mirror of
https://github.com/smyalygames/FiniteVolumeGPU.git
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198 lines
7.3 KiB
Python
198 lines
7.3 KiB
Python
# -*- coding: utf-8 -*-
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"""
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This python module implements the classical Lax-Friedrichs numerical
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scheme for the shallow water equations
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Copyright (C) 2016 SINTEF ICT
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This program is free software: you can redistribute it and/or modify
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it under the terms of the GNU General Public License as published by
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the Free Software Foundation, either version 3 of the License, or
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(at your option) any later version.
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This program is distributed in the hope that it will be useful,
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but WITHOUT ANY WARRANTY; without even the implied warranty of
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MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
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GNU General Public License for more details.
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You should have received a copy of the GNU General Public License
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along with this program. If not, see <http://www.gnu.org/licenses/>.
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"""
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#Import packages we need
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import numpy as np
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import logging
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import pycuda.compiler as cuda_compiler
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import pycuda.gpuarray
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import pycuda.driver as cuda
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from GPUSimulators import Common
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class BaseSimulator:
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"""
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Initialization routine
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context: GPU context to use
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kernel_wrapper: wrapper function of GPU kernel
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h0: Water depth incl ghost cells, (nx+1)*(ny+1) cells
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hu0: Initial momentum along x-axis incl ghost cells, (nx+1)*(ny+1) cells
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hv0: Initial momentum along y-axis incl ghost cells, (nx+1)*(ny+1) cells
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nx: Number of cells along x-axis
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ny: Number of cells along y-axis
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dx: Grid cell spacing along x-axis (20 000 m)
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dy: Grid cell spacing along y-axis (20 000 m)
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dt: Size of each timestep (90 s)
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g: Gravitational accelleration (9.81 m/s^2)
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"""
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def __init__(self, \
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context, \
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h0, hu0, hv0, \
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nx, ny, \
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ghost_cells_x, ghost_cells_y, \
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dx, dy, dt, \
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g, \
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block_width, block_height):
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#Get logger
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self.logger = logging.getLogger(__name__ + "." + self.__class__.__name__)
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self.context = context
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if (self.context.autotuner):
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peak_configuration = self.context.autotuner.get_peak_performance(self.__class__)
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block_width = int(peak_configuration["block_width"])
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block_height = int(peak_configuration["block_height"])
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self.logger.debug("Used autotuning to get block size [%d x %d]", block_width, block_height)
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#Create a CUDA stream
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self.stream = cuda.Stream()
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#Create data by uploading to device
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self.data = Common.SWEDataArakawaA(self.stream, \
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nx, ny, \
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ghost_cells_x, ghost_cells_y, \
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h0, hu0, hv0)
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#Save input parameters
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#Notice that we need to specify them in the correct dataformat for the
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#GPU kernel
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self.nx = np.int32(nx)
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self.ny = np.int32(ny)
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self.dx = np.float32(dx)
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self.dy = np.float32(dy)
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self.dt = np.float32(dt)
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self.g = np.float32(g)
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#Keep track of simulation time
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self.t = 0.0;
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#Compute kernel launch parameters
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self.local_size = (block_width, block_height, 1)
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self.global_size = ( \
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int(np.ceil(self.nx / float(self.local_size[0]))), \
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int(np.ceil(self.ny / float(self.local_size[1]))) \
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)
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"""
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Function which simulates forward in time using the default simulation type
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"""
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def simulate(self, t_end):
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raise(exceptions.NotImplementedError("Needs to be implemented in subclass"))
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"""
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Function which simulates t_end seconds using forward Euler
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Requires that the stepEuler functionality is implemented in the subclasses
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"""
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def simulateEuler(self, t_end):
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with Common.Timer(self.__class__.__name__ + ".simulateEuler") as t:
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# Compute number of timesteps to perform
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n = int(t_end / self.dt + 1)
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for i in range(0, n):
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# Compute timestep for "this" iteration
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local_dt = np.float32(min(self.dt, t_end-i*self.dt))
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# Stop if end reached (should not happen)
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if (local_dt <= 0.0):
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break
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# Step with forward Euler
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self.stepEuler(local_dt)
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self.logger.info("%s simulated %f seconds to %f with %d steps in %f seconds", self.__class__.__name__, t_end, self.t, n, t.secs)
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return self.t, n
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"""
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Function which simulates t_end seconds using Runge-Kutta 2
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Requires that the stepRK functionality is implemented in the subclasses
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"""
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def simulateRK(self, t_end, order):
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with Common.Timer(self.__class__.__name__ + ".simulateRK") as t:
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# Compute number of timesteps to perform
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n = int(t_end / self.dt + 1)
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for i in range(0, n):
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# Compute timestep for "this" iteration
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local_dt = np.float32(min(self.dt, t_end-i*self.dt))
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# Stop if end reached (should not happen)
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if (local_dt <= 0.0):
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break
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# Perform all the Runge-Kutta substeps
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self.stepRK(local_dt, order)
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self.logger.info("%s simulated %f seconds to %f with %d steps in %f seconds", self.__class__.__name__, t_end, self.t, n, t.secs)
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return self.t, n
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"""
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Function which simulates t_end seconds using second order dimensional splitting (XYYX)
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Requires that the stepDimsplitX and stepDimsplitY functionality is implemented in the subclasses
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"""
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def simulateDimsplit(self, t_end):
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with Common.Timer(self.__class__.__name__ + ".simulateDimsplit") as t:
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# Compute number of timesteps to perform
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n = int(t_end / (2.0*self.dt) + 1)
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for i in range(0, n):
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# Compute timestep for "this" iteration
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local_dt = np.float32(0.5*min(2*self.dt, t_end-2*i*self.dt))
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# Stop if end reached (should not happen)
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if (local_dt <= 0.0):
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break
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# Perform the dimensional split substeps
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self.stepDimsplitXY(local_dt)
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self.stepDimsplitYX(local_dt)
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self.logger.info("%s simulated %f seconds to %f with %d steps in %f seconds", self.__class__.__name__, t_end, self.t, 2*n, t.secs)
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return self.t, 2*n
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"""
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Function which performs one single timestep of size dt using forward euler
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"""
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def stepEuler(self, dt):
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raise(NotImplementedError("Needs to be implemented in subclass"))
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def stepRK(self, dt, substep):
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raise(NotImplementedError("Needs to be implemented in subclass"))
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def stepDimsplitXY(self, dt):
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raise(NotImplementedError("Needs to be implemented in subclass"))
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def stepDimsplitYX(self, dt):
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raise(NotImplementedError("Needs to be implemented in subclass"))
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def sim_time(self):
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return self.t
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def download(self):
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return self.data.download(self.stream)
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def synchronize(self):
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self.stream.synchronize()
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