コード例 #1
0
ファイル: metropolis.py プロジェクト: vrgsdaniel/CBio
 def __init__(self,
              pose_init,
              niter,
              ntraj,
              use_criterion,
              annealing=False,
              max_add=25,
              kT0=100):
     self.trajectories = []
     self.final_energies = np.zeros(ntraj)
     self.ntraj = ntraj
     self.niter = niter
     pose = pose_init()
     # movers needed to convert to centroid and full atom
     movers = {
         "pmover": PyMOLMover(),
         "centroid": SwitchResidueTypeSetMover("centroid"),
         "fa_mover": SwitchResidueTypeSetMover("fa_standard")
     }
     # initialise trajectories with clone of initial pose
     for i in range(ntraj):
         tr = Trajectory(i, pose.clone(), movers, niter, use_criterion,
                         annealing, max_add, kT0)
         tr.set_score_fn(tr.centroid_score)
         self.trajectories.append(tr)
コード例 #2
0
def pep_run(decoy_name, n_decoys, pose, sf='docking', pymol_ip_addr=None):
    """
    Tested score function is 'docking' not sure if this is the best. Is there a way to run this in a 
    distributed fashion? Each decoy takes ~3 minutes on my machine.
    """
    if pymol_ip_addr:
        pmm = PyMOLMover(pymol_ip_addr,
                         65000)  #enter the IP that pymol displays on startup
        pmm.keep_history(True)

    # Score function and starting PDB
    sf = create_score_function(sf)  # no idea what this sf is...
    #pose = pose_from_pdb(pdb)

    # Creating FlexPepDock protocol using init options
    fpdock = FlexPepDockingProtocol()

    jd = PyJobDistributor(decoy_name, n_decoys, sf)
    while not jd.job_complete:
        pp = Pose()
        pp.assign(pose)
        fpdock.apply(pp)
        if pymol_ip_addr:
            pmm.apply(pp)
        jd.output_decoy(
            pp)  # this will output a PDB file, which is not really necessary.
コード例 #3
0
##################################################################
################### MUTATE PROTEIN ###############################
##################################################################

# make score function
scorefxn = get_fa_scorefxn()

# mutate protein
print(fa_working.pdb_info().pdb2pose('H', 12))
mutater = pyrosetta.rosetta.protocols.simple_moves.MutateResidue()
mutater.set_target(386)
mutater.set_res_name('PRO')
mutater.apply(fa_working)

# see in PyMOL
pymol = PyMOLMover()
pymol.pymol_name('mutated_superantigen')
pymol.apply(fa_working)

##################################################################
################### RELAX LOCALLY ################################
##################################################################

# relax pose, store lowest energy
# (i.e. import fast relax method from lecture7)
# task factory, what to design, where and how...
# (dock mcm protocol, get interface residues)
# interface energy optimization

from fast_relax_function import *
fast_relax(fa_working, fast_relax_rounds=1)
コード例 #4
0
def pose_scoring(pose, display_residues = []):
    """
    Extracts and displays various score evaluations on the input  <pose>
		and its  <display_residues>  including:
		total score
		score term evaluations
		per-residue score
		radius of gyration (approximate)

    """
    # this object is contained in PyRosetta v2.0 and above
    # create a PyMOLMover for exporting structures directly to PyMOL
    pymover = PyMOLMover()

    # 1. score the pose using the default full-atom (fa) ScoreFunction
    # a ScoreFunction is essentially a list of weights indicating which
    #    ScoreTypes are "on" and how they are scaled when summed together
    # ScoreTypes define what scoring methods are performed on the pose
    # some ScoreTypes are centroid or fullatom specific, others are not
    # there are (at least) 5 ways to obtain the general fullatom ScoreFunction
    # the 1st (a) and 2nd (b) methods are only present since PyRosetta v2.0
    #
    # a. this method returns the hard-coded set of weights for the standard
    #    fullatom ScoreFunction, which is currently called "ref2015"
    fa_scorefxn = get_fa_scorefxn()

    # b. this method returns a ScoreFunction with its weights set based on
    #    files stored in the database/scoring/weights (.wts files)
    full_scorefxn = create_score_function('ref2015')

    # c. this method sets the weights based on 'ref2015.wts' and then
    #    corrects them based on 'docking.wts_patch'
    ws_patch_scorefxn = create_score_function('ref2015', 'docking')  # create_score_function_ws_patch('ref2015', 'docking')

    # d. this method returns a ScoreFunction with its weights set by loading
    #    weights from 'ref2015' followed by an adjustment by setting
    #    weights from 'docking.wts_patch'
    patch_scorefxn = create_score_function('ref2015')
    patch_scorefxn.apply_patch_from_file('docking')

    # e. here an empty ScoreFunction is created and the weights are set manually
    scorefxn = ScoreFunction()
    scorefxn.set_weight(core.scoring.fa_atr, 0.800)    # full-atom attractive score
    scorefxn.set_weight(core.scoring.fa_rep, 0.440)    # full-atom repulsive score
    scorefxn.set_weight(core.scoring.fa_sol, 0.750)    # full-atom solvation score
    scorefxn.set_weight(core.scoring.fa_intra_rep, 0.004)    # f.a. intraresidue rep. score
    scorefxn.set_weight(core.scoring.fa_elec, 0.700)    # full-atom electronic score
    scorefxn.set_weight(core.scoring.pro_close, 1.000)    # proline closure
    scorefxn.set_weight(core.scoring.hbond_sr_bb, 1.170)    # short-range hbonding
    scorefxn.set_weight(core.scoring.hbond_lr_bb, 1.170)    # long-range hbonding
    scorefxn.set_weight(core.scoring.hbond_bb_sc, 1.170)    # backbone-sidechain hbonding
    scorefxn.set_weight(core.scoring.hbond_sc, 1.100)    # sidechain-sidechain hbonding
    scorefxn.set_weight(core.scoring.dslf_fa13, 1.000)    # disulfide full-atom score
    scorefxn.set_weight(core.scoring.rama, 0.200)    # ramachandran score
    scorefxn.set_weight(core.scoring.omega, 0.500)    # omega torsion score
    scorefxn.set_weight(core.scoring.fa_dun, 0.560)    # fullatom Dunbrack rotamer score
    scorefxn.set_weight(core.scoring.p_aa_pp, 0.320)
    scorefxn.set_weight(core.scoring.ref, 1.000)    # reference identity score

    # ScoreFunction a, b, and e above have the same weights and thus return
    #    the same score for an input pose.  Likewise, c and d should return the
    #    same scores.
    # 2. output the ScoreFunction evaluations
    #ws_patch_scorefxn(pose)    # to prevent verbose output on the next line
    print( '='*80 )
    print( 'ScoreFunction a:', fa_scorefxn(pose) )
    print( 'ScoreFunction b:', full_scorefxn(pose) )
    print( 'ScoreFunction c:', ws_patch_scorefxn(pose) )
    print( 'ScoreFunction d:', patch_scorefxn(pose) )
    print( 'ScoreFunction e:', scorefxn(pose) )
    pose_score = scorefxn(pose)

    # 3. obtain the pose Energies object and all the residue total scores
    energies = pose.energies()
    residue_energies = [energies.residue_total_energy(i)
        for i in range(1, pose.total_residue() + 1)]

    # 4. obtain the non-zero weights of the ScoreFunction, active ScoreTypes
    weights = [core.scoring.ScoreType(s)
        for s in range(1, int(core.scoring.end_of_score_type_enumeration) + 1)
        if scorefxn.weights()[core.scoring.ScoreType(s)]]
    # 5. obtain all the pose energies using the weights list
    # Energies.residue_total_energies returns an EMapVector of the unweighted
    #    score values, here they are multiplied by their weights
    #    remember when performing individual investigation, these are the raw
    #    unweighted score!
    residue_weighted_energies_matrix = [
        [energies.residue_total_energies(i)[w] * scorefxn.weights()[w]
        for i in range(1, pose.total_residue() + 1)]
        for w in weights]

    # Unfortunately, hydrogen bonding scores are NOT stored in the structure
    #    returned by Energies.residue_total_energies
    # 6. hydrogen bonding information must be extracted separately
    pose_hbonds = core.scoring.hbonds.HBondSet()
    core.scoring.hbonds.fill_hbond_set( pose , False , pose_hbonds )

    # 7. create a dictionary with the pose residue numbers as keys and the
    #    residue hydrogen bonding information as values
    # hydrogen bonding information is stored as test in the form:
    # (donor residue) (donor atom) => (acceptor residue) (accecptor atom) |score
    hbond_dictionary = {}
    for residue in range(1, pose.total_residue() + 1):
        hbond_text = ''
        for hbond in range(1, pose_hbonds.nhbonds() + 1):
            hbond = pose_hbonds.hbond(hbond)
            acceptor_residue = hbond.acc_res()
            donor_residue = hbond.don_res()
            if residue == acceptor_residue or residue == donor_residue:
                hbond_text += str(donor_residue).ljust(4) + ' ' + \
                    str(pose.residue(donor_residue).atom_name(\
                        hbond.don_hatm() )).strip().ljust(4) + \
                    ' => ' + str(acceptor_residue).ljust(4) + ' ' + \
                    str(pose.residue(acceptor_residue).atom_name(\
                        hbond.acc_atm() )).strip().ljust(4) + \
                    ' |score: ' + str(hbond.energy()) + '\n'
        hbond_dictionary[residue] = hbond_text

    # 8. approximate the radius of gyration
    # there is an rg ScoreType in PyRosetta for performing this computation so
    #    a ScoreFunction can be made as an Rg calculator, likewise you can
    #    bias a structure towards more or less compact structures using this
    # NOTE: this is NOT the true radius of gyration for a protein, it uses
    #    the Residue.nbr_atom coordinates to save time, this nbr_atom is the
    #    Residue atom closest to the Residue's center of geometry
    RadG = ScoreFunction()
    RadG.set_weight(core.scoring.rg , 1)
    pose_radg = RadG(pose)

    # 9. output the pose information
	# the information is not expressed sequentially as it is produced because
	#    several PyRosetta objects and methods output intermediate information
	#    to screen, this would produce and unattractive output
    print( '='*80 )
    print( 'Loaded from' , pose.pdb_info().name() )
    print( pose.total_residue() , 'residues' )
    print( 'Radius of Gyration ~' , pose_radg )
    print( 'Total Rosetta Score:' , pose_score )
    scorefxn.show(pose)
    # this object is contained in PyRosetta v2.0 and above
    pymover.apply(pose)
    pymover.send_energy(pose)

    # 10. output information on the requested residues
    for i in display_residues:
        print( '='*80 )
        print( 'Pose numbered Residue' , i )
        print( 'Total Residue Score:' , residue_energies[i-1] )
        print( 'Score Breakdown:\n' + '-'*45 )
        # loop over the weights, extract the scores from the matrix
        for w in range(len(weights)):
            print( '\t' + core.scoring.name_from_score_type(weights[w]).ljust(20) + ':\t' ,\
                residue_weighted_energies_matrix[w][i-1] )
        print( '-'*45 )
        # print the hydrogen bond information
        print( 'Hydrogen bonds involving Residue ' + str(i) + ':' )
        print( hbond_dictionary[i][:-1] )
    print( '='*80 )
コード例 #5
0
def packer_task(pose, PDB_out=False):
    """
    Demonstrates the syntax necessary for basic usage of the PackerTask object
		performs demonstrative sidechain packing and selected design
		using  <pose>  and writes structures to PDB files if  <PDB_out>
		is True

    """
    # create a copy of the pose
    test_pose = Pose()
    test_pose.assign(pose)

    # this object is contained in PyRosetta v2.0 and above
    pymover = PyMOLMover()

    # create a standard ScoreFunction
    scorefxn = get_fa_scorefxn(
    )  #  create_score_function_ws_patch('standard', 'score12')

    ############
    # PackerTask
    # a PackerTask encodes preferences and options for sidechain packing, an
    #    effective Rosetta methodology for changing sidechain conformations, and
    #    design (mutation)
    # a PackerTask stores information on a per-residue basis
    # each residue may be packed or designed
    # PackerTasks are handled slightly differently in PyRosetta
    ####pose_packer = PackerTask()    # this line will not work properly
    pose_packer = standard_packer_task(test_pose)
    # the pose argument tells the PackerTask how large it should be

    # sidechain packing "optimizes" a pose's sidechain conformations by cycling
    #    through (Dunbrack) rotamers (sets of chi angles) at a specific residue
    #    and selecting the rotamer which achieves the lowest score,
    #    enumerating all possibilities for all sidechains simultaneously is
    #    impractically expensive so the residues to be packed are individually
    #    optimized in a "random" order
    # packing options include:
    #    -"freezing" the residue, preventing it from changing conformation
    #    -including the original sidechain conformation when determining the
    #        lowest scoring conformation
    pose_packer.restrict_to_repacking()  # turns off design
    pose_packer.or_include_current(True)  # considers original conformation
    print(pose_packer)

    # packing and design can be performed by a PackRotamersMover, it requires
    #    a ScoreFunction, for optimizing the sidechains and a PackerTask,
    #    setting the packing and design options
    packmover = protocols.minimization_packing.PackRotamersMover(
        scorefxn, pose_packer)

    scorefxn(pose)  # to prevent verbose output on the next line
    print('\nPre packing score:', scorefxn(test_pose))
    test_pose.pdb_info().name('original')  # for PyMOLMover
    pymover.apply(test_pose)

    packmover.apply(test_pose)
    print('Post packing score:', scorefxn(test_pose))
    test_pose.pdb_info().name('packed')  # for PyMOLMover
    pymover.apply(test_pose)
    if PDB_out:
        test_pose.dump_pdb('packed.pdb')

    # since the PackerTask specifies how the sidechains change, it has been
    #    extended to include sidechain constitutional changes allowing
    #    protein design, this method of design is very similar to sidechain
    #    packing; all rotamers of the possible mutants at a single residue
    #    are considered and the lowest scoring conformation is selected
    # design options include:
    #    -allow all amino acids
    #    -allow all amino acids except cysteine
    #    -allow specific amino acids
    #    -prevent specific amino acids
    #    -allow polar amino acids only
    #    -prevent polar amino acids
    #    -allow only the native amino acid
    # the myriad of packing and design options can be set manually or, more
    #    commonly, using a specific file format known as a resfile
    #    resfile syntax is explained at:
    #    http://www.rosettacommons.org/manuals/archive/rosetta3.1_user_guide/file_resfiles.html
    # manually setting deign options is tedious, the methods below are handy
    #    for creating resfiles
    # mutate the "middle" residues
    center = test_pose.total_residue() // 2
    specific_design = {}
    for i in range(center - 2, center + 3):
        specific_design[i] = 'ALLAA'
    # write a resfile to perform these mutations
    generate_resfile_from_pose(test_pose,
                               'sample_resfile',
                               False,
                               specific=specific_design)

    # setup the design PackerTask, use the generated resfile
    pose_design = standard_packer_task(test_pose)
    rosetta.core.pack.task.parse_resfile(test_pose, pose_design,
                                         'sample_resfile')
    print(pose_design)

    # prepare a new structure
    test_pose.assign(pose)

    # perform design
    designmover = protocols.minimization_packing.PackRotamersMover(
        scorefxn, pose_design)
    print(
        '\nDesign with all proteogenic amino acids at (pose numbered)\
        residues', center - 2, 'to', center + 2)
    print('Pre-design score:', scorefxn(test_pose))
    print( 'Pre-design sequence: ...' + \
        test_pose.sequence()[center - 5:center + 4] + '...' )

    designmover.apply(test_pose)  # perform design
    print('\nPost-design score:', scorefxn(test_pose))
    print( 'Post-design sequence: ...' + \
        test_pose.sequence()[center - 5:center + 4] + '...' )
    test_pose.pdb_info().name('designed')  # for PyMOLMover
    pymover.apply(test_pose)
    if PDB_out:
        test_pose.dump_pdb('designed.pdb')
コード例 #6
0
def movemap(pose, PDB_out=False):
    """
    Demonstrates the syntax necessary for basic usage of the MoveMap object
        performs these changes with a demonstrative backbone minimization
        using  <pose>  and writes structures to PDB files if  <PDB_out>  is True

    """

    #########
    # MoveMap
    # a MoveMap encodes what data is allowed to change in a Pose, referred to as
    #    its degrees of freedom
    # a MoveMap is separate from a Pose and is usually required by a Mover so
    #    that the correct degrees of freedom are manipulated, in this way,
    #    MoveMap and Pose objects often work in parallel
    # several MoveMap's can correspond to the same Pose
    # a MoveMap stores information on a per-residue basis about the
    #    backbone ({phi, psi, omega}) and chi ({chi_i}) torsion angle sets
    #    the MoveMap can only set these sets of torsions to True or False, it
    #    cannot set freedom for the individual angles (such as phi free and psi
    #    fixed)
    # the MoveMap has no upper-limit on its residue information, it defaults to
    #    all residues (up to residue 99999999) backbone and chi False
    # you can view the MoveMap per-residue torsion settings by using the
    #    MoveMap.show( Pose.total_residue() ) method (the input argument is the
    #    highest residue to output, it does not support viewing a range)
    pose_move_map = MoveMap()
    # change all backbone torsion angles
    pose_move_map.set_bb(True)
    # change all chi angle torsion angles (False by default)
    pose_move_map.set_chi(False)
    # change a single backbone torsion angles
    #pose_move_map.set_bb(1, True)    # example syntax
    # change a single residue's chi torsion angles
    #pose_move_map.set_chi(1, True)    # example syntax
    pose_move_map.show(pose.total_residue())

    # perform gradient based minimization on the "median" residues, this
    #    method (MinMover) determines the gradient of an input pose using a
    #    ScoreFunction for evaluation and a MoveMap to define the degrees of
    #    freedom
    # create a standard ScoreFunction
    scorefxn = get_fa_scorefxn(
    )  #  create_score_function_ws_patch('standard', 'score12')
    # redefine the MoveMap to include the median half of the residues
    # turn "off" all backbone torsion angles
    pose_move_map.set_bb(False)  # reset to backbone False
    # turn "on" a range of residue backbone torsion angles
    pose_move_map.set_bb_true_range(int(pose.total_residue() / 4),
                                    int(pose.total_residue() * 3 / 4))
    # create the MinMover
    minmover = protocols.minimization_packing.MinMover()
    minmover.score_function(scorefxn)
    minmover.movemap(pose_move_map)

    # create a copy of the pose
    test_pose = Pose()
    test_pose.assign(pose)
    # apply minimization
    scorefxn(test_pose)  # to prevent verbose output on the next line

    pymover = PyMOLMover()
    #### uncomment the line below and "comment-out" the two lines below to
    ####    export the structures into different PyMOL states of the same object
    #pymover.keep_history = True    # enables viewing across states

    #### comment-out the line below, changing PDBInfo names tells the
    ####    PyMOLMover to produce new objects
    test_pose.pdb_info().name('original')
    pymover.apply(test_pose)
    print('\nPre minimization score:', scorefxn(test_pose))

    minmover.apply(test_pose)
    if PDB_out:
        test_pose.dump_pdb('minimized.pdb')

    print('Post minimization score:', scorefxn(test_pose))
    #### comment-out the line below
    test_pose.pdb_info().name('minimized')
    pymover.apply(test_pose)
コード例 #7
0
###################################################################
## Loop through and store lowest energy docking pose
lowest_energy_pose = Pose()
lowest_energy = float('inf')

for i in range(3):
    # rotate and translate superantigen (8 degrees rot, 3 ang trans)
    pert_mover = rigid_moves.RigidBodyPerturbMover(jump_num, 8, 3)
    pert_mover.apply(fa_working)

    # minimize the energy
    min_mover.apply(fa_working)

    # score pose
    print('working pose energy: ')
    curr_score = scorefxn(fa_working)
    print(curr_score)

    # store values
    if curr_score < lowest_energy:
        lowest_energy = curr_score

###################################################################

# see in PyMOL
pymol = PyMOLMover()
pymol.keep_history(True)
pymol.apply(fa_starting)
pymol.apply(fa_working)
コード例 #8
0
def scanning(pdb_filename,
             partners,
             mutant_aa='A',
             interface_cutoff=8.0,
             output=False,
             trials=1,
             trial_output=''):
    """
    Performs "scanning" at an interface within  <pdb_filename>  between
        <partners>  by mutating relevant residues to  <mutant_aa>  and repacking
        residues within  <pack_radius>  Angstroms, further repacking all
        residues within  <interface_cutoff>  of the interface residue, scoring
        the complex and subtracting the score of a pose with the partners
        separated by 500 Angstroms.
        <trials>  scans are performed (to average results) with summaries written
        to  <trial_output>_(trial#).txt.
        Structures are exported to a PyMOL instance.

    """
    # 1. create a pose from the desired PDB file
    pose = Pose()
    pose_from_file(pose, pdb_filename)

    # 2. setup the docking FoldTree and other related parameters
    dock_jump = 1
    movable_jumps = Vector1([dock_jump])
    protocols.docking.setup_foldtree(pose, partners, movable_jumps)

    # 3. create ScoreFuncions for the Interface and "ddG" calculations
    # the pose's Energies objects MUST be updated for the Interface object to
    #    work normally
    scorefxn = get_fa_scorefxn()  #  create_score_function('standard')
    scorefxn(pose)  # needed for proper Interface calculation

    # setup a "ddG" ScoreFunction, custom weights
    ddG_scorefxn = ScoreFunction()
    ddG_scorefxn.set_weight(core.scoring.fa_atr, 0.44)
    ddG_scorefxn.set_weight(core.scoring.fa_rep, 0.07)
    ddG_scorefxn.set_weight(core.scoring.fa_sol, 1.0)
    ddG_scorefxn.set_weight(core.scoring.hbond_bb_sc, 0.5)
    ddG_scorefxn.set_weight(core.scoring.hbond_sc, 1.0)

    # 4. create an Interface object for the pose
    interface = Interface(dock_jump)
    interface.distance(interface_cutoff)
    interface.calculate(pose)

    # 5. create a PyMOLMover for sending output to PyMOL (optional)
    pymover = PyMOLMover()
    pymover.keep_history(True)  # for multiple trajectories
    pymover.apply(pose)
    pymover.send_energy(pose)

    # 6. perform scanning trials
    # the large number of packing operations introduces a lot of variability,
    #    for best results, perform several trials and average the results,
    #    these score changes are useful to QUALITATIVELY defining "hotspot"
    #    residues
    # this script does not use a PyJobDistributor since no PDB files are output
    for trial in range(trials):
        # store the ddG values in a dictionary
        ddG_mutants = {}
        for i in range(1, pose.total_residue() + 1):
            # for residues at the interface
            if interface.is_interface(i) == True:
                # this way you can TURN OFF output by providing False arguments
                #    (such as '', the default)
                filename = ''
                if output:
                    filename = pose.pdb_info().name()[:-4] + '_' +\
                        pose.sequence()[i-1] +\
                        str(pose.pdb_info().number(i)) + '->' + mutant_aa
                # determine the interace score change upon mutation
                ddG_mutants[i] = interface_ddG(pose, i, mutant_aa,
                                               movable_jumps, ddG_scorefxn,
                                               interface_cutoff, filename)

        # output results
        print('=' * 80)
        print('Trial', str(trial + 1))
        print(
            'Mutants (PDB numbered)\t\"ddG\" (interaction dependent score change)'
        )
        residues = list(ddG_mutants.keys()
                        )  # list(...) conversion is for python3 compatbility
        residues.sort()  # easier to read
        display = [
            pose.sequence()[i - 1] + str(pose.pdb_info().number(i)) +
            mutant_aa + '\t' + str(ddG_mutants[i]) + '\n' for i in residues
        ]
        print(''.join(display)[:-1])
        print('=' * 80)

        # write to file
        f = open(trial_output + '_' + str(trial + 1) + '.txt', 'w')
        f.writelines(display)
        f.close()

    #### alternate output using scanning_analysis (see below), only display
    ####    mutations with "deviant" score changes
    print('Likely Hotspot Residues')
    for hotspot in scanning_analysis(trial_output):
        print(hotspot)
    print('=' * 80)
コード例 #9
0
def interface_ddG(pose,
                  mutant_position,
                  mutant_aa,
                  movable_jumps,
                  scorefxn='',
                  cutoff=8.0,
                  out_filename=''):
    # 1. create a reference copy of the pose
    wt = Pose()  # the "wild-type"
    wt.assign(pose)

    # 2. setup a specific default ScoreFunction
    if not scorefxn:
        # this is a modified version of the scoring function discussed in
        #    PNAS 2002 (22)14116-21, without environment dependent hbonding
        scorefxn = ScoreFunction()
        scorefxn.set_weight(fa_atr, 0.44)
        scorefxn.set_weight(fa_rep, 0.07)
        scorefxn.set_weight(fa_sol, 1.0)
        scorefxn.set_weight(hbond_bb_sc, 0.5)
        scorefxn.set_weight(hbond_sc, 1.0)

    # 3. create a copy of the pose for mutation
    mutant = Pose()
    mutant.assign(pose)

    # 4. mutate the desired residue
    # the pack_radius argument of mutate_residue (see below) is redundant
    #    for this application since the area around the mutation is already
    #    repacked
    mutant = mutate_residue(mutant, mutant_position, mutant_aa, 0.0, scorefxn)

    # 5. calculate the "interaction energy"
    # the method calc_interaction_energy is exposed in PyRosetta however it
    #    does not alter the protein conformation after translation and may miss
    #    significant interactions
    # an alternate method for manually separating and scoring is provided called
    #    calc_binding_energy (see Interaction Energy vs. Binding Energy below)
    wt_score = calc_binding_energy(wt, scorefxn, mutant_position, cutoff)
    mut_score = calc_binding_energy(mutant, scorefxn, mutant_position, cutoff)
    #### the method calc_interaction_energy separates an input pose by
    ####    500 Angstroms along the jump defined in a Vector1 of jump numbers
    ####    for movable jumps, a ScoreFunction must also be provided
    #### if setup_foldtree has not been applied, calc_interaction_energy may be
    ####    wrong (since the jumps may be wrong)
    #wt_score = calc_interaction_energy(wt, scorefxn, movable_jumps)
    #mut_score = calc_interaction_energy(mutant, scorefxn, movable_jumps)
    ddg = mut_score - wt_score

    # 6. output data (optional)
    # -export the mutant structure to PyMOL (optional)
    mutant.pdb_info().name(pose.sequence()[mutant_position - 1] +
                           str(pose.pdb_info().number(mutant_position)) +
                           mutant.sequence()[mutant_position - 1])
    pymover = PyMOLMover()
    scorefxn(mutant)
    pymover.apply(mutant)
    pymover.send_energy(mutant)

    # -write the mutant structure to a PDB file
    if out_filename:
        mutant.dump_pdb(out_filename)

    return ddg
コード例 #10
0
#! /usr/bin/python
# This file simply contains a list of commands copied from a carbohydrates
# tutorial/demo that I am writing.  ~Labonte

from __future__ import print_function

import pyrosetta
import pyrosetta.rosetta as rosetta

from pyrosetta import init, PyMOLMover, pose_from_file, pose_from_sequence
from pyrosetta.rosetta import core, protocols

init('-constant_seed -include_sugars')
import os; os.chdir('.test.output')

pm = PyMOLMover()


# Linear Oligosaccharides & IUPAC Sequences

from rosetta.core.pose import pose_from_saccharide_sequence

glucose = pose_from_saccharide_sequence('alpha-D-Glcp')
galactose = pose_from_saccharide_sequence('Galp')
mannose = pose_from_saccharide_sequence('->3)-a-D-Manp')
maltotriose = pose_from_saccharide_sequence('a-D-Glcp-' * 3)
isomaltose = pose_from_saccharide_sequence('->6)-Glcp-' * 2)
lactose = pose_from_saccharide_sequence('b-D-Galp-(1->4)-a-D-Glcp')

pm.apply(isomaltose)
pm.apply(glucose)
コード例 #11
0
##################################################################
################### IMPORT MODULES ###############################
##################################################################

# import pyrosetta
from pyrosetta import *

init(
    "-mh:path:scores_BB_BB motif_dock/xh_16_ -mh:score:use_ss1 false -mh:score:use_ss2 false -mh:score:use_aa1 true -mh:score:use_aa2 true"
)  # for docking

# setup pymol
from pyrosetta import PyMOLMover

pymol = PyMOLMover()

# import additional modules
from pyrosetta.teaching import *
import rosetta.protocols.rigid as rigid_moves
from rosetta.protocols.minimization_packing import *
from pyrosetta import PyMOLMover
import numpy as np
from rosetta.protocols import minimization_packing as pack_min
from rosetta.protocols.relax import FastRelax
import matplotlib.pyplot as plt

# import and clean pdb (superantigen + TCR + MHC)
from pyrosetta.toolbox import cleanATOM

cleanATOM("2ICW_MHC.pdb")
コード例 #12
0
def fold_tree(PDB_out=False):
    """
    Demonstrates the syntax necessary for basic usage of the FoldTree object
        performs these changes with a demonstrative pose example and writes
        structures to PDB files if  <PDB_out>  is True

    """

    ##########
    # FoldTree
    # a FoldTree encodes the internal coordinate dependencies of a Pose
    # a Pose object MUST have a FoldTree
    # the FoldTree allows regions of a pose to become independent,
    #    it is used in many important applications, particularly:
    #    loop modeling: where changes to the conformation of a loop region
    #    should NOT alter the conformation of the entire protein
    #    rigid-body docking: where changes in the position of one docking
    #    partner should not alter the position of the other docking partner
    # a FoldTree is effectively a list of Edge objects, you can view the Edges
    #    by printing the FoldTree ("print FoldTree")
    # the length of a FoldTree (FoldTree.size) MUST match the length of its
    #    corresponding Pose (Pose.total_residue)
    # it is possible to create an improper FoldTree, the method
    #    FoldTree.check_fold_tree returns True if the FoldTree is complete and
    #    usable and False otherwise
    # some Edge objects are Jumps, indicating a "jump" in the internal
    #    coordinate dependency
    # when a FoldTree is created, it can accept an optional integer argument
    #    setting the FoldTree to contain a single Edge with a length equal to
    #    the input integer value, the same result is attained by creating an
    #    empty FoldTree (no input arguments) and using the method
    #    FoldTree.simple_tree with an input integer equal to the size of the
    #    FoldTree

    # 1. create the example pose
    test_pose = pose_from_sequence('ACDEFGHIKLMNPQRSTVWY' * 3)

    # 2. setup the jump points, where a jump is anchored, and the cutpoint
    cutpoint = int(test_pose.total_residue() /
                   2)  # integer division, no decimal
    low_jump_point = cutpoint - 10
    high_jump_point = cutpoint + 10

    # the easiest way to create a new complete FoldTree is to use the method
    #    FoldTree.simple_tree to create and empty FoldTree and assign jumps to
    #    it using the method FoldTree.new_jump
    # the FoldTree constructor is overloaded to accept an input integer
    #    indicating how large to make the FoldTree

    # 3. create a simple, one jump FoldTree for the pose
    # a. using FoldTree.new_jump
    #pose_fold_tree = FoldTree(test_pose.total_residue())
    #### these two lines produce the same FoldTree as the one above
    pose_fold_tree = FoldTree()
    pose_fold_tree.simple_tree(test_pose.total_residue())

    pose_fold_tree.new_jump(low_jump_point, high_jump_point, cutpoint)
    print('\nThe first FoldTree is proper:', pose_fold_tree.check_fold_tree())

    # b. using FoldTree.add_edge
    # a more difficult method for creating a FoldTree is simply to create it
    #    empty and use the method FoldTree.add_edge to fill the FoldTree with
    #    new Edge data
    pose_fold_tree = FoldTree()
    pose_fold_tree.add_edge(1, low_jump_point, -1)
    pose_fold_tree.add_edge(low_jump_point, cutpoint, -1)
    pose_fold_tree.add_edge(low_jump_point, high_jump_point, 1)
    pose_fold_tree.add_edge(high_jump_point, test_pose.total_residue(), -1)
    pose_fold_tree.add_edge(high_jump_point, cutpoint + 1, -1)
    print('The second FoldTree is proper:', pose_fold_tree.check_fold_tree())

    # demonstrate FoldTree's effect on structure
    # 4. linearize it
    for i in range(1, test_pose.total_residue() + 1):
        test_pose.set_phi(i, -180)
        test_pose.set_psi(i, 180)
        test_pose.set_omega(i, 180)

    # the Pose.fold_tree method is an overloaded getter/setter,
    #    providing it with no input returns the Pose's FoldTree object
    #    providing a FoldTree object as input overwrites the Pose's current
    #    FoldTree with the new one
    # the FoldTree is set here to prevent problems when "linearizing"
    test_pose.fold_tree(pose_fold_tree)

    # this object is contained in PyRosetta v2.0 and above (optional)
    pymover = PyMOLMover()

    # 5. change and display the new structures
    # a. export "linearized" structure
    test_pose.pdb_info().name('linearized')  # for PyMOLMover
    pymover.apply(test_pose)
    if PDB_out:
        test_pose.dump_pdb('linearized.pdb')
    print('\nlinearized structure output')

    # b. make an early change
    test_pose.set_phi(low_jump_point - 10, 50)
    test_pose.pdb_info().name('pre_jump')  # for PyMOLMover
    pymover.apply(test_pose)  # all downstream residues move
    if PDB_out:
        test_pose.dump_pdb('pre_jump.pdb')
    print('pre jump perturbed structure output')

    # c. make a change in the first edge created by the jump
    test_pose.set_phi(low_jump_point + 5, 50)
    test_pose.pdb_info().name('early_in_jump')  # for PyMOLMover
    pymover.apply(test_pose)  # residues up to the cutpoint change
    if PDB_out:
        test_pose.dump_pdb('early_in_jump.pdb')
    print('first internal jump edge perturbed structure output')

    # d. make a change in the second edge created by the jump
    test_pose.set_phi(high_jump_point - 5, 50)
    test_pose.pdb_info().name('late_in_jump')  # for PyMOLMover
    pymover.apply(test_pose)  # residues down to the cutpoint change
    if PDB_out:
        test_pose.dump_pdb('late_in_jump.pdb')
    print('second internal jump edge perturbed structure output')

    # e. make a late change
    test_pose.set_phi(high_jump_point + 10, 50)
    test_pose.pdb_info().name('post_jump')  # for PyMOLMover
    pymover.apply(test_pose)  # all residues downstream move
    if PDB_out:
        test_pose.dump_pdb('post_jump.pdb')
    print('post jump perturbed structure output')
print(pose)
print(pose.sequence())
print("Protein has", pose.total_residue(), "residues.")
print(pose.residue(500).name())
print(pose.pdb_info().chain(500))
print(pose.pdb_info().number(500))
print(pose.phi(5))
print(pose.psi(5))
print(pose.chi(1, 5))
R5N = AtomID(1, 5)
R5CA = AtomID(2, 5)
R5C = AtomID(3, 5)
print(pose.conformation().bond_length(R5N, R5CA))
print(pose.conformation().bond_length(R5CA, R5C))
from pyrosetta import PyMOLMover
pymol = PyMOLMover()
pymol.apply(pose)
# Calculating energy score
print("Calculating energy score of 6Q21 protein")
ras = pose_from_pdb("6q21.pdb")
print(ras)
print(ras.sequence())
from pyrosetta.teaching import *
scorefxn = get_fa_scorefxn()
print("Score function of 6Q21 protein is :")
print(scorefxn)
scorefxn2 = ScoreFunction()
scorefxn2.set_weight(fa_atr, 1.0)
scorefxn2.set_weight(fa_rep, 1.0)
print(scorefxn(ras))
scorefxn.show(ras)
コード例 #14
0
from pyrosetta import init, pose_from_file, create_score_function, Pose, MoveMap, PyMOLMover
from pyrosetta.rosetta import core, protocols
from pyrosetta.teaching import MinMover, SmallMover, ShearMover, TrialMover, MonteCarlo, RepeatMover

init(extra_options = "-constant_seed")  # WARNING: option '-constant_seed' is for testing only! MAKE SURE TO REMOVE IT IN PRODUCTION RUNS!!!!!
import os; os.chdir('.test.output')

start = pose_from_file("../test/data/workshops/1YY8.clean.pdb")
test = Pose()
test.assign(start)

start.pdb_info().name("start")
test.pdb_info().name("test")

pmm = PyMOLMover()
pmm.apply(start)
pmm.apply(test)
pmm.keep_history(True)
print( pmm )

# Small and Shear Moves
kT = 1.0
n_moves = 1
movemap = MoveMap()
movemap.set_bb(True)
small_mover = SmallMover(movemap, kT, n_moves)
shear_mover = ShearMover(movemap, kT, n_moves)

small_mover.angle_max("H", 5)
small_mover.angle_max("E", 5)
コード例 #15
0
res_path = sys.argv[2]
OUT = sys.argv[3]
weight_file = sys.argv[4]

from pyrosetta import *
from rosetta import *
from rosetta.protocols.rigid import *
from rosetta.core.scoring import *
from pyrosetta import PyMOLMover
from rosetta.protocols.rigid import *
import pyrosetta.rosetta.protocols.rigid as rigid_moves
from pyrosetta.rosetta.protocols.minimization_packing import MinMover

init()

pmm = PyMOLMover()
pmm.keep_history(True)

#os.system('mkdir working_dir')
working_dir = os.getcwd()
#os.system('cd working_dir')


def add_cst(pose, resi, resj, lb, up):
    res_i = pose.pdb_info().pdb2pose('A', res=resi)

    res_j = pose.pdb_info().pdb2pose('B', res=resj)

    if res_i != 0 and res_j != 0:

        atm_i = 'CA' if pose.residue(res_i).name()[0:3] == 'GLY' else 'CB'
コード例 #16
0
ft.add_edge(1, 13, -1)
ft.add_edge(13, 19, -1)
ft.add_edge(13, 26, 1)
ft.add_edge(26, 20, -1)
ft.add_edge(26, 116, -1)

print(ft)
ft.check_fold_tree()

pose.fold_tree(ft)

for res in (10, 13, 16, 23, 26, 30):
    pose.set_phi(res, 180)
    pose.dump_pdb("loop" + str(res) + ".pdb")

pmm = PyMOLMover()
pmm.apply(pose)
# no longer supported: pmm.send_foldtree(pose)
# no longer supported: pmm.view_foldtree_diagram(pose, ft)

ft.clear()
ft.simple_tree(116)
ft.new_jump(76, 85, 80)

# Cyclic Coordination Descent (CCD) Loop Closure
movemap = MoveMap()
movemap.set_bb(True)
movemap.set_chi(True)

loop1 = protocols.loops.Loop(15, 24, 19)
add_single_cutpoint_variant(pose, loop1)
コード例 #17
0
def pose_structure(pose, display_residues=[]):
    """
    Extracts and displays various structural properties of the input  <pose>
        and its  <display_residues>  including:
            -PDB numbering
            -chain identification
            -sequence
            -secondary structure

    """
    # store the pose's number of residues, example Python syntax
    nres = pose.total_residue()

    # 1. obtain the pose's sequence
    sequence = pose.sequence()

    # 2. obtain a list of PDB numbering and icode as a single string
    pdb_info = pose.pdb_info()
    PDB_nums = [(str(pdb_info.number(i)) + pdb_info.icode(i)).strip()
                for i in range(1, nres + 1)]
    # 3. obtains a list of the chains organized by residue
    chains = [pdb_info.chain(i) for i in range(1, nres + 1)]
    # 4. extracts a list of the unique chain IDs
    unique_chains = []
    for c in chains:
        if c not in unique_chains:
            unique_chains.append(c)

    # start outputting information to screen
    print('\n' + '=' * 80)
    print('Loaded from', pdb_info.name())
    print(nres, 'residues')
    print(len(unique_chains), 'chain(s) (' + str(unique_chains)[1:-1] + ')')
    print('Sequence:\n' + sequence)

    # this object is contained in PyRosetta v2.0 and above
    # 5. obtain the pose's secondary structure as predicted by PyRosetta's
    #    built-in DSSP algorithm
    DSSP = protocols.moves.DsspMover()
    DSSP.apply(pose)  # populates the pose's Pose.secstruct
    ss = pose.secstruct()
    print('Secondary Structure:\n' + ss)
    print('\t' + str(100. * ss.count('H') / len(ss))[:4] + '% Helical')
    print('\t' + str(100. * ss.count('E') / len(ss))[:4] + '% Sheet')
    print('\t' + str(100. * ss.count('L') / len(ss))[:4] + '% Loop')

    # 6. obtain the phi, psi, and omega torsion angles
    phis = [pose.phi(i) for i in range(1, nres + 1)]
    psis = [pose.psi(i) for i in range(1, nres + 1)]
    omegas = [pose.omega(i) for i in range(1, nres + 1)]

    # this object is contained in PyRosetta v2.0 and above
    # create a PyMOLMover for exporting structures directly to PyMOL
    pymover = PyMOLMover()
    pymover.apply(pose)  # export the structure to PyMOL (optional)

    # 7. output information on the requested residues
    # use a simple dictionary to make output nicer
    ss_dict = {'L': 'Loop', 'H': 'Helix', 'E': 'Strand'}
    for i in display_residues:
        print('=' * 80)
        print('Pose numbered Residue', i)
        print('PDB numbered Residue', PDB_nums[i - 1])
        print('Single Letter:', sequence[i - 1])
        print('Chain:', chains[i - 1])
        print('Secondary Structure:', ss_dict[ss[i - 1]])
        print('Phi:', phis[i - 1])
        print('Psi:', psis[i - 1])
        print('Omega:', omegas[i - 1])
        # extract the chis
        chis = [pose.chi(j + 1, i) for j in range(pose.residue(i).nchi())]
        for chi_no in range(len(chis)):
            print('Chi ' + str(chi_no + 1) + ':', chis[chi_no])
    print('=' * 80)
コード例 #18
0
def sample_single_loop_modeling(pdb_filename,
                                loop_begin,
                                loop_end,
                                loop_cutpoint,
                                frag_filename,
                                frag_length,
                                outer_cycles_low=2,
                                inner_cycles_low=5,
                                init_temp_low=2.0,
                                final_temp_low=0.8,
                                outer_cycles_high=5,
                                inner_cycles_high=10,
                                init_temp_high=2.2,
                                final_temp_high=0.6,
                                jobs=1,
                                job_output='loop_output'):
    """
    Performs simple single loop construction on the input  <pdb_filename>
        with loop from  <loop_begin>  to  <loop_end>  with a
        cutpoint at  <loop_cutpoint>  using fragments of length  <frag_length>
        in the file  <frag_filename>.  <jobs>  trajectories are performed,
        each using a low resolution (centroid) simulated annealing with
        <outer_cycles>  rounds and  <inner_cycles>  steps per round decrementing
        "temperature" from  <init_temp>  to  <final_temp>  geometrically.
        Output structures are named  <job_output>_(job#).pdb.

    """
    # 1. create a pose from the desired PDB file
    p = Pose()
    pose_from_file(p, pdb_filename)

    # 2. create a reference copy of the pose in fullatom
    starting_p = Pose()
    starting_p.assign(p)

    #### if you are constructing multiple loops simultaneously, changes will
    ####    occur in most of the steps below

    # 3. create the Loop object
    #    (note: Loop objects merely specify residues, they contain no
    #         conformation data)
    my_loop = protocols.loops.Loop(loop_begin, loop_end, loop_cutpoint)
    #### if using multiple loops, add additional Loop objects
    # 4. use the Loop to set the pose FoldTree
    protocols.loops.set_single_loop_fold_tree(p, my_loop)
    #### alternate FoldTree setup, if you uncomment the lines below,
    ####    comment-out the set_single_loop_foldtree line above (line 189)
    #### -create an empty FoldTree
    #ft = FoldTree()
    #### -make it a single edge the length of pose
    #ft.simple_tree(p.total_residue())
    #### -insert a jump corresponding to the single loop region
    #ft.add_jump(loop_begin - 2, loop_end + 2, loop_cutpoint)
    #### -give the pose this FoldTree (set it to this object), this will
    ####     erase any previous FoldTree held by the pose
    #p.fold_tree(ft)
    #### there is also a fold_tree_from_loops method in exposed which sets up
    ####    a FoldTree but it is different from set_single_loop_foldtree in
    ####    that is creates jumps +/- 1 residue from their corresponding loop
    ####    endpoints and requires a third argument, the FoldTree to setup

    # 5. sets the cut-point residues as cut-point variants
    protocols.loops.add_single_cutpoint_variant(p, my_loop)

    # 6. create the MoveMap, allow the loop region backbone and
    #    all chi torsions to be free
    movemap = MoveMap()
    movemap.set_bb_true_range(loop_begin, loop_end)
    movemap.set_chi(True)  # sets all chi torsions free

    # 7. setup the fragment Mover
    # this "try--except" is used to catch improper fragment files
    try:
        fragset = core.fragment.ConstantLengthFragSet(frag_length,
                                                      frag_filename)
        #### the ConstantLengthFragSet is overloaded, this same
        ####    ConstantLengthFragSet can be obtained with different syntax
        # to obtain custom fragments, see Generating Fragment Files below
    except:
        raise IOError('Make sure frag_length matches the fragments in\n\
            frag_file and that frag_file is valid')
    fragment_mover = protocols.simple_moves.ClassicFragmentMover(
        fragset, movemap)

    # 8. create a Mover for loop modeling using CCD (low resolution)
    ccd_closure = protocols.loops.loop_closure.ccd.CCDLoopClosureMover(
        my_loop, movemap)

    # 9. create ScoreFunctions
    # for centroid, use the default centroid ScoreFunction with chainbreak on
    scorefxn_low = create_score_function('cen_std')
    # the chainbreak ScoreType exists to penalize broken bonds
    # try creating a broken pose in the interpreter and use a ScoreFunction
    #    with a chainbreak score to investigate its impact, the score is 0.0
    #    except when a bond is broken
    # this penalizes failures caused by CCD failing to close the loop
    scorefxn_low.set_weight(core.scoring.chainbreak, 1)
    # for fullatom, used for packing and scoring final output
    scorefxn_high = get_fa_scorefxn(
    )  #  create_score_function_ws_patch('standard', 'score12')

    # 10. setup sidechain packing Mover
    task_pack = core.pack.task.TaskFactory.create_packer_task(starting_p)
    task_pack.restrict_to_repacking()  # prevents design, packing only
    task_pack.or_include_current(True)  # considers original sidechains
    pack = protocols.minimization_packing.PackRotamersMover(
        scorefxn_high, task_pack)

    # 11. setup the high resolution refinement
    # by creating a Loops object,
    #    (note: Loops is basically a list of Loop objects),
    sample_loops = protocols.loops.Loops()
    # giving it the loop to remodel,
    sample_loops.add_loop(my_loop)
    # and creating a fullatom CCD Mover (high resolution)
    # this Mover is somewhat abnormal since it handles everything itself, it:
    #    -creates its own MoveMap for the loop regions
    #    -creates its own ScoreFunction (default to get_fa_scorefxn())
    #    -creates its own FoldTree for the pose based on the loops
    #    -creates its own MonteCarlo object for monitoring the pose
    #    -performs "simulated annealing" with 3 outer cycles and 90 inner
    #        cycles, very similar to the protocol outlined ere
    #    -creates its own backbone Movers (SmallMover, ShearMover)
    #    -creates its own PackRotamersMover, it does NOT restrict repacking
    #        to the loop regions and can alter all sidechain conformations
    loop_refine = LoopMover_Refine_CCD(sample_loops)
    # some of these parameters or objects can be set but the protocol
    #    executed by this Mover is effectively untouchable
    #loop_refine.set_score_function(scorefxn_high)    # in beta v2 and above
    loop_refine.temp_initial(init_temp_high)
    loop_refine.temp_final(init_temp_high)
    loop_refine.outer_cycles(outer_cycles_high)
    loop_refine.max_inner_cycles(inner_cycles_high)

    # 12. create centroid <--> fullatom conversion Movers
    to_centroid = SwitchResidueTypeSetMover('centroid')
    to_fullatom = SwitchResidueTypeSetMover('fa_standard')
    # and a Mover to recover sidechain conformations
    #    when a protocol samples backbone torsion space in centroid,
    #    the sidechain conformations are neglected, when it is transferred
    #    to fullatom, we typically set the sidechain conformations to their
    #    "original" values and perform sidechain packing,
    #    a ReturnSidechainMover saves a pose's sidechains (in this case
    #    staring_pose) and when applied, inserts these conformations
    #    into the input pose
    recover_sidechains = protocols.simple_moves.ReturnSidechainMover(
        starting_p)

    # 13. create a reference copy of the pose in centroid
    # the first stage of each trajectory is in centroid
    #    so a centroid reference is needed and the pose must start in centroid
    to_centroid.apply(p)
    starting_p_centroid = Pose()
    starting_p_centroid.assign(p)

    # 14. create the geometric "temperature" increment for simulated annealing
    gamma = pow((final_temp_low / init_temp_low),
                (1.0 / (outer_cycles_low * inner_cycles_low)))

    # 15. create a PyMOLMover for exporting structures to PyMOL
    pymov = PyMOLMover()
    # uncomment the line below to load structures into successive states
    #pymov.keep_history(True)
    scorefxn_high(starting_p)  # for exporting the scores
    pymov.apply(starting_p)
    pymov.send_energy(starting_p)

    # 16. create a (Py)JobDistributor
    # a PyJobDistributor uses the job_output argument to name all output files
    #    and performs the specified number (int) of jobs
    # a ScoreFunction is required since the PyJobDistributor output .fasc file
    #    contains scoring information about each output PDB
    jd = PyJobDistributor(job_output, jobs, scorefxn_high)
    jd.native_pose = starting_p

    # 17. perform the loop modeling protocol
    counter = 0  # for exporting to PyMOL
    while not jd.job_complete:
        # a. set necessary variables for the new trajectory
        # -reload the starting pose (centroid)
        p.assign(starting_p_centroid)
        # -change the pose's PDBInfo.name, for exporting to PyMOL
        counter += 1
        p.pdb_info().name(job_output + '_' + str(counter) + '_cen')
        # -reset the starting "temperature" (to init_temp)
        kT = init_temp_low
        # -create a MonteCarlo object for this trajectory
        #    a MonteCarlo object assesses pass/fail by the Metropolis Criteria
        #    and also records information on the lowest scoring pose
        mc = MonteCarlo(p, scorefxn_low, kT)

        # b. "randomize" the loop
        #### this section may change if you intend to use multiple loops or
        ####    alter the sampling method to "randomize" the loop
        # -by breaking it open,
        for i in range(loop_begin, loop_end + 1):
            p.set_phi(i, -180)
            p.set_psi(i, 180)
        pymov.apply(p)
        # -and then inserting fragments
        #    the number of insertions performed is somewhat arbitrary
        for i in range(loop_begin, loop_end + 1):
            fragment_mover.apply(p)
        pymov.apply(p)
        ####

        # low resolution loop modeling:
        # c. simulated annealing incrementing kT geometrically
        #    from init_temp to final_temp
        #### this section may change if you intend to use multiple loops or
        ####    alter the sampling method for low resolution modeling
        for i in range(1, outer_cycles_low + 1):
            # -start with the lowest scoring pose
            mc.recover_low(p)  # loads mc's lowest scoring pose into p
            # -take several steps of in the simulated annealing by
            for j in range(1, inner_cycles_low + 1):
                # >increasing the "temperature"
                kT = kT * gamma
                mc.set_temperature(kT)
                # >inserting a fragment,
                fragment_mover.apply(p)
                pymov.apply(p)
                # >performing CCD,
                ccd_closure.apply(p)
                pymov.apply(p)
                # >and assessing the Metropolis Criteria
                mc.boltzmann(p)
        ####

        # the LoopMover_Refine_CCD makes A LOT of moves, DO NOT expect to
        #    see useful results if you use the PyMOLMover keep_history option, the large
        #    number of intermediates will slow processing to a halt

        # d. convert the best structure (lowest scoring) into fullatom by:
        # -recovering the best (centroid) structure (lowest scoring),
        mc.recover_low(p)  # loads mc's lowest scoring pose into p
        # -switching the ResidueTypeSet to fullatom (from centroid),
        to_fullatom.apply(p)
        # -recovering the original sidechain conformations,
        recover_sidechains.apply(p)
        # -and packing the result (since the backbone conformation has changed)
        pack.apply(p)
        pymov.apply(p)
        p.pdb_info().name(job_output + '_' + str(counter) + '_fa')

        # high-resolution refinement:
        #### this section may change if you intend to use multiple loops or
        ####    alter the sampling method for high resolution refinement
        # e. apply the LoopMover_Refine_CCD
        loop_refine.apply(p)

        # f. output the decoy (pose result from this trajectory)
        #    include the loop RMSD (Lrsmd)
        # -output a PDB file using the PyJobDistributor
        lrms = protocols.loops.loop_rmsd(p, starting_p, sample_loops, True)
        jd.additional_decoy_info = ' Lrmsd: ' + str(lrms)
        jd.output_decoy(p)
        # -export the structure to PyMOL
        pymov.apply(p)
        pymov.send_energy(p)
コード例 #19
0
def sample_refinement(pdb_filename,
                      kT=1.0,
                      smallmoves=3,
                      shearmoves=5,
                      backbone_angle_max=7,
                      cycles=9,
                      jobs=1,
                      job_output='refine_output'):
    """
    Performs fullatom structural refinement on the input  <pdb_filename>  by
        perturbing backbone torsion angles with a maximum perturbation of
        <backbone_angle_max>  for  <cycles>  trials of
        <smallmoves>  perturbations of a random residue's phi or psi and
        <shearmoves>  perturbations of a random residue's phi and the preceding
        residue's psi followed by gradient based backbone torsion angle
        minimization and sidechain packing with an acceptance criteria scaled
        by  <kT>.  <jobs>  trajectories are performed, continually exporting
        structures to a PyMOL instance.
        Output structures are named  <job_output>_(job#).pdb.
    """
    # 1. create a pose from the desired PDB file
    pose = Pose()
    pose_from_file(pose, pdb_filename)

    # 2. create a reference copy of the pose in fullatom
    starting_pose = Pose()
    starting_pose.assign(pose)

    # 3. create a standard ScoreFunction
    #### implement the desired ScoreFunction here
    scorefxn = get_fa_scorefxn()  #  create_score_function('standard')

    #### If you wish to use the ClassRelax protocol, uncomment the following
    ####    line and comment-out the protocol setup below
    #refinement = protocols.relax.ClassicRelax( scorefxn )

    #### Setup custom high-resolution refinement protocol
    #### backbone refinement protocol

    # 4. create a MoveMap, all backbone torsions free
    movemap = MoveMap()
    movemap.set_bb(True)

    # 5. create a SmallMover
    # a SmallMover perturbs a random (free in the MoveMap) residue's phi or psi
    #    torsion angle for an input number of times and accepts of rejects this
    #    change based on the Metropolis Criteria using the "rama" ScoreType and
    #    the parameter kT
    # set the maximum angle to backbone_angle_max, apply it smallmoves times
    smallmover = protocols.simple_moves.SmallMover(movemap, kT, smallmoves)
    # angle_max is secondary structure dependent, however secondary structure
    #    has not been evaulated in this protocol, thus they are all set
    #    to the same value0
    smallmover.angle_max(backbone_angle_max)  # sets all at once
    #### use the overloaded version of the SmallMover.angle_max method if you
    ####    want to use secondary structure biased moves
    #smallmover.angle_max('H', backbone_angle_max)
    #smallmover.angle_max('E', backbone_angle_max)
    #smallmover.angle_max('L', backbone_angle_max)

    # 6. create a ShearMover
    # a ShearMover is identical to a SmallMover except that the angles perturbed
    #    are instead a random (free in the MoveMap) residue's phi and the
    #    preceding residue's psi, this reduces the downstream structural change
    # set the maximum angle to backbone_angle_max, apply it shearmoves times
    shearmover = protocols.simple_moves.ShearMover(movemap, kT, shearmoves)
    # same angle_max restictions as SmallMover
    shearmover.angle_max(backbone_angle_max)
    #### use the overloaded version of the SmallMover.angle_max method if you
    ####    want to use secondary structure biased moves
    #shearmover.angle_max('H', backbone_angle_max)
    #shearmover.angle_max('E', backbone_angle_max)
    #shearmover.angle_max('L', backbone_angle_max)

    # 7. create a MinMover, for backbone torsion minimization
    minmover = protocols.minimization_packing.MinMover()
    minmover.movemap(movemap)
    minmover.score_function(scorefxn)

    #### sidechain refinement protocol, simple packing

    # 8. setup a PackRotamersMover
    to_pack = standard_packer_task(starting_pose)
    to_pack.restrict_to_repacking()  # prevents design, packing only
    to_pack.or_include_current(True)  # considers the original sidechains
    packmover = protocols.minimization_packing.PackRotamersMover(
        scorefxn, to_pack)

    #### assess the new structure
    # 9. create a PyMOLMover
    pymover = PyMOLMover()
    # uncomment the line below to load structures into successive states
    #pymover.keep_history(True)
    #### the PyMOLMover slows down the protocol SIGNIFICANTLY but provides
    ####    very informative displays
    #### the keep_history flag (when True) tells the PyMOLMover to store new
    ####    structures into successive states, for a single trajectory, this
    ####    allows you to see intermediate changes (depending on where the
    ####    PyMOLMover is applied), when using a JobDistributor or otherwise
    ####    displaying multiple trajectories with a single protocol, the output
    ####    can get confusing to interpret, by changing the pose's PDBInfo.name
    ####    the structure will load into a new PyMOL state
    #### try uncommenting the lines below to see different output
    #pymover.update_energy(True)    # see the total score in color

    # 10. export the original structure, and scores, to PyMOL
    pymover.apply(pose)
    scorefxn(pose)
    pymover.send_energy(pose)

    # 11. setup a RepeatMover on a TrialMover of a SequenceMover (wow!)
    # -setup a TrialMover
    #    a. create a SequenceMover of the previous moves
    #### add any other moves you desire
    combined_mover = SequenceMover()
    combined_mover.add_mover(smallmover)
    combined_mover.add_mover(shearmover)
    combined_mover.add_mover(minmover)
    combined_mover.add_mover(packmover)
    #### explore the protocol using the PyMOLMover, try viewing structures
    ####    before they are accepted or rejected
    combined_mover.add_mover(pymover)
    #    b. create a MonteCarlo object to define success/failure
    mc = MonteCarlo(pose, scorefxn, kT)  # must reset for each trajectory!
    # c. create the TrialMover
    trial = TrialMover(combined_mover, mc)

    #### explore the protocol using the PyMOLMover, try viewing structures
    ####    after acceptance/rejection, comment-out the lines below
    #original_trial = TrialMover(combined_mover, mc)
    #trial = SequenceMover()
    #trial.add_mover(original_trial)
    #trial.add_mover(pymover)

    #### for each trajectory, try cycles number of applications

    # -create the RepeatMover
    refinement = RepeatMover(trial, cycles)
    ####

    # 12. create a (Py)JobDistributor
    jd = PyJobDistributor(job_output, jobs, scorefxn)
    jd.native_pose = starting_pose

    # 13. store the score evaluations for output
    # printing the scores as they are produced would be difficult to read,
    #    Rosetta produces a lot of verbose output when running
    scores = [0] * (jobs + 1)
    scores[0] = scorefxn(starting_pose)

    # 14. perform the refinement protocol
    counter = 0  # for exporting to PyMOL
    while not jd.job_complete:
        # a. set necessary variables for the new trajectory
        # -reload the starting pose
        pose.assign(starting_pose)
        # -change the pose's PDBInfo.name, for the PyMOLMover
        counter += 1
        pose.pdb_info().name(job_output + '_' + str(counter))
        # -reset the MonteCarlo object (sets lowest_score to that of p)
        mc.reset(pose)
        #### if you create a custom protocol, you may have additional
        ####    variables to reset, such as kT

        #### if you create a custom protocol, this section will most likely
        ####    change, many protocols exist as single Movers or can be
        ####    chained together in a sequence (see above) so you need
        ####    only apply the final Mover
        # b. apply the refinement protocol
        refinement.apply(pose)
        ####

        # c. output the lowest scoring decoy structure for this trajectory
        # -recover and output the decoy structure to a PDB file
        mc.recover_low(pose)
        jd.output_decoy(pose)
        # -export the final structure to PyMOL for each trajectory
        pose.pdb_info().name(job_output + '_' + str(counter) + '_final')
        pymover.apply(pose)
        pymover.send_energy(pose)  # see the total score in color

        # -store the final score for this trajectory
        scores[counter] = scorefxn(pose)

    # 15. output the score evaluations
    print('Original Score\t:\t', scores[0])
    for i in range(1, len(scores)):  # print out the job scores
        print(job_output + '_' + str(i) + '\t:\t', scores[i])

    return scores  # for other protocols
コード例 #20
0
)  # -loops:test_cycles is only needed for self-test, please make sure to remove it on production run
# WARNING: option '-constant_seed' is for testing only! MAKE SURE TO REMOVE IT IN PRODUCTION RUNS!!!!!
import os
os.chdir('.test.output')

p = core.import_pose.pose_from_file("../test/data/2cpl_min.pdb")

starting_p = Pose()
starting_p.assign(p)

scorefxn_low = protocols.loops.get_cen_scorefxn(
)  #  create_score_function( 'cen_std' )
scorefxn_high = protocols.loops.get_fa_scorefxn(
)  #  create_score_function_ws_patch( 'standard', 'score12' )

pymol = PyMOLMover()  # If Pymol server is running, centroid stage will display

loop_begin = 145
loop_end = 155
loop_cut = 150
my_loop = protocols.loops.Loop(loop_begin, loop_end, loop_cut)
my_loops = protocols.loops.Loops()
my_loops.add_loop(my_loop)
print(my_loop)

protocols.loops.set_single_loop_fold_tree(p, my_loop)

movemap = MoveMap()
movemap.set_bb_true_range(loop_begin, loop_end)
movemap.set_chi(True)
コード例 #21
0
        torsion = pose.psi(res)
        a = random.gauss(torsion, 25)
        pose.set_psi(res, a)


# initialize pose objects
last_pose = Pose()
low_pose = Pose()

# create poly-A chain and set all peptide bonds to trans
p = pose_from_sequence("AAAAAAAAAA", "fa_standard")
for res in range(1, p.total_residue() + 1):
    p.set_omega(res, 180)

# use the PyMOLMover to echo this structure to PyMOL
pmm = PyMOLMover()
pmm.apply(p)

# set score function to include Van der Wals and H-bonds only
score = ScoreFunction()
score.set_weight(fa_atr, 0.8)
score.set_weight(fa_rep, 0.44)
score.set_weight(hbond_sr_bb, 1.17)

# initialize low score objects
low_pose.assign(p)
low_score = score(p)

for i in range(100):
    last_score = score(p)
    last_pose.assign(p)
コード例 #22
0
hset = ras.get_hbonds()
hset.show(ras)
hset.show(ras, 24)

pose = pose_from_file("../test/data/workshops/1YY9.clean.pdb")

rsd1_num = pose.pdb_info().pdb2pose('D', 102)
rsd2_num = pose.pdb_info().pdb2pose('A', 408)
print(rsd1_num)
print(rsd2_num)
rsd1 = pose.residue(rsd1_num)
rsd2 = pose.residue(rsd2_num)

emap = EMapVector()
scorefxn.eval_ci_2b(rsd1, rsd2, pose, emap)
print(emap[fa_atr])
print(emap[fa_rep])
print(emap[fa_sol])

pymol = PyMOLMover()
ras.pdb_info().name("ras")
pymol.send_energy(ras)
pymol.send_energy(ras, "fa_atr")
pymol.send_energy(ras, "fa_sol")
pymol.update_energy(True)
pymol.energy_type(fa_atr)
pymol.apply(ras)
# no longer supported: pymol.label_energy(ras, "fa_rep")
# no longer supported: pymol.send_hbonds(ras)