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	<title>Complex Impedance - Revision history</title>
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	<updated>2026-04-28T02:56:40Z</updated>
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		<id>http://openelectrical.org/index.php?title=Complex_Impedance&amp;diff=8&amp;oldid=prev</id>
		<title>Jules: Created page with &quot;Complex impedances are commonly used quantities in the analysis of AC power systems. A complex impedance is represented by the following relation:  : &lt;math&gt; Z = R + jX \, &lt;/ma...&quot;</title>
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		<updated>2020-11-16T13:50:54Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;Complex impedances are commonly used quantities in the analysis of AC power systems. A complex impedance is represented by the following relation:  : &amp;lt;math&amp;gt; Z = R + jX \, &amp;lt;/ma...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;Complex impedances are commonly used quantities in the analysis of AC power systems. A complex impedance is represented by the following relation:&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt; Z = R + jX \, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Where &amp;lt;math&amp;gt; Z \, &amp;lt;/math&amp;gt; is the complex impedance (&amp;lt;math&amp;gt; \Omega &amp;lt;/math&amp;gt;)&lt;br /&gt;
:: &amp;lt;math&amp;gt; R \, &amp;lt;/math&amp;gt; is the resistance (&amp;lt;math&amp;gt; \Omega &amp;lt;/math&amp;gt;)&lt;br /&gt;
:: &amp;lt;math&amp;gt; X \, &amp;lt;/math&amp;gt; is the reactance (&amp;lt;math&amp;gt; \Omega &amp;lt;/math&amp;gt;)&lt;br /&gt;
:: &amp;lt;math&amp;gt; j \, &amp;lt;/math&amp;gt; is the complex component, i.e. &amp;lt;math&amp;gt; \sqrt{-1} \, &amp;lt;/math&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
For more details about why complex quantities are used in electrical engineering, see the article on [[Complex_Electrical_Quantities|complex electrical quantities]].&lt;br /&gt;
&lt;br /&gt;
== Complex Arithmetic ==&lt;br /&gt;
&lt;br /&gt;
The manipulation of complex impedances follow the rules of complex arithmetic. &lt;br /&gt;
&lt;br /&gt;
=== Series Impedances ===&lt;br /&gt;
&lt;br /&gt;
Two impedances in series can be combined by simply adding the individual real and complex terms (i.e. resistance and reactance components). For example, given:&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt; Z_{1} = R_{1} + jX_{1} \, &amp;lt;/math&amp;gt;&lt;br /&gt;
: &amp;lt;math&amp;gt; Z_{2} = R_{2} + jX_{2} \, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Then,&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt; Z_{1} + Z_{2} = R_{1} + R_{2} + j \left( X_{1} + X_{2} \right) \, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Parallel Impedances ===&lt;br /&gt;
&lt;br /&gt;
Two impedances in parallel can be combined according to the following standard relation:&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt; Z_{1} || Z_{2} = \frac{Z_{1} Z_{2}}{Z_{1} + Z_{2}} \, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
However, note that the multiplication and division of complex numbers is more involved than simply multiplying or dividing the real and complex terms:&lt;br /&gt;
&lt;br /&gt;
* '''Multiplication:''' involves multiplying cross-terms, i.e.&lt;br /&gt;
: &amp;lt;math&amp;gt; Z_{1} \times Z_{2} = \left( R_{1} + jX_{1} \right) \left( R_{2} + jX_{2} \right) \, &amp;lt;/math&amp;gt;&lt;br /&gt;
::: &amp;lt;math&amp;gt; = R_{1} R_{2} + j^{2} X_{1} X_{2} +j \left( R_{1} X_{2} \right) +j \left( X_{1} R_{2} \right) \, &amp;lt;/math&amp;gt;&lt;br /&gt;
::: &amp;lt;math&amp;gt; = R_{1} R_{2} - X_{1} X_{2} +j \left( R_{1} X_{2} + X_{1} R_{2} \right) \, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* '''Division:''' involves multiplying by the complex conjugate of the denominator, i.e&lt;br /&gt;
: &amp;lt;math&amp;gt; \frac{Z_{1}}{Z_{2}} = \frac{\left( R_{1} + jX_{1} \right)}{\left( R_{2} + jX_{2} \right)} \, &amp;lt;/math&amp;gt;&lt;br /&gt;
::: &amp;lt;math&amp;gt; = \frac{\left( R_{1} + jX_{1} \right)}{\left( R_{2} + jX_{2} \right)} \times \frac{\left( R_{2} - jX_{2} \right)}{\left( R_{2} - jX_{2} \right)} \, &amp;lt;/math&amp;gt;&lt;br /&gt;
::: &amp;lt;math&amp;gt; = \frac{R_{1} R_{2} + X_{1} X_{2} +j \left( R_{1} X_{2} - X_{1} R_{2} \right)}{\left( R_{2}^{2} + X_{2}^{2} \right)} \, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Category:Fundamentals]]&lt;/div&gt;</summary>
		<author><name>Jules</name></author>
	</entry>
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