Beispiel #1
0
def sample(C_si, C_rel):
    # Imports
    import sir_ddft
    import numpy as np
    from numpy import pi, sqrt
    from dispy.dispynode import dispynode_logger

    # Constants
    NUM_THREADS = 2
    DT = 0.1
    MIN_TIME = 10
    TIMEOUT = 400
    THRESHOLD = 1e-4

    # Use model parameters from original publication
    C_sd = C_si / C_rel
    L = 10
    N = 512  # Powers of 2 are favorable for the internal FFT
    dx = L / N
    params = sir_ddft.SIRParameters(1.0, 0.1)
    diff_params = sir_ddft.SIRDiffusionParameters(0.01, 0.01, 0.01)
    ddft_params = sir_ddft.SIRDDFTParameters(1.0, 1.0, 1.0, C_sd, 100, C_si,
                                             100)
    x = np.linspace(0, L, N, endpoint=False) + dx / 2
    x, y = np.meshgrid(x, x)
    S = lambda x, y: np.exp(-1 / (L * 2.0 * L / 50.0) * ((x - L / 2)**2 +
                                                         (y - L / 2)**2))
    norm_fac = N**2 / np.sum(S(x, y)) * sqrt(pi) / 5
    S = lambda x, y, S=S: S(x, y) * norm_fac
    I = lambda x, y: 0.001 * S(x, y)
    total_SIR = np.sum(S(x, y) + I(x, y)) * dx * dx  # Total population

    # Create initial state and solver
    grid = sir_ddft.Grid2D.new_equidistant(0, L, 0, L, N, N)
    state = sir_ddft.SIRStateSpatial2D(
        grid, lambda x, y: [S(x, y), I(x, y), 0.0])
    solver = sir_ddft.SIRDDFT2DSolver(params, diff_params, ddft_params, state,
                                      NUM_THREADS)

    t = []
    S = []
    I = []
    R = []

    def store_result(result):
        t.append(result["time"])
        S.append(np.sum(result["S"]) * dx * dx)
        I.append(np.sum(result["I"]) * dx * dx)
        R.append(np.sum(result["R"]) * dx * dx)

    store_result(solver.get_result())

    while t[-1] < MIN_TIME or (I[-1] / total_SIR > THRESHOLD
                               and t[-1] < TIMEOUT):
        solver.add_time(DT)
        solver.integrate()
        store_result(solver.get_result())
        dispynode_logger.info(t[-1])

    return (t, S, I, R)
Beispiel #2
0
import numpy as np
from numpy import pi, sqrt

import os, os.path
import sys
sys.path.append(os.path.abspath(os.path.join(__file__, "../../../target/release")))
import sir_ddft

from common_2d import run_sim

L=10
N=512
params = sir_ddft.SIRParameters(1.0,0.1)
diff_params = sir_ddft.SIRDiffusionParameters(0.01,0.01,0.01)
ddft_params = sir_ddft.SIRDDFTParameters(1.0,1.0,1.0,-10,100,-30,100)
grid = sir_ddft.Grid2D.new_equidistant(0,L,0,L,N,N)
S = lambda x,y: np.exp(-1/(L*2.0*L/50.0)*((x-L/2)**2 + (y-L/2)**2)) * 2.832
I = lambda x,y: 0.001*S(x,y)
state  = sir_ddft.SIRStateSpatial2D(grid, lambda x,y: [S(x,y),I(x,y),0.0])
solver = sir_ddft.SIRDDFT2DSolver(params, diff_params, ddft_params, state, 6)

run_sim(solver, 0.1, 200, "SIR DDFT model")
Beispiel #3
0
import numpy as np

import os, os.path
import sys
sys.path.append(
    os.path.abspath(os.path.join(__file__, "../../../target/release")))
import sir_ddft as sir_ddft

from common_1d import run_sim

params = sir_ddft.SIRParameters(0.5, 0.1)
diff_params = sir_ddft.SIRDiffusionParameters(0.01, 0.01, 0.01)
ddft_params = sir_ddft.SIRDDFTParameters(1.0, 1.0, 1.0, -5, 100, -10, 100)
grid = sir_ddft.Grid1D.new_equidistant(0, 1, 256)


def initfunc(x):
    variance = 50**(-2)
    S = np.exp(-(x - 0.5)**2 / (2 * variance)) / np.sqrt(2 * np.pi * variance)
    return [S, S * 0.001, 0.0]


state = sir_ddft.SIRStateSpatial1D(grid, initfunc)
solver = sir_ddft.SIRDDFT1DSolver(params, diff_params, ddft_params, state, 4)

run_sim(solver, 0.25, 400, "SIR DDFT model")