mirror of
https://github.com/peter-tanner/starcore-explorer-bad.git
synced 2024-12-02 18:10:28 +08:00
114 lines
36 KiB
Plaintext
114 lines
36 KiB
Plaintext
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{
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"cells": [
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{
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"cell_type": "markdown",
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"metadata": {
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"tags": []
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},
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"source": [
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"## Matplotlib"
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]
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},
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{
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"cell_type": "code",
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"execution_count": 1,
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"metadata": {},
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"outputs": [],
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"source": [
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"import numpy as np\n",
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"import matplotlib.pyplot as plt"
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]
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},
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{
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"cell_type": "code",
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"execution_count": 2,
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"metadata": {},
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"outputs": [],
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"source": [
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"x = np.linspace(0, 10, 1000)\n",
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"plt.plot(x, np.sin(x));"
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]
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},
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{
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"cell_type": "code",
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"execution_count": 3,
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"metadata": {},
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"outputs": [
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{
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"data": {
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"image/png": "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"text/plain": [
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"<pyolite.display.Image object at 0x254e300>"
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]
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},
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"metadata": {},
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"output_type": "display_data"
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}
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],
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"source": [
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"plt.show()"
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]
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},
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{
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"cell_type": "markdown",
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"metadata": {
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"tags": []
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},
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"source": [
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"## Matplotlib: support for widgets backend"
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]
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},
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{
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"cell_type": "code",
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"execution_count": null,
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"metadata": {},
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"outputs": [],
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"source": [
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"%pip install -q ipympl"
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]
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},
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{
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"cell_type": "code",
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"execution_count": null,
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"metadata": {},
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"outputs": [],
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"source": [
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"%matplotlib widget"
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]
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},
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{
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"cell_type": "code",
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"execution_count": null,
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"metadata": {},
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"outputs": [],
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"source": [
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"x = np.linspace(0, 10, 1000)\n",
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"plt.plot(x, np.sin(x))"
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]
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}
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],
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"metadata": {
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"kernelspec": {
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"display_name": "Python (Pyodide)",
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"language": "python",
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"name": "python"
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},
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"language_info": {
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"codemirror_mode": {
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"name": "python",
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"version": 3
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},
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"file_extension": ".py",
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"mimetype": "text/x-python",
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"name": "python",
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"nbconvert_exporter": "python",
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"pygments_lexer": "ipython3",
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"version": "3.8"
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},
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"orig_nbformat": 4,
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"toc-showcode": false
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},
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"nbformat": 4,
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"nbformat_minor": 4
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}
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