Created
May 20, 2016 04:25
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from __future__ import division | |
import numpy as np | |
import matplotlib.pyplot as plt | |
from copy import copy | |
""" | |
This script draws the Gosper island, a hexagon-based fractal that tiles the plane. | |
https://en.wikipedia.org/wiki/Gosper_curve#Properties | |
""" | |
n = 5 | |
def hexwalk(n): | |
if n == 1: | |
return 'FR'*6 | |
return hexwalk(n-1).replace('F', 'FRFLF') | |
radius = 100. | |
mass = 1. | |
step_size = radius / 7**(.5*(n-1)) | |
cur_angle = 0.0 | |
cur_pos = np.array([0.0, 0.0]) | |
my_positions = [] | |
positions = [] | |
for char in hexwalk(n): | |
if char == 'F': | |
cur_pos += np.array([step_size*np.cos(cur_angle), step_size*np.sin(cur_angle)]) | |
elif char == 'R': | |
cur_angle -= np.radians(60.0) | |
elif char == 'L': | |
cur_angle += np.radians(60.0) | |
my_positions.append(copy(cur_pos)) | |
my_positions = np.vstack(my_positions) | |
plt.plot(my_positions[:, 0], my_positions[:, 1]) | |
plt.show() | |
unique_positions = [] | |
cur_row = None | |
for row in my_positions: | |
if cur_row is None: | |
cur_row = row | |
unique_positions.append(row) | |
else: | |
if (row == cur_row).all(): | |
continue | |
else: | |
unique_positions.append(row) | |
cur_row = row | |
unique_positions = np.vstack(unique_positions) | |
unique_positions -= np.sum(unique_positions, axis=0)/unique_positions.shape[0] | |
#angles = np.linspace(-np.pi, np.pi, 200) | |
#unique_positions = np.vstack((radius*np.cos(angles), radius*np.sin(angles))).T | |
plt.plot(unique_positions[:, 0], unique_positions[:, 1]) | |
plt.show() | |
def rot(theta): | |
return np.array([[np.cos(theta), -np.sin(theta)], [np.sin(theta), np.cos(theta)]]) | |
def inertia_triangle(p1, p2): | |
"""Polar inertia around the z axis for a triangle formed by p1, p2 and the | |
origin """ | |
a = np.linalg.norm(p2 - p1) | |
b = np.linalg.norm(p1) | |
c = np.linalg.norm(p2) | |
return -1/48*np.sqrt(-(a-b-c)*(a+b-c)*(a-b+c)*(a+b+c))*(a**2-3*(b**2+c**2)) | |
def area_triangle(p1, p2): | |
a = np.linalg.norm(p2 - p1) | |
b = np.linalg.norm(p1) | |
c = np.linalg.norm(p2) | |
return 1/4*np.sqrt((a+b+c)*(b+c-a)*(c+a-b)*(a+b-c)) | |
inertia = 0 | |
area = 0 | |
for i in range(unique_positions.shape[0]): | |
#tri = plt.Polygon([np.array([0, 0]), unique_positions[i-1, :], unique_positions[i, :]]) | |
#fig = plt.figure() | |
#ax = fig.add_subplot(111) | |
#ax.plot(unique_positions[:, 0], unique_positions[:, 1]) | |
#ax.add_patch(tri) | |
#plt.show() | |
inertia += inertia_triangle(unique_positions[i-1, :], unique_positions[i, :]) | |
area += area_triangle(unique_positions[i-1, :], unique_positions[i, :]) | |
true_m = mass*radius**2.*3./4 | |
print("Radius : {}".format(radius)) | |
print("Total inertia: {}".format(inertia)) | |
print("Inertia/area : {}".format(inertia/area)) | |
print("Error: {}".format(abs((inertia/area - true_m)/true_m))) |
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