27
Should I sow QM in my fields? Ewa Chudyk Cresset UGM, 18-19 th June 2015, Cambridge, UK

Should I sow QM in my fields? - Cresset Home Page€¦ · Should I sow QM in my fields? ... • Exploration of these receptor-ligand interactions provide ... • The cycle calculates

Embed Size (px)

Citation preview

Should I sow QM in my fields?

Ewa Chudyk

Cresset UGM, 18-19th June 2015, Cambridge, UK

PAGE

Agenda

1

Fragment Molecular Orbitals (FMO)

Contribution of various interactions to binding energy

Protein-ligand field complementarity & SAR interpretation

QSAR analysis with Forge and FMO

PAGE

MM and QM system description

2

Summary

Molecular mechanics (MM):

• Fast

• Can be applied to large

systems

• Low level of accuracy

• Polarisation not included

(usually)

• Limited parametrization

Quantum mechanics (QM):

• Higher level of accuracy

• Electrons explicitly defined

• Can study chemical reactions

• Slower

• Sampling not included

• Difficult to apply to large systems

Non-classical intermolecular forces: cation-π, dipole-π, halogen-π, carbonyl n-π*,

also charge transfer and polarization important in ligand binding

Is MM description good enough to understand drug binding?

PAGE

Fragment molecular orbital (FMO)

3

About the method

• “Visual inspection” and molecular mechanics do not fully

explain complex protein-ligand interactions

• FMO is a quantum mechanical method that has been

developed1 for application to large (biological) systems

• FMO provides detailed analysis of protein-ligand

interactions and their chemical nature

− Calculate individual contribution of each residue and water

molecule to binding enthalpy

• Exploration of these receptor-ligand interactions provide

key insights for further SBDD

PIE (Pair Interaction Energy)

Fragmentation of peptide

1Fedorov DG and Kitaura K. J. Phys. Chem. A, Vol. 111, No. 30, 2007

11

22

44

33

5

PAGE 4

Pair interaction energy decomposition analysis (PIEDA)

Electrostatic (PIEes)Forces between point charges / (permanent and induced)

dipoles/quadrupoles

Charge transfer (PIEct)Interactions between occupied orbital of

the donor and unoccupied orbital of the

acceptor. Orbital energy gap and overlap

are the important factors.

Dispersion (PIEdis)Non-polar molecule can have dipolar moment for a

short period of time due to the movement of

electrons within the molecule; this induces weak

dipole-dipole interaction

Exchange repulsion (PIEex)Forces between molecules placed close together and always

repulsive. Mainly due to the overlap of two occupied orbitals.

δ+ δ- δ+ δ-

+ - or

C C: :

C C:

e-

Four energy terms obtained

1Fedorov DG and Kitaura K. J. Phys. Chem. A, Vol. 111, No. 30, 2007

PAGE

Cyclin-dependent kinase 2 (CDK-2)

5

Details on the receptor

• Involved in the control of the cell

cycle

• CDK-2 inhibitors might have

anticancer properties

• Good target to examine binding

affinities

• Previously published QSAR study1

• Range of different interactions within

the binding pocket

• 14 available crystal structures of

protein-ligand complexes

1Mazanetz M. et. al.; J Cheminform. 2011 Jan 10;3(1)

PAGE

28 CDK-2 inhibitors

6

Details on the ligands

NN

N

SO

O

O N

NN

N N

N

Cl

N

N S

O

O

N

N

Cl

N

N

Cl

N

N

N

N

N

NN+

N

NN

N

NN

O

NN

O

NNS

O

O

N

O

NNN

N NN

N

N

NN

O

NF

O

N

N N

O

N

F

N

NN

O

N

F

O

O

N

NN

O

N

FO N

NN

O

N

F

O

F

N

O

NN

N

O

NO

N

N

N

O

F

F

N

O

NN

NO

FF

N

O

NN

N

O

F

F

O

N

O

NN

N

O

F

F

N+

N

O

NN

N

OF

F

N+

N

O

NN

N

O

F

F

N+

N

O

NN

NO

FF

F

N+

N

O

NN

NO

FO

N+

N

O

NN

NO

FCl

N+

N

O

NN

N

O

N+

Cl

Cl

185.0 µM120.0 µM 1000.0 µM 7.0 µM 1.9 µM 1.5 µM 0.03 µM

3.0 µM0.66 µM 97.0 µM 25.0 µM 85.0 µM

0.85 µM 0.73 µM

1.6 µM0.09 µM 0.14 µM

F

N

O

NN

N

O

F

F

0.003 µM 0.025 µM 0.012 µM 0.019 µM

0.038 µM 0.14 µM 0.044 µM0.91 µM 0.052 µM 0.063 µM

0.082 µM

Wyatt P.G. et al., J.Med. Chem. 2008, 51: 4986-4999

• Activity of the molecules ranging from 1000 µM to 3 nM

• Half of the inhibitors available as protein-ligand complex crystal structures (green)

PAGE

R-group decomposition

7

The most potent CDK-2 inhibitors

Wyatt P.G. et al., J.Med. Chem. 2008, 51: 4986-4999

• Protein volume excluded

constraint improves

alignment

• The most active inhibitors

align with high Cresset

scores (above 0.8)

R1

R2

R2:

R1:

• Electrostatic interactions dominant

in the core of the molecule

• Hydrophobic interactions to

periphery

PAGE

Cyclin-dependent kinase 2 (CDK-2)

8

Binding pocket and subpockets

• Hydrogen bond interactions in the centre of

the pocket

• What drives SAR of both subpockets?

• To be able to explain activity of those

molecules more details analysis is required:

F

N

O

NN

N

O

F

F

N

O

NN

N

OF

F

N+

N

O

NN

N

O

F

F

N+

0.003 µM

0.14 µM 0.044 µM

F

N

O

NN

N

O

0.14 µM

#18

#17

#23 #24

PAGE

Cyclin-dependent kinase 2 (CDK-2)

9

FMO interactions

• Different interactions dominate in every

inhibitor part

S1

S2

S2S1 Core

PAGE

Electrostatic complementarity (EC)

10

About the method

Davenport and Heifetz et al., ,Assay Drug Dev Technol., Dec 2010, 8, 6, 781

• “Electrostatic Complementarity” (EC) is a method to calculate the electrostatic attraction and

repulsion between the protein and ligand and map it on the ligand surface

• The EC is mainly SAR/QSAR analysis and design tool for lead optimization

• It provide the medicinal chemist not only with the overall degree of electrostatic behavior, but also

highlights the most significant regions for modifications in order to maximize the effect on binding

affinity to the protein

• The and derived from the electrostatic potential around protein and ligand

• The more active inhibitor, the more negative ECScore

protein

kjiE,,

ligand

kjiE,,

∑∑∑= = =

×=

N

i

N

j

ligand

kji

N

k

protein

kjiScore EEEC1 1

,,

1

,,

PAGE 11

#18, IC50: 0.003 µM

EC for the most potent inhibitor

Protein ESP+

Protein ESP-

Ligand ESP+

Ligand ESP-

Protein

ESP

Ligand

ESP

Electrostatic Attraction

Electrostatic Repulsion

EC

PAGE

Electrostatic complementarity

12

Crystal structure complexes

• Lack of correlation between electrostatic complementarity score and inhibition

• Possibly electrostatics is not a driving force in inhibitor binding

PAGE

EC in ligand optimization

13

Inhibitor’s core

• ECScore reproduces ligand ranking

• Inhibitor core interactions dominated by

electrostatics – high complementarity

Electrostatic Attraction

Electrostatic Repulsion

NN

N

SO

O

ON

Cl

N

N

N

N

185.0 µM

120.0 µM

1.5 µM

Inhibitor Activity [µM] ECScore

#1 185 -45.1

#2 120 -66.0

#6 1.5 -114.4

#1 #2#6

Leu83Glu81

Leu83

Leu83

Glu81

Glu81

Leu134

Gln134

WAT

Leu134 Ile10

Val18

PAGE

EC in ligand optimization

14

S1 subpocket

• Electrostatic complementarity does not

reproduce activity ranking

• Other effects than electrostatics must be

strong within S1 pocket

• Charge transfer and dispersion may play an

important role

Electrostatic Attraction

Electrostatic Repulsion

F

N

O

NN

N

O

F

N

O

NN

N

O

F

F

0.14 µM

0.003 µM

#18

#17

Inhibitor Activity [µM] ECScore

#18 0.003 -101.5

#17 0.14 -126.3

PAGE

F

N

O

NN

N

O

F

F

Core

Leu134

Val18

Lys33

Asp145

Asn132

#18

FMO effects around the S1 subpocket

15

Physical nature of interactions

• Total interaction energies:

� #18: -25.3 kcal/mol

� #17: -7.1 kcal/mol

• Difference between #18 and #17

comes from interactions with Lys33

and Asp145

• Charge transfer significantly

contributes to binding

#18 #17

0.14 µM0.003 µM

#18 #17

#18 #17

F

N

O

NN

N

O

PAGE

EC and FMO in ligand optimization

16

Interactions within the S2 subpocket

• ECScores do not reproduce activity ranking

• Dispersion and charge transfer as important

as electrostatics

0.003 µM 0.14 µM 0.044 µM

#18 #23 #24

ECScore -101.5 -163.5 -209.3

#23 #24

F

N

O

NN

N

O

F

FN

O

NN

N

OF

F

N+

N

O

NN

N

O

F

F

N+

PAGE

QSAR model with FMO

17

Cyclin-dependent kinase 2 inhibitors

1Mazanetz M. et. al.; J Cheminform. 2011 Jan 10;3(1)

• PLS model used

• 14 inhibitors with crystal structures as a

training set, remaining 14 as a test set

• Descriptors included:

• The sum of the enthalpic contributions

from FMO

• The polar solvation term

• The nonpolar solvation term

• The entropic term

• Solvation component improves correlation

Observed ∆G

Pre

dic

ted

∆G

R2=0.94

Test Set

Training Set

PAGE

QSAR model with Forge

18

Cyclin-dependent kinase 2 inhibitors

• Six different models tested

• The best model:

− The most active ligand as a reference

− Manual adjustment of the alignment

− “Normal” alignment conditions

− Protein as volume excluded

• PLS model (as for FMO) as implemented

in Forge – “3D descriptors”

• Electrostatic model descriptors dominate

around the inhibitor core

• All other interactions (hydrophobic

pockets) represented as steric positive and

negative effectsCresset field descriptors from the training

set around the reference cmpd

PAGE

QSAR model with Forge

19

Cyclin-dependent kinase 2 inhibitors

• Ligand-based QSAR model based on the best

inhibitor alignment with protein volume-excluded

• Test set points slightly closer to the trend line

than in the FMO study

• Results comparable with FMO structure-based

QSAR model (R2=0.94)

R2=0.89

Observed ∆G

Pre

dic

ted

∆G

Test Set

Training Set

PAGE

Summary

20

• QM approach helps to deconvolute the drivers of molecular interactions

• QSAR performance with FMO and Forge are equally good

• Both approaches have been proven complementary useful in inhibitor optimization

PAGE

Acknowledgement

21

• Evotec (Comp Chem group)

− Dr. Mike Bodkin

− Dr. Alexander Heifetz

− Dr. Mike Mazanetz

− Dr. Inaki Morao

− Dr. Tim James

− Dr. Mirco Meniconi

• FMO Developers

− Dr. Dmitri Fedorov

• Cresset Support Team

Your contact:

Ewa Chudyk, PhDSenior Scientist

+44.(0) 1235 44 [email protected]

PAGE

Calculating binding affinities

23

Thermodynamic cycle

• The cycle calculates the receptor (R), ligand (L), and

complex (C) in vacuum and then transfers them to

solvent to find the solvation free energy

• The reported IC50 values can be used to calculate

free binding energy for each ligand

• Non-classical effects, including charge transfer and

polarization, were proven to play an important part in

binding (e.g., hydrogen bonding)

Schematic view of the

thermodynamic cycle used in the

derivation of the binding affinity

∆����� = − ln ��� = ∆� − ∆�

PAGE

How ECScore calculated?

24

More details

Davenport and Heifetz et al., ,Assay Drug Dev Technol., Dec 2010, 8, 6, 781

PAGE

MEP around the most potent inhibitor

25

AM1-BCC charges vs Cresset charges

• Both methods give similar description of the ligand alone

• This does not provide any information on interactions with the receptor

Ligand ESP+

Ligand ESP-

PAGE

Charge transfer within P1 subpocket

26

Asp145

Lys33

Direction of charge transfer