<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2012.312272</article-id><article-id pub-id-type="publisher-id">AM-25597</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Generalized Entropy of Order Statistics
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>icha</surname><given-names>Thapliyal</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>H.</surname><given-names>C. Taneja</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Applied Mathematics, Delhi Technological University, Delhi, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>richa31aug@gmail.com(IT)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>12</day><month>12</month><year>2012</year></pub-date><volume>03</volume><issue>12</issue><fpage>1977</fpage><lpage>1982</lpage><history><date date-type="received"><day>September</day>	<month>4,</month>	<year>2012</year></date><date date-type="rev-recd"><day>October</day>	<month>12,</month>	<year>2012</year>	</date><date date-type="accepted"><day>October</day>	<month>20,</month>	<year>2012</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this communication, we consider and study a generalized two parameters entropy of order statistics and derive bounds for it. The generalized residual entropy using order statistics has also been discussed.
 
</p></abstract><kwd-group><kwd>Entropy; Order Statistics; Probability Integral Transformation; Residual Entropy; Generalized Information</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Suppose <img src="22-7401093\39ebb37a-32a6-4c1d-9b13-da27cacfed4c.jpg" /> are <img src="22-7401093\74f9b6ea-884b-48b0-9eff-b151fe5250a4.jpg" /> independent and identically distributed observations from a distribution<img src="22-7401093\5e21f855-75bd-49c4-ae6a-3b2fb474d226.jpg" />, where <img src="22-7401093\33ecd68e-d5bf-4437-ab77-ac6a374069e1.jpg" /> is differentiable with a density <img src="22-7401093\0cf441cb-1364-40b1-892d-7d32b31ce51c.jpg" /> which is positive in an interval and zero elsewhere. The order statistics of the sample is defined by the arrangement of <img src="22-7401093\59cacc73-e641-40cc-b5d2-d3cecdcbe70a.jpg" /> from the smallest to largest denoted as<img src="22-7401093\7b9ff432-290f-46ba-86e2-fe68fe6c0795.jpg" />. Then the p.d.f. of the <img src="22-7401093\19d8d3f2-abf3-4cff-8365-455e497a6891.jpg" /> order statistics<img src="22-7401093\e3311a2b-04c5-44eb-b83f-9c2095ab592a.jpg" />, is given by</p><disp-formula id="scirp.25597-formula70094"><label>(1)</label><graphic position="anchor" xlink:href="22-7401093\f332f1b1-267b-43ff-ad9e-33f4529ee97a.jpg"  xlink:type="simple"/></disp-formula><p>for details refer to [<xref ref-type="bibr" rid="scirp.25597-ref1">1</xref>].</p><p>Order statistics has been studied by statisticians for some time and has been applied to problems of statistical estimation [<xref ref-type="bibr" rid="scirp.25597-ref2">2</xref>], reliability analysis, image coding [<xref ref-type="bibr" rid="scirp.25597-ref3">3</xref>] etc. Some information theoretic aspects of order statistics have been discussed in the literature. Wong and Chen [<xref ref-type="bibr" rid="scirp.25597-ref4">4</xref>] showed that the difference between average entropy of order statistics and the entropy of a data distribution is a constant. Park [<xref ref-type="bibr" rid="scirp.25597-ref5">5</xref>] showed some recurrence relations for entropy of order statistics. Information properties of order statistics based on Shannon entropy [<xref ref-type="bibr" rid="scirp.25597-ref6">6</xref>] and Kullback-Leibler [<xref ref-type="bibr" rid="scirp.25597-ref7">7</xref>] measure using probability integral transformation have been studied by Ebrahimi et al. [<xref ref-type="bibr" rid="scirp.25597-ref8">8</xref>]. Arghami and Abbasnejad [<xref ref-type="bibr" rid="scirp.25597-ref9">9</xref>] studied Renyi entropy properties based on order statistics. The Renyi [<xref ref-type="bibr" rid="scirp.25597-ref10">10</xref>] entropy is a single parameter entropy. We consider a generalized two parameter, the Verma entropy [<xref ref-type="bibr" rid="scirp.25597-ref11">11</xref>], and study it in context with order statistics. Verma entropy plays a vital role as a measure of complexity and uncertainty in different areas such as physics, electronics and engineering to describe many chaotic systems. Considering the importance of this entropy measure, it will be worthwhile to study it in case of order statistics. The rest of the article is organized as follows:</p><p>In Section 2, we express generalized entropy of <img src="22-7401093\57ec7a23-cf89-4279-aab1-0a840c58bf95.jpg" /> order statistics in terms of generalized entropy of <img src="22-7401093\d8d10b3e-c609-44de-bf42-a59bff2c0ffe.jpg" /> order statistics of uniform distribution and study some of its properties. Section 3 provides bounds for entropy of order statistics. In Section 4, we derive an expression for residual generalized entropy of order statistics using residual generalized entropy for uniform distribution.</p></sec><sec id="s2"><title>2. Generalized Entropy of Order Statistics</title><p>Let <img src="22-7401093\f66c2350-0fbb-4ed4-b866-7a4cb6b73988.jpg" /> be a random variable having an absolutely continuous cdf <img src="22-7401093\49f5074a-570f-45a4-9871-f16c5b6b5cc8.jpg" /> and pdf<img src="22-7401093\a74f4e3c-4b75-4d2a-acb6-e97833dc320e.jpg" />, then Verma [<xref ref-type="bibr" rid="scirp.25597-ref11">11</xref>] entropy of the random variable <img src="22-7401093\f933cf4e-dd01-4511-a006-2c47d2df2607.jpg" /> with parameters <img src="22-7401093\bde17007-2bb9-4fc7-92cf-6d839c25cb5f.jpg" /> is defined as:</p><disp-formula id="scirp.25597-formula70095"><label>(2)</label><graphic position="anchor" xlink:href="22-7401093\43e5cd0c-7037-4405-b757-2387ecb8b377.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="22-7401093\3277635c-1ccc-49ae-8fe2-56908e4167e7.jpg" /></p><p>is the Renyi entropy, and</p><p><img src="22-7401093\6420636f-5bcc-495c-b6e6-ff737f905735.jpg" /></p><p>is the Shannon entropy .</p><p>We use the probability integral transformation of the random variable <img src="22-7401093\5ebb5de4-9e86-4df4-a8c8-e9104fb63d41.jpg" /> where the distribution of U is the standard uniform distribution. If <img src="22-7401093\7d8e1ddd-da64-4b38-88c6-45a256deddb1.jpg" /> are the order statistics of a random sample <img src="22-7401093\c4b17cb1-c895-4c53-ae14-363c37809851.jpg" /> from uniform distribution, then it is easy to see using (1) that <img src="22-7401093\7eac1432-eae2-4305-b86f-0209b0d8cf87.jpg" /> has beta distribution with parameters <img src="22-7401093\e2a6570c-3e17-414d-b641-ffbb73fcb2df.jpg" /> and<img src="22-7401093\6b7278b4-4420-4b89-926d-4d2223c4fa46.jpg" />. Using probability integral transformation, entropy (2) of the random variable <img src="22-7401093\308e00b0-f81d-4e60-a17e-22701d8f07f8.jpg" /> can be represented as</p><disp-formula id="scirp.25597-formula70096"><label>(3)</label><graphic position="anchor" xlink:href="22-7401093\8fe9201a-8be6-4ba5-9e8f-98d08c332965.jpg"  xlink:type="simple"/></disp-formula><p>Next, we prove the following result:</p><p>Theorem 2.1 The generalized entropy of <img src="22-7401093\0c2279ac-32ca-4fa7-b4f3-922a8b35727c.jpg" /> can be expressed as</p><disp-formula id="scirp.25597-formula70097"><label>(4)</label><graphic position="anchor" xlink:href="22-7401093\9dffa109-222a-4459-8ab3-ae132fe9a535.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="22-7401093\c62e5f50-dc6a-4b66-9d85-4b008063a4ea.jpg" /> denotes the entropy of the beta distribution with parameters <img src="22-7401093\a260685d-b9cb-4e02-bd0a-202fdd915d46.jpg" /> and<img src="22-7401093\1295cfff-8fe4-4d21-b6b9-b0c6fe6c949f.jpg" />, <img src="22-7401093\f1184ab3-42e5-41dd-a4fc-25e26f082c88.jpg" />denotes expectation of <img src="22-7401093\5c4b99b9-c75a-413d-b66e-c89d17adf21b.jpg" /> over <img src="22-7401093\2c6aa5f7-1ee2-4cb9-99f7-eb1fb693390e.jpg" /> and <img src="22-7401093\a6dc57d6-2733-4279-b857-bc6fbb7ec02a.jpg" /> is the beta density with parameters <img src="22-7401093\465e05d6-75f2-47da-a1c7-90267ed598c4.jpg" /> and</p><p><img src="22-7401093\e32d42ff-0dd3-47b9-90ff-4df18da90361.jpg" />.</p><p>Proof: Since <img src="22-7401093\9edb6990-8478-4996-bb25-7674c9fc148f.jpg" /> which implies<img src="22-7401093\53579c22-8c46-4b2d-9feb-ab3da3f189f1.jpg" />. Thus, from (3) we have</p><disp-formula id="scirp.25597-formula70098"><label>(5)</label><graphic position="anchor" xlink:href="22-7401093\f82e7219-b458-44b4-bd87-9460346baaf3.jpg"  xlink:type="simple"/></disp-formula><p>It is easy to see that the entropy (2) for the beta distribution with parameters <img src="22-7401093\3d81349f-04f0-4677-8e7c-792634909bd7.jpg" /> and <img src="22-7401093\beb01301-16c6-4160-8e81-52d22e71188d.jpg" /> (that is, the <img src="22-7401093\ad260766-012d-4ed6-996b-bfb652fcfc7e.jpg" /> order statistics of uniform distribution) is given by</p><disp-formula id="scirp.25597-formula70099"><label>(6)</label><graphic position="anchor" xlink:href="22-7401093\e22306c7-9527-4ced-8d50-dfdd273a40b7.jpg"  xlink:type="simple"/></disp-formula><p>Using (6) in (5), the desired result (4) follows.</p><p>In particular, by taking<img src="22-7401093\683d21c2-42df-4b01-a817-03c842352015.jpg" />, (4) reduces to</p><p><img src="22-7401093\6e6d2b25-d38e-4fe3-a314-748d6fe6b148.jpg" /></p><p>a result derived by Ebrahimi et al. [<xref ref-type="bibr" rid="scirp.25597-ref8">8</xref>].</p><p>Remark: In reliability engineering <img src="22-7401093\4e8b0b46-3c84-4bbd-9cc7-090e8c05a425.jpg" />-outof-<img src="22-7401093\15445e84-75d1-4f3c-aa0f-f083173be567.jpg" /> systems are very important kind of structures. A <img src="22-7401093\ee58a940-6d08-401c-8adc-ffcb5510a48c.jpg" />-out-of-<img src="22-7401093\47792696-1240-49dd-a85b-d2df70f3b7dc.jpg" /> system functions iff atleast</p><p><img src="22-7401093\3e12816f-0bd2-4e4d-a3fe-ed6d7c9f5fb8.jpg" />components out of <img src="22-7401093\ff043e55-6f77-4e49-b857-1a671a4fbf78.jpg" /> components function. If <img src="22-7401093\d4ac27ed-dd4d-4c1b-b44a-20dffbc77bd2.jpg" /> denote the independent lifetimes of the components of such system, then the lifetime of the system is equal to the order statistic<img src="22-7401093\100ee7c4-a29a-4936-a2cc-144b5cd668c8.jpg" />. The special case of <img src="22-7401093\a7451b20-4f35-4bc6-bef5-3a34ae5dde86.jpg" /> and<img src="22-7401093\3dc2951e-fc63-4982-a2d2-f9ee8556011f.jpg" />, that is for sample minima and maxima correspond to series and parallel systems respectively. In the following example, we calculate entropy (4) for sample maxima and minima for an exponential distribution.</p><p>Example 2.1 Let <img src="22-7401093\d722a85e-8932-48cb-9bd8-d9caa417249d.jpg" /> be a random variable having the exponential distribution with pdf</p><p><img src="22-7401093\6136ff77-07f2-4b47-a5c7-50fb0b37b27c.jpg" /></p><p>Here, <img src="22-7401093\4e6f8857-d07a-4a74-b95a-1ddffb3fea9d.jpg" />and the expectation term is given by</p><p><img src="22-7401093\0d4fc6c2-5aee-439d-96e8-fd61efc69448.jpg" /></p><p>For<img src="22-7401093\ebaf93fa-5c3d-4b8a-997a-dc070b6dadd4.jpg" />, from (6), we have</p><p><img src="22-7401093\c8399e13-e104-4bbd-ada3-a9b1b9ec5677.jpg" /></p><p>Hence, using (4)</p><p><img src="22-7401093\012aa507-2a79-4be0-ae00-4a0e1e777ac5.jpg" />which confirms that the sample minimum has an exponential distribution with parameter<img src="22-7401093\b82cc5b3-c389-4b61-bf73-01bbb3c0b44a.jpg" />, since</p><p><img src="22-7401093\cdf9d735-9b95-4790-ac1d-c0f384814646.jpg" /></p><p>where <img src="22-7401093\859bba97-a9b1-4b6f-859b-d80bf8e0d824.jpg" /> is an exponential variate with parameter<img src="22-7401093\042497c3-759c-4589-bca1-be08fc1d6ec0.jpg" />. Also</p><p><img src="22-7401093\88f018bf-32e2-49ee-9360-d333ede83521.jpg" /></p><p>Hence, the difference between the generalized entropy of first order statistics i.e. the sample minimum and the generalized entropy of parent distribution is independent of parameter<img src="22-7401093\65e360b7-ea37-41ed-8853-d72eb1a1d224.jpg" />, but it depends upon sample size<img src="22-7401093\002e0ba8-2cbf-4b69-9415-f73952d6c750.jpg" />. Similarly, for sample maximum, we have</p><p><img src="22-7401093\2ed5d261-7680-47d9-b2ca-481622b99c19.jpg" /></p><p>It can be seen easily that the difference between <img src="22-7401093\169d8308-9709-44ff-9aa4-656228f43d2e.jpg" /> and <img src="22-7401093\8ae8b03e-ff3c-4b4e-916c-76125c6e88f5.jpg" /> is</p><p><img src="22-7401093\6a8e65ad-df53-428a-a92e-a3809aa2ca3e.jpg" /></p><p>which is also independent of parameter<img src="22-7401093\fee7f210-8a9f-448e-b3be-67e7dd1c025a.jpg" />.</p></sec><sec id="s3"><title>3. Bounds for the Generalized Entropy of Order Statistics</title><p>In this section, we find the bounds for generalized entropy for order statistics (4) in terms of entropy (2). We prove the following result.</p><p>Theorem 3.1 For any random variable <img src="22-7401093\e5b4ddb6-276b-4818-a627-4884a081534d.jpg" /> with<img src="22-7401093\9a36732f-5fae-4967-85b1-c4c683205f2c.jpg" />, the entropy of the <img src="22-7401093\aee8dff8-b3c2-49f6-ae1b-a2415d59cdd1.jpg" /> order statistics <img src="22-7401093\62037462-5ea5-4bca-99d3-1f6d12862b5c.jpg" /> is bounded above as</p><disp-formula id="scirp.25597-formula70100"><label>(7)</label><graphic position="anchor" xlink:href="22-7401093\d9b757a2-8f94-48c0-9745-0e8cf3a8bc1a.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="22-7401093\3098fd37-8bf9-41fb-ba34-05452a069f5d.jpg" /></p><p>and, bounded below as</p><disp-formula id="scirp.25597-formula70101"><label>(8)</label><graphic position="anchor" xlink:href="22-7401093\904d2435-99ff-406d-b895-6504d1f4e177.jpg"  xlink:type="simple"/></disp-formula><p>where, <img src="22-7401093\c33fd6eb-a173-42a5-9f6d-736f297e66ff.jpg" />, and <img src="22-7401093\602668bc-3119-4524-b946-6c1600290de4.jpg" /> is the mode of the distribution and <img src="22-7401093\af99195b-e3e3-4d86-b245-754fe82beb44.jpg" /> is pdf of the random variable<img src="22-7401093\0ab43ecb-28e6-412e-85ea-3490fbbde7e7.jpg" />.</p><p>Proof: The mode of the beta distribution <img src="22-7401093\6afffb1f-1d08-4e92-afa7-6bfb051f7ae6.jpg" /> is<img src="22-7401093\76c80d28-f779-4c24-8aee-22456f1ec546.jpg" />. Thus,</p><p><img src="22-7401093\e5c6f82d-4b7d-41b3-820c-fbef525dcfd1.jpg" /></p><p>For<img src="22-7401093\0de91b5c-3627-4cd0-b5d0-d196ba281d53.jpg" />, from (4)</p><p><img src="22-7401093\53d68be3-1689-4937-8a9a-e72dc5b1df63.jpg" /></p><p>which gives (7).</p><p>From (4) we can write</p><p><img src="22-7401093\b65416af-c01a-48cd-ac8b-29b830ad12ec.jpg" /></p><p>Example 3.1 For the uniform distribution over the interval <img src="22-7401093\5d2d8c8b-f153-4fef-a0a9-a7e7afae055c.jpg" /> we have</p><p><img src="22-7401093\44ffea34-6246-48d0-b32c-9b5892eb898c.jpg" /></p><p>and from (6),</p><p><img src="22-7401093\4388a91c-d8fb-4209-be13-a0bf4675f86b.jpg" /></p><p>and</p><p><img src="22-7401093\12ac3586-7b0d-4f0e-9e13-1abe6fa16b07.jpg" /></p><p>Hence, using (7) we get</p><p><img src="22-7401093\a32ba668-00da-40ef-b3b9-11d9cf404f6e.jpg" /></p><p>Further, for uniform distribution over the interval</p><p><img src="22-7401093\ac4f53dd-6ba7-40ea-b44b-510b391a87d7.jpg" />,<img src="22-7401093\258fd61e-ea87-433d-b419-5a164f77546b.jpg" />. Using (8) we get</p><p><img src="22-7401093\a8190779-c224-4d6e-a77b-be0ce32ccd40.jpg" /></p><p>Thus, for uniform distribution, we have</p><p><img src="22-7401093\f411b7e1-21a7-4aab-a409-edbf8831458f.jpg" /></p><p>We can check that the bounds for <img src="22-7401093\6373a483-3941-4c27-9dc8-10203dc942f7.jpg" /> are same as that of<img src="22-7401093\04998f1b-1f64-4ab0-b1d5-c40cce0e7e13.jpg" />.</p><p>Example 3.2 For the exponential distribution with parameter<img src="22-7401093\8adc4423-d4bf-421f-984d-d1b6ae5eb3e2.jpg" />, we have <img src="22-7401093\efb0bf7a-8463-436e-92dc-5a0905810602.jpg" /> and</p><p><img src="22-7401093\83a57ffb-9869-48b0-9813-a37de042fd8e.jpg" /></p><p>Thus, as calculated in Example 2.1</p><p><img src="22-7401093\daf6a14b-d063-46e3-a9af-6c76013ae238.jpg" /></p><p>Using Theorem 3.1</p><p><img src="22-7401093\b97043f6-27ba-48ec-8754-b0e79a2dcf32.jpg" /></p><p>Here we observe that the difference between upper bound and <img src="22-7401093\187b76f5-c982-4f25-8d07-f49f06140024.jpg" /> is<img src="22-7401093\f7ba6a79-e749-4d65-a2a1-af41a3717e12.jpg" />, which is an increasing function of n. Thus, for the exponential distribution upper bound is not useful when sample size is large.</p></sec><sec id="s4"><title>4. The Generalized Residual Entropy of Order Statistics</title><p>In reliability theory and survival analysis, <img src="22-7401093\b0a4ce68-9cb9-4bd2-9fc1-82a5a1d84bdf.jpg" />usually denotes a duration such as the lifetime. The residual lifetime of the system when it is still operating at time<img src="22-7401093\de37c84d-d411-4061-bd3b-b661a9bb3420.jpg" />, given by <img src="22-7401093\31326af1-e959-4a3e-9fe1-bbbcd47f9c10.jpg" /> has the probability density</p><p><img src="22-7401093\a565de10-b08d-412d-8eb0-7adf3e5d1195.jpg" />, where<img src="22-7401093\d3767696-c355-4f90-9328-aff252b1da75.jpg" />. Ebrahimi [<xref ref-type="bibr" rid="scirp.25597-ref12">12</xref>] proposed the entropy of the residual lifetime <img src="22-7401093\cce40274-d94e-46d1-9977-8b46abd439a2.jpg" /> as</p><disp-formula id="scirp.25597-formula70102"><label>(9)</label><graphic position="anchor" xlink:href="22-7401093\61058f27-b06b-4fa6-9e67-115b0c0b45f8.jpg"  xlink:type="simple"/></disp-formula><p>Obviously, when<img src="22-7401093\b0b62d20-0c5d-482b-8a94-951fcf9584de.jpg" />, it reduces to Shannon entropy.</p><p>The generalized residual entropy of the type <img src="22-7401093\5bc5c42a-b0ed-433d-a1b3-b7718e9cb1d8.jpg" /> is defined as</p><disp-formula id="scirp.25597-formula70103"><label>(10)</label><graphic position="anchor" xlink:href="22-7401093\c65d71fa-1f4e-4849-be71-9d944a2baeae.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="22-7401093\cc890170-1c7b-4138-a88a-ff8119481b78.jpg" />. When<img src="22-7401093\b79c81e8-bcc2-43c8-9eca-c77240548727.jpg" />, it reduces to (2).</p><p>We note that the density function and survival function of <img src="22-7401093\fa19b29b-e28b-4d9a-87de-36e7328fed81.jpg" /> (refer to [<xref ref-type="bibr" rid="scirp.25597-ref13">13</xref>]), denoted by <img src="22-7401093\44ecce70-1ac5-4cf9-b1a4-a2c734617604.jpg" /> and<img src="22-7401093\caa05bd3-7d39-4717-9b92-96a851cabaa5.jpg" />, respectively are</p><disp-formula id="scirp.25597-formula70104"><label>(11)</label><graphic position="anchor" xlink:href="22-7401093\459a8eae-7a09-4c7d-8700-2d8757733a1f.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.25597-formula70105"><label>(12)</label><graphic position="anchor" xlink:href="22-7401093\bc720e38-5d28-4e01-a6cb-9b487f87006e.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.25597-formula70106"><label>(13)</label><graphic position="anchor" xlink:href="22-7401093\c7be4287-c2b5-4b92-841f-d126484705ae.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.25597-formula70107"><label>(14)</label><graphic position="anchor" xlink:href="22-7401093\3b7f00de-6b43-4c86-b788-f255bda98e73.jpg"  xlink:type="simple"/></disp-formula><p><img src="22-7401093\2617c2f9-ae73-432d-969d-a87b2909182d.jpg" />and <img src="22-7401093\b5cb2e67-b046-4278-bb7a-18357a6b029e.jpg" /> are known as the beta and incomplete beta functions respectively. In the next lemmawe derive an expression for <img src="22-7401093\ab354845-9e34-49b4-8187-22990caab8aa.jpg" /> for the dynamic version of <img src="22-7401093\b58825c1-5f48-408f-8dce-74319ea2b3d5.jpg" /> as given by (6).</p><p>Lemma 4.1 Let <img src="22-7401093\14683fba-cb55-4b92-8217-e10152cbb925.jpg" /> be the <img src="22-7401093\89f4611b-9d87-42de-8e20-da747d38954f.jpg" /> order statistics based on a random sample of size <img src="22-7401093\ca03c363-3806-40ee-bfd3-9a69e1c67ce2.jpg" /> from uniform distribution on<img src="22-7401093\c04d59b3-5061-4144-b506-06a7ff0ea4e8.jpg" />. Then</p><disp-formula id="scirp.25597-formula70108"><label>(15)</label><graphic position="anchor" xlink:href="22-7401093\72f264ef-a84b-4d8f-ab84-12e70b7440b2.jpg"  xlink:type="simple"/></disp-formula><p>Proof: For uniform distribution using (10), we have</p><disp-formula id="scirp.25597-formula70109"><label>(16)</label><graphic position="anchor" xlink:href="22-7401093\8ebd57f6-ca12-4dec-b4e7-e45ea4ae6ff1.jpg"  xlink:type="simple"/></disp-formula><p>Putting values from (11) and (13) in (16), we get the desired result (15).</p><p>If we put <img src="22-7401093\c9d5d41d-db4e-4ef5-81a1-d86c2e877df9.jpg" /> in (15), we get (6).</p><p>Using this, in the following theorem, we will show that the residual entropy of order statistics <img src="22-7401093\dc3dd8ad-bf66-4dc7-a257-e7bc6e42ac43.jpg" /> can be represented in terms of residual entropy of uniform distribution.</p><p>Theorem 4.1 Let <img src="22-7401093\f0711a35-464f-4664-9431-8aed0bf7487f.jpg" /> be an absolutely continuous distribution function with density<img src="22-7401093\eca48465-67ea-4882-b504-96992f8b9fb8.jpg" />. Then, generalized residual entropy of the <img src="22-7401093\d3735864-e33a-4cc2-951e-a325a299604c.jpg" /> order statistics can be represented as</p><disp-formula id="scirp.25597-formula70110"><label>(17)</label><graphic position="anchor" xlink:href="22-7401093\3feb5260-7d67-4165-8fe7-a6096f0ef370.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="22-7401093\04e192e0-7e29-49f8-b4aa-c3d27e41fe74.jpg" /></p><p>Proof: Using the probability integral transformation</p><p><img src="22-7401093\dc96d2a2-319d-4c8f-b23a-c62ed9447a70.jpg" /></p><p>and above lemma, the result follows.</p><p>Take <img src="22-7401093\146fd01a-1a60-4718-b414-965ed9afae82.jpg" /> in (17), it reduces to (4).</p><p>Example 4.1 Suppose that <img src="22-7401093\cae56d0e-943b-486d-a7cc-84c511b3b30c.jpg" /> is exponentially distributed random variable with mean<img src="22-7401093\50e5c116-d861-4532-84ec-1f0f8de50708.jpg" />. Then,</p><p><img src="22-7401093\47eaab70-35c0-4362-843b-b19d7cdadba9.jpg" /></p><p>and we have</p><p><img src="22-7401093\bd8fb069-778a-4aa3-86f3-3c10dbc62a10.jpg" /></p><p>For<img src="22-7401093\31fe18ec-ce9d-4284-80c3-2b9d8a75a836.jpg" />, Theorem 4.1 gives</p><p><img src="22-7401093\6c3263e5-0b08-4b64-897e-8185c674e998.jpg" /></p><p>Also</p><p><img src="22-7401093\e1db77c3-c59f-4e16-b179-df2f2ad38254.jpg" /></p><p>Hence</p><p><img src="22-7401093\2a45796e-3f36-445d-9c24-cca785181f15.jpg" /></p><p>So, in the exponential case the difference between generalized residual entropy of the lifetime of a series system and residual generalized entropy of the lifetime of each component is independent of time.</p></sec><sec id="s5"><title>5. Conclusion</title><p>The two parameters generalized entropy plays a vital role as a measure of complexity and uncertainty in different areas such as physics, electronics and engineering to describe many chaotic systems. 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