In our scenario, we want to calculate the value of \pi. To do this, we''ll be throwing darts at a square dart board (dimensions : 1 by 1) with a quadrant (radius : 1) in it. After throwing a bunch of darts at the board, we'll find the ratio of the number of darts that end up inside the quadrant to the total number of darts we threw and then multiply that number by 4 to get an estimate for the value of \pi
Lets work through the math
4 \times \frac{A_{quadrant}}{A_{square}} = 4 \times \frac{\frac{1}{4}\pi r^{2}}{(1)^2} = 4 \times \frac{\frac{1}{4}\pi(1)^2}{(1)^2} = 4 \times \frac{\frac{1}{4}\pi}{1} \approx \frac{N_{hits}}{N_{trials}} \approx \pi
In our Monte Carlo simulation, we'll be sampling random points onto our 1 by 1 space and comparing the number of points that end up in the quadrant to the total number of points.
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#!/usr/bin/env python | |
# Estimating the value of pi via Monte Carlo simulation | |
from random import random | |
import sys | |
trials = eval(sys.argv[1]) # take input from cli | |
hits = 0 | |
for i in range(trials): | |
x, y = random() , random() # generate random x,y in (0,1] at each run | |
if x**2 + y**2 < 1 : # defines the edge of the quadrant | |
hits = hits + 1 | |
print 'hits : %d, trials: %d, estimate pi = %1.4F' %(hits, trials, 4*(float(hits) / trials)) |
From the code sample above and my cli, we see that as we increase the number of trials, our estimated value of \pi gets closer to the real value. And if you run enough trials you will approach steady state (true value). Another version of the code sample runs a lot of trials, so you can visually see what's happening to the estimated value of \pi
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#!/usr/bin/env python | |
# Estimating the value of pi via Monte Carlo simulation | |
from random import random | |
import numpy as np | |
import matplotlib.pyplot as plt | |
trials = list(np.linspace(10,1000000, 1000)) # different number of trials | |
pi = [] | |
def mc_multiple_runs(trials, hits = 0): | |
''' | |
(float, int) -> (float) | |
This function returns the number of hits you get for each monte carlo run | |
''' | |
for i in range(int(trials)): | |
x, y = random() , random() # generate random x,y in (0,1] at each run | |
if x**2 + y**2 < 1 : # defines the edge of the quadrant | |
hits = hits + 1 | |
return float(hits) | |
for i in trials: | |
pi.append(4*(mc_multiple_runs(i)/i)) | |
print 'hits : %d, trials: %d, estimate pi = %1.4F' %(mc_multiple_runs(i), i, 4*(mc_multiple_runs(i)/i) ) | |
# plot graphs | |
plt.plot(trials, pi, 'g') | |
plt.title('Estimating the value of pi via Monte Carlo') | |
plt.xlabel('# of Trials') | |
plt.ylabel('Estimated value of pi') | |
plt.ylim(3.11,3.17) | |
plt.show() | |
plt.hist(pi, bins = np.linspace(3.12,3.16,50), color='green') | |
plt.title('Estimating the value of pi via Monte Carlo') | |
plt.xlabel('Estimated value of pi') | |
plt.ylabel('Trials') | |
plt.xlim(3.13,3.15) | |
plt.show() |
See the graph below. The peaks occur between 3.140 and 3.144, which tells us that the true value of \pi lies somewhere in that range
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