aanma | R Documentation |
Perform all-atom elastic network model normal modes calculation of a protein structure.
aanma(...)
## S3 method for class 'pdb'
aanma(pdb, pfc.fun = NULL, mass = TRUE, temp = 300,
keep = NULL, hessian = NULL, outmodes = "calpha", rm.wat = TRUE,
reduced = FALSE, rtb = FALSE, nmer = 1, ...)
rtb(hessian, pdb, mass = TRUE, nmer = 1, verbose = TRUE)
... |
additional arguments to |
pdb |
an object of class |
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. If NULL, the default function ‘aaenm2’ will be employed. (See details below). |
mass |
logical, if TRUE the Hessian will be mass-weighted. |
temp |
numerical, temperature for which the amplitudes for scaling the atomic displacement vectors are calculated. Set ‘temp=NULL’ to avoid scaling. |
keep |
numerical, final number of modes to be stored. Note that all subsequent analyses are limited to this subset of modes. This option is useful for very large structures and cases where memory may be limited. |
hessian |
hessian matrix as obtained from |
outmodes |
either a character (‘calpha’ or ‘noh’) or atom
indices as obtained from |
rm.wat |
logical, if TRUE water molecules will be removed before calculation. |
reduced |
logical, if TRUE the coarse-grained (‘4-bead’) ENM will be employed. (See details below). |
rtb |
logical, if TRUE the rotation-translation block based approximate modes will be calculated. (See details below). |
nmer |
numerical, defines the number of residues per block (used only
when |
verbose |
logical, if TRUE print detailed processing message |
This function builds an elastic network model (ENM) based on all
heavy atoms of input pdb
, and performs subsequent normal mode
analysis (NMA) in various manners. By default, the ‘aaenm2’ force
field (defining of the spring constants between atoms) is used, which was
obtained by fitting to a local energy minimum of a crambin model
derived from the AMBER99SB force field. It employs a pair force constant
function which falls as r^-6, and specific force constants for
covalent and intra-residue atom pairs. See also load.enmff
for other force field options.
The outmodes
argument controls the type of output modes. There are
two standard types of output modes: ‘noh’ and ‘calpha’.
outmodes='noh'
invokes regular all-atom based ENM-NMA. When
outmodes='calpha'
, an effective Hessian with respect to all C-alpha
atoms will be first calculated using the same formula as in Hinsen et al.
NMA is then performed on this effective C-alpha based Hessian. In addition,
users can provide their own atom selection (see atom.select
)
as the value of outmodes
for customized output modes generation.
When reduced=TRUE
, only a selection of all heavy atoms is used
to build the ENM. More specifically, three to five atoms per residue
constitute the model. Here the N, CA, C atoms represent the protein
backbone, and zero to two selected side chain atoms represent the side chain
(selected based on side chain size and the distance to CA). This
coarse-grained ENM has significantly improved computational efficiency and
similar prediction accuracy with respect to the all-atom ENM.
When rtb=TRUE
, rotation-translation block (RTB) based approximate
modes will be calculated. In this method, each residue is assumed to be a
rigid body (or ‘block’) that has only rotational and translational
degrees of freedom. Intra-residue deformation is thus ignored.
(See Durand et al 1994 and Tama et al. 2000 for more details). N residues per
block is also supported, where N=1, 2, 3, etc. (See argument nmer
).
The RTB method has significantly improved computational efficiency and
similar prediction accuracy with respect to the all-atom ENM.
By default the function will diagonalize the mass-weighted Hessian matrix. The resulting mode vectors are moreover scaled by the thermal fluctuation amplitudes.
Returns an object of class ‘nma’ with the following components:
modes |
numeric matrix with columns containing the normal mode
vectors. Mode vectors are converted to unweighted Cartesian
coordinates when |
frequencies |
numeric vector containing the vibrational
frequencies corresponding to each mode (for |
force.constants |
numeric vector containing the force constants
corresponding to each mode (for |
fluctuations |
numeric vector of atomic fluctuations. |
U |
numeric matrix with columns containing the raw
eigenvectors. Equals to the |
L |
numeric vector containing the raw eigenvalues. |
xyz |
numeric matrix of class |
mass |
numeric vector containing the residue masses used for the mass-weighting. |
temp |
numerical, temperature for which the amplitudes for scaling the atomic displacement vectors are calculated. |
triv.modes |
number of trivial modes. |
natoms |
number of C-alpha atoms. |
call |
the matched call. |
Lars Skjaerven & Xin-Qiu Yao
Hinsen, K. et al. (2000) Chem. Phys. 261, 25. Durand, P. et al. (1994) Biopolymers 34, 759. Tama, F. et al. (2000) Proteins 41, 1.
nma.pdb
for C-alpha based NMA, aanma.pdbs
for
ensemble all-atom NMA, load.enmff
for available ENM force
fields, and fluct.nma
, mktrj.nma
, and
dccm.nma
for various post-NMA calculations.
## Not run:
# All-atom NMA takes relatively long time - Don't run by default.
## Fetch stucture
pdb <- read.pdb( system.file("examples/1hel.pdb", package="bio3d") )
## Calculate all-atom normal modes
modes.aa <- aanma(pdb, outmodes='noh')
## Calculate all-atom normal modes with RTB approximation
modes.aa.rtb <- aanma(pdb, outmodes='noh', rtb=TRUE)
## Compare the two modes
rmsip(modes.aa, modes.aa.rtb)
## Calculate C-alpha normal modes.
modes <- aanma(pdb)
## Calculate C-alpha normal modes with reduced ENM.
modes.cg <- aanma(pdb, reduced=TRUE)
## Calculate C-alpha normal modes with RTB approximation
modes.rtb <- aanma(pdb, rtb=TRUE)
## Compare modes
rmsip(modes, modes.cg)
rmsip(modes, modes.rtb)
## Print modes
print(modes)
## Plot modes
plot(modes)
## Visualize modes
#m7 <- mktrj.nma(modes, mode=7, file="mode_7.pdb", pdb=pdb)
## End(Not run)
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