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6ba812c8b193df42eeb5de9ab7cfb35d
mooc-rr
Commits
9ac75620
Commit
9ac75620
authored
Feb 25, 2021
by
Miguel Felipe Silva Vasconcelos
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#+TITLE:
Your title
#+TITLE:
On the computation of pi
#+AUTHOR:
Your name
#+AUTHOR:
Miguel Felipe Silva Vasconcelos
#+DATE:
Today's date
#+DATE:
25-02-2021
#+LANGUAGE: en
#+LANGUAGE: en
# #+PROPERTY: header-args :eval never-export
# #+PROPERTY: header-args :eval never-export
...
@@ -11,84 +11,74 @@
...
@@ -11,84 +11,74 @@
#+HTML_HEAD: <script type="text/javascript" src="http://www.pirilampo.org/styles/lib/js/jquery.stickytableheaders.js"></script>
#+HTML_HEAD: <script type="text/javascript" src="http://www.pirilampo.org/styles/lib/js/jquery.stickytableheaders.js"></script>
#+HTML_HEAD: <script type="text/javascript" src="http://www.pirilampo.org/styles/readtheorg/js/readtheorg.js"></script>
#+HTML_HEAD: <script type="text/javascript" src="http://www.pirilampo.org/styles/readtheorg/js/readtheorg.js"></script>
* Some explanations
* Asking the math library
My computer tells me that \pi is approximatively
This is an org-mode document with code examples in R. Once opened in
#+begin_src python :results value :session *python* :exports both
Emacs, this document can easily be exported to HTML, PDF, and Office
from math import *
formats. For more information on org-mode, see
pi
https://orgmode.org/guide/.
#+end_src
When you type the shortcut =C-c C-e h o=, this document will be
exported as HTML. All the code in it will be re-executed, and the
results will be retrieved and included into the exported document. If
you do not want to re-execute all code each time, you can delete the #
and the space before ~#+PROPERTY:~ in the header of this document.
Like we showed in the video, Python code is included as follows (and
is exxecuted by typing ~C-c C-c~):
#+begin_src python :results output :exports both
#+RESULTS:
print("Hello world!")
: 3.141592653589793
* Buffon's needle
Applying the method of [[https://en.wikipedia.org/wiki/Buffon%27s_needle_problem][Buffon's]] needle, we get the approximation
#+begin_src python :results value :session *python* :exports both
import numpy as np
np.random.seed(seed=42)
N = 10000
x = np.random.uniform(size=N, low=0, high=1)
theta = np.random.uniform(size=N, low=0, high=pi/2)
2/(sum((x+np.sin(theta))>1)/N)
#+end_src
#+end_src
#+RESULTS:
#+RESULTS:
:
Hello world!
:
3.128911138923655
And now the same but in an Python session. With a session, Python's
* Using a surface fraction argument
state, i.e. the values of all the variables, remains persistent from
A method that is easier to understand and does not make use of the sin
one code block to the next. The code is still executed using ~C-c
function is based on the fact that if $X \sim U(0,1)$ and $Y \sim U(0,1)$,
C-c~.
then $P[X^2+Y^2 \le 1]=\pi/4$ (see
[[https://en.wikipedia.org/wiki/Monte_Carlo_method]["Monte Carlo
method" on Wikipedia]]). The following code uses this approach:
#+begin_src python :results output :session :exports both
import numpy
x=numpy.linspace(-15,15)
print(x)
#+end_src
#+RESULTS:
#+begin_example
[-15. -14.3877551 -13.7755102 -13.16326531 -12.55102041
#+begin_src python :results output :session *python* :var matplot_lib_filename="figure.png" :exports code
-11.93877551 -11.32653061 -10.71428571 -10.10204082 -9.48979592
-8.87755102 -8.26530612 -7.65306122 -7.04081633 -6.42857143
-5.81632653 -5.20408163 -4.59183673 -3.97959184 -3.36734694
-2.75510204 -2.14285714 -1.53061224 -0.91836735 -0.30612245
0.30612245 0.91836735 1.53061224 2.14285714 2.75510204
3.36734694 3.97959184 4.59183673 5.20408163 5.81632653
6.42857143 7.04081633 7.65306122 8.26530612 8.87755102
9.48979592 10.10204082 10.71428571 11.32653061 11.93877551
12.55102041 13.16326531 13.7755102 14.3877551 15. ]
#+end_example
Finally, an example for graphical output:
#+begin_src python :results output file :session :var matplot_lib_filename="./cosxsx.png" :exports results
import matplotlib.pyplot as plt
import matplotlib.pyplot as plt
plt.figure(figsize=(10,5))
np.random.seed(seed=42)
plt.plot(x,numpy.cos(x)/x)
N = 1000
plt.tight_layout()
x = np.random.uniform(size=N, low=0, high=1)
y = np.random.uniform(size=N, low=0, high=1)
accept = (x*x+y*y) <= 1
reject = np.logical_not(accept)
fig, ax = plt.subplots(1)
ax.scatter(x[accept], y[accept], c='b', alpha=0.2, edgecolor=None)
ax.scatter(x[reject], y[reject], c='r', alpha=0.2, edgecolor=None)
ax.set_aspect('equal')
plt.savefig(matplot_lib_filename)
plt.savefig(matplot_lib_filename)
print(matplot_lib_filename)
print(matplot_lib_filename)
#+end_src
#+end_src
#+RESULTS:
#+RESULTS:
[[file:./cosxsx.png]]
: figure.png
Note the parameter ~:exports results~, which indicates that the code
[[./figure.png]]
will not appear in the exported document. We recommend that in the
context of this MOOC, you always leave this parameter setting as
~:exports both~, because we want your analyses to be perfectly
It is then straightforward to obtain a (not really good) approximation
transparent and reproducible.
to \pi by counting how many times, on average, $X^2+Y^2$ is smaller than 1:
Watch out: the figure generated by the code block is /not/ stored in
the org document. It's a plain file, here named ~cosxsx.png~. You have
#+begin_src python :results value :session *python* :exports both
to commit it explicitly if you want your analysis to be legible and
4*np.mean(accept)
understandable on GitLab.
#+end_src
Finally, don't forget that we provide in the resource section of this
#+RESULTS:
MOOC a configuration with a few keyboard shortcuts that allow you to
: 3.112
quickly create code blocks in Python by typing ~<p~, ~<P~ or ~<PP~
followed by ~Tab~.
Now it's your turn! You can delete all this information and replace it
by your computational document.
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