Title: Molecular Dynamics simulations
1Molecular Dynamics simulations
Bert de Groot Max Planck institute for
biophysical chemistry Göttingen, Germany
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3Molecular Dynamics Simulations
Schrödinger equation
Born-Oppenheimer approximation
Nucleic motion described classically
Empirical force field
4Molecular Dynamics Simulations
Interatomic interactions
5Molecular dynamics-(MD) simulations of Biopolymers
- Motions of nuclei are described classically,
- Potential function Eel describes the electronic
influence on motions of the nuclei and is
approximated empirically ? classical MD
Covalent bonds
Non-bonded interactions
Eibond
approximated
exact
KBT
?0
R
6Force-Field
7Molecular Dynamics Simulation
Molecule (classical) N-particle
system Newtonian equations of motion
with
Integrate numerically via the leapfrog scheme
with ?t ? 1fs!
(equivalent to the Verlet algorithm)
8BPTI Molecular Dynamics (300K)
9Computational task
Solve the Newtonian equations of motion
10Non-bonded interactions
Coulomb potential
Lennard-Jones potential
11Use of constraints toincrease the integration
step
The SHAKE algorithm
?t 1fs --gt 2 fs
12Molecular dynamics is very expensive ...
Example F1-ATPase in water (183 674 atoms), 1
nanosecond 106 integration steps 8.4
1011 flop per step n(n-1)/2 interactions
total 8.4 1017 flop on a 100 Mflop/s
workstation ca 250 years ...but performance
has been improved by use of multiple time
stepping ca. 25 years structure
adapted multipole methods ca. 6 years
FAMUSAMM ca. 2 years parallel
computers ca. 55 days
13- Limits of MD-Simulations
- classical description chemical
reactions not described poor description of
H-atoms (proton-transfer) poor description of
low-T (quantum) effects simplified
electrostatic model simplified force field - only small systems accessible (104 ... 106
atoms) - only short time spans accessible (ps ... µs)
14MD-Experiments with Argon Gas
15Role of environment - solvent
explicit or implicit?
box or droplet?
16Surface (tension) effects?
periodic boundary conditions
and the minimum image convention
17Proteins jump between many, hierarchically
ordered conformational substates
H. Frauenfelder et al., Science 229 (1985) 337
18Reversible Folding Dynamics of a ß-Peptide
X. Daura, B. Jaun, D. Seebach, W.F. van
Gunsteren, A.E. Mark, J. Mol. Biol. 280 (1998) 925
19- MD Simulations
- external coupling temperature
(potential truncation, integration errors)
pressure (density equilibration) system
translation/rotation - analysis
- energies (individual terms, pressure,
temperature) coordinates (numerical analysis,
visual inspection!) ? mechanisms -
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