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ca693b8bd1eb5f2789da9233f56f5d25
mooc-rr
Commits
3fcff9f3
Commit
3fcff9f3
authored
Apr 10, 2024
by
Tommy Rushton
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More notebook reproduction.
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figure_pi_mc2.png
module2/exo1/figure_pi_mc2.png
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toy_document_orgmode_python_en.org
module2/exo1/toy_document_orgmode_python_en.org
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...
@@ -29,86 +29,54 @@ Applying the method of
...
@@ -29,86 +29,54 @@ Applying the method of
#+begin_src python :results value :session :exports both
#+begin_src python :results value :session :exports both
import numpy as np
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
* Some explanations
#+RESULTS:
: 3.128911138923655
This is an org-mode document with code examples in R. Once opened in
* Using a surface fraction argument
Emacs, this document can easily be exported to HTML, PDF, and Office
formats. For more information on org-mode, see
https://orgmode.org/guide/.
When you type the shortcut =C-c C-e h o=, this document will b
e
A method that is easier to understand and does not make use of th
e
exported as HTML. All the code in it will be re-executed, and the
$\sin$ function is based on the fact that if $X ~ U(0,1)$ and $Y ~
results will be retrieved and included into the exported document. If
U(0,1)$, then $P[X^2 + Y^2 \leq 1] = \pi/4$ (see
you do not want to re-execute all code each time, you can delete the #
[[https://en.wikipedia.org/wiki/Monte_Carlo_method]["Monte Carlo
and the space before ~#+PROPERTY:~ in the header of this document.
Method" on Wikipedia]]). The following code uses this approach:
Like we showed in the video, Python code is included as follows (and
#+begin_src python :results output file :session :var matplot_lib_filename="figure_pi_mc2.png" :exports both
i
s exxecuted by typing ~C-c C-c~):
i
mport matplotlib.pyplot as plt
#+begin_src python :results output :exports both
np.random.seed(seed=42)
print("Hello world!")
N = 1000
#+end_src
x = np.random.uniform(size=N, low=0, high=1)
y = np.random.uniform(size=N, low=0, high=1)
#+RESULTS:
accept = (x*x+y*y) <= 1
: Hello world!
reject = np.logical_not(accept)
And now the same but in an Python session. With a session, Python's
fig, ax = plt.subplots(1)
state, i.e. the values of all the variables, remains persistent from
ax.scatter(x[accept], y[accept], c='b', alpha=0.2, edgecolor=None)
one code block to the next. The code is still executed using ~C-c
ax.scatter(x[reject], y[reject], c='r', alpha=0.2, edgecolor=None)
C-c~.
ax.set_aspect('equal')
#+begin_src python :results output :session :exports both
plt.savefig(matplot_lib_filename)
import numpy
print(matplot_lib_filename)
x=numpy.linspace(-15,15)
print(x)
#+end_src
#+end_src
#+RESULTS:
#+RESULTS:
#+begin_example
[[file:figure_pi_mc2.png]]
[-15. -14.3877551 -13.7755102 -13.16326531 -12.55102041
-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
plt.figure(figsize=(10,5))
It is then straightforward to obtain a (not really good) approximation
plt.plot(x,numpy.cos(x)/x)
to $\pi$ by counting how many times, on average, $X^2 + Y^2$ is smaller
plt.tight_layout()
than 1:
plt.savefig(matplot_lib_filename)
#+begin_src python :results value :session :exports both
print(matplot_lib_filename
)
4*np.mean(accept
)
#+end_src
#+end_src
#+RESULTS:
#+RESULTS:
[[file:./cosxsx.png]]
: 3.112
Note the parameter ~:exports results~, which indicates that the code
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
transparent and reproducible.
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
to commit it explicitly if you want your analysis to be legible and
understandable on GitLab.
Finally, don't forget that we provide in the resource section of this
MOOC a configuration with a few keyboard shortcuts that allow you to
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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