Routines & Functions¶
The distribution version of the Tinker package contains over 1000 separate programs, subroutines and functions. This section contains a brief description of the purpose of most of these code units. Further information can be found in the comments located at the top of each source code file.
ACTIVE Subroutine
“active” sets the list of atoms that are used during each potential energy function calculation
ADDBASE Subroutine
“addbase” builds the Cartesian coordinates for a single nucleic acid base; coordinates are read from the Protein Data Bank file or found from internal coordinates, then atom types are assigned and connectivity data generated
ADDBOND Subroutine
“addbond” adds entries to the attached atoms list in order to generate a direct connection between two atoms
ADDIONS Subroutine
“addions” takes a currently defined solvated system and places ions, with removal of solvent molecules
ADDSIDE Subroutine
“addside” builds the Cartesian coordinates for a single amino acid side chain; coordinates are read from the Protein Data Bank file or found from internal coordinates, then atom types are assigned and connectivity data generated
ADJACENT Function
“adjacent” finds an atom connected to atom “i1” other than atom “i2”; if no such atom exists, then the closest atom in space is returned
ADJUST Subroutine
“adjust” modifies site bounds on the PME grid and returns an offset into the B-spline coefficient arrays
ALCHEMY Program
“alchemy” computes the free energy difference corresponding to a small perturbation by Boltzmann weighting the potential energy difference over a number of sample states; current version (incorrectly) considers the charge energy to be intermolecular in finding the perturbation energies
ALTELEC Subroutine
“altelec” constructs mutated electrostatic parameters based on the lambda mutation parameter “elambda”
ALTERCHG Subroutine
“alterchg” calculates the change in atomic partial charge or monopole values due to bond and angle charge flux coupling
ALTERPOL Subroutine
“alterpol” finds an output set of atomic multipole parameters which when used with an intergroup polarization model will give the same electrostatic potential around the molecule as the input set of multipole parameters with all atoms in one polarization group
ALTTORS Subroutine
“alttors” constructs mutated torsional parameters based on the lambda mutation parameter “tlambda”
AMBERYZE Subroutine
“amberyze” prints the force field parameters in a format needed by the Amber setup protocol for using AMOEBA within Amber
ANALYSIS Subroutine
“analysis” calls the series of routines needed to calculate the potential energy and perform energy partitioning analysis in terms of type of interaction or atom number
ANALYZE Program
“analyze” computes and displays the total potential energy; options are provided to display system and force field info, partition the energy by atom or by potential function type, show force field parameters by atom; output the large energy interactions and find electrostatic and inertial properties
ANGCHG Subroutine
“angchg” computes modifications to atomic partial charges or monopoles due to angle bending using a charge flux formulation
ANGGUESS Function
“angguess” sets approximate angle bend force constants based on atom type and connected atoms
ANGLES Subroutine
“angles” finds the total number of bond angles and stores the atom numbers of the atoms defining each angle; for each angle to a trivalent central atom, the third bonded atom is stored for use in out-of-plane bending
ANNEAL Program
“anneal” performs a simulated annealing protocol by means of variable temperature molecular dynamics using either linear, exponential or sigmoidal cooling schedules
ANORM Function
“anorm” finds the norm (length) of a vector; used as a service routine by the Connolly surface area and volume computation
APBSEMPOLE Subroutine
APBSFINAL Subroutine
APBSINDUCE Subroutine
APBSINITIAL Subroutine
APBSNLINDUCE Subroutine
ARCEDIT Program
“arcedit” is a utility program for coordinate files which concatenates multiple coordinate sets into a new archive or performs any of several manipulations on an existing archive
ASET Subroutine
“aset” computes by recursion the A functions used in the evaluation of Slater-type (STO) overlap integrals
ATOMYZE Subroutine
“atomyze” prints the potential energy components broken down by atom and to a choice of precision
ATTACH Subroutine
“attach” generates lists of 1-3, 1-4 and 1-5 connectivities starting from the previously determined list of attached atoms (ie, 1-2 connectivity)
AUXINIT Subroutine
“auxinit” initializes auxiliary variables and settings for inertial extended Lagrangian induced dipole prediction
AVGPOLE Subroutine
“avgpole” condenses the number of multipole atom types based upon atoms with equivalent attachments and additional user specified sets of equivalent atoms
BAOAB Subroutine
“baoab” implements a constrained stochastic dynamics time step using the geodesic BAOAB scheme
BAR Program
“bar” computes the free energy, enthalpy and entropy difference between two states via Zwanzig free energy perturbation (FEP) and Bennett acceptance ratio (BAR) methods
BARCALC Subroutine
BASEFILE Subroutine
“basefile” extracts from an input filename the portion consisting of any directory name and the base filename; also reads any keyfile and sets information level values
BCUCOF Subroutine
“bcucof” determines the coefficient matrix needed for bicubic interpolation of a function, gradients and cross derivatives
BCUINT Subroutine
“bcuint” performs a bicubic interpolation of the function value on a 2D spline grid
BCUINT1 Subroutine
“bcuint1” performs a bicubic interpolation of the function value and gradient along the directions of a 2D spline grid
BCUINT2 Subroutine
“bcuint2” performs a bicubic interpolation of the function value, gradient and Hessian along the directions of a 2D spline grid
BEEMAN Subroutine
“beeman” performs a single molecular dynamics time step via the Beeman multistep recursion formula; uses original coefficients or Bernie Brooks’ “Better Beeman” values
BETACF Function
“betacf” computes a rapidly convergent continued fraction needed by routine “betai” to evaluate the cumulative Beta distribution
BETAI Function
“betai” evaluates the cumulative Beta distribution function as the probability that a random variable from a distribution with Beta parameters “a” and “b” will be less than “x”
BIGBLOCK Subroutine
“bigblock” replicates the coordinates of a single unit cell to give a larger unit cell as a block of repeated units
BIOSORT Subroutine
“biosort” renumbers and formats biotype parameters used to convert biomolecular structure into force field atom types
BITORS Subroutine
“bitors” finds the total number of bitorsions as pairs of adjacent torsional angles, and the numbers of the five atoms defining each bitorsion
BMAX Function
“bmax” computes the maximum order of the B functions needed for evaluation of Slater-type (STO) overlap integrals
BNDCHG Subroutine
“bndchg” computes modifications to atomic partial charges or monopoles due to bond stretch using a charge flux formulation
BNDERR Function
“bnderr” is the distance bound error function and derivatives; this version implements the original and Havel’s normalized lower bound penalty, the normalized version is preferred when lower bounds are small (as with NMR NOE restraints), the original penalty is needed if large lower bounds are present
BNDGUESS Function
“bndguess” sets approximate bond stretch force constants based on atom type and connected atoms
BONDS Subroutine
“bonds” finds the total number of covalent bonds and stores the atom numbers of the atoms defining each bond
BORN Subroutine
“born” computes the Born radius of each atom for use with the various implicit solvation models
BORN1 Subroutine
“born1” computes derivatives of the Born radii with respect to atomic coordinates and increments total energy derivatives and virial components for potentials involving Born radii
BOUNDS Subroutine
“bounds” finds the center of mass of each molecule and translates any stray molecules back into the periodic box
BOXMIN Subroutine
“boxmin” uses minimization of valence and vdw potential energy to expand and refine a collection of solvent molecules in a periodic box
BOXMIN1 Function
“boxmin1” is a service routine that computes the energy and gradient during refinement of a periodic box
BSET Subroutine
“bset” computes by downward recursion the B functions used in the evaluation of Slater-type (STO) overlap integrals
BSPLGEN Subroutine
“bsplgen” gets B-spline coefficients and derivatives for a single PME atomic site along a particular direction
BSPLINE Subroutine
“bspline” calculates the coefficients for an n-th order B-spline approximation
BSPLINE_FILL Subroutine
“bspline_fill” finds B-spline coefficients and derivatives for PME atomic sites along the fractional coordinate axes
BSSTEP Subroutine
“bsstep” takes a single Bulirsch-Stoer step with monitoring of local truncation error to ensure accuracy
BUSSI Subroutine
“bussi” performs a single molecular dynamics time step via the Bussi-Parrinello isothermal-isobaric algorithm
CALENDAR Subroutine
“calendar” returns the current time as a set of integer values representing the year, month, day, hour, minute and second
CART_TO_FRAC Subroutine
“cart_to_frac” computes a transformation matrix to convert a multipole object in Cartesian coordinates to fractional
CBUILD Subroutine
“cbuild” performs a complete rebuild of the partial charge electrostatic neighbor list for all sites
CELLANG Subroutine
“cellang” computes atomic coordinates and unit cell parameters from fractional coordinates and lattice vectors
CELLATOM Subroutine
“cellatom” completes the addition of a symmetry related atom to a unit cell by updating the atom type and attachment arrays
CENTER Subroutine
“center” moves the weighted centroid of each coordinate set to the origin during least squares superposition
CERROR Subroutine
“cerror” is the error handling routine for the Connolly surface area and volume computation
CFFTB Subroutine
“cfftb” computes the backward complex discrete Fourier transform, the Fourier synthesis
CFFTB1 Subroutine
CFFTF Subroutine
“cfftf” computes the forward complex discrete Fourier transform, the Fourier analysis
CFFTF1 Subroutine
CFFTI Subroutine
“cffti” initializes arrays used in both forward and backward transforms; “ifac” is the prime factorization of “n”, and “wsave” contains a tabulation of trigonometric functions
CFFTI1 Subroutine
CHIRER Function
“chirer” computes the chirality error and its derivatives with respect to atomic Cartesian coordinates as a sum the squares of deviations of chiral volumes from target values
CHKANGLE Subroutine
“chkangle” tests angles to be constrained for their presence in small rings and removes constraints that are redundant
CHKAROM Function
“chkatom” tests for the presence of a specified atom as a member of an aromatic ring
CHKPOLE Subroutine
“chkpole” inverts atomic multipole moments as necessary at sites with chiral local reference frame definitions
CHKRING Subroutine
“chkring” tests an atom or a set of connected atoms for their presence within a single 3- to 6-membered ring
CHKSIZE Subroutine
“chksize” computes a measure of overall global structural expansion or compaction from the number of excess upper or lower bounds matrix violations
CHKSOCKET Subroutine
CHKTREE Subroutine
“chktree” tests a minimum energy structure to see if it belongs to the correct progenitor in the existing map
CHKTTOR Subroutine
“chkttor” tests the attached atoms at a torsion-torsion central site and inverts the angle values if the site is chiral
CHKXYZ Subroutine
“chkxyz” finds any pairs of atoms with identical Cartesian coordinates, and prints a warning message
CHOLESKY Subroutine
“cholesky” uses a modified Cholesky method to solve the linear system Ax = b, returning “x” in “b”; “A” is a real symmetric positive definite matrix with its upper triangle (including the diagonal) stored by rows
CIRPLN Subroutine
“cirpln” determines the points of intersection between a specified circle and plane
CJKM Function
“cjkm” computes the coefficients of spherical harmonics expressed in prolate spheroidal coordinates
CLIGHT Subroutine
“clight” performs a complete rebuild of the partial charge pair neighbor list for all sites using the method of lights
CLIMBER Subroutine
CLIMBRGD Subroutine
CLIMBROT Subroutine
CLIMBTOR Subroutine
CLIMBXYZ Subroutine
CLIST Subroutine
“clist” performs an update or a complete rebuild of the nonbonded neighbor lists for partial charges
CLUSTER Subroutine
“cluster” gets the partitioning of the system into groups and stores a list of the group to which each atom belongs
CMP_TO_FMP Subroutine
“cmp_to_fmp” transforms the atomic multipoles from Cartesian to fractional coordinates
COLUMN Subroutine
“column” takes the off-diagonal Hessian elements stored as sparse rows and sets up indices to allow column access
COMMAND Subroutine
“command” uses the standard Unix-like iargc/getarg routines to get the number and values of arguments specified on the command line at program runtime
COMPRESS Subroutine
“compress” transfers only the non-buried tori from the temporary tori arrays to the final tori arrays
CONNECT Subroutine
“connect” sets up the attached atom arrays starting from a set of internal coordinates
CONNOLLY Subroutine
“connolly” uses the algorithms from the AMS/VAM programs of Michael Connolly to compute the analytical molecular surface area and volume of a collection of spherical atoms; thus it implements Fred Richards’ molecular surface definition as a set of analytically defined spherical and toroidal polygons
CONNYZE Subroutine
“connyze” prints information onconnected atoms as lists of all atom pairs that are 1-2 through 1-5 interactions
CONTACT Subroutine
“contact” constructs the contact surface, cycles and convex faces
CONTROL Subroutine
“control” gets initial values for parameters that determine the output style and information level provided by Tinker
COORDS Subroutine
“coords” converts the three principal eigenvalues/vectors from the metric matrix into atomic coordinates, and calls a routine to compute the rms deviation from the bounds
CORRELATE Program
“correlate” computes the time correlation function of some user-supplied property from individual snapshot frames taken from a molecular dynamics or other trajectory
CREATEJVM Subroutine
CREATESERVER Subroutine
CREATESYSTEM Subroutine
CREATEUPDATE Subroutine
CRYSTAL Program
“crystal” is a utility which converts between fractional and Cartesian coordinates, and can generate full unit cells from asymmetric units
CSPLINE Subroutine
“cspline” computes the coefficients for a periodic interpolating cubic spline
CUTOFFS Subroutine
“cutoffs” initializes and stores spherical energy cutoff distance windows, Hessian element and Ewald sum cutoffs, and allocates pairwise neighbor lists
CYTSY Subroutine
“cytsy” solves a system of linear equations for a cyclically tridiagonal, symmetric, positive definite matrix
CYTSYP Subroutine
“cytsyp” finds the Cholesky factors of a cyclically tridiagonal symmetric, positive definite matrix given by two vectors
CYTSYS Subroutine
“cytsys” solves a cyclically tridiagonal linear system given the Cholesky factors
D1D2 Function
“d1d2” is a utility function used in computation of the reaction field recursive summation elements
DAMPDIR Subroutine
“dampdir” generates coefficients for the direct field damping function for powers of the interatomic distance
DAMPEWALD Subroutine
“dampewald” generates coefficients for Ewald error function damping for powers of the interatomic distance
DAMPMUT Subroutine
“dampmut” generates coefficients for the mutual field damping function for powers of the interatomic distance
DAMPPOLAR Subroutine
“damppolar” generates coefficients for the charge penetration damping function used for polarization interactions
DAMPPOLE Subroutine
“damppole” generates coefficients for the charge penetration damping function for powers of the interatomic distance
DAMPPOT Subroutine
“damppot” generates coefficients for the charge penetration damping function used for the electrostatic potential
DAMPREP Subroutine
“damprep” generates coefficients for the Pauli repulsion damping function for powers of the interatomic distance
DAMPTHOLE Subroutine
“dampthole” finds coefficients for the original Thole damping function used by AMOEBA and for mutual polarization by AMOEBA+
DAMPTHOLED Subroutine
“damptholed” finds coefficients for the original Thole damping function used by AMOEBA or for the alternate direct polarization damping used by AMOEBA+
DBUILD Subroutine
“dbuild” performs a complete rebuild of the damped dispersion neighbor list for all sites
DCFLUX Subroutine
“dcflux” takes as input the electrostatic potential at each atomic site and calculates gradient chain rule corrections due to charge flux coupled with bond stretching and angle bending
DEFLATE Subroutine
“deflate” uses the power method with deflation to compute the few largest eigenvalues and eigenvectors of a symmetric matrix
DELETE Subroutine
“delete” removes a specified atom from the Cartesian coordinates list and shifts the remaining atoms
DEPTH Function
DESTROYJVM Subroutine
DESTROYSERVER Subroutine
DFIELD0A Subroutine
“dfield0a” computes the direct electrostatic field due to permanent multipole moments via a double loop
DFIELD0B Subroutine
“dfield0b” computes the direct electrostatic field due to permanent multipole moments via a pair list
DFIELD0C Subroutine
“dfield0c” computes the mutual electrostatic field due to permanent multipole moments via Ewald summation
DFIELD0D Subroutine
“dfield0d” computes the direct electrostatic field due to permanent multipole moments for use with with generalized Kirkwood implicit solvation
DFIELD0E Subroutine
“dfield0e” computes the direct electrostatic field due to permanent multipole moments for use with in Poisson-Boltzmann
DFIELDI Subroutine
“dfieldi” computes the electrostatic field due to permanent multipole moments
DFTMOD Subroutine
“dftmod” computes the modulus of the discrete Fourier transform of “bsarray” and stores it in “bsmod”
DIAGBLK Subroutine
“diagblk” performs diagonalization of the Hessian for a block of atoms within a larger system
DIAGQ Subroutine
“diagq” is a matrix diagonalization routine which is derived from the classical given, housec, and eigen algorithms with several modifications to increase efficiency and accuracy
DIFFEQ Subroutine
“diffeq” performs the numerical integration of an ordinary differential equation using an adaptive stepsize method to solve the corresponding coupled first-order equations of the general form dyi/dx = f(x,y1,…,yn) for yi = y1,…,yn
DIFFUSE Program
“diffuse” finds the self-diffusion constant for a homogeneous liquid via the Einstein relation from a set of stored molecular dynamics frames; molecular centers of mass are unfolded and mean squared displacements are computed versus time separation
DIST2 Function
“dist2” finds the distance squared between two points; used as a service routine by the Connolly surface area and volume computation
DISTGEOM Program
“distgeom” uses a metric matrix distance geometry procedure to generate structures with interpoint distances that lie within specified bounds, with chiral centers that maintain chirality, and with torsional angles restrained to desired values; the user also has the ability to interactively inspect and alter the triangle smoothed bounds matrix prior to embedding
DLIGHT Subroutine
“dlight” performs a complete rebuild of the damped dispersion pair neighbor list for all sites using the method of lights
DLIST Subroutine
“dlist” performs an update or a complete rebuild of the nonbonded neighbor lists for damped dispersion sites
DMDUMP Subroutine
“dmdump” puts the distance matrix of the final structure into the upper half of a matrix, the distance of each atom to the centroid on the diagonal, and the individual terms of the bounds errors into the lower half of the matrix
DOCUMENT Program
“document” generates a formatted description of all the routines and modules, an index of routines called by each source file, a list of all valid keywords, a list of include file dependencies as needed by a Unix-style Makefile, or a formatted force field parameter summary
DOT Function
“dot” finds the dot product of two vectors
DSTMAT Subroutine
“dstmat” selects a distance matrix containing values between the previously smoothed upper and lower bounds; the distance values are chosen from uniform distributions, in a triangle correlated fashion, or using random partial metrization
DYNAMIC Program
“dynamic” computes a molecular or stochastic dynamics trajectory in one of the standard statistical mechanical ensembles and using any of several possible integration methods
EANGANG Subroutine
“eangang” calculates the angle-angle potential energy
EANGANG1 Subroutine
“eangang1” calculates the angle-angle potential energy and first derivatives with respect to Cartesian coordinates
EANGANG2 Subroutine
“eangang2” calculates the angle-angle potential energy second derivatives with respect to Cartesian coordinates using finite difference methods
EANGANG2A Subroutine
“eangang2a” calculates the angle-angle first derivatives for a single interaction with respect to Cartesian coordinates; used in computation of finite difference second derivatives
EANGANG3 Subroutine
“eangang3” calculates the angle-angle potential energy; also partitions the energy among the atoms
EANGLE Subroutine
“eangle” calculates the angle bending potential energy; projected in-plane angles at trigonal centers, special linear or Fourier angle bending terms are optionally used
EANGLE1 Subroutine
“eangle1” calculates the angle bending potential energy and the first derivatives with respect to Cartesian coordinates; projected in-plane angles at trigonal centers, special linear or Fourier angle bending terms are optionally used
EANGLE2 Subroutine
“eangle2” calculates second derivatives of the angle bending energy for a single atom using a mixture of analytical and finite difference methods; projected in-plane angles at trigonal centers, special linear or Fourier angle bending terms are optionally used
EANGLE2A Subroutine
“eangle2a” calculates bond angle bending potential energy second derivatives with respect to Cartesian coordinates
EANGLE2B Subroutine
“eangle2b” computes projected in-plane bending first derivatives for a single angle with respect to Cartesian coordinates; used in computation of finite difference second derivatives
EANGLE3 Subroutine
“eangle3” calculates the angle bending potential energy, also partitions the energy among the atoms; projected in-plane angles at trigonal centers, spceial linear or Fourier angle bending terms are optionally used
EANGTOR Subroutine
“eangtor” calculates the angle-torsion potential energy
EANGTOR1 Subroutine
“eangtor1” calculates the angle-torsion energy and first derivatives with respect to Cartesian coordinates
EANGTOR2 Subroutine
“eangtor2” calculates the angle-torsion potential energy second derivatives with respect to Cartesian coordinates
EANGTOR3 Subroutine
“eangtor3” calculates the angle-torsion potential energy; also partitions the energy terms among the atoms
EBOND Subroutine
“ebond” calculates the bond stretching energy
EBOND1 Subroutine
“ebond1” calculates the bond stretching energy and first derivatives with respect to Cartesian coordinates
EBOND2 Subroutine
“ebond2” calculates second derivatives of the bond stretching energy for a single atom at a time
EBOND3 Subroutine
“ebond3” calculates the bond stretching energy; also partitions the energy among the atoms
EBUCK Subroutine
“ebuck” calculates the Buckingham exp-6 van der Waals energy
EBUCK0A Subroutine
“ebuck0a” calculates the Buckingham exp-6 van der Waals energy using a pairwise double loop
EBUCK0B Subroutine
“ebuck0b” calculates the Buckingham exp-6 van der Waals energy using the method of lights
EBUCK0C Subroutine
“ebuck0c” calculates the Buckingham exp-6 van der Waals energy using a pairwise neighbor list
EBUCK0D Subroutine
“ebuck0d” calculates the Buckingham exp-6 van der Waals energy via a Gaussian approximation for potential energy smoothing
EBUCK1 Subroutine
“ebuck1” calculates the Buckingham exp-6 van der Waals energy and its first derivatives with respect to Cartesian coordinates
EBUCK1A Subroutine
“ebuck1a” calculates the Buckingham exp-6 van der Waals energy and its first derivatives using a pairwise double loop
EBUCK1B Subroutine
“ebuck1b” calculates the Buckingham exp-6 van der Waals energy and its first derivatives using the method of lights
EBUCK1C Subroutine
“ebuck1c” calculates the Buckingham exp-6 van der Waals energy and its first derivatives using a pairwise neighbor list
EBUCK1D Subroutine
“ebuck1d” calculates the Buckingham exp-6 van der Waals energy and its first derivatives via a Gaussian approximation for potential energy smoothing
EBUCK2 Subroutine
“ebuck2” calculates the Buckingham exp-6 van der Waals second derivatives for a single atom at a time
EBUCK2A Subroutine
“ebuck2a” calculates the Buckingham exp-6 van der Waals second derivatives using a double loop over relevant atom pairs
EBUCK2B Subroutine
“ebuck2b” calculates the Buckingham exp-6 van der Waals second derivatives via a Gaussian approximation for use with potential energy smoothing
EBUCK3 Subroutine
“ebuck3” calculates the Buckingham exp-6 van der Waals energy and partitions the energy among the atoms
EBUCK3A Subroutine
“ebuck3a” calculates the Buckingham exp-6 van der Waals energy and partitions the energy among the atoms using a pairwise double loop
EBUCK3B Subroutine
“ebuck3b” calculates the Buckingham exp-6 van der Waals energy and also partitions the energy among the atoms using the method of lights
EBUCK3C Subroutine
“ebuck3c” calculates the Buckingham exp-6 van der Waals energy and also partitions the energy among the atoms using a pairwise neighbor list
EBUCK3D Subroutine
“ebuck3d” calculates the Buckingham exp-6 van der Waals energy via a Gaussian approximation for potential energy smoothing
ECHARGE Subroutine
“echarge” calculates the charge-charge interaction energy
ECHARGE0A Subroutine
“echarge0a” calculates the charge-charge interaction energy using a pairwise double loop
ECHARGE0B Subroutine
“echarge0b” calculates the charge-charge interaction energy using the method of lights
ECHARGE0C Subroutine
“echarge0c” calculates the charge-charge interaction energy using a pairwise neighbor list
ECHARGE0D Subroutine
“echarge0d” calculates the charge-charge interaction energy using a particle mesh Ewald summation
ECHARGE0E Subroutine
“echarge0e” calculates the charge-charge interaction energy using a particle mesh Ewald summation and the method of lights
ECHARGE0F Subroutine
“echarge0f” calculates the charge-charge interaction energy using a particle mesh Ewald summation and a neighbor list
ECHARGE0G Subroutine
“echarge0g” calculates the charge-charge interaction energy for use with potential smoothing methods
ECHARGE1 Subroutine
“echarge1” calculates the charge-charge interaction energy and first derivatives with respect to Cartesian coordinates
ECHARGE1A Subroutine
“echarge1a” calculates the charge-charge interaction energy and first derivatives with respect to Cartesian coordinates using a pairwise double loop
ECHARGE1B Subroutine
“echarge1b” calculates the charge-charge interaction energy and first derivatives with respect to Cartesian coordinates using the method of lights
ECHARGE1C Subroutine
“echarge1c” calculates the charge-charge interaction energy and first derivatives with respect to Cartesian coordinates using a pairwise neighbor list
ECHARGE1D Subroutine
“echarge1d” calculates the charge-charge interaction energy and first derivatives with respect to Cartesian coordinates using a particle mesh Ewald summation
ECHARGE1E Subroutine
“echarge1e” calculates the charge-charge interaction energy and first derivatives with respect to Cartesian coordinates using a particle mesh Ewald summation and the method of lights
ECHARGE1F Subroutine
“echarge1f” calculates the charge-charge interaction energy and first derivatives with respect to Cartesian coordinates using a particle mesh Ewald summation and a neighbor list
ECHARGE1G Subroutine
“echarge1g” calculates the charge-charge interaction energy and first derivatives with respect to Cartesian coordinates for use with potential smoothing methods
ECHARGE2 Subroutine
“echarge2” calculates second derivatives of the charge-charge interaction energy for a single atom
ECHARGE2A Subroutine
“echarge2a” calculates second derivatives of the charge-charge interaction energy for a single atom using a pairwise loop
ECHARGE2B Subroutine
“echarge2b” calculates second derivatives of the charge-charge interaction energy for a single atom using a neighbor list
ECHARGE2C Subroutine
“echarge2c” calculates second derivatives of the reciprocal space charge-charge interaction energy for a single atom using a particle mesh Ewald summation via numerical differentiation
ECHARGE2D Subroutine
“echarge2d” calculates second derivatives of the real space charge-charge interaction energy for a single atom using a pairwise loop
ECHARGE2E Subroutine
“echarge2e” calculates second derivatives of the real space charge-charge interaction energy for a single atom using a pairwise neighbor list
ECHARGE2F Subroutine
“echarge2f” calculates second derivatives of the charge-charge interaction energy for a single atom for use with potential smoothing methods
ECHARGE2R Subroutine
“echarge2r” computes reciprocal space charge-charge first derivatives; used to get finite difference second derivatives
ECHARGE3 Subroutine
“echarge3” calculates the charge-charge interaction energy and partitions the energy among the atoms
ECHARGE3A Subroutine
“echarge3a” calculates the charge-charge interaction energy and partitions the energy among the atoms using a pairwise double loop
ECHARGE3B Subroutine
“echarge3b” calculates the charge-charge interaction energy and partitions the energy among the atoms using the method of lights
ECHARGE3C Subroutine
“echarge3c” calculates the charge-charge interaction energy and partitions the energy among the atoms using a pairwise neighbor list
ECHARGE3D Subroutine
“echarge3d” calculates the charge-charge interaction energy and partitions the energy among the atoms using a particle mesh Ewald summation
ECHARGE3E Subroutine
“echarge3e” calculates the charge-charge interaction energy and partitions the energy among the atoms using a particle mesh Ewald summation and the method of lights
ECHARGE3F Subroutine
“echarge3f” calculates the charge-charge interaction energy and partitions the energy among the atoms using a particle mesh Ewald summation and a pairwise neighbor list
ECHARGE3G Subroutine
“echarge3g” calculates the charge-charge interaction energy and partitions the energy among the atoms for use with potential smoothing methods
ECHGDPL Subroutine
“echgdpl” calculates the charge-dipole interaction energy
ECHGDPL1 Subroutine
“echgdpl1” calculates the charge-dipole interaction energy and first derivatives with respect to Cartesian coordinates
ECHGDPL2 Subroutine
“echgdpl2” calculates second derivatives of the charge-dipole interaction energy for a single atom
ECHGDPL3 Subroutine
“echgdpl3” calculates the charge-dipole interaction energy; also partitions the energy among the atoms
ECHGTRN Subroutine
“echgtrn” calculates the charge transfer potential energy
ECHGTRN0A Subroutine
“echgtrn0a” calculates the charge transfer interaction energy using a double loop
ECHGTRN0B Subroutine
“echgtrn0b” calculates the charge transfer interaction energy using the method of lights
ECHGTRN0C Subroutine
“echgtrn0c” calculates the charge transfer interaction energy using a neighbor list
ECHGTRN1 Subroutine
“echgtrn1” calculates the charge transfer energy and first derivatives with respect to Cartesian coordinates
ECHGTRN1A Subroutine
“echgtrn1a” calculates the charge transfer interaction energy and first derivatives using a double loop
ECHGTRN1B Subroutine
“echgtrn1b” calculates the charge transfer energy and first derivatives using a pairwise neighbor list
ECHGTRN2 Subroutine
“echgtrn2” calculates the second derivatives of the charge transfer energy using a double loop over relevant atom pairs
ECHGTRN3 Subroutine
“echgtrn3” calculates the charge transfer energy; also partitions the energy among the atoms
ECHGTRN3A Subroutine
“echgtrn3a” calculates the charge transfer interaction energy and also partitions the energy among the atoms using a pairwise double loop
ECHGTRN3B Subroutine
“echgtrn3b” calculates the charge transfer interaction energy and also partitions the energy among the atoms using the method of lights
ECHGTRN3C Subroutine
“echgtrn3c” calculates the charge transfer interaction energy and also partitions the energy among the atoms using a pairwise neighbor list
ECRECIP Subroutine
“ecrecip” evaluates the reciprocal space portion of the particle mesh Ewald energy due to partial charges
ECRECIP1 Subroutine
“ecrecip1” evaluates the reciprocal space portion of the particle mesh Ewald summation energy and gradient due to partial charges
EDIFF Subroutine
“ediff” calculates the energy of polarizing the vacuum induced dipoles to their SCRF polarized values
EDIFF1A Subroutine
“ediff1a” calculates the energy and derivatives of polarizing the vacuum induced dipoles to their SCRF polarized values using a double loop
EDIFF1B Subroutine
“ediff1b” calculates the energy and derivatives of polarizing the vacuum induced dipoles to their SCRF polarized values using a neighbor list
EDIFF3 Subroutine
“ediff3” calculates the energy of polarizing the vacuum induced dipoles to their generalized Kirkwood values with energy analysis
EDIPOLE Subroutine
“edipole” calculates the dipole-dipole interaction energy
EDIPOLE1 Subroutine
“edipole1” calculates the dipole-dipole interaction energy and first derivatives with respect to Cartesian coordinates
EDIPOLE2 Subroutine
“edipole2” calculates second derivatives of the dipole-dipole interaction energy for a single atom
EDIPOLE3 Subroutine
“edipole3” calculates the dipole-dipole interaction energy; also partitions the energy among the atoms
EDISP Subroutine
“edisp” calculates the damped dispersion potential energy
EDISP0A Subroutine
“edisp0a” calculates the damped dispersion potential energy using a pairwise double loop
EDISP0B Subroutine
“edisp0b” calculates the damped dispersion potential energy using a pairwise neighbor list
EDISP0C Subroutine
“edisp0c” calculates the dispersion interaction energy using particle mesh Ewald summation and a double loop
EDISP0D Subroutine
“edisp0d” calculates the dispersion interaction energy using particle mesh Ewald summation and a neighbor list
EDISP1 Subroutine
“edisp1” calculates the damped dispersion energy and first derivatives with respect to Cartesian coordinates
EDISP1A Subroutine
“edisp1a” calculates the damped dispersion energy and derivatives with respect to Cartesian coordinates using a pairwise double loop
EDISP1B Subroutine
“edisp1b” calculates the damped dispersion energy and derivatives with respect to Cartesian coordinates using a pairwise neighbor list
EDISP1C Subroutine
“edisp1c” calculates the damped dispersion energy and derivatives with respect to Cartesian coordinates using particle mesh Ewald summation and a double loop
EDISP1D Subroutine
“edisp1d” calculates the damped dispersion energy and derivatives with respect to Cartesian coordinates using particle mesh Ewald summation and a neighbor list
EDISP2 Subroutine
“edisp2” calculates the damped dispersion second derivatives for a single atom at a time
EDISP3 Subroutine
“edisp3” calculates the dispersion energy; also partitions the energy among the atoms
EDISP3A Subroutine
“edisp3a” calculates the dispersion potential energy and also partitions the energy among the atoms using a pairwise double loop
EDISP3B Subroutine
“edisp3b” calculates the damped dispersion potential energy and also partitions the energy among the atomsusing a pairwise neighbor list
EDISP3C Subroutine
“edisp3c” calculates the dispersion interaction energy using particle mesh Ewald summation and a double loop
EDISP3D Subroutine
“edisp3d” calculates the damped dispersion energy and analysis using particle mesh Ewald summation and a neighbor list
EDREAL0C Subroutine
“edreal0c” calculates the damped dispersion potential energy using a particle mesh Ewald sum and pairwise double loop
EDREAL0D Subroutine
“edreal0d” evaluated the real space portion of the damped dispersion energy using a neighbor list
EDREAL1C Subroutine
“edreal1c” evaluates the real space portion of the Ewald summation energy and gradient due to damped dispersion interactions via a double loop
EDREAL1D Subroutine
“edreal1d” evaluates the real space portion of the Ewald summation energy and gradient due to damped dispersion interactions via a neighbor list
EDREAL3C Subroutine
“edreal3c” calculates the real space portion of the damped dispersion energy and analysis using Ewald and a double loop
EDREAL3D Subroutine
“edreal3d” evaluated the real space portion of the damped dispersion energy and analysis using Ewald and a neighbor list
EDRECIP Subroutine
“edrecip” evaluates the reciprocal space portion of the particle mesh Ewald energy due to damped dispersion
EDRECIP1 Subroutine
“edrecip1” evaluates the reciprocal space portion of particle mesh Ewald energy and gradient due to damped dispersion
EGAUSS Subroutine
“egauss” calculates the Gaussian expansion van der Waals energy
EGAUSS0A Subroutine
“egauss0a” calculates the Gaussian expansion van der Waals energy using a pairwise double loop
EGAUSS0B Subroutine
“egauss0b” calculates the Gaussian expansion van der Waals energy using the method of lights
EGAUSS0C Subroutine
“egauss0c” calculates the Gaussian expansion van der Waals energy using a pairwise neighbor list
EGAUSS0D Subroutine
“egauss0d” calculates the Gaussian expansion van der Waals energy for use with potential energy smoothing
EGAUSS1 Subroutine
“egauss1” calculates the Gaussian expansion van der Waals interaction energy and its first derivatives with respect to Cartesian coordinates
EGAUSS1A Subroutine
“egauss1a” calculates the Gaussian expansion van der Waals interaction energy and its first derivatives using a pairwise double loop
EGAUSS1B Subroutine
“egauss1b” calculates the Gaussian expansion van der Waals energy and its first derivatives with respect to Cartesian coordinates using the method of lights
EGAUSS1C Subroutine
“egauss1c” calculates the Gaussian expansion van der Waals energy and its first derivatives with respect to Cartesian coordinates using a pairwise neighbor list
EGAUSS1D Subroutine
“egauss1d” calculates the Gaussian expansion van der Waals interaction energy and its first derivatives for use with potential energy smoothing
EGAUSS2 Subroutine
“egauss2” calculates the Gaussian expansion van der Waals second derivatives for a single atom at a time
EGAUSS2A Subroutine
“egauss2a” calculates the Gaussian expansion van der Waals second derivatives using a pairwise double loop
EGAUSS2B Subroutine
“egauss2b” calculates the Gaussian expansion van der Waals second derivatives for use with potential energy smoothing
EGAUSS3 Subroutine
“egauss3” calculates the Gaussian expansion van der Waals interaction energy and partitions the energy among the atoms
EGAUSS3A Subroutine
“egauss3a” calculates the Gaussian expansion van der Waals energy and partitions the energy among the atoms using a pairwise double loop
EGAUSS3B Subroutine
“egauss3b” calculates the Gaussian expansion van der Waals energy and partitions the energy among the atoms using the method of lights
EGAUSS3C Subroutine
“egauss3c” calculates the Gaussian expansion van der Waals energy and partitions the energy among the atoms using a pairwise neighbor list
EGAUSS3D Subroutine
“egauss3d” calculates the Gaussian expansion van der Waals interaction energy and partitions the energy among the atoms for use with potential energy smoothing
EGB0A Subroutine
“egb0a” calculates the generalized Born polarization energy for the GB/SA solvation models using a pairwise double loop
EGB0B Subroutine
“egb0b” calculates the generalized Born polarization energy for the GB/SA solvation models using a pairwise neighbor list
EGB0C Subroutine
“egb0c” calculates the generalized Born polarization energy for the GB/SA solvation models for use with potential smoothing methods via analogy to the smoothing of Coulomb’s law
EGB1A Subroutine
“egb1a” calculates the generalized Born electrostatic energy and first derivatives of the GB/SA solvation models using a double loop
EGB1B Subroutine
“egb1b” calculates the generalized Born electrostatic energy and first derivatives of the GB/SA solvation models using a neighbor list
EGB1C Subroutine
“egb1c” calculates the generalized Born energy and first derivatives of the GB/SA solvation models for use with potential smoothing methods
EGB2A Subroutine
“egb2a” calculates second derivatives of the generalized Born energy term for the GB/SA solvation models
EGB2B Subroutine
“egb2b” calculates second derivatives of the generalized Born energy term for the GB/SA solvation models for use with potential smoothing methods
EGB3A Subroutine
“egb3a” calculates the generalized Born electrostatic energy for GB/SA solvation models using a pairwise double loop; also partitions the energy among the atoms
EGB3B Subroutine
“egb3b” calculates the generalized Born electrostatic energy for GB/SA solvation models using a pairwise neighbor list; also partitions the energy among the atoms
EGB3C Subroutine
“egb3c” calculates the generalized Born electrostatic energy for GB/SA solvation models for use with potential smoothing methods via analogy to the smoothing of Coulomb’s law; also partitions the energy among the atoms
EGEOM Subroutine
“egeom” calculates the energy due to restraints on positions, distances, angles and torsions as well as Gaussian basin and spherical droplet restraints
EGEOM1 Subroutine
“egeom1” calculates the energy and first derivatives with respect to Cartesian coordinates due to restraints on positions, distances, angles and torsions as well as Gaussian basin and spherical droplet restraints
EGEOM2 Subroutine
“egeom2” calculates second derivatives of restraints on positions, distances, angles and torsions as well as Gaussian basin and spherical droplet restraints
EGEOM3 Subroutine
“egeom3” calculates the energy due to restraints on positions, distances, angles and torsions as well as Gaussian basin and droplet restraints; also partitions energy among the atoms
EGK Subroutine
“egk” calculates the generalized Kirkwood electrostatic solvation free energy for the GK/NP implicit solvation model
EGK0A Subroutine
“egk0a” calculates the electrostatic portion of the implicit solvation energy via the generalized Kirkwood model
EGK1 Subroutine
“egk1” calculates the implicit solvation energy and derivatives via the generalized Kirkwood plus nonpolar implicit solvation
EGK1A Subroutine
“egk1a” calculates the electrostatic portion of the implicit solvation energy and derivatives via the generalized Kirkwood model
EGK3 Subroutine
“egk3” calculates the generalized Kirkwood electrostatic energy for GK/NP solvation models; also partitions the energy among the atoms
EGK3A Subroutine
“egk3a” calculates the electrostatic portion of the implicit solvation energy via the generalized Kirkwood model; also partitions the energy among the atoms
EHAL Subroutine
“ehal” calculates the buffered 14-7 van der Waals energy
EHAL0A Subroutine
“ehal0a” calculates the buffered 14-7 van der Waals energy using a pairwise double loop
EHAL0B Subroutine
“ehal0b” calculates the buffered 14-7 van der Waals energy using the method of lights
EHAL0C Subroutine
“ehal0c” calculates the buffered 14-7 van der Waals energy using a pairwise neighbor list
EHAL1 Subroutine
“ehal1” calculates the buffered 14-7 van der Waals energy and its first derivatives with respect to Cartesian coordinates
EHAL1A Subroutine
“ehal1a” calculates the buffered 14-7 van der Waals energy and its first derivatives with respect to Cartesian coordinates using a pairwise double loop
EHAL1B Subroutine
“ehal1b” calculates the buffered 14-7 van der Waals energy and its first derivatives with respect to Cartesian coordinates using the method of lights
EHAL1C Subroutine
“ehal1c” calculates the buffered 14-7 van der Waals energy and its first derivatives with respect to Cartesian coordinates using a pairwise neighbor list
EHAL2 Subroutine
“ehal2” calculates the buffered 14-7 van der Waals second derivatives for a single atom at a time
EHAL3 Subroutine
“ehal3” calculates the buffered 14-7 van der Waals energy and partitions the energy among the atoms
EHAL3A Subroutine
“ehal3a” calculates the buffered 14-7 van der Waals energy and partitions the energy among the atoms using a pairwise double loop
EHAL3B Subroutine
“ehal3b” calculates the buffered 14-7 van der Waals energy and also partitions the energy among the atoms using the method of lights
EHAL3C Subroutine
“ehal3c” calculates the buffered 14-7 van der Waals energy and also partitions the energy among the atoms using a pairwise neighbor list
EHPMF Subroutine
“ehpmf” calculates the hydrophobic potential of mean force energy using a pairwise double loop
EHPMF1 Subroutine
“ehpmf1” calculates the hydrophobic potential of mean force energy and first derivatives using a pairwise double loop
EHPMF3 Subroutine
“ehpmf3” calculates the hydrophobic potential of mean force nonpolar energy; also partitions the energy among the atoms
EIGEN Subroutine
“eigen” uses the power method to compute the largest eigenvalues and eigenvectors of the metric matrix, “valid” is set true if the first three eigenvalues are positive
EIGENRGD Subroutine
EIGENROT Subroutine
EIGENROT Subroutine
EIGENTOR Subroutine
EIGENXYZ Subroutine
EIMPROP Subroutine
“eimprop” calculates the improper dihedral potential energy
EIMPROP1 Subroutine
“eimprop1” calculates improper dihedral energy and its first derivatives with respect to Cartesian coordinates
EIMPROP2 Subroutine
“eimprop2” calculates second derivatives of the improper dihedral angle energy for a single atom
EIMPROP3 Subroutine
“eimprop3” calculates the improper dihedral potential energy; also partitions the energy terms among the atoms
EIMPTOR Subroutine
“eimptor” calculates the improper torsion potential energy
EIMPTOR1 Subroutine
“eimptor1” calculates improper torsion energy and its first derivatives with respect to Cartesian coordinates
EIMPTOR2 Subroutine
“eimptor2” calculates second derivatives of the improper torsion energy for a single atom
EIMPTOR3 Subroutine
“eimptor3” calculates the improper torsion potential energy; also partitions the energy terms among the atoms
ELJ Subroutine
“elj” calculates the Lennard-Jones 6-12 van der Waals energy
ELJ0A Subroutine
“elj0a” calculates the Lennard-Jones 6-12 van der Waals energy using a pairwise double loop
ELJ0B Subroutine
“elj0b” calculates the Lennard-Jones 6-12 van der Waals energy using the method of lights
ELJ0C Subroutine
“elj0c” calculates the Lennard-Jones 6-12 van der Waals energy using a pairwise neighbor list
ELJ0D Subroutine
“elj0d” calculates the Lennard-Jones 6-12 van der Waals energy via a Gaussian approximation for potential energy smoothing
ELJ0E Subroutine
“elj0e” calculates the Lennard-Jones 6-12 van der Waals energy for use with stophat potential energy smoothing
ELJ1 Subroutine
“elj1” calculates the Lennard-Jones 6-12 van der Waals energy and its first derivatives with respect to Cartesian coordinates
ELJ1A Subroutine
“elj1a” calculates the Lennard-Jones 6-12 van der Waals energy and its first derivatives using a pairwise double loop
ELJ1B Subroutine
“elj1b” calculates the Lennard-Jones 6-12 van der Waals energy and its first derivatives using the method of lights
ELJ1C Subroutine
“elj1c” calculates the Lennard-Jones 12-6 van der Waals energy and its first derivatives using a pairwise neighbor list
ELJ1D Subroutine
- “elj1d” calculates the Lennard-Jones 6-12 van der Waals energy
and its first derivatives via a Gaussian approximation for potential energy smoothing
ELJ1E Subroutine
“elj1e” calculates the van der Waals interaction energy and its first derivatives for use with stophat potential energy smoothing
ELJ2 Subroutine
“elj2” calculates the Lennard-Jones 6-12 van der Waals second derivatives for a single atom at a time
ELJ2A Subroutine
“elj2a” calculates the Lennard-Jones 6-12 van der Waals second derivatives using a double loop over relevant atom pairs
ELJ2B Subroutine
“elj2b” calculates the Lennard-Jones 6-12 van der Waals second derivatives via a Gaussian approximation for use with potential energy smoothing
ELJ2C Subroutine
“elj2c” calculates the Lennard-Jones 6-12 van der Waals second derivatives for use with stophat potential energy smoothing
ELJ3 Subroutine
“elj3” calculates the Lennard-Jones 6-12 van der Waals energy and also partitions the energy among the atoms
ELJ3A Subroutine
“elj3a” calculates the Lennard-Jones 6-12 van der Waals energy and also partitions the energy among the atoms using a pairwise double loop
ELJ3B Subroutine
“elj3b” calculates the Lennard-Jones 6-12 van der Waals energy and also partitions the energy among the atoms using the method of lights
ELJ3C Subroutine
“elj3c” calculates the Lennard-Jones van der Waals energy and also partitions the energy among the atoms using a pairwise neighbor list
ELJ3D Subroutine
“elj3d” calculates the Lennard-Jones 6-12 van der Waals energy and also partitions the energy among the atoms via a Gaussian approximation for potential energy smoothing
ELJ3E Subroutine
“elj3e” calculates the Lennard-Jones 6-12 van der Waals energy and also partitions the energy among the atoms for use with stophat potential energy smoothing
EMBED Subroutine
“embed” is a distance geometry routine patterned after the ideas of Gordon Crippen, Irwin Kuntz and Tim Havel; it takes as input a set of upper and lower bounds on the interpoint distances, chirality restraints and torsional restraints, and attempts to generate a set of coordinates that satisfy the input bounds and restraints
EMETAL Subroutine
“emetal” calculates the transition metal ligand field energy
EMETAL1 Subroutine
“emetal1” calculates the transition metal ligand field energy and its first derivatives with respect to Cartesian coordinates
EMETAL2 Subroutine
“emetal2” calculates the transition metal ligand field second derivatives for a single atom at a time
EMETAL3 Subroutine
“emetal3” calculates the transition metal ligand field energy and also partitions the energy among the atoms
EMM3HB Subroutine
“emm3hb” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding energy
EMM3HB0A Subroutine
“emm3hb0a” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding energy using a pairwise double loop
EMM3HB0B Subroutine
“emm3hb0b” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding energy using the method of lights
EMM3HB0C Subroutine
“emm3hb0c” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding energy using a pairwise neighbor list
EMM3HB1 Subroutine
“emm3hb1” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding energy with respect to Cartesian coordinates
EMM3HB1A Subroutine
“emm3hb1a” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding energy with respect to Cartesian coordinates using a pairwise double loop
EMM3HB1B Subroutine
“emm3hb1b” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding energy with respect to Cartesian coordinates using the method of lights
EMM3HB1C Subroutine
“emm3hb1c” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding energy with respect to Cartesian coordinates using a pairwise neighbor list
EMM3HB2 Subroutine
“emm3hb2” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding second derivatives for a single atom at a time
EMM3HB3 Subroutine
“emm3hb3” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding energy, and partitions the energy among the atoms
EMM3HB3A Subroutine
“emm3hb3” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding energy, and partitions the energy among the atoms
EMM3HB3B Subroutine
“emm3hb3b” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding energy using the method of lights
EMM3HB3C Subroutine
“emm3hb3c” calculates the MM3 exp-6 van der Waals and directional charge transfer hydrogen bonding energy using a pairwise neighbor list
EMPOLE Subroutine
“empole” calculates the electrostatic energy due to atomic multipole interactions
EMPOLE0A Subroutine
“empole0a” calculates the atomic multipole interaction energy using a double loop
EMPOLE0B Subroutine
“empole0b” calculates the atomic multipole interaction energy using a neighbor list
EMPOLE0C Subroutine
“empole0c” calculates the atomic multipole interaction energy using particle mesh Ewald summation and a double loop
EMPOLE0D Subroutine
“empole0d” calculates the atomic multipole interaction energy using particle mesh Ewald summation and a neighbor list
EMPOLE1 Subroutine
“empole1” calculates the atomic multipole energy and first derivatives with respect to Cartesian coordinates
EMPOLE1A Subroutine
“empole1a” calculates the multipole energy and derivatives with respect to Cartesian coordinates using a pairwise double loop
EMPOLE1B Subroutine
“empole1b” calculates the multipole energy and derivatives with respect to Cartesian coordinates using a neighbor list
EMPOLE1C Subroutine
“empole1c” calculates the multipole energy and derivatives with respect to Cartesian coordinates using particle mesh Ewald summation and a double loop
EMPOLE1D Subroutine
“empole1d” calculates the multipole energy and derivatives with respect to Cartesian coordinates using particle mesh Ewald summation and a neighbor list
EMPOLE2 Subroutine
“empole2” calculates second derivatives of the multipole energy for a single atom at a time
EMPOLE2A Subroutine
“empole2a” computes multipole first derivatives for a single atom; used to get finite difference second derivatives
EMPOLE3 Subroutine
“empole3” calculates the electrostatic energy due to atomic multipole interactions, and partitions the energy among atoms
EMPOLE3A Subroutine
“empole3a” calculates the atomic multipole interaction energy using a double loop, and partitions the energy among atoms
EMPOLE3B Subroutine
“empole3b” calculates the atomic multipole interaction energy using a neighbor list, and partitions the energy among the atoms
EMPOLE3C Subroutine
“empole3c” calculates the atomic multipole interaction energy using a particle mesh Ewald summation and double loop, and partitions the energy among the atoms
EMPOLE3D Subroutine
“empole3d” calculates the atomic multipole interaction energy using particle mesh Ewald summation and a neighbor list, and partitions the energy among the atoms
EMREAL0C Subroutine
“emreal0c” evaluates the real space portion of the Ewald sum energy due to atomic multipoles using a double loop
EMREAL0D Subroutine
“emreal0d” evaluates the real space portion of the Ewald sum energy due to atomic multipoles using a neighbor list
EMREAL1C Subroutine
“emreal1c” evaluates the real space portion of the Ewald summation energy and gradient due to multipole interactions via a double loop
EMREAL1D Subroutine
“emreal1d” evaluates the real space portion of the Ewald summation energy and gradient due to multipole interactions via a neighbor list
EMREAL3C Subroutine
“emreal3c” evaluates the real space portion of the Ewald sum energy due to atomic multipole interactions and partitions the energy among the atoms
EMREAL3D Subroutine
“emreal3d” evaluates the real space portion of the Ewald sum energy due to atomic multipole interactions, and partitions the energy among the atoms using a pairwise neighbor list
EMRECIP Subroutine
“emrecip” evaluates the reciprocal space portion of the particle mesh Ewald energy due to atomic multipole interactions
EMRECIP1 Subroutine
“emrecip1” evaluates the reciprocal space portion of particle mesh Ewald summation energy and gradient due to multipoles
ENERGY Function
“energy” calls the subroutines to calculate the potential energy terms and sums up to form the total energy
ENP Subroutine
“enp” calculates the nonpolar implicit solvation energy as a sum of cavity and dispersion terms
ENP1 Subroutine
“enp1” calculates the nonpolar implicit solvation energy and derivatives as a sum of cavity and dispersion terms
ENP3 Subroutine
“enp3” calculates the nonpolar implicit solvation energy as a sum of cavity and dispersion terms; also partitions the energy among the atoms
ENRGYZE Subroutine
“enrgyze” is an auxiliary routine for the analyze program that performs the energy analysis and prints the total and intermolecular energies
EOPBEND Subroutine
“eopbend” computes the out-of-plane bend potential energy at trigonal centers via a Wilson-Decius-Cross or Allinger angle
EOPBEND1 Subroutine
“eopbend1” computes the out-of-plane bend potential energy and first derivatives at trigonal centers via a Wilson-Decius-Cross or Allinger angle
EOPBEND2 Subroutine
“eopbend2” calculates second derivatives of the out-of-plane bend energy via a Wilson-Decius-Cross or Allinger angle for a single atom using finite difference methods
EOPBEND2A Subroutine
“eopbend2a” calculates out-of-plane bend first derivatives at a trigonal center via a Wilson-Decius-Cross or Allinger angle; used in computation of finite difference second derivatives
EOPBEND3 Subroutine
“eopbend3” computes the out-of-plane bend potential energy at trigonal centers via a Wilson-Decius-Cross or Allinger angle; also partitions the energy among the atoms
EOPDIST Subroutine
“eopdist” computes the out-of-plane distance potential energy at trigonal centers via the central atom height
EOPDIST1 Subroutine
“eopdist1” computes the out-of-plane distance potential energy and first derivatives at trigonal centers via the central atom height
EOPDIST2 Subroutine
“eopdist2” calculates second derivatives of the out-of-plane distance energy for a single atom via the central atom height
EOPDIST3 Subroutine
“eopdist3” computes the out-of-plane distance potential energy at trigonal centers via the central atom height; also partitions the energy among the atoms
EPB Subroutine
“epb” calculates the implicit solvation energy via the Poisson-Boltzmann plus nonpolar implicit solvation
EPB1 Subroutine
“epb1” calculates the implicit solvation energy and derivatives via the Poisson-Boltzmann plus nonpolar implicit solvation
EPB1A Subroutine
“epb1a” calculates the solvation energy and gradients for the PB/NP solvation model
EPB3 Subroutine
“epb3” calculates the implicit solvation energy via the Poisson-Boltzmann model; also partitions the energy among the atoms
EPITORS Subroutine
“epitors” calculates the pi-system torsion potential energy
EPITORS1 Subroutine
“epitors1” calculates the pi-system torsion potential energy and first derivatives with respect to Cartesian coordinates
EPITORS2 Subroutine
“epitors2” calculates the second derivatives of the pi-system torsion energy for a single atom using finite difference methods
EPITORS2A Subroutine
“epitors2a” calculates the pi-system torsion first derivatives; used in computation of finite difference second derivatives
EPITORS3 Subroutine
“epitors3” calculates the pi-system torsion potential energy; also partitions the energy terms among the atoms
EPOLAR Subroutine
“epolar” calculates the polarization energy due to induced dipole interactions
EPOLAR0A Subroutine
“epolar0a” calculates the induced dipole polarization energy using a double loop, and partitions the energy among atoms
EPOLAR0B Subroutine
“epolar0b” calculates the induced dipole polarization energy using a neighbor list
EPOLAR0C Subroutine
“epolar0c” calculates the dipole polarization energy with respect to Cartesian coordinates using particle mesh Ewald summation and a double loop
EPOLAR0D Subroutine
“epolar0d” calculates the dipole polarization energy with respect to Cartesian coordinates using particle mesh Ewald summation and a neighbor list
EPOLAR0E Subroutine
“epolar0e” calculates the dipole polarizability interaction from the induced dipoles times the electric field
EPOLAR1 Subroutine
“epolar1” calculates the induced dipole polarization energy and first derivatives with respect to Cartesian coordinates
EPOLAR1A Subroutine
“epolar1a” calculates the dipole polarization energy and derivatives with respect to Cartesian coordinates using a pairwise double loop
EPOLAR1B Subroutine
“epolar1b” calculates the dipole polarization energy and derivatives with respect to Cartesian coordinates using a neighbor list
EPOLAR1C Subroutine
“epolar1c” calculates the dipole polarization energy and derivatives with respect to Cartesian coordinates using particle mesh Ewald summation and a double loop
EPOLAR1D Subroutine
“epolar1d” calculates the dipole polarization energy and derivatives with respect to Cartesian coordinates using particle mesh Ewald summation and a neighbor list
EPOLAR1E Subroutine
“epolar1e” calculates the dipole polarizability interaction from the induced dipoles times the electric field
EPOLAR2 Subroutine
“epolar2” calculates second derivatives of the dipole polarization energy for a single atom at a time
EPOLAR2A Subroutine
“epolar2a” computes polarization first derivatives for a single atom with respect to Cartesian coordinates; used to get finite difference second derivatives
EPOLAR3 Subroutine
“epolar3” calculates the induced dipole polarization energy, and partitions the energy among atoms
EPOLAR3A Subroutine
“epolar3a” calculates the induced dipole polarization energy using a double loop, and partitions the energy among atoms
EPOLAR3B Subroutine
“epolar3b” calculates the induced dipole polarization energy using a neighbor list, and partitions the energy among atoms
EPOLAR3C Subroutine
“epolar3c” calculates the polarization energy and analysis with respect to Cartesian coordinates using particle mesh Ewald and a double loop
EPOLAR3D Subroutine
“epolar3d” calculates the polarization energy and analysis with respect to Cartesian coordinates using particle mesh Ewald and a neighbor list
EPOLAR3E Subroutine
“epolar3e” calculates the dipole polarizability interaction from the induced dipoles times the electric field
EPREAL0C Subroutine
“epreal0c” calculates the induced dipole polarization energy using particle mesh Ewald summation and a double loop
EPREAL0D Subroutine
“epreal0d” calculates the induced dipole polarization energy using particle mesh Ewald summation and a neighbor list
EPREAL1C Subroutine
“epreal1c” evaluates the real space portion of the Ewald summation energy and gradient due to dipole polarization via a double loop
EPREAL1D Subroutine
“epreal1d” evaluates the real space portion of the Ewald summation energy and gradient due to dipole polarization via a neighbor list
EPREAL3C Subroutine
“epreal3c” calculates the induced dipole polarization energy and analysis using particle mesh Ewald summation and a double loop
EPREAL3D Subroutine
“epreal3d” calculates the induced dipole polarization energy and analysis using particle mesh Ewald and a neighbor list
EPRECIP Subroutine
“eprecip” evaluates the reciprocal space portion of particle mesh Ewald summation energy due to dipole polarization
EPRECIP1 Subroutine
“eprecip1” evaluates the reciprocal space portion of the particle mesh Ewald summation energy and gradient due to dipole polarization
EQUCLC Subroutine
EREPEL Subroutine
“erepel” calculates the Pauli exchange repulsion energy
EREPEL0A Subroutine
“erepel0a” calculates the Pauli repulsion interaction energy using a double loop
EREPEL0B Subroutine
“erepel0b” calculates the Pauli repulsion interaction energy using a pairwise neighbor list
EREPEL1 Subroutine
“erepel1” calculates the Pauli repulsion energy and first derivatives with respect to Cartesian coordinates
EREPEL1A Subroutine
“erepel1a” calculates the Pauli repulsion energy and first derivatives with respect to Cartesian coordinates using a pairwise double loop
EREPEL1B Subroutine
“erepel1b” calculates the Pauli repulsion energy and first derivatives with respect to Cartesian coordinates using a pariwise neighbor list
EREPEL2 Subroutine
“erepel2” calculates the second derivatives of the Pauli repulsion energy
EREPEL2A Subroutine
“erepel2a” computes Pauli repulsion first derivatives for a single atom via a double loop; used to get finite difference second derivatives
EREPEL3 Subroutine
“erepel3” calculates the Pauli repulsion energy and partitions the energy among the atoms
EREPEL3A Subroutine
“erepel3a” calculates the Pauli repulsion energy and also partitions the energy among the atoms using a double loop
EREPEL3B Subroutine
“erepel3b” calculates the Pauli repulsion energy and also partitions the energy among the atoms using a neighbor list
ERF Function
“erf” computes a numerical approximation to the value of the error function via a Chebyshev approximation
ERFC Function
“erfc” computes a numerical approximation to the value of the complementary error function via a Chebyshev approximation
ERFCORE Subroutine
“erfcore” evaluates erf(x) or erfc(x) for a real argument x; when called with mode set to 0 it returns erf, a mode of 1 returns erfc; uses rational functions that approximate erf(x) and erfc(x) to at least 18 significant decimal digits
ERFIK Subroutine
“erfik” compute the reaction field energy due to a single pair of atomic multipoles
ERFINV Function
“erfinv” evaluates the inverse of the error function for an argument in the range (-1,1) using a rational function approximation followed by cycles of Newton-Raphson correction
ERXNFLD Subroutine
“erxnfld” calculates the macroscopic reaction field energy arising from a set of atomic multipoles
ERXNFLD1 Subroutine
“erxnfld1” calculates the macroscopic reaction field energy and derivatives with respect to Cartesian coordinates
ERXNFLD2 Subroutine
“erxnfld2” calculates second derivatives of the macroscopic reaction field energy for a single atom at a time
ERXNFLD3 Subroutine
“erxnfld3” calculates the macroscopic reaction field energy, and also partitions the energy among the atoms
ESOLV Subroutine
“esolv” calculates the implicit solvation energy for surface area, generalized Born, generalized Kirkwood and Poisson-Boltzmann solvation models
ESOLV1 Subroutine
“esolv1” calculates the implicit solvation energy and first derivatives with respect to Cartesian coordinates for surface area, generalized Born, generalized Kirkwood and Poisson-Boltzmann solvation models
ESOLV2 Subroutine
“esolv2” calculates second derivatives of the implicit solvation energy for surface area, generalized Born, generalized Kirkwood and Poisson-Boltzmann solvation models
ESOLV2A Subroutine
“esolv2a” calculates second derivatives of the implicit solvation potential energy by finite differences
ESOLV2B Subroutine
“esolv2b” finds implicit solvation gradients needed for calculation of the Hessian matrix by finite differences
ESOLV3 Subroutine
“esolv3” calculates the implicit solvation energy for surface area, generalized Born, generalized Kirkwood and Poisson-Boltzmann solvation models; also partitions the energy among the atoms
ESTRBND Subroutine
“estrbnd” calculates the stretch-bend potential energy
ESTRBND1 Subroutine
“estrbnd1” calculates the stretch-bend potential energy and first derivatives with respect to Cartesian coordinates
ESTRBND2 Subroutine
“estrbnd2” calculates the stretch-bend potential energy second derivatives with respect to Cartesian coordinates
ESTRBND3 Subroutine
“estrbnd3” calculates the stretch-bend potential energy; also partitions the energy among the atoms
ESTRTOR Subroutine
“estrtor” calculates the stretch-torsion potential energy
ESTRTOR1 Subroutine
“estrtor1” calculates the stretch-torsion energy and first derivatives with respect to Cartesian coordinates
ESTRTOR2 Subroutine
“estrtor2” calculates the stretch-torsion potential energy second derivatives with respect to Cartesian coordinates
ESTRTOR3 Subroutine
“estrtor3” calculates the stretch-torsion potential energy; also partitions the energy terms among the atoms
ETORS Subroutine
“etors” calculates the torsional potential energy
ETORS0A Subroutine
“etors0a” calculates the torsional potential energy using a standard sum of Fourier terms
ETORS0B Subroutine
“etors0b” calculates the torsional potential energy for use with potential energy smoothing methods
ETORS1 Subroutine
“etors1” calculates the torsional potential energy and first derivatives with respect to Cartesian coordinates
ETORS1A Subroutine
“etors1a” calculates the torsional potential energy and first derivatives with respect to Cartesian coordinates using a standard sum of Fourier terms
ETORS1B Subroutine
“etors1b” calculates the torsional potential energy and first derivatives with respect to Cartesian coordinates for use with potential energy smoothing methods
ETORS2 Subroutine
“etors2” calculates the second derivatives of the torsional energy for a single atom
ETORS2A Subroutine
“etors2a” calculates the second derivatives of the torsional energy for a single atom using a standard sum of Fourier terms
ETORS2B Subroutine
“etors2b” calculates the second derivatives of the torsional energy for a single atom for use with potential energy smoothing methods
ETORS3 Subroutine
“etors3” calculates the torsional potential energy; also partitions the energy among the atoms
ETORS3A Subroutine
“etors3a” calculates the torsional potential energy using a standard sum of Fourier terms and partitions the energy among the atoms
ETORS3B Subroutine
“etors3b” calculates the torsional potential energy for use with potential energy smoothing methods and partitions the energy among the atoms
ETORTOR Subroutine
“etortor” calculates the torsion-torsion potential energy
ETORTOR1 Subroutine
“etortor1” calculates the torsion-torsion energy and first derivatives with respect to Cartesian coordinates
ETORTOR2 Subroutine
“etortor2” calculates the torsion-torsion potential energy second derivatives with respect to Cartesian coordinates
ETORTOR3 Subroutine
“etortor3” calculates the torsion-torsion potential energy; also partitions the energy terms among the atoms
EUREY Subroutine
“eurey” calculates the Urey-Bradley 1-3 interaction energy
EUREY1 Subroutine
“eurey1” calculates the Urey-Bradley interaction energy and its first derivatives with respect to Cartesian coordinates
EUREY2 Subroutine
“eurey2” calculates second derivatives of the Urey-Bradley interaction energy for a single atom at a time
EUREY3 Subroutine
“eurey3” calculates the Urey-Bradley energy; also partitions the energy among the atoms
EVCORR Subroutine
“evcorr” computes the long range van der Waals correction to the energy via numerical integration
EVCORR1 Subroutine
“evcorr1” computes the long range van der Waals correction to the energy and virial via numerical integration
EWALDCOF Subroutine
“ewaldcof” finds an Ewald coefficient such that all terms beyond the specified cutoff distance will have a value less than a specified tolerance
EWCA Subroutine
“ewca” find the Weeks-Chandler-Andersen dispersion energy of a solute using an HCT-like method
EWCA1 Subroutine
“ewca1” finds the Weeks-Chandler-Anderson dispersion energy and derivatives of a solute
EWCA3 Subroutine
“ewca3” find the Weeks-Chandler-Andersen dispersion energy of a solute; also partitions the energy among the atoms
EWCA3X Subroutine
“ewca3x” finds the Weeks-Chandler-Anderson dispersion energy of a solute using a numerical “onion shell” method; also partitions the energy among the atoms
EWCAX Subroutine
“ewcax” finds the Weeks-Chandler-Anderson dispersion energy of a solute using a numerical “onion shell” method
EXFIELD Subroutine
“exfield” calculates the electrostatic energy due to an external electric field applied to the system
EXFIELD1 Subroutine
“exfield1” calculates the electrostatic energy, gradient and virial due to an external electric field applied to the system
EXFIELD3 Subroutine
“exfield3” calculates the electrostatic energy and partitions the energy among the atomsdue to an external electric field applied to the system
EXPLORE Subroutine
“explore” uses simulated annealing on an initial crude embedded distance geoemtry structure to refine versus the bound, chirality, planarity and torsional error functions
EXTENT Subroutine
“extent” finds the largest interatomic distance in a system
EXTRA Subroutine
“extra” calculates any additional user defined potential energy contribution
EXTRA1 Subroutine
“extra1” calculates any additional user defined potential energy contribution and its first derivatives
EXTRA2 Subroutine
“extra2” calculates second derivatives of any additional user defined potential energy contribution for a single atom at a time
EXTRA3 Subroutine
“extra3” calculates any additional user defined potential contribution and also partitions the energy among the atoms
FATAL Subroutine
“fatal” terminates execution due to a user request, a severe error or some other nonstandard condition
FFTBACK Subroutine
“fftback” performs a 3-D FFT backward transform via a single 3-D transform or three separate 1-D transforms
FFTCLOSE Subroutine
“fftclose” does cleanup after performing a 3-D FFT by destroying the FFTW plans for the forward and backward transforms
FFTFRONT Subroutine
“fftfront” performs a 3-D FFT forward transform via a single 3-D transform or three separate 1-D transforms
FFTSETUP Subroutine
“fftsetup” does initialization for a 3-D FFT to be computed via either the FFTPACK or FFTW libraries
FIELD Subroutine
“field” sets the force field potential energy functions from a parameter file and modifications specified in a keyfile
FINAL Subroutine
“final” performs any final program actions such as deallocation of global memory, prints a status message, and then pauses if necessary to avoid closing the execution window
FINDATM Subroutine
“findatm” locates a specific PDB atom name type within a range of atoms from the PDB file, returns zero if the name type was not found
FITRSD Subroutine
“fitrsd” computes residuals for electrostatic potential fitting including total charge restraints, dipole and quadrupole moment targets, and restraints to initial parameter values
FITTORS Subroutine
“fittors” refines torsion parameters based on a quantum mechanical optimized energy surface
FIXFRAME Subroutine
“fixframe” is a service routine that alters the local frame definition for specified atoms
FIXPDB Subroutine
“fixpdb” corrects problems with PDB files by converting residue and atom names to the standard forms used by Tinker
FIXPOLE Subroutine
“fixpole” performs unit conversion of the multipole components, rounds moments to desired precision, and enforces integer net charge and traceless quadrupoles
FLATTEN Subroutine
“flatten” sets the type of smoothing method and the extent of surface deformation for use with potential energy smoothing
FPHI_MPOLE Subroutine
“fphi_mpole” extracts the permanent multipole potential from the particle mesh Ewald grid
FPHI_TO_CPHI Subroutine
“fphi_to_cphi” transforms the reciprocal space potential from fractional to Cartesian coordinates
FPHI_UIND Subroutine
“fphi_uind” extracts the induced dipole potential from the particle mesh Ewald grid
FRACDIST Subroutine
“fracdist” computes a normalized distribution of the pairwise fractional distances between the smoothed upper and lower bounds
FRAC_TO_CART Subroutine
“frac_to_cart” computes a transformation matrix to convert a multipole object in fraction coordinates to Cartesian
FRAME13 Subroutine
“frame13” finds local coordinate frame defining atoms in cases where the use of 1-3 connected atoms is required
FREEUNIT Function
“freeunit” finds an unopened Fortran I/O unit and returns its numerical value from 1 to 99; the units already assigned to “input” and “iout” (usually 5 and 6) are skipped since they have special meaning as the default I/O units
GAMMLN Function
“gammln” uses a series expansion due to Lanczos to compute the natural logarithm of the Gamma function at “x” in [0,1]
GAUSSJORDAN Subroutine
“gaussjordan” solves a system of linear equations by using the method of Gaussian elimination with partial pivoting
GDA Program
“gda” implements Gaussian Density Annealing (GDA) algorithm for global optimization via simulated annealing
GDA1 Subroutine
GDA2 Function
GDA3 Subroutine
GDASTAT Subroutine
for a GDA integration step; also saves the coordinates
GENDOT Subroutine
“gendot” finds the coordinates of a specified number of surface points for a sphere with the input radius and coordinate center
GEODESIC Subroutine
“geodesic” smooths the upper and lower distance bounds via the triangle inequality using a sparse matrix version of a shortest path algorithm
GEOMETRY Function
“geometry” finds the value of the interatomic distance, angle or dihedral angle defined by two to four input atoms
GETARC Subroutine
“getarc” asks for a coordinate archive or trajectory file name, then reads the formatted or binary archive file
GETBASE Subroutine
“getbase” finds the base heavy atoms for a single nucleotide residue and copies the names and coordinates to the Protein Data Bank file
GETCART Subroutine
“getcart” asks for a Cartesian coordinate file name, then reads the formatted or binary coordinates file
GETCHUNK Subroutine
“getchunk” determines the number of grid point “chunks” used along each axis of the PME grid for parallelization
GETDCD Subroutine
“getdcd” asks for a binary DCD trajectory file name and the corresponding Tinker coordinates file, then reads the initial set of DCD coordinates
GETINT Subroutine
“getint” asks for an internal coordinate file name, then reads the internal coordinates and computes Cartesian coordinates
GETKEY Subroutine
“getkey” finds a valid keyfile and stores its contents as line images for subsequent keyword parameter searching
GETMOL Subroutine
“getmol” asks for a MDL MOL molecule file name, then reads the coordinates from the file
GETMOL2 Subroutine
“getmol2” asks for a Tripos MOL2 molecule file name, then reads the coordinates from the file
GETMONITOR Subroutine
GETNUCH Subroutine
“getnuch” finds the nucleotide hydrogen atoms for a single residue and copies the names and coordinates to the Protein Data Bank file
GETNUMB Subroutine
“getnumb” searches an input string from left to right for an integer and puts the numeric value in “number”; returns zero with “next” unchanged if no integer value is found
GETPDB Subroutine
“getpdb” asks for a Protein Data Bank file name, then reads in the coordinates file
GETPRB Subroutine
“getprb” tests for a possible probe position at the interface between three neighboring atoms
GETPRM Subroutine
“getprm” finds the potential energy parameter file and then opens and reads the parameters
GETPROH Subroutine
“getproh” finds the hydrogen atoms for a single amino acid residue and copies the names and coordinates to the Protein Data Bank file
GETREF Subroutine
“getref” copies structure information from the reference area into the standard variables for the current system structure
GETSEQ Subroutine
“getseq” asks the user for the amino acid sequence and torsional angle values needed to define a peptide
GETSEQN Subroutine
“getseqn” asks the user for the nucleotide sequence and torsional angle values needed to define a nucleic acid
GETSIDE Subroutine
“getside” finds the side chain heavy atoms for a single amino acid residue and copies the names and coordinates to the Protein Data Bank file
GETSTRING Subroutine
“getstring” searches for a quoted text string within an input character string; the region between the first and second double quote is returned as the “text”; if the actual text is too long, only the first part is returned
GETTEXT Subroutine
“gettext” searches an input string for the first string of non-blank characters; the region from a non-blank character to the first space or tab is returned as “text”; if the actual text is too long, only the first part is returned
GETTIME Subroutine
“gettime” finds the elapsed wall clock and CPU times in seconds since the last call to “settime”
GETTOR Subroutine
“gettor” tests for a possible torus position at the interface between two atoms, and finds the torus radius, center and axis
GETWORD Subroutine
“getword” searches an input string for the first alphabetic character (A-Z or a-z); the region from this first character to the first blank space or separator is returned as a “word”; if the actual word is too long, only the first part is returned
GETXYZ Subroutine
“getxyz” asks for a Cartesian coordinate file name, then reads in the coordinates file
GHMCSTEP Subroutine
“ghmcstep” performs a single stochastic dynamics time step via the generalized hybrid Monte Carlo (GHMC) algorithm to ensure exact sampling from the Boltzmann density
GHMCTERM Subroutine
“ghmcterm” finds the friction and fluctuation terms needed to update velocities during GHMC stochastic dynamics
GRADFAST Subroutine
“gradfast” calculates the potential energy and first derivatives for the fast-evolving local valence potential energy terms
GRADIENT Subroutine
“gradient” calls subroutines to calculate the potential energy and first derivatives with respect to Cartesian coordinates
GRADRGD Subroutine
“gradrgd” calls subroutines to calculate the potential energy and first derivatives with respect to rigid body coordinates
GRADROT Subroutine
“gradrot” calls subroutines to calculate the potential energy and its torsional first derivatives
GRADSLOW Subroutine
“gradslow” calculates the potential energy and first derivatives for the slow-evolving nonbonded potential energy terms
GRAFIC Subroutine
“grafic” outputs the upper & lower triangles and diagonal of a square matrix in a schematic form for visual inspection
GRID_DISP Subroutine
“grid_disp” places the damped dispersion coefficients onto the particle mesh Ewald grid
GRID_MPOLE Subroutine
“grid_mpole” places the fractional atomic multipoles onto the particle mesh Ewald grid
GRID_PCHG Subroutine
“grid_pchg” places the fractional atomic partial charges onto the particle mesh Ewald grid
GRID_UIND Subroutine
“grid_uind” places the fractional induced dipoles onto the particle mesh Ewald grid
GROUPS Subroutine
“groups” tests a set of atoms to see if all are members of a single atom group or a pair of atom groups; if so, then the correct intra- or intergroup weight is assigned
GRPLINE Subroutine
“grpline” tests each atom group for linearity of the sites contained in the group
GSORT Subroutine
“gsort” uses the Gram-Schmidt algorithm to build orthogonal vectors for sliding block interative matrix diagonalization
GYRATE Subroutine
“gyrate” computes the radius of gyration of a molecular system from its atomic coordinates; only active atoms are included
HANGLE Subroutine
“hangle” constructs hybrid angle bending parameters given an initial state, final state and “lambda” value
HATOM Subroutine
“hatom” assigns a new atom type to each hybrid site
HBOND Subroutine
“hbond” constructs hybrid bond stretch parameters given an initial state, final state and “lambda” value
HCHARGE Subroutine
“hcharge” constructs hybrid charge interaction parameters given an initial state, final state and “lambda” value
HDIPOLE Subroutine
“hdipole” constructs hybrid dipole interaction parameters given an initial state, final state and “lambda” value
HESSBLK Subroutine
“hessblk” calls subroutines to calculate the Hessian elements for each atom in turn with respect to Cartesian coordinates
HESSIAN Subroutine
“hessian” calls subroutines to calculate the Hessian elements for each atom in turn with respect to Cartesian coordinates
HESSRGD Subroutine
“hessrgd” computes the numerical Hessian elements with respect to rigid body coordinates via 6*ngroup+1 gradient evaluations
HESSROT Subroutine
“hessrot” computes numerical Hessian elements with respect to torsional angles; either the diagonal or the full matrix can be calculated; the full matrix needs nomega+1 gradient evaluations while the diagonal needs just two evaluations
HETATOM Subroutine
“hetatom” translates water molecules and ions in Protein Data Bank format to a Cartesian coordinate file and sequence file
HIMPTOR Subroutine
“himptor” constructs hybrid improper torsional parameters given an initial state, final state and “lambda” value
HOOVER Subroutine
“hoover” applies a combined thermostat and barostat via a Nose-Hoover chain algorithm
HSTRBND Subroutine
“hstrbnd” constructs hybrid stretch-bend parameters given an initial state, final state and “lambda” value
HSTRTOR Subroutine
“hstrtor” constructs hybrid stretch-torsion parameters given an initial state, final state and “lambda” value
HTORS Subroutine
“htors” constructs hybrid torsional parameters for a given initial state, final state and “lambda” value
HVDW Subroutine
“hvdw” constructs hybrid van der Waals parameters given an initial state, final state and “lambda” value
HYBRID Subroutine
“hybrid” constructs the hybrid hamiltonian for a specified initial state, final state and mutation parameter “lambda”
IJKPTS Subroutine
“ijkpts” stores a set of indices used during calculation of macroscopic reaction field energetics
IMAGE Subroutine
“image” takes the components of pairwise distance between two points in a periodic box and converts to the components of the minimum image distance
IMAGEN Subroutine
“imagen” takes the components of pairwise distance between two points and converts to the components of the minimum image distance
IMAGER Subroutine
“imager” takes the components of pairwise distance between two points in the same or neighboring periodic boxes and converts to the components of the minimum image distance
IMPOSE Subroutine
“impose” performs the least squares best superposition of two atomic coordinate sets via a quaternion method; upon return, the first coordinate set is unchanged while the second set is translated and rotated to give best fit; the final root mean square fit is returned in “rmsvalue”
INDTCGA Subroutine
“indtcga” computes the induced dipoles and intermediates used in polarization force calculation for the TCG method with dp cross terms = true, initial guess mu0 = 0 and using a diagonal preconditioner
INDTCGB Subroutine
“indtcgb” computes the induced dipoles and intermediates used in polarization force calculation for the TCG method with dp cross terms = true, initial guess mu0 = direct and using diagonal preconditioner
INDUCE Subroutine
“induce” computes the induced dipole moments at polarizable sites due to direct or mutual polarization
INDUCE0A Subroutine
“induce0a” computes the induced dipole moments at polarizable sites using a preconditioned conjugate gradient solver
INDUCE0B Subroutine
“induce0b” computes and stores the induced dipoles via the truncated conjugate gradient (TCG) method
INDUCE0C Subroutine
“induce0c” computes the induced dipole moments at polarizable sites for generalized Kirkwood SCRF and vacuum environments
INDUCE0D Subroutine
“induce0d” computes the induced dipole moments at polarizable sites for Poisson-Boltzmann SCRF and vacuum environments
INEDGE Subroutine
“inedge” inserts a concave edge into the linked list for its temporary torus
INERTIA Subroutine
“inertia” computes the principal moments of inertia for the system, and optionally translates the center of mass to the origin and rotates the principal axes onto the global axes
INITATOM Subroutine
“initatom” sets the atomic symbol, standard atomic weight, van der Waals radius and covalent radius for each element in the periodic table
INITERR Function
“initerr” is the initial error function and derivatives for a distance geometry embedding; it includes components from the local geometry and torsional restraint errors
INITIAL Subroutine
“initial” sets up original values for some parameters and variables that might not otherwise get initialized
INITMMFF Subroutine
“initmmff” initializes some parameter values for the Merck Molecular force field
INITPRM Subroutine
“initprm” completely initializes a force field by setting all parameters to zero and using defaults for control values
INITRES Subroutine
“initres” sets biopolymer residue names and biotype codes used in PDB file conversion and automated generation of structures
INITROT Subroutine
“initrot” sets the torsional angles which are to be rotated in subsequent computation, by default automatically selects all rotatable single bonds; optionally makes atoms inactive when they are not moved by any torsional rotation
INSERT Subroutine
“insert” adds the specified atom to the Cartesian coordinates list and shifts the remaining atoms
INTEDIT Program
“intedit” allows the user to extract information from or alter the values within an internal coordinates file
INTERPOL Subroutine
“interpol” computes intergroup induced dipole moments for use during removal of intergroup polarization
INTXYZ Program
“intxyz” takes as input an internal coordinates file, converts to and then writes out Cartesian coordinates
INVBETA Function
“invbeta” computes the inverse Beta distribution function via a combination of Newton iteration and bisection search
INVERT Subroutine
“invert” inverts a matrix using the Gauss-Jordan method
IPEDGE Subroutine
“ipedge” inserts convex edge into linked list for atom
JACOBI Subroutine
“jacobi” performs a matrix diagonalization of a real symmetric matrix by the method of Jacobi rotations
JUSTIFY Subroutine
“justify” converts a text string to right justified format with leading blank spaces
KANGANG Subroutine
“kangang” assigns the parameters for angle-angle cross term interactions and processes new or changed parameter values
KANGLE Subroutine
“kangle” assigns the force constants and ideal angles for the bond angles; also processes new or changed parameters
KANGLEM Subroutine
“kanglem” assigns the force constants and ideal angles for bond angles according to the Merck Molecular Force Field (MMFF)
KANGTOR Subroutine
“kangtor” assigns parameters for angle-torsion interactions and processes new or changed parameter values
KATOM Subroutine
“katom” assigns an atom type definitions to each atom in the structure and processes any new or changed values
KBOND Subroutine
“kbond” assigns a force constant and ideal bond length to each bond in the structure and processes any new or changed parameter values
KBONDM Subroutine
“kbondm” assigns a force constant and ideal bond length to each bond according to the Merck Molecular Force Field (MMFF)
KCHARGE Subroutine
“kcharge” assigns partial charges to the atoms within the structure and processes any new or changed values
KCHARGEM Subroutine
“kchargem” assigns partial charges to the atoms according to the Merck Molecular Force Field (MMFF)
KCHGFLX Subroutine
“kchgflx” assigns a force constant and ideal bond length to each bond in the structure and processes any new or changed parameter values
KCHGTRN Subroutine
“kchgtrn” assigns charge magnitude and damping parameters for charge transfer interactions and processes any new or changed values for these parameters
KCHIRAL Subroutine
“kchiral” determines the target value for each chirality and planarity restraint as the signed volume of the parallelpiped spanned by vectors from a common atom to each of three other atoms
KDIPOLE Subroutine
“kdipole” assigns bond dipoles to the bonds within the structure and processes any new or changed values
KDISP Subroutine
“kdisp” assigns C6 coefficients and damping parameters for dispersion interactions and processes any new or changed values for these parameters
KENEG Subroutine
“keneg” applies primary and secondary electronegativity bond length corrections to applicable bond parameters
KEWALD Subroutine
“kewald” assigns particle mesh Ewald parameters and options for a periodic system
KEXTRA Subroutine
“kextra” assigns parameters to any additional user defined potential energy contribution
KGB Subroutine
“kgb” initializes parameters needed for the generalized Born implicit solvation models
KGEOM Subroutine
“kgeom” asisgns parameters for geometric restraint terms to be included in the potential energy calculation
KGK Subroutine
“kgk” initializes parameters needed for the generalized Kirkwood implicit solvation model
KHPMF Subroutine
“khpmf” initializes parameters needed for the hydrophobic potential of mean force nonpolar implicit solvation model
KIMPROP Subroutine
“kimprop” assigns potential parameters to each improper dihedral in the structure and processes any changed values
KIMPTOR Subroutine
“kimptor” assigns torsional parameters to each improper torsion in the structure and processes any changed values
KINAUX Subroutine
“kinaux” computes the total kinetic energy and temperature for auxiliary dipole variables used in iEL polarization
KINETIC Subroutine
“kinetic” computes the total kinetic energy and kinetic energy contributions to the pressure tensor by summing over velocities
KMETAL Subroutine
“kmetal” assigns ligand field parameters to transition metal atoms and processes any new or changed parameter values
KMPOLE Subroutine
“kmpole” assigns atomic multipole moments to the atoms of the structure and processes any new or changed values
KNP Subroutine
“knp” initializes parameters needed for the cavity-plus- dispersion nonpolar implicit solvation model
KONVEC Subroutine
“konvec” finds a Hessian-vector product via finite-difference evaluation of the gradient based on atomic displacements
KOPBEND Subroutine
“kopbend” assigns the force constants for out-of-plane bends at trigonal centers via Wilson-Decius-Cross or Allinger angles; also processes any new or changed parameter values
KOPBENDM Subroutine
“kopbendm” assigns the force constants for out-of-plane bends according to the Merck Molecular Force Field (MMFF)
KOPDIST Subroutine
“kopdist” assigns the force constants for out-of-plane distance at trigonal centers via the central atom height; also processes any new or changed parameter values
KORBIT Subroutine
“korbit” assigns pi-orbital parameters to conjugated systems and processes any new or changed parameters
KPB Subroutine
“kpb” assigns parameters needed for the Poisson-Boltzmann implicit solvation model implemented via APBS
KPITORS Subroutine
“kpitors” assigns pi-system torsion parameters to torsions needing them, and processes any new or changed values
KPOLAR Subroutine
“kpolar” assigns atomic dipole polarizabilities to the atoms within the structure and processes any new or changed values
KREPEL Subroutine
“krepel” assigns the size values, exponential parameter and number of valence electrons for Pauli repulsion interactions and processes any new or changed values for these parameters
KSA Subroutine
“ksa” initializes parameters needed for surface area-based implicit solvation models including ASP and SASA
KSOLV Subroutine
“ksolv” assigns implicit solvation energy parameters for the surface area, generalized Born, generalized Kirkwood, Poisson-Boltzmann, cavity-dispersion and HPMF models
KSTRBND Subroutine
“kstrbnd” assigns parameters for stretch-bend interactions and processes new or changed parameter values
KSTRBNDM Subroutine
“kstrbndm” assigns parameters for stretch-bend interactions according to the Merck Molecular Force Field (MMFF)
KSTRTOR Subroutine
“kstrtor” assigns stretch-torsion parameters to torsions needing them, and processes any new or changed values
KTORS Subroutine
“ktors” assigns torsional parameters to each torsion in the structure and processes any new or changed values
KTORSM Subroutine
“ktorsm” assigns torsional parameters to each torsion according to the Merck Molecular Force Field (MMFF)
KTORTOR Subroutine
“ktortor” assigns torsion-torsion parameters to adjacent torsion pairs and processes any new or changed values
KUREY Subroutine
“kurey” assigns the force constants and ideal distances for the Urey-Bradley 1-3 interactions; also processes any new or changed parameter values
KVDW Subroutine
“kvdw” assigns the parameters to be used in computing the van der Waals interactions and processes any new or changed values for these parameters
LATTICE Subroutine
“lattice” stores the periodic box dimensions and sets angle values to be used in computing fractional coordinates
LBFGS Subroutine
“lbfgs” is a limited memory BFGS quasi-newton nonlinear optimization routine
LIGASE Subroutine
“ligase” translates a nucleic acid structure in Protein Data Bank format to a Cartesian coordinate file and sequence file
LIGHTS Subroutine
“lights” computes the set of nearest neighbor interactions using the method of lights algorithm
LINBODY Subroutine
“linbody” finds the angular velocity of a linear rigid body given the inertia tensor and angular momentum
LMSTEP Subroutine
“lmstep” computes a Levenberg-Marquardt step during a nonlinear least squares calculation using ideas from the MINPACK LMPAR routine and the internal doubling strategy of Dennis and Schnabel
LOCALMIN Subroutine
“localmin” is used during normal mode local search to perform a Cartesian coordinate energy minimization
LOCALRGD Subroutine
“localrgd” is used during the PSS local search procedure to perform a rigid body energy minimization
LOCALROT Subroutine
“localrot” is used during the PSS local search procedure to perform a torsional space energy minimization
LOCALXYZ Subroutine
“localxyz” is used during the potential smoothing and search procedure to perform a local optimization at the current smoothing level
LOCERR Function
“locerr” is the local geometry error function and derivatives including the 1-2, 1-3 and 1-4 distance bound restraints
LOWCASE Subroutine
“lowcase” converts a text string to all lower case letters
MAJORIZE Subroutine
“majorize” refines the projected coordinates by attempting to minimize the least square residual between the trial distance matrix and the distances computed from the coordinates
MAKEBAR Subroutine
MAKEBOX Subroutine
“makebox” builds a periodic box of a desired size by randomly copying a specified number of monomers into a target box size, followed by optional excluded volume refinement
MAKEINT Subroutine
“makeint” converts Cartesian to internal coordinates where selection of internal coordinates is controlled by “mode”
MAKEPDB Subroutine
“makepdb” cconstructs a Protein Data Bank file from a set of Cartesian coordinates with special handling for systems consisting of biopolymer chains, ligands and water molecules
MAKEREF Subroutine
“makeref” copies the information contained in the “xyz” file of the current structure into corresponding reference areas
MAKEXYZ Subroutine
“makexyz” generates a complete set of Cartesian coordinates for a full structure from the internal coordinate values
MAPCHECK Subroutine
“mapcheck” checks the current minimum energy structure for possible addition to the master list of local minima
MATCH1 Subroutine
“match1” finds and stores the first multipole component found on a line of output from Stone’s GDMA program
MATCH2 Subroutine
“match2” finds and stores the second multipole component found on a line of output from Stone’s GDMA program
MATCH3 Subroutine
“match3” finds and stores the third multipole component found on a line of output from Stone’s GDMA program
MAXWELL Function
“maxwell” returns a speed in Angstroms/picosecond randomly selected from a 3-D Maxwell-Boltzmann distribution for the specified particle mass and system temperature
MBUILD Subroutine
“mbuild” performs a complete rebuild of the atomic multipole electrostatic neighbor list for all sites
MCM1 Function
“mcm1” is a service routine that computes the energy and gradient for truncated Newton optimization in Cartesian coordinate space
MCM2 Subroutine
“mcm2” is a service routine that computes the sparse matrix Hessian elements for truncated Newton optimization in Cartesian coordinate space
MCMSTEP Function
“mcmstep” implements the minimization phase of an MCM step via Cartesian minimization following a Monte Carlo step
MDINIT Subroutine
“mdinit” initializes the velocities and accelerations for a molecular dynamics trajectory, including restarts
MDREST Subroutine
“mdrest” finds and removes any translational or rotational kinetic energy of the overall system center of mass
MDSAVE Subroutine
“mdsave” writes molecular dynamics trajectory snapshots and auxiliary files with velocity, force or induced dipole data; also checks for user requested termination of a simulation
MDSTAT Subroutine
“mdstat” is called at each molecular dynamics time step to form statistics on various average values and fluctuations, and to periodically save the state of the trajectory
MEASFN Subroutine
MEASFQ Subroutine
MEASFS Subroutine
MEASPM Subroutine
“measpm” computes the volume of a single prism section of the full interior polyhedron
MECHANIC Subroutine
“mechanic” sets up needed parameters for the potential energy calculation and reads in many of the user selectable options
MERGE Subroutine
“merge” combines the reference and current structures into a single new “current” structure containing the reference atoms followed by the atoms of the current structure
METRIC Subroutine
“metric” takes as input the trial distance matrix and computes the metric matrix of all possible dot products between the atomic vectors and the center of mass using the law of cosines and the following formula for the distances to the center of mass:
MIDERR Function
“miderr” is the secondary error function and derivatives for a distance geometry embedding; it includes components from the distance bounds, local geometry, chirality and torsional restraint errors
MINIMIZ1 Function
“minimiz1” is a service routine that computes the energy and gradient for a low storage BFGS optimization in Cartesian coordinate space
MINIMIZE Program
“minimize” performs energy minimization in Cartesian coordinate space using a low storage BFGS nonlinear optimization
MINIROT Program
“minirot” performs an energy minimization in torsional angle space using a low storage BFGS nonlinear optimization
MINIROT1 Function
“minirot1” is a service routine that computes the energy and gradient for a low storage BFGS nonlinear optimization in torsional angle space
MINPATH Subroutine
“minpath” is a routine for finding the triangle smoothed upper and lower bounds of each atom to a specified root atom using a sparse variant of the Bellman-Ford shortest path algorithm
MINRIGID Program
“minrigid” performs an energy minimization of rigid body atom groups using a low storage BFGS nonlinear optimization
MINRIGID1 Function
“minrigid1” is a service routine that computes the energy and gradient for a low storage BFGS nonlinear optimization of rigid bodies
MLIGHT Subroutine
“mlight” performs a complete rebuild of the atomic multipole pair neighbor list for all sites using the method of lights
MLIST Subroutine
“mlist” performs an update or a complete rebuild of the nonbonded neighbor lists for atomic multipoles
MMID Subroutine
“mmid” implements a modified midpoint method to advance the integration of a set of first order differential equations
MODECART Subroutine
MODERGD Subroutine
MODEROT Subroutine
MODESRCH Subroutine
MODETORS Subroutine
MODULI Subroutine
“moduli” sets the moduli of the inverse discrete Fourier transform of the B-splines
MOL2XYZ Program
“mol2xyz” takes as input a Tripos MOL2 coordinates file, converts to and then writes out Cartesian coordinates
MOLECULE Subroutine
“molecule” counts the molecules, assigns each atom to its molecule and computes the mass of each molecule
MOLMERGE Subroutine
“molmerge” connects fragments and removes duplicate atoms during generation of a unit cell from an asymmetric unit
MOLSETUP Subroutine
“molsetup” generates trial parameters needed to perform polarizable multipole calculations on a structure read from distributed multipole analysis output
MOLUIND Subroutine
“moluind” computes the molecular induced dipole components in the presence of an external electric field
MOLXYZ Program
“molxyz” takes as input a MDL MOL coordinates file, converts to and then writes out Cartesian coordinates
MOMENTS Subroutine
“moments” computes the total electric charge, dipole and quadrupole moments for the active atoms as a sum over the partial charges, bond dipoles and atomic multipole moments
MOMFULL Subroutine
“momfull” computes the electric moments for the full system as a sum over the partial charges, bond dipoles and atomic multipole moments
MOMYZE Subroutine
“momyze” finds and prints the total charge, dipole moment components, radius of gyration and moments of inertia
MONTE Program
“monte” performs a Monte Carlo-Minimization conformational search using Cartesian single atom or torsional move sets
MUTATE Subroutine
“mutate” constructs the hybrid hamiltonian for a specified initial state, final state and mutation parameter “lambda”
NBLIST Subroutine
“nblist” builds and maintains nonbonded pair neighbor lists for vdw, dispersion, electrostatic and polarization terms
NEARBY Subroutine
“nearby” finds all of the through-space neighbors of each atom for use in surface area and volume calculations
NEEDUPDATE Subroutine
NEWATM Subroutine
“newatm” creates and defines an atom needed for the Cartesian coordinates file, but which may not present in the original Protein Data Bank file
NEWTON Program
“newton” performs an energy minimization in Cartesian coordinate space using a truncated Newton method
NEWTON1 Function
“newton1” is a service routine that computes the energy and gradient for truncated Newton optimization in Cartesian coordinate space
NEWTON2 Subroutine
“newton2” is a service routine that computes the sparse matrix Hessian elements for truncated Newton optimization in Cartesian coordinate space
NEWTROT Program
“newtrot” performs an energy minimization in torsional angle space using a truncated Newton conjugate gradient method
NEWTROT1 Function
“newtrot1” is a service routine that computes the energy and gradient for truncated Newton conjugate gradient optimization in torsional angle space
NEWTROT2 Subroutine
“newtrot2” is a service routine that computes the sparse matrix Hessian elements for truncated Newton optimization in torsional angle space
NEXTARG Subroutine
“nextarg” finds the next unused command line argument and returns it in the input character string
NEXTTEXT Function
“nexttext” finds and returns the location of the first non-blank character within an input text string; zero is returned if no such character is found
NORMAL Function
“normal” generates a random number from a normal Gaussian distribution with a mean of zero and a variance of one
NOSE Subroutine
“nose” performs a single molecular dynamics time step via a Nose-Hoover extended system isothermal-isobaric algorithm
NSPLINE Subroutine
“nspline” computes coefficients for an nonperiodic cubic spline with natural boundary conditions where the first and last second derivatives are already known
NUCBASE Subroutine
“nucbase” builds the side chain for a single nucleotide base in terms of internal coordinates
NUCCHAIN Subroutine
“nucchain” builds up the internal coordinates for a nucleic acid sequence from the sugar type, backbone and glycosidic torsional values
NUCLEIC Program
“nucleic” builds the internal and Cartesian coordinates of a polynucleotide from nucleic acid sequence and torsional angle values for the nucleic acid backbone and side chains
NUMBER Function
“number” converts a text numeral into an integer value; the input string must contain only numeric characters
NUMERAL Subroutine
“numeral” converts an input integer number into the corresponding right- or left-justified text numeral
NUMGRAD Subroutine
“numgrad” computes the gradient of the objective function “fvalue” with respect to Cartesian coordinates of the atoms via a one-sided or two-sided numerical differentiation
OCVM Subroutine
“ocvm” is an optimally conditioned variable metric nonlinear optimization routine without line searches
OLDATM Subroutine
“oldatm” get the Cartesian coordinates for an atom from the Protein Data Bank file, then assigns the atom type and atomic connectivities
OPBGUESS Function
“opbguess” sets approximate out-of-plane bend force constants based on atom type and connected atoms
OPENEND Subroutine
“openend” opens a file on a Fortran unit such that the position is set to the bottom for appending to the end of the file
OPREP Subroutine
“oprep” sets up the frictional and random terms needed to update positions and velocities for the BAOAB integrator
OPTFIT Function
OPTIMIZ1 Function
“optimiz1” is a service routine that computes the energy and gradient for optimally conditioned variable metric optimization in Cartesian coordinate space
OPTIMIZE Program
“optimize” performs energy minimization in Cartesian coordinate space using an optimally conditioned variable metric method
OPTINIT Subroutine
“optinit” initializes values and keywords used by multiple structure optimization methods
OPTIROT Program
“optirot” performs an energy minimization in torsional angle space using an optimally conditioned variable metric method
OPTIROT1 Function
“optirot1” is a service routine that computes the energy and gradient for optimally conditioned variable metric optimization in torsional angle space
OPTRIGID Program
“optrigid” performs an energy minimization of rigid body atom groups using an optimally conditioned variable metric method
OPTRIGID1 Function
“optrigid1” is a service routine that computes the energy and gradient for optimally conditioned variable metric optimization of rigid bodies
OPTSAVE Subroutine
“optsave” is used by the optimizers to write imtermediate coordinates and other relevant information; also checks for user requested termination of an optimization
ORBITAL Subroutine
“orbital” finds and organizes lists of atoms in a pisystem, bonds connecting pisystem atoms and torsions whose central atoms are both pisystem atoms
ORIENT Subroutine
“orient” computes a set of reference Cartesian coordinates in standard orientation for each rigid body atom group
ORTHOG Subroutine
“orthog” performs an orthogonalization of an input matrix via the modified Gram-Schmidt algorithm
OVERLAP Subroutine
“overlap” computes the overlap for two parallel p-orbitals given the atomic numbers and distance of separation
PARAMYZE Subroutine
“paramyze” prints the force field parameters used in the computation of each of the potential energy terms
PARTYZE Subroutine
“partyze” prints the energy component and number of interactions for each of the potential energy terms
PASSB Subroutine
PASSB2 Subroutine
PASSB3 Subroutine
PASSB4 Subroutine
PASSB5 Subroutine
PASSF Subroutine
PASSF2 Subroutine
PASSF3 Subroutine
PASSF4 Subroutine
PASSF5 Subroutine
PATH Program
“path” locates a series of structures equally spaced along a conformational pathway connecting the input reactant and product structures; a series of constrained optimizations orthogonal to the path is done via Lagrangian multipliers
PATH1 Function
PATHPNT Subroutine
“pathpnt” finds a structure on the synchronous transit path with the specified path value “tpath”
PATHSCAN Subroutine
“pathscan” makes a scan of a synchronous transit pathway by computing structures and energies for specific path values
PATHVAL Subroutine
“pathval” computes the synchronous transit path value for the specified structure
PAULING Subroutine
“pauling” uses a rigid body optimization to approximately pack multiple polypeptide chains
PAULING1 Function
“pauling1” is a service routine that computes the energy and gradient for optimally conditioned variable metric optimization of rigid bodies
PBDIRECTPOLFORCE Subroutine
PBEMPOLE Subroutine
“pbempole” calculates the permanent multipole PB energy, field, forces and torques
PBMUTUALPOLFORCE Subroutine
PDBATOM Subroutine
“pdbatom” adds an atom to the Protein Data Bank file
PDBXYZ Program
“pdbxyz” takes as input a Protein Data Bank file and then converts to and writes out a Cartesian coordinates file and, for biopolymers, a sequence file
PIALTER Subroutine
“pialter” modifies bond lengths and force constants according to the “planar” P-P-P bond order values; also alters 2-fold torsional parameters based on the “nonplanar” bond orders
PICALC Subroutine
“picalc” performs a modified Pariser-Parr-Pople molecular orbital calculation for each conjugated pisystem
PIMOVE Subroutine
“pimove” rotates the vector between atoms “list(1)” and “list(2)” so that atom 1 is at the origin and atom 2 along the x-axis; the atoms defining the respective planes are also moved and their bond lengths normalized
PIPLANE Subroutine
“piplane” selects the three atoms which specify the plane perpendicular to each p-orbital; the current version will fail in certain situations, including ketenes, allenes, and isolated or adjacent triple bonds
PISCF Subroutine
“piscf” performs an SCF molecular orbital calculation for a pisystem to determine bond orders used in parameter scaling
PITILT Subroutine
“pitilt” calculates for each pibond the ratio of the actual p-orbital overlap integral to the ideal overlap if the same orbitals were perfectly parallel
PLACE Subroutine
“place” finds the probe sites by putting the probe sphere tangent to each triple of neighboring atoms
PMONTE Subroutine
“pmonte” implements a Monte Carlo barostat via random trial changes in the periodic box volume and shape
POLARGRP Subroutine
“polargrp” generates members of the polarization group of each atom and separate lists of the 1-2, 1-3 and 1-4 group connectivities
POLARIZE Program
“polarize” computes the molecular polarizability by applying an external field along each axis followed by diagonalization of the resulting polarizability tensor
POLEDIT Program
“poledit” provides for the modification and manipulation of polarizable atomic multipole electrostatic models
POLESORT Subroutine
“polesort” sorts a set of atomic multipole parameters based on the atom types of centers involved
POLYMER Subroutine
“polymer” tests for the presence of an infinite polymer extending across periodic boundaries
POLYP Subroutine
“polyp” is a polynomial product routine that multiplies two algebraic forms
POTENTIAL Program
“potential” calculates the electrostatic potential for a molecule at a set of grid points; optionally compares to a target potential or optimizes electrostatic parameters
POTGRID Subroutine
“potgrid” generates electrostatic potential grid points in radially distributed shells based on the molecular surface
POTNRG Function
POTOFF Subroutine
“potoff” clears the forcefield definition by turning off the use of each of the potential energy functions
POTPOINT Subroutine
“potpoint” calculates the electrostatic potential at a grid point “i” as the total electrostatic interaction energy of the system with a positive charge located at the grid point
POTSTAT Subroutine
“potstat” computes and prints statistics for the electrostatic potential over a set of grid points
POTWRT Subroutine
PRECONBLK Subroutine
“preconblk” applies a preconditioner to an atom block section of the Hessian matrix
PRECOND Subroutine
“precond” solves a simplified version of the Newton equations Ms = r, and uses the result to precondition linear conjugate gradient iterations on the full Newton equations in “tnsolve”
PRESSURE Subroutine
“pressure” uses the internal virial to find the pressure in a periodic box and maintains a constant desired pressure via a barostat method
PRESSURE2 Subroutine
“pressure2” applies a box size and velocity correction at the half time step as needed for the Monte Carlo barostat
PRIORITY Function
“priority” decides which of a set of connected atoms should have highest priority in construction of a local coordinate frame and returns its atom number; if all atoms are of equal priority then zero is returned
PRMEDIT Program
“prmedit” reformats an existing parameter file, and revises type and class numbers based on the “atom” parameter ordering
PRMFORM Subroutine
“prmform” formats each individual parameter record to conform to a consistent text layout
PRMKEY Subroutine
“prmkey” parses a text string to extract keywords related to force field potential energy functional forms and constants
PRMORDER Subroutine
“prmorder” places a list of atom type or class numbers into canonical order for potential energy parameter definitions
PRMSORT Subroutine
“prmsort” places a list of atom type or class numbers into canonical order for potential energy parameter definitions
PRMVAR Subroutine
“prmvar” determines the optimization values from the corresponding electrostatic potential energy parameters
PRMVAR Subroutine
“prmvar” determines the optimization values from the corresponding valence potential energy parameters
PROCHAIN Subroutine
“prochain” builds up the internal coordinates for an amino acid sequence from the phi, psi, omega and chi values
PROJCT Subroutine
PROJECT Subroutine
“project” reads locked vectors from a binary file and projects them out of the components of the set of trial eigenvectors using the relation Y = X - U * U^T * X
PROJECTK Subroutine
“projectk” reads locked vectors from a binary file and projects them out of the components of the set of trial eigenvectors using the relation Y = X - U * U^T * X
PROMO Subroutine
“promo” writes a banner message containing information about the Tinker version, release date and copyright notice
PROPERTY Function
“property” takes two input snapshot frames and computes the value of the property for which the correlation function is being accumulated
PROSIDE Subroutine
“proside” builds the side chain for a single amino acid residue in terms of internal coordinates
PROTEIN Program
“protein” builds the internal and Cartesian coordinates of a polypeptide from amino acid sequence and torsional angle values for the peptide backbone and side chains
PRTARC Subroutine
“prtarc” writes a Cartesian coordinates archive as either a formatted or binary disk file
PRTARCB Subroutine
“prtarcb” writes out a set of Cartesian coordinates for all active atoms in the CHARMM DCD binary format
PRTARCF Subroutine
“prtarcf” writes out a set of Cartesian coordinates for all active atoms in the Tinker XYZ archive format
PRTDYN Subroutine
“prtdyn” writes out the information needed to restart a molecular dynamics trajectory to an external disk file
PRTERR Subroutine
“prterr” writes out a set of coordinates to a disk file prior to aborting on a serious error
PRTFIT Subroutine
“prtfit” makes a key file containing results from fitting a charge or multipole model to an electrostatic potential grid
PRTINT Subroutine
“prtint” writes out a set of Z-matrix internal coordinates to an external disk file
PRTMOD Subroutine
“prtmod” writes out a set of modified Cartesian coordinates with an optional atom number offset to an external disk file
PRTMOL2 Program
“prtmol2” writes out a set of coordinates in Tripos MOL2 format to an external disk file
PRTPDB Subroutine
“prtpdb” writes out a set of Protein Data Bank coordinates to an external disk file
PRTPOLE Subroutine
“prtpole” creates a coordinates file, and a key file with atomic multipoles corrected for intergroup polarization
PRTPRM Subroutine
“prtprm” writes out a formatted listing of the default set of potential energy parameters for a force field
PRTSEQ Subroutine
“prtseq” writes out a biopolymer sequence to an external disk file with 15 residues per line and distinct chains separated by blank lines
PRTVAL Subroutine
“prtval” writes the final valence parameter results to the standard output and appends the values to a key file
PRTVIB Subroutine
“prtvib” writes to an external disk file a series of coordinate sets representing motion along a vibrational normal mode
PRTXYZ Subroutine
“prtxyz” writes out a set of Cartesian coordinates to an external disk file
PSCALE Subroutine
“pscale” implements a Berendsen barostat by scaling the coordinates and box dimensions via coupling to an external constant pressure bath
PSS Program
“pss” implements the potential smoothing plus search method for global optimization in Cartesian coordinate space with local searches performed in Cartesian or torsional space
PSS1 Function
“pss1” is a service routine that computes the energy and gradient during PSS global optimization in Cartesian coordinate space
PSS2 Subroutine
“pss2” is a service routine that computes the sparse matrix Hessian elements during PSS global optimization in Cartesian coordinate space
PSSRGD1 Function
“pssrgd1” is a service routine that computes the energy and gradient during PSS global optimization over rigid bodies
PSSRIGID Program
“pssrigid” implements the potential smoothing plus search method for global optimization for a set of rigid bodies
PSSROT Program
“pssrot” implements the potential smoothing plus search method for global optimization in torsional space
PSSROT1 Function
“pssrot1” is a service routine that computes the energy and gradient during PSS global optimization in torsional space
PSSWRITE Subroutine
PTEST Subroutine
“ptest” determines the numerical virial tensor, and compares analytical to numerical values for dE/dV and isotropic pressure
PTINCY Function
PZEXTR Subroutine
“pzextr” is a polynomial extrapolation routine used during Bulirsch-Stoer integration of ordinary differential equations
QIROTMAT Subroutine
“qirotmat” finds a rotation matrix that describes the interatomic vector
QONVEC Subroutine
“qonvec” is a vector utility routine used during sliding block iterative matrix diagonalization
QRFACT Subroutine
“qrfact” computes the QR factorization of an m by n matrix a via Householder transformations with optional column pivoting; the routine determines an orthogonal matrix q, a permutation matrix p, and an upper trapezoidal matrix r with diagonal elements of nonincreasing magnitude, such that a*p = q*r; the Householder transformation for column k, k = 1,2,…,min(m,n), is of the form:
QRSOLVE Subroutine
“qrsolve” solves a*x = b and d*x = 0 in the least squares sense; used with routine “qrfact” to solve least squares problems
QUATFIT Subroutine
“quatfit” uses a quaternion-based method to achieve the best fit superposition of two sets of coordinates
RADIAL Program
“radial” finds the radial distribution function for a specified pair of atom types via analysis of a set of coordinate frames
RANDOM Function
“random” generates a random number on [0,1] via a long period generator due to L’Ecuyer with Bays-Durham shuffle
RANVEC Subroutine
“ranvec” generates a unit vector in 3-dimensional space with uniformly distributed random orientation
RATTLE Subroutine
“rattle” implements the first portion of the RATTLE algorithm by correcting atomic positions and half-step velocities to maintain interatomic distance and absolute spatial constraints
RATTLE2 Subroutine
“rattle2” implements the second portion of the RATTLE algorithm by correcting the full-step velocities in order to maintain interatomic distance constraints
READBLK Subroutine
“readblk” reads in a set of snapshot frames and transfers the values to internal arrays for use in the computation of time correlation functions
READCART Subroutine
“readcart” gets a set of Cartesian coordinates from either a formatted or binary disk file
READDCD Subroutine
“readdcd” reads in a set of Cartesian coordinates from an external disk file in CHARMM DCD binary format
READDYN Subroutine
“readdyn” get the positions, velocities and accelerations for a molecular dynamics restart from an external disk file
READGARC Subroutine
“readgarc” reads data from Gaussian archive section; each entry is terminated with a backslash symbol
READGAU Subroutine
“readgau” reads an ab initio optimized structure, forces, Hessian and frequencies from a Gaussian 09 output file
READGDMA Subroutine
“readgdma” takes the DMA output in spherical harmonics from the GDMA program and converts to Cartesian multipoles in the global coordinate frame
READINT Subroutine
“readint” gets a set of Z-matrix internal coordinates from an external file
READMOL Subroutine
“readmol” gets a set of MDL MOL coordinates from an external disk file
READMOL2 Subroutine
“readmol2” gets a set of Tripos MOL2 coordinates from an external disk file
READPDB Subroutine
“readpdb” gets a set of Protein Data Bank coordinates from an external disk file
READPOT Subroutine
“readpot” gets a set of grid points and target electrostatic potential values from an external disk file
READPRM Subroutine
“readprm” processes the potential energy parameter file in order to define the default force field parameters
READSEQ Subroutine
“readseq” gets a biopolymer sequence containing one or more separate chains from an external file; all lines containing sequence must begin with the starting sequence number, the actual sequence is read from subsequent nonblank characters
READXYZ Subroutine
“readxyz” gets a set of Cartesian coordinates from an external disk file
REFINE Subroutine
“refine” performs minimization of the atomic coordinates of an initial crude embedded distance geometry structure versus the bound, chirality, planarity and torsional error functions
RELEASEMONITOR Subroutine
REPLICA Subroutine
“replica” decides between images and replicates for generation of periodic boundary conditions, and sets the cell replicate list if the replicates method is to be used
RESPA Subroutine
“respa” performs a single multiple time step molecular dynamics step using the reversible reference system propagation algorithm (r-RESPA) via a Verlet core with the potential split into fast- and slow-evolving portions
RFINDEX Subroutine
“rfindex” finds indices for each multipole site for use in computing reaction field energetics
RGDSTEP Subroutine
“rgdstep” performs a single molecular dynamics time step via a rigid body integration algorithm
RIBOSOME Subroutine
“ribosome” translates a polypeptide structure in Protein Data Bank format to a Cartesian coordinate file and sequence file
RIGIDXYZ Subroutine
“rigidxyz” computes Cartesian coordinates for a rigid body group via rotation and translation of reference coordinates
RINGS Subroutine
“rings” searches the structure for small rings and stores their constituent atoms, and optionally reduces large rings into their component smaller rings
RMSERROR Subroutine
“rmserror” computes the maximum absolute deviation and the rms deviation from the distance bounds, and the number and rms value of the distance restraint violations
RMSFIT Function
“rmsfit” computes the rms fit of two coordinate sets
ROTANG Function
ROTCHECK Function
“rotcheck” tests a specified candidate rotatable bond for the disallowed case where inactive atoms are found on both sides of the candidate bond
ROTEULER Subroutine
“roteuler” computes a set of Euler angle values consistent with an input rotation matrix
ROTFRAME Subroutine
“rotframe” takes the global multipole moments and rotates them into the local coordinate frame defined at each atomic site
ROTLIST Subroutine
“rotlist” generates the minimum list of all the atoms lying to one side of a pair of directly bonded atoms; optionally finds the minimal list by choosing the side with fewer atoms
ROTMAT Subroutine
“rotmat” finds the rotation matrix that rotates the local coordinate system into the global frame at a multipole site
ROTPOLE Subroutine
“rotpole” constructs the set of atomic multipoles in the global frame by applying the correct rotation matrix for each site
ROTRGD Subroutine
“rotrgd” finds the rotation matrix for a rigid body due to a single step of dynamics
ROTSITE Subroutine
“rotsite” rotates the local frame atomic multipoles at a specified site into the global coordinate frame by applying a rotation matrix
SADDLE Program
“saddle” finds a transition state between two conformational minima using a combination of ideas from the synchronous transit (Halgren-Lipscomb) and quadratic path (Bell-Crighton) methods
SADDLE1 Function
“saddle1” is a service routine that computes the energy and gradient for transition state optimization
SADDLES Subroutine
“saddles” constructs circles, convex edges and saddle faces
SAVEYZE Subroutine
“saveyze” prints the atomic forces and/or the induced dipoles to separate external disk files
SBGUESS Subroutine
“sbguess” sets approximate stretch-bend force constants based on atom type and connected atoms
SCAN Program
“scan” attempts to find all the local minima on a potential energy surface via an iterative series of local searches along normal mode directions
SCAN1 Function
“scan1” is a service routine that computes the energy and gradient during exploration of a potential energy surface via iterative local search
SCAN2 Subroutine
“scan2” is a service routine that computes the sparse matrix Hessian elements during exploration of a potential energy surface via iterative local search
SCANPDB Subroutine
“scanpdb” reads the first model in a Protein Data Bank file and sets chains, alternate sites and insertion records to be used
SDAREA Subroutine
“sdarea” optionally scales the atomic friction coefficient of each atom based on its accessible surface area
SDSTEP Subroutine
“sdstep” performs a single stochastic dynamics time step via the velocity Verlet integration algorithm
SDTERM Subroutine
“sdterm” finds the frictional and random terms needed to update positions and velocities during stochastic dynamics
SEARCH Subroutine
“search” is a unidimensional line search based upon parabolic extrapolation and cubic interpolation using both function and gradient values
SETACCELERATION Subroutine
SETATOMIC Subroutine
SETATOMTYPES Subroutine
SETCHARGE Subroutine
SETCHUNK Subroutine
“setchunk” marks a chunk in the PME spatial table which is overlapped by the B-splines for a site
SETCONNECTIVITY Subroutine
SETCOORDINATES Subroutine
SETELECT Subroutine
“setelect” assigns partial charge, bond dipole and atomic multipole parameters for the current structure, as needed for computation of the electrostatic potential
SETENERGY Subroutine
SETFILE Subroutine
SETFORCEFIELD Subroutine
SETFRAME Subroutine
“setframe” assigns a local coordinate frame at each atomic multipole site using high priority connected atoms along axes
SETGRADIENTS Subroutine
SETINDUCED Subroutine
SETKEYWORD Subroutine
SETMASS Subroutine
SETMDTIME Subroutine
SETMOL2 Program
“setmol2” assigns MOL2 atom names/types/charges and bond types based upon atomic numbers and connectivity
SETNAME Subroutine
SETPAIR Program
“setpair” is a service routine that assigns flags, sets cutoffs and allocates arrays used by different pairwise neighbor methods
SETPOLAR Subroutine
“setpolar” assigns atomic polarizabilities, Thole damping or charge penetration parameters, and polarization groups with user modification of these values
SETPRM Subroutine
“setprm” counts and allocates memory space for force field parameter values involving multiple atom types or classes as found in the parameter file and keyfile
SETSTEP Subroutine
SETSTORY Subroutine
SETTIME Subroutine
“settime” initializes the wall clock and elapsed CPU times
SETUPDATED Subroutine
SETVELOCITY Subroutine
SHAKE Subroutine
“shake” implements the SHAKE algorithm by correcting atomic positions to maintain interatomic distance and absolute spatial constraints
SHAKE2 Subroutine
“shake2” modifies the gradient to remove components along any holonomic distance contraints using a variant of SHAKE
SHAKEUP Subroutine
“shakeup” initializes any holonomic constraints for use with the SHAKE and RATTLE algorithms
SHROTMAT Subroutine
“shrotmat” finds the rotation matrix that converts spherical harmonic quadrupoles from the local to the global frame given the required dipole rotation matrix
SHROTSITE Subroutine
“shrotsite” converts spherical harmonic multipoles from the local to the global frame given required rotation matrices
SIGMOID Function
“sigmoid” implements a normalized sigmoidal function on the interval [0,1]; the curves connect (0,0) to (1,1) and have a cooperativity controlled by beta, they approach a straight line as beta -> 0 and get more nonlinear as beta increases
SIMPLEX Subroutine
“simplex” is a general multidimensional Nelder-Mead simplex optimization routine requiring only repeated evaluations of the objective function
SIMPLEX1 Function
“simplex1” is a service routine used only by the Nelder-Mead simplex optimization method
SKTDYN Subroutine
“sktdyn” sends the current dynamics info via a socket
SKTINIT Subroutine
“sktinit” sets up socket communication with the graphical user interface by starting a Java virtual machine, initiating a server, and loading an object with system information
SKTKILL Subroutine
“sktkill” closes the server and Java virtual machine
SKTOPT Subroutine
“sktopt” sends the current optimization info via a socket
SLATER Subroutine
“slater” is a general routine for computing the overlap integrals between two Slater-type orbitals
SNIFFER Program
“sniffer” performs a global energy minimization using a discrete version of Griewank’s global search trajectory
SNIFFER1 Function
“sniffer1” is a service routine that computes the energy and gradient for the Sniffer global optimization method
SOAK Subroutine
“soak” takes a currently defined solute system and places it into a solvent box, with removal of any solvent molecules that overlap the solute
SORT Subroutine
“sort” takes an input list of integers and sorts it into ascending order using the Heapsort algorithm
SORT10 Subroutine
“sort10” takes an input list of character strings and sorts it into alphabetical order using the Heapsort algorithm, duplicate values are removed from the final sorted list
SORT2 Subroutine
“sort2” takes an input list of reals and sorts it into ascending order using the Heapsort algorithm; it also returns a key into the original ordering
SORT3 Subroutine
“sort3” takes an input list of integers and sorts it into ascending order using the Heapsort algorithm; it also returns a key into the original ordering
SORT4 Subroutine
“sort4” takes an input list of integers and sorts it into ascending absolute value using the Heapsort algorithm
SORT5 Subroutine
“sort5” takes an input list of integers and sorts it into ascending order based on each value modulo “m”
SORT6 Subroutine
“sort6” takes an input list of character strings and sorts it into alphabetical order using the Heapsort algorithm
SORT7 Subroutine
“sort7” takes an input list of character strings and sorts it into alphabetical order using the Heapsort algorithm; it also returns a key into the original ordering
SORT8 Subroutine
“sort8” takes an input list of integers and sorts it into ascending order using the Heapsort algorithm, duplicate values are removed from the final sorted list
SORT9 Subroutine
“sort9” takes an input list of reals and sorts it into ascending order using the Heapsort algorithm, duplicate values are removed from the final sorted list
SPACEFILL Program
“spacefill” computes the surface area and volume of a structure; the van der Waals, accessible-excluded, and contact-reentrant definitions are available
SPECTRUM Program
“spectrum” computes a power spectrum over a wavelength range from the velocity autocorrelation as a function of time
SPHERE Subroutine
“sphere” finds a specified number of uniformly distributed points on a sphere of unit radius centered at the origin
SQUARE Subroutine
“square” is a nonlinear least squares routine derived from the IMSL BCLSF routine and the MINPACK LMDER routine; the Jacobian is estimated by finite differences and bounds can be specified for the variables to be refined
SUFFIX Subroutine
“suffix” checks a filename for the presence of an extension, and appends an extension and version if none is found
SUPERPOSE Program
“superpose” takes pairs of structures and superimposes them in the optimal least squares sense; it will attempt to match all atom pairs or only those specified by the user
SURFACE Subroutine
“surface” performs an analytical computation of the weighted solvent accessible surface area of each atom and the first derivatives of the area with respect to Cartesian coordinates
SURFACE1 Subroutine
“surface1” performs an analytical computation of the weighted solvent accessible surface area of each atom and the first derivatives of the area with respect to Cartesian coordinates
SURFATOM Subroutine
“surfatom” performs an analytical computation of the surface area of a specified atom; a simplified version of “surface”
SURFATOM1 Subroutine
“surfatom1” performs an analytical computation of the surface area and first derivatives with respect to Cartesian coordinates of a specified atom
SWITCH Subroutine
“switch” sets the coeffcients used by the fifth and seventh order polynomial switching functions for spherical cutoffs
SYMMETRY Subroutine
“symmetry” applies symmetry operators to the fractional coordinates of the asymmetric unit in order to generate the symmetry related atoms of the full unit cell
SYSTYZE Subroutine
“systyze” is an auxiliary routine for the analyze program that prints general information about the molecular system and the force field model
TABLE_FILL Subroutine
“table_fill” constructs an array which stores the spatial regions of the particle mesh Ewald grid with contributions from each site
TANGENT Subroutine
“tangent” finds the projected gradient on the synchronous transit path for a point along the transit pathway
TCGSWAP Subroutine
“tcgswap” switches two sets of induced dipole quantities for use with the TCG induced dipole solver
TCG_ALPHA12 Subroutine
“tcg_alpha12” computes source1 = alpha*source1 and source2 = alpha*source2
TCG_ALPHA22 Subroutine
“tcg_alpha22” computes result1 = alpha*source1 and result2 = alpha*source2
TCG_ALPHAQUAD Subroutine
“tcg_alphaquad” computes the quadratic form, <a*alpha*b>, where alpha is the diagonal atomic polarizability matrix
TCG_DOTPROD Subroutine
“tcg_dotprod” computes the dot product of two vectors of length n elements
TCG_RESOURCE Subroutine
“tcg_resource” sets the number of mutual induced dipole pairs based on the passed argument
TCG_T0 Subroutine
“tcg_t0” applies T matrix to ind/p, and returns v3d/p T = 1/alpha + Tu
TCG_UFIELD Subroutine
“tcg_ufield” applies -Tu to ind/p and returns v3d/p
TCG_UPDATE Subroutine
“tcg_update” computes pvec = alpha*rvec + beta*pvec; if the preconditioner is not used, then alpha = identity
TEMPER Subroutine
“temper” computes the instantaneous temperature and applies a thermostat via Berendsen or Bussi-Parrinello velocity scaling, Andersen stochastic collisions or Nose-Hoover chains; also uses Berendsen scaling for any iEL induced dipole variables
TEMPER2 Subroutine
“temper2” applies a velocity correction at the half time step as needed for the Nose-Hoover thermostat
TESTGRAD Program
“testgrad” computes and compares the analytical and numerical gradient vectors of the potential energy function with respect to Cartesian coordinates
TESTHESS Program
“testhess” computes and compares the analytical and numerical Hessian matrices of the potential energy function with respect to Cartesian coordinates
TESTPAIR Program
“testpair” performs a set of timing tests to compare the evaluation of potential energy and energy/gradient using different methods for finding pairwise neighbors
TESTPOL Program
“testpol” compares the induced dipoles from direct polarization, mutual SCF iterations, perturbation theory extrapolation (OPT), and truncated conjugate gradient (TCG) solvers
TESTROT Program
“testrot” computes and compares the analytical and numerical gradient vectors of the potential energy function with respect to rotatable torsional angles
TESTVIR Program
“testvir” computes the analytical internal virial and compares it to a numerical virial derived from the finite difference derivative of the energy with respect to lattice vectors
TIMER Program
“timer” measures the CPU time required for file reading and parameter assignment, potential energy computation, energy and gradient computation, and Hessian matrix evaluation
TIMEROT Program
“timerot” measures the CPU time required for file reading and parameter assignment, potential energy computation, energy and gradient over torsions, and torsional angle Hessian matrix evaluation
TNCG Subroutine
“tncg” implements a truncated Newton optimization algorithm in which a preconditioned linear conjugate gradient method is used to approximately solve Newton’s equations; special features include use of an explicit sparse Hessian or finite-difference gradient-Hessian products within the PCG iteration; the exact Newton search directions can be used optionally; by default the algorithm checks for negative curvature to prevent convergence to a stationary point having negative eigenvalues; if a saddle point is desired this test can be removed by disabling “negtest”
TNSOLVE Subroutine
“tnsolve” uses a linear conjugate gradient method to find an approximate solution to the set of linear equations represented in matrix form by Hp = -g (Newton’s equations)
TORFIT1 Function
“torfit1” is a service routine that computes the energy and gradient for a low storage BFGS optimization in Cartesian coordinate space
TORGUESS Subroutine
“torguess” set approximate torsion amplitude parameters based on atom type and connected atoms
TORPHASE Subroutine
“torphase” sets the n-fold amplitude and phase values for each torsion via sorting of the input parameters
TORQUE Subroutine
“torque” takes the torque values on a single site defined by a local coordinate frame and converts to Cartesian forces on the original site and sites specifying the local frame, also gives the x,y,z-force components needed for virial computation
TORSER Function
“torser” computes the torsional error function and its first derivatives with respect to the atomic Cartesian coordinates based on the deviation of specified torsional angles from desired values, the contained bond angles are also restrained to avoid a numerical instability
TORSFIT Program
“torsfit” refines torsional force field parameters based on a quantum mechanical potential surface and analytical gradient
TORSIONS Subroutine
“torsions” finds the total number of torsional angles and the numbers of the four atoms defining each torsional angle
TORUS Subroutine
“torus” sets a list of all of the temporary torus positions by testing for a torus between each atom and its neighbors
TOTERR Function
“toterr” is the error function and derivatives for a distance geometry embedding; it includes components from the distance bounds, hard sphere contacts, local geometry, chirality and torsional restraint errors
TRANSFORM Subroutine
“transform” diagonalizes the current basis vectors to produce trial roots for sliding block iterative matrix diagonalization
TRANSIT Function
“transit” evaluates the synchronous transit function and gradient; linear and quadratic transit paths are available
TRBASIS Subroutine
“trbasis” forms translation and rotation basis vectors used during vibrational analysis via block iterative diagonalization
TRIANGLE Subroutine
“triangle” smooths the upper and lower distance bounds via the triangle inequality using a full-matrix variant of the Floyd-Warshall shortest path algorithm; this routine is usually much slower than the sparse matrix shortest path methods in “geodesic” and “trifix”, and should be used only for comparison with answers generated by those routines
TRIFIX Subroutine
“trifix” rebuilds both the upper and lower distance bound matrices following tightening of one or both of the bounds between a specified pair of atoms, “p” and “q”, using a modification of Murchland’s shortest path update algorithm
TRIGGER Subroutine
“trigger” constructs a set of initial trial vectors for use during sliding block iterative matrix diagonalization
TRIMHEAD Subroutine
“trimhead” removes blank spaces before the first non-blank character in a text string by shifting the string to the left
TRIMTEXT Function
“trimtext” finds and returns the location of the last non-blank character before the first null character in an input text string; the function returns zero if no such character is found
TRIPLE Function
“triple” finds the triple product of three vectors; used as a service routine by the Connolly surface area and volume computation
TRUST Subroutine
“trust” updates the model trust region for a nonlinear least squares calculation based on ideas found in NL2SOL and Dennis and Schnabel’s book
UBUILD Subroutine
“ubuild” performs a complete rebuild of the polarization preconditioner neighbor list for all sites
UDIRECT1 Subroutine
“udirect1” computes the reciprocal space contribution of the permanent atomic multipole moments to the field
UDIRECT2A Subroutine
“udirect2a” computes the real space contribution of the permanent atomic multipole moments to the field via a double loop
UDIRECT2B Subroutine
“udirect2b” computes the real space contribution of the permanent atomic multipole moments to the field via a neighbor list
UFIELD0A Subroutine
“ufield0a” computes the mutual electrostatic field due to induced dipole moments via a double loop
UFIELD0B Subroutine
“ufield0b” computes the mutual electrostatic field due to induced dipole moments via a pair list
UFIELD0C Subroutine
“ufield0c” computes the mutual electrostatic field due to induced dipole moments via Ewald summation
UFIELD0D Subroutine
“ufield0d” computes the mutual electrostatic field due to induced dipole moments for use with with generalized Kirkwood implicit solvation
UFIELD0E Subroutine
“ufield0e” computes the mutual electrostatic field due to induced dipole moments via a Poisson-Boltzmann solver
UFIELDI Subroutine
“ufieldi” computes the electrostatic field due to intergroup induced dipole moments
ULIGHT Subroutine
“ulight” performs a complete rebuild of the polarization preconditioner pair neighbor list for all sites using the method of lights
ULIST Subroutine
“ulist” performs an update or a complete rebuild of the neighbor lists for the polarization preconditioner
ULSPRED Subroutine
“ulspred” uses standard extrapolation or a least squares fit to set coefficients of an induced dipole predictor polynomial
UMUTUAL1 Subroutine
“umutual1” computes the reciprocal space contribution of the induced atomic dipole moments to the field
UMUTUAL2A Subroutine
“umutual2a” computes the real space contribution of the induced atomic dipole moments to the field via a double loop
UMUTUAL2B Subroutine
“umutual2b” computes the real space contribution of the induced atomic dipole moments to the field via a neighbor list
UNITCELL Subroutine
“unitcell” gets the periodic boundary box size and related values from an external keyword file
UPCASE Subroutine
“upcase” converts a text string to all upper case letters
URYGUESS Function
“uryguess” sets approximate Urey-Bradley force constants based on atom type and connected atoms
USCALE0A Subroutine
“uscale0a” builds and applies a preconditioner for the conjugate gradient induced dipole solver using a double loop
USCALE0B Subroutine
“uscale0b” builds and applies a preconditioner for the conjugate gradient induced dipole solver using a neighbor pair list
VALENCE Program
“valence” refines force field parameters for valence terms based on a quantum mechanical optimized structure and frequencies
VALFIT1 Function
“valfit1” is a service routine that computes the RMS error and gradient for valence parameters fit to QM results
VALGUESS Subroutine
“valguess” sets approximate valence parameter values based on quantum mechanical structure and frequency data
VALMIN1 Function
“valmin1” is a service routine that computes the molecular energy and gradient during valence parameter optimization
VALRMS Function
“valrms” evaluates a valence parameter goodness-of-fit error function based on comparison of forces, frequencies, bond lengths and angles to QM results
VAM Subroutine
“vam” takes the analytical molecular surface defined as a collection of spherical and toroidal polygons and uses it to compute the volume and surface area
VARPRM Subroutine
“varprm” copies the current optimization values into the corresponding electrostatic potential energy parameters
VARPRM Subroutine
“varprm” copies the current optimization values into the corresponding valence potential energy parameters
VBUILD Subroutine
“vbuild” performs a complete rebuild of the van der Waals pair neighbor list for all sites
VCROSS Subroutine
“vcross” finds the cross product of two vectors
VDWERR Function
“vdwerr” is the hard sphere van der Waals bound error function and derivatives that penalizes close nonbonded contacts, pairwise neighbors are generated via the method of lights
VDWGUESS Subroutine
“vdwguess” sets initial VDW parameters based on atom type and connected atoms
VECANG Function
“vecang” finds the angle between two vectors handed with respect to a coordinate axis; returns an angle in the range [0,2*pi]
VERLET Subroutine
“verlet” performs a single molecular dynamics time step via the velocity Verlet multistep recursion formula
VERSION Subroutine
“version” checks the name of a file about to be opened; if if “old” status is passed, the name of the highest current version is returned; if “new” status is passed the filename of the next available unused version is generated
VIBBIG Program
“vibbig” performs large-scale vibrational mode analysis using only vector storage and gradient evaluations; preconditioning is via an approximate inverse from a block diagonal Hessian, and a sliding block method is used to converge any number of eigenvectors starting from either lowest or highest frequency
VIBRATE Program
“vibrate” performs a vibrational normal mode analysis; the Hessian matrix of second derivatives is determined and then diagonalized both directly and after mass weighting; output consists of the eigenvalues of the force constant matrix as well as the vibrational frequencies and displacements
VIBROT Program
“vibrot” computes the eigenvalues and eigenvectors of the torsional Hessian matrix
VIRIYZE Subroutine
“propyze” finds and prints the internal virial, the dE/dV value and an estimate of the pressure
VLIGHT Subroutine
“vlight” performs a complete rebuild of the van der Waals pair neighbor list for all sites using the method of lights
VLIST Subroutine
“vlist” performs an update or a complete rebuild of the nonbonded neighbor lists for vdw sites
VNORM Subroutine
“vnorm” normalizes a vector to unit length; used as a service routine by the Connolly surface area and volume computation
VOLUME Subroutine
“volume” calculates the excluded volume via the Connolly analytical volume and surface area algorithm
VOLUME1 Subroutine
“volume1” calculates first derivatives of the total excluded volume with respect to the Cartesian coordinates of each atom
VOLUME2 Subroutine
“volume2” calculates second derivatives of the total excluded volume with respect to the Cartesian coordinates of the atoms
WATSON Subroutine
“watson” uses a rigid body optimization to approximately align the paired strands of a nucleic acid double helix
WATSON1 Function
“watson1” is a service routine that computes the energy and gradient for optimally conditioned variable metric optimization of rigid bodies
WIGGLE Subroutine
“wiggle” applies a random perturbation to the atomic coordinates to avoid numerical instabilities for various linear, planar and symmetric structures
XTALERR Subroutine
“xtalerr” computes an error function value derived from lattice energies, dimer intermolecular energies and the gradient with respect to structural parameters
XTALFIT Program
“xtalfit” determines optimized van der Waals and electrostatic parameters by fitting to crystal structures, lattice energies, and dimer structures and interaction energies
XTALMIN Program
“xtalmin” performs a full crystal energy minimization by optimizing over fractional atomic coordinates and the six lattice lengths and angles
XTALMIN1 Function
“xtalmin1” is a service routine that computes the energy and gradient with respect to fractional coordinates and lattice dimensions for a crystal energy minimization
XTALMOVE Subroutine
“xtalmove” converts fractional to Cartesian coordinates for rigid molecules during optimization of force field parameters
XTALPRM Subroutine
“xtalprm” stores or retrieves a molecular structure; used to make a previously stored structure the active structure, or to store a structure for later use
XTALWRT Subroutine
“xtalwrt” prints intermediate results during fitting of force field parameters to structures and energies
XYZATM Subroutine
“xyzatm” computes the Cartesian coordinates of a single atom from its defining internal coordinate values
XYZEDIT Program
“xyzedit” provides for modification and manipulation of the contents of Cartesian coordinates files
XYZINT Program
“xyzint” takes as input a Cartesian coordinates file, then converts to and writes out an internal coordinates file
XYZMOL2 Program
“xyzmol2” takes as input a Cartesian coordinates file, converts to and then writes out a Tripos MOL2 file
XYZPDB Program
“xyzpdb” takes as input a Cartesian coordinates file, then converts to and writes out a Protein Data Bank file
XYZRIGID Subroutine
“xyzrigid” computes the center of mass and Euler angle rigid body coordinates for each atom group in the system
ZATOM Subroutine
“zatom” adds an atom to the end of the current Z-matrix and then increments the atom counter; atom type, defining atoms and internal coordinates are passed as arguments
ZHELP Subroutine
“zhelp” prints the general information and instructions for the Z-matrix editing program
ZVALUE Subroutine
“zvalue” gets user supplied values for selected coordinates as needed by the internal coordinate editing program