martini workshop 2021 introduction to martini 3
TRANSCRIPT
PAULO C. T. SOUZA
Martini Workshop 2021
Introduction to Martini 3
Overview of the presentation
• Basic CG modeling principles
• Revisiting Martini 2
• Problems of the previous
model
• Introduction to Martini 3
• Beads
• Validation
• Improvements2
van Gunsteren et al, Angew. Chem. 2006, 45, 4064 – 4092
Degrees of freedom
Boundary Conditions:
Temperature
Pressure
Walls or periodic
boundaries
External forces
Methods to generate
configurations
Forces between particles
Bonded interactions
Non-bonded interactions
MOLECULAR
MODEL
Electrons and Nucleus
United or All-atom
Coarse-grained
Implicit model
- Unbiased MD
-Biased methods
-Monte Carlo
-Docking, etc.
Four essential ingredients for molecular modeling:Choice depends of the problem studied
3
When should
we use CG?
When/Why use coarse-graining methods?
Connecting all-atom to continuum scale
-“toy model” for ideas
- get more sampling
CG for
smaller scales?
Tutorial
backward
Tutorial
TS2CG
Tutorial
Protein-small
molecule Binding
4
Different ways of coarse-graining
Experimental data
Atomistic
Models
Coarse-Grained
Models
• Pragmatic approach
• Reproduce faithfully certain experimental properties
• Developed with certain application area in mind
Examples:Go models
SIRAH model
• Hierarchical approach
• Interactions at CG level from the collective interactions at
atomistic level
• General method applicable to any system
Examples: - Iterative Boltzmann inversion potentials
- Force matching
BOTTOM-UP
TOP-DOWN
5
• Build block approach (“Lego”).
• Chemical specificity
• Fast (102 - 103 speed-up)
• Implementation in atomistic MD
codes.
• Compatibility and versatility
• Parameterization combining
Bottom-Up and Top-Down
approaches
The Martini Model: Key features
Approximately 4:1 mapping of
non-hydrogen atoms
6
From beads to complex systems
Parametrization with
atomistic simulations
Bottom-up
Building blocks
Simple systems
Complex Systems
Top-down
Calibration with
thermodynamics datanon-bonded
interaction
bonded
interactions
Insights of
collective
processes
Characterizaton
of assembles
and materials
Extensive
tests in model
systems
Comparison
with atomistic
data
7
MARTINI 2: THE BEADS TYPES
C = non-polar
N = intermediate
P = polar
Q = charged
(+1/-1)
C1
C2
C3
C4
C5
Nda
Nd /Na
N0
P1
P2
P3
P4
P5
Qda
Qd/ Qa
Q0
18 Bead Chemical Types 3 Bead Sizes
R = Regular
0.47 nm
S=Small
0.43 nmT=Tiny
0.32 nm
- +
R-S
0.47 nm
R-T
0.47 nm
S-T
0.43 nm
Linear/
Branched
molecules
Ringsnucleobases
- +
Marrink et. al JPCB,2007
Hyd
rop
ho
bic
ity s
ca
le
8Uusitalo et. al JCTC,2015
THE HEART OF MARTINI 2: THE INTERACTION MATRIX
9
MAPPING AND BONDED POTENTIALS
• Where the beads were placed?
• Center of mass: general rule
• Exceptions:
• Corrections in bond lenghts to improve
certain properties.
• Cα for proteins (Elnedyn approach)
• Fuzzy approach: a CG model can represent
more than one molecule. Example: lipids
• Bonded potentials: the ones
typically used in atomistic MD
codesTutorial
Parametrization new CG models10
Huge success of Martini 2 during 14 years
Google scholar: ~ 4500 citations only for the main paper:
S.J. Marrink at al. JPCB, 111:7812-7824, 2007.
Two recent high-impact examples of applications:
1) PIP2 stabilizes active states of
GPCRs and enhances selectivity of
G-protein couplingof GPCR .Yen et al, Nature 2018.
2) Reversible Self-Assembly of
Superstructured Networks.Freeman et al, Science 2018.
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There are some limitations …
• Missing entropy, compensated by reduced enthalpy
• Driving forces may be wrong in some cases
• Temperature dependence and hydrophobic effect.
• Be careful with time scales
Fundamental problems related with CG approach
Coarse-grained Atomistic 12
AND there were also unexpected problems
Solu
ble
pro
tein
Sugars
Schmalhorst et al, JCTC, 2017
Stark et tal, JCTC, 2013
Javanainen et al, Plos One, 2017
TM
pro
tein
s
No internal cavities
and limited flexibility
apo-rhodopsin
Wrong partitions Dissociation barriers
Bereau and Kremer, JCTC, 2015 Uusitalo et al, JCTC, 2015
Issues in miscibility
Cyclohexane/Benzene
Alessandri et al, to be published 2021
Excessive aggregation
Limited chemical space
slightly soluble miscibleinsoluble
ON OO OOCH3
OC
O
slightly soluble
And others…Thanks for Martini
Community!
Kanekal and Bereau , JCP, 2019
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Solution? Full reparametrization of Martini
Lego in ~1980
Lego today
Easy-to-use versus Accuracy?
First Lego ~1949
Martini 1:
for lipids
Marrink et. al JPCB,2004
Martini 2:
for biomolecules
Marrink et. al JPCB,2007.
Martini 3:
for general purpose
Souza et. al Nature Methods,2021.
14
Martini 3: what is new?
1) Improved interactions and packingReparametrized all bead sizes and types, cross interactions and bonds
2) Better Coverage of Chemical SpaceNew beads and ways to modify them.
Kanekal and Bereau , JCP, 2019
4) Embracing Gō models for proteins
Poma et al, JCTC, 2017
Alessandri,Souza et al, JCTC, 2019
3) Reformulation of charged beads
Jungwirth and Cremer, Nature Chemistry, 2014
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How did we get the new model/parameters?
Defining the interaction matrix and interaction levels
Mainly Calibration Mainly Validation
Multiscaling
- Water/oil partitioning
- Miscibility
- Densities
- Trends in solvation
- Trends in vap. enthalpy
Quality control
- quick simulation tests
- Yes/No answers.
- avoid parameters with
clear problems
Quantitative tests
- expensive tests.
- big/complex systems
- taskforces and external
collaborators
Defining your
universe
- # of types and sizes
- # of interaction levels
- Rules for mapping
- Rules for bonds
- Bead assignments
- Interaction matrix
Tier 0 Tier 1 Tier 2
Souza et. al Nature Methods,2021.
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MARTINI 3: THE BEAD CHEMICAL TYPES
C = non-polar
N = intermediate
P = polar
Q=charged
X = halo compounds
C1
C2
C3
C4
C5
C6
N1
N2
N3
N4
N5
N6
P1
P2
P3
P4
P5
P6
Q1
Q2
Q3
Q4
Q5
Total of 29 Bead Chemical Types
- 1 +1
Souza et. al Nature Methods,2021.
Hyd
rop
ho
bic
ity a
nd
mis
cib
ility s
ca
le
W= Specific beads for water
Expansion of bead subtypes
X1
X2
X3
X4
-2 +2 D = divalent charged
molecules
New beads!
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NEW INTERACTION MATRIX OF MARTINI 3
LJ and Reaction-field (or PME)
Souza et. al Nature Methods,2021.18
MARTINI 3: THE BEAD SIZES
3 Bead Sizes
Regular
0.47 nm
Small
0.41 nmTiny
0.34 nm
R-S
0.43 nm
R-T
0.395 nm
S-T
0.365 nm
3-12-1
4-1
Souza et. al Nature Methods,2021.
4-1 3-1 2-1
- Well-balanced sizes- Improved
partitioning
- Improved barriers
for dissociation
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WELL-DEFINED MAPPING RULES
Souza et. al Nature Methods,2021.
Lecture and Tutorial:
Parametrization new CG models
20
MARTINI 3: THE BEAD LABELS
d a
Souza et. al Nature Methods,2021.
Electron poor (v) / Electron rich (e)
v e
H-donor (d) / H-acceptor (a)Credits: Vishal Maingi
Hydrogen bonding Electron polarizability
- The can be added to all P and N beads.
- Example: P1d, P1a beads use in
nucleobses .
- They can be added to all C and X beads.
- Example: C5e and C5v beads use in aedamers.
- A total of 9 new labels
are available.
- Considering:
Martini 2 Martini 3
Beads 54 843
Pair interactions 1,485 355,746
Parameters ~60 ~1,301chemical
types sizes labelsX X
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MARTINI 3 PROTEIN MODELS: STILL UNDER DEVELOPMENT
1) Models for side chains
• New models for all
side chains.
• No over or under-
mapping.
• Side chain dihedral
corrections
• Bead type does not
depends of the
secondary structure.
• Default bead is P2
• Exceptions: certain
residues as glycine
and proline.
• Mapping and bonded
parameters are still
based on Martini 2.
2) Model for
backbone
22Protein tutorials and Lecturer about
Elastic and Go Models
3) Bias to keep tertiary structure
Some examples of improvements in proteins
Souza et. al Nature Methods, 2021.
Improved protein-protein
interactions
Predicting binding modes
Proteins have cavities and pores now!
Coarse-graining and Martini
- Simple models that allow affordable, but
meaningful MD simulations.
Martini 3, a general purpose force-field:
- Improved interactions and packing
- Better coverage of chemical space
- Improvements in Martini 3
- Proteins are less sticky
- Cavities and channels are there now.
- New applications of Martini 3?
Take-home message
Lecturer
Siewert J. Marrink
Thanks!
Acknowledgements
Alex de VriesUniversity of Groningen
Riccardo AlessandriUniversity of Chicago
Jonathan BarnoudUniversity of Bristol
Sebastian ThallmairFrankfurt Institute for Advanced Studies
Siewert J. MarrinkUniversity of Groningen
Acknowledgements
University of Groningen
Ignacio Faustino
Fabian Grunewald
Ilias Patmanidis
Haleh Abdizadeh
Bart M.H. Bruininks
Tsjerk Wassenaar
Peter C. Kroon
Josef Melcr
Weria Pezeshkian
Melanie Konig
Petteri Vainikka
Carlos Ramírez-Palacios
Maria Tsanai.
University of Calgary
Valentina Corradi
D. Peter Tieleman
University of Bergen
Hanif M. Khan
Nathalie Reuter
Czech Academy of Sciences
Matti Javanainen
Hector Martinez-Seara
University of Helsinki
Ilpo Vattulainen
NIH – US
Jan Domanski (also Oxford)
Robert B. Best
PharmCADD
Sangwook Wu
CNRS/ University of Lyon
Vincent Nieto
Luca Monticelli
University of Auckland
Xavier Periole
Case Western Reserve University
Amita Sahoo
Matthias Buck
Polish Academy of Sciences
Rodrigo Moreira
Adolfo Poma
Università della Svizzera italiana
Paolo Conflitti
Stefano Raniolo
Vittorio Limongelli
Universidad de Santiago de Chile
Raúl Mera-Adasme
University of California San Diego
Clarisse Gravina Ricci
ITQB NOVA
Manuel Nuno Melo