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Description
Issue created to implement contact definition from the paper from Best, Hummer, and Eaton, "Native contacts determine protein folding mechanisms in atomistic simulations" PNAS (2013).
There was a snniped in mdtraj that could be used:
def best_hummer_q(traj, native):
"""Compute the fraction of native contacts according the definition from
Best, Hummer and Eaton [1]
Parameters
----------
traj : md.Trajectory
The trajectory to do the computation for
native : md.Trajectory
The 'native state'. This can be an entire trajectory, or just a single frame.
Only the first conformation is used
Returns
-------
q : np.array, shape=(len(traj),)
The fraction of native contacts in each frame of `traj`
References
----------
..[1] Best, Hummer, and Eaton, "Native contacts determine protein folding
mechanisms in atomistic simulations" PNAS (2013)
"""
BETA_CONST = 50 # 1/nm
LAMBDA_CONST = 1.8
NATIVE_CUTOFF = 0.45 # nanometers
# get the indices of all of the heavy atoms
heavy = native.topology.select_atom_indices("heavy")
# get the pairs of heavy atoms which are farther than 3
# residues apart
heavy_pairs = np.array(
[
(i, j)
for (i, j) in combinations(heavy, 2)
if abs(
native.topology.atom(i).residue.index
- native.topology.atom(j).residue.index
)
> 3
]
)
# compute the distances between these pairs in the native state
heavy_pairs_distances = md.compute_distances(native[0], heavy_pairs)[0]
# and get the pairs s.t. the distance is less than NATIVE_CUTOFF
native_contacts = heavy_pairs[heavy_pairs_distances < NATIVE_CUTOFF]
print("Number of native contacts", len(native_contacts))
# now compute these distances for the whole trajectory
r = md.compute_distances(traj, native_contacts)
# and recompute them for just the native state
r0 = md.compute_distances(native[0], native_contacts)
q = np.mean(
1.0 / (1 + np.exp(BETA_CONST * (r - LAMBDA_CONST * r0))), axis=1
)
return q
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