Source code for imod.wq.adv

import textwrap

from imod.wq.pkgbase import Package


[docs] class AdvectionFiniteDifference(Package): """ Solve the advection term using the explicit Finite Difference method (MIXELM = 0) with upstream weighting Attributes ---------- courant: float Courant number (PERCEL) is the number of cells (or a fraction of a cell) advection will be allowed in any direction in one transport step. For implicit finite-difference or particle tracking based schemes, there is no limit on PERCEL, but for accuracy reasons, it is generally not set much greater than one. Note, however, that the PERCEL limit is checked over the entire model grid. Thus, even if PERCEL > 1, advection may not be more than one cell’s length at most model locations. For the explicit finite-difference, PERCEL is also a stability constraint, which must not exceed one and will be automatically reset to one if a value greater than one is specified. weighting : string {"upstream", "central"}, optional Indication of which weighting scheme should be used, set to default value "upstream" (NADVFD = 0 or 1) Default value: "upstream" """ _pkg_id = "adv" _keywords = {"weighting": {"upstream": 0, "central": 1}} _template = ( "[adv]\n" " mixelm = 0\n" " percel = {courant}\n" " nadvfd = {weighting}\n" )
[docs] def __init__(self, courant=0.75, weighting="upstream"): super().__init__() self["courant"] = courant self["weighting"] = weighting
def _pkgcheck(self, ibound=None): self._check_positive(["courant"])
[docs] class AdvectionMOC(Package): """ Solve the advection term using the Method of Characteristics (MIXELM = 1) Nota bene: number of particles settings have not been tested. The defaults here are chosen conservatively, with many particles. This increases both memory usage and computational effort. Attributes ----------- courant: float Courant number (PERCEL) is the number of cells (or a fraction of a cell) advection will be allowed in any direction in one transport step. For implicit finite-difference or particle tracking based schemes, there is no limit on PERCEL, but for accuracy reasons, it is generally not set much greater than one. Note, however, that the PERCEL limit is checked over the entire model grid. Thus, even if PERCEL > 1, advection may not be more than one cell’s length at most model locations. For the explicit finite-difference, PERCEL is also a stability constraint, which must not exceed one and will be automatically reset to one if a value greater than one is specified. max_nparticles: int is the maximum total number of moving particles allowed (MXPART). tracking: string {"euler", "runge-kutta", "hybrid"}, optional indicates which particle tracking algorithm is selected for the Eulerian-Lagrangian methods. ITRACK = 1, the first-order Euler algorithm is used; ITRACK = 2, the fourth-order Runge-Kutta algorithm is used; this option is computationally demanding and may be needed only when PERCEL is set greater than one. ITRACK = 3, the hybrid 1st and 4th order algorithm is used; the Runge- Kutta algorithm is used in sink/source cells and the cells next to sinks/sources while the Euler algorithm is used elsewhere. Default value is "hybrid". weighting_factor: float, optional is a concentration weighting factor (WD) between 0.5 and 1. It is used for operator splitting in the particle tracking based methods. The value of 0.5 is generally adequate. The value may be adjusted to achieve better mass balance. Generally, it can be increased toward 1.0 as advection becomes more dominant. Default value: 0.5. dconcentration_epsilon: float, optional is a small Relative Cell Concentration Gradient below which advective transport is considered negligible. A value around 10-5 is generally adequate. Default value: 1.0e-5. nplane: int, optional is a flag indicating whether the random or fixed pattern is selected for initial placement of moving particles. NPLANE = 0, the random pattern is selected for initial placement. Particles are distributed randomly in both the horizontal and vertical directions by calling a random number generator. This option is usually preferred and leads to smaller mass balance discrepancy in nonuniform or diverging/converging flow fields. NPLANE > 0, the fixed pattern is selected for initial placement. The value of NPLANE serves as the number of vertical "planes" on which initial particles are placed within each cell block. The fixed pattern may work better than the random pattern only in relatively uniform flow fields. For two-dimensional simulations in plan view, set NPLANE = 1. For cross sectional or three-dimensional simulations, NPLANE = 2 is normally adequate. Increase NPLANE if more resolution in the vertical direction is desired. Default value: 2. nparticles_no_advection: int, optional is number of initial particles per cell to be placed at cells where the Relative Cell Concentration Gradient is less than or equal to DCEPS. Generally, NPL can be set to zero since advection is considered insignificant when the Relative Cell Concentration Gradient is less than or equal to DCEPS. Setting NPL equal to NPH causes a uniform number of particles to be placed in every cell over the entire grid (i.e., the uniform approach). Default value: 10. nparticles_advection: int, optional is number of initial particles per cell to be placed at cells where the Relative Cell Concentration Gradient is greater than DCEPS. The selection of NPH depends on the nature of the flow field and also the computer memory limitation. Generally, use a smaller number in relatively uniform flow fields and a larger number in relatively nonuniform flow fields. However, values exceeding 16 in twodimensional simulation or 32 in three-dimensional simulation are rarely necessary. If the random pattern is chosen, NPH particles are randomly distributed within the cell block. If the fixed pattern is chosen, NPH is divided by NPLANE to yield the number of particles to be placed per vertical plane. Default value: 40. cell_min_nparticles: int, optional is the minimum number of particles allowed per cell. If the number of particles in a cell at the end of a transport step is fewer than NPMIN, new particles are inserted into that cell to maintain a sufficient number of particles. NPMIN can be set to zero in relatively uniform flow fields, and a number greater than zero in diverging/converging flow fields. Generally, a value between zero and four is adequate. Default value is 5. cell_max_nparticles: int, optional is the maximum number of particles allowed per cell. If the number of particles in a cell exceeds NPMAX, all particles are removed from that cell and replaced by a new set of particles equal to NPH to maintain mass balance. Generally, NPMAX can be set to approximately twice of NPH. Default value: 80. """ _pkg_id = "adv" _keywords = {"tracking": {"euler": 1, "runge-kutta": 2, "hybrid": 3}} _template = textwrap.dedent( """ [adv] mixelm = 1 percel = {courant} mxpart = {max_nparticles} itrack = {tracking} wd = {weighting_factor} dceps = {dconcentration_epsilon} nplane = {nplane} npl = {nparticles_no_advection} nph = {nparticles_advection} npmin = {cell_min_nparticles} npmax = {cell_max_nparticles} """ )
[docs] def __init__( self, courant=0.75, tracking="hybrid", weighting_factor=0.5, dconcentration_epsilon=1.0e-5, nplane=2, nparticles_no_advection=10, nparticles_advection=40, cell_min_nparticles=5, cell_max_nparticles=80, ): super().__init__() self["courant"] = courant self["tracking"] = tracking self["weighting_factor"] = weighting_factor self["dconcentration_epsilon"] = dconcentration_epsilon self["nplane"] = nplane self["nparticles_no_advection"] = nparticles_no_advection self["nparticles_advection"] = nparticles_advection self["cell_min_nparticles"] = cell_min_nparticles self["cell_max_nparticles"] = cell_max_nparticles
def _pkgcheck(self, ibound=None): self._check_positive(["courant", "weighting_factor"])
[docs] class AdvectionModifiedMOC(Package): """ Solve the advention term using the Modified Method of Characteristics (MIXELM = 2) Courant number (PERCEL) is the number of cells (or a fraction of a cell) advection will be allowed in any direction in one transport step. Attributes ---------- courant: float Courant number (PERCEL) is the number of cells (or a fraction of a cell) advection will be allowed in any direction in one transport step. For implicit finite-difference or particle tracking based schemes, there is no limit on PERCEL, but for accuracy reasons, it is generally not set much greater than one. Note, however, that the PERCEL limit is checked over the entire model grid. Thus, even if PERCEL > 1, advection may not be more than one cell’s length at most model locations. For the explicit finite-difference, PERCEL is also a stability constraint, which must not exceed one and will be automatically reset to one if a value greater than one is specified. tracking: string, {"euler", "runge-kutta", "hybrid"} indicates which particle tracking algorithm is selected for the Eulerian-Lagrangian methods. ITRACK = 1, the first-order Euler algorithm is used; ITRACK = 2, the fourth-order Runge-Kutta algorithm is used; this option is computationally demanding and may be needed only when PERCEL is set greater than one. ITRACK = 3, the hybrid 1st and 4th order algorithm is used; the Runge- Kutta algorithm is used in sink/source cells and the cells next to sinks/sources while the Euler algorithm is used elsewhere. weighting_factor: float is a concentration weighting factor (WD) between 0.5 and 1. It is used for operator splitting in the particle tracking based methods. The value of 0.5 is generally adequate. The value may be adjusted to achieve better mass balance. Generally, it can be increased toward 1.0 as advection becomes more dominant. dconcentration_epsilon: float, optional is a small Relative Cell Concentration Gradient (DCEPS) below which advective transport is considered negligible. A value around 1.0e-5 is generally adequate. Default value: 1.0e-5. sink_particle_placement: int indicates whether the random or fixed pattern is selected for initial placement of particles to approximate sink cells in the MMOC scheme. (NLSINK) sink_nparticles: int is the number of particles used to approximate sink cells in the MMOC scheme. (NPSINK) """ _pkg_id = "adv" _keywords = {"tracking": {"euler": 1, "runge-kutta": 2, "hybrid": 3}} _template = ( "[adv]\n" " mixelm = 2\n" " percel = {courant}\n" " itrack = {tracking}\n" " wd = {weighting_factor}\n" " interp = 1\n" " nlsink = {sink_particle_placement}\n" " npsink = {sink_nparticles}\n" )
[docs] def __init__( self, courant=1.0, tracking="hybrid", weighting_factor=0.5, dconcentration_epsilon=1.0e-5, sink_particle_placement=2, sink_nparticles=40, ): super().__init__() self["courant"] = courant self["tracking"] = tracking self["weighting_factor"] = weighting_factor self["sink_particle_placement"] = sink_particle_placement self["sink_nparticles"] = sink_nparticles
def _pkgcheck(self, ibound=None): self._check_positive(["courant", "weighting_factor"])
[docs] class AdvectionHybridMOC(Package): """ Hybrid Method of Characteristics and Modified Method of Characteristics with MOC or MMOC automatically and dynamically selected (MIXELM = 3) Attributes ---------- courant: float Courant number (PERCEL) is the number of cells (or a fraction of a cell) advection will be allowed in any direction in one transport step. For implicit finite-difference or particle tracking based schemes, there is no limit on PERCEL, but for accuracy reasons, it is generally not set much greater than one. Note, however, that the PERCEL limit is checked over the entire model grid. Thus, even if PERCEL > 1, advection may not be more than one cell’s length at most model locations. For the explicit finite-difference, PERCEL is also a stability constraint, which must not exceed one and will be automatically reset to one if a value greater than one is specified. max_particles: int is the maximum total number of moving particles allowed (MXPART). tracking: int indicates which particle tracking algorithm is selected for the Eulerian-Lagrangian methods. ITRACK = 1, the first-order Euler algorithm is used; ITRACK = 2, the fourth-order Runge-Kutta algorithm is used; this option is computationally demanding and may be needed only when PERCEL is set greater than one. ITRACK = 3, the hybrid 1st and 4th order algorithm is used; the Runge- Kutta algorithm is used in sink/source cells and the cells next to sinks/sources while the Euler algorithm is used elsewhere. weighting_factor: float is a concentration weighting factor (WD) between 0.5 and 1. It is used for operator splitting in the particle tracking based methods. The value of 0.5 is generally adequate. The value may be adjusted to achieve better mass balance. Generally, it can be increased toward 1.0 as advection becomes more dominant. dceps: float is a small Relative Cell Concentration Gradient below which advective transport is considered negligible. A value around 10-5 is generally adequate. nplane: int is a flag indicating whether the random or fixed pattern is selected for initial placement of moving particles. NPLANE = 0, the random pattern is selected for initial placement. Particles are distributed randomly in both the horizontal and vertical directions by calling a random number generator. This option is usually preferred and leads to smaller mass balance discrepancy in nonuniform or diverging/converging flow fields. NPLANE > 0, the fixed pattern is selected for initial placement. The value of NPLANE serves as the number of vertical "planes" on which initial particles are placed within each cell block. The fixed pattern may work better than the random pattern only in relatively uniform flow fields. For two-dimensional simulations in plan view, set NPLANE = 1. For cross sectional or three-dimensional simulations, NPLANE = 2 is normally adequate. Increase NPLANE if more resolution in the vertical direction is desired. npl: int is number of initial particles per cell to be placed at cells where the Relative Cell Concentration Gradient is less than or equal to DCEPS. Generally, NPL can be set to zero since advection is considered insignificant when the Relative Cell Concentration Gradient is less than or equal to DCEPS. Setting NPL equal to NPH causes a uniform number of particles to be placed in every cell over the entire grid (i.e., the uniform approach). nph: int is number of initial particles per cell to be placed at cells where the Relative Cell Concentration Gradient is greater than DCEPS. The selection of NPH depends on the nature of the flow field and also the computer memory limitation. Generally, use a smaller number in relatively uniform flow fields and a larger number in relatively nonuniform flow fields. However, values exceeding 16 in twodimensional simulation or 32 in three-dimensional simulation are rarely necessary. If the random pattern is chosen, NPH particles are randomly distributed within the cell block. If the fixed pattern is chosen, NPH is divided by NPLANE to yield the number of particles to be placed per vertical plane. npmin: int is the minimum number of particles allowed per cell. If the number of particles in a cell at the end of a transport step is fewer than NPMIN, new particles are inserted into that cell to maintain a sufficient number of particles. NPMIN can be set to zero in relatively uniform flow fields, and a number greater than zero in diverging/converging flow fields. Generally, a value between zero and four is adequate. npmax: int is the maximum number of particles allowed per cell. If the number of particles in a cell exceeds NPMAX, all particles are removed from that cell and replaced by a new set of particles equal to NPH to maintain mass balance. Generally, NPMAX can be set to approximately twice of NPH. dchmoc: real is the critical Relative Concentration Gradient for controlling the selective use of either MOC or MMOC in the HMOC solution scheme. The MOC solution is selected at cells where the Relative Concentration Gradient is greater than DCHMOC; The MMOC solution is selected at cells where the Relative Concentration Gradient is less than or equal to DCHMOC """ _pkg_id = "adv"
[docs] def __init__( self, courant=0.75, tracking="hybrid", weighting_factor=0.5, dconcentration_epsilon=1.0e-5, nplane=2, nparticles_no_advection=10, nparticles_advection=40, cell_min_nparticles=5, cell_max_nparticles=80, sink_particle_placement=2, sink_nparticles=40, dconcentration_hybrid=1.0e-4, ): super().__init__() self["courant"] = courant self["tracking"] = tracking self["weighting_factor"] = weighting_factor self["dconcentration_epsilon"] = dconcentration_epsilon self["nplane"] = nplane self["nparticles_no_advection"] = nparticles_no_advection self["nparticles_advection"] = nparticles_advection self["cell_min_nparticles"] = cell_min_nparticles self["cell_max_nparticles"] = cell_max_nparticles self["sink_particle_placement"] = sink_particle_placement self["sink_nparticles"] = sink_nparticles self["dconcentration_hybrid"] = dconcentration_hybrid
def _pkgcheck(self, ibound=None): self._check_positive(["courant", "weighting_factor"])
[docs] class AdvectionTVD(Package): """ Total Variation Diminishing (TVD) formulation (ULTIMATE, MIXELM = -1). Attributes ---------- courant : float Courant number (PERCEL) is the number of cells (or a fraction of a cell) advection will be allowed in any direction in one transport step. For implicit finite-difference or particle tracking based schemes, there is no limit on PERCEL, but for accuracy reasons, it is generally not set much greater than one. Note, however, that the PERCEL limit is checked over the entire model grid. Thus, even if PERCEL > 1, advection may not be more than one cell’s length at most model locations. For the explicit finite-difference, PERCEL is also a stability constraint, which must not exceed one and will be automatically reset to one if a value greater than one is specified. """ _pkg_id = "adv" _template = "[adv]\n" " mixelm = -1\n" " percel = {courant}\n"
[docs] def __init__(self, courant=0.75): super().__init__() self["courant"] = courant
def _pkgcheck(self, ibound=None): self._check_positive(["courant"])