Created
December 17, 2018 10:13
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import matplotlib.pyplot as plt | |
import numpy as np | |
class CubicKernel: | |
def __init__(self, dim): | |
self.dim = dim | |
if dim == 1: | |
self.sigma = 2. / 3. | |
elif dim == 1: | |
self.sigma = 10. * 0.5 * 1. / np.pi | |
def get_wij(self, rij, h): | |
frac_1_h = 1. / h | |
q = rij * frac_1_h | |
if q >= 0. and q < 1.: | |
tmp = 1. - 1.5 * q**2. + 0.75 * q**3. | |
elif q >= 1. and q < 2.: | |
tmp = 0.25 * (2. - q)**3. | |
else: | |
tmp = 0. | |
return tmp * self.sigma * frac_1_h**self.dim | |
def get_dwij(self, xij, dwij, rij, h): | |
if rij > 1e-12: | |
frac_1_h = 1. / h | |
q = rij * frac_1_h | |
if q > 2.: | |
tmp = 0. | |
elif q > 1. and q <= 2.: | |
tmp = - 0.75 * frac_1_h * (2. - q)**(2.) | |
else: | |
tmp = - 0.75 * frac_1_h * (4. * q - 3. * q**(2.)) | |
dw_drij = tmp * self.sigma * frac_1_h**(self.dim) | |
# xij is x_i - x_j | |
dwij[0] = dw_drij * xij[0] * 1. / rij | |
dwij[1] = dw_drij * xij[1] * 1. / rij | |
else: | |
dwij[0] = 0. | |
dwij[1] = 0. | |
def get_wij(rng, h): | |
ck = CubicKernel(1) | |
wij = np.zeros_like(rng) | |
for i in range(len(rng)): | |
rij = abs(rng[i]) | |
wij[i] = ck.get_wij(rij, 1.) | |
return wij | |
def get_dwij(rng, h): | |
ck = CubicKernel(1) | |
dwij_array = np.zeros_like(rng) | |
dwij = [0., 0.] | |
for i in range(len(rng)): | |
rij = abs(rng[i]) | |
xij = [-rng[i], 0.] | |
ck.get_dwij(xij, dwij, rij, 1.) | |
dwij_array[i] = dwij[0] | |
return dwij_array | |
def sin_aproximation(pos, kernel): | |
spacing = pos[2] - pos[1] | |
h = np.ones_like(pos) * spacing * 1.2 | |
sin_actual = np.sin(pos) | |
sin_sph = np.zeros_like(pos) | |
for i in range(len(pos)): | |
for j in range(len(pos)): | |
# position between particles | |
rij = abs(pos[i] - pos[j]) | |
sin_sph[i] += sin_actual[j] * kernel.get_wij(rij, h[i]) * spacing | |
return sin_sph, sin_actual | |
def sin_deriv_aproximation(pos, kernel): | |
spacing = pos[2] - pos[1] | |
h = np.ones_like(pos) * spacing * 1.2 | |
sin_actual = np.sin(pos) | |
sin_deriv_actual = np.cos(pos) | |
sin_deriv_sph = np.zeros_like(pos) | |
for i in range(len(pos)): | |
dwij = [0., 0.] | |
for j in range(len(pos)): | |
# position between particles | |
rij = abs(pos[i] - pos[j]) | |
xij = [(pos[i] - pos[j]), 0.] | |
kernel.get_dwij(xij, dwij, rij, h[i]) | |
sin_deriv_sph[i] += sin_actual[j] * dwij[0] * spacing | |
return sin_deriv_sph, sin_deriv_actual | |
def plot_kernel(): | |
rng = np.linspace(-3., 3., 100) | |
wij = get_wij(rng, 1.) | |
plt.plot(rng, wij) | |
plt.show() | |
def plot_deriv_kernel(): | |
rng = np.linspace(-3., 3., 100) | |
dwij = get_dwij(rng, 1.) | |
plt.plot(rng, dwij) | |
plt.show() | |
def plot_sin(): | |
ck = CubicKernel(1) | |
x = np.linspace(-np.pi, np.pi, 100) | |
sin_sph, sin_actual = sin_aproximation(x, ck) | |
plt.plot(x, sin_actual) | |
plt.plot(x, sin_sph) | |
plt.show() | |
def plot_deriv_sin(): | |
ck = CubicKernel(1) | |
x = np.linspace(-np.pi, np.pi, 1000) | |
sin_deriv_sph, sin_actual = sin_deriv_aproximation(x, ck) | |
plt.plot(x, sin_actual) | |
plt.plot(x, sin_deriv_sph) | |
plt.show() | |
def main(): | |
# plot_kernel() | |
# plot_deriv_kernel() | |
# plot_sin() | |
plot_deriv_sin() | |
if __name__ == '__main__': | |
main() |
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