M Govindammal1, S Kannan2, P Srinivasan3, M Prasath1. 1. Department of Physics, Periyar University Centre for Post Graduate and Research Studies, Dharmapuri, 635 205, India. 2. Centre for High Computing, CSIR-Central Leather Research Institute (CLRI), Chennai, 600020, India. 3. Chikkaiah Naicker College, Erode, 638004, India.
Abstract
Quercitrin is an anti-lung cancer agent. It is a naturally occurring flavonoid and its derivatives are mainly present in nuts and beverages. It is mainly available as a glycoside, and the quercitrin glycosides are found to prevent the metastasis of cancer. Quercitrin is optimized with 6-311++G(d,p) basis set using the B3LYP method to attain its minimum energy structure. The vibrational studies of the Quercitrin compound were elucidated with reference to Potential Energy Distribution (PED). The geometrical parameters were obtained and correlated with experimental values. To examine the nature of the charge transfer mechanism of Quercitrin, the HOMO-LUMO energy gap is computed. The anti-cancer activity of Quercitrin has been explored using molecular docking study that are used to estimate how the ligand interacts with protein, specifically to identify the best-fit orientation of the ligand, its binding mode, and intermolecular interactions of amino acid residues in the binding region of B-RAF kinase protein. The binding affinity of the compound Quercitrin (-7.14 kcal/mol) was found using AutoDock and validated with a Glide XP score in Schrodinger tool (-8.01 kcal/mol). MD simulations of protein-ligand complexes were monitored for 100 ns, from which the RMSD, RMSF, Rg, H-bonds, and interaction energy calculations were executed. From these investigations, it is identified that the compound quercitrin has maintained good structural stability, compactness, higher Hydrogen bonds, and interaction energies than the Imidazopyridinyl benzamide inhibitor.
Quercitrin is an anti-lung cancer agent. It is a naturally occurring flavonoid and its derivatives are mainly present in nuts and beverages. It is mainly available as a glycoside, and the quercitrin glycosides are found to prevent the metastasis of cancer. Quercitrin is optimized with 6-311++G(d,p) basis set using the B3LYP method to attain its minimum energy structure. The vibrational studies of the Quercitrin compound were elucidated with reference to Potential Energy Distribution (PED). The geometrical parameters were obtained and correlated with experimental values. To examine the nature of the charge transfer mechanism of Quercitrin, the HOMO-LUMO energy gap is computed. The anti-cancer activity of Quercitrin has been explored using molecular docking study that are used to estimate how the ligand interacts with protein, specifically to identify the best-fit orientation of the ligand, its binding mode, and intermolecular interactions of amino acid residues in the binding region of B-RAF kinase protein. The binding affinity of the compound Quercitrin (-7.14 kcal/mol) was found using AutoDock and validated with a Glide XP score in Schrodinger tool (-8.01 kcal/mol). MD simulations of protein-ligand complexes were monitored for 100 ns, from which the RMSD, RMSF, Rg, H-bonds, and interaction energy calculations were executed. From these investigations, it is identified that the compound quercitrin has maintained good structural stability, compactness, higher Hydrogen bonds, and interaction energies than the Imidazopyridinyl benzamide inhibitor.
Lung cancer is the crucial reason for morbidity and mortality worldwide in both sexes and is most widely recognized as a reason for malignancy-related deaths [1]. Non-Small Cell Lung cancer (NSCLC) is a highly aggressive and recurrent kind of lung cancer. Globally, NSCLC is considered responsible for about 85% of all lung cancers [2]. B-RAF is a kinase protein and a member of the RAF family of Ser/Thr kinase family which is highly downstream of the Ras/Raf/MEK/ERK signaling pathway [3, 4]. B-RAF mutations have been found in 3–4% of NSCLC [5]. If the MEK/ERK signaling pathway is activated in human cancer, B-RAF kinases are supposed to be a prominent therapeutic target. B-RAF is involved in complex activity such as phosphorylation/dephosphorylation process resulting in kinase activation/deactivation [6, 7].Quercitrin is an active natural bioflavonoid, a plant derivative that mostly appears in the glycoside structure [8]. The bounded sugar moiety in the Quercitrin compound makes the Quercitrin aglycone soluble and improves the absorption and bioavailability. Quercitrin exhibits anti-cancer properties against NSCLC. It is reported to inhibit quercitrin–induced apoptosis in the NSCLC cell line A549 with an IC50 value of 50 μm [9]. Quercitrin displays an anti-oxidant property and has become the focus point for revealing the anti-cancer activity [10]. Vibrational spectroscopic studies have been carried out to recognize and examine the chemical bonding and intramolecular bonds of quercitrin. The vibrational analysis of Quercitrin was discovered using quantum chemical calculations using the DFT approach. The theoretical findings match up with the experimental results. The most reactive area of the Quercitrin is illustrated using the molecular electrostatic potential map (MEP). The chemical reactivity of quercitrin is determined by the Fukui function. The bio-availability compound was scrutinized with ADMET prediction analysis along with Lipinski's rule of five. A molecular docking evaluation was employed to explore the intermolecular interactions of quercitrin in the binding site of the B-RAF kinase protein. The analyses, such as HOMO-LUMO, MEP, and ADMET predictions, are utilized to find the anti-cancer behavior of Quercitrin against NSCLC.
Materials and methods
Experimental methods
Quercitrin was procured in solid form with a purity of ≥95% and no further purification of the compound has been made for spectral studies. The PERKIN ELMER (4000-400 cm−1) spectrometer with the KBr pellet technique was used to obtain the FT-IR spectrum of Quercitrin. Additionally, the FT-Raman spectrum was accomplished for Quercitrin in the region of 4000–100 cm−1 with a resolution of 2 cm−1 employing Brucker RFS 27- Nd: YAG laser source of 1064 nm at SAIF-IITM.
Computational methods
The Quercitrin compound was optimized using the DFT method employing the B3LYP level of theory by Gaussian09 software [11]. The geometrical parameters of the optimized geometry were generated using the Gaussview 0.5 software package [12]. The VEDA 4xx program package [13] was used to obtain the Potential Energy Distribution percentage (PED %) and fundamental vibrational assignments of Quercitrin. The biological properties of the ADME assessment of the compound were obtained using an online tool, the Molinspiration Cheminformatics server. The ligand (Quercitrin) and protein (B-RAF kinase) were docked with the aid of Autodock 4.2 [14]. The structural and interaction patterns of the protein-ligand complex are visualized and generated using the PyMol [15], Chimera [16], and Ligplot [17] software packages. The genetic algorithm and Lamarckian GA were employed to search for the appropriate conformers and for binding affinity. The number of points in the X, Y and Z dimensions are 24, 26, and 24 respectively. The center grid box in the X, Y and Z centres are -23.905, 5.081, and -6.037 respectively. The total grid points per map are 16875, with a spacing of 1 Å. The docking conformations are generated in AutoDock Vina, and those conformations are graded on the basis of binding free energy, by applying Eq. (1),where ΔGbind represents the binding free energy, ΔGvdw the van der Waals interaction, ΔGdesolv the desolvation effect, ΔGHbond the hydrogen bonding interaction, ΔGele the electrostatic interaction, ΔGinternal the internal energy, ΔGtorsion and ΔGunbound represents the torsional free energy, and unbound systems energy respectively.The AutoDock results were further validated with the Extra Precision Glide XP score in Maestro, the Schrodinger suite [18]. The molecular dynamics (MD) simulation of docked structures of protein-ligand complexes was carried out for a 100 ns time period using the GROMACS program, version 2019.5 [19]. With the SPC216 (simple point charge) water model, the molecular system was solvated in a cubic box [20]. Amber 99SB force field was executed and the system was examined at the same temperature of 300 K over a 100 ns period of time. The PBC (periodic boundary condition) was applied to the system and the ligand topology parameters were generated using the ACPYPE server [21]. The system was energy minimized and the position restrained MD was carried out for 1000 ps using NVT and NPT ensembles with the Parrinello-Rahman pressure coupling [22]. The RMSD, RMSF, radius of gyration and interaction energy were analyzed using the GROMACS program.
Results and discussion
Structural aspects
The Quercitrin structure was drawn utilizing the Chemdraw8.0 tool [23] and optimized with the DFT method to get the energy minimized structures using the B3LYP levels of theory [24, 25]. The Optimized geometrical parameters of the Quercitrin compound were generated using Gaussian 09 and GaussView5.0 as shown in Figure 1. With the crystal structure of Quercitrin not yet known, we have calculated the theoretical predictions on structural parameters of Quercitrin with available X-ray diffraction data [26] and the results are presented in Table 1. The Quercitrin's threshold converged at the limits of its maximum force value of 0.000010 (a.u) and displacement value of 0.000878 (a.u). The dipole moment value of the compound is found to be 8.2324 Debye. The quercitrin contains twelve C–H, twenty C–C, fifteen C–O, and eight O–H bonds. The C–C bond lengths of the phenol ring range from 1.359 to 1.369 Å. The ketone groups in Quercitrin have bond lengths of C(2)–O(12)→1.376/1.384∗Å, C(3)–O(11)→1.218/1.266∗Å, C(9)–O(10)→1.363/1.373∗Å, and O(1)–O(10)→1.366/1.373∗ (∗ denotes the Observed value). The highest bond length value, found in Quercitrin is C(16)–C(17) with 1.542 Å due to a double bond. The ketone group exhibits the bond angle of C(2)–C(1)–O(10) and the value is found to be 119.9/120.5°∗.
Figure 1
The scaled ball and stick model of optimized structure of Quercitrin molecule with atoms numbering scheme.
Table 1
Bond lengths and bond angles of quercitrin molecule compared with XRD data.
Bond Length (Å)
Calculated
Expa
Bond Angle (o)
Calculated
Expa
C(1)-C(2)
1.359
1.369
C(2)-C(1)-O(10)
119.9
120.5
C(1)-O(10)
1.366
1.373
C(2)-C(1)-C(25)
128.9
127.8
C(1)-C(25)
1.473
1.468
O(10)-C(1)-C(25)
111.1
111.6
C(2)-C(3)
1.480
1.445
C(1)-C(2)-C(3)
122.9
120.9
C(2)-O(12)
1.376
1.384
C(1)-C(2)-O(12)
121.1
122.1
C(3)-C(4)
1.479
1.433
C(3)-C(2)-O(12)
115.8
116.7
C(3)-O(11)
1.218
1.266
C(2)-C(3)-C(4)
113.7
116.2
C(4)-C(5)
1.419
1.429
C(2)-C(3)-O(11)
121.5
121.6
C(4)-C(9)
1.404
1.402
C(4)-C(3)-O(11)
124.8
122.2
C(5)-C(6)
1.393
1.359
C(3)-C(4)-C(5)
123.9
122.4
C(5)-O(24)
1.351
1.359
C(3)-C(4)-C(9)
119.6
120.6
C(6)-C(7)
1.400
1.399
C(5)-C(4)-C(9)
116.5
116.9
C(6)-H(33)
1.087
1.393
C(4)-C(5)-C(6)
120.6
120.9
C(7)-C(8)
1.387
-
C(4)-C(5)-O(24)
118.5
118.8
C(7)-O(23)
1.361
1.347
C(6)-C(5)-O(25)
120.8
120.3
C(8)-C(9)
1.392
1.373
C(5)-C(6)-C(7)
120.5
119.9
C(8)-H(34)
1.081
-
C(5)-C(6)-H(33)
119.5
-
C(9)-O(10)
1.363
1.373
C(7)-C(6)-H(33)
120.0
-
O(12)-C(14)
1.410
1.442
C(6)-C(7)-C(8)
120.5
121.2
O(12)-H(50)
2.289
-
C(6)-C(7)-O(23)
122.0
116.2
O(13)-C(14)
1.420
1.398
C(8)-C(7)-O(23)
117.5
122.5
O(13)-C(18)
1.440
1.442
C(7)-C(8)-C(9)
118.2
118
C(14)-C(15)
1.535
1.517
C(7)-C(8)-H(34)
121.0
-
C(14)-H(35)
1.098
-
C(9)-C(8)-H(34)
120.8
-
C(15)-C(16)
1.536
1.534
C(4)-C(9)-C(8)
123.7
123
C(15)-O(22)
1.415
1.422
C(4)-C(9)-O(10)
121.5
121.7
C(15)-H(36)
1.092
-
C(8)-C(9)-O(10)
114.8
117.4
C(16)-C(17)
1.542
1.513
C(1)-O(10)-C(9)
122.0
C(16)-O(21)
1.440
1.416
C(2)-O(12)-C(14)
117.2
116.1
C(16)-H(37)
1.095
-
C(14)-O(13)-C(18)
115.5
116.3
C(17)-C(18)
1.536
1.542
O(12)-C(14)-O(13)
107.9
112.3
C(17)-O(20)
1.425
1.426
O(12)-C(14)-C(15)
106.1
105.3
C(17)-H(38)
1.095
-
O(12)-C(14)-H(35)
109.9
-
C(18)-C(19)
1.529
1.511
O(13)-C(14)-C(15)
111.3
112.9
C(18)-H(39)
1.093
-
O(13)-C(14)-H(35)
110.1
-
C(19)-H(40)
1.094
-
C(15)-C(14)-H(35)
111.4
-
C(19)-H(41)
1.089
-
C(14)-C(15)-C(16)
111.2
109.4
C(19)-H(42)
1.093
-
C(14)-C(15)-O(22)
112.1
107.7
O(20)-H(43)
0.967
-
C(14)-C(15)-H(36)
106.2
-
O(21)-H(44)
0.961
-
C(16)-C(15)-O(22)
110.6
110.6
O(22)-H(45)
0.967
-
C(16)-C(15)-H(36)
109.3
-
O(23)-H(46)
0.963
-
O(22)-C(15)-H(36)
107.2
-
O(24)-H(47)
0.963
C(15)-C(16)-C(17)
111.8
110.0
C(25)-C(26)
1.409
1.396
C(15)-C(16)-O(21)
106.0
113.2
C(25)-C(30)
1.404
1.398
C(15)-C(16)-H(37)
108.2
-
C(26)-C(27)
1.382
1.380
C(17)-C(16)-O(21)
112.4
107.8
C(26)-H(48)
1.083
-
C(17)-C(16)-H(37)
108.5
-
C(27)-C(28)
1.404
1.401
O(21)-C(16)-H(37)
109.9
-
C(27)-O(32)
1.378
1.358
C(16)-C(17)-C(18)
112.1
112.3
C(28)-C(29)
1.390
-
C(16)-C(17)-O(20)
108.8
110.6
C(28)-O(31)
1.358
1.359
C(16)-C(17)-H(38)
109.4
-
C(29)-O(30)
1.391
-
C(18)-C(17)-O(20)
109.6
109.9
C(29)-H(49)
1.083
-
C(18)-C(17)-H(38)
110.3
-
O(30)-H(50)
1.079
-
O(20)-C(17)-H(38)
106.5
-
O(31)-H(51)
0.966
-
O(13)-C(18)-C(17)
107.1
111.3
O(13)-C(18)-C(19)
113.7
106.5
O(13)-C(18)-H(39)
103.1
-
C(17)-C(18)-C(19)
116.9
111.6
C(17)-C(18)-H(39)
106.5
-
C(19)-C(18)-H(39)
108.4
-
C(18)-C(19)-H(40)
109.3
-
C(18)-C(19)-H(41)
113.1
-
C(18)-C(19)-H(42)
109.2
-
H(40)-C(19)-H(41)
107.7
-
H(40)-C(19)-H(42)
108.0
-
H(41)-C(19)-H(42)
109.4
-
C(17)-O(20)-H(43)
106.9
-
C(16)-O(21)-H(44)
108.9
-
C(15)-O(22)-H(45)
105.7
-
C(7)-O(23)-H(46)
109.6
-
C(5)-O(24)-H(47)
108.8
-
C(1)-C(25)-C(26)
118.9
119.4
C(1)-C(25)-C(30)
122.6
121.5
C(26)-C(25)-C(30)
118.4
118.4
C(25)-C(26)-C(27)
120.6
121.3
C(25)-C(26)-H(48)
119.8
-
C(27)-C(26)-C(28)
119.6
-
C(26)-C(27)-C(28)
120.7
119.5
C(26)-C(27)-O(32)
124.5
118.5
C(28)-C(27)-O(32)
114.8
122.3
C(27)-C(28)-C(29)
118.9
119.5
C(27)-C(28)-O(31)
120.6
114.9
C(29)-C(28)-O(31)
120.5
125.4
C(28)-C(29)-C(30)
120.8
125.4
C(28)-C(29)-H(49)
118.6
-
C(30)-C(29)-H(49)
120.6
-
C(25)-C(30)-C(29)
120.5
120.7
C(25)-C(30)-H(50)
120.4
-
C(29)-C(30)-H(50)
119.0
-
C(28)-O(31)-H(51)
107.8
-
C(27)-O(32)-H(52)
110.0
-
aExperimental values taken from ref [26].
The scaled ball and stick model of optimized structure of Quercitrin molecule with atoms numbering scheme.Bond lengths and bond angles of quercitrin molecule compared with XRD data.aExperimental values taken from ref [26].
Vibrational assignments
The Quercitrin, which is found to be more stable, pertains to C1 point symmetry. The DFT method is used to estimate the vibrational spectroscopic studies with a basis set of 6–311++G(d, p), which has a scaling factor of 0.961 and its PED % is calculated [27]. Table 2 illustrates the theoretical and experimental vibrational variables of the quercitrin. The FT-IR and FT-Raman spectra of Quercitrin are shown in Figures 2 and 3, respectively.
Table 2
The experimental (FT-IR and FT-Raman) and theoretical vibrational frequencies using DFT for quercitrin.
Species
Experimental Wavenumbers(cm−1)
Theoretical wave number (cm−1)
Vibrational assignments
FT-IR
FT-RAMAN
Unscaled
scaled
IR intensities
RAMAN Activities
Rel
Abs
Rel
Abs
W(150)
3853
3703
55
13
119
14
OH stretching (92)
W(149)
3850
3700
68
16
97
12
OH stretching (100)
W(148)
3834
3684
94
22
199
24
OH stretching (92)
W(147)
3817
3668
58
14
187
22
OH stretching (100)
W(146)
3783
3636
146
34
181
22
OH stretching (100)
W(145)
3611
3764
3617
77
18
12
1
OH stretching (100)
W(144)
3763
3616
30
7
53
6
OH stretching (100)
W(143)
3122
3242
3115
8
2
37
4
CH stretching (99)
W(142)
3078
3221
3095
0
0
72
9
CH stretching (100)
W(141)
3194
3069
5
1
138
17
CH stretching (99)
W(140)
3185
3061
6
1
30
4
CH stretching (97)
W(139)
3143
3021
11
3
16
2
CH stretching (98)
W(138)
3139
3017
19
5
189
23
CH stretching (98)
W(137)
3097
2976
30
7
78
9
CH stretching (93)
W(136)
3086
2966
12
3
61
7
CH stretching (92)
W(135)
3064
2945
24
6
136
16
CH stretching (98)
W(134)
3046
2927
49
12
244
29
CH stretching (94)
W(133)
3039
2921
44
10
93
11
CH stretching (95)
W(132)
3036
2917
3
1
60
7
CH stretching (84)
W(131)
2816
3003
2886
21
5
26
3
CH stretching (97)
W(130)
1641
1660
1733
1665
324
76
145
17
OC stretching (85)
W(129)
1602
1604
1665
1600
424
100
239
29
CC stretching (62)
W(128)
1657
1593
31
7
29
3
CC stretching (47)
W(127)
1653
1588
129
31
787
94
CC stretching (26)
W(126)
1557
1635
1571
194
46
165
20
CC stretching (30)
W(125)
1517
1546
1617
1554
54
13
836
100
CC stretching (22)
W(124)
1558
1497
167
39
13
2
CC stretching (42)
W(123)
1536
1476
23
6
23
3
CC stretching (38)
W(122)
1445
1438
1512
1453
5
1
5
1
CC stretching (26)
W(121)
1494
1436
7
2
10
1
CC stretching (21)
W(120)
1419
1481
1423
248
58
14
2
CC stretching (41)
W(119)
1402
1469
1412
68
16
8
1
CC stretching (32)
W(118)
1387
1448
1392
67
16
15
2
OC stretching (10)
W(117)
1431
1375
46
11
24
3
OC stretching (56)
W(116)
1368
1428
1372
35
8
9
1
OC stretching (10)
W(115)
1417
1362
30
7
184
22
OC stretching (22)
W(114)
1415
1359
12
3
50
6
OC stretching (10)
W(113)
1412
1357
27
6
29
3
CC bending (20)
W(112)
1406
1351
16
4
48
6
OC stretching (30)
W(111)
1395
1341
5
1
2
0
OC stretching (10)
W(110)
1385
1331
21
5
81
10
CC stretching (10)
W(109)
1322
1382
1328
29
7
4
0
OC stretching (20)
W(108)
1315
1372
1318
31
7
12
1
OC stretching (52)
W(107)
1362
1309
349
82
257
31
OC stretching (36)
W(106)
1354
1301
4
1
16
2
OC stretching (66)
W(105)
1334
1282
24
6
28
3
CC stretching (22)
W(104)
1318
1267
90
21
46
6
CC stretching (13)
W(103)
1256
1316
1265
20
5
24
3
OC stretching (14)
W(102)
1300
1249
348
82
10
1
CC stretching (32)
W(101)
1293
1243
14
3
6
1
CC stretching (22)
W(100)
1274
1225
33
8
7
1
OC stretching (49)
W(99)
1273
1223
42
10
12
1
CCC bending (10)
W(98)
1205
1217
1267
1217
36
8
3
0
CCC bending (28)
W(97)
1243
1195
50
12
26
3
CCC bending (12)
W(96)
1175
1225
1177
111
26
113
14
CCO bending (11)
W(95)
1218
1170
318
75
26
3
HOC bending (56)
W(94)
1214
1166
33
8
2
0
HOC bending (63)
W(93)
1158
1205
1158
8
2
16
2
HOC bending (57)
W(92)
1199
1152
232
55
7
1
HOC bending (46)
W(91)
1182
1136
168
40
33
4
HOC bending (54)
W(90)
1172
1126
194
46
0
0
HOC bending (45)
W(89)
1120
1110
1168
1123
132
31
7
1
HOC bending (49)
W(88)
1136
1092
96
23
3
0
HCC bending (48)
W(87)
1134
1089
34
8
4
0
HCC bending (40)
W(86)
1129
1085
56
13
2
0
HCC bending (57)
W(85)
1067
1113
1070
114
27
3
0
HCC bending (33)
W(84)
1104
1061
116
27
10
1
HCC bending (23)
W(83)
1098
1056
17
4
4
0
HCO bending (69)
W(82)
1082
1039
91
21
3
0
HCO bending (23)
W(81)
1071
1029
61
14
2
0
HCO bending (40)
W(80)
1066
1025
138
32
5
1
HCC bending (44)
W(79)
1004
991
1046
1005
132
31
7
1
HCC bending (60)
W(78)
1028
988
18
4
10
1
HCH bending (59)
W(77)
970
1014
975
16
4
6
1
HCH bending (62)
W(76)
1009
969
105
25
5
1
HCH bending (59)
W(75)
997
958
44
10
14
2
OCC bending (15)
W(74)
940
982
943
15
3
1
0
CCO bending (22)
W(73)
930
894
45
11
7
1
CCC bending (25)
W(72)
865
918
882
15
4
5
1
CCO bending (13)
W(71)
894
859
15
4
3
0
CCC bending (12)
W(70)
832
867
833
50
12
1
0
CCC bending (20)
W(69)
850
817
14
3
7
1
CCC bending (16)
W(68)
807
843
810
4
1
2
0
CCO bending (14)
W(67)
824
792
6
1
6
1
CCC bending (16)
W(66)
787
785
819
787
3
1
9
1
OCC bending (37)
W(65)
774
808
777
34
8
2
0
OCC bending (44)
W(64)
798
767
35
8
28
3
COC bending (11)
W(63)
790
759
3
1
8
1
OCC bending (42)
W(62)
722
755
726
47
11
1
0
OCC bending (37)
W(61)
732
704
5
1
6
1
CCC bending (14)
W(60)
682
712
685
3
1
3
0
OCC bending (11)
W(59)
705
678
2
0
3
0
OCC bending (38)
W(58)
691
664
4
1
5
1
COC bending (15)
W(57)
673
647
4
1
4
0
OCC bending (18)
W(56)
624
638
666
640
42
10
2
0
OCO bending (20)
W(55)
639
614
13
3
5
1
OCC bending (12)
W(54)
602
633
608
6
2
7
1
OCC bending (51)
W(53)
592
619
595
8
2
1
0
OCC bending (10)
W(52)
606
582
17
4
15
2
OCC bending (20)
W(51)
572
596
573
17
4
2
0
OCC bending (40)
W(50)
586
563
2
0
6
1
OCC bending (35)
W(49)
573
551
22
5
9
1
HOCC torsion (58)
W(48)
571
548
8
2
2
0
HOCC torsion (78)
W(47)
526
549
528
3
1
2
0
HOCC torsion (75)
W(46)
534
513
7
2
1
0
HOCC torsion (89)
W(45)
487
516
496
28
7
18
2
HOCC torsion (78)
W(44)
503
483
79
19
2
0
HOCC torsion (88)
W(43)
490
471
102
24
2
0
HOCC torsion (83)
W(42)
490
471
23
5
1
0
HCCC torsion (75)
W(41)
469
450
51
12
4
0
HCCC torsion (67)
W(40)
468
450
20
5
2
0
HCCC torsion (74)
W(39)
466
448
19
5
1
0
HCCC torsion (79)
W(38)
448
430
28
7
1
0
HCCC torsion (82)
W(37)
430
413
6
2
2
0
HCOC torsion (33)
W(36)
409
393
42
10
2
0
HCOC torsion (28)
W(35)
403
388
15
4
3
0
HCCC torsion (50)
W(34)
391
376
17
4
5
1
HCCC torsion (43)
W(33)
373
359
27
6
2
0
HCCC torsion (49)
W(32)
359
345
15
4
3
0
CCCC torsion (36)
W(31)
345
332
4
1
1
0
CCCO torsion (36)
W(30)
343
330
108
25
4
0
CCCC torsion (51)
W(29)
337
324
11
3
0
0
CCOC torsion (52)
W(28)
324
312
2
0
1
0
CCCC torsion (29)
W(27)
312
300
3
1
0
0
CCCC torsion (37)
W(26)
301
289
11
3
1
0
CCCC torsion (37)
W(25)
296
285
1
0
3
0
COCC torsion (44)
W(24)
267
257
18
4
2
0
OCCC torsion (63)
W(23)
267
256
19
5
0
0
COCC torsion (58)
W(22)
256
246
25
6
3
0
OCOC torsion (81)
W(21)
250
241
16
4
1
0
COCO torsion (50)
W(20)
239
230
0
0
0
0
CCCO torsion
W(19)
233
224
6
1
1
0
CCOC torsion (14)
W(18)
221
213
21
5
2
0
CCCH out (67)
W(17)
219
210
31
7
4
0
CCCH out (31)
W(16)
217
208
71
17
2
0
CCCH out (26)
W(15)
205
197
14
3
2
0
OCCC out (43)
W(14)
199
192
4
1
1
0
OCCC out (28)
W(13)
181
174
8
2
0
0
OCCC out (37)
W(12)
162
172
165
1
0
1
0
OCCC out (10)
W(11)
137
131
0
0
3
0
OCCC out (11)
W(10)
114
109
2
1
0
0
OCCC out (21)
W(9)
93
89
0
0
0
0
OCCC out (36)
W(8)
92
88
3
1
0
0
OCCC out (58)
W(7)
75
78
75
0
0
1
0
CCOC out (22)
W(6)
61
58
0
0
2
0
COOC out (20)
W(5)
46
44
0
0
4
0
OCCC out (38)
W(4)
37
36
1
0
1
0
CCCC out (23)
W(3)
29
28
1
0
3
0
CCOC out (22)
W(2)
24
23
1
0
2
0
CCOC out (40)
W(1)
14
13
1
0
3
0
CCCC out (38)
1. Stretching, Bending, Torsion and Out.
2. Scaling Factor 0.961 for B3LYP6-311++G (d,p) [ref. 27].
3. Relative absorption intensity normalized with highest peak absorption equal to 100.
4. Relative Raman intensity normalized to 100.
Figure 2
Calculated and experimental FT-IR spectra of quercitrin.
Figure 3
Calculated and Experimental FT-Raman spectra of Quercitrin.
The experimental (FT-IR and FT-Raman) and theoretical vibrational frequencies using DFT for quercitrin.1. Stretching, Bending, Torsion and Out.2. Scaling Factor 0.961 for B3LYP6-311++G (d,p) [ref. 27].3. Relative absorption intensity normalized with highest peak absorption equal to 100.4. Relative Raman intensity normalized to 100.Calculated and experimental FT-IR spectra of quercitrin.Calculated and Experimental FT-Raman spectra of Quercitrin.
O–H vibrations
The O–H hydroxyl stretching vibrations are tremendously effective for intra or intermolecular hydrogen bonding in the quercitrin. K. Muthu et.al reported the hydroxyl stretching vibrations in the 3600-3400 cm−1 range [28]. The O–H stretching vibrations of the Quercitrin, predicted by theoretical calculation, were observed at 3703, 3700, 3684, 3636, 3617, and 3616 cm−1 with a 100 % PED contribution. It is supported by the experimental FT-IR spectra observed at 3611cm−1.
C–H vibrations
The aromatic C–H stretching vibrations mostly appear in the range of 3100 to 3000 cm−1 [29]. Manjusha et.al reported the C–H stretching vibrations in the 2850-3000 cm−1 range [30]. In Quercitrin, C–H stretching vibrations occur from 3115 to 2886 cm−1. The experimental bands of FT-IR spectra were observed at 3122 and 2816 cm−1 and FT-Raman was observed at 3078 cm−1. The maximum PED contribution is 100%. Moreover, HCC bending bands are registered at 1067 and 1004 cm−1 in FT-IR and 991cm−1 in FT-Raman. Theoretically, HCH bending bands appear at 983,970 cm−1.
C–O vibrations
The stretching vibrations of C–O and the carbonyl C=O group are commonly disclosed in the range of 1740–1660 cm−1 [31]. The C–O stretching bands of the Quercitrin are noticed theoretically at 1665, 1392, 1375, 1372, 1362, 1359,1351, 1341, 1328, 1318, 1309, 1301, 1265, and 1225 cm−1 for the 6–311 G (d,p) basis set. The experimental values noticed at 1452, 1242, 1175, 1128, and 1003 cm−1 for FT-IR spectra and values at 1177 and 1226 cm−1 for FT-Raman spectra are in great concurrence with the values predicted using theoretical calculations with the 6-311G++ (d,p) basis set. These values are supported by the average potential energy distribution value of 85%. The blended vibration positions at 774,722, 682, 592, and 572cm−1for FT-IR are assigned to the OCC bending vibration. The other COC bending vibrations are observed at 624 in FT-IR and 638 cm−1 in FT-Raman. The CCO bending vibrations are recorded at 865, 807 and 787cm−1in FT-IR and at 1175 and 940cm−1in FT-Raman.
C–C vibrations
In carbon-carbon stretching vibrations, the bands between 1300–1000 cm−1 are designated as C–C ring stretching vibrations [32, 33]. The theoretical C–C stretching vibration for Quercitrin is reported at 1600, 1593, 1653, 1635, 1617, 1558, 1536, 1512, 1494, 1481, 1467, 1357, 1331, 1282, 1267, 1249, and 1243 cm−1. For the Quercitrin, the experimental CC stretching vibration values in FT-IR are observed at 1600, 1557, 1517, 1445, and 1419 cm-1, and the FT-Raman values are 1604, 1546, 1438, and 1402 cm-1.
Frontier molecular orbitals (FMO's)
FMOs assume a significant part during molecular interaction. The HOMO-LUMO energy gap and other FMO energies of the Quercitrin were plotted and represented in Figure 4. The FMOs fundamental descriptors are represented in Table 3 and Figure 4, [34, 35, 36]. The calculated HOMO energy value is -4.198eV, the LUMO value is -0.154 eV, and the bandgap energy value is 4.044 eV, for the quercitrin compound. It shows good charge transfer inside the molecule, and its biological activity is high [37]. The chemical softness of the quercitrin was found to be 0.247 eV. The low softness values of the quercitrin confirm the high stability and reactivity of the molecule. The chemical hardness of the quercitrin was computed to be 2.022 eV. The chemical potential and electrophilicity index values of quercitrin show that the molecule is a good bioactive drug.
Figure 4
Frontier molecular orbital of the Quercitrin molecule.
Table 3
Global chemical reactivity descriptors of the Quercitrin.
Parameters (eV)
values
HOMO energy (EHOMO)
-4.1984
LUMO energy (ELUMO)
-0.1542
Energy gap (eV)
4.0442
Ionization potential(I)
4.1984
Electron affinity(A)
0.1542
Electronegativity (χ)
2.1763
Chemical potential (μ)
-2.1763
Chemical Hardness (η)
2.0221
Chemical softness (S)
0.2472
Electrophilicity (ω)
1.1711
Frontier molecular orbital of the Quercitrin molecule.Global chemical reactivity descriptors of the Quercitrin.
Molecular electrostatic potential
The molecular electrostatic potential surface Using the Gaussview 5.0 tool, for the quercitrin is depicted in Figure 5 (a) [38,39]. The MEP surface is exposed by various colors due to the increasing electron density in the order of red < orange < yellow < green < sky blue < blue. The 3D colour code MEP map ranges between-7.797 × 10−2 (red colour) and 7.797 × 10−2 (blue colour) for the Quercitrin, whereas the red color indicates the nucleophilic attack, which is the strongest attraction and the blue colour expresses electrophilic attack, which is the strongest repulsion. In the quercitrin, the negative region is more focused around the O(10), O(11), O(12), O(13), O(20), O(21), O(22), O(23), O(24), O(31), and O(32) atoms. Figure 5(b) depicts the contour map for Quercitrin, which clearly shows the density around various atoms.
Figure 5
a) Molecular Electrostatic Potential surface map of Quercitrin and b) Contour map of electrostatic potential of the total density of the Quercitrin.
a) Molecular Electrostatic Potential surface map of Quercitrin and b) Contour map of electrostatic potential of the total density of the Quercitrin.
Local reactivity descriptors
The Fukui function is an important aspect of developing a pharmaceutical product since it is used to identify the electron density based on local reactivity descriptors, which are used to predict the chemical reactivity of the molecule [40, 41, 42, 43]. The atoms may possess a positive or negative mulliken charge in accordance with the number of electrons surrounding them. Figure 6 depicts the histogram of the computed Mulliken charge of the Quercitrin without hydrogen atoms, as well as all the oxygen atoms that have a negative charge and carbon atoms C1 to C9, C14, C15, C17, C27, and C28 that have a positive charge, while the molecule's other carbon atoms have negative charges. C3 has the highest positive value (0.389) of all the carbon atoms, whereas the oxygen atom has the highest negative value (−0.433) and the results are reported in Table 4. The computed fk+ value shows the possible site for nucleophilic attack (due to positive value) and is in the order of C1, C2, C6, C8, O24, C27, C28, C30, O31, and O, and the fk− value shows the possible site for electrophilic attack (due to negative value) and is in the order of C4, C7, C9, C18, and C25.
Figure 6
The histogram of calculated Mulliken charge of Quercitrin molecule expect hydrogen.
Table 4
Condensed Mulliken atomic charges, Fukui function fk and descriptors (sf)k and (ωf)k values for Quercitrin.
Atom. No
Mulliken atomic charges
Fukui Function
Local softness
Electrophilicityindex
qN+1
qN
qN-1
fk+
fk-
(sf)+
(sf)-
(ωf)+
(ωf)-
C1
0.318
0.291
0.240
0.027
0.051
0.007
0.013
0.032
0.060
C2
0.098
0.020
-0.016
0.078
0.036
0.019
0.009
0.091
0.042
C3
0.389
0.372
0.250
0.017
0.122
0.004
0.030
0.020
0.143
C4
-0.214
-0.214
-0.177
0.010
-0.037
0.010
-0.009
0.000
-0.044
C5
0.190
0.171
0.098
0.019
0.072
0.005
0.018
0.023
0.085
C6
-0.107
-0.142
-0.125
0.035
-0.017
0.009
-0.004
0.041
-0.020
C7
0.168
0.160
0.169
0.008
-0.009
0.002
-0.002
0.009
-0.011
C8
-0.053
-0.094
-0.117
0.040
0.024
0.010
0.006
0.047
0.028
C9
0.212
0.218
0.269
-0.007
-0.051
-0.002
-0.013
-0.008
-0.060
O10
-0.337
-0.354
-0.514
0.017
0.160
0.004
0.040
0.020
0.187
O11
-0.250
-0.305
-0.344
0.055
0.039
0.014
0.010
0.064
0.046
O12
-0.358
-0.383
-0.419
0.026
0.035
0.006
0.009
0.030
0.041
O13
-0.390
-0.387
-0.291
-0.003
-0.096
-0.001
-0.024
-0.003
-0.113
C14
0.288
0.303
0.264
-0.015
0.039
-0.004
0.010
-0.017
0.046
C15
0.023
0.028
0.093
-0.005
-0.065
-0.001
-0.016
-0.006
-0.077
C16
0.002
-0.001
0.010
0.003
-0.011
0.001
-0.003
0.003
-0.013
C17
0.070
0.074
0.062
-0.003
0.011
-0.001
0.003
-0.004
0.013
C18
-0.032
-0.019
0.050
-0.013
-0.069
-0.003
-0.017
-0.015
-0.081
C19
-0.283
-0.284
-0.323
0.001
0.039
0.000
0.010
0.001
0.046
O20
-0.376
-0.396
-0.394
0.019
-0.001
0.005
0.000
0.023
-0.001
O21
-0.433
-0.426
-0.407
-0.007
-0.019
-0.002
-0.005
-0.008
-0.022
O22
-0.392
-0.393
-0.397
0.000
0.004
0.000
0.001
0.000
0.005
O23
-0.327
-0.353
-0.423
0.027
0.069
0.007
0.017
0.031
0.081
O24
-0.279
-0.301
-0.379
0.022
0.079
0.005
0.019
0.026
0.092
C25
-0.188
-0.202
-0.156
0.015
-0.047
0.004
-0.012
0.017
-0.055
C26
0.011
-0.023
-0.082
0.034
0.059
0.008
0.014
0.039
0.069
C27
0.149
0.117
0.145
0.032
-0.029
0.008
-0.007
0.038
-0.033
C28
0.206
0.173
0.155
0.033
0.018
0.008
0.004
0.039
0.021
C29
-0.082
-0.107
-0.134
0.025
0.027
0.006
0.007
0.030
0.032
C30
-0.020
-0.056
-0.101
0.036
0.045
0.009
0.011
0.042
0.053
O31
-0.286
-0.354
-0.431
0.067
0.077
0.017
0.019
0.079
0.091
O32
-0.374
-0.412
-0.451
0.038
0.038
0.009
0.009
0.045
0.045
The histogram of calculated Mulliken charge of Quercitrin molecule expect hydrogen.Condensed Mulliken atomic charges, Fukui function fk and descriptors (sf)k and (ωf)k values for Quercitrin.
ADMET, drug-likeness properties and bioactivity score
Lipinski's rule of five [44, 45] and ADMET prediction [46] are both applied to assess the bioavailability of bulk material in drug discovery and development. In this study all the molecular characteristics of the Quercitrin were examined using the Molinspiration cheminformatics tool. Since the H-bond acceptor range is 11 (>10) and the H-bond donor range is 7 (>5) and TPSA 190 (>140), Quercitrin does not obey Lipinski's rule of five, as shown in Table 5 [47]. From ADMET, it is found that the compound quercitrin is orally available to humans, and the results are represented in Table 6. The AMES test's toxicity demonstrates that it is a non-carcinogenic and non-mutagenic molecule. The title compound was seen as a non-inhibitor for hERG (human ether -a-go-go gene), which proposes that it does not hinder any potassium channels.
Table 5
Prediction of drug-likeness properties for Quercitrin.
Descriptors
Properties
Hydrogen bond donor (HBD)
7
Hydrogen bond acceptor (HBA)
11
Partition coefficient (MilogP)
0.64
Molecular weight (MW)
448.34
Topological polar surface area (TPSA) (Å2)
190.2
Number of atoms
52
Number of rotatable bonds
3
Table 6
Prediction of ADMET profiles of Quercitrin.
A
B
C
D
E
F
G
H
I
J
0.0393
Non
52.709
76.443
-4.573
Suitable
Qualified
Mutagen
Violated
Non-inhibitor
A:ADMET_BBB.
B: P-glycoprotein inhibitor.
C: Human intestinal absorption (HIA+, %).
D: Plasma protein binding (PPB, %).
E: ADMET_SK logP.
F: Lipinski's rule.
G:CMC-like rule.
H:Ames_test
I: Lead-like rule.
J: hERG- I&II inhibitor.
Prediction of drug-likeness properties for Quercitrin.Prediction of ADMET profiles of Quercitrin.A:ADMET_BBB.B: P-glycoprotein inhibitor.C: Human intestinal absorption (HIA+, %).D: Plasma protein binding (PPB, %).E: ADMET_SK logP.F: Lipinski's rule.G:CMC-like rule.H:Ames_testI: Lead-like rule.J: hERG- I&II inhibitor.Molinspiration is a web server tool utilized to predict the bioactivity score of the Quercitrin against regular human targets. The values are given in Table 7 which shows it as a moderately active compound. Bioactive scores for kinase protein, nuclear receptor ligands, and enzyme inhibitors were 0.08, 0.17, and 0.37, respectively. The projected values for GPCR, ion channel modulators, and protease inhibitors are -0.01, -0.08, and -0.06, respectively: These expected values are relatively active. Based on these findings, we can conclude that quercitrin has the potential to be used as an anti-cancer drug in the future.
Table 7
Bioactivity score of Quercitrin.
Compound
GPCR
Ion channel modulator
Kinase inhibitor
Nuclear receptor ligand
Protease inhibitor
Enzyme inhibitor
Quercitrin
-0.01
-0.08
0.08
0.17
-0.06
0.37
Bioactivity score of Quercitrin.
Molecular docking study
The optimized Quercitrin structure is converted to PDB format and docked with the B-RAF protein (RCSB with PDB ID 6B8U) [48]. The resolution of the corresponding protein has a lower value of 2.68Å so that we can get an optimum structure for the B-RAF protein. The active site of the B-RAF protein comprises the residues Glu 501, Cys 532, Asp 594, and Phe 595; respective binding energy values are shown in Table 8. The amino acids Phe 595, Gln 530, Cys 532, and Ser 536 of B-RAF protein forms strong conventional hydrogen bond interactions with atoms H(44), H(45), H(46), and H(51) of the Quercitrin with a distance of 2.2, 2.1, 2.3, and 2.2Å, respectively Figure 7 (a). The residues Trp 531, Ala 481, and Ile 463 of B-RAF protein form pi-pi stacked interaction with Quercitrin which is shown in Figure 7 (b). Figure 7 (c) represents the Quercitrin docked into the binding cavity (2D view, Ligplot) of the B-RAF protein. The compound which has numerically higher binding energy is found to possess increased binding affinity towards target protein [49]. This result reveals that quercitrin interacts well with the B-RAF kinase protein and fits well into the binding cavity of the B-RAF target protein. The binding affinity of the compound Quercitrin, which has a -7.14 kcal/mol using AutoDock, was validated with the Glide XP score in Schrodinger software (−8.01 kcal/mol). In addition, the binding score of Imidazopyridinyl benzamide bound with B-RAF protein was also calculated using AutoDock (−5.21 kcal/mol) and Schrodinger's Glide XP (−6.41). From these docking results, it is found that quercitrin has a numerically higher binding energy and is found to be a potent anti-cancer agent than Imidazopyridinyl benzamide.
Table 8
Molecular docking results and Hydrogen bonding distances between B-RAF protein and inhibitors such as Quercitrin and Imidazopyridinyl benzamide.
Compounds
Bonded residues
Bond distance (Å)
Binding energy Kcal/mol
Reference RMSD (Å)
Autodock
Schrodinger maestro xpGlide
Quercitrin
Phe 595Ser 536Gln 530Cys 532
2.22.22.12.0
-7.14
-8.01
1.816
Imidazopyridinyl benzamide
Phe 595Asp 594Glu 501Cys 532
3.12.92.82.5
-5.21
-6.41
1.780
Figure 7
a) The position of the ligand Quercitrin in the binding cavity of the B-RAF Protein b) 2D view of distance for hydrogen bond interaction of Quercitrin with amino acid residues of B-RAF Protein and c) The ligplot showing intermolecular interaction of Quercitrin molecule in the active site of B-RAF Protein.
Molecular docking results and Hydrogen bonding distances between B-RAF protein and inhibitors such as Quercitrin and Imidazopyridinyl benzamide.a) The position of the ligand Quercitrin in the binding cavity of the B-RAF Protein b) 2D view of distance for hydrogen bond interaction of Quercitrin with amino acid residues of B-RAF Protein and c) The ligplot showing intermolecular interaction of Quercitrin molecule in the active site of B-RAF Protein.
Molecular dynamics simulations
Analysis of structural stability, fluctuations and compactness of the protein
The structural stability of the Quercitrin and Imidazopyridinyl benzamide inhibitors bound to B-RAF protein was performed and compared using the Root Mean Square Deviation (RMSD) as shown in Figure 8 (a). For the last 20 ns, the Quercitrin has maintained RMSD value of around 0.20 nm. Though both the inhibitors maintain good stability of the protein, quercitrin is found to possess a low RMSD value and has shown higher stability of the protein in comparison with the Imidazopyridinyl benzamide inhibitor. The fluctuations of amino acid residues of B-RAF protein bound to Quercitrin and Imidazopyridinyl benzamide inhibitors were carried out using Root Mean Square Fluctuations (RMSF) analysis as shown in Figure 8 (b). The residue at position 493 of the Imidazopyridinyl benzamide bound B-RAF protein shows higher fluctuations at 0.53 nm, whereas the Quercitrin bound protein has 0.29 nm. On comparing the fluctuations of the two inhibitors, the Quercitrin bounded protein has low fluctuations and shows higher stability of the protein structure. The compactness of the protein can be identified from the analysis of the radius of gyration (Rg). From Figure 9, it is clearly known that the Quercitrin bounded protein has a lower value of Rg value than the Imidazopyridinyl benzamide bounded B-RAF protein. The Rg value of the Quercitrin-bound protein remained at 1.91 nm for the final 40 ns of MD simulation, whereas the Rg value of the Imidazopyridinyl benzamide-bound B-RAF protein ended at 1.96 nm.
Figure 8
a) Root Mean Square Deviation (RMSD) and b) Root Mean Square Fluctuation (RMSF) of B-RAF protein bounded to Quercitrin and Imidazopyridinyl benzamide inhibitors.
Figure 9
Radius of gyration (Rg) of the B-RAF protein bounded to Quercitrin and Imidazopyridinyl benzamide inhibitors.
a) Root Mean Square Deviation (RMSD) and b) Root Mean Square Fluctuation (RMSF) of B-RAF protein bounded to Quercitrin and Imidazopyridinyl benzamide inhibitors.Radius of gyration (Rg) of the B-RAF protein bounded to Quercitrin and Imidazopyridinyl benzamide inhibitors.
Analysis of hydrogen bonding and interaction energy analysis
The hydrogen bonds between the protein and ligands (Quercitrin and Imidazopyridinyl benzamide) were monitored throughout the MD simulation of 100 ns as shown in Figure 10. From Figure 10, it is evident that the Quercitrin has maintained 3 to 4 hydrogen bonds throughout the MD simulation, whereas the Imidazopyridinyl benzamide maintains 2 to 1 hydrogen bond. The total interaction energy, which is the sum of electrostatic and van der Waals (vdW) interactions, between the B-RAF protein and ligands (Quercitrin and Imidazopyridinyl benzamide), is shown in Figure 11 and Table 9. According to Table 9, quercitrin has a numerically higher interaction energy of 299.59 kj/mol (−71.60 kcal/mol) than Imidazopyridinyl benzamide, which has a numerically lower interaction energy of 269.39 kj/mol (−64.38 kcal/mol). For the two ligands, the vdW (−223.33 kj/mol (−53.37 kcal/mol) for Quercitrin and -169.63 kj/mol (−40.54 kcal/mol) for Imidazopyridinyl benzamide) interaction is found to be higher than electrostatic (−76.24 kj/mol (−18.22 kcal/mol) for Quercitrin and -99.76 kj/mol (−23.84 kcal/mol) for Imidazopyridinyl benzamide)) interactions. From this analysis, it is clearly known that quercitrin has higher affinity and is more bound to B-RAF protein than Imidazopyridinyl benzamide inhibitors.
Figure 10
Hydrogen bonding interactions of Quercitrin and Imidazopyridinyl benzamide with B-RAF protein.
Figure 11
Total interaction energy between the inhibitors (Quercitrin and Imidazopyridinyl benzamide) and B-RAF protein.
Table 9
Total interaction energy of Quercitrin and Imidazopyridinyl benzamide inhibitors bounded to B-RAF protein. Energies are in kj/mol.
S. No.
Compounds
Electrostatic
vdW
Total interaction energy
1
Quercitrin
-99.76
-163.63
-269.39
2
Imidazopyridinyl benzamide
-76.24
-223.33
-299.59
Hydrogen bonding interactions of Quercitrin and Imidazopyridinyl benzamide with B-RAF protein.Total interaction energy between the inhibitors (Quercitrin and Imidazopyridinyl benzamide) and B-RAF protein.Total interaction energy of Quercitrin and Imidazopyridinyl benzamide inhibitors bounded to B-RAF protein. Energies are in kj/mol.
Conclusion
The Quercitrin was structurally drawn and optimised to its lowest energy conformation, and bond length and bond angles were calculated and compared to experimental XRD data. The experimental and observed results of the Quercitrin compound's vibrational spectra (those based on PED %) were compared. The charge transfer inside the molecule is clearly described by the HOMO-LUMO, MEP, and Mulliken analyses. The molecular docking calculations were validated with two docking tools, AutoDock and Schrodinger's Glide XP. The binding affinity of the Quercitrin compound has a numerically higher binding affinity -7.14 kcal/mol (AutoDock) and -8.01 kcal/mol (Glide XP score in Schrodinger software) than the Imidazopyridinyl benzamide inhibitor.In addition, MD simulations of protein-ligand complexes were monitored for 100 ns, from which the RMSD, RMSF, Rg, H-bonds, and interaction energy calculations were executed. Quercitrin is found to have a low RMSD value and has shown higher stability of the protein compared to Imidazopyridinyl benzamide inhibitor. From RMSF analysis, the Quercitrin bounded protein has low fluctuations and shows higher stability of the protein structure. Throughout the 100 ns of MD simulation, Quercitrin maintained 3 to 4 hydrogen bonds, whereas Imidazopyridinyl benzamide maintained 2 to 1 hydrogen bond. From these investigations, it is identified that the compound quercitrin has maintained good structural stability, compactness, higher Hydrogen bonds, and interaction energies than the Imidazopyridinyl benzamide inhibitors. Finally, it is concluded that quercitrin bounds well in the binding domain of B-RAF kinase protein.
Declarations
Author contribution statement
Govindammal M: Conceived and designed the experiments; Performed the experiments; Analyzed and interpreted the data; Contributed reagents, materials, analysis tools or data; Wrote the paper.Kannan S: Performed the experiments; Analyzed and interpreted the data; Contributed reagents, materials, analysis tools or data.Srinivasan P: Contributed reagents, materials, analysis tools or data.Prasath M: Conceived and designed the experiments; Analyzed and interpreted the data; Wrote the paper.
Funding statement
This research did not receive any specific grant from funding agencies in the public, commercial, or not-for-profit sectors.
Data availability statement
Data included in article/supplementary material/referenced in article.
Declaration of interests statement
The authors declare no conflict of interest.
Additional information
No additional information is available for this paper.
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