schrodinger.application.jaguar.utils module¶
Jaguar utility functions.
Copyright Schrodinger, LLC. All rights reserved.
- class schrodinger.application.jaguar.utils.FreeEnergy(temp, gibbs, property_key)¶
Bases:
tuple
- temp: float¶
Alias for field number 0
- gibbs: float¶
Alias for field number 1
- property_key: str¶
Alias for field number 2
- __contains__(key, /)¶
Return key in self.
- __len__()¶
Return len(self).
- count(value, /)¶
Return number of occurrences of value.
- index(value, start=0, stop=9223372036854775807, /)¶
Return first index of value.
Raises ValueError if the value is not present.
- class schrodinger.application.jaguar.utils.ChgAt(index, charge)¶
Bases:
tuple
- index: int¶
Alias for field number 0
- charge: int¶
Alias for field number 1
- __contains__(key, /)¶
Return key in self.
- __len__()¶
Return len(self).
- count(value, /)¶
Return number of occurrences of value.
- class schrodinger.application.jaguar.utils.LewisStructure(charges, bonds, score, unpaired)¶
Bases:
tuple
- charges: List[schrodinger.application.jaguar.utils.ChgAt]¶
Alias for field number 0
- bonds: List[Tuple[int, int]]¶
Alias for field number 1
- score: float¶
Alias for field number 2
- unpaired: bool¶
Alias for field number 3
- __contains__(key, /)¶
Return key in self.
- __len__()¶
Return len(self).
- count(value, /)¶
Return number of occurrences of value.
- index(value, start=0, stop=9223372036854775807, /)¶
Return first index of value.
Raises ValueError if the value is not present.
- class schrodinger.application.jaguar.utils.LewisModes(value)¶
Bases:
enum.IntEnum
An enumeration.
- STD = 0¶
- PRINT = 1¶
- RINGCHAIN = 2¶
- THOROUGH = 3¶
- FINDALL = 4¶
- exception schrodinger.application.jaguar.utils.RingFlipError¶
Bases:
ValueError
Error in when flipping rings that indicates bad or insufficient user input.
- __init__(*args, **kwargs)¶
- args¶
- with_traceback()¶
Exception.with_traceback(tb) – set self.__traceback__ to tb and return self.
- schrodinger.application.jaguar.utils.append_outfiles_to_recover_file(recover_file: str, outfiles: Iterable[str])¶
Append list of output file paths to a YAML-format .recover file.
- Parameters
recover_file – .recover file name
outfiles – output file paths
- schrodinger.application.jaguar.utils.get_jobname(prefix: str, str_to_hash: str) str ¶
Construct a jobname based on the given string prefix (typically the backend script name) and a string to be hashed (typically based on the cmdline being used to invoke the job.)
- schrodinger.application.jaguar.utils.split_jag_ext(filename)¶
Split the extension off the filename, but account for the fact that Jaguar extensions might be .xx.mae, where xx are some digits. bob.01.mae -> bob bob.out -> bob bob.maegz -> bob, etc.
- Parameters
filename (str) – The file name to split
- Return type
str
- Returns
The base file name without extension
- schrodinger.application.jaguar.utils.restart_name(input_name: str, mae_name: Optional[str] = None) str ¶
Wrapper to extract restartname from mmjag routine
Allows for calls where
mae_name
is not defined or where input name is an empty string (would cause segfault in mmjag function)
- schrodinger.application.jaguar.utils.basic_windows_path(dos_path: str) str ¶
Convert extended length Windows path to standard. Does nothing on other OS’s.
- Parameters
dos_path – a (Windows) file path, which may have WINDOWS_EXTENDED_PATH_TAG to indicate extended path length
- Returns
A file path which has not extended length tags
- schrodinger.application.jaguar.utils.get_stoichiometry_string(atom_list: List[str]) str ¶
Take atom list and return stoichiometry string. For example, atom_list = [‘H’, ‘H’, ‘O’] yields stoichiometry string = ‘H2O’.
- Parameters
atom_list – list of element names
- Returns
stoichiometry string
- schrodinger.application.jaguar.utils.validate_stoichiometry(reactants: List[jin.JaguarInput], products: List[jin.JaguarInput]) Optional[str] ¶
This function validates stoichiometry for a reaction defined by the list of reactants and products. If stoichiometry is not valid this function return text string explaining what was wrong. In case of valid stoichiometry returns None.
- Parameters
reactants – list of
JaguarInput
objects for reactantsproducts – list of
JaguarInput
objects products
- Returns
string with warning message or None
- schrodinger.application.jaguar.utils.base_functional(func: str) str ¶
Extract basename of DFT functional
Removes a posteriori model suffixes from the functional, e.g. B3LYP-D3 -> B3LYP PBE0-d -> PBE0 b3lyp-loc-MM -> b3lyp
- Parameters
func – full name of functional, case-insensitive
- Returns
functional name, with corrections (e.g. dispersion, LOC) removed
- schrodinger.application.jaguar.utils.get_number_electrons(st: schrodinger.structure._structure.Structure) int ¶
Count the number of electrons disregarding charges.
- Parameters
st – the structure
- Returns
the number of electrons
- schrodinger.application.jaguar.utils.get_total_charge(structure: schrodinger.structure._structure.Structure) int ¶
Return the total charge of the structure If the property i_m_Molecular_charge is defined we use that, else we sum the formal charges
- Parameters
structure – whose total charge must be calculated
- Returns
total charge of structure
- schrodinger.application.jaguar.utils.elmnt_mult_dict() Dict[str, int] ¶
make a dictionary of element:multiplicity for all neutral elements up to Oganesson (118)
The values are from the ground state term symbol as reported by NIST at http://physics.nist.gov/PhysRefData/Elements/index.html as of 4.2014
- schrodinger.application.jaguar.utils.remove_gibbs_energies(st: schrodinger.structure._structure.Structure, allowed_temps: Tuple = ())¶
Remove gibbs energy properties from a structure but allow some exceptions. This allows one to ‘unclutter’ the project table.
- Parameters
st – structure containing gibbs energy properties
allowed_temps – temperatures that are allowed to remain as properties
- schrodinger.application.jaguar.utils.parse_gibbs_energies(st: schrodinger.structure._structure.Structure, inf_sep: bool = False, std_conc: bool = False)¶
Extract the temperature, gibbs energy and property keys for free energy and store these in a dict relating temperature to FreeEnergy instances.
- Parameters
st – the structure
inf_sep – True indicates infinitely separated energy
std_conc – True indicates Gibbs energy at std state concentration
- Returns
a dict relating temperature to a FreeEnergy instance with attributes storing these data
- schrodinger.application.jaguar.utils.gibbs_energy_property_string(temp: float, inf_sep: bool = False, std_conc: bool = False) str ¶
Construct the property key string for Gibbs energy at a particular temperature
- Parameters
temp – temperature in Kelvin
inf_sep – True indicates infinitely separated energy
std_conc – True indicates Gibbs energy at std state concentration
- Returns
a property key string
- schrodinger.application.jaguar.utils.convert_gibbs_energy_to_std_conc(st: schrodinger.structure._structure.Structure) Dict ¶
Convert std state (1 atm) Gibbs energies to a std state of 1 Molar concentration. The energies are returned as a dict relating temperature to FreeEnergy instances. The energies are also stored as structure level properties. This is intended to be used with AutoTS for rate calculations and we assume the free energies were computed at 1 atm of pressure.
- Parameters
st – the structure
- Returns
a dict relating temperature to a FreeEnergy instance with attributes storing these data
- schrodinger.application.jaguar.utils.compute_std_conc_gibbs_energy(gibbs: float, temp: float, press: float, con: float) float ¶
Convert Gibbs energy which was computed at a pressure of press to a concentration of con using the formula G = G_0 + kT log(CRT/P_0) where we’ve used the ideal gas law to relate P = CRT
- Parameters
gibbs – Gibbs free energy in a.u. evaluated at a pressure of press
press – Pressure at which the Gibbs energy was evaluated in atm
temp – Temperature at which the Gibbs energy was evaluated in Kelvin
con – Concentration which defines the standard state in moles/Liter
- schrodinger.application.jaguar.utils.group_items(items: List, comparator: Callable, **kwargs) List[List] ¶
Put items into groups using a comparator.
These will be returned as a list of lists, each list representing a group. The first item of the first group will be the first item in the list items. The groups have the property that Comparator(item1, item2, args) returns True for all pairs in a group.
- Parameters
items – a list of items to group
comparator – this function compares two items and returns a boolean indicating whether they are equivalent.
kwargs (keyword argument list) – keyword arguments passed to the comparator which is called as comparator(item1, item2,
*args
)
- Returns
a list of lists of items
- schrodinger.application.jaguar.utils.beta_au(temp: float) float ¶
Beta = 1/kT in a.u.
- schrodinger.application.jaguar.utils.beta_kcalmol(temp: float) float ¶
Beta = 1/kT in kcal/mol
- schrodinger.application.jaguar.utils.copy_structure_bonding(ref_st: schrodinger.structure._structure.Structure, updated_st: schrodinger.structure._structure.Structure)¶
Copy all bonding and formal charges from reference structure onto a structure instance we want to update. Also update FF atom-typing. Assumes number of atoms and atom numbering is the same in both structures.
- Parameters
ref_st – structure to copy bonding from
updated_st – structure to copy bonding to
- schrodinger.application.jaguar.utils.sync_dummy_atoms(ref_st: schrodinger.structure._structure.Structure, st: schrodinger.structure._structure.Structure)¶
Sync dummy atoms in ref_st and st. This is useful after calling mmjag_connect to reset bonding. We check atomic number and XYZ coordinates to classify which atoms are the “same” or “different”. But note for dummy atoms, we do not require XYZ to be the same.
We then try to sync the two structures by handling two possibilities:
Existence of new dummy atoms at the end of the atom list in ref_st compared to st; they will be added to the end of st.
Non-existence of dummy atoms at any location in ref_st compared to st; they will be deleted from st.
- Parameters
ref_st – structure to copy atoms from
st – structure to copy atoms to
- Raises
AssertionError – Fails to sync
- schrodinger.application.jaguar.utils.mmjag_reset_connectivity(st: schrodinger.structure._structure.Structure)¶
Reset connectivity and Lewis structure using mmjag algorithm. i.e input st is modified to have new bonds, bond orders and formal charges. All other properties should be preserved.
- Parameters
st – structure to clean up
- schrodinger.application.jaguar.utils.mmjag_update_lewis(st: schrodinger.structure._structure.Structure, mode: schrodinger.application.jaguar.utils.LewisModes = LewisModes.STD) List[schrodinger.application.jaguar.utils.LewisStructure] ¶
Update Lewis structure for a given connectivity using mmjag algorithm. This can be used instead of, or to complement, e.g. the mmlewis code. Unlike mmjag_reset_connectivity, the connectivity will be preserved.
If mode is
LewisModes.PRINT
, the lewis structure determination information will be returnedIf mode is
LewisModes.RINGCHAIN
, special Lewis structure scoring for ring-chain tautomers will be used (and lewis structure information will be returned)If mode is
LewisModes.THOROUGH
, the lewis structure search will be lengthenedIf mode is
LewisModes.FINDALL
, the lewis structure search will be lengthened and suboptimal results will be included in the output data (which is sorted to have the best first).If the mmjag Lewis code fails to update the bonding, the original bonding will be preserved.
- Parameters
st – structure to clean up
mode – specifies if std or ring-chain scoring should be used and whether the data is returned from lewis.cpp. Only STD, PRINT, RINGCHAIN, THOROUGH, and FINDALL are acceptable values
- Returns
If mode is PRINT, RINGCHAIN, THOROUGH, or FINDALL, parsed lewis structure data is returned as namedtuple; an empty list is returned if mode is STD.
- schrodinger.application.jaguar.utils.parse_lewis_data(lewis_data: List[str]) List[schrodinger.application.jaguar.utils.LewisStructure] ¶
Parse the string-formatted Lewis data from mmjag into a data structure for easy use.
- Parameters
lewis_data – the line-by-line output of mmjag/lewis.cpp run on a structure
- Returns
NamedTuples containing charge, multiple bond, and score
- schrodinger.application.jaguar.utils.get_charges(lewis_output: List[str]) Tuple[List[List[schrodinger.application.jaguar.utils.ChgAt]], List[bool]] ¶
Parse charges from lewis code string output
- Parameters
lewis_output – the line-by-line output of mmjag/lewis.cpp run on a structure
- Returns
For each structure in the lewis_output (the length of the list), list of the charged atom and their charges, whether structure contains unpaired spins
- schrodinger.application.jaguar.utils.get_bonds(lewis_output: List[str]) List[List[Tuple[int, int]]] ¶
Parse bonds from lewis code string output
- Parameters
lewis_output – the line-by-line output of mmjag/lewis.cpp run on a structure
- Returns
For each structure in the lewis_output (the length of the list), list of the multiple bonds in the structure (NB: a triple bond is noted by being present in the list twice)
- schrodinger.application.jaguar.utils.get_scores(lewis_output: List[str]) List[float] ¶
Parse scores from lewis code string output
- Parameters
lewis_output (list of strings) – the line-by-line output of mmjag/lewis.cpp run on a structure
- Return type
list of floats
- Returns
For each structure in the lewis_output (the length of the list), that structures score according to the mmjag/lewis.cpp code (see there for more details)
- schrodinger.application.jaguar.utils.apply_lewis(st: schrodinger.structure._structure.Structure, lewis_st: schrodinger.application.jaguar.utils.LewisStructure) schrodinger.structure._structure.Structure ¶
Return a copy of a structure with a Lewis structure as described by the LewisStructure given.
- Parameters
st – structure on which to apply Lewis structure
lewis_st – Namedtuple containing charge, multiple bond, and score
- Returns
a structure with the desired Lewis structure applied
- class schrodinger.application.jaguar.utils.GenOptions(kwdict=None)¶
Bases:
object
A class to convert keyword value pairs defined in a single string into a data structure, and allow them to be converted back into a string.
Here are some example strings:
'igeopt=1 mp2=3' 'igeopt=1 maxitg=1 iacc=1'
- eq_re = re.compile('\\s*=\\s*')¶
- key_val_re = re.compile('(?P<key>[^= ]+)=(?P<value>[^= \\n]+(\\s+\\d+)?)\\s*')¶
- OK = 0¶
- PARTIAL = 1¶
- ERROR = 2¶
- __init__(kwdict=None)¶
- static fromString(string)¶
Create a GenOptions instance from the provided string.
- static testString(string, gen_options=None)¶
Test the state of the provided string. If gen_options is provided, set its values based on the keyword value pairs in the string.
Parameters
- string (str)
Input string to read for settings.
- gen_options (GenOptions)
A gen_options instance to modify according to the values in ‘string’.
- toString()¶
- commandLineOptions()¶
- isEquivalent(other)¶
- schrodinger.application.jaguar.utils.is_spiro_junction(rings: List[List[int]], at_idx: int) bool ¶
Check if a given atom is a simple spiro junction between rings
If an atom is both part of a fused ring system and is a spiro junction, we will return False.
- Parameters
rings – ordered list of atom indexes proceeding around around a ring (as generated by
st.find_rings()
)at_idx – index of atom to check if it is a spiro junction, i.e. an atom which is the only atom shared between two rings.
- Returns
True if
at_idx
is a spiro junction
- schrodinger.application.jaguar.utils.flip_ring_conformation(st: schrodinger.structure._structure.Structure, at1_idx: int, at2_idx: Optional[int] = None) schrodinger.structure._structure.Structure ¶
Flip a ring conformation (i.e. boat-like) to a good (chair-like) one. Only applies to 4-membered rings or greater.
We fix the ring conformation by rotating the two torsions of the substituents on either side of
at1
(the atom of the ring on the “wrong” side). This keeps their substituents pointed in good places. Specifically,at1
is moved to the unique position (other than where it starts) with the same bond distances to its nearest neighbors in the ring and where all angles involving at1 and one side of the ring are preserved. We have to rotate one of the substituent-at1 torsions back to fix theat1
non-ring substituents.- Parameters
st – structure to fix the conformation of
at1_idx – atom index of the atom that needs to be flipped to the opposite side of the ring
at2_idx – atom index adjacent to
at1_idx
in the ring to be flipped, used to disambiguate in spiro compounds whenat1_idx
is the junction
- Returns
structure with corrected ring conformation
- schrodinger.application.jaguar.utils.get_signed_angles_for_ring_flip_torsions(b_at3_xyz: numpy.array, b_at2_xyz: numpy.array, at1_xyz: numpy.array, f_at2_xyz: numpy.array, f_at3_xyz: numpy.array) Tuple[float, float] ¶
Get the angles to rotate the torsions adjacent to the moving atom in a ring flip.
We rotate the two torsions on either side of
at1
(the atom of the ring that needs to move to the other side of the ring in the ring-flip) so that the substituents of those neighboring ring atoms (i.e. b_at2 and f_at2) are pointing in sensible directions. How the angle to rotate these torsions is calculated is a bit complicated.After some experimentation, the most reliable choice is to find the angle such that when rotating about the b_at3-b_at2 axis, the distance from at1 to f_at2 is held constant. This corresponds to finding the intersection of the circle swept out by at1 when rotating about the b_at3-b_at2 axis with the sphere of radius length(f_at2-at1). This intersection occurs at two points and at1 is currently at one of those points. We therefore need to find the angle about each torsion to rotate that moves at1 to the other point.
Note, this should make round-trips a no-op. Note also that the exact angles between substituents around b_at2 will be held constant but this is not the case for f_at2. In general, the angles to at1 of other f_at2 substituents can change, though the degree is usually small and especially so when the b_at3-b_at2 and f_at3-f_at2 axes are parallel which is often the case for 6-membered rings.
- Parameters
b_at3_xyz – xyz coordinates of the atom 2 positions “behind” the atom being flipped
b_at2_xyz – xyz coordinates of the atom 1 position “behind” the atom being flipped
at1_xyz – xyz coordinates of the atom being flipped
f_at2_xyz – xyz coordinates of the atom 1 position “ahead” the atom being flipped
f_at3_xyz – xyz coordinates of the atom 2 positions “ahead” the atom being flipped
- schrodinger.application.jaguar.utils.get_3point_normal(center: numpy.array, sub1: numpy.array, sub2: numpy.array, sub3: numpy.array) numpy.array ¶
Get the hypothetical location of a 4th tetrahedral substituent from center atom and three substituents, 1A from center.
- Parameters
center – xyz coordinates of central atom assumed to be a tetrahedron
sub1 – xyz coordinates of first substituent of
center
sub2 – xyz coordinates of second substituent of
center
sub3 – xyz coordinates of third substituent of
center
- Returns
xyz coordinates of 4th substituent, at unit distance from
center
- schrodinger.application.jaguar.utils.get_plane_alignment_angle(at1: numpy.array, at2: numpy.array, at3: numpy.array, at4: numpy.array, at5: numpy.array, at6: numpy.array, rot_axis: numpy.array) float ¶
Determine the angle about
rot_axis
to rotate the plane defined byat4
,at5
, andat6
such that it is aligned with the plane defined byat1
,at2
, andat3
.That is, define a plane P1 by points
at1
,at2
, andat3
and a plane P2 byat4
,at5
, andat6
. Suppose we can rotate the pointsat4
,at5
, andat6
about an axis defined byrot_axis
. The function returns the angle that makes the angle between P1 and P2 0 (degrees).- Parameters
at1 – xyz-coordinate of point1 in P1
at2 – xyz-coordinate of point2 in P1
at3 – xyz-coordinate of point3 in P1
at4 – xyz-coordinate of point1 in P2
at5 – xyz-coordinate of point2 in P2
at6 – xyz-coordinate of point3 in P2
rot_axis – vector defining rotation axis
- Returns
angle which aligns P1 and P2 when P2 is rotated about rot_axis
- schrodinger.application.jaguar.utils.project_vec_onto_plane(vec, plane_normal)¶
Project a vector onto a plane defined by a vector normal to the plane