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+{
+ "cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Analyse du risque de défaillance des joints toriques de la navette Challenger"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "Le 27 Janvier 1986, veille du décollage de la navette *Challenger*, eu\n",
+ "lieu une télé-conférence de trois heures entre les ingénieurs de la\n",
+ "Morton Thiokol (constructeur d'un des moteurs) et de la NASA. La\n",
+ "discussion portait principalement sur les conséquences de la\n",
+ "température prévue au moment du décollage de 31°F (juste en dessous de\n",
+ "0°C) sur le succès du vol et en particulier sur la performance des\n",
+ "joints toriques utilisés dans les moteurs. En effet, aucun test\n",
+ "n'avait été effectué à cette température.\n",
+ "\n",
+ "L'étude qui suit reprend donc une partie des analyses effectuées cette\n",
+ "nuit là et dont l'objectif était d'évaluer l'influence potentielle de\n",
+ "la température et de la pression à laquelle sont soumis les joints\n",
+ "toriques sur leur probabilité de dysfonctionnement. Pour cela, nous\n",
+ "disposons des résultats des expériences réalisées par les ingénieurs\n",
+ "de la NASA durant les 6 années précédant le lancement de la navette\n",
+ "Challenger.\n",
+ "\n"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Chargement des données\n",
+ "Nous commençons donc par charger ces données:"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 1,
+ "metadata": {},
+ "outputs": [
+ {
+ "data": {
+ "text/html": [
+ "
\n",
+ "\n",
+ "
\n",
+ " \n",
+ "
\n",
+ "
\n",
+ "
Date
\n",
+ "
Count
\n",
+ "
Temperature
\n",
+ "
Pressure
\n",
+ "
Malfunction
\n",
+ "
\n",
+ " \n",
+ " \n",
+ "
\n",
+ "
0
\n",
+ "
4/12/81
\n",
+ "
6
\n",
+ "
66
\n",
+ "
50
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
1
\n",
+ "
11/12/81
\n",
+ "
6
\n",
+ "
70
\n",
+ "
50
\n",
+ "
1
\n",
+ "
\n",
+ "
\n",
+ "
2
\n",
+ "
3/22/82
\n",
+ "
6
\n",
+ "
69
\n",
+ "
50
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
3
\n",
+ "
11/11/82
\n",
+ "
6
\n",
+ "
68
\n",
+ "
50
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
4
\n",
+ "
4/04/83
\n",
+ "
6
\n",
+ "
67
\n",
+ "
50
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
5
\n",
+ "
6/18/82
\n",
+ "
6
\n",
+ "
72
\n",
+ "
50
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
6
\n",
+ "
8/30/83
\n",
+ "
6
\n",
+ "
73
\n",
+ "
100
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
7
\n",
+ "
11/28/83
\n",
+ "
6
\n",
+ "
70
\n",
+ "
100
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
8
\n",
+ "
2/03/84
\n",
+ "
6
\n",
+ "
57
\n",
+ "
200
\n",
+ "
1
\n",
+ "
\n",
+ "
\n",
+ "
9
\n",
+ "
4/06/84
\n",
+ "
6
\n",
+ "
63
\n",
+ "
200
\n",
+ "
1
\n",
+ "
\n",
+ "
\n",
+ "
10
\n",
+ "
8/30/84
\n",
+ "
6
\n",
+ "
70
\n",
+ "
200
\n",
+ "
1
\n",
+ "
\n",
+ "
\n",
+ "
11
\n",
+ "
10/05/84
\n",
+ "
6
\n",
+ "
78
\n",
+ "
200
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
12
\n",
+ "
11/08/84
\n",
+ "
6
\n",
+ "
67
\n",
+ "
200
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
13
\n",
+ "
1/24/85
\n",
+ "
6
\n",
+ "
53
\n",
+ "
200
\n",
+ "
2
\n",
+ "
\n",
+ "
\n",
+ "
14
\n",
+ "
4/12/85
\n",
+ "
6
\n",
+ "
67
\n",
+ "
200
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
15
\n",
+ "
4/29/85
\n",
+ "
6
\n",
+ "
75
\n",
+ "
200
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
16
\n",
+ "
6/17/85
\n",
+ "
6
\n",
+ "
70
\n",
+ "
200
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
17
\n",
+ "
7/29/85
\n",
+ "
6
\n",
+ "
81
\n",
+ "
200
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
18
\n",
+ "
8/27/85
\n",
+ "
6
\n",
+ "
76
\n",
+ "
200
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
19
\n",
+ "
10/03/85
\n",
+ "
6
\n",
+ "
79
\n",
+ "
200
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
20
\n",
+ "
10/30/85
\n",
+ "
6
\n",
+ "
75
\n",
+ "
200
\n",
+ "
2
\n",
+ "
\n",
+ "
\n",
+ "
21
\n",
+ "
11/26/85
\n",
+ "
6
\n",
+ "
76
\n",
+ "
200
\n",
+ "
0
\n",
+ "
\n",
+ "
\n",
+ "
22
\n",
+ "
1/12/86
\n",
+ "
6
\n",
+ "
58
\n",
+ "
200
\n",
+ "
1
\n",
+ "
\n",
+ " \n",
+ "
\n",
+ "
"
+ ],
+ "text/plain": [
+ " Date Count Temperature Pressure Malfunction\n",
+ "0 4/12/81 6 66 50 0\n",
+ "1 11/12/81 6 70 50 1\n",
+ "2 3/22/82 6 69 50 0\n",
+ "3 11/11/82 6 68 50 0\n",
+ "4 4/04/83 6 67 50 0\n",
+ "5 6/18/82 6 72 50 0\n",
+ "6 8/30/83 6 73 100 0\n",
+ "7 11/28/83 6 70 100 0\n",
+ "8 2/03/84 6 57 200 1\n",
+ "9 4/06/84 6 63 200 1\n",
+ "10 8/30/84 6 70 200 1\n",
+ "11 10/05/84 6 78 200 0\n",
+ "12 11/08/84 6 67 200 0\n",
+ "13 1/24/85 6 53 200 2\n",
+ "14 4/12/85 6 67 200 0\n",
+ "15 4/29/85 6 75 200 0\n",
+ "16 6/17/85 6 70 200 0\n",
+ "17 7/29/85 6 81 200 0\n",
+ "18 8/27/85 6 76 200 0\n",
+ "19 10/03/85 6 79 200 0\n",
+ "20 10/30/85 6 75 200 2\n",
+ "21 11/26/85 6 76 200 0\n",
+ "22 1/12/86 6 58 200 1"
+ ]
+ },
+ "execution_count": 1,
+ "metadata": {},
+ "output_type": "execute_result"
+ }
+ ],
+ "source": [
+ "import numpy as np\n",
+ "import pandas as pd\n",
+ "data = pd.read_csv(\"shuttle.csv\")\n",
+ "data"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "Le jeu de données nous indique la date de l'essai, le nombre de joints\n",
+ "toriques mesurés (il y en a 6 sur le lançeur principal), la\n",
+ "température (en Farenheit) et la pression (en psi), et enfin le\n",
+ "nombre de dysfonctionnements relevés. "
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Inspection graphique des données\n",
+ "~~Les vols où aucun incident n'est relevé n'apportant aucun information\n",
+ "sur l'influence de la température ou de la pression sur les\n",
+ "dysfonctionnements, nous nous concentrons sur les expériences où au\n",
+ "moins un joint a été défectueux.~~ Au lieu de ne considérer que les cas de défaillances, on prend en compte **tous les essais.**\n"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 15,
+ "metadata": {},
+ "outputs": [],
+ "source": [
+ "#data = data[data.Malfunction>0]\n",
+ "#data"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "~~Très bien, nous avons une variabilité de température importante mais\n",
+ "la pression est quasiment toujours égale à 200, ce qui devrait\n",
+ "simplifier l'analyse.~~ Dans la suite, on **néglige les effets de la pression.**\n",
+ "\n",
+ "Comment la fréquence ~~d'échecs~~ **des résultats** varie-t-elle avec la température ?\n"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 16,
+ "metadata": {},
+ "outputs": [
+ {
+ "data": {
+ "image/png": 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\n",
+ "text/plain": [
+ "
"
+ ]
+ },
+ "metadata": {
+ "needs_background": "light"
+ },
+ "output_type": "display_data"
+ }
+ ],
+ "source": [
+ "%matplotlib inline\n",
+ "pd.set_option('mode.chained_assignment',None) # this removes a useless warning from pandas\n",
+ "import matplotlib.pyplot as plt\n",
+ "\n",
+ "data[\"Frequency\"]=data.Malfunction/data.Count\n",
+ "data.plot(x=\"Temperature\",y=\"Frequency\",kind=\"scatter\",ylim=[0,1])\n",
+ "plt.grid(True)"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "~~À première vue, ce n'est pas flagrant mais bon, essayons quand même\n",
+ "d'estimer l'impact de la température $t$ sur la probabilité de\n",
+ "dysfonctionnements d'un joint. ~~Beaucoup plus de points que lors de l'analyse fournie au début de l'exercice en incluant ceux correspondants aux essais réussis. On poursuit avec une estimation de la probabilité de défaillance.\n"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Estimation de l'influence de la température\n",
+ "\n",
+ "Supposons que chacun des 6 joints toriques est endommagé avec la même\n",
+ "probabilité et indépendamment des autres et que cette probabilité ne\n",
+ "dépend que de la température. Si on note $p(t)$ cette probabilité, le\n",
+ "nombre de joints $D$ dysfonctionnant lorsque l'on effectue le vol à\n",
+ "température $t$ suit une loi binomiale de paramètre $n=6$ et\n",
+ "$p=p(t)$. Pour relier $p(t)$ à $t$, on va donc effectuer une\n",
+ "régression logistique."
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 17,
+ "metadata": {},
+ "outputs": [
+ {
+ "data": {
+ "text/html": [
+ "
\n",
+ "
Generalized Linear Model Regression Results
\n",
+ "
\n",
+ "
Dep. Variable:
Frequency
No. Observations:
23
\n",
+ "
\n",
+ "
\n",
+ "
Model:
GLM
Df Residuals:
21
\n",
+ "
\n",
+ "
\n",
+ "
Model Family:
Binomial
Df Model:
1
\n",
+ "
\n",
+ "
\n",
+ "
Link Function:
logit
Scale:
1.0000
\n",
+ "
\n",
+ "
\n",
+ "
Method:
IRLS
Log-Likelihood:
-3.9210
\n",
+ "
\n",
+ "
\n",
+ "
Date:
Tue, 25 Jan 2022
Deviance:
3.0144
\n",
+ "
\n",
+ "
\n",
+ "
Time:
17:21:38
Pearson chi2:
5.00
\n",
+ "
\n",
+ "
\n",
+ "
No. Iterations:
6
Covariance Type:
nonrobust
\n",
+ "
\n",
+ "
\n",
+ "
\n",
+ "
\n",
+ "
coef
std err
z
P>|z|
[0.025
0.975]
\n",
+ "
\n",
+ "
\n",
+ "
Intercept
5.0850
7.477
0.680
0.496
-9.570
19.740
\n",
+ "
\n",
+ "
\n",
+ "
Temperature
-0.1156
0.115
-1.004
0.316
-0.341
0.110
\n",
+ "
\n",
+ "
"
+ ],
+ "text/plain": [
+ "\n",
+ "\"\"\"\n",
+ " Generalized Linear Model Regression Results \n",
+ "==============================================================================\n",
+ "Dep. Variable: Frequency No. Observations: 23\n",
+ "Model: GLM Df Residuals: 21\n",
+ "Model Family: Binomial Df Model: 1\n",
+ "Link Function: logit Scale: 1.0000\n",
+ "Method: IRLS Log-Likelihood: -3.9210\n",
+ "Date: Tue, 25 Jan 2022 Deviance: 3.0144\n",
+ "Time: 17:21:38 Pearson chi2: 5.00\n",
+ "No. Iterations: 6 Covariance Type: nonrobust\n",
+ "===============================================================================\n",
+ " coef std err z P>|z| [0.025 0.975]\n",
+ "-------------------------------------------------------------------------------\n",
+ "Intercept 5.0850 7.477 0.680 0.496 -9.570 19.740\n",
+ "Temperature -0.1156 0.115 -1.004 0.316 -0.341 0.110\n",
+ "===============================================================================\n",
+ "\"\"\""
+ ]
+ },
+ "execution_count": 17,
+ "metadata": {},
+ "output_type": "execute_result"
+ }
+ ],
+ "source": [
+ "import statsmodels.api as sm\n",
+ "\n",
+ "data[\"Success\"]=data.Count-data.Malfunction\n",
+ "data[\"Intercept\"]=1\n",
+ "\n",
+ "logmodel=sm.GLM(data['Frequency'], data[['Intercept','Temperature']], family=sm.families.Binomial(sm.families.links.logit)).fit()\n",
+ "\n",
+ "logmodel.summary()"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "L'estimateur le plus probable du paramètre de température est ~~0.0014~~ **-0.1156**\n",
+ "et l'erreur standard de cet estimateur est de ~~0.122~~ **0.115**, autrement dit ~~on\n",
+ "ne peut pas distinguer d'impact particulier et il faut prendre nos\n",
+ "estimations avec des pincettes.~~ la température semble avoir un effet significatif mais l'incertitude est grande.\n"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Estimation de la probabilité de dysfonctionnant des joints toriques\n",
+ "La température prévue le jour du décollage est de 31°F. Essayons\n",
+ "d'estimer la probabilité de dysfonctionnement des joints toriques à\n",
+ "cette température à partir du modèle que nous venons de construire:\n"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 18,
+ "metadata": {},
+ "outputs": [
+ {
+ "data": {
+ "image/png": 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NHDlygXNuUE3tAjlbprqkOfQTIQbIAk4DEoHPzewL59yqgxZy7gngCYBBgwa5ESNGBLD5n8rOzqa2y4ab7OxsbvrFCJq0Wc9dby8jp6Q1t47uEeqyaiXa3pdo6Eu09APUl6MVSLjnAu2qTGcCm6pps905txfYa2YfA/2AVUhAfnlCB1ZvLWRq9lq6NE/hgiyNIikitRfIMfccoKuZdTSzOOBi4K1D2rwJnGRmMWaWBAwFlge31OhmZtx1Ti9O6NyU219fwoLvdoa6JBGJYDWGu3OuHLgBmIMvsF92zi01s0lmNsnfZjnwLrAY+Ap4yjn3bf2VHZ1ivR4evWwgrdMTuO75BeTt1hk0IlI7AZ3n7pyb7Zzr5pzr7Jy7xz/vMefcY1XaTHHO9XTO9XbOPVhfBUe79KQ4pv1yECVllUx4VmfQiEjt6ArVMNSlRSoPXzqAlVvy+a+XdaNtETl6CvcwNbJ7C/77rON4d+kWHv7P6lCXIyIRRgOHhbFrTuzIii0FPPj+arq3TOXMPq1DXZKIRAjtuYcxM+Oe83ozsH06v3v5G5Zt0m36RCQwCvcwt/8+rGmJsVz73Hx2FJaEuiQRiQAK9wjQIjWBJ67IYnthCb/+59e6i5OI1EjhHiH6ZqZz/wV9+XL9Tv749tJQlyMiYU5fqEaQMQPasnxzPo9/vI6erdO4dGj7UJckImFKe+4R5veje3BKt+bc+da3zN+gIQpEpHoK9wjj9RgPXzyAzGOSmPTCAjZpiAIRqYbCPQKlJcXy5BVZFJdVct3zCyguqwh1SSISZhTuEapLi1T+dlF/luTt4fbXl1DTTVdEpHFRuEew03u25Hend+ONhXlM+3R9qMsRkTCicI9wN4zswuherfjz7OV8snpbqMsRkTChcI9wHo/xwLh+dGmRwg0vLmTjjn2hLklEwoDCPQqkxMfw5BW+++Ve+5zGgBcRhXvUOLZpMv+4dACrtxZwyyvf6AtWkUZO4R5FTuranNvO7MG/v93CIx+uCXU5IhJCCvcoc+1JnRjTvw1/eW8V7y/7IdTliEiIKNyjjJlx3wV96dWmCTfPXMSarYWhLklEQkDhHoUSYr08Pn4Q8TEeJj43nz1FZaEuSUQamMI9SrVNT2Tq5Vls3LmP38xYSIVusi3SqCjco9iQjhnceU4vsldu44G5K0Ndjog0II3nHuUuH9qeZZvymZq9lp6tm3B2vzahLklEGoD23KOcmfHHc3ox6NhjmPzqN3ybtyfUJYlIA1C4NwJxMR6mXp7FMUlxTHxuPtt1k22RqKdwbySap8bz5BWD2LG3lF+9sIDSct1kWySaKdwbkd5t0/i/sX3J2bCLO99aqiEKRKKYvlBtZM7t35blmwt47KO19GydyvhhHUJdkojUA+25N0KTR3Xn1B4t+OPby/hs7fZQlyMi9UDh3gh5PcZDF/enQ7Nkrv/n1xoDXiQKKdwbqdSEWJ66YhCVDiY8l0NBsYYoEIkmCvdGrEOzZB69bCBrt+3l5hmLNESBSBRRuDdyw7s0486ze/LBiq1MmaMhCkSihc6WEcYffywrt/jOoOnWMoXzB2aGuiQRqaOA9tzNbLSZrTSzNWZ22xHaDTazCjMbG7wSpb6ZGXed04thnZpy22tLWPDdzlCXJCJ1VGO4m5kXeAQ4E+gJXGJmPQ/T7n5gTrCLlPoX6/Uw9fKBtElPYOJzC8jdpTNoRCJZIHvuQ4A1zrl1zrlSYAZwbjXtbgReA7YGsT5pQOlJcUy7cjClFZVMeHa+zqARiWBW0yXo/kMso51zE/zT44GhzrkbqrRpC7wInApMA95xzr1azbomAhMBWrZsmTVjxoxaFV1YWEhKSkqtlg034diXpdsr+MuCYno383LzwHg8ZgEtF459qa1o6Uu09APUl/1Gjhy5wDk3qKZ2gXyhWt3/7EM/ER4EbnXOVdgRgsA59wTwBMCgQYPciBEjAtj8T2VnZ1PbZcNNOPZlBJCW+R1/mPUtnxS24M6zewW0XDj2pbaipS/R0g9QX45WIOGeC7SrMp0JbDqkzSBghj/YmwFnmVm5c25WUKqUBnf58ceybttenp63nk7NkjUGjUiECSTcc4CuZtYRyAMuBi6t2sA513H/czObju+wjII9wv2/nx/Hdzv2cudbS8nMSGJk9xahLklEAlTjF6rOuXLgBnxnwSwHXnbOLTWzSWY2qb4LlNDxeoyHLxnAca2bcMM/v2bZpvxQlyQiAQroPHfn3GznXDfnXGfn3D3+eY855x6rpu2V1X2ZKpEpOT6Gab8cTGpCLNc8m8OWPcWhLklEAqDhB6RGrdISmHblIPKLyrh6eg6FJeWhLklEaqBwl4D0apPGI5cNZOUPBdzw4teUV+g2fSLhTOEuARvRvQV/Orc32Su3cceb3+o2fSJhTAOHyVG5dGh7cnft49HstbRNT+SGU7uGuiQRqYbCXY7a5FHd2bKnmAfmrqJVWiJjszSKpEi4UbjLUTMz7rugL1sLSrjttcU0T43nlG7Na7WuWQvzmDJnJZt2F9EmPZHJo7ozZkDbIFcs9UXvX/jSMXeplbgY3yiS3Vqm8qsXFvDN97uPeh2zFuZx++tLyNtdhAPydhdx++tLmLUwL/gFS9Dp/QtvCneptdSEWKZfPZimKXFcPT2HLXuP7gyaKXNWUlRWcdC8orIK3REqQuj9C28Kd6mTFqkJPHvVEBzwwPxifsgP/CKnTbuLjmq+hBe9f+FN4S511ql5CtOvGkxhqeOKaV+xZ19g48C3SU88qvkSXvT+hTeFuwRF38x0bhqYwPrte7n62Rz2ldZ8FevkUd1JjPUeNC8x1svkUd3rq0wJIr1/4U3hLkHTs6mXBy/uz8KNu5j0wteUlh/5GPyYAW259/w+tE1PxIC26Ynce34fnW0RIfT+hTedCilBdVaf1tx3fl9+/9pifjtzEQ9fMgCv5/A3cBkzoK3CIILp/QtfCncJunGD25FfXMbd/1pOcryX+87vi+cIAS8iwadwl3ox4aROFBSX89AHq0mM9XLXOb040i0YRSS4FO5Sb27+WVf2lZbz5CfrSYjzctvoHgp4kQaicJd6Y2b891nHsa+0gsc/Wkd8jJffnd4t1GWJNAoKd6lXZsafzu1NaXklD3+wmliPceNpGklSpL4p3KXeeTy+gcYqKh1/eW8VMV4PvxrROdRliUQ1hbs0CK/HmHJhP8orHfe/uwKH49cjuoS6LJGopXCXBuP1GH8d1w8z+L93V+IcXD9SAS9SHxTu0qBivB7+Oq4/hm9UwfIKx02nddFZNCJBpnCXBuf1GH8Z1x+vx8Pf3l9FSXkFk0d1V8CLBJHCXULC6zGmjO1LXIyHR7PXUlxWyR2/OE4BLxIkCncJGY/H+PN5vYmP8fD0vPXsKy3nnvP6HHEsGhEJjMJdQsrMuPPsnqQmxPD3/6yhsKScv47rT1yMBiwVqQuFu4ScmfFfZ3QnJT6Ge/+9goLicqZePpCkOP3zFKkt7R5J2LjulM7cd34fPlm9jUuf/JJde0tDXZJIxFK4S1i5eEh7Hr0si2Wb87nw8c/J0/04RWpF4S5hZ3TvVjx71RB+yC/mvEfmsWxTfqhLEok4CncJS8M6N+WVScPwmDHu8c/5ZPW2UJckElEU7hK2erRqwhvXn0DmMYlc9UwOM3M2hrokkYihcJew1jotkVcmDWNY56bc+toS7n93BZWVLtRliYQ9hbuEvdSEWJ6+cjCXDGnP1Oy1/OqfC9hXWh7qskTCWkDhbmajzWylma0xs9uqef0yM1vs//nMzPoFv1RpzGK9Hv58Xm/u+EVP3lv2A2Onfs4mnUkjclg1hruZeYFHgDOBnsAlZtbzkGbrgVOcc32BPwFPBLtQETPjmhM7Mu3KwXy/cx9n//1Tvlq/M9RliYSlQPbchwBrnHPrnHOlwAzg3KoNnHOfOed2+Se/ADKDW6bIj0Z2b8Eb1w8nLTGWS5/8guc/34BzOg4vUpXV9J/CzMYCo51zE/zT44GhzrkbDtP+FqDH/vaHvDYRmAjQsmXLrBkzZtSq6MLCQlJSUmq1bLhRX2pvX5nj8cUlfLOtguFtYriiVxzx3uAMOhYt70u09APUl/1Gjhy5wDk3qMaGzrkj/gAXAk9VmR4P/P0wbUcCy4GmNa03KyvL1daHH35Y62XDjfpSNxUVle5v7610HW57x43620du/bbCoKw3Wt6XaOmHc+rLfsB8V0O+OucCOiyTC7SrMp0JbDq0kZn1BZ4CznXO7QhgvSJ15vEYN/+sG89cOZjNe4o5+++f8q/Fm0NdlkjIBRLuOUBXM+toZnHAxcBbVRuYWXvgdWC8c25V8MsUObIR3Vvwr5tOpHOLFK5/8WvumPUtxWUVoS5LJGRqDHfnXDlwAzAH3yGXl51zS81skplN8jf7H6Ap8KiZLTKz+fVWschhZB6TxMvXDePakzry/BffMeaReaz+oSDUZYmEREADZjvnZgOzD5n3WJXnE4CffIEq0tBmL9nM7CVbAFj1QwFnPfwJY/q3Zd6a7WzeU0yb9EQmj+rOmAFtg77tWQvzmDJnJZt2F9XrdgLxh1lLeOnL77m5dxnX3D6bS4a24+4xfUJSi4SG7oYgUWPWwjxuf30JRf7DMZUOXIXjlQW5B9rk7S7i9teXAAQ1eA/ddn1tJxB/mLWEF774cRyeCucOTCvgGw8NPyBRY8qclQfCdb/qTvQtKqtgypyV9b7t+thOIF768vujmi/RSeEuUeNohiMI9k1ADrftUAyRUHGYa1cON1+ik8Jdokab9MSA23oM3lyUF7QrWw+37aOpKVi8Vv2FXIebL9FJ4S5RY/Ko7iTGeg+aF+sxYg+5ajU+xkPmMUn8ZsYiJjw7n9xd++pl24mxXiaP6l7ndR+tS4a2O6r5Ep0U7hI1xgxoy73n96FteiIGtE1PZMqF/Zgytt9B8+6/oC8f3jKCP/z8OD5bu4PT//oxT3y8lrKKyqBu+97z+4TkbJm7x/Th8uPbH9hT95px+fHt9WVqI6OzZSSqjBnQttpArW7ehJM6Mbp3K+56ayl/nr2C1xbk8cdze3F8p6ZB3XYo3D2mD3eP6UN2djZrLxsR6nIkBLTnLo1a5jFJPPXLwTwxPovCknIufuILbnppITuLa78XLxIOtOcuApzRqxUndW3O1I/W8thHa3m3spLvvKu47pROJMXpv4lEHu25i/glxnn53end+OB3p9C/hZeHPljNyAeymZmzkQrdt1UijMJd5BDtMpL4df8EXpk0jNZpidz62hLOfOhj3lv2g24KIhFD4S5yGIM7ZPDGr0/g0csGUlbhuPa5+Yx59DM+Xb1dIS9hT+EucgRmxll9WvPeb0/m/gv6sC2/mMunfcm4xz9n3hqFvIQvhbtIAGK8Hi4a3J7/3DKC/z23F9/vLOKyp77kgqmf8Z8VOlwj4UfhLnIUEmK9XDGsA9mTR/Cnc3vxQ34JV0+fz1kPf8obC3PrdCGUSDAp3EVqISHWy3h/yD9wYT/KKir57cxvOPn/PuTxj9ayZ19ZqEuURk4n8IrUQazXw9isTM4f0JbsVVt54uN13PvvFTz4/mouyGrLFcM60K1laqjLlEZI4S4SBB6PcWqPlpzaoyVLN+1h+rwNvDw/lxe+2MjQjhlcfvyxnNGrJfEx3ppXJhIECneRIOvVJo0pF/bj9rOO4+X53/PCF99x40sLyUiO44KBbRk3qB1dtTcv9UzhLlJPMpLjmHRKZyae1IlP12znpa828sy8DTz5yXr6ZaYxNiuTn/dtQ0ZyXKhLlSikcBepZx6PcXK35pzcrTnbC0uYtTCPVxfkcsebS/nj28sY0b05Z/drw8+Oa0lyvP5LSnDoX5JIA2qWEs+Ekzox4aROLN+cz6yFeby5aBPvL99KQqyHU3u04MzerRnZowUpCnqpA/3rEQmR41o34bjWTbh1dA/mf7eLt7/ZxL+/3cLsJVuIi/FwUpdmnN6zJacd15LmqfGhLlcijMJdJMQ8HmNIxwyGdMzgrnN6seC7Xcxespn3lv3AByu2YraEvpnpnNajBSO6N6d3mzQ8Ht0PVY5M4S4SRrxVgv7Os3uyfHMBHyz3hfzf3l/FX99bRUZyHCd2acaJXZtxYpc9/m12AAANA0lEQVRmIbkJt4Q/hbtImDIzerZpQs82TbjxtK5sLyzh09XbyV65lU/XbOetbzYB0LFZMsd3yuD4Tk0Z0jGD1mkKe1G4i0SMZinxB+7T6pxj5Q8FfLp6O5+v3cE732zmpa++B6BdRiKDj81g4LHH4Aoqqah0eHUYp9FRuItEIDOjR6sm9GjVhAkndaK8opLlmwv4asNOvlq/g49Xb+P1hXkA3Jczh76Z6fRrl06/zDT6tkunTVoCZgr8aKZwF4kCMV4PfTLT6JOZxjUndsQ5x8ad+3jh3c8oSWnNwo27mfbpOsoqfEMTH5MUS++2afRs7Tvsc1zrJnRslkysV2MJRguFu0gUMjOObZrM8LaxjBjRG4CS8gpWbC5gce5ulm7K59tNe3hm3gZK/cMUx3k9dGqeTPdWqXRtkULXlql0aZFC+4wkhX4EUriLNBLxMV7foZl26QfmlVVUsm7bXpZvzmfFlgJWbMln/oZdvLlo04E2sV6jfUYSHZul0Kl5Msc2TaJj02TaN02idVqijueHKYW7SCMW6/XQvVUq3VsdPJBZYUk5a7YWsnZrIWu2FbJ+217Wb9/Lx6u3UVpeWWV5o216Iu0yksg8JonMYxJpm55I22MSaZOeSMvUeGK01x8SCncR+YmU+Bj6t0unf5W9fIDKSseW/GI2bN/Lhh37+H7XPjbu2Efurn3M3bSFHXtLD2rvMWiRmkCrtARaNfE9tmgST4vUBFqkxtOiSTzNUuLJSIrThVlBpnAXkYB5PEabdN9e+Qldfvr6vtJyNu0uIndXEZv3FLN5dxGb9hTzQ34xa7YVMm/tdgqKy3+ynNdjZCTH0TQ5jmYp8TRNiSMjOY6MpDgyUuI4JimO73ZU0HJzPsckxZGWGEtCrEdn/ByBwl1EgiYpLoYuLVLp0uLw49XvKy1na34JWwtK2FpQzPaCErYXlrKtoIQde0vZXljCxp372LW3lIKSgz8I7s/55MDzOK+HtKRYmiTEkJYYS5PEWJokxJKaEEPqgccYUuJ//En2//iee0mKi4na7wwCCnczGw08BHiBp5xz9x3yuvlfPwvYB1zpnPs6yLWKRK1ZC/OYMmclm3YX0SY9kcmjuvPK/I3MW7vzQJvhnTO4cFD7n7QDfjJv/nc7eenL77m5dxnX3D6bS4a24+4xfQLa7pgBbQ87P5Dl92+7wjm8Zj/ZdlJcDB2axbDo+9019uXOs3tycrfm7NxXyofzcujQrSe79pXx2drtZK/cxraCEgqKy/B6jLIKx4bte8kvLqeguOzAaZ81iY/xkBTnC/qkOC+JcV4SY70kxXlJiPU9T4jzkhDjJSHWQ0Lsj4/xMR7iY/yPsT8+j9v/4/3xebzXS2yMEev14FxgtdVFjeFuZl7gEeB0IBfIMbO3nHPLqjQ7E+jq/xkKTPU/ikgNZi3M4/bXl1BUVgFA3u4ibp656Cft5q3deVDY5+0uYvKr34CDskp3YN7vZi6isspyFc7xwhcbAQ4K2eq2e/vrS5j/3U5eW5D3k/nAQQFf3fJ12fbkV74B40Ao5+0u4o43l3Lv+X0YM6AtW5p6GdGnNbMW5vHB8q0Hli0uq+T7nUUH2u1XXFZBYUk5hcXlFBSXU1hSzt6ScvaWlrO3pIK9JeXsK61gb2k5+0p9z4tKKw487thbemC6pLyC4rJKisoqqKisezCf2TGWkSPrvJojCmTPfQiwxjm3DsDMZgDnAlXD/VzgOef7OPrCzNLNrLVzbnPQKxaJMlPmrDwQVEerur3TymraAbz05fcHBWx12y0qqziw133o/ClzVh4UntUtX5dtl1UTmoFut7p2vj1sL81SgjtccllFJcVlFZSUV1JS7nte6n/ue6ygpKyS0grf9IHH8krKKnw/nl0bg1pTdaymPw/MbCww2jk3wT89HhjqnLuhSpt3gPucc5/6pz8AbnXOzT9kXROBif7J7sDKWtbdDNhey2XDjfoSnhqsL3GtumTV17or9u3Bm5R2YLp0y5oFddluXZYPwrLNgO1HWrbqNsJcXf59Heuca15To0D23Kv7tuHQT4RA2uCcewJ4IoBtHrkgs/nOuUF1XU84UF/CU7T0xczml+/ZGvH9gOh5T6Bh+hLI1QW5QLsq05nAplq0ERGRBhJIuOcAXc2so5nFARcDbx3S5i3gCvM5Htij4+0iIqFT42EZ51y5md0AzMF3KuTTzrmlZjbJ//pjwGx8p0GuwXcq5FX1VzIQhEM7YUR9CU/R0pdo6QeoL0elxi9URUQk8mhEHxGRKKRwFxGJQmEf7maWYGZfmdk3ZrbUzP7on59hZu+Z2Wr/4zGhrjUQZuY1s4X+awMiuR8bzGyJmS0ys/n+eZHal3Qze9XMVpjZcjMbFol9MbPu/vdj/0++md0coX35rf//+7dm9pI/ByKuHwBm9ht/P5aa2c3+efXel7APd6AEONU51w/oD4z2n5FzG/CBc64r8IF/OhL8BlheZTpS+wEw0jnXv8r5upHal4eAd51zPYB++N6fiOuLc26l//3oD2ThO7nhDSKsL2bWFrgJGOSc643vRI6LibB+AJhZb+BafFf69wN+YWZdaYi+OOci5gdIAr7GN27NSqC1f35rYGWo6wug/kz/G3kq8I5/XsT1w1/rBqDZIfMiri9AE2A9/pMLIrkvh9R/BjAvEvsCtAW+BzLwndH3jr8/EdUPf50X4htscf/0HcDvG6IvkbDnvv9QxiJgK/Cec+5LoKXzn0vvf2wRyhoD9CC+N7bqEByR2A/wXYE818wW+IeVgMjsSydgG/CM/3DZU2aWTGT2paqLgZf8zyOqL865POABYCOwGd91M3OJsH74fQucbGZNzSwJ3ynj7WiAvkREuDvnKpzvT81MYIj/T52IYma/ALY65yJl7IuaDHfODcQ3Iuj1ZnZyqAuqpRhgIDDVOTcA2EsE/Ll/JP6LDc8BXgl1LbXhP/58LtARaAMkm9nloa2qdpxzy4H7gfeAd4FvgJ/eraQeRES47+ec2w1kA6OBH8ysNYD/cWsISwvEcOAcM9sAzABONbMXiLx+AOCc2+R/3IrvuO4QIrMvuUCu/69BgFfxhX0k9mW/M4GvnXM/+KcjrS8/A9Y757Y558qA14ETiLx+AOCcm+acG+icOxnYCaymAfoS9uFuZs3NLN3/PBHfG78C35AHv/Q3+yXwZmgqDIxz7nbnXKZzrgO+P5n/45y7nAjrB4CZJZtZ6v7n+I6HfksE9sU5twX43sy6+2edhm8464jrSxWX8OMhGYi8vmwEjjezJDMzfO/JciKvHwCYWQv/Y3vgfHzvTb33JeyvUDWzvsCz+L4x9wAvO+f+18yaAi8D7fH9Y7jQObfz8GsKH2Y2ArjFOfeLSOyHmXXCt7cOvsMaLzrn7onEvgCYWX/gKSAOWIdv+AwPkdmXJHxfRnZyzu3xz4u498V/yvNF+A5hLAQmAClEWD8AzOwToClQBvzOOfdBQ7wnYR/uIiJy9ML+sIyIiBw9hbuISBRSuIuIRCGFu4hIFFK4i4hEoUBukC3SoPyniX3gn2wFVOAbIgBgiHOuNCSFHYGZXQ3M9p83LxJyOhVSwpqZ3QUUOuceCINavM65isO89ilwg3Nu0VGsL8Y51yCXokvjo8MyElHM7JfmG99/kZk9amYeM4sxs91mNsXMvjazOWY21Mw+MrN1ZnaWf9kJZvaG//WVZvaHANd7t5l9hW9coz+aWY5/fO7HzOcifMNRz/QvH2dmuVWurD7ezN73P7/bzB43s/fwDVYWY2Z/9W97sZlNaPjfqkQjhbtEDP+AcecBJ/gHkovBN5QDQBow1z+YWSlwF77L1i8E/rfKaob4lxkIXGpm/QNY79fOuSHOuc+Bh5xzg4E+/tdGO+dmAouAi5xvPPWaDhsNAM52zo0HJuIbUG4IMBjfIGzta/P7EalKx9wlkvwMXwDO9w05QiK+S+0Bipxz7/mfL8E3TGy5mS0BOlRZxxzn3C4AM5sFnIjv/8Hh1lvKj0MtAJxmZpOBBKAZsAD491H2403nXLH/+RnAcWZW9cOkK75L0kVqTeEukcSAp51zdxw00ywGXwjvV4nvDl77n1f9d37ol0yuhvUWOf8XU/5xW/4BDHTO5ZnZ3fhCvjrl/PiX8aFt9h7Sp1875z5AJIh0WEYiyfvAODNrBr6zampxCOMM890zNQnfmOHzjmK9ifg+LLb7R8W8oMprBUBqlekN+G51xyHtDjUH+LX/g2T/fVATj7JPIj+hPXeJGM65Jf7RAt83Mw++UfYmAZuOYjWfAi8CnYHn95/dEsh6nXM7zOxZfMMbfwd8WeXlZ4CnzKwI33H9u4AnzWwL8NUR6nkc38iAi/yHhLbi+9ARqROdCimNhv9MlN7OuZtDXYtIfdNhGRGRKKQ9dxGRKKQ9dxGRKKRwFxGJQgp3EZEopHAXEYlCCncRkSj0/wHRUJwHFwSFegAAAABJRU5ErkJggg==\n",
+ "text/plain": [
+ "
"
+ ]
+ },
+ "metadata": {
+ "needs_background": "light"
+ },
+ "output_type": "display_data"
+ }
+ ],
+ "source": [
+ "%matplotlib inline\n",
+ "data_pred = pd.DataFrame({'Temperature': np.linspace(start=30, stop=90, num=121), 'Intercept': 1})\n",
+ "data_pred['Frequency'] = logmodel.predict(data_pred[['Intercept','Temperature']])\n",
+ "data_pred.plot(x=\"Temperature\",y=\"Frequency\",kind=\"line\",ylim=[0,1])\n",
+ "plt.scatter(x=data[\"Temperature\"],y=data[\"Frequency\"])\n",
+ "plt.grid(True)"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false,
+ "scrolled": true
+ },
+ "source": [
+ "~~Comme on pouvait s'attendre au vu des données initiales, la\n",
+ "température n'a pas d'impact notable sur la probabilité d'échec des\n",
+ "joints toriques. Elle sera d'environ 0.2, comme dans les essais\n",
+ "précédents où nous il y a eu défaillance d'au moins un joint. Revenons\n",
+ "à l'ensemble des données initiales pour estimer la probabilité de\n",
+ "défaillance d'un joint:~~La température semble avoir un effet vraiment important, puisque la fréquence d'échec du joint semble être de l'ordre de 0.85 avec cependant de grandes incertitudes. **Ne pas tenir compte de ce qui se trouve ci-dessous.**\n"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 14,
+ "metadata": {},
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "0.06521739130434782\n"
+ ]
+ }
+ ],
+ "source": [
+ "data = pd.read_csv(\"shuttle.csv\")\n",
+ "print(np.sum(data.Malfunction)/np.sum(data.Count))"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "Cette probabilité est donc d'environ $p=0.065$, sachant qu'il existe\n",
+ "un joint primaire un joint secondaire sur chacune des trois parties du\n",
+ "lançeur, la probabilité de défaillance des deux joints d'un lançeur\n",
+ "est de $p^2 \\approx 0.00425$. La probabilité de défaillance d'un des\n",
+ "lançeur est donc de $1-(1-p^2)^3 \\approx 1.2%$. Ça serait vraiment\n",
+ "pas de chance... Tout est sous contrôle, le décollage peut donc avoir\n",
+ "lieu demain comme prévu.\n",
+ "\n",
+ "Seulement, le lendemain, la navette Challenger explosera et emportera\n",
+ "avec elle ses sept membres d'équipages. L'opinion publique est\n",
+ "fortement touchée et lors de l'enquête qui suivra, la fiabilité des\n",
+ "joints toriques sera directement mise en cause. Au delà des problèmes\n",
+ "de communication interne à la NASA qui sont pour beaucoup dans ce\n",
+ "fiasco, l'analyse précédente comporte (au moins) un petit\n",
+ "problème... Saurez-vous le trouver ? Vous êtes libre de modifier cette\n",
+ "analyse et de regarder ce jeu de données sous tous les angles afin\n",
+ "d'expliquer ce qui ne va pas."
+ ]
+ }
+ ],
+ "metadata": {
+ "celltoolbar": "Hide code",
+ "kernelspec": {
+ "display_name": "Python 3",
+ "language": "python",
+ "name": "python3"
+ },
+ "language_info": {
+ "codemirror_mode": {
+ "name": "ipython",
+ "version": 3
+ },
+ "file_extension": ".py",
+ "mimetype": "text/x-python",
+ "name": "python",
+ "nbconvert_exporter": "python",
+ "pygments_lexer": "ipython3",
+ "version": "3.6.4"
+ }
+ },
+ "nbformat": 4,
+ "nbformat_minor": 2
+}
diff --git a/module3/exo2/exercice.ipynb b/module3/exo2/exercice.ipynb
index 0bbbe371b01e359e381e43239412d77bf53fb1fb..dca166a653a7e4fa951948972c3169a05f34b13c 100644
--- a/module3/exo2/exercice.ipynb
+++ b/module3/exo2/exercice.ipynb
@@ -1,6 +1,2271 @@
{
- "cells": [],
+ "cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false
+ },
+ "source": [
+ "# Incidence de la varicelle"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false
+ },
+ "source": [
+ "## Chargement des données"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 32,
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false
+ },
+ "outputs": [],
+ "source": [
+ "%matplotlib inline\n",
+ "import pandas as pd\n",
+ "import matplotlib.pyplot as plt\n",
+ "import isoweek"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false
+ },
+ "source": [
+ "On commence par récupérer les données depuis le site [Réseau Sentinelles](https://www.sentiweb.fr/france/fr/?) en naviguant dans le menu de gauche: `Surveillance continue`-> `Bases de données` puis `Accès aux données`. On sélectionne `Varicelle (1991 - en cours)` dans le menu déroulant intitulé `Maladie/Indicateur` puis, dans l'onglet `Télécharger` on prend soin de télécharger les données au format CSV afin de déterminer l'URL permettant d'accéder à ces données. Celle-ci est stockée sous la forme d'une chaîne de caractères dans la variable suivante:"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 33,
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false
+ },
+ "outputs": [],
+ "source": [
+ "data_url = \"https://www.sentiweb.fr/datasets/incidence-PAY-7.csv\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false
+ },
+ "source": [
+ "La lecture des données brutes donne:"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 34,
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false
+ },
+ "outputs": [
+ {
+ "data": {
+ "text/html": [
+ "
"
+ ],
+ "text/plain": [
+ "Empty DataFrame\n",
+ "Columns: [week, indicator, inc, inc_low, inc_up, inc100, inc100_low, inc100_up, geo_insee, geo_name]\n",
+ "Index: []"
+ ]
+ },
+ "execution_count": 35,
+ "metadata": {},
+ "output_type": "execute_result"
+ }
+ ],
+ "source": [
+ "missing_lines = raw_data[raw_data.isnull().any(axis=1)]\n",
+ "missing_lines"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false
+ },
+ "source": [
+ "On voit que la variable `missing_lines` est vide, ce qui indique que le jeux de données ne souffre pas de \"trous\". On copie le jeu de données dans une nouvelle variable, qui est celle sur laquelle les traitements seront effectués:"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 36,
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false
+ },
+ "outputs": [],
+ "source": [
+ "data = raw_data"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false
+ },
+ "source": [
+ "Ensuite, on reformule la numérotation des semaines. En effet, dans le tableau ci-dessus, les semaines sont numérotées avec six chiffres: les quatres premiers chiffres correspondent à l'année, et les deux derniers au numéro de la semaine, ce qui donne l'impression à `pandas` qu'il s'agit d'un entier alors que ce n'est pas le cas. De plus, une telle numérotation ne peut pas être interprétée par `pandas`, il faut donc la reformuler. Cela est réalisé avec la librairie `isoweek`. On écrit une fonction `conversionDate`qui sera appliquée à l'ensemble de la première colonne du jeu de données:"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 40,
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false
+ },
+ "outputs": [],
+ "source": [
+ "def conversionDate(dateInt):\n",
+ " \n",
+ " dateStr = str(dateInt)\n",
+ " annee = int(dateStr[:4])\n",
+ " semaine = int(dateStr[4:])\n",
+ " s = isoweek.Week(annee, semaine)\n",
+ " return pd.Period(s.day(0), 'W')"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 41,
+ "metadata": {
+ "hideCode": false,
+ "hidePrompt": false
+ },
+ "outputs": [
+ {
+ "data": {
+ "text/html": [
+ "