pyro.incompressible package#

The pyro solver for incompressible flow. This implements as second-order approximate projection method. The general flow is:

create the limited slopes of u and v (in both directions)
get the advective velocities through a piecewise linear Godunov method
enforce the divergence constraint on the velocities through a projection (the MAC projection)
recompute the interface states using the new advective velocity
update U in time to get the provisional velocity field
project the final velocity to enforce the divergence constraint.

The projections are done using multigrid

Subpackages#

pyro.incompressible.problems package

Submodules#

pyro.incompressible.incomp_interface module#

pyro.incompressible.incomp_interface.apply_gradp_corrections(dt, u_xl, u_xr, u_yl, u_yr, v_xl, v_xr, v_yl, v_yr, gradp_x, gradp_y)[source]#

Parameters:

gridGrid2d: The grid object
dtfloat: The timestep
u_xl, u_xrndarray ndarray: left and right states of x-velocity in x-interface.
u_yl, u_yrndarray ndarray: left and right states of x-velocity in y-interface.
v_xl, v_xrndarray ndarray: left and right states of y-velocity in x-interface.
v_yl, u_yrndarray ndarray: left and right states of y-velocity in y-interface.

Returns:

outndarray, ndarray, ndarray, ndarray, ndarray, ndarray, ndarray, ndarray: correct the interface states of the left and right states of u and v on both the x- and y-interfaces interface states with the pressure gradient terms.

pyro.incompressible.incomp_interface.apply_other_source_terms(dt, u_xl, u_xr, u_yl, u_yr, v_xl, v_xr, v_yl, v_yr, source_x, source_y)[source]#

Parameters:

gridGrid2d: The grid object
dtfloat: The timestep
u_xl, u_xrndarray ndarray: left and right states of x-velocity in x-interface.
u_yl, u_yrndarray ndarray: left and right states of x-velocity in y-interface.
v_xl, v_xrndarray ndarray: left and right states of y-velocity in x-interface.
v_yl, u_yrndarray ndarray: left and right states of y-velocity in y-interface.
source_x, source_yndarray: Any other source terms

Returns:

outndarray, ndarray, ndarray, ndarray, ndarray, ndarray, ndarray, ndarray: correct the interface states of the left and right states of u and v on both the x- and y-interfaces interface states with the source terms.

pyro.incompressible.incomp_interface.mac_vels(grid, dt, u, v, ldelta_ux, ldelta_vx, ldelta_uy, ldelta_vy, gradp_x, gradp_y, source_x=None, source_y=None)[source]#

Calculate the MAC velocities in the x and y directions.

Parameters:

gridGrid2d: The grid object
dtfloat: The timestep
u, vndarray: x-velocity and y-velocity
ldelta_ux, ldelta_uy: ndarray: Limited slopes of the x-velocity in the x and y directions
ldelta_vx, ldelta_vy: ndarray: Limited slopes of the y-velocity in the x and y directions
gradp_x, gradp_yndarray: Pressure gradients in the x and y directions
source_x, source_yndarray: Any other source terms

Returns:

outndarray, ndarray: MAC velocities in the x and y directions

pyro.incompressible.incomp_interface.states(grid, dt, u, v, ldelta_ux, ldelta_vx, ldelta_uy, ldelta_vy, gradp_x, gradp_y, u_MAC, v_MAC, source_x=None, source_y=None)[source]#

This is similar to mac_vels, but it predicts the interface states of both u and v on both interfaces, using the MAC velocities to do the upwinding.

Parameters:

gridGrid2d: The grid object
dtfloat: The timestep
u, vndarray: x-velocity and y-velocity
ldelta_ux, ldelta_uy: ndarray: Limited slopes of the x-velocity in the x and y directions
ldelta_vx, ldelta_vy: ndarray: Limited slopes of the y-velocity in the x and y directions
gradp_x, gradp_yndarray: Pressure gradients in the x and y directions
u_MAC, v_MACndarray: MAC velocities in the x and y directions
source_x, source_yndarray: Any other source terms

Returns:

outndarray, ndarray, ndarray, ndarray: x and y velocities predicted to the interfaces

pyro.incompressible.simulation module#

class pyro.incompressible.simulation.Simulation(solver_name, problem_name, problem_func, rp, *, problem_finalize_func=None, problem_source_func=None, timers=None, data_class=<class 'pyro.mesh.patch.CellCenterData2d'>)[source]#

Bases: Simulation

define_other_bc()[source]#: Used to set up user-defined BC’s (see e.g. incompressible_viscous)

do_other_update_velocity(U_MAC, U_INT)[source]#: Change the method for updating the velocity from the projected velocity and interface states (see e.g. incompressible_viscous)

dovis()[source]#: Do runtime visualization

evolve(other_update_velocity=False, other_source_term=False)[source]#: Evolve the incompressible equations through one timestep.

initialize(*, other_bc=False, aux_vars=())[source]#: Initialize the grid and variables for incompressible flow and set the initial conditions for the chosen problem.

other_source_term()[source]#: Add source terms (other than gradp) for getting interface state values, in the x and y directions

preevolve()[source]#: preevolve is called before we being the timestepping loop. For the incompressible solver, this does an initial projection on the velocity field and then goes through the full evolution to get the value of phi. The fluid state (u, v) is then reset to values before this evolve.

pyro.incompressible package

Contents

pyro.incompressible package#

Subpackages#

Submodules#

pyro.incompressible.incomp_interface module#

pyro.incompressible.simulation module#