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		<title>Kirchhoff&#8217;s Current Law (KCL) Explained</title>
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		<pubDate>Wed, 24 Feb 2021 10:29:13 +0000</pubDate>
				<category><![CDATA[Network Analysis / Network Theory]]></category>
		<category><![CDATA[KCL]]></category>
		<category><![CDATA[KCL example]]></category>
		<category><![CDATA[Kirchhoff&#039;s circuit laws]]></category>
		<category><![CDATA[Kirchhoff&#039;s current law]]></category>
		<category><![CDATA[Kirchhoff&#039;s Current Law (KCL) Explained]]></category>
		<category><![CDATA[Kirchhoff&#039;s Current Law problems]]></category>
		<category><![CDATA[Kirchhoff&#039;s law]]></category>
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					<description><![CDATA[<p>Kirchhoff&#8217;s Current Law (KCL) is also known as Kirchhoff’s first law or Kirchhoff’s junction law. Statement : “Algebraic sum of branch currents at node is zero at all instance of time.” Or &#8220;At any node (junction) in a network, the sum of currents flowing into that node is equal to the sum of currents flowing ... <a title="Kirchhoff&#8217;s Current Law (KCL) Explained" class="read-more" href="https://www.allaboutelectronics.org/kirchhoffs-current-law-kcl-explained/">Read more<span class="screen-reader-text">Kirchhoff&#8217;s Current Law (KCL) Explained</span></a></p>
<p>The post <a href="https://www.allaboutelectronics.org/kirchhoffs-current-law-kcl-explained/">Kirchhoff&#8217;s Current Law (KCL) Explained</a> appeared first on <a href="https://www.allaboutelectronics.org">ALL ABOUT ELECTRONICS</a>.</p>
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<p>Kirchhoff&#8217;s Current Law (KCL) is also known as Kirchhoff’s first law or Kirchhoff’s junction law.</p>



<p class="has-text-color" style="color:#c90d74"><strong>Statement : </strong>“Algebraic sum of branch currents at node is zero at all instance of time.” </p>



<p class="has-text-align-center has-text-color" style="color:#c90d74">Or</p>



<p class="has-text-color" style="color:#c90d74">&#8220;At any node (junction) in a network, the sum of currents flowing into that node is equal to the sum of currents flowing out of that node.”</p>



<div class="wp-block-image"><figure class="aligncenter size-large"><a href="https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_1.png"><img fetchpriority="high" decoding="async" width="620" height="515" src="https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_1.png" alt="" class="wp-image-1534" srcset="https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_1.png 620w, https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_1-300x249.png 300w" sizes="(max-width: 620px) 100vw, 620px" /></a></figure></div>



<p class="has-text-align-center"><strong>Fig.1 Electrical Network with 5 branches</strong></p>



<p>To understand the statement, let&#8217;s consider one example. As shown in Fig. 1, the network has one node N and 5 branches. The current in five branches is<sub> </sub>I<sub>1, </sub>I<sub>2, </sub>I<sub>3, </sub>I<sub>4,</sub> and I<sub>5</sub>. The current I<sub>1</sub>, I<sub>2</sub>, and I<sub>3</sub> are entering the node N, while current I<sub>4</sub> and I<sub>5 </sub>are leaving the node. </p>



<h3 class="has-text-color wp-block-heading" style="color:#1500ad"><strong>Sign Convention</strong></h3>



<p>If current is entering the node, then consider it as positive current. Similarly, if current is leaving the node then it can be considered as negative current. The same is shown in Fig.2.</p>



<figure class="wp-block-image size-large is-resized"><a href="https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_2.png"><img decoding="async" src="https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_2.png" alt="" class="wp-image-1537" width="608" height="164" srcset="https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_2.png 981w, https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_2-300x81.png 300w, https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_2-768x207.png 768w" sizes="(max-width: 608px) 100vw, 608px" /></a></figure>



<p class="has-text-align-center"><strong>Fig.2 Sign Convention for Kirchhoff&#8217;s Current Law (KCL</strong>)</p>



<p>Therefore, for the network shown in Fig. 1, current I<sub>1</sub>, I<sub>2</sub>, and I<sub>3</sub> will be positive, while current I<sub>4</sub> and I<sub>5</sub> will be negative.</p>



<p>And according the Kirchhoff&#8217;s Current Law, the algebraic sum of all these current is zero.</p>



<p>Therefore, I<sub>1</sub> + I<sub>2 </sub>+ I<sub>3</sub> &#8211; I<sub>4</sub> &#8211; I<sub>5 </sub>= 0 </p>



<p><strong>∴</strong>  I<sub>1</sub> + I<sub>2</sub> + I<sub>3</sub> = I<sub>4</sub> + I<sub>5</sub>   &#8212;&#8212;-(1)</p>



<p>It shows that, the sum of currents entering the node is equal to the sum of currents leaving the node.</p>



<h3 class="has-text-color wp-block-heading" style="color:#1500a3"><strong>KCL is a law of Conservation of Charge</strong></h3>



<p>The current is the rate at which the charge is flowing. </p>



<p><strong>∴</strong> Current (I) = Q/t</p>



<p>Therefore, the equation 1 can be written as</p>



<figure class="wp-block-image size-large is-resized"><a href="https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_3.png"><img decoding="async" src="https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_3.png" alt="" class="wp-image-1540" width="326" height="98" srcset="https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_3.png 512w, https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_3-300x90.png 300w" sizes="(max-width: 326px) 100vw, 326px" /></a></figure>



<p>And further after the simplification, Q<sub>1</sub> + Q<sub>2</sub> + Q<sub>3</sub> = Q<sub>4 </sub>+ Q<sub>5</sub> &#8212;&#8212;&#8212;-(2)</p>



<p>Equation 2 shows that, the charge which is entering the node is equal to the charge which is leaving the node. </p>



<p>Therefore, Kirchhoff&#8217;s Current Law (KCL) is the law of conservation of charge. </p>



<h3 class="has-text-color wp-block-heading" style="color:#1500a3"><strong>Example</strong></h3>



<p>For the given circuit if, I<sub>2</sub> = 2A, I<sub>4</sub> = -1A and I<sub>5</sub> = -4A then find current I<sub>6</sub></p>



<figure class="wp-block-image size-large"><a href="https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_4-3.png"><img loading="lazy" decoding="async" width="990" height="588" src="https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_4-3.png" alt="" class="wp-image-1545" srcset="https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_4-3.png 990w, https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_4-3-300x178.png 300w, https://www.allaboutelectronics.org/wp-content/uploads/2021/02/KCL_4-3-768x456.png 768w" sizes="(max-width: 990px) 100vw, 990px" /></a></figure>



<p class="has-text-align-center"><strong>Fig. 3  Kirchhoff&#8217;s Current Law (KCL) Example </strong></p>



<h4 class="has-text-color wp-block-heading" style="color:#c90d74"><strong>Solution:</strong></h4>



<p>Applying KCL at node B, </p>



<p>I<sub>3 </sub>+ I<sub>6</sub> = I1  and I<sub>1</sub> = 2A (Given)</p>



<p><strong>∴</strong> I<sub>6</sub> = 2 &#8211; I<sub>3</sub>  &#8212;&#8212;&#8212; (3)</p>



<p>Similarly, applying KCL at node C,</p>



<p>I<sub>2</sub> + I<sub>5</sub> = I<sub>3</sub>    and I<sub>5</sub> = -4 A (Given)</p>



<p><strong>∴</strong> I<sub>3</sub> = I<sub>2</sub> &#8211; 4 &#8212;&#8212;&#8212;-(4)</p>



<p>Similarly, applying KCL at node A,</p>



<p>I<sub>1</sub> + I<sub>4</sub> = I<sub>2</sub>  and I<sub>4</sub> = -1 A and I<sub>1</sub> = 2A (Given)</p>



<p><strong>∴</strong>  <strong>I<sub>2</sub> = 2 -1 = 1A</strong></p>



<p>From equation 4, <strong>I<sub>3</sub> = 1 &#8211; 4 = -3A</strong></p>



<p>And by putting the value of I<sub>3 </sub>in equation 3,</p>



<p><strong>I<sub>6</sub> = 2 &#8211; (-3) = 5A</strong></p>



<p class="has-text-color" style="color:#c90d74">Therefore, for the given circuit, current I<sub>6</sub> = 5A</p>



<p>For more information on Kirchhoff&#8217;s Current Law (KCL) check this video:</p>



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