1 | var md = require('markdown-it')(),
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2 | mk = require('./index');
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3 |
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4 | md.use(mk);
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5 |
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6 | var input = document.getElementById('input'),
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7 | output = document.getElementById('output'),
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8 | button = document.getElementById('button');
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9 |
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10 | button.addEventListener('click', function(ev){
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11 |
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12 | var result = md.render(input.value);
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13 |
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14 | output.innerHTML = result;
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15 |
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16 | });
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17 |
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18 | /*
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19 |
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20 | # Some Math
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21 |
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22 | $\sqrt{3x-1}+(1+x)^2$
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23 |
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24 | # Maxwells Equations
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25 |
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26 | $\nabla \times \vec{\mathbf{B}} -\, \frac1c\, \frac{\partial\vec{\mathbf{E}}}{\partial t}
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27 | = \frac{4\pi}{c}\vec{\mathbf{j}} \nabla \cdot \vec{\mathbf{E}} = 4 \pi \rho$
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28 |
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29 | $\nabla \times \vec{\mathbf{E}}\, +\, \frac1c\, \frac{\partial\vec{\mathbf{B}}}{\partial t} = \vec{\mathbf{0}}$ (curl of $\vec{\mathbf{E}}$ is proportional to the time derivative of $\vec{\mathbf{B}}$)
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30 |
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31 | $\nabla \cdot \vec{\mathbf{B}} = 0$
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32 |
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33 |
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34 |
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35 | \sqrt{3x-1}+(1+x)^2
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36 |
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37 | c = \pm\sqrt{a^2 + b^2}
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38 |
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39 | Maxwell's Equations
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40 |
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41 | \nabla \times \vec{\mathbf{B}} -\, \frac1c\, \frac{\partial\vec{\mathbf{E}}}{\partial t}
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42 | = \frac{4\pi}{c}\vec{\mathbf{j}} \nabla \cdot \vec{\mathbf{E}} = 4 \pi \rho
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43 |
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44 | \nabla \times \vec{\mathbf{E}}\, +\, \frac1c\, \frac{\partial\vec{\mathbf{B}}}{\partial t} = \vec{\mathbf{0}}
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45 |
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46 | \nabla \cdot \vec{\mathbf{B}} = 0
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47 |
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48 | Same thing in a LaTeX array
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49 | \begin{array}{c}
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50 |
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51 | \nabla \times \vec{\mathbf{B}} -\, \frac1c\, \frac{\partial\vec{\mathbf{E}}}{\partial t} &
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52 | = \frac{4\pi}{c}\vec{\mathbf{j}} \nabla \cdot \vec{\mathbf{E}} & = 4 \pi \rho \\
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53 |
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54 | \nabla \times \vec{\mathbf{E}}\, +\, \frac1c\, \frac{\partial\vec{\mathbf{B}}}{\partial t} & = \vec{\mathbf{0}} \\
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55 |
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56 | \nabla \cdot \vec{\mathbf{B}} & = 0
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57 |
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58 | \end{array}
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59 |
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60 |
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61 | \begin{array}{c}
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62 | y_1 \\
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63 | y_2 \mathtt{t}_i \\
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64 | z_{3,4}
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65 | \end{array}
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66 |
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67 | \begin{array}{c}
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68 | x' &=& &x \sin\phi &+& z \cos\phi \\
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69 | z' &=& - &x \cos\phi &+& z \sin\phi \\
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70 | \end{array}
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71 |
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72 |
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73 |
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74 | # Maxwell's Equations
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75 |
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76 |
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77 | equation | description
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78 | ----------|------------
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79 | $\nabla \cdot \vec{\mathbf{B}} = 0$ | divergence of $\vec{\mathbf{B}}$ is zero
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80 | $\nabla \times \vec{\mathbf{E}}\, +\, \frac1c\, \frac{\partial\vec{\mathbf{B}}}{\partial t} = \vec{\mathbf{0}}$ | curl of $\vec{\mathbf{E}}$ is proportional to the rate of change of $\vec{\mathbf{B}}$
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81 | $\nabla \times \vec{\mathbf{B}} -\, \frac1c\, \frac{\partial\vec{\mathbf{E}}}{\partial t} = \frac{4\pi}{c}\vec{\mathbf{j}} \nabla \cdot \vec{\mathbf{E}} = 4 \pi \rho$ | wha?
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82 |
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83 | ![electricity](http://i.giphy.com/Gty2oDYQ1fih2.gif)
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84 | */
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