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		<title>GATE-2012 ECE Q10 (networks)</title>
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		<pubDate>Fri, 05 Apr 2013 01:08:16 +0000</pubDate>
		<dc:creator>Krishna Sankar</dc:creator>
				<category><![CDATA[GATE]]></category>
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		<description>Question 10 on networks from GATE (Graduate Aptitude Test in Engineering) 2012 Electronics and Communication Engineering paper. Q10. The average power delivered to an impedance  by a current  is (A) 44.2W (B) 50W (C) 62.5W [...]&lt;div class='yarpp-related-rss'&gt;
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				<content:encoded><![CDATA[<p></p><p>Question 10 on networks from GATE (Graduate Aptitude Test in Engineering) 2012 Electronics and Communication Engineering paper.</p>
<h2>Q10. The average power delivered to an impedance <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{(4-3j)\Omega}" align="absmiddle" border="0" /> by a current <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{5\cos\(100\pi t + 100\)A}" align="absmiddle" border="0" /> is</h2>
<h2>(A) 44.2W</h2>
<h2>(B) 50W</h2>
<h2>(C) 62.5W</h2>
<h2>(D) 125W</h2>
<p><img title="More..." alt="" src="http://www.dsplog.com/db-install/wp-includes/js/tinymce/plugins/wordpress/img/trans.gif" /></p>
<h2>Solution</h2>
<p>The average power delivered to the load is integral of the instantaneous power over some period <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?T" align="absmiddle" border="0" />, i.e.</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?P_{avg}=\frac{1}{T}\int_TV_i(t)I_i(t)dt" align="absmiddle" border="0" /></p>
<p>Given that <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?V_i(t)=I_i(t)R_L" align="absmiddle" border="0" />, the equation reduces to,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?P_{avg}=\frac{1}{T}\int_TI^2_i(t)R_L dt=I^2_{rms}R_L" align="absmiddle" border="0" />.</p>
<p>In our example with <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?I_i(t)={5\cos\(100\pi t + 100\)}" align="absmiddle" border="0" /></p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}I^2_{rms}&amp;=&amp;\frac{1}{T}\int_TI^2_i(t)dt\\&amp;=&amp;\frac{1}{T}\int_T\(5\cos\(100\pi%20t%20+%20100\)\)^2dt\\&amp;=&amp;\frac{5^2}{2}\end{array}" align="absmiddle" border="0" /></p>
<p>Plugging in,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?P_{avg}=\|I_{rms}^\|^2{R_L}=\frac{25}{2}*4 = 50W" align="absmiddle" border="0" />.</p>
<p><strong>Based on the above, the right choice is (B) 50W</strong></p>
<p><strong> </strong></p>
<h2>References</h2>
<p>[1] GATE Examination Question Papers [Previous Years] from Indian Institute of Technology, Madras <a href="http://gate.iitm.ac.in/gateqps/2012/ec.pdf">http://gate.iitm.ac.in/gateqps/2012/ec.pdf</a></p>
<p>[2] <a href="http://en.wikipedia.org/wiki/Maximum_power_transfer_theorem">http://en.wikipedia.org/wiki/Maximum_power_transfer_theorem</a></p>
<p>[3] <a href="http://en.wikipedia.org/wiki/AC_power">http://en.wikipedia.org/wiki/AC_power</a></p>
<p>&nbsp;</p>
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		<title>GATE-2012 ECE Q18 (signals)</title>
		<link>http://feedproxy.google.com/~r/dsplogdotcom/~3/z8qGvtENW14/</link>
		<comments>http://www.dsplog.com/2013/03/31/gate-2012-ece-q18-signals/#comments</comments>
		<pubDate>Sun, 31 Mar 2013 06:51:55 +0000</pubDate>
		<dc:creator>Krishna Sankar</dc:creator>
				<category><![CDATA[GATE]]></category>
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		<category><![CDATA[Q18]]></category>
		<category><![CDATA[Signals]]></category>

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		<description>Question 18 on signals from GATE (Graduate Aptitude Test in Engineering) 2012 Electronics and Communication Engineering paper. Q18. If , then the region of convergence (ROC) of its Z transform  in the z-plane will be (A)  [...]&lt;div class='yarpp-related-rss'&gt;
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				<content:encoded><![CDATA[<p></p><p>Question 18 on signals from GATE (Graduate Aptitude Test in Engineering) 2012 Electronics and Communication Engineering paper.</p>
<h2>Q18. If <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{x[n]=\(1/3\)^{|n|}-\(1/2\)^nu[n]}" align="absmiddle" border="0" />, then the region of convergence (ROC) of its Z transform  in the z-plane will be</h2>
<h2>(A) <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{\frac{1}{3}&lt;|z|&lt;3}" align="absmiddle" border="0" /></h2>
<h2>(B) <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{\frac{1}{3}&lt;|z|&lt;\frac{1}{2}}" align="absmiddle" border="0" /></h2>
<h2>(C) <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{\frac{1}{2}&lt;|z|&lt;3}" align="absmiddle" border="0" /></h2>
<h2>(D) <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{\frac{1}{3}&lt;|z|}" align="absmiddle" border="0" /></h2>
<p><img title="More..." alt="" src="http://www.dsplog.com/db-install/wp-includes/js/tinymce/plugins/wordpress/img/trans.gif" /></p>
<h2>Solution</h2>
<p>As discussed in Chapter 3 of <strong>Discrete-Time Signal Processing, 2nd Edition, Alan V. Oppenheim, John R. Buck, Ronald W. Schafer <strong>(<a href="http://www.amazon.com/gp/product/0137549202/ref=as_li_qf_sp_asin_tl?ie=UTF8&amp;camp=1789&amp;creative=9325&amp;creativeASIN=0137549202&amp;linkCode=as2&amp;tag=dl04-20">Buy from Amazon.com</a><img alt="" src="http://www.assoc-amazon.com/e/ir?t=dl04-20&amp;l=as2&amp;o=1&amp;a=0137549202" width="1" height="1" border="0" />, <a href="http://www.flipkart.com/discrete-time-signal-processing-2nd/p/itmdytssutw6gmbz?pid=9788131704929&amp;affid=krishnadsp">Buy from Flipkart.com</a>)</strong>, </strong>the z transform of a sequence <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?x[n]" align="absmiddle" border="0" /> is defined as</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?X(z) = \sum_{-\infty}^{\infty}x[n]z^{-n}" align="absmiddle" border="0" />.</p>
<p>For any given sequence, the values of z for which the z transform converges is called the <strong>Region Of Convergence (ROC)</strong> i.e.</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}ROC&amp;=&amp;z:\|\sum_{n=-\infty}^{\infty}x[n]z^{-n}\|&lt;\infty\end{array}" align="absmiddle" border="0" /></p>
<p>In our case,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?{x[n]=\underbrace{\(1/3\)^{|n|}}_{x_1[n]}-\underbrace{\(1/2\)^nu[n]}_{x_2[n]}" align="absmiddle" border="0" />.</p>
<p>Finding the z transform of <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?x_1[n]" align="absmiddle" border="0" />,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}X_1(z)=\sum_{-\infty}^{\infty}x_1[n]z^{-n}&amp;=&amp;\sum_{-\infty}^{\infty}\(1/3\)^{|n|}z^{-n}\\&amp;=&amp;\underbrace{\dots+\(\frac{1}{3}\)^2z^2+\(\frac{1}{3}\)^1z^1}_{n=-\infty\mbox{%20to%20}-1}+\underbrace{1+\(\frac{1}{3}\)^1z^{-1}+\(\frac{1}{3}\)^2z^{-2}+\dots}_{n=0\mbox{%20to%20}\infty}\\&amp;=&amp;\underbrace{\sum_{1}^{\infty}\(\frac{z}{3}\)^n}_{|z|&lt;3}+\underbrace{\sum_{0}^{\infty}\(\frac{1}{3z}\)^n}_{|z|&gt;{\frac{1}{3}}\end{array}" align="absmiddle" border="0" /></p>
<p>The first term in the series <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?X_1(z)" align="absmiddle" border="0" /> converges for <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?|z|&lt;3" align="absmiddle" border="0" /> and the second term will be converging for <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?|z|&gt;\frac{1}{3}" align="absmiddle" border="0" />.</p>
<p>Now, finding the z transform of <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?x_2[n]" align="absmiddle" border="0" />,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}X_2(z)=\sum_{-\infty}^{\infty}x_2[n]z^{-n}&amp;=&amp;\sum_{-\infty}^{\infty}\(1/2\)^{n}u[n]z^{-n}\\&amp;=&amp;\underbrace{1+\(\frac{1}{2}\)^1z^{-1}+\(\frac{1}{3}\)^2z^{-2}+\dots}_{n=0\mbox{%20to%20}\infty}\\&amp;=&amp;amp\underbrace{\sum_{0}^{\infty}\(\frac{1}{2z}\)^n}_{|z|&gt;{\frac{1}{2}}\end{array}" align="absmiddle" border="0" /><br />
The term in the series <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?X_2(z)" align="absmiddle" border="0" /> converges for <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?|z|&gt;\frac{1}{2}" align="absmiddle" border="0" />.</p>
<p>Combining both the terms,  the Region Of Convergence is the region of overlap of the two terms, i.e. <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?|z|&gt;\frac{1}{2}" align="absmiddle" border="0" /> and <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?|z|&lt;3" align="absmiddle" border="0" />.</p>
<p>&nbsp;</p>
<p><strong>Based on the above, the right choice is (C) <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?{\frac{1}{2}&lt;|z|&lt;3}" align="absmiddle" border="0" /></strong></p>
<p><strong> </strong></p>
<h2>References</h2>
<p>[1] GATE Examination Question Papers [Previous Years] from Indian Institute of Technology, Madras <a href="http://gate.iitm.ac.in/gateqps/2012/ec.pdf">http://gate.iitm.ac.in/gateqps/2012/ec.pdf</a></p>
<p><strong>[2] Discrete-Time Signal Processing, 2nd Edition, Alan V. Oppenheim, John R. Buck, Ronald W. Schafer (<a href="http://www.amazon.com/gp/product/0137549202/ref=as_li_qf_sp_asin_tl?ie=UTF8&amp;camp=1789&amp;creative=9325&amp;creativeASIN=0137549202&amp;linkCode=as2&amp;tag=dl04-20">Buy from Amazon.com</a><img style="border: none !important; margin: 0px !important;" alt="" src="http://www.assoc-amazon.com/e/ir?t=dl04-20&amp;l=as2&amp;o=1&amp;a=0137549202" width="1" height="1" border="0" />, <a href="http://www.flipkart.com/discrete-time-signal-processing-2nd/p/itmdytssutw6gmbz?pid=9788131704929&amp;affid=krishnadsp">Buy from Flipkart.com</a>)</strong></p>
<p>&nbsp;</p>
<p>&nbsp;</p>
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		<title>Migrated to Amazon EC2 instance (from shared hosting)</title>
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		<pubDate>Mon, 11 Mar 2013 01:20:38 +0000</pubDate>
		<dc:creator>Krishna Sankar</dc:creator>
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		<description>Being not too happy with the speed of the shared hosting, decided to move the blog to an Amazon Elastic Compute Cloud (Amazon EC2) instance.  Given this is a baby step, picked up a micro instance [...]&lt;div class='yarpp-related-rss'&gt;
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				<content:encoded><![CDATA[<p></p><p>Being not too happy with the speed of the shared hosting, decided to move the blog to an <a title="Amazon Elastic Compute Cloud" href="http://aws.amazon.com/ec2/" target="_blank">Amazon Elastic Compute Cloud (Amazon EC2)</a> instance.  Given this is a baby step, picked up a micro instance running an Ubuntu server and installed <a title="Apache web server" href="http://en.wikipedia.org/wiki/Apache_HTTP_Server" target="_blank">Apache web server</a>, <a title="wiki entry on MySQL" href="http://en.wikipedia.org/wiki/MySQL" target="_blank">MySQL</a>, <a title="wiki entry on PHP" href="http://en.wikipedia.org/wiki/PHP" target="_blank">PHP</a> . After doing a bit of tweaking with this new instance, imported the SQL database and other files from the shared hosting and pointed the A name record to the new IP address. This switch happened over this weekend.</p>
<p>One particular issue which I faced was frequent crashing of MySQL due to memory limitations. Followed few online instructions to improve the situation and the current configuration seems to be holding up (but this is a cause of worry &#8211; need to figure the right solution).</p>
<p>Anyhow, hope you like the decreased page load time! <img src='http://www.dsplog.com/db-install/wp-includes/images/smilies/icon_smile.gif' alt=':-)' class='wp-smiley' /> </p>
<p><strong>Some helpful links from the web:</strong></p>
<p><strong></strong>a) <a title="How to install WordPress on Amazon EC2" href="http://iampuneet.com/wordpress-amazon-ec2/" target="_blank">How to install WordPress on Amazone EC2</a></p>
<p>b) <a title="Move WordPress site from shared hosting to Amazon EC2" href="http://blog.lopau.com/move-wordpress-site-from-shared-hosting-to-amazon-ec2/" target="_blank">Move WordPress site from shared hosting to Amazon EC2</a></p>
<p>c) <a title="DIY: Enable CGI on your Apache server" href="http://www.techrepublic.com/blog/doityourself-it-guy/diy-enable-cgi-on-your-apache-server/1066" target="_blank">DIY: Enable CGI on your Apache server</a></p>
<p>d) <a title="Import MySQL Dumpfile, SQL Datafile Into My Database" href="http://www.cyberciti.biz/faq/import-mysql-dumpfile-sql-datafile-into-my-database/" target="_blank">Import MySQL Dumpfile, SQL Datafile Into My Database</a></p>
<p>e) <a title="Making WordPress Stable on EC2-Micro" href="http://www.frameloss.org/2011/11/04/making-wordpress-stable-on-ec2-micro/" target="_blank">Making WordPress Stable on EC2-Micro</a></p>
<p>f) <a title="http://www.lavluda.com/2007/07/15/how-to-enable-mod_rewrite-in-apache22-debian/" href="how to enable mod_rewrite in apache2.2 (debian/ubuntu)" target="_blank">how to enable mod_rewrite in apache2.2 (debian/ubuntu)</a></p>
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		<title>GATE-2012 ECE Q28 (electromagnetics)</title>
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		<pubDate>Wed, 20 Feb 2013 01:50:01 +0000</pubDate>
		<dc:creator>Krishna Sankar</dc:creator>
				<category><![CDATA[GATE]]></category>
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		<category><![CDATA[electromagnetics]]></category>

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		<description>Question 28 on electromagnetics from GATE (Graduate Aptitude Test in Engineering) 2012 Electronics and Communication Engineering paper. Q28. A transmission line with a characteristic impedance of 100 is used to match a 50 section to a 200 section. If the matching [...]&lt;div class='yarpp-related-rss'&gt;
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				<content:encoded><![CDATA[<p></p><p>Question 28 on electromagnetics from GATE (Graduate Aptitude Test in Engineering) 2012 Electronics and Communication Engineering paper.</p>
<h2>Q28. A transmission line with a characteristic impedance of 100<img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{\Omega}" align="bottom" border="0" /> is used to match a 50<img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{\Omega}" align="bottom" border="0" /> section to a 200<img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{\Omega}" align="bottom" border="0" /> section. If the matching is to be done both at 429MHz and 1GHz, the length of the transmission line can be approximately</h2>
<h2>(A) 82.5cm</h2>
<h2>(B) 1.05m</h2>
<h2>(C) 1.58m</h2>
<h2>(D) 1.75m</h2>
<p><img title="More..." alt="" src="http://www.dsplog.com/db-install/wp-includes/js/tinymce/plugins/wordpress/img/trans.gif" /></p>
<h2>Solution</h2>
<p>To answer this question, let us first understand the propagation in a transmission line,  termination and the concept of impedance matching. The <strong>section 2.1 in Microwave Engineering, David M Pozar (<a href="http://www.amazon.com/gp/product/0470631554/ref=as_li_tf_tl?ie=UTF8&amp;camp=1789&amp;creative=9325&amp;creativeASIN=0470631554&amp;linkCode=as2&amp;tag=dl04-20">buy from Amazon.com</a><img style="border: none !important; margin: 0px !important;" alt="" src="http://www.assoc-amazon.com/e/ir?t=dl04-20&amp;l=as2&amp;o=1&amp;a=0470631554" width="1" height="1" border="0" />, <a href="http://www.flipkart.com/microwave-engineering-3rd/p/itmdytmvtyj3arjj?pid=9788126510498&amp;affid=krishnadsp">Buy from Flipkart.com</a>) </strong> is used as reference.</p>
<p>Consider a transmission line of very small length <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Delta z" align="bottom" border="0" /> having the parameters as show in figure below.</p>
<p><img class="alignnone size-full wp-image-1943" alt="transmission_line_model" src="http://www.dsplog.com/db-install/wp-content/uploads/2013/02/transmission_line_model.png" width="378" height="150" /></p>
<p><strong>Figure : Transmission line model <strong> (Reference Figure 2.1 in <strong>Microwave Engineering, David M Pozar (<a href="http://www.amazon.com/gp/product/0470631554/ref=as_li_tf_tl?ie=UTF8&amp;camp=1789&amp;creative=9325&amp;creativeASIN=0470631554&amp;linkCode=as2&amp;tag=dl04-20">buy from Amazon.com</a><img alt="" src="http://www.assoc-amazon.com/e/ir?t=dl04-20&amp;l=as2&amp;o=1&amp;a=0470631554" width="1" height="1" border="0" />, <a href="http://www.flipkart.com/microwave-engineering-3rd/p/itmdytmvtyj3arjj?pid=9788126510498&amp;affid=krishnadsp">Buy from Flipkart.com</a>)</strong></strong></strong></p>
<p>&nbsp;</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?R" align="bottom" border="0" /> is the resistance per unit length <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Omega/m" align="absmiddle" border="0" />,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?L" align="bottom" border="0" /> is the inductance per unit length <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?H/m" align="absmiddle" border="0" />,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?G" align="bottom" border="0" /> is the conductance per unit length <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?S/m" align="absmiddle" border="0" />,</p>
<p><strong><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?C" align="bottom" border="0" /></strong> is the capacitance per unit length<img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?F/m" align="absmiddle" border="0" />.</p>
<p>Applying Kirchoff&#8217;s voltage law,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?v(z,t)-R\Delta%20zi(z,t)-L\Delta%20z\frac{\partial%20i(z,t)}{\partial%20t}-v(z+\Delta%20z%20,t)=0" align="absmiddle" border="0" /></p>
<p>Applying Kirchoff&#8217;s current law,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?i(z,t)-G\Delta%20zv(z+\Delta%20z,t)-C\Delta%20z\frac{\partial%20v(z+\Delta%20z,t)}{\partial%20t}-i(z+\Delta%20z%20,t)=0" align="absmiddle" border="0" /></p>
<p>Dividing the above equations by <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Delta z" align="bottom" border="0" /> and taking the limit <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Delta z \rightarrow 0" align="absmiddle" border="0" />,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\frac{\partial%20v(z,t)}{\partial%20z}=-Ri(z,t)%20-%20L\frac{\partial%20i(z,t)}{\partial%20t}" align="absmiddle" border="0" /></p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\frac{\partial%20i(z,t)}{\partial%20z}=-Gv(z,t)%20-%20C\frac{\partial%20v(z,t)}{\partial%20t}" align="absmiddle" border="0" /></p>
<p>If we assume that the inputs are sinusoidal, then the above equation can be re-written as</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\frac{dV(z)}{dz}=-(R+jwL)I(z)" align="absmiddle" border="0" /></p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\frac{dI(z)}{dz}=-(G+jwC)V(z)" align="absmiddle" border="0" /></p>
<p>Substituting,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\frac{d^2V(z)}{dz}-\gamma^2V(z)=0" align="absmiddle" border="0" />,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\frac{d^2I(z)}{dz}-\gamma^2I(z)=0" align="absmiddle" border="0" />,</p>
<p>where</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\gamma=\alpha+j\beta%20=%20\sqrt%7B(R+jwL)(G+jwC)%7D" align="absmiddle" border="0" />.</p>
<p>The solution to the above equations are,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?V(z)%20=%20V_0^+e^{-\gamma%20z}+V_0^-e^{\gamma%20z}" align="absmiddle" border="0" /></p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?I(z)%20=%20I_0^+e^{-\gamma%20z}+I_0^-e^{\gamma%20z}" align="absmiddle" border="0" />.</p>
<p>The current on the line can be alternately expressed as,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?I(z)%20=\frac{\gamma}{R+jwL}\(V_0^+e^{-\gamma%20z}-V_0^-e^{\gamma%20z}\)=\frac{1}{Z_0}\(V_0^+e^{-\gamma%20z}-V_0^-e^{\gamma%20z}\)" align="absmiddle" border="0" />,</p>
<p>where the characteristic impedance of the line is defined as,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_0=\frac{R+jwL}{\gamma}=\sqrt{\frac{R+jwL}{G+jwC}}" align="absmiddle" border="0" />.</p>
<p>The wavelength on the line is,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\lambda=\frac{2\pi}{\beta}" align="absmiddle" border="0" />.</p>
<p><strong>Loss less transmission line case</strong></p>
<p>For a lossless transmission line, we can set <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?R=G=0" align="bottom" border="0" />.</p>
<p>Then the propagation constant reduces to<img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}\alpha=0,&amp;\beta = \omega\sqrt{LC}\end{array}" align="absmiddle" border="0" />, the characteristic impedance is <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_0=\sqrt{\frac{L}{C}}" align="absmiddle" border="0" /> and the voltage and current on the line can be written as,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?V(z)%20=%20V_0^+e^{-j\beta%20z}+V_0^-e^{j\beta%20z}" align="absmiddle" border="0" /></p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?I(z)%20=\frac{1}{Z_0}\(V_0^+e^{-j\beta%20z}-V_0^-e^{j\beta%20z}\)" align="absmiddle" border="0" /></p>
<h2>Terminated lossless transmission line</h2>
<p>Consider a transmission line terminated with load impedance <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_L" align="absmiddle" border="0" /> as shown in figure below.</p>
<p><img class="alignnone size-full wp-image-1944" alt="transmission_line_with_load_impedance" src="http://www.dsplog.com/db-install/wp-content/uploads/2013/02/transmission_line_with_load_impedance.png" width="367" height="235" /></p>
<p><strong>Figure: Transmission line with load impedance (Reference Figure 2.4 in <strong>Microwave Engineering, David M Pozar (<a href="http://www.amazon.com/gp/product/0470631554/ref=as_li_tf_tl?ie=UTF8&amp;camp=1789&amp;creative=9325&amp;creativeASIN=0470631554&amp;linkCode=as2&amp;tag=dl04-20">buy from Amazon.com</a><img alt="" src="http://www.assoc-amazon.com/e/ir?t=dl04-20&amp;l=as2&amp;o=1&amp;a=0470631554" width="1" height="1" border="0" />, <a href="http://www.flipkart.com/microwave-engineering-3rd/p/itmdytmvtyj3arjj?pid=9788126510498&amp;affid=krishnadsp">Buy from Flipkart.com</a>)</strong></strong></p>
<p>At the load <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?z=0" align="absmiddle" border="0" />, the relation between the total voltage and current is related to the load impedance <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_L" align="absmiddle" border="0" /></p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_L=\frac{V(0)}{I(0)}=\frac{V_0^{+}+V_0^{-}}{V_0^{+}-V_0^-}Z_0" align="absmiddle" border="0" />.</p>
<p>Alternatively,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?V_0^{-}=\frac{Z_L-Z_0}{Z_L+Z_0}V_0^{+}" align="bottom" border="0" />.</p>
<p>The reflection coefficient <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_L" align="absmiddle" border="0" /> is defined as the amplitude of the reflected voltage to the incident voltage,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Gamma=\frac{V_0^{-}}{V_0^{+}}=\frac{Z_L-Z_0}{Z_L+Z_0}" align="absmiddle" border="0" />.</p>
<p><strong>For no reflection to happen, i.e <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Gamma=0" align="absmiddle" border="0" />, the load impedance <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_L" align="absmiddle" border="0" /> should be equal to the characteristic impedance <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_0" align="absmiddle" border="0" /> of the transmission line. The above equation captures the impedance seen at the load <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?z=0" align="absmiddle" border="0" />. </strong></p>
<p>The voltage and current on the line can be represented using <strong><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Gamma" align="absmiddle" border="0" /> </strong>as,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?V(z)%20=%20V_0^+\(e^{-j\beta%20z}+\Gamma e^{j\beta%20z}\)" align="absmiddle" border="0" /></p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?I(z)%20=\frac{V_0^+}{Z_0}\(e^{-j\beta%20z}-\Gamma e^{j\beta%20z}\)" align="absmiddle" border="0" /></p>
<p>When looking from a point <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?z=-l" align="absmiddle" border="0" /> from the load, the input impedance seen is,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{llllll}Z_{in}&amp;=&amp;\frac{V(-l)}{I(-l)}&amp;=&amp;\frac{V_0^{+}\(e^{j\beta%20l}%20+%20\Gamma%20e^{-j\beta%20l}\)}{\frac{V_0^{+}}{Z_0}\(e^{j\beta%20l}%20-%20\Gamma%20e^{-j\beta%20l}\)}\end{array}" align="absmiddle" border="0" />.</p>
<p>Substituting for <strong><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Gamma" align="absmiddle" border="0" />, </strong></p>
<p><strong></strong><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{llllll}Z_{in}&amp;=&amp;Z_0\frac{\(Z_L+Z_0\)e^{j\beta%20l}%20+(Z_L-Z_0)%20%20e^{-j\beta%20l}}{\(Z_L+Z_0\)e^{j\beta%20l}%20-\(Z_L-Z_0\)%20e^{-j\beta%20l}}\\&amp;=&amp;Z_0\frac{Z_L+jZ_0\tan%20\beta%20l}{Z_0+jZ_L\tan%20\beta%20l}\end{array}" align="absmiddle" border="0" />.</p>
<p>&nbsp;</p>
<p><strong>Special case when <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?{l =\lambda/4}" align="absmiddle" border="0" /> (and it&#8217;s odd multiples)</strong></p>
<p>For the case when <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?{l =\(2n+1\)\frac{\lambda}{4}}" align="absmiddle" border="0" /> the input impedance seen is,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{llll}Z_{in}&amp;=&amp;Z_0\frac{Z_L+jZ_0\tan%20\beta%20l}{Z_0+jZ_L\tan%20\beta%20l}\\&amp;=&amp;Z_0\frac{Z_L+jZ_0\tan\(\frac{2\pi}{\lambda}\frac{(2n+1)\lambda}{4}\)}{Z_0+jZ_L\tan\(\frac{2\pi}{\lambda}\frac{(2n+1)\lambda}{4}\)}\\&amp;=&amp;Z_0\frac{Z_0}{Z_L}=\frac{Z_0^2}{Z_L}\end{array}" align="absmiddle" border="0" />.</p>
<p>This result can be used to for impedance matching.</p>
<h2>Quarter wave transformer</h2>
<p>Consider a circuit with load <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?R_L" align="absmiddle" border="0" /> and a line with characteristic impedance <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_0" align="absmiddle" border="0" /> connected by a transmission line of characteristic impedance <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_1" align="absmiddle" border="0" /> with length <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\lambda/4" align="absmiddle" border="0" />.</p>
<p><img class="alignnone size-full wp-image-1946" alt="quarter_wave_matching_transformer" src="http://www.dsplog.com/db-install/wp-content/uploads/2013/02/quarter_wave_matching_transformer.png" width="352" height="266" /></p>
<p><strong>Figure: Quarter Wave Matching transformer (Reference Figure 2.16 in <strong>Microwave Engineering, David M Pozar (<a href="http://www.amazon.com/gp/product/0470631554/ref=as_li_tf_tl?ie=UTF8&amp;camp=1789&amp;creative=9325&amp;creativeASIN=0470631554&amp;linkCode=as2&amp;tag=dl04-20">buy from Amazon.com</a><img alt="" src="http://www.assoc-amazon.com/e/ir?t=dl04-20&amp;l=as2&amp;o=1&amp;a=0470631554" width="1" height="1" border="0" />, <a href="http://www.flipkart.com/microwave-engineering-3rd/p/itmdytmvtyj3arjj?pid=9788126510498&amp;affid=krishnadsp">Buy from Flipkart.com</a>)</strong></strong></p>
<p>The input impedance seen is,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{llll}Z_{in}&amp;=&amp;Z_1\frac{R_L+jZ_1\tan%20\beta%20l}{Z_1+jR_L\tan%20\beta%20l} \\&amp;=&amp;Z_0\frac{Z_L+jZ_0\tan\(\frac{2\pi}{\lambda}\frac{\lambda}{4}\)}{Z_0+jZ_L\tan\(\frac{2\pi}{\lambda}\frac{\lambda}{4}\)}&amp; \mbox{  } &amp;  \(\beta l =\frac{2\pi}{\lambda}\frac{\lambda}{4}\right  \pi/2\) \\&amp;=&amp;Z_1\frac{Z_1}{R_L}=\frac{Z_1^2}{R_L}\end{array}" align="absmiddle" border="0" />.</p>
<p>So if we choose <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_1 = \sqrt{Z_0R_L}" align="absmiddle" border="0" />, then the input impedance seen is <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_{in} = Z_0" align="absmiddle" border="0" /> which is the condition required for having no reflection i.e. <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Gamma=0" align="absmiddle" border="0" />.</p>
<p>One important aspect to note here is that <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Gamma=0" align="absmiddle" border="0" /> is not guaranteed for all frequencies, but rather only for certain frequencies. The frequency dependence can be found by finding the frequencies for which <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\beta l=\(2n+1\)\frac{\pi}{2}" align="absmiddle" border="0" /> .</p>
<p>Replacing <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi? l=\frac{\lambda_0}{4}" align="absmiddle" border="0" /> where <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\lambda_0" align="absmiddle" border="0" /> is the wave length corresponding to frequency <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?f_0" align="absmiddle" border="0" />,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\beta l = \(\frac{2\pi}{\lambda}\)\(\frac{\lambda_0}{4}\)=\(\frac{2\pi f}{v_p}\)\(\frac{v_p}{4f_0}\)=\frac{\pi f}{2 f_0}" align="absmiddle" border="0" />.</p>
<p>It can be seen that only for <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?f=\(2n+1\)f_0" align="absmiddle" border="0" /> , the term <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\beta l=\(2n+1\)\frac{\pi}{2}" align="absmiddle" border="0" /> resulting in reflection coefficient <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Gamma=0" align="absmiddle" border="0" /> only for those frequencies.</p>
<h2>Solving the GATE question</h2>
<p>Applying all this to the problem at hand, we have <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?Z_0=50" align="absmiddle" border="0" />, <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?R_L=200" align="absmiddle" border="0" />  and <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?R_1=100" align="absmiddle" border="0" />.</p>
<p>Given that <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?R_1=\sqrt{Z_0 R_L} = \sqrt{50 * 200 }=100" align="absmiddle" border="0" />, we know that a quarter wave transformer is used to achieve impedance matching.</p>
<p>Now we also know that we need to match for two frequencies <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?f_{1}=429\mbox{ MHz}" align="absmiddle" border="0" /> and <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?f_{2}=1\mbox{ GHz}" align="absmiddle" border="0" />.</p>
<p>The wavelength for each frequencies are,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\lambda_{1}=\frac{3e^8}{429e^6}*100\simeq 70\mbox{ cm}" align="absmiddle" border="0" /></p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\lambda_{2}=\frac{3e^8}{1e^9}*100\simeq 30\mbox{ cm}" align="absmiddle" border="0" /></p>
<p>The least common multiple of these two wavelength is, <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\lambda_{lcm}=\mbox{lcm}\(70,30\)=210\mbox{ cm}" align="absmiddle" border="0" /> and the corresponding quarter wave length is <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\frac{\lambda_{lcm}}{4}=52.5\mbox{ cm}" align="absmiddle" border="0" />.</p>
<p>Given than <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\frac{\lambda_{lcm}}{4}=52.5\mbox{ cm}" align="absmiddle" border="0" /> is not listed in the options, we can go for the next higher odd multiple i.e. <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?52.5*3=157.5 \simeq 1.58\mbox{ m}" align="absmiddle" border="0" /></p>
<p><strong>Based on the above, the right choice is (C) 1.58m</strong></p>
<p>&nbsp;</p>
<h2>References</h2>
<p>[1] GATE Examination Question Papers [Previous Years] from Indian Institute of Technology, Madras <a href="http://gate.iitm.ac.in/gateqps/2012/ec.pdf">http://gate.iitm.ac.in/gateqps/2012/ec.pdf</a></p>
<p>[2] <strong>Microwave Engineering, David M Pozar (<a href="http://www.amazon.com/gp/product/0470631554/ref=as_li_tf_tl?ie=UTF8&amp;camp=1789&amp;creative=9325&amp;creativeASIN=0470631554&amp;linkCode=as2&amp;tag=dl04-20">buy from Amazon.com</a><img alt="" src="http://www.assoc-amazon.com/e/ir?t=dl04-20&amp;l=as2&amp;o=1&amp;a=0470631554" width="1" height="1" border="0" />, <a href="http://www.flipkart.com/microwave-engineering-3rd/p/itmdytmvtyj3arjj?pid=9788126510498&amp;affid=krishnadsp">Buy from Flipkart.com</a>) </strong></p>
<p>&nbsp;</p>
<p>&nbsp;</p>
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		<title>Image Rejection Ratio (IMRR) with transmit IQ gain/phase imbalance</title>
		<link>http://feedproxy.google.com/~r/dsplogdotcom/~3/hVKmqG316wc/</link>
		<comments>http://www.dsplog.com/2013/01/31/imrr-transmit-iq-gain-phase-imbalance/#comments</comments>
		<pubDate>Thu, 31 Jan 2013 01:47:36 +0000</pubDate>
		<dc:creator>Krishna Sankar</dc:creator>
				<category><![CDATA[Analog]]></category>
		<category><![CDATA[imbalance]]></category>
		<category><![CDATA[IQ]]></category>
		<category><![CDATA[modulator]]></category>

		<guid isPermaLink="false">http://www.dsplog.com/?p=1913</guid>
		<description>The post on IQ imbalance in transmitter, briefly discussed the effect of amplitude and phase imbalance and also showed that IQ imbalance results in spectrum at the image frequency. In this article, we will quantify [...]&lt;div class='yarpp-related-rss'&gt;
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&lt;/div&gt;
&lt;/div&gt;</description>
				<content:encoded><![CDATA[<p></p><p>The post on <a title="IQ imbalance in transmitter" href="http://www.dsplog.com/2009/03/08/iq-imbalance-in-transmitter/" target="_blank">IQ imbalance in transmitter</a>, briefly discussed the effect of amplitude and phase imbalance and also showed that IQ imbalance results in spectrum at the image frequency. In this article, we will quantify the power of the image with respect to the desired tone (also known as<strong> IMage Rejection Ratio IMRR</strong>) for different values of gain and phase imbalance.</p>
<p><span id="more-1913"></span></p>
<h2>System Model</h2>
<p>Consider an IQ modulator having gain of <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\alpha" align="absmiddle" border="0" /> and <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\beta" align="absmiddle" border="0" /> on each arm and phase imbalance of <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\phi" align="absmiddle" border="0" /> as shown in figure below.</p>
<p style="text-align: center;"><a href="http://www.dsplog.com/db-install/wp-content/uploads/2013/01/iq_modulator_with_gain_phase_imbalance.png"><img class="alignnone size-full wp-image-1915" alt="iq_modulator_with_gain_phase_imbalance" src="http://www.dsplog.com/db-install/wp-content/uploads/2013/01/iq_modulator_with_gain_phase_imbalance.png" width="210" height="195" /></a></p>
<p style="text-align: center;"><strong>Figure : IQ modulator with gain and phase imbalance</strong></p>
<p>The output signal is,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?y(t) = \alpha x_i(t) \cos\(2\pi f_c t + \frac{\phi}{2}\) - \beta x_q(t) \sin\(2\pi f_c t - \frac{\phi}{2}\)" align="absmiddle" border="0" />.</p>
<p>Considering an ideal IQ demodulator multiplying the received signal <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?y(t)" align="absmiddle" border="0" /> with <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\cos\(2\pi f_c t\)" align="absmiddle" border="0" /> and <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\sin\(2\pi f_c t\)" align="absmiddle" border="0" /> respectively,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}x'_i(t)&amp;=&amp;\int_0^T\[\alpha x_i(t)%20\cos\(2\pi%20f_c%20t%20+%20\frac{\phi}{2}\)%20-\beta x_q(t)%20\sin\(2\pi%20f_c%20t%20-%20\frac{\phi}{2}\)\]\cos\(2\pi%20f_c%20t%20\)\\&amp;=&amp;\frac{1}{2}\[\alpha x_i(t)\cos\(\frac{\phi}{2}\)+\beta x_q(t)\sin\(\frac{\phi}{2}\)\]\end{array}" align="absmiddle" border="0" />.</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}x'_q(t)&amp;=&amp;\int_0^T\[\alpha x_i(t)%20\cos\(2\pi%20f_c%20t%20+%20\frac{\phi}{2}\)%20-\beta x_q(t)%20\sin\(2\pi%20f_c%20t%20-%20\frac{\phi}{2}\)\]\[-\sin\(2\pi%20f_c%20t%20\)\]\\&amp;=&amp;\frac{1}{2}\[\alpha x_i(t)\sin\(\frac{\phi}{2}\)+\beta x_q(t)\cos\(\frac{\phi}{2}\)\]\end{array}" align="absmiddle" border="0" />.</p>
<p>Ignoring the common term <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\frac{1}{2}" align="absmiddle" border="0" /> and writing the base band equivalent form,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{\[\begin{array}x'_i(t)\\x'_q(t)\end{array}\]=\[\begin{array}\alpha%20\cos\(\frac{\phi}{2}\)%20&amp;%20\beta%20\sin\(\frac{\phi}{2}\)\\\alpha%20\sin\(\frac{\phi}{2}\)%20&amp;%20\beta%20\cos\(\frac{\phi}{2}\)\end{array}\]\[\begin{array}x_i(t)\\x_q(t)\end{array}\]}" align="absmiddle" border="0" />.</p>
<p><strong>This is the model for transmit IQ imbalance. </strong></p>
<p>&nbsp;</p>
<h2>Image Rejection Ratio (IMRR) with transmit IQ imbalance</h2>
<p>By sending a complex sinusoidal <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?e^{j\omega t}" align="bottom" border="0" />, and by taking ratio of the power of the signal at the image frequency <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?-\omega" align="bottom" border="0" />  and desired frequency <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?+\omega" align="bottom" border="0" /> , the image rejection ratio can be computed.</p>
<p>Let <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?x(t) = e^{j\omega t}" align="absmiddle" border="0" /> and correspondingly, <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?x_i(t) = \cos\(\omega t\)" align="absmiddle" border="0" /> and <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?x_q(t) = \sin\(\omega t\)" align="absmiddle" border="0" />.</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}x'_i(t)&amp;=&amp;\[\alpha\cos\(\frac{\phi}{2}\)\cos\(\omega t\)+\beta \sin\(\frac{\phi}{2}\)\sin\(\omega t\)\]\end{array}" align="absmiddle" border="0" /></p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}x'_q(t)&amp;=&amp;\[\alpha \sin\(\frac{\phi}{2}\) \cos\(\omega t\) +\beta \cos\(\frac{\phi}{2}\) \sin\(\omega t\) \]\end{array}" align="absmiddle" border="0" /></p>
<p><strong>Finding the <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?+\omega" align="bottom" border="0" /> component</strong></p>
<p>To find the <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?+\omega" align="bottom" border="0" /> component, multiply the received signal <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?x'(t)" align="absmiddle" border="0" /> with <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?e^{-j\omega t} = \cos\(\omega t\)-j\sin\(\omega t\)" align="absmiddle" border="0" /> and integrate over period <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?T" align="absmiddle" border="0" />.</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}Y_{+w}&amp;=&amp;\int_0^T\[x'_i(t)%20+%20jx'_q(t)%20\]\[\cos\(\omega%20t\)%20-%20j\sin\(\omega%20t\)\]\\&amp;=&amp;\int_0^T\[x'_i(t)\cos\(\omega%20t\)%20+%20x'_q(t)\sin\(\omega%20t\)%20\]+%20j\[-x'_i(t)\sin\(\omega%20t\)+x'_q(t)\cos\(\omega%20t\)\]\\&amp;=&amp;\frac{1}{2}\(\[\alpha\cos\(\frac{\phi}{2}\)+\beta\cos\(\frac{\phi}{2}\)\]%20+%20j\[-\beta\sin\(\frac{\phi}{2}\)+\alpha\sin\(\frac{\phi}{2}\)\]\)\end{array}" align="absmiddle" border="0" /></p>
<p>The power of the <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?+\omega" align="bottom" border="0" /> component is,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lllll}P_{+w}&amp;=&amp;\|Y_{+w}\|^2&amp;=&amp;\|\frac{1}{2}\(\[\alpha\cos\(\frac{\phi}{2}\)+\beta\cos\(\frac{\phi}{2}\)\]%20+%20j\[-\beta\sin\(\frac{\phi}{2}\)+\alpha\sin\(\frac{\phi}{2}\)\]\)\|^2\\&amp;&amp;&amp;=&amp;\frac{1}{4}\[\alpha^2\cos^2\(\frac{\phi}{2}\)+\beta^2\cos^2\(\frac{\phi}{2}\)+2\alpha\beta\cos^2\(\frac{\phi}{2}\)+\alpha^2\sin^2\(\frac{\phi}{2}\)+\beta^2\sin^2\(\frac{\phi}{2}\)-2\alpha\beta\sin^2\(\frac{\phi}{2}\)\]\\&amp;&amp;&amp;=&amp;\frac{1}{4}\[\alpha^2%20+%20\beta^2+2\alpha\beta\cos\(\phi\)\]\end{array}" align="absmiddle" border="0" /></p>
<p>&nbsp;</p>
<p><strong>Finding the <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?-\omega" align="bottom" border="0" /> component</strong></p>
<p>To find the <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?-\omega" align="bottom" border="0" /> component, multiply the received signal <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?x'(t)" align="absmiddle" border="0" /> with <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?e^{j\omega t} = \cos\(\omega t\)+j\sin\(\omega t\)" align="absmiddle" border="0" /> and integrate over period <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?T" align="absmiddle" border="0" />.</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}Y_{+w}&amp;=&amp;\int_0^T\[x'_i(t)%20+%20jx'_q(t)%20\]\[\cos\(\omega%20t\)%20+%20j\sin\(\omega%20t\)\]\\&amp;=&amp;\int_0^T\[x'_i(t)\cos\(\omega%20t\)%20-%20x'_q(t)\sin\(\omega%20t\)%20\]+%20j\[x'_i(t)\sin\(\omega%20t\)+x'_q(t)\cos\(\omega%20t\)\]\\&amp;=&amp;\frac{1}{2}\(\[\alpha\cos\(\frac{\phi}{2}\)-\beta\cos\(\frac{\phi}{2}\)\]%20+%20j\[\beta\sin\(\frac{\phi}{2}\)+\alpha\sin\(\frac{\phi}{2}\)\]\)\end{array}" align="absmiddle" border="0" /></p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lllll}P_{-w}&amp;=&amp;\|Y_{-w}\|^2&amp;=&amp;\|\frac{1}{2}\(\[\alpha\cos\(\frac{\phi}{2}\)-\beta\cos\(\frac{\phi}{2}\)\]%20+%20j\[\beta\sin\(\frac{\phi}{2}\)+\alpha\sin\(\frac{\phi}{2}\)\]\)\|^2\\&amp;&amp;&amp;=&amp;\frac{1}{4}\[\alpha^2\cos^2\(\frac{\phi}{2}\)+\beta^2\cos^2\(\frac{\phi}{2}\)-2\alpha\beta\cos^2\(\frac{\phi}{2}\)+\alpha^2\sin^2\(\frac{\phi}{2}\)+\beta^2\sin^2\(\frac{\phi}{2}\)+2\alpha\beta\sin^2\(\frac{\phi}{2}\)\]\\&amp;&amp;&amp;=&amp;\frac{1}{4}\[\alpha^2%20+%20\beta^2-2\alpha\beta\cos\(\phi\)\]\end{array}" align="absmiddle" border="0" /></p>
<p><strong>The Image Rejection Ratio (IMRR) is</strong></p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}IMRR%20&amp;%20=%20&amp;%20\frac{P_{-w}}{P_{+w}}\\&amp;=&amp;\frac{\alpha^2%20+%20\beta^2-2\alpha\beta\cos\(\phi\)}{\alpha^2%20+%20\beta^2+2\alpha\beta\cos\(\phi\)}\end{array}" align="absmiddle" border="0" />.</p>
<p>Substituting <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\alpha" align="absmiddle" border="0" /> and <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\beta" align="absmiddle" border="0" /> with variable <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\gamma = \frac{\alpha}{\beta}" align="absmiddle" border="0" /> and <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\epsilon = \gamma-1" align="absmiddle" border="0" />, the equation simplifies to,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}IMRR%20&amp;%20&amp;=&amp;\frac{\gamma^2%20+1-2\gamma\cos\(\phi\)}{\gamma^2%20+1+2\gamma\cos\(\phi\)}\end{array}" align="absmiddle" border="0" />.</p>
<p><strong>A useful approximation to IMRR</strong></p>
<p>When there is no phase imbalance i.e <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\phi=0" align="absmiddle" border="0" />, the equation reduces to,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}IMRR_{(\phi=0)}&amp;=&amp;\frac{\gamma^2%20+1-2\gamma}{\gamma^2%20+1+2\gamma}=\frac{(\gamma-1)^2}{(\gamma+1)^2}\\&amp;=&amp;\frac{\epsilon^2}{(\epsilon+2)^2}=\frac{\epsilon^2}{\epsilon^2+4\epsilon+4}\\&amp;\simeq &amp;\frac{\epsilon^2}{4}\end{array}" align="absmiddle" border="0" />.</p>
<p>When there is no gain imbalance i.e <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\gamma=1" align="absmiddle" border="0" />, the equation reduces to,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\begin{array}{lll}IMRR_{(\gamma=1)}&amp;=&amp;\frac{2\(1-\cos(\phi)\)}{2\(1+\cos(\phi)\)}\\&amp;=&amp;\tan^2\(\frac{\phi}{2}\)\\&amp;\simeq &amp;\frac{\phi^2}{4}\end{array}" align="absmiddle" border="0" />.</p>
<p>As these two are independent, they can be added to give an approximate value of Image Rejection Ratio.</p>
<p><strong>Summarizing, the Image Rejection Ratio for a given value of gain imbalance <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\gamma, \mbox{ } \(\epsilon = \gamma-1\)" align="absmiddle" border="0" /> and phase imbalance <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\phi" align="absmiddle" border="0" />is,</strong></p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Huge{\begin{array}{lll}IMRR%20&amp;%20&amp;=&amp;\frac{\gamma^2%20+1-2\gamma\cos\(\phi\)}{\gamma^2%20+1+2\gamma\cos\(\phi\)}&amp;\simeq&amp;\frac{\epsilon^2+\phi^2}{4}\end{array}}" align="absmiddle" border="0" />.</p>
<p><strong>Simulation Results</strong></p>
<p>Simple Matlab/Octave code plotting the simulated and theoretical values of Image Rejection for different values of gain and phase imbalance.</p>
<pre>clear; close all

N  = 64;
fm = 2;
gammadB_v = [-3:.1:3];
phiDeg_v  = [-6:.2:6];
[tt gammadB_zeroIdx ] = min(abs((gammadB_v-0)));
[tt phiDeg_zeroIdx  ] = min(abs((phiDeg_v-0)));

for (ii = 1:length(gammadB_v))
   for (jj = 1:length(phiDeg_v))
      gammadB    = gammadB_v(ii); 
      phiDeg     = phiDeg_v(jj);
      gammaLin   = 10^(gammadB/20); 
      phiRad     = phiDeg*pi/180;
      epsilonLin = gammaLin -1 ;

      % transmitted signal
      xt        = exp(j*2*pi*fm*[0:N-1]/N);
      % received signal with IQ imbalance
      xht_re    = gammaLin*cos(phiRad/2)*real(xt) + sin(phiRad/2)*imag(xt);
      xht_im    = gammaLin*sin(phiRad/2)*real(xt) + cos(phiRad/2)*imag(xt);
      xht       = xht_re + j*xht_im; 

      % taking ifft() to find the +fm and -fm components
      yF        = fft(xht,N);
      y_pfm     = yF(fm+1);
      y_nfm     = yF(N-fm+1);

      est_imrr_lin    = (abs(y_nfm)./abs(y_pfm))^2;
      theory_imrr_lin = (gammaLin^2 + 1  - 2*gammaLin*cos(phiRad))./(gammaLin^2 + 1  + 2*gammaLin*cos(phiRad));
      approx_imrr_lin = (epsilonLin^2 + phiRad^2)/4;

      est_imrr_dB(ii,jj)    = 10*log10(est_imrr_lin);
      theory_imrr_dB(ii,jj) = 10*log10(theory_imrr_lin);
      approx_imrr_dB(ii,jj) = 10*log10(approx_imrr_lin);
   end
end

figure
plot(gammadB_v,theory_imrr_dB(:,phiDeg_zeroIdx),'bs-'); hold on
plot(gammadB_v,est_imrr_dB(:,phiDeg_zeroIdx),'md-');
plot(gammadB_v,approx_imrr_dB(:,phiDeg_zeroIdx),'gx-');
xlabel('gain imbalance, dB'); ylabel('image rejection, dB'); grid on;
legend('theory','estimated','approx')
title('Image Rejection Ratio with gain imbalance alone');
axis([-3 3 -50 -10]);

figure
plot(phiDeg_v,theory_imrr_dB(gammadB_zeroIdx,:),'bs-'); hold on
plot(phiDeg_v,est_imrr_dB(gammadB_zeroIdx,:),'md-');
plot(phiDeg_v,approx_imrr_dB(gammadB_zeroIdx,:),'gx-');
xlabel('phase imbalance, degree'); ylabel('image rejection, dB'); grid on;
legend('theory','estimated','approx')
title('Image Rejection Ratio with phase imbalance alone');
axis([-6 6 -50 -20]);</pre>
<p><img class="alignnone  wp-image-1922" alt="image_rejection_ratio_gain_imbalance_alone" src="http://www.dsplog.com/db-install/wp-content/uploads/2013/01/image_rejection_ratio_gain_imbalance_alone.png" width="448" height="335" /></p>
<p><strong>Figure : Image Rejection Ratio (IMRR) with gain imbalance alone</strong></p>
<p><img class="alignnone  wp-image-1923" alt="image_rejection_ratio_phase_imbalance_alone" src="http://www.dsplog.com/db-install/wp-content/uploads/2013/01/image_rejection_ratio_phase_imbalance_alone.png" width="448" height="335" /></p>
<p><strong>Figure : Image Rejection Ratio (IMRR) with phase imbalance alone</strong></p>
<p>&nbsp;</p>
<p><strong>Observations</strong></p>
<p>1) The approximate expression holds good for reasonable values of gain and phase imbalance.</p>
<p>2) As a rule of thumb, the following numbers are useful :</p>
<p><strong>   - For 1 degree of phase imbalance, the Image Rejection Ratio (IMRR) is around -41dB</strong></p>
<p><strong>   - For 1dB of gain imbalance, the Image Rejection Ratio (IMRR) is around -25dB</strong></p>
<p>&nbsp;</p>
<h2>References</h2>
<p><strong>[1] Cavers, J.K.; Liao, M.W.; , &#8220;Adaptive compensation for imbalance and offset losses in direct conversion transceivers,&#8221; Vehicular Technology, IEEE Transactions on , vol.42, no.4, pp.581-588, Nov 1993 doi: 10.1109/25.260752</strong></p>
<p>[2] Table of trignometric identities <a href="http://www.sosmath.com/trig/Trig5/trig5/trig5.html">http://www.sosmath.com/trig/Trig5/trig5/trig5.html</a></p>
<div class='yarpp-related-rss'>
<h3>Related posts:</h3>
<div class="yarpp-thumbnails-horizontal">
<a class='yarpp-thumbnail' href='http://www.dsplog.com/2009/03/08/iq-imbalance-in-transmitter/' title='IQ imbalance in transmitter'>
<img width="120" height="62" src="http://www.dsplog.com/db-install/wp-content/uploads/2009/03/iq_modulation_transmit_receive.png" class="attachment-yarpp-thumbnail wp-post-image" alt="iq_modulation_transmit_receive" /><span class="yarpp-thumbnail-title">IQ imbalance in transmitter</span></a>
<a class='yarpp-thumbnail' href='http://www.dsplog.com/2007/06/10/first-order-digital-pll-for-tracking-constant-phase-offset/' title='First order digital PLL for tracking constant phase offset'>
<img width="120" height="77" src="http://www.dsplog.com/db-install/wp-content/uploads/2007/06/first_order_pll.jpg" class="attachment-yarpp-thumbnail wp-post-image" alt="first_order_pll" /><span class="yarpp-thumbnail-title">First order digital PLL for tracking constant phase offset</span></a>
<a class='yarpp-thumbnail' href='http://www.dsplog.com/2007/12/16/using-cordic-for-phase-and-magnitude-computation/' title='Using CORDIC for phase and magnitude computation'>
<img width="90" height="120" src="http://www.dsplog.com/db-install/wp-content/uploads/2008/04/cordic_for_phase_magnitude.jpg" class="attachment-yarpp-thumbnail wp-post-image" alt="Flow chart for the operations involved when CORDIC is used for phase and magnitude computation" /><span class="yarpp-thumbnail-title">Using CORDIC for phase and magnitude computation</span></a>
<a class='yarpp-thumbnail' href='http://www.dsplog.com/2008/09/19/equal-gain-combining/' title='Equal Gain Combining (EGC)'>
<img width="120" height="98" src="http://www.dsplog.com/db-install/wp-content/uploads/2008/09/snr_gain_equal_gain_combining.png" class="attachment-yarpp-thumbnail wp-post-image" alt="Gain in Eb/N0 with equal gain combining" /><span class="yarpp-thumbnail-title">Equal Gain Combining (EGC)</span></a>
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		<description>Question 15 on communication from GATE (Graduate Aptitude Test in Engineering) 2012 Electronics and Communication Engineering paper. Q15. A source alphabet consists of N symbols with the probability of the first two symbols being the [...]&lt;div class='yarpp-related-rss'&gt;
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				<content:encoded><![CDATA[<p></p><p>Question 15 on communication from GATE (Graduate Aptitude Test in Engineering) 2012 Electronics and Communication Engineering paper.</p>
<h2>Q15. A source alphabet consists of N symbols with the probability of the first two symbols being the same. A source encoder increases the probability of the first symbol by a small amount <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{\epsilon}" align="absmiddle" border="0" /> and decreases that of the second by <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?\Large{\epsilon}" align="absmiddle" border="0" />. After encoding, the entropy of the source</h2>
<h2>(A) increases</h2>
<h2>(B) remains the same</h2>
<h2>(C) increases only if N=2</h2>
<h2>(D) decreases</h2>
<p><img title="More..." alt="" src="http://www.dsplog.com/db-install/wp-includes/js/tinymce/plugins/wordpress/img/trans.gif" /></p>
<h2>Solution</h2>
<p>Entropy of a random variable <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?X" align="absmiddle" border="0" /> is defined as ,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?H(X)=-\sum_{x\in X}p(x)\log_2 p(x)" align="absmiddle" border="0" /> .</p>
<p><strong>Refer </strong>Chapter 2 in Elements of Information Theory, Thomas M. Cover, Joy A. Thomas (<a href="http://www.amazon.com/gp/product/0471241954/ref=as_li_ss_tl?ie=UTF8&amp;camp=1789&amp;creative=390957&amp;creativeASIN=0471241954&amp;linkCode=as2&amp;tag=dl04-20">Buy from Amazon.com</a><img alt="" src="http://www.assoc-amazon.com/e/ir?t=dl04-20&amp;l=as2&amp;o=1&amp;a=0471241954" width="1" height="1" border="0" />, <a href="http://www.flipkart.com/elements-information-theory-1st/p/itmdytmgcgtszgtx?pid=9788126508143&amp;affid=krishnadsp">Buy from Flipkart.com</a>)</p>
<p>Let us consider a simple case where <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?X" align="absmiddle" border="0" /> can take two values 1 and 0 with probability <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?p" align="absmiddle" border="0" /> and <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?1-p" align="absmiddle" border="0" /> respectively, i.e.</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?X%20=%20\{\begin{array}{lll}1,%20&amp;&amp;%20\mbox{probability,%20}p\\0,&amp;&amp;\mbox{probability,%20}1-p\end{array}" align="absmiddle" border="0" />.</p>
<p>The entropy of <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?X" align="absmiddle" border="0" /> is,</p>
<p><img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?H(X)=-p\log_2p - (1-p)\log_2(1-p)" align="absmiddle" border="0" />.</p>
<p>The plot of the entropy versus the probability<img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?p" align="absmiddle" border="0" /> is shown in the figure below.</p>
<pre>clear all; close
p = [0:.001:1];
hx = -p.*log2(p) - (1-p).*log2(1-p);
plot(p,hx);
xlabel('probability, p'); ylabel('H(X)');
title('entropy versus probability, p'); 
axis([0 1 0 1]);grid on;</pre>
<p><img class="alignnone  wp-image-1904" alt="entropy_versus_probability" src="http://www.dsplog.com/db-install/wp-content/uploads/2013/01/entropy_versus_probability.png" width="540" height="405" /></p>
<p><strong>Figure : Entropy versus probability for binary symmetric source</strong></p>
<p>It can be see that the entropy (also termed as uncertainty) is maximum when <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?p=1/2" align="absmiddle" border="0" /> and for other values of <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?p" align="absmiddle" border="0" />, the entropy is lower. The entropy becomes 0 when <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?p=0\mbox{ or }1" align="absmiddle" border="0" /> i.e. when the value of <img alt="" src="http://www.dsplog.com/cgi-bin/mimetex.cgi?X" align="absmiddle" border="0" /> becomes deterministic. If we extend this to a source with more than two symbols,  <strong>when probability of one of the symbols  becomes more higher than the other, the uncertainty decreases and hence entropy also decreases</strong>.</p>
<p><strong>Based on the above, the right choice is (D) decreases</strong></p>
<p><strong> </strong></p>
<h2>References</h2>
<p>[1] GATE Examination Question Papers [Previous Years] from Indian Institute of Technology, Madras <a href="http://gate.iitm.ac.in/gateqps/2012/ec.pdf">http://gate.iitm.ac.in/gateqps/2012/ec.pdf</a></p>
<p><strong>[2] Elements of Information Theory, Thomas M. Cover, Joy A. Thomas (<a href="http://www.amazon.com/gp/product/0471241954/ref=as_li_ss_tl?ie=UTF8&amp;camp=1789&amp;creative=390957&amp;creativeASIN=0471241954&amp;linkCode=as2&amp;tag=dl04-20">Buy from Amazon.com</a><img style="border: none !important; margin: 0px !important;" alt="" src="http://www.assoc-amazon.com/e/ir?t=dl04-20&amp;l=as2&amp;o=1&amp;a=0471241954" width="1" height="1" border="0" />, <a href="http://www.flipkart.com/elements-information-theory-1st/p/itmdytmgcgtszgtx?pid=9788126508143&amp;affid=krishnadsp">Buy from Flipkart.com</a>)</strong></p>
<p>&nbsp;</p>
<p>&nbsp;</p>
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		<title>GATE-2012 ECE Q7 (digital)</title>
		<link>http://feedproxy.google.com/~r/dsplogdotcom/~3/iL8qDp8dEJQ/</link>
		<comments>http://www.dsplog.com/2013/01/23/gate-2012-ece-q7-digital/#comments</comments>
		<pubDate>Wed, 23 Jan 2013 01:23:05 +0000</pubDate>
		<dc:creator>Krishna Sankar</dc:creator>
				<category><![CDATA[GATE]]></category>
		<category><![CDATA[2012]]></category>
		<category><![CDATA[Digital]]></category>
		<category><![CDATA[ECE]]></category>
		<category><![CDATA[Q7]]></category>

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		<description>Question 7 on digital from GATE (Graduate Aptitude Test in Engineering) 2012 Electronics and Communication Engineering paper. Q7. The output Y of a 2-bit comparator is logic 1 whenever the 2 bit input A is [...]&lt;div class='yarpp-related-rss'&gt;
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				<content:encoded><![CDATA[<p></p><p>Question 7 on digital from GATE (Graduate Aptitude Test in Engineering) 2012 Electronics and Communication Engineering paper.</p>
<h2>Q7. The output Y of a 2-bit comparator is logic 1 whenever the 2 bit input A is greater than 2 bit input B. The number of combinations for which output is logic 1 is</h2>
<h2>(A) 4</h2>
<h2>(B) 6</h2>
<h2>(C) 8</h2>
<h2>(D) 10</h2>
<p><img title="More..." alt="" src="http://www.dsplog.com/db-install/wp-includes/js/tinymce/plugins/wordpress/img/trans.gif" /></p>
<h2>Solution</h2>
<p>Let&#8217;s write all the 16 possible combinations of A and B and count the number of times A is greater than B. Can easily see that the count is 16.</p>
<table border="1" cellspacing="0">
<colgroup span="3" width="85"></colgroup>
<tbody>
<tr>
<td align="CENTER" height="16"><b>A</b></td>
<td align="CENTER"><b>B</b></td>
<td align="CENTER"><b>Out</b></td>
</tr>
<tr>
<td align="CENTER" height="16">0</td>
<td align="CENTER">0</td>
<td align="CENTER">0</td>
</tr>
<tr>
<td align="CENTER" height="16">0</td>
<td align="CENTER">1</td>
<td align="CENTER">0</td>
</tr>
<tr>
<td align="CENTER" height="16">0</td>
<td align="CENTER">2</td>
<td align="CENTER">0</td>
</tr>
<tr>
<td align="CENTER" height="16">0</td>
<td align="CENTER">3</td>
<td align="CENTER">0</td>
</tr>
<tr>
<td align="CENTER" height="16">1</td>
<td align="CENTER">0</td>
<td align="CENTER">1</td>
</tr>
<tr>
<td align="CENTER" height="16">1</td>
<td align="CENTER">1</td>
<td align="CENTER">0</td>
</tr>
<tr>
<td align="CENTER" height="16">1</td>
<td align="CENTER">2</td>
<td align="CENTER">0</td>
</tr>
<tr>
<td align="CENTER" height="16">1</td>
<td align="CENTER">3</td>
<td align="CENTER">0</td>
</tr>
<tr>
<td align="CENTER" height="16">2</td>
<td align="CENTER">0</td>
<td align="CENTER">1</td>
</tr>
<tr>
<td align="CENTER" height="16">2</td>
<td align="CENTER">1</td>
<td align="CENTER">1</td>
</tr>
<tr>
<td align="CENTER" height="16">2</td>
<td align="CENTER">2</td>
<td align="CENTER">0</td>
</tr>
<tr>
<td align="CENTER" height="16">2</td>
<td align="CENTER">3</td>
<td align="CENTER">0</td>
</tr>
<tr>
<td align="CENTER" height="16">3</td>
<td align="CENTER">0</td>
<td align="CENTER">1</td>
</tr>
<tr>
<td align="CENTER" height="16">3</td>
<td align="CENTER">1</td>
<td align="CENTER">1</td>
</tr>
<tr>
<td align="CENTER" height="16">3</td>
<td align="CENTER">2</td>
<td align="CENTER">1</td>
</tr>
<tr>
<td align="CENTER" height="16">3</td>
<td align="CENTER">3</td>
<td align="CENTER">0</td>
</tr>
<tr>
<td align="CENTER" height="16"></td>
<td align="CENTER"></td>
<td align="CENTER"></td>
</tr>
<tr>
<td align="CENTER" height="16"></td>
<td align="CENTER"><b>TOTAL</b></td>
<td align="CENTER"><b>6</b></td>
</tr>
</tbody>
</table>
<p>Alternately, pick each value of A and count the number of instances when A is greater than B. The count is 0 + 1 + 2 + 3 for A = 0,1,2,3 respectively.</p>
<p><strong>Based on the above, the right choice is (B) 6</strong></p>
<p><strong> </strong></p>
<h2>References</h2>
<p>[1] GATE Examination Question Papers [Previous Years] from Indian Institute of Technology, Madras <a href="http://gate.iitm.ac.in/gateqps/2012/ec.pdf">http://gate.iitm.ac.in/gateqps/2012/ec.pdf</a></p>
<p>&nbsp;</p>
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