1 / 19

Molecular Mechanics

Molecular Mechanics. Calculation of energy of atoms, force on atoms & their resulting motion Newtonian mechanics Use Improve trial structure by eliminating distortion, steric clashes, finding better conformation. Study motion of molecule eg rigid body motion of domains etc. Potential Energy.

nola
Télécharger la présentation

Molecular Mechanics

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Molecular Mechanics • Calculation of energy of atoms, force on atoms & their resulting motion • Newtonian mechanics • Use • Improve trial structure by eliminating distortion, steric clashes, finding better conformation. • Study motion of molecule eg rigid body motion of domains etc

  2. Potential Energy • Components • (1) bond length Bonds behave like spring with equilibrium bond length depending on bond type. Increase or decrease from equilibrium length requires higher energy.

  3. Potential Energy • (2) bond angle • Bond angles have equilibrium value eg 108 for H-C-H • Behave as if sprung. • Increase or decrease in angle requires higher energy.

  4. Potential Energy • (3) torsion angle Rotation can occur about single bond in A-B-C-D but energy depends on torsion angle (angle between CD & AB viewed along BC). Staggered conformations (angle +60, -60 or 180 are preferred). .

  5. Potential Energy • (4) van der Waals interactions Interactions between atoms not near neighbours expressed by Lennard-Jones potential. Very high repulsive force if atoms closer than sum of van der Waals radii. Attractive force if distance greater. Because of strong distance dependence, van der Waals interactions become negligible at distances over 15 A

  6. Potential Energy • (5) Electrostatic interactions • All atoms have partial charge eg in C=O C has partial positive charge, O atom partial negative charge. • Two atoms that have the same charge repel one another, those with unlike charge attract. • Dielectric constant to use in uncertain. • Dipoles. In many cases molecules made of neutral groups. Two adjacent atoms have opposite charges & behave like dipole. In this case the potential energy falls off as 1/r3 • Electrostatic energy falls off much less quickly than for van der Waals interactions and may not be negligible even at 30 A.

  7. Potential Energy • Cut off • Calculation of interaction between non-bonded atoms takes most of the computation • This is lessened if a cut off distance is applied - assumed that above this distance the interaction between two atoms is negligible

  8. Potential Energy • Potential Energy is given by the sum of these contributions: Hydrogen bonds are usually supposed to arise by electrostatic interactions but occasionally a small extra term is added.

  9. Potential To reduce the complexity of calculations atoms grouped into types (potential atom types) • eg all H´s in methane are the same & similar to H´s in ethane • the C atoms in ethane are different from those in ethylene • the O in a C=O group is different from the O in a C-O-H group. But O atoms in alcohols are similar.

  10. Force fields • A force field is the description of how potential energy depends on parameters • Several force fields are available • AMBER used for proteins and nucleic acids • cvff (consistent valence force field) Force fields differ: in the precise form of the equations in values of the constants for each atom type

  11. Energy minimisation • Calculation of how atoms should move to minimise TOTAL potential energy • At minimum, forces on every atom are zero. • Optimising structure to remove strain & steric clashes • However, in general finds local rather than global minimum. Energy barriers are not overcome even if much lower energy state is possible ie structures may be locked in. Hence not useful as a search strategy.

  12. Energy minimisation • Potential energy depends on many parameters • Problem of finding minimum value of a function with >1 parameters. Know value of function at several points. • Grid search is computationally not feasible • Methods • Steepest descents • Conjugate gradients

  13. Energy minimisation Example 1 Hexabenzene ring has been made in InsightII. The strain is small. This will be energy minimised. Example 2 Pentabenzene ring has been made in InsightII. This has a large strain which will be reduced on energy minimisation.

  14. Energy minimisation Example 3 Energy minimisation of ADP+Pi at the active site of myosin. The crystal structure used is the motor domain complexed with ADP+vanadate and the vanadate has been replaced by Pi. What happens to the stereochemistry of the Pi? Example 4 Energy minimisation of GTP at the active site of myosin. ATP has been replaced by GTP. How does the guanine base fit?

  15. Molecular dynamics • Energy minimisation gives local minimum, not necessarily global minimum. • Give molecule thermal energy so can explore conformational space & overcome energy barriers. • Give atoms initial velocity random value + direction. Scale velocities so total kinetic energy =3/2kT * number atoms • Solve equation of motion to work out position of atoms at 1 fs.

  16. Molecular dynamics • Higher the temperature the greater and faster the motion & more of conformational space sampled. • Use • (a) to overcome energy barriers to find better structure • (b) explore motion

  17. Molecular Dynamics Example 1 Molecular dynamics simulation of pentabenzene

  18. Molecular Dynamics Example 2 Molecular dynamics simulation showing movement of ATP, Mg, side chains and water in the active site of myosin.

  19. Water • A protein is surrounded with water molecules. Side chains on surface of interact with water. Modelling a protein without water is not realistic. • Ideally surround protein with large bath of water. But computationally intensive & large number of combinations of water positions & interactions • In practice surround protein with thin layer of water.

More Related