4.2.5. Calculating root mean square quantities — MDAnalysis.analysis.rms

Author

Oliver Beckstein, David L. Dotson, John Detlefs

Year

2016

Copyright

GNU Public License v2

New in version 0.7.7.

Changed in version 0.11.0: Added RMSF analysis.

Changed in version 0.16.0: Refactored RMSD to fit AnalysisBase API

The module contains code to analyze root mean square quantities such as the coordinat root mean square distance (RMSD) or the per-residue root mean square fluctuations (RMSF).

This module uses the fast QCP algorithm [Theobald2005] to calculate the root mean square distance (RMSD) between two coordinate sets (as implemented in MDAnalysis.lib.qcprot.CalcRMSDRotationalMatrix()).

When using this module in published work please cite [Theobald2005].

See also

MDAnalysis.analysis.align

aligning structures based on RMSD

MDAnalysis.lib.qcprot

implements the fast RMSD algorithm.

4.2.5.1. Example applications

4.2.5.1.1. Calculating RMSD for multiple domains

In this example we will globally fit a protein to a reference structure and investigate the relative movements of domains by computing the RMSD of the domains to the reference. The example is a DIMS trajectory of adenylate kinase, which samples a large closed-to-open transition. The protein consists of the CORE, LID, and NMP domain.

• superimpose on the closed structure (frame 0 of the trajectory), using backbone atoms

• calculate the backbone RMSD and RMSD for CORE, LID, NMP (backbone atoms)

The trajectory is included with the test data files. The data in RMSD.results.rmsd is plotted with matplotlib.pyplot.plot() (see Figure RMSD plot figure):

import MDAnalysis
from MDAnalysis.tests.datafiles import PSF,DCD,CRD
u = MDAnalysis.Universe(PSF,DCD)
ref = MDAnalysis.Universe(PSF,DCD)     # reference closed AdK (1AKE) (with the default ref_frame=0)
#ref = MDAnalysis.Universe(PSF,CRD)    # reference open AdK (4AKE)

import MDAnalysis.analysis.rms

R = MDAnalysis.analysis.rms.RMSD(u, ref,
           select="backbone",             # superimpose on whole backbone of the whole protein
           groupselections=["backbone and (resid 1-29 or resid 60-121 or resid 160-214)",   # CORE
                            "backbone and resid 122-159",                                   # LID
                            "backbone and resid 30-59"])                                    # NMP
R.run()

import matplotlib.pyplot as plt
rmsd = R.results.rmsd.T   # transpose makes it easier for plotting
time = rmsd[1]
fig = plt.figure(figsize=(4,4))
ax = fig.add_subplot(111)
ax.plot(time, rmsd[2], 'k-',  label="all")
ax.plot(time, rmsd[3], 'k--', label="CORE")
ax.plot(time, rmsd[4], 'r--', label="LID")
ax.plot(time, rmsd[5], 'b--', label="NMP")
ax.legend(loc="best")
ax.set_xlabel("time (ps)")
ax.set_ylabel(r"RMSD ($\AA$)")
fig.savefig("rmsd_all_CORE_LID_NMP_ref1AKE.pdf")

RMSD plot for backbone and CORE, LID, NMP domain of the protein.

4.2.5.2. Functions

MDAnalysis.analysis.rms.rmsd(a, b, weights=None, center=False, superposition=False)

Returns RMSD between two coordinate sets a and b.

a and b are arrays of the coordinates of N atoms of shape \(N times 3\) as generated by, e.g., MDAnalysis.core.groups.AtomGroup.positions().

Note

If you use trajectory data from simulations performed under periodic boundary conditions then you must make your molecules whole before performing RMSD calculations so that the centers of mass of the mobile and reference structure are properly superimposed.

Parameters

• a (array_like) – coordinates to align to b

• b (array_like) – coordinates to align to (same shape as a)

• weights (array_like (optional)) – 1D array with weights, use to compute weighted average

• center (bool (optional)) – subtract center of geometry before calculation. With weights given compute weighted average as center.

• superposition (bool (optional)) – perform a rotational and translational superposition with the fast QCP algorithm [Theobald2005] before calculating the RMSD; implies center=True.

Returns

rmsd – RMSD between a and b

Return type

float

Notes

The RMSD \(\rho(t)\) as a function of time is calculated as

\[\rho(t) = \sqrt{\frac{1}{N} \sum_{i=1}^N w_i \left(\mathbf{x}_i(t) - \mathbf{x}_i^{\text{ref}}\right)^2}\]

It is the Euclidean distance in configuration space of the current configuration (possibly after optimal translation and rotation) from a reference configuration divided by \(1/\sqrt{N}\) where \(N\) is the number of coordinates.

The weights \(w_i\) are calculated from the input weights weights \(w'_i\) as relative to the mean:

\[w_i = \frac{w'_i}{\langle w' \rangle}\]

Example

>>> import MDAnalysis as mda
>>> from MDAnalysis.analysis.rms import rmsd
>>> from MDAnalysis.tests.datafiles import PSF, DCD
>>> u = mda.Universe(PSF, DCD)
>>> bb = u.select_atoms('backbone')
>>> A = bb.positions.copy()  # coordinates of first frame
>>> _ = u.trajectory[-1]  # forward to last frame
>>> B = bb.positions.copy()  # coordinates of last frame
>>> rmsd(A, B, center=True)
6.838544558398293

Changed in version 0.8.1: center keyword added

Changed in version 0.14.0: superposition keyword added

4.2.5.3. Analysis classes

class MDAnalysis.analysis.rms.RMSD(atomgroup, reference=None, select='all', groupselections=None, weights=None, weights_groupselections=False, tol_mass=0.1, ref_frame=0, **kwargs)

Class to perform RMSD analysis on a trajectory.

The RMSD will be computed for two groups of atoms and all frames in the trajectory belonging to atomgroup. The groups of atoms are obtained by applying the selection selection select to the changing atomgroup and the fixed reference.

Note

If you use trajectory data from simulations performed under periodic boundary conditions then you must make your molecules whole before performing RMSD calculations so that the centers of mass of the selected and reference structure are properly superimposed.

Run the analysis with RMSD.run(), which stores the results in the array RMSD.results.rmsd.

Changed in version 1.0.0: save() method was removed, use np.savetxt() on RMSD.results.rmsd instead.

Changed in version 2.0.0: rmsd results are now stored in a MDAnalysis.analysis.base.Results instance.

Parameters

• atomgroup (AtomGroup or Universe) – Group of atoms for which the RMSD is calculated. If a trajectory is associated with the atoms then the computation iterates over the trajectory.

• reference (AtomGroup or Universe (optional)) – Group of reference atoms; if None then the current frame of atomgroup is used.

• select (str or dict or tuple (optional)) –

  The selection to operate on; can be one of:

  1. any valid selection string for select_atoms() that produces identical selections in atomgroup and reference; or

  2. a dictionary {'mobile': sel1, 'reference': sel2} where sel1 and sel2 are valid selection strings that are applied to atomgroup and reference respectively (the MDAnalysis.analysis.align.fasta2select() function returns such a dictionary based on a ClustalW or STAMP sequence alignment); or

  3. a tuple (sel1, sel2)

  When using 2. or 3. with sel1 and sel2 then these selection strings are applied to atomgroup and reference respectively and should generate groups of equivalent atoms. sel1 and sel2 can each also be a list of selection strings to generate a AtomGroup with defined atom order as described under Ordered selections).

• groupselections (list (optional)) –

  A list of selections as described for select, with the difference that these selections are always applied to the full universes, i.e., atomgroup.universe.select_atoms(sel1) and reference.universe.select_atoms(sel2). Each selection describes additional RMSDs to be computed after the structures have been superimposed according to select. No additional fitting is performed.The output contains one additional column for each selection.

  Note

  Experimental feature. Only limited error checking implemented.

• weights ({“mass”, None} or array_like (optional)) –

  1. “mass” will use masses as weights for both select and groupselections.

  2. None will weigh each atom equally for both select and groupselections.

  3. If 1D float array of the same length as atomgroup is provided, use each element of the array_like as a weight for the corresponding atom in select, and assumes None for groupselections.

• weights_groupselections (False or list of {“mass”, None or array_like} (optional)) –

  1. False will apply imposed weights to groupselections from weights option if weights is either "mass" or None. Otherwise will assume a list of length equal to length of groupselections filled with None values.

  2. A list of {“mass”, None or array_like} with the length of groupselections will apply the weights to groupselections correspondingly.

• tol_mass (float (optional)) – Reject match if the atomic masses for matched atoms differ by more than tol_mass.

• ref_frame (int (optional)) – frame index to select frame from reference

• verbose (bool (optional)) – Show detailed progress of the calculation if set to True; the default is False.

Raises

• SelectionError – If the selections from atomgroup and reference do not match.

• TypeError – If weights or weights_groupselections is not of the appropriate type; see also MDAnalysis.lib.util.get_weights()

• ValueError – If weights are not compatible with atomgroup (not the same length) or if it is not a 1D array (see MDAnalysis.lib.util.get_weights()). A ValueError is also raised if the length of weights_groupselections are not compatible with groupselections.

Notes

The root mean square deviation \(\rho(t)\) of a group of \(N\) atoms relative to a reference structure as a function of time is calculated as

\[\rho(t) = \sqrt{\frac{1}{N} \sum_{i=1}^N w_i \left(\mathbf{x}_i(t) - \mathbf{x}_i^{\text{ref}}\right)^2}\]

The weights \(w_i\) are calculated from the input weights weights \(w'_i\) as relative to the mean of the input weights:

\[w_i = \frac{w'_i}{\langle w' \rangle}\]

The selected coordinates from atomgroup are optimally superimposed (translation and rotation) on the reference coordinates at each time step as to minimize the RMSD. Douglas Theobald’s fast QCP algorithm [Theobald2005] is used for the rotational superposition and to calculate the RMSD (see MDAnalysis.lib.qcprot for implementation details).

The class runs various checks on the input to ensure that the two atom groups can be compared. This includes a comparison of atom masses (i.e., only the positions of atoms of the same mass will be considered to be correct for comparison). If masses should not be checked, just set tol_mass to a large value such as 1000.

See also

rmsd

New in version 0.7.7.

Changed in version 0.8: groupselections added

Changed in version 0.16.0: Flexible weighting scheme with new weights keyword.

Deprecated since version 0.16.0: Instead of mass_weighted=True (removal in 0.17.0) use new weights='mass'; refactored to fit with AnalysisBase API

Changed in version 0.17.0: removed deprecated mass_weighted keyword; groupselections are not rotationally superimposed any more.

Changed in version 1.0.0: filename keyword was removed.

results.rmsd

Contains the time series of the RMSD as an N×3 numpy.ndarray array with content [[frame, time (ps), RMSD (A)], [...], ...].

New in version 2.0.0.

rmsd

Alias to the results.rmsd attribute.

Deprecated since version 2.0.0: Will be removed in MDAnalysis 3.0.0. Please use results.rmsd instead.

run(start=None, stop=None, step=None, frames=None, verbose=None, *, progressbar_kwargs={})

Perform the calculation

Parameters

• start (int, optional) – start frame of analysis

• stop (int, optional) – stop frame of analysis

• step (int, optional) – number of frames to skip between each analysed frame

• frames (array_like, optional) –

  array of integers or booleans to slice trajectory; frames can only be used instead of start, stop, and step. Setting both frames and at least one of start, stop, step to a non-default value will raise a ValueError.

  New in version 2.2.0.

• verbose (bool, optional) – Turn on verbosity

• progressbar_kwargs (dict, optional) – ProgressBar keywords with custom parameters regarding progress bar position, etc; see MDAnalysis.lib.log.ProgressBar for full list.

Changed in version 2.2.0: Added ability to analyze arbitrary frames by passing a list of frame indices in the frames keyword argument.

Changed in version 2.5.0: Add progressbar_kwargs parameter, allowing to modify description, position etc of tqdm progressbars

class MDAnalysis.analysis.rms.RMSF(atomgroup, **kwargs)

Calculate RMSF of given atoms across a trajectory.

Note

No RMSD-superposition is performed; it is assumed that the user is providing a trajectory where the protein of interest has been structurally aligned to a reference structure (see the Examples section below). The protein also has be whole because periodic boundaries are not taken into account.

Run the analysis with RMSF.run(), which stores the results in the array RMSF.results.rmsf.

Parameters

• atomgroup (AtomGroup) – Atoms for which RMSF is calculated

• verbose (bool (optional)) – Show detailed progress of the calculation if set to True; the default is False.

Raises

ValueError – raised if negative values are calculated, which indicates that a numerical overflow or underflow occured

Notes

The root mean square fluctuation of an atom \(i\) is computed as the time average

\[\rho_i = \sqrt{\left\langle (\mathbf{x}_i - \langle\mathbf{x}_i\rangle)^2 \right\rangle}\]

No mass weighting is performed.

This method implements an algorithm for computing sums of squares while avoiding overflows and underflows [Welford1962].

Examples

In this example we calculate the residue RMSF fluctuations by analyzing the \(\text{C}_\alpha\) atoms. First we need to fit the trajectory to the average structure as a reference. That requires calculating the average structure first. Because we need to analyze and manipulate the same trajectory multiple times, we are going to load it into memory using the MemoryReader. (If your trajectory does not fit into memory, you will need to write out intermediate trajectories to disk or generate an in-memory universe that only contains, say, the protein):

import MDAnalysis as mda
from MDAnalysis.analysis import align

from MDAnalysis.tests.datafiles import TPR, XTC

u = mda.Universe(TPR, XTC, in_memory=True)
protein = u.select_atoms("protein")

# 1) the current trajectory contains a protein split across
#    periodic boundaries, so we first make the protein whole and
#    center it in the box using on-the-fly transformations
import MDAnalysis.transformations as trans

not_protein = u.select_atoms('not protein')
transforms = [trans.unwrap(protein),
              trans.center_in_box(protein, wrap=True),
              trans.wrap(not_protein)]
u.trajectory.add_transformations(*transforms)

# 2) fit to the initial frame to get a better average structure
#    (the trajectory is changed in memory)
prealigner = align.AlignTraj(u, u, select="protein and name CA",
                             in_memory=True).run()

# 3) reference = average structure
ref_coordinates = u.trajectory.timeseries(asel=protein).mean(axis=1)
# make a reference structure (need to reshape into a 1-frame
# "trajectory")
reference = mda.Merge(protein).load_new(ref_coordinates[:, None, :],
                                        order="afc")

We created a new universe reference that contains a single frame with the averaged coordinates of the protein. Now we need to fit the whole trajectory to the reference by minimizing the RMSD. We use MDAnalysis.analysis.align.AlignTraj:

aligner = align.AlignTraj(u, reference,
                          select="protein and name CA",
                          in_memory=True).run()

The trajectory is now fitted to the reference (the RMSD is stored as aligner.results.rmsd for further inspection). Now we can calculate the RMSF:

from MDAnalysis.analysis.rms import RMSF

calphas = protein.select_atoms("name CA")
rmsfer = RMSF(calphas, verbose=True).run()

and plot:

import matplotlib.pyplot as plt

plt.plot(calphas.resnums, rmsfer.results.rmsf)

References

Welford1962

B. P. Welford. Note on a method for calculating corrected sums of squares and products. Technometrics, 4(3):419–420, 1962. doi:10.1080/00401706.1962.10490022.

New in version 0.11.0.

Changed in version 0.16.0: refactored to fit with AnalysisBase API

Deprecated since version 0.16.0: the keyword argument quiet is deprecated in favor of verbose.

Changed in version 0.17.0: removed unused keyword weights

Changed in version 1.0.0: Support for the start, stop, and step keywords has been removed. These should instead be passed to RMSF.run().

results.rmsf

Results are stored in this N-length numpy.ndarray array, giving RMSFs for each of the given atoms.

New in version 2.0.0.

rmsf

Alias to the results.rmsf attribute.

Deprecated since version 2.0.0: Will be removed in MDAnalysis 3.0.0. Please use results.rmsf instead.

run(start=None, stop=None, step=None, frames=None, verbose=None, *, progressbar_kwargs={})

Perform the calculation

Parameters

• start (int, optional) – start frame of analysis

• stop (int, optional) – stop frame of analysis

• step (int, optional) – number of frames to skip between each analysed frame

• frames (array_like, optional) –

  array of integers or booleans to slice trajectory; frames can only be used instead of start, stop, and step. Setting both frames and at least one of start, stop, step to a non-default value will raise a ValueError.

  New in version 2.2.0.

• verbose (bool, optional) – Turn on verbosity

• progressbar_kwargs (dict, optional) – ProgressBar keywords with custom parameters regarding progress bar position, etc; see MDAnalysis.lib.log.ProgressBar for full list.

Changed in version 2.2.0: Added ability to analyze arbitrary frames by passing a list of frame indices in the frames keyword argument.

Changed in version 2.5.0: Add progressbar_kwargs parameter, allowing to modify description, position etc of tqdm progressbars