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  • __copyright__ = """
    Copyright (C) 2017 Bogdan Enache
    Copyright (C) 2021 University of Illinois Board of Trustees
    """
    
    
    __license__ = """
    Permission is hereby granted, free of charge, to any person obtaining a copy
    of this software and associated documentation files (the "Software"), to deal
    in the Software without restriction, including without limitation the rights
    to use, copy, modify, merge, publish, distribute, sublicense, and/or sell
    copies of the Software, and to permit persons to whom the Software is
    furnished to do so, subject to the following conditions:
    
    The above copyright notice and this permission notice shall be included in
    all copies or substantial portions of the Software.
    
    THE SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS OR
    IMPLIED, INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY,
    FITNESS FOR A PARTICULAR PURPOSE AND NONINFRINGEMENT. IN NO EVENT SHALL THE
    AUTHORS OR COPYRIGHT HOLDERS BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER
    LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING FROM,
    OUT OF OR IN CONNECTION WITH THE SOFTWARE OR THE USE OR OTHER DEALINGS IN
    THE SOFTWARE.
    """
    
    import logging
    
    import os
    
    import numpy as np
    
    import pyopencl as cl
    
    import pyopencl.tools as cl_tools
    
    from arraycontext import flatten
    
    from meshmode.mesh import BTAG_ALL
    
    from pytools.obj_array import flat_obj_array
    
    import grudge.dof_desc as dof_desc
    
    import grudge.op as op
    
    from grudge.array_context import PyOpenCLArrayContext
    
    
    logger = logging.getLogger(__name__)
    
    # {{{ plotting (keep in sync with `weak.py`)
    
    class Plotter:
    
        def __init__(self, actx, dcoll, order, visualize=True, ylim=None):
    
            self.actx = actx
    
            self.dim = dcoll.ambient_dim
    
    
            self.visualize = visualize
            if not self.visualize:
                return
    
            if self.dim == 1:
                import matplotlib.pyplot as pt
                self.fig = pt.figure(figsize=(8, 8), dpi=300)
    
                self.ylim = ylim
    
    
                volume_discr = dcoll.discr_from_dd(dof_desc.DD_VOLUME_ALL)
    
                self.x = actx.to_numpy(flatten(volume_discr.nodes()[0], self.actx))
    
            else:
                from grudge.shortcuts import make_visualizer
    
                self.vis = make_visualizer(dcoll)
    
        def __call__(self, evt, basename, overwrite=True):
    
            if not self.visualize:
                return
    
            if self.dim == 1:
    
                u = self.actx.to_numpy(flatten(evt.state_component, self.actx))
    
                filename = f"{basename}.png"
    
                if not overwrite and os.path.exists(filename):
                    from meshmode import FileExistsError
    
                    raise FileExistsError(f"output file '{filename}' already exists")
    
                ax = self.fig.gca()
    
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                ax.plot(self.x, u, "-")
                ax.plot(self.x, u, "k.")
    
                if self.ylim is not None:
                    ax.set_ylim(self.ylim)
    
    
                ax.set_xlabel("$x$")
                ax.set_ylabel("$u$")
    
                ax.set_title(f"t = {evt.t:.2f}")
    
                self.fig.savefig(filename)
    
                self.vis.write_vtk_file(f"{basename}.vtu", [
    
                    ("u", evt.state_component)
    
                    ], overwrite=overwrite)
    
    def main(ctx_factory, dim=2, order=4, use_quad=False, visualize=False,
            flux_type="upwind"):
    
        cl_ctx = ctx_factory()
        queue = cl.CommandQueue(cl_ctx)
    
        actx = PyOpenCLArrayContext(
            queue,
    
            allocator=cl_tools.MemoryPool(cl_tools.ImmediateAllocator(queue)),
            force_device_scalars=True,
    
        # domain [0, d]^dim
        d = 1.0
        # number of points in each dimension
        npoints = 25
    
    
        if use_quad:
            qtag = dof_desc.DISCR_TAG_QUAD
    
        # {{{ discretization
    
        from meshmode.mesh.generation import generate_regular_rect_mesh
        mesh = generate_regular_rect_mesh(
                a=(0,)*dim, b=(d,)*dim,
    
                npoints_per_axis=(npoints,)*dim,
    
        from meshmode.discretization.poly_element import QuadratureSimplexGroupFactory
    
            discr_tag_to_group_factory = {
    
                qtag: QuadratureSimplexGroupFactory(order=4*order)
    
            discr_tag_to_group_factory = {}
    
        from grudge.discretization import make_discretization_collection
    
        dcoll = make_discretization_collection(
    
            actx, mesh, order=order,
            discr_tag_to_group_factory=discr_tag_to_group_factory
        )
    
        # {{{ advection operator
    
        # gaussian parameters
    
        def f_halfcircle(x):
            source_center = np.array([d/2, d/2, d/2])[:dim]
            dist = x - source_center
            return (
                    (0.5+0.5*actx.np.tanh(500*(-np.dot(dist, dist) + 0.4**2)))
                    * (0.5+0.5*actx.np.tanh(500*(dist[0]))))
    
        def zero_inflow_bc(dtag, t=0):
    
            dd = dof_desc.as_dofdesc(dtag, qtag)
    
            return dcoll.discr_from_dd(dd).zeros(actx)
    
        from grudge.models.advection import VariableCoefficientAdvectionOperator
    
        x = actx.thaw(dcoll.nodes())
    
    
        # velocity field
        if dim == 1:
            c = x
        else:
            # solid body rotation
            c = flat_obj_array(
                np.pi * (d/2 - x[1]),
                np.pi * (x[0] - d/2),
                0
            )[:dim]
    
        adv_operator = VariableCoefficientAdvectionOperator(
            dcoll,
            c,
            inflow_u=lambda t: zero_inflow_bc(BTAG_ALL, t),
            quad_tag=qtag,
            flux_type=flux_type
        )
    
    
    
        def rhs(t, u):
    
            return adv_operator.operator(t, u)
    
        dt = actx.to_numpy(adv_operator.estimate_rk4_timestep(actx, dcoll, fields=u))
    
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        logger.info("Timestep size: %g", dt)
    
    
    
        from grudge.shortcuts import set_up_rk4
    
        dt_stepper = set_up_rk4("u", float(dt), u, rhs)
    
        plot = Plotter(actx, dcoll, order, visualize=visualize,
    
                ylim=[-0.1, 1.1])
    
        for event in dt_stepper.run(t_end=final_time):
            if not isinstance(event, dt_stepper.StateComputed):
                continue
    
                norm_u = actx.to_numpy(op.norm(dcoll, event.state_component, 2))
    
                plot(event, "fld-var-velocity-%04d" % step)
    
                logger.info("[%04d] t = %.5f |u| = %.5e", step, event.t, norm_u)
                # NOTE: These are here to ensure the solution is bounded for the
                # time interval specified
                assert norm_u < 1
    
    
    
    if __name__ == "__main__":
    
        import argparse
    
        parser = argparse.ArgumentParser()
        parser.add_argument("--dim", default=2, type=int)
    
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        parser.add_argument("--order", default=4, type=int)
    
        parser.add_argument("--use-quad", action="store_true")
        parser.add_argument("--visualize", action="store_true")
    
        parser.add_argument("--flux", default="upwind",
                help="'central' or 'upwind'. Run with central to observe aliasing "
                "instability. Add --use-quad to fix that instability.")
    
        args = parser.parse_args()
    
        logging.basicConfig(level=logging.INFO)
        main(cl.create_some_context,
    
             dim=args.dim,
    
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             order=args.order,
    
             use_quad=args.use_quad,
    
             visualize=args.visualize,
             flux_type=args.flux)