#include <BALL/SOLVATION/poissonBoltzmann.h>
Static Public Attributes | |
static const String | VERBOSITY |
static const String | PRINT_TIMING |
static const String | SPACING |
static const String | BORDER |
static const String | IONIC_STRENGTH |
static const String | SOLUTE_DC |
static const String | SOLVENT_DC |
static const String | PROBE_RADIUS |
static const String | ION_RADIUS |
static const String | TEMPERATURE |
static const String | BOUNDARY |
static const String | CHARGE_DISTRIBUTION |
static const String | DIELECTRIC_SMOOTHING |
static const String | OFFSET |
static const String | RMS_CRITERION |
static const String | MAX_CRITERION |
static const String | CHECK_AFTER_ITERATIONS |
static const String | MAX_ITERATIONS |
static const String | LOWER |
static const String | UPPER |
static const String | BOUNDING_BOX_LOWER |
static const String | BOUNDING_BOX_UPPER |
Symbolic names for option keys. This struct contains a symbolic name for each recognized key in FDPB::options.
Definition at line 216 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::BORDER [static] |
The border of the system. Use this option to define the aumount of space left between the bounding box of the solute and the border of the cubic grid in every direction. Use units of Angstrom with this option. The default is 4 A.
border | float |
Definition at line 255 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::BOUNDARY [static] |
Boundary condition for solving the differential equation. This parameter defines the type of boundary condition will be used for initializing the equation solver. Possible options are: zero, Debye, Coulomb, dipole and focusing. Default is dipole.
boundary_condition | String |
Definition at line 308 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::BOUNDING_BOX_LOWER [static] |
The lower corner of the bounding box of the solute molecule. This option works like
bounding_box_lower | Vector3 |
Definition at line 398 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::BOUNDING_BOX_UPPER [static] |
The upper corner of the bounding box of the solute molecule. This is the analogous option to
bounding_box_upper | Vector3 |
Definition at line 404 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::CHARGE_DISTRIBUTION [static] |
Charge distribution of the system. This parameter chooses the method used for distributing charges oiver grid points. Possible methods are: trilinear and uniform. The default is uniform.
border | float |
Definition at line 317 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::CHECK_AFTER_ITERATIONS [static] |
Checking frequency. This option defines the number of iterations which will be performed without checking the criterions. The default is 10.
check_after_iterations | int |
Definition at line 365 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::DIELECTRIC_SMOOTHING [static] |
Smoothing the dielectric constant. With this option you can choose a smoothing function for the dielectric thus permitting a smooth transition from the inside of the molecule (usually dc = 2.0) to the surrounding solvent (78.5). You have the followin options: none, uniform and harmonic. Default is none. different dielectric constant
dielectric_smoothing | String |
Definition at line 329 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::ION_RADIUS [static] |
The ion exclusion radius.
ion_radius | float |
Definition at line 292 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::IONIC_STRENGTH [static] |
The ionic strength of the salt solution This parameter defines the ionic strength of the salt solution in which the Poisson-Boltzmann calculation takes place. This parameter is given in units of mol/l. The default is 0, i. e. only a Poisson equation will be calculated.
ionic_strength | float |
Definition at line 265 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::LOWER [static] |
The lower corner of the grid. This option contains the lower corner of the grid. It can be used to fix it before setting up the solver. If this option was not used for initializing the solver gtrid it contains the automatically computed lower corner after the calculation. Use a vector of Angstroms with this option.
lower | Vector3 |
Definition at line 385 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::MAX_CRITERION [static] |
Define the MAX criterion. This option defines the upper limit for the residuals. If the maximum residuals are below this value and the RMS lies below rms_criterion, the iteration terminates. The default is 1e-4.
max_criterion | float |
Definition at line 357 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::MAX_ITERATIONS [static] |
The upper limit of iterations. Use this option to define the maximum number of iterations to be performed. If the solver does not terminate when this number of iterations is reached, the calculation did not converge. The default is 500 interations.
max_iterations | int |
Definition at line 375 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::OFFSET [static] |
Use an offset. This option allows to offset the wohle system by the vector defined in thos option. The calculation does not use an offset by default. Use threedimensional vectors in units of Angstrom with this option.
offset | Vector3 |
Definition at line 338 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::PRINT_TIMING [static] |
Print the timing for each step.
This prints the timing (if Option::verbosity > 1) of each setup routine and the time needed to solve the equations.
print_timing | bool |
Definition at line 236 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::PROBE_RADIUS [static] |
The probe radius used for calculating the SAS of the molecule. This parameter defaults to 1.4 A (water).
probe_radius | float |
Definition at line 286 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::RMS_CRITERION [static] |
Define the RMS criterion. This option defines the RMS criterion in Angstrom used for terminating the iteration of the solver. If the RMS lies below rms_criterion and the maximum residuals are below max_criterion, the iteration terminates. The default is 1e-5 Angstrom.
rms_criterion | float |
Definition at line 348 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::SOLUTE_DC [static] |
The dielectric constant of the solute. This parameter derfaults to 2.0.
solute_dielectric_constant | float |
Definition at line 272 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::SOLVENT_DC [static] |
The dielectric constant of the solvent. This parameter defaults to 78.0.
solvent_dielectric_constant | float |
Definition at line 279 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::SPACING [static] |
The grid spacing in Angstrom. Use this option to define the distance between a grid point and its closest neighbour in units o Angstrom. The default spacing is 0.6 A.
spacing | float |
Definition at line 245 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::TEMPERATURE [static] |
The temperature of the system. This parameter needs values in units of K. The default temperature is 298.15 K = 25.15 deg C.
temperature | float |
Definition at line 299 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::UPPER [static] |
The upper corner of the grid. This is the analogous option to
upper | Vector3 |
Definition at line 391 of file poissonBoltzmann.h.
const String BALL::FDPB::Option::VERBOSITY [static] |
The verbosity level. Use integer values with this option. 0 = terse
verbosity | integer |
Definition at line 225 of file poissonBoltzmann.h.