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	<title>Durofy &#187; diode resistance</title>
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		<title>Semiconductor Devices - The Semiconductor Diode</title>
		<link>http://www.durofy.com/technology/the-semiconductor-diode/</link>
		<comments>http://www.durofy.com/technology/the-semiconductor-diode/#comments</comments>
		<pubDate>Wed, 26 Aug 2009 02:45:58 +0000</pubDate>
		<dc:creator>Rishabh Dev</dc:creator>
				<category><![CDATA[Technology]]></category>
		<category><![CDATA[Analog]]></category>
		<category><![CDATA[analog devices]]></category>
		<category><![CDATA[analog devices basics]]></category>
		<category><![CDATA[analog ectronic devices]]></category>
		<category><![CDATA[analog electronics basics]]></category>
		<category><![CDATA[diffusion diode capacitance]]></category>
		<category><![CDATA[diode as capacitor]]></category>
		<category><![CDATA[diode capacitance]]></category>
		<category><![CDATA[diode characterisctics]]></category>
		<category><![CDATA[diode current]]></category>
		<category><![CDATA[diode resistance]]></category>
		<category><![CDATA[electronic devices]]></category>
		<category><![CDATA[pn junction]]></category>
		<category><![CDATA[semiconductor diode]]></category>
		<category><![CDATA[transition diode capacitance]]></category>

		<guid isPermaLink="false">http://zarrata.com/durofy/?p=151</guid>
		<description><![CDATA[In the previous post on the P-N junction, we looked at the formation of a P-N junction. The resulting device is called a diode. The semiconductor diode is closest to the ideal diode. To study electronic devices made up of the P-N junctions, we look into their VI characteristics. The VI characteristics of a device [...]]]></description>
			<content:encoded><![CDATA[<p>In the <a href="http://www.durofy.com/technology/the-p-n-junction/">previous post on the P-N junction</a>, we looked at the formation of a P-N junction. The resulting device is called a diode.</p>
<p>The semiconductor diode is closest to the ideal diode. To study electronic devices made up of the P-N junctions, we look into their VI characteristics.</p>
<p>The VI characteristics of a device is simply a plot of the V vs I curve for the device. For instance, the resistor follows ohm's law &amp; hence, we obtain a liner VI characteristic for resistance.</p>
<p>The curve below shows the VI characteristics of an ideal &amp; a real diode...</p>
<p style="text-align: center;"><img class="aligncenter" src="https://lh5.googleusercontent.com/-4YNBDc8X2yU/T1QxaZ6HtfI/AAAAAAAAAjc/Nw4F_Rrj5LM/s497/analog10.jpg" alt="diode_charactersictics" /></p>
<p>The curve in the first quadrant represents the diode in its forward bias. The diode starts conducting at the voltage <strong>V<sub>c</sub></strong> called the <em>Cut In Voltage</em>. This voltage is about 0.6 V for Silicon &amp; 0.2 V for Germanium.</p>
<p>In case of the reverse bias, a small current flows. This current, independent of the applied voltage &amp; present only due to the minority charge carries, is called the reverse saturation current.</p>
<p>In reverse bias, the external applied voltage breaks the covalent bonds in the junction region. This leads to the breakdown of the junction at a specific voltage called the breakdown voltage(<strong>V <sub>b</sub></strong>).</p>
<p>Notice that we only consider V<sub>b</sub> in the real case. Hence, ideally, there should be almost no current in the reverse bias state, &amp; hence, no breakdown of the junction.</p>
<blockquote><p>The breakdown simply means that the diode now allows all the current to flow through it. It is just a malfunctioning of the diode &amp; not the damage of the diode. The diode is otherwise supposed to allow current through just one direction &amp; stop all the current in the other.</p></blockquote>
<p>Further, two kinds of resistances exist in the diode corresponding to the direct &amp; alternating currents respectively.</p>
<p style="text-align: center;"><img class="aligncenter" src="https://lh6.googleusercontent.com/-tTKYO8PHUzM/T1QxbPbBBHI/AAAAAAAAAjo/ohxz9RD7Gi8/s290/analog11.jpg" alt="diode_resistance" /></p>
<p>The diode can also behave as a capacitor, and even as a variable capacitor. There are two different ways of looking at a diode as a capacitor.</p>
<p style="text-align: center;"><img class="aligncenter" src="https://lh3.googleusercontent.com/-baS0nSzl4Cs/T1Qxb5kD-8I/AAAAAAAAAj4/EQG94iTGSVE/s514/analog12.jpg" alt="diode_capacitance" /></p>
<p>The current that flows through the diode depends upon the applied voltage &amp; the temperature(&amp; hence, the voltage due to the temperature). It is given by...</p>
<p style="text-align: center;"><img class="aligncenter" src="http://latex.codecogs.com/gif.latex?\200dpi%20I%20=%20I_{0}(e^{\frac{eV}{\eta%20kT}}-1)" alt="" width="227" height="43" /></p>
<p>where I<sub>0</sub> is the reverse saturation current, e is the electronic charge, k is the Boltzmann constant, V the applied voltage &amp; T is the temperature. The term kT/e is also called the voltage equivalent temperature. Also,  η is a constant = 1 (for silicon)<br />
&amp; 2 (for germanium).</p>
<p>All other diodes like the Zener Diode, LED, etc are derived from the basic semiconductor diode with a few changes in their design &amp; functions.</p>
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