Skip to content

Commit cc03d69

Browse files
steven-jasteven-ja
committed
errata corrige notes
1 parent 93fb61f commit cc03d69

File tree

8 files changed

+30
-35
lines changed

8 files changed

+30
-35
lines changed

‎content/notes/physics/electromagnetism/index.md‎

Lines changed: 3 additions & 2 deletions
Original file line numberDiff line numberDiff line change
@@ -9,7 +9,7 @@ menu:
99
weight: 10
1010
---
1111
<!-- A Sample Program -->
12-
{{< note title="Maxwell Equation (Integral)">}}
12+
{{< note title="Maxwell Equations (Integral)">}}
1313
1. **Gauss' Law**:
1414

1515
$$ \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$
@@ -26,12 +26,13 @@ $$ \oint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{l} = -\frac{d}{dt} \\int_{\
2626
$$ \oint_{\partial \Omega} \mathbf{B} \cdot d\mathbf{l} = \mu_0 \left(\iint_{\Sigma} \mathbf{J} \cdot d\mathbf{S} + \epsilon_0 \frac{d}{dt} \iint_{\Sigma} \mathbf{E} \cdot d\mathbf{S}\right) $$
2727
{{< /note >}}
2828

29-
{{< note title="Maxwell Equation (Differential)">}}
29+
{{< note title="Maxwell Equations (Differential)">}}
3030
1. **Gauss' Law**:
3131

3232
$$ \nabla \cdot \mathbf{E} = \frac{\rho}{\epsilon_0} $$
3333

3434
2. **Gauss' Law for Magnetism**:
35+
3536
$$ \nabla \cdot \mathbf{B} = 0 $$
3637

3738
3. **Maxwell-Faraday Equation**:

‎public/index.json‎

Lines changed: 1 addition & 1 deletion
Large diffs are not rendered by default.

‎public/index.xml‎

Lines changed: 1 addition & 1 deletion
Original file line numberDiff line numberDiff line change
@@ -128,7 +128,7 @@ To achieve this, we will utilize the yfinance library to fetch stock information
128128
<pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
129129

130130
<guid>http://localhost:1313/notes/physics/electromagnetism/</guid>
131-
<description>Maxwell Equation (Integral) Gauss&amp;rsquo; Law: $$ \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$
131+
<description>Maxwell Equations (Integral) Gauss&amp;rsquo; Law: $$ \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$
132132
Gauss&amp;rsquo; Law for Magnetism: $$ \iint_{\partial \Omega} \mathbf{B} \cdot d\mathbf{S} = 0 $$
133133
Maxwell-Faraday Equation:
134134
$$ \oint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{l} = -\frac{d}{dt} \int_{\Sigma} \mathbf{B} \cdot d\mathbf{S} $$

‎public/notes/index.html‎

Lines changed: 7 additions & 9 deletions
Original file line numberDiff line numberDiff line change
@@ -293,7 +293,7 @@
293293
<!-- A Sample Program -->
294294
<div class="note-card ">
295295
<div class="item">
296-
<h5 class="note-title"><span>Maxwell Equation (Integral)</span></h5>
296+
<h5 class="note-title"><span>Maxwell Equations (Integral)</span></h5>
297297

298298
<div class="card">
299299
<div class="card-body"><ol>
@@ -322,21 +322,19 @@ <h5 class="note-title"><span>Maxwell Equation (Integral)</span></h5>
322322

323323
<div class="note-card ">
324324
<div class="item">
325-
<h5 class="note-title"><span>Maxwell Equation (Differential)</span></h5>
325+
<h5 class="note-title"><span>Maxwell Equations (Differential)</span></h5>
326326

327327
<div class="card">
328328
<div class="card-body"><ol>
329329
<li><strong>Gauss&rsquo; Law</strong>:</li>
330330
</ol>
331331
<p>$$ \nabla \cdot \mathbf{E} = \frac{\rho}{\epsilon_0} $$</p>
332332
<ol start="2">
333-
<li>
334-
<p><strong>Gauss&rsquo; Law for Magnetism</strong>:
335-
$$ \nabla \cdot \mathbf{B} = 0 $$</p>
336-
</li>
337-
<li>
338-
<p><strong>Maxwell-Faraday Equation</strong>:</p>
339-
</li>
333+
<li><strong>Gauss&rsquo; Law for Magnetism</strong>:</li>
334+
</ol>
335+
<p>$$ \nabla \cdot \mathbf{B} = 0 $$</p>
336+
<ol start="3">
337+
<li><strong>Maxwell-Faraday Equation</strong>:</li>
340338
</ol>
341339
<p>$$ \nabla \times \mathbf{E} = \frac{\partial \mathbf{B}}{\partial t} $$</p>
342340
<ol start="4">

‎public/notes/index.xml‎

Lines changed: 1 addition & 1 deletion
Original file line numberDiff line numberDiff line change
@@ -24,7 +24,7 @@
2424
<pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
2525

2626
<guid>http://localhost:1313/notes/physics/electromagnetism/</guid>
27-
<description>Maxwell Equation (Integral) Gauss&amp;rsquo; Law: $$ \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$
27+
<description>Maxwell Equations (Integral) Gauss&amp;rsquo; Law: $$ \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$
2828
Gauss&amp;rsquo; Law for Magnetism: $$ \iint_{\partial \Omega} \mathbf{B} \cdot d\mathbf{S} = 0 $$
2929
Maxwell-Faraday Equation:
3030
$$ \oint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{l} = -\frac{d}{dt} \int_{\Sigma} \mathbf{B} \cdot d\mathbf{S} $$

‎public/notes/physics/electromagnetism/index.html‎

Lines changed: 9 additions & 11 deletions
Original file line numberDiff line numberDiff line change
@@ -26,7 +26,7 @@
2626
<meta property="og:url" content="http://localhost:1313/notes/physics/electromagnetism/">
2727
<meta property="og:site_name" content="Stefano Giannini">
2828
<meta property="og:title" content="Electromagnetism">
29-
<meta property="og:description" content="Maxwell Equation (Integral) Gauss’ Law: $$ \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$
29+
<meta property="og:description" content="Maxwell Equations (Integral) Gauss’ Law: $$ \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$
3030
Gauss’ Law for Magnetism: $$ \iint_{\partial \Omega} \mathbf{B} \cdot d\mathbf{S} = 0 $$
3131
Maxwell-Faraday Equation:
3232
$$ \oint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{l} = -\frac{d}{dt} \int_{\Sigma} \mathbf{B} \cdot d\mathbf{S} $$
@@ -38,7 +38,7 @@
3838

3939
<meta name="twitter:card" content="summary">
4040
<meta name="twitter:title" content="Electromagnetism">
41-
<meta name="twitter:description" content="Maxwell Equation (Integral) Gauss’ Law: $$ \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$
41+
<meta name="twitter:description" content="Maxwell Equations (Integral) Gauss’ Law: $$ \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$
4242
Gauss’ Law for Magnetism: $$ \iint_{\partial \Omega} \mathbf{B} \cdot d\mathbf{S} = 0 $$
4343
Maxwell-Faraday Equation:
4444
$$ \oint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{l} = -\frac{d}{dt} \int_{\Sigma} \mathbf{B} \cdot d\mathbf{S} $$
@@ -307,7 +307,7 @@
307307
<!-- A Sample Program -->
308308
<div class="note-card ">
309309
<div class="item">
310-
<h5 class="note-title"><span>Maxwell Equation (Integral)</span></h5>
310+
<h5 class="note-title"><span>Maxwell Equations (Integral)</span></h5>
311311

312312
<div class="card">
313313
<div class="card-body"><ol>
@@ -336,21 +336,19 @@ <h5 class="note-title"><span>Maxwell Equation (Integral)</span></h5>
336336

337337
<div class="note-card ">
338338
<div class="item">
339-
<h5 class="note-title"><span>Maxwell Equation (Differential)</span></h5>
339+
<h5 class="note-title"><span>Maxwell Equations (Differential)</span></h5>
340340

341341
<div class="card">
342342
<div class="card-body"><ol>
343343
<li><strong>Gauss&rsquo; Law</strong>:</li>
344344
</ol>
345345
<p>$$ \nabla \cdot \mathbf{E} = \frac{\rho}{\epsilon_0} $$</p>
346346
<ol start="2">
347-
<li>
348-
<p><strong>Gauss&rsquo; Law for Magnetism</strong>:
349-
$$ \nabla \cdot \mathbf{B} = 0 $$</p>
350-
</li>
351-
<li>
352-
<p><strong>Maxwell-Faraday Equation</strong>:</p>
353-
</li>
347+
<li><strong>Gauss&rsquo; Law for Magnetism</strong>:</li>
348+
</ol>
349+
<p>$$ \nabla \cdot \mathbf{B} = 0 $$</p>
350+
<ol start="3">
351+
<li><strong>Maxwell-Faraday Equation</strong>:</li>
354352
</ol>
355353
<p>$$ \nabla \times \mathbf{E} = \frac{\partial \mathbf{B}}{\partial t} $$</p>
356354
<ol start="4">

‎public/notes/physics/index.html‎

Lines changed: 7 additions & 9 deletions
Original file line numberDiff line numberDiff line change
@@ -298,7 +298,7 @@
298298
<!-- A Sample Program -->
299299
<div class="note-card ">
300300
<div class="item">
301-
<h5 class="note-title"><span>Maxwell Equation (Integral)</span></h5>
301+
<h5 class="note-title"><span>Maxwell Equations (Integral)</span></h5>
302302

303303
<div class="card">
304304
<div class="card-body"><ol>
@@ -327,21 +327,19 @@ <h5 class="note-title"><span>Maxwell Equation (Integral)</span></h5>
327327

328328
<div class="note-card ">
329329
<div class="item">
330-
<h5 class="note-title"><span>Maxwell Equation (Differential)</span></h5>
330+
<h5 class="note-title"><span>Maxwell Equations (Differential)</span></h5>
331331

332332
<div class="card">
333333
<div class="card-body"><ol>
334334
<li><strong>Gauss&rsquo; Law</strong>:</li>
335335
</ol>
336336
<p>$$ \nabla \cdot \mathbf{E} = \frac{\rho}{\epsilon_0} $$</p>
337337
<ol start="2">
338-
<li>
339-
<p><strong>Gauss&rsquo; Law for Magnetism</strong>:
340-
$$ \nabla \cdot \mathbf{B} = 0 $$</p>
341-
</li>
342-
<li>
343-
<p><strong>Maxwell-Faraday Equation</strong>:</p>
344-
</li>
338+
<li><strong>Gauss&rsquo; Law for Magnetism</strong>:</li>
339+
</ol>
340+
<p>$$ \nabla \cdot \mathbf{B} = 0 $$</p>
341+
<ol start="3">
342+
<li><strong>Maxwell-Faraday Equation</strong>:</li>
345343
</ol>
346344
<p>$$ \nabla \times \mathbf{E} = \frac{\partial \mathbf{B}}{\partial t} $$</p>
347345
<ol start="4">

‎public/notes/physics/index.xml‎

Lines changed: 1 addition & 1 deletion
Original file line numberDiff line numberDiff line change
@@ -11,7 +11,7 @@
1111
<pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
1212

1313
<guid>http://localhost:1313/notes/physics/electromagnetism/</guid>
14-
<description>Maxwell Equation (Integral) Gauss&amp;rsquo; Law: $$ \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$
14+
<description>Maxwell Equations (Integral) Gauss&amp;rsquo; Law: $$ \iint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{S} = 4 \pi \iiint_{\Omega} \rho dV $$
1515
Gauss&amp;rsquo; Law for Magnetism: $$ \iint_{\partial \Omega} \mathbf{B} \cdot d\mathbf{S} = 0 $$
1616
Maxwell-Faraday Equation:
1717
$$ \oint_{\partial \Omega} \mathbf{E} \cdot d\mathbf{l} = -\frac{d}{dt} \int_{\Sigma} \mathbf{B} \cdot d\mathbf{S} $$

0 commit comments

Comments
 (0)