Ion-Dipole Correction and CWBSol of Integration Equation Theory of - - PowerPoint PPT Presentation

ion dipole correction and cwbsol of integration equation
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Ion-Dipole Correction and CWBSol of Integration Equation Theory of - - PowerPoint PPT Presentation

Ion-Dipole Correction and CWBSol of Integration Equation Theory of Liquid Siqin CAO Department of Chemistry The Hong Kong University of Science and Technology May 25, 2020 Integration Equation Theory of Liquid with Ion-Dipole Correction


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SLIDE 1

Ion-Dipole Correction and CWBSol

  • f Integration Equation Theory of Liquid

Siqin CAO

Department of Chemistry The Hong Kong University of Science and Technology

May 25, 2020

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SLIDE 2

Integration Equation Theory of Liquid with Ion-Dipole Correction

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SLIDE 3

Solvation

Denis Bucher, Pieter Stouten, Nicolas Triballeau, J. Chem. Inf. Model 58, 692−699 (2018) Takashi Imai, Koji Oda, Andriy Kovalenko, Fumio Hirata, Akinori Kidera, JACS 131, 12430–12440 (2009)

WaterFLAP 3D-RISM WaterMap Water placement Fragment based drug design SZMAP

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SLIDE 4

Integration Equation Theory of Liquid

water around 1d5q

ρ(2)

ij (ri, rj) = ρiρjgij(ri, rj)

103 faster than MD; Perfect if accurate 3D-RISM RISM: reference interaction site model Two equations are enough

hij(rij) = cij(rij) + ∑

k

cik(rik) * (hkj(rkj) + skj(rkj)) ≈ cij(rij) + ∑

k

cik(rik) * (hkj(rkj) + skj(rkj)) ln gij = −vij+hij − cij+Bij

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SLIDE 5

Multibody issues of IET

1 5 2 3 4 r (Å)

(a) (c) (d)

  • f LYS
  • n 5TXD

NH+

3

  • f ARG
  • n 5TJ1

NH+

2

1 2 5 r (Å)

PLHNC MD

(b)

5TXD 5TJ1

gPLHNC(r) = { e−vγ(r)+hγ(r)−c(r), ln g ≤ C 1 − vγ(r) + hγ(r) − c(r) − C + eC, ln g > C IET has issues for water around negative charge ions

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SLIDE 6

Multibody issues of IET

r (Å) 5 1 2 3 5 5 5 4 1 2 3 5 5 5 5

around 5TXD

Cl−

  • f GLU
  • n 5TJ1

O−

5TXD 5TJ1

KH PSE2 PSE3 PLHNC MD

IET has issues for water around negative charge ions

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SLIDE 7

Multibody issues of IET

Sketches from khanacademy.org

1 r (Å) 5 3 5 7 Water around a negative charge group 1 5 2 4 3 r (Å) Water around a positive charge group

Issue is related to multibody effect, but IET is single-body theory

In IET, both are treated in mean-field way: ∫ cH(r′ )ρb

HhHO(|r′ − r|)d3r′

= ℱ−1[cH(k)hHO(|k|)]

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SLIDE 8

Hydrogen bond potential

H-bond was modeled with an explicit potential function, the General hydrogen bond function, in the last century:

[1] A. T. Hagler, S. Lifson, and P . Dauber, JACS 101, 5122 (1979) [2] F . A. Momany, R. F . McGuire, A. W. Burgess, and . A. Scheraga, J. Phys. Chem. 79, 2361 (1975) [3] Wendy D. Cornell, ..., Peter A. Kollman, JACS 117, 5179 (1995) [4] Garret Vanderkool, J. Phys. Chem. 87, 5121-5129 (1983) [5] Felcy Fabiola, Richard Bertram, Andrei Korostelev, and Michael S. Chapman, Protein Sci. 11: 1415–1423 (2002) (DOI 10.1110/ps.4890102)

General hydrogen bond used to be available in AMBER Now, people believe H-Bond is resulted from electric interactions. Therefore: (1) H-bond interaction is short range; (2) The nature of H-bond interaction is electric interaction

An example: hydrogen bond interaction

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SLIDE 9

Ion-Dipole Correction

ln gO(r) = − (vO(r) − ΔvIDC

O

(r)) + hO(r) − cO(r) + BO(r) ΔvIDC

αO (r) ≈ ⟨pOH ⋅ EO⟩ ≈

1 4πε0 ⟨ QαqH εr(rH)rαH − QαqH εr(rH)rαO⟩ rαH = rαO ± bOH bOH = 0.954Å

Implementation:

vLJ

αO(r) + ΔvIDC αO (r) → vnew αO (r)

εr(rH) = { εr(water) (rαH ≤ rαO) εr(surface) (rαH > rαO)

bOH rαH rαO

Ion-Dipole Correction (IDC): a potential function for multibody effect

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SLIDE 10

Water distribution around ions

KH PSE2 PSE3 PLHNC MD

5TXD Original With IDC

r (Å) 1 2 3 5 5 5 5 1 2 3 5 5 5 5 4 4

Cl−

IDC works for ions

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SLIDE 11

Water distribution around strongly polar group of protein

r (Å)

(b)

GLU . O−

1 2 3 5 5 5 5

(c)

1 2 3 KH PSE2 PSE3 5 5 5 5

Original With correction

PLHNC MD

(a)

5TJ1

IDC works for negatively charged groups of protein

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SLIDE 12

Water distribution around strongly polar group of DNA

DT . O−

(b) (c)

Original With correction

r (Å) 1 2 3 5 5 5 5 1 2 3 5 5 5 5

6JCD

(a)

KH PSE2 PSE3 PLHNC MD

IDC works for negatively charged backbone of DNA

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SLIDE 13

Water distribution around a large protein: chaperon

Ring 1 Ring 2 Ring 1 Ring 2 |------- Close -------| |------- Open -------|

5 5 5 5 5 5 5 5 5 5 5 5 1 2 3 1 2 3 5 5 5 5 5 5 5 5 5 5 5 5 1 2 3 1 2 3 Open Rings Close Rings Open Rings Close Rings |----- Ring 1 ------||--------------- Ring 2 ---------------| |----- Ring 1 ------||--------------- Ring 2 ---------------|

231ARG 230ILE 63GLU 65LYS 44PHE 2ALA 255GLU 226LYS 63GLU 65LYS 44PHE 2ALA 231ARG 230ILE 63GLU 65LYS 44PHE 2ALA 255GLU 226LYS 63GLU 65LYS 44PHE 2ALA

3DRISM-KH 3DRISM-PSE2-IDC MD

(a) (b) (c) (d)

r (nm)

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SLIDE 14

Free energy calculation

Solvation free energy

ΔμKH = ∑

αγ ∫ [−cαγ(r) − 1

2 cαγ(r)hαγ(r) + 1 2 hαγ(r)2Θ(−hαγ(r))] ρb

γ d3r

ΔμS = ΔμKH + aV + b ΔμKH = ∫ dλ ⟨ ∂uIDC ∂λ ⟩ = ∫ dλ ⟨ ∂uuv ∂λ ⟩ + ∫ dλ ⟨ ∂ΔuIDC ∂λ ⟩

SFE in 1990s: the excessive chemical potential SFE in 2010s: the universal correction SFE with IDC correction: Approximation:

∫ dλ ⟨ ∂ΔuIDC ∂λ ⟩ ≈ LJorig − LJIDC 2

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SLIDE 15

Universal correction scheme

  • 30
  • 20
  • 10

10

  • 20
  • 10

10

  • 30

FEP (kcal/mol) IET (kcal/mol)

〇 Straightforward UC with PSE2-IDC 〇 3DRISM-PSE2-UC with IDC

r MUE RMSE

kcal/mol

Straight 0.9705 1.8 2.5 LR 0.9859 1.2 1.7 r MUE RMSE

kcal/mol

GF-UC 0.9884 0.7 1.1 KH-UC 0.9955 0.6 1.0 PSE2-UC 0.9950 0.6 1.0

  • 30
  • 20
  • 10

10

  • 20
  • 10

10

  • 30

FEP (kcal/mol) IET (kcal/mol)

╳ 3DRISM-KH-GF-UC 〇 3DRISM-KH-UC

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SLIDE 16

Summary

  • 3DRISM-HNC is good for positively charged ionic

solutes, but has deviations of solvation peaks around negatively charged solutes.

  • Ion-Dipole Correction will generate first solvation

peaks at correct locations.

  • PSE2 is the recommended closure.
  • Solvation free energy functional needs to be

investigated.

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SLIDE 17

CWBSol: The Clear Water Bay Solvation Package

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SLIDE 18

CWBSol

php -S 127.0.0.1:8080 -t path_of_CWBSol

CWBSol: a graphics interface to IET calculations Platforms: Server:

Linux with PHP 5+ and GCC 4+ MacOS 10.9+ with PHP 5+ Windows with WSL or Cygwin Client: Chrome, FireFox, Safari, Edge

(Internet Explorer not supported)

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CWBSol: easy to install

Only required: FFTW CWBSol: one-click install Configuration: all options are listed with explanations FFTW: one-click install

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CWBSol: easy to run

Options are listed, with default values One-click to see help message Everything stored on server Support: PDB GRO XTC (need GROMACS enabled) TOP PRMTOP And more...

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SLIDE 21

CWBSol: easy to visualize

RDF 3D distributions One-click to view

(need ImageMagick and GNUPLOT)

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SLIDE 22

CWBSol: an one-click tutorial

Do calculation: Watch the calculation: See the results: If troubles encountered:

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SLIDE 23

CWBSol: the efficiency

5TXD 5TJ1 6JCD Chaperon MD AMBER RISMHI3D 1 100 10000

Efficiency 285 105 802 120715 Atom Number:

1000 10

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SLIDE 24

Summary

  • CWBSol can efficiently perform IET.
  • Can run on laptop or a remote server.
  • Easy to install. No need to suffer from installing a lot
  • f libraries.
  • Support the most common file formats: TOP and

PRMTOP; PDB / GRO and XTC

  • Support all the closures that I can find on paper
  • Not yet 100% finished
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SLIDE 25

Thank you