deformation.nma: Deformation Analysis

In bio3d: Biological Structure Analysis

Deformation Analysis

Description

Calculate deformation energies from Normal Mode Analysis.

Usage

deformation.nma(nma, mode.inds = NULL, pfc.fun = NULL, ncore = NULL)

Arguments

nma	a list object of class "nma" (obtained with nma).
mode.inds	a numeric vector of mode indices in which the calculation should be based.
pfc.fun	customized pair force constant (‘pfc’) function. The provided function should take a vector of distances as an argument to return a vector of force constants. See nma for examples.
ncore	number of CPU cores used to do the calculation. ncore>1 requires package ‘parallel’ installed.

Details

Deformation analysis provides a measure for the amount of local flexibility of the protein structure - i.e. atomic motion relative to neighbouring atoms. It differs from ‘fluctuations’ (e.g. RMSF values) which provide amplitudes of the absolute atomic motion.

Deformation energies are calculated based on the nma object. By default the first 20 non-trivial modes are included in the calculation.

See examples for more details.

Value

Returns a list with the following components:

ei	numeric matrix containing the energy contribution (E) from each atom (i; row-wise) at each mode index (column-wise).
sums	deformation energies corresponding to each mode.

Author(s)

Lars Skjaerven

References

Hinsen, K. (1998) Proteins 33, 417–429. Grant, B.J. et al. (2006) Bioinformatics 22, 2695–2696.

See Also

nma

Examples

# Running the example takes some time - testing excluded

## Fetch stucture
pdb <- read.pdb( system.file("examples/1hel.pdb", package="bio3d") )

## Calculate (vibrational) normal modes
modes <- nma(pdb)

## Calculate deformation energies
def.energies <- deformation.nma(modes)


## Not run: 
## Fluctuations of first non-trivial mode
def.energies <- deformation.nma(modes, mode.inds=seq(7, 16))

write.pdb(pdb=NULL, xyz=modes$xyz,
          b=def.energies$ei[,1])

## End(Not run)

bio3d documentation built on Oct. 30, 2024, 1:08 a.m.