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		<title>Thakshashila: Created page with &quot;= Gauss&#039;s Law (Electric): Definition and Mathematical Representation =  == Introduction == &#039;&#039;&#039;Gauss’s Law&#039;&#039;&#039; is a fundamental law in electrostatics that relates the electric flux through a closed surface to the total electric charge enclosed by that surface. It is one of the four equations in Maxwell&#039;s Equations and provides a powerful method for calculating electric fields, especially with high symmetry.  == Mathematical Formulation ==  === Integral Form === &lt;math...&quot;</title>
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		<summary type="html">&lt;p&gt;Created page with &amp;quot;= Gauss&amp;#039;s Law (Electric): Definition and Mathematical Representation =  == Introduction == &amp;#039;&amp;#039;&amp;#039;Gauss’s Law&amp;#039;&amp;#039;&amp;#039; is a fundamental law in electrostatics that relates the electric flux through a closed surface to the total electric charge enclosed by that surface. It is one of the four equations in &lt;a href=&quot;/index.php?title=Maxwell%27s_Equations&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;Maxwell&amp;#039;s Equations (page does not exist)&quot;&gt;Maxwell&amp;#039;s Equations&lt;/a&gt; and provides a powerful method for calculating electric fields, especially with high symmetry.  == Mathematical Formulation ==  === Integral Form === &amp;lt;math...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;= Gauss&amp;#039;s Law (Electric): Definition and Mathematical Representation =&lt;br /&gt;
&lt;br /&gt;
== Introduction ==&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Gauss’s Law&amp;#039;&amp;#039;&amp;#039; is a fundamental law in electrostatics that relates the electric flux through a closed surface to the total electric charge enclosed by that surface. It is one of the four equations in [[Maxwell&amp;#039;s Equations]] and provides a powerful method for calculating electric fields, especially with high symmetry.&lt;br /&gt;
&lt;br /&gt;
== Mathematical Formulation ==&lt;br /&gt;
&lt;br /&gt;
=== Integral Form ===&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\oint_{\text{closed surface}} \vec{E} \cdot d\vec{A} = \frac{Q_{\text{enc}}}{\varepsilon_0}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Where:&lt;br /&gt;
* &amp;lt;math&amp;gt;\vec{E}&amp;lt;/math&amp;gt; is the electric field vector,&lt;br /&gt;
* &amp;lt;math&amp;gt;d\vec{A}&amp;lt;/math&amp;gt; is an infinitesimal area vector on the closed surface (pointing outward),&lt;br /&gt;
* &amp;lt;math&amp;gt;Q_{\text{enc}}&amp;lt;/math&amp;gt; is the total electric charge enclosed within the surface,&lt;br /&gt;
* &amp;lt;math&amp;gt;\varepsilon_0&amp;lt;/math&amp;gt; is the vacuum permittivity (&amp;lt;math&amp;gt;\varepsilon_0 \approx 8.854 \times 10^{-12}\, \text{C}^2/\text{N·m}^2&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
=== Differential Form ===&lt;br /&gt;
Using the divergence theorem, Gauss&amp;#039;s Law can also be expressed in differential form:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\nabla \cdot \vec{E} = \frac{\rho}{\varepsilon_0}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Where:&lt;br /&gt;
* &amp;lt;math&amp;gt;\nabla \cdot \vec{E}&amp;lt;/math&amp;gt; is the divergence of the electric field,&lt;br /&gt;
* &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt; is the volume charge density (charge per unit volume).&lt;br /&gt;
&lt;br /&gt;
== Physical Meaning ==&lt;br /&gt;
Gauss&amp;#039;s Law states that the total electric flux through a closed surface is proportional to the amount of electric charge enclosed within that surface. The law implies:&lt;br /&gt;
&lt;br /&gt;
* A net outward flux occurs when positive charge is enclosed.&lt;br /&gt;
* A net inward flux occurs when negative charge is enclosed.&lt;br /&gt;
* If no charge is enclosed, the net electric flux is zero.&lt;br /&gt;
&lt;br /&gt;
== Applications of Gauss’s Law ==&lt;br /&gt;
&lt;br /&gt;
Gauss’s Law is especially useful when dealing with problems involving symmetry:&lt;br /&gt;
&lt;br /&gt;
=== 1. Spherical Symmetry ===&lt;br /&gt;
For a point charge &amp;lt;math&amp;gt;q&amp;lt;/math&amp;gt; at the center of a spherical surface of radius &amp;lt;math&amp;gt;r&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
E \cdot 4\pi r^2 = \frac{q}{\varepsilon_0} \quad \Rightarrow \quad E = \frac{1}{4\pi\varepsilon_0} \cdot \frac{q}{r^2}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== 2. Cylindrical Symmetry ===&lt;br /&gt;
For an infinite line charge with linear charge density &amp;lt;math&amp;gt;\lambda&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
E \cdot (2\pi r L) = \frac{\lambda L}{\varepsilon_0} \quad \Rightarrow \quad E = \frac{\lambda}{2\pi \varepsilon_0 r}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== 3. Planar Symmetry ===&lt;br /&gt;
For an infinite plane of surface charge density &amp;lt;math&amp;gt;\sigma&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
E = \frac{\sigma}{2 \varepsilon_0}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Conditions for Application ==&lt;br /&gt;
&lt;br /&gt;
* Symmetry is essential — spherical, cylindrical, or planar.&lt;br /&gt;
* The electric field must be constant in magnitude over the chosen Gaussian surface.&lt;br /&gt;
* The surface must be closed.&lt;br /&gt;
&lt;br /&gt;
== Relation to Coulomb&amp;#039;s Law ==&lt;br /&gt;
&lt;br /&gt;
Gauss’s Law is consistent with [[Coulomb’s Law]] and can be derived from it for point charges. Conversely, Coulomb’s Law can also be derived from Gauss’s Law under the assumption of spherical symmetry.&lt;br /&gt;
&lt;br /&gt;
== See Also ==&lt;br /&gt;
* [[Electric Field]]&lt;br /&gt;
* [[Electric Flux]]&lt;br /&gt;
* [[Coulomb&amp;#039;s Law]]&lt;br /&gt;
* [[Maxwell&amp;#039;s Equations]]&lt;br /&gt;
* [[Charge Density]]&lt;br /&gt;
* [[Vacuum Permittivity]]&lt;br /&gt;
* [[Electrostatics]]&lt;/div&gt;</summary>
		<author><name>Thakshashila</name></author>
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