–ligand
interaction profiler).[83]
Authors: Muharrem Dinçer; Namik Ozdemir; Ahmet Cetin; Ahmet Cansiz; Orhan Büyükgüngör Journal: Acta Crystallogr C Date: 2005-10-27 Impact factor: 1.172
Authors: Lamya H Al-Wahaibi; Bavanandan Rahul; Ahmed A B Mohamed; Mohammed S M Abdelbaky; Santiago Garcia-Granda; Ali A El-Emam; M Judith Percino; Subbiah Thamotharan Journal: ACS Omega Date: 2021-03-03