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| 29 | + <meta property="og:description" content="Maxwell Equation (Integral) Gauss’ Law: $$ \qquad \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$ |
| 30 | +Gauss’ Law for Magnetism $$ \qquad \iint_{\partial \Omega} \mathbf{B} \cdot d\mathbf{S} = 0 $$ "> |
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| 38 | + <meta name="twitter:description" content="Maxwell Equation (Integral) Gauss’ Law: $$ \qquad \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$ |
| 39 | +Gauss’ Law for Magnetism $$ \qquad \iint_{\partial \Omega} \mathbf{B} \cdot d\mathbf{S} = 0 $$ "> |
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| 328 | + <!-- A Sample Program --> |
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329 | 331 | <h5 class="note-title"><span>Maxwell Equation (Integral)</span></h5>
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330 | 332 |
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331 | 333 | <div class="card">
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| - <div class="card-body">$$\delta + 5 $$</div> |
| 334 | + <div class="card-body"><ul> |
| 335 | +<li><strong>Gauss’ Law</strong>:</li> |
| 336 | +</ul> |
| 337 | +<p>$$ \qquad \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$</p> |
| 338 | +<ul> |
| 339 | +<li><strong>Gauss’ Law for Magnetism</strong> |
| 340 | +$$ \qquad \iint_{\partial \Omega} \mathbf{B} \cdot d\mathbf{S} = 0 $$</li> |
| 341 | +</ul></div> |
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