def simulationFPT(trajectorynum):
'''
Calculates first passage time of a trajectory with random initial
conditions and final state the trimer state
:param trajectorynum: number of trajectories on which to calculate the FPT
:return: state, first passage time
'''
# Define dummy trajectory to extract bound states from python (needed to use getState function)
dummyTraj = msmrd2.trajectories.patchyDimer2(2, 1)
# Require more lax tolerances since trimer bends the dimer binding angle and shortens the distance
# (can be tested this works very well by plotting with vmd).
dummyTraj.setTolerances(0.50, 0.5 * 2 * np.pi)
# Define simulation boundaries (choose either spherical or box)
boxBoundary = msmrd2.box(boxsize, boxsize, boxsize, 'periodic')
# Define potential
potentialPatchyParticleAngular2 = patchyParticleAngular2(
sigma, strength, angularStrength, patchesCoordinates)
# Define integrator and boundary (over-damped Langevin)
seed = int(-1 * trajectorynum) # Negative seed, uses random device as seed
integrator = odLangevinSelective(dt, seed, bodytype)
integrator.setBoundary(boxBoundary)
integrator.setPairPotential(potentialPatchyParticleAngular2)
# Generate random position and orientation particle list with two particles
seed = int(trajectorynum)
partlist = particleTools.randomParticleList(numparticles, boxsize,
overlapThreshold, D, Drot,
seed)
# Set activePatchList
for part in partlist:
part.setActivePatchList(len(patchesCoordinates))
# Calculates the first passage times for the trime. Each trajectory is integrated until
# a bound state is reached. The output in the files is the elapsed time.
unbound = True
ii = 0
while (unbound):
ii += 1
integrator.integrate(partlist)
# Check status every 5000 timesteps (adds possible error of up to 5000*dt = 0.5), but
# speeds up simulations
if (ii % 5000 == 0):
ringFormations = integrator.findClosedBindingLoops(partlist)
if (3 in ringFormations):
unbound = False
return 'trimeric-loop', integrator.clock
elif (4 in ringFormations):
unbound = False
return 'tetrameric-loop', integrator.clock
elif (5 in ringFormations):
unbound = False
return "pentameric-loop", integrator.clock
elif integrator.clock >= 400.0:
unbound = False
return 'Failed at:', integrator.clock
def runParallelSims(simnumber):
# Define seed
seed = int(simnumber)
random.seed(seed)
# Create unbound MSMlist (CTMSMs)
# MSM for particle type0
MSMtype = 0
markovModel0 = ctmsm(MSMtype, -1 * seed) # random variable seed
D0list = np.array([1.0])
Drot0list = np.array([1.0])
markovModel0.setD(D0list)
markovModel0.setDrot(Drot0list)
# MSM for particle type1
MSMtype = 1
ratematrix = np.array([[-0.5, 0.5], [6.0, -6.0]])
markovModel1 = ctmsm(MSMtype, ratematrix, -2 * seed)
D1list = np.array([0.5, 1.0])
Drot1list = np.array([0.5, 1.0])
markovModel1.setD(D1list)
markovModel1.setDrot(Drot1list)
unboundMSMlist = [markovModel0, markovModel1]
# Define boundary
boxBoundary = msmrd2.box(boxsize, boxsize, boxsize, boundaryType)
# Define particle list
particleList = particleTools.randomParticleMSList(Nparticles, boxsize,
separationDistance,
particleTypes,
unboundMSMlist, seed)
# Defines patchy protein potential
potentialPatchyProteinMS = patchyProteinMarkovSwitch(
sigma, strength, angularStrength, patchesCoordinates1,
patchesCoordinates2)
# Integrator definition
seed = int(
-1 * simnumber
) # random seed (negative and different for every simulation, good for parallelization)
integrator = odLangevinMS(unboundMSMlist, dt, seed, bodytype)
integrator.setBoundary(boxBoundary)
integrator.setPairPotential(potentialPatchyProteinMS)
# Creates simulation
sim = msmrd2.simulation(integrator)
# Output filename definition
filename = basefilename + "_{:04d}".format(simnumber)
# Runs simulation
sim.run(particleList, timesteps, stride, bufferSize, filename, outTxt,
outH5, outChunked, trajtype)
print("Simulation " + str(simnumber) + ", done.")
def simulationFPT(trajectorynum):
'''
Calculates first passage time of a trajectory with random initial
conditions and final state a bound state
:param trajectorynum: number of trajectories on which to calculate the FPT
:return: state, first passage time
'''
# Define dummy trajectory to extract bound states from python (needed to use getState function)
dummyTraj = msmrd2.trajectories.patchyDimer(2, 1, radialBounds[0], minimumUnboundRadius)
# Define simulation boundaries (choose either spherical or box)
boxBoundary = msmrd2.box(boxsize, boxsize, boxsize, 'periodic')
# Define potential
potentialPatchyParticleAngular = patchyParticleAngular(sigma, strength, angularStrength, patchesCoordinates)
# Define integrator and boundary (over-damped Langevin)
seed = int(-1*trajectorynum) # Negative seed, uses random device as seed
integrator = odLangevin(dt, seed, bodytype)
integrator.setBoundary(boxBoundary)
integrator.setPairPotential(potentialPatchyParticleAngular)
# Generate random position and orientation particle list with two particles
seed = int(trajectorynum)
partlist = generateParticleList(initialState, boxsize, D, Drot, seed)
# Calculates the first passage times for a given bound state. Each trajectory is integrated until
# the target bound state is reached. The output in the files is the elapsed time.
intransition = True
while(intransition):
integrator.integrate(partlist)
currentState = dummyTraj.getState(partlist[0], partlist[1])
if targetState == 'A' and currentState in boundStatesA:
intransition = False
return 'A', integrator.clock
elif targetState == 'B' and currentState in boundStatesB:
intransition = False
return 'B', integrator.clock
elif integrator.clock >= 10000.0:
intransition = False
return 'Failed at:', integrator.clock
boxsize = parameterDictionary['boxsize']
boundaryType = parameterDictionary['boundaryType']
# Calculated parameters
#dtEffective = dt*stride # needed to obtain rate dictionary
effectivetimeSteps = int(totalTimeSteps / stride)
fnamebase = parentDirectory + 'simDimer_'
bufferSize = effectivetimeSteps
# Set trajectory discretizator
#radialLowerBound = 1.25 #default values
#radialUpperBound = 2.25 #default values
discretizator = msmrd2.trajectories.patchyDimer(numParticles, bufferSize)
# Set boundary (important for discretizer)
boxBoundary = msmrd2.box(boxsize, boxsize, boxsize, boundaryType)
discretizator.setBoundary(boxBoundary)
# Loads H5 files and generates discrete trajectories at once directly on c++.
dtrajs = []
for i in range(nfiles):
filename = fnamebase + str(i).zfill(4) + '.h5'
dtraj = discretizator.discretizeTrajectoryH5(filename)
dtrajs.append(dtraj)
print("Loading file ", i + 1, " of ", nfiles, " done.", end="\r")
print("\nDone loading files")
# Write discrete trajectory to xyz files
for i, dtraj in enumerate(dtrajs):
datafile = open(fnamebase + str(i).zfill(4) + '_discrete.xyz', 'w')
for j in range(len(dtraj)):
def simulationFPT(trajectorynum):
'''
Calculates first passage time of a trajectory with random initial
conditions and final state a bound state
:param trajectorynum: number of trajectories on which to calculate the FPT
:return: state, first passage time
'''
# Define dummy trajectory to extract bound states from python (needed to use getState function)
dummyTraj = msmrd2.trajectories.patchyProtein(numparticles, 1024,
radialBounds[0],
minimumUnboundRadius)
# Define base seed
seed = int(-1 * trajectorynum) # Negative seed, uses random device as seed
# Create unbound MSMlist (CTMSMs)
# MSM for particle type0
MSMtype = 0
markovModel0 = ctmsm(MSMtype, -1 * seed) # random variable seed
D0list = np.array([1.0])
Drot0list = np.array([1.0])
markovModel0.setD(D0list)
markovModel0.setDrot(Drot0list)
# MSM for particle type1
MSMtype = 1
ratematrix = np.array([[-0.5, 0.5], [6.0, -6.0]])
markovModel1 = ctmsm(MSMtype, ratematrix, -2 * seed)
D1list = np.array([0.5, 1.0])
Drot1list = np.array([0.5, 1.0])
markovModel1.setD(D1list)
markovModel1.setDrot(Drot1list)
unboundMSMlist = [markovModel0, markovModel1]
# Define simulation boundaries (choose either spherical or box)
boxBoundary = msmrd2.box(boxsize, boxsize, boxsize, 'periodic')
# Define potential
potentialPatchyProtein = patchyProteinMarkovSwitch(sigma, strength,
angularStrength,
patchesCoordinates1,
patchesCoordinates2)
# Define integrator and boundary (over-damped Langevin)
integrator = odLangevinMS(unboundMSMlist, dt, seed, bodytype)
integrator.setBoundary(boxBoundary)
integrator.setPairPotential(potentialPatchyProtein)
# Generate random position and orientation particle list with two particles
seed = int(trajectorynum)
partlist = generateParticleList(initialState,
boxsize,
particleTypes,
unboundMSMlist,
randomSeed=-1)
# Calculates the first passage times for a given bound state. Each trajectory is integrated until
# a bound state is reached. The output in the files is the elapsed time.
bound = True
while (bound):
integrator.integrate(partlist)
boundState = dummyTraj.getState(partlist[0], partlist[1])
if boundState == 0:
bound = False
return initialState, integrator.clock
elif integrator.clock >= 15000.0:
bound = False
return 'failed', integrator.clock
def MSMRDsimulationFPT(initialState, finalState, trajectorynum):
'''
Calculates first passage time of a trajectory with random initial
conditions and final state a bound state
:param trajectorynum: trajectory number (index on parallel computation) on which to calculate the FPT
:param initialState: initial bound state
:param finalState final bound state
:return: initial bound state, final bound state and first passage time
'''
# Define discretization
discretization = msmrd2.discretizations.positionOrientationPartition(radialBounds[1],
numSphericalSectionsPos, numRadialSectionsQuat, numSphericalSectionsQuat)
discretization.setThetasOffset(np.pi/4.0);
# Define boundary
boxBoundary = msmrd2.box(boxsize,boxsize,boxsize,'periodic')
# Define isotropic potential (no patches)
potentialPatchyProtein = patchyProteinMarkovSwitch(sigma, strength, angularStrength,
patchesCoordinates1, patchesCoordinates2)
# Define base seed
seed = int(-1*trajectorynum) # Negative seed, uses random device as seed
# Load rate dicitionary
pickle_in = open(MSMdirectory + "MSM_patchyProtein_t6.00E+06_s25_lagt" + str(lagtime) + ".pickle","rb")
mainMSM = pickle.load(pickle_in)
tmatrix = mainMSM['transition_matrix']
activeSet = mainMSM['active_set']
# Create unbound MSMlist (CTMSMs)
# MSM for particle type0
MSMtype = 0
markovModel0 = ctmsm(MSMtype, -1*seed) # random variable seed
D0list = np.array([1.0])
Drot0list = np.array([1.0])
markovModel0.setD(D0list)
markovModel0.setDrot(Drot0list)
# MSM for particle type1
MSMtype = 1
ratematrix = np.array([[-0.5,0.5],[6.0,-6.0]])
markovModel1 = ctmsm(MSMtype, ratematrix, -2*seed)
D1list = np.array([0.5, 1.0])
Drot1list = np.array([0.5, 1.0])
markovModel1.setD(D1list)
markovModel1.setDrot(Drot1list)
unboundMSMlist = [markovModel0, markovModel1]
# Set coupling MSM for MSM/RD
seed = int(-3*trajectorynum) # Negative seed, uses random device as seed
couplingMSM = msmrdMSM(numBoundStates, maxNumBoundStates, tmatrix, activeSet, realLagtime, seed)
couplingMSM.setDbound(Dbound, DboundRot)
# Define integrator, boundary and discretization
seed = -int(1*trajectorynum) # Negative seed, uses random device as seed
integrator = msmrdPatchyProtein(dt, seed, bodytype, numParticleTypes, radialBounds, unboundMSMlist, couplingMSM)
integrator.setBoundary(boxBoundary)
integrator.setDiscretization(discretization)
integrator.setPairPotential(potentialPatchyProtein)
# Creates random particle list
seed = int(trajectorynum)
partlist = generateParticleList(initialState, boxsize, particleTypes, couplingMSM, seed)
# Calculates the first passage times from initialState to finalState. Each trajectory is integrated until
# a finalState is reached or until it times out. The output in the files is the elapsed time.
searchingEndState = True
while(searchingEndState):
integrator.integrate(partlist)
currentState = partlist[0].boundState
if currentState == finalState:
searchingEndState = False
return initialState, finalState, integrator.clock
elif integrator.clock >= 15000.0:
searchingEndState = False
return 'failed', 'failed', integrator.clock
def MSMRDsimulationFPT(trajectorynum):
'''
Calculates first passage time of a trajectory with random initial
conditions and final state a bound state
:param trajectorynum: trajectory number (index on parallel computation) on which to calculate the FPT
:return: state, first passage time
'''
# Define discretization
discretization = msmrd2.discretizations.positionOrientationPartition(
radialBounds[1], numSphericalSectionsPos, numRadialSectionsQuat,
numSphericalSectionsQuat)
# Define boundary
boxBoundary = msmrd2.box(boxsize, boxsize, boxsize, 'periodic')
# Load rate dicitionary
pickle_in = open(
MSMdirectory + "MSM_patchyDimer_t3.00E+06_s25_lagt" + str(lagtime) +
".pickle", "rb")
mainMSM = pickle.load(pickle_in)
tmatrix = mainMSM['transition_matrix']
activeSet = mainMSM['active_set']
# Set unbound MSM
seed = int(-2 * trajectorynum) # Negative seed, uses random device as seed
unboundMSM = ctmsm(MSMtype, ratematrix, seed)
unboundMSM.setD(Dlist)
unboundMSM.setDrot(Drotlist)
# Set coupling MSM
seed = int(-3 * trajectorynum) # Negative seed, uses random device as seed
couplingMSM = msmrdMSM(numBoundStates, maxNumBoundStates, tmatrix,
activeSet, realLagtime, seed)
couplingMSM.setDbound(Dbound, DboundRot)
# Define integrator, boundary and discretization
seed = -int(1 * trajectorynum) # Negative seed, uses random device as seed
integrator = msmrdIntegrator(dt, seed, bodytype, numParticleTypes,
radialBounds, unboundMSM, couplingMSM)
integrator.setBoundary(boxBoundary)
integrator.setDiscretization(discretization)
# Generate random position and orientation particle list with two particles
seed = int(trajectorynum)
partlist = particleTools.randomParticleMSList(numParticles, boxsize,
minimumUnboundRadius,
partTypes, [unboundMSM],
seed)
# Calculates the first passage times for a given bound state. Each trajectory is integrated until
# a bound state is reached. The output in the files is the elapsed time.
unbound = True
while (unbound):
integrator.integrate(partlist)
currentState = partlist[0].boundState
if currentState in boundStatesA:
unbound = False
return 'A', integrator.clock
elif currentState in boundStatesB:
unbound = False
return 'B', integrator.clock
elif integrator.clock >= 10000.0:
unbound = False
return 'Failed at:', integrator.clock
def MSMRDsimulationFPT(trajectorynum):
'''
Calculates first passage time of a trajectory with random initial
conditions and final state a bound state
:param trajectorynum: trajectory number (index on parallel computation) on which to calculate the FPT
:return: state, first passage time
'''
# Define discretization
discretization = msmrd2.discretizations.positionOrientationPartition(
radialBounds[1], numSphericalSectionsPos, numRadialSectionsQuat,
numSphericalSectionsQuat)
# Define boundary
boxBoundary = msmrd2.box(boxsize, boxsize, boxsize, 'periodic')
# Load rate dicitionary
pickle_in = open(
"../../data/pentamer/MSMs/MSM_dimerForPentamer_t3.00E+06_s25_lagt" +
str(lagtime) + ".pickle", "rb") # Same MSM as trimer
mainMSM = pickle.load(pickle_in)
tmatrix = mainMSM['transition_matrix']
activeSet = mainMSM['active_set']
# Set unbound MSM
seed = int(-2 * trajectorynum) # Negative seed, uses random device as seed
unboundMSM = ctmsm(MSMtype, ratematrix, seed)
unboundMSM.setD(Dlist)
unboundMSM.setDrot(Drotlist)
# Set coupling MSM
seed = int(-3 * trajectorynum) # Negative seed, uses random device as seed
couplingMSM = msmrdMSM(numBoundStates, maxNumBoundStates, tmatrix,
activeSet, realLagtime, seed)
couplingMSM.setDbound(Dbound, DboundRot)
# Define integrator, boundary and discretization
seed = -int(1 * trajectorynum) # Negative seed, uses random device as seed
integrator = msmrdMultiParticleIntegrator(dt, seed, bodytype,
numParticleTypes, radialBounds,
unboundMSM, couplingMSM,
DlistCompound, DrotlistCompound)
integrator.setBoundary(boxBoundary)
integrator.setDiscretization(discretization)
# Generate random position and orientation particle list with two particles
seed = int(trajectorynum)
partlist = particleTools.randomParticleMSList(numParticles, boxsize,
minimumUnboundRadius,
partTypes, [unboundMSM],
seed)
# Calculates the first passage times to a given bound state. Each trajectory is integrated until
# a bound state is reached. The output in the files is the elapsed time.
unbound = True
ii = 0
while (unbound):
ii += 1
integrator.integrate(partlist)
# Check status every 5000 timesteps (adds possible error of up to 5000*dt = 0.5), but
# speeds up simulations
if (ii % 5000 == 0):
ringFormations = integrator.findClosedBindingLoops(partlist)
if (3 in ringFormations):
unbound = False
return 'trimeric-loop', integrator.clock
elif (4 in ringFormations):
unbound = False
return 'tetrameric-loop', integrator.clock
elif (5 in ringFormations):
unbound = False
return "pentameric-loop", integrator.clock
elif integrator.clock >= 400.0:
unbound = False
return 'Failed at:', integrator.clock
