<?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">JMF</journal-id><journal-title-group><journal-title>Journal of Mathematical Finance</journal-title></journal-title-group><issn pub-type="epub">2162-2434</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmf.2016.61019</article-id><article-id pub-id-type="publisher-id">JMF-63977</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Business&amp;Economics</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Burr Distribution as an Actuarial Risk Model and the Computation of Some of Its Actuarial Quantities Related to the Probability of Ruin
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>agriti</surname><given-names>Das</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>Dilip</surname><given-names>C. Nath</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Statistics, Gauhati University, Assam, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>jagritistat123.das@gmail.com(AD)</email>;<email>dilipc.nath@gmail.com(DCN)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>05</day><month>02</month><year>2016</year></pub-date><volume>06</volume><issue>01</issue><fpage>213</fpage><lpage>231</lpage><history><date date-type="received"><day>12</day>	<month>January</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>26</month>	<year>February</year>	</date><date date-type="accepted"><day>29</day>	<month>February</month>	<year>2016</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 paper, we have used an algorithm to fit the Burr XII distribution to a set of insurance data. As it is well known, the probability of ultimate ruin is obtained as a solution to an integro-differential equation and in case, the claim severity is distributed as Burr XII distribution, this equation has to be solved numerically to obtain an approximation to the probability of ultimate ruin. Two numerical algorithms, namely the stable recursive algorithm and the method of product integration have been used to obtain numerically an approximation to this probability of ultimate ruin. The use of these two numerical algorithms provides a scope for comparing the consistency in values obtained by them. The first two moments of the time to ruin in case of Burr XII distributed claim severity have also been computed using the probability of ultimate ruin obtained through the stable recursive algorithm as an input. All these computations have been done under the assumption of the classical risk model. 
 
</p></abstract><kwd-group><kwd>Stable Algorithms in Ruin Theory</kwd><kwd> Product Integration</kwd><kwd> Time to Ruin</kwd><kwd> Classical Risk Model</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>An actuarial risk model is concerned with the study of the mathematical aspects observed in the behavior of a collection of risks generated by an insurance portfolio. In general insurance risk modeling, the two quantities of paramount importance are the number of claims arriving in a fixed time period and size of each claim. Modeling of the former aspect is done in terms of a discrete distribution, more specifically a counting distribution whereas the claim severity is modeled through what is known as a loss distribution.</p><p>There are compelling reasons to use mathematical models to describe insurance loss amounts (claim severities). As specified, in [<xref ref-type="bibr" rid="scirp.63977-ref1">1</xref>] in the most general sense, all of actuarial science is about loss distributions. For any insurance company, the sound statistical analysis of the underlying claim scenario, reflected in terms of loss modeling is of uttermost importance because it is the basis on which lies the subsequent determination of various actuarial quantities of interest like probability of ruin, premium loading, pure premium, expected profits, reserved to be maintained and the impact of reinsurance and deductibles.</p><p>A good introduction to the subject of fitting distribution to losses is given in [<xref ref-type="bibr" rid="scirp.63977-ref2">2</xref>] . Most data in general insurance are skewed to the right and therefore distributions with high degree of positive skewness such as Lognormal, Pareto, Gamma, Weibull and Burr had been used by actuaries to fit claim sizes [<xref ref-type="bibr" rid="scirp.63977-ref2">2</xref>] . However as stated in [<xref ref-type="bibr" rid="scirp.63977-ref3">3</xref>] , in different classes of insurance business, it is not clear which distributions are suitable for modeling claims arising in different portfolios.</p><p>The three-parameter Burr XII distribution was originally used in the analysis of lifetime data and is becoming increasingly useful in the context of actuarial science [<xref ref-type="bibr" rid="scirp.63977-ref4">4</xref>] . The data used in this paper are on motor insurance where one typical characteristics is the occurrence of large but infrequent claims and hence there is a need to fit and use a statistical distribution which is heavy tailed and highly skewed towards the right and this justifies why heavy tailed distributions such as Pareto, Weibull and Burr are suitable candidates for loss modeling in motor insurance (see [<xref ref-type="bibr" rid="scirp.63977-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.63977-ref6">6</xref>] ). Although there can be other suitable models for loss modeling in general insurance, we are primarily concerned with the Burr distribution as a loss model for our claim data and have concentrated on the computation of various actuarial quantities like the probability of ruin and the moments of the time to ruin when the loss model or claim severity model is Burr XII. Literature ([<xref ref-type="bibr" rid="scirp.63977-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.63977-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.63977-ref8">8</xref>] ) reveals that no closed form expression is available for the determination of these quantities in case of Burr XII distributed claim amounts and hence, we resort to numerical techniques to compute them. Briefly our objectives for this paper are:</p><p>1) To fit the Burr XII distribution to a set of insurance data through an algorithm mentioned in [<xref ref-type="bibr" rid="scirp.63977-ref9">9</xref>] and to assess the goodness of fit through some statistics based on the empirical distribution functions (EDF statistics).</p><p>2) To compute the probability of ultimate ruin when the claim severity is distributed as our fitted Burr XII distribution as well as a Burr XII distribution with a set of illustrative values for its parameters, using two numerical algorithms namely a stable recursive algorithm and the method of Product Integration.</p><p>3) To compute the first two moments of the time to ruin in case of Burr XII distributed claim severity.</p><p>The first part of the paper deals with the Watkins [<xref ref-type="bibr" rid="scirp.63977-ref9">9</xref>] algorithm for obtaining the MLE of the parameters of the Burr XII distribution, followed by testing the goodness of fit through some statistics based on the empirical distribution function (EDF). This is followed by the computation of the probability of ultimate ruin for various values of the initial surplus through the adaptation of the two above mentioned numerical methods. The concluding section deals with the computation of the moments of the time to ruin in case of Burr XII distributed claim severity.</p><p>The illustrative Burr XII distribution that is being used is the one that is being fitted to the Property Claim Services (PCS) dataset covering losses resulting from natural catastrophic events in USA that occurred between 1990 and 1999 [<xref ref-type="bibr" rid="scirp.63977-ref10">10</xref>] .</p></sec><sec id="s2"><title>2. Methodology</title><sec id="s2_1"><title>2.1. Fitting of the Burr Distribution</title><p>The pdf of the three parameter Burr XII distribution is given by</p><disp-formula id="scirp.63977-formula193"><label>(2.1.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x7.png"  xlink:type="simple"/></disp-formula><p>The algorithm for finding the maximum likelihood estimators (MLE) for the parameters of the Burr XII distribution is taken from [<xref ref-type="bibr" rid="scirp.63977-ref9">9</xref>] and this algorithm exploits the link between the three parameter Burr XII distribution and the two parameter Weibull distribution with the latter emerging as the limiting case of the former.</p><p>The cumulative distribution function for the two parameter Weibull distribution is given by</p><disp-formula id="scirp.63977-formula194"><label>(2.1.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x8.png"  xlink:type="simple"/></disp-formula><p>in which the positive parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x9.png" xlink:type="simple"/></inline-formula> are respectively the shape and the scale parameters.</p><p>The basic two parameter Burr XII distribution with shape parameters α and τ has the cumulative distribution function</p><disp-formula id="scirp.63977-formula195"><label>(2.1.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x10.png"  xlink:type="simple"/></disp-formula><p>An scale parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x11.png" xlink:type="simple"/></inline-formula> is introduced into (2.1.3) by substituting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x12.png" xlink:type="simple"/></inline-formula> thereby giving the cdf of y as</p><disp-formula id="scirp.63977-formula196"><label>(2.1.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x13.png"  xlink:type="simple"/></disp-formula><p>Letting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x14.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x15.png" xlink:type="simple"/></inline-formula>remaining finite, it is seen that the Burr XII distribution emerges as the limiting</p><p>distribution for the Weibull distribution with shape parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x16.png" xlink:type="simple"/></inline-formula> and scale parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x17.png" xlink:type="simple"/></inline-formula></p><p>If we consider a sample of “m” items <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x18.png" xlink:type="simple"/></inline-formula> from the Weibull distribution whose cdf is given by (2.1.2), the log likelihood function is given by</p><disp-formula id="scirp.63977-formula197"><label>(2.1.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x19.png"  xlink:type="simple"/></disp-formula><p>And the log likelihood function of the Burr XII distribution is given by</p><disp-formula id="scirp.63977-formula198"><label>(2.1.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x20.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x21.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x22.png" xlink:type="simple"/></inline-formula></p><p>The main steps of the algorithm are:</p><p>Step 1: First, we find the maximum likelihood of the parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x23.png" xlink:type="simple"/></inline-formula> appearing in (2.1.2) using the Multi parameter Newton Raphson Iterative method yielding the two values <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x24.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x25.png" xlink:type="simple"/></inline-formula>.</p><p>Step 2: Then, we rescale the original data by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x26.png" xlink:type="simple"/></inline-formula> so that in implementing the Newton Raphson for determin-</p><p>ing the MLEs of the parameters of the Burr XII distribution, the utilized values are the rescaled values<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x27.png" xlink:type="simple"/></inline-formula>.</p><p>The argument in [<xref ref-type="bibr" rid="scirp.63977-ref9">9</xref>] leads us to conclude that rescaling the data introduces a large amount of stability into the algorithm. After the parameter estimates have been obtained, the MLE for the original observations are obtained by undoing the effect of scaling on the estimated values. In Appendix, we have given a very brief introduction to the Multi Parameter Newton Raphson method and have obtained the gradient and hessian matrices for the Weibull and the Burr XII distribution which are required for obtaining the maximum likelihood estimators for the parameters of the Weibull and the Burr XII distributions respectively.</p></sec><sec id="s2_2"><title>2.2. Classical Risk Model</title><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x28.png" xlink:type="simple"/></inline-formula> denote the surplus process of an insurer as</p><disp-formula id="scirp.63977-formula199"><label>(2.2.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x29.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x30.png" xlink:type="simple"/></inline-formula> is the initial surplus, c is the rate of premium income per unit time and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x31.png" xlink:type="simple"/></inline-formula> is the aggregate claim process and we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x32.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x33.png" xlink:type="simple"/></inline-formula> is a homogeneous Poisson process with parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x34.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x35.png" xlink:type="simple"/></inline-formula>denotes the amount of the ith claim and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x36.png" xlink:type="simple"/></inline-formula> is a sequence of iid random variables with</p><p>distribution function F such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x37.png" xlink:type="simple"/></inline-formula> and probability density function f. We denote <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x38.png" xlink:type="simple"/></inline-formula> by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x39.png" xlink:type="simple"/></inline-formula>. Also we have<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x40.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x41.png" xlink:type="simple"/></inline-formula> is the security loading factor.</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x42.png" xlink:type="simple"/></inline-formula> denote the time to ruin from initial surplus u so that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x43.png" xlink:type="simple"/></inline-formula> and define</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x44.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x45.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x46.png" xlink:type="simple"/></inline-formula>is known as the ultimate ruin probability</p><p>whereas <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x47.png" xlink:type="simple"/></inline-formula> is the finite time ruin probability. For a detailed discussion on the Classical Risk model and the probability of ruin refer to [<xref ref-type="bibr" rid="scirp.63977-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.63977-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.63977-ref11">11</xref>] -[<xref ref-type="bibr" rid="scirp.63977-ref13">13</xref>] .</p><p>However it needs to be noted that the Classical Risk Model involves many simplication criterions which might make it deviate from real life situations. For example, the classical risk model assumes that the intensity parameter λ is independent of time, independence between claim severity distribution and claim number distribution, premium is received continuously in time, surplus earns no interest and is neither subjected to tax, no effect of inflation etc. Despite such assumptions, Classical Risk model still constitute the basis of many models in insurance mathematics.</p><p>Probability of Ruin is a very important component of the operational risk theory. It reflects the volatility in the business and can serve as a useful tool in long range planning for the use of insurer’s funds. Ruin, in some sense, corresponds to the insolvency of the insurance company although; solvency/insolvency of an insurance company involves many other complicated considerations.</p></sec><sec id="s2_3"><title>2.3. A Stable Recursive Algorithm for the Evaluation of the Ultimate Ruin Probabilities</title><p>Probability of ruin can be obtained as the solution of an integro differential equation [<xref ref-type="bibr" rid="scirp.63977-ref14">14</xref>] . Stable Recursive Algorithm as the name suggests, is a recursive algorithm which is used to solve the convolution part of the integro differential equation for the probability of ultimate ruin and this in turn leads to the bounds of the ultimate ruin probability within a prescribed tolerance level.</p><p>According to [<xref ref-type="bibr" rid="scirp.63977-ref14">14</xref>] , for calculating the infinite time ruin probability numerically, one has to solve the following integral equation</p><disp-formula id="scirp.63977-formula200"><label>(2.3.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x48.png"  xlink:type="simple"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x49.png" xlink:type="simple"/></inline-formula></p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x50.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x51.png" xlink:type="simple"/></inline-formula> (2.3.2)</p><p>The usual approach is to apply a discretization technique to approximate the integral in (2.3.1) (see [<xref ref-type="bibr" rid="scirp.63977-ref15">15</xref>] -[<xref ref-type="bibr" rid="scirp.63977-ref17">17</xref>] ). A discretization technique is said to be effective if it does not lead to the propagation of errors thereby producing stable numerical results.</p><p>In Reference [<xref ref-type="bibr" rid="scirp.63977-ref18">18</xref>] , an efficient discretization technique for the convolution integral have been introduced and it is given in the form of a theorem stated therein (Section 2, Equation (5)).</p><p>Reference [<xref ref-type="bibr" rid="scirp.63977-ref19">19</xref>] have used another version of this theorem to obtain analytically upper and lower bounds of the infinite time ruin probabilities in case of constraints in the claim size distributions whereas [<xref ref-type="bibr" rid="scirp.63977-ref18">18</xref>] have used it to obtain a stable recursive algorithm for deducing the numerical bounds on the infinite time ruin probabilities and as mentioned there, a practical procedure for implementing the stable recursive algorithm is indicated as given below.</p><p>1) First carry out the sub division of the interval <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x52.png" xlink:type="simple"/></inline-formula> as given <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x53.png" xlink:type="simple"/></inline-formula> where</p><p>“n” the number of intervals is chosen to be sufficiently large.</p><p>2) For every <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x54.png" xlink:type="simple"/></inline-formula> let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x55.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x56.png" xlink:type="simple"/></inline-formula> then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x57.png" xlink:type="simple"/></inline-formula> for every <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x58.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x59.png" xlink:type="simple"/></inline-formula> for every <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x60.png" xlink:type="simple"/></inline-formula> since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x61.png" xlink:type="simple"/></inline-formula> is a decreasing function of y.</p><p>3) Then the upper bound and the lower bound to the probability of ruin is given by.</p><p>Upper bound is</p><disp-formula id="scirp.63977-formula201"><label>(2.3.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x62.png"  xlink:type="simple"/></disp-formula><p>and the lower bound is</p><disp-formula id="scirp.63977-formula202"><label>(2.3.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x63.png"  xlink:type="simple"/></disp-formula><p>with of course,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x64.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x65.png" xlink:type="simple"/></inline-formula></p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x66.png" xlink:type="simple"/></inline-formula>can be approximated by</p><disp-formula id="scirp.63977-formula203"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x67.png"  xlink:type="simple"/></disp-formula><p>An upper bound for the error in the estimation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x68.png" xlink:type="simple"/></inline-formula> is given by</p><disp-formula id="scirp.63977-formula204"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x69.png"  xlink:type="simple"/></disp-formula><p>The stability of this numerical procedure is justified from the fact that there is no cumulative effect of propa-</p><p>gation of error as it can be shown that if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x70.png" xlink:type="simple"/></inline-formula> are calculated with an error <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x71.png" xlink:type="simple"/></inline-formula> then the error <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x72.png" xlink:type="simple"/></inline-formula> on is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x73.png" xlink:type="simple"/></inline-formula> bounded by</p><disp-formula id="scirp.63977-formula205"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x74.png"  xlink:type="simple"/></disp-formula><p>For the derivation of the bounds and the full justification on the stability of this method, see [<xref ref-type="bibr" rid="scirp.63977-ref18">18</xref>] .</p>Computing the Function h(x) for the Burr XII Distribution<p>We have from (2.3.2),</p><disp-formula id="scirp.63977-formula206"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x75.png"  xlink:type="simple"/></disp-formula><p>For the Burr XII distribution given in (2.2.1), we have</p><disp-formula id="scirp.63977-formula207"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x76.png"  xlink:type="simple"/></disp-formula><p>Therefore,</p><disp-formula id="scirp.63977-formula208"><label>(2.3.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x77.png"  xlink:type="simple"/></disp-formula><p>Now, it can be shown that,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x78.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x79.png" xlink:type="simple"/></inline-formula></p><p>Using this in Equation (2.3.5), we have,</p><disp-formula id="scirp.63977-formula209"><label>(2.3.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x80.png"  xlink:type="simple"/></disp-formula><p>And this can be computed using the pbeta function of R Software.</p><p>Also, we have,</p><disp-formula id="scirp.63977-formula210"><label>(2.3.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x81.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_4"><title>2.4. Product Integration</title><p>Product integration which was traditionally used to numerically solve Volterra Integral equation of the second type (see [<xref ref-type="bibr" rid="scirp.63977-ref20">20</xref>] ) can also be used to compute the ultimate ruin probabilities, especially while dealing with heavy tailed claim severity distributions [<xref ref-type="bibr" rid="scirp.63977-ref21">21</xref>] .</p><p>As stated in Section (2.3), for calculating the infinite time ruin probability numerically, one has to solve the integral Equation (2.3.1) which can also be put in the form (of a Volterra integral equation of the second kind) as shown below</p><disp-formula id="scirp.63977-formula211"><label>, (2.4.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x82.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.63977-formula212"><label>(2.4.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x83.png"  xlink:type="simple"/></disp-formula><p>And <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x84.png" xlink:type="simple"/></inline-formula> (2.4.3)</p><p>Since, the early 1980’s, the numerical methods for the evaluation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x85.png" xlink:type="simple"/></inline-formula> were based on the discretization of the Risk process and then computing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x86.png" xlink:type="simple"/></inline-formula> recursively using some initial conditions. However, the recursive schemes usually suffer from the drawback of being slow and less accurate because the quadrature rule employed in the recursive schemes are usually of low order. The method of Product integration used to evaluate numerically the Probability of Ultimate Ruin as given in [<xref ref-type="bibr" rid="scirp.63977-ref21">21</xref>] and as justified there are fast and accurate and are more suitable for dealing with heavy tailed distributions such as Burr XII distribution. As such, in this paper, as a second method, we have used product integration to compute the probability of ultimate ruin as prescribed in [<xref ref-type="bibr" rid="scirp.63977-ref21">21</xref>] . For a detailed description of this method refer to [<xref ref-type="bibr" rid="scirp.63977-ref21">21</xref>] , although we have highlighted the execution procedure of this method.</p><p>The Volterra integral equation of the second kind is given by</p><disp-formula id="scirp.63977-formula213"><label>(2.4.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x87.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x88.png" xlink:type="simple"/></inline-formula> is the kernel (and is known) and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x89.png" xlink:type="simple"/></inline-formula> is the unknown function to be determined. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x90.png" xlink:type="simple"/></inline-formula> or one of it’s low order derivative is badly behaved in one of its arguments, Newton Cotes integration formulae may produce inaccurate results or converge slowly. To deal with such situations, when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x91.png" xlink:type="simple"/></inline-formula> is badly behaved, [<xref ref-type="bibr" rid="scirp.63977-ref20">20</xref>] and [<xref ref-type="bibr" rid="scirp.63977-ref22">22</xref>] recommend the use of Product Integration.</p><p>We first factorize <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x92.png" xlink:type="simple"/></inline-formula> as,</p><disp-formula id="scirp.63977-formula214"><label>(2.4.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x93.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x94.png" xlink:type="simple"/></inline-formula> is smooth and well behaved and can be accurately approximated by a suitable Langrange’s Interpolation Polynomial and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x95.png" xlink:type="simple"/></inline-formula> is badly behaved.</p><p>The interval <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x96.png" xlink:type="simple"/></inline-formula> is divided into n subintervals <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x97.png" xlink:type="simple"/></inline-formula> where</p><disp-formula id="scirp.63977-formula215"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x98.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63977-formula216"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x99.png"  xlink:type="simple"/></disp-formula><p>A quadrature rule of the form</p><disp-formula id="scirp.63977-formula217"><label>(2.4.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x100.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x101.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x102.png" xlink:type="simple"/></inline-formula> is used to approximate the integral appearing in (2.4.1). The weights <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x103.png" xlink:type="simple"/></inline-formula> are determined by ensuring that the rule of Equation (2.4.6) is exact when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x104.png" xlink:type="simple"/></inline-formula> is a polynomial in t of degree<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x105.png" xlink:type="simple"/></inline-formula>.</p><p>It is assumed that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x106.png" xlink:type="simple"/></inline-formula> moments <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x107.png" xlink:type="simple"/></inline-formula> exist for this is necessary for the application of the method of Product Integration and for each i, the moments <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x108.png" xlink:type="simple"/></inline-formula> can be calculated as</p><disp-formula id="scirp.63977-formula218"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x109.png"  xlink:type="simple"/></disp-formula><p>Assuming, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x110.png" xlink:type="simple"/></inline-formula>is linear in t i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x111.png" xlink:type="simple"/></inline-formula>, it can be shown that</p><disp-formula id="scirp.63977-formula219"><label>(2.4.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x112.png"  xlink:type="simple"/></disp-formula><p>And finally, the estimate of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x113.png" xlink:type="simple"/></inline-formula> is given by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x114.png" xlink:type="simple"/></inline-formula>, where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x115.png" xlink:type="simple"/></inline-formula> are obtained recursively by</p><disp-formula id="scirp.63977-formula220"><label>(2.4.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x116.png"  xlink:type="simple"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x117.png" xlink:type="simple"/></inline-formula> and the weights <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x118.png" xlink:type="simple"/></inline-formula> are given by</p><disp-formula id="scirp.63977-formula221"><label>(2.4.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x119.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x120.png" xlink:type="simple"/></inline-formula>for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x121.png" xlink:type="simple"/></inline-formula> (2.4.10)</p><disp-formula id="scirp.63977-formula222"><label>(2.4.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x122.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x123.png" xlink:type="simple"/></inline-formula> (2.4.12)</p><disp-formula id="scirp.63977-formula223"><label>(2.4.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x124.png"  xlink:type="simple"/></disp-formula><p>For accelerating the convergence, as mentioned in [<xref ref-type="bibr" rid="scirp.63977-ref21">21</xref>] we have used the Richardson’s Extrapolation technique (Also see [<xref ref-type="bibr" rid="scirp.63977-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.63977-ref24">24</xref>] ).</p><sec id="s2_4_1"><title>2.4.1. Product Integration for the Computation of the Ultimate Probability of Ruin for Burr Distributed Claims</title><p>We have used product integration to compute the Ultimate Probability of Ruin for Burr XII distributed claims taking an illustrative value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x125.png" xlink:type="simple"/></inline-formula> as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x126.png" xlink:type="simple"/></inline-formula></p><p>We have considered the Burr distribution which has been fitted to our data as well as a Burr distribution with a set of illustrative values for its parameters.</p><p>Here</p><disp-formula id="scirp.63977-formula224"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x127.png"  xlink:type="simple"/></disp-formula><p>which gives</p><disp-formula id="scirp.63977-formula225"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x128.png"  xlink:type="simple"/></disp-formula><p>As derived in (2.3.7),</p><disp-formula id="scirp.63977-formula226"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x129.png"  xlink:type="simple"/></disp-formula><p>From (2.4.3), we have</p><disp-formula id="scirp.63977-formula227"><label>(2.4.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x130.png"  xlink:type="simple"/></disp-formula><p>As for this distribution, all the moments <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x131.png" xlink:type="simple"/></inline-formula> exist for any finite s, Product Integration can be used.</p><p>Let</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x132.png" xlink:type="simple"/></inline-formula>and</p><disp-formula id="scirp.63977-formula228"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x133.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_4_2"><title>2.4.2. Computation of the Weights When the Claim Severity Distribution Is Burr XII</title><disp-formula id="scirp.63977-formula229"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x134.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x135.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.63977-formula230"><label>(2.4.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x136.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.63977-formula231"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x137.png"  xlink:type="simple"/></disp-formula><p>And <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x138.png" xlink:type="simple"/></inline-formula> (w is any upper limit of the integral, w &gt; 0,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x139.png" xlink:type="simple"/></inline-formula>) can be computed using the</p><p>pbeta function of the R software.</p><p>Similarly, from (2.4.13), we have</p><disp-formula id="scirp.63977-formula232"><label>(2.4.16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x140.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s2_5"><title>2.5. The Moment of the Time to Ruin</title><p>The distribution of the time to ruin is an interesting quantity related to the probability of ruin and plays a vital role in warning the management for possible adverse situations. There is no closed form expression developed for the distribution of the time to ruin except for the Exponential distribution and the Erlang group of distributions [<xref ref-type="bibr" rid="scirp.63977-ref25">25</xref>] and hence the computation of the moments except for the mentioned distributions has to be done numerically.</p><p>Initial ideas on this aspect can be found in [<xref ref-type="bibr" rid="scirp.63977-ref26">26</xref>] and working on those ideas, [<xref ref-type="bibr" rid="scirp.63977-ref25">25</xref>] presented methods from which explicit solutions for the moments of the time to ruin can be found recursively provided that an explicit solution exist for the ultimate ruin probability. Reference [<xref ref-type="bibr" rid="scirp.63977-ref27">27</xref>] simplified the results of [<xref ref-type="bibr" rid="scirp.63977-ref28">28</xref>] to make them mathematically tractable for numerical computation and have used them to calculate the approximate values for the moments of the time to ruin when explicit solutions for the probability of ultimate ruin do not exist. In their numerical computations, values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x141.png" xlink:type="simple"/></inline-formula> have been calculated from the stable algorithms described in [<xref ref-type="bibr" rid="scirp.63977-ref29">29</xref>] . (Also see [<xref ref-type="bibr" rid="scirp.63977-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.63977-ref31">31</xref>] .)</p><p>Reference [<xref ref-type="bibr" rid="scirp.63977-ref28">28</xref>] showed that the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x142.png" xlink:type="simple"/></inline-formula> moment of the distribution of the time to ruin T is given by</p><disp-formula id="scirp.63977-formula233"><label>(2.5.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x143.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x144.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x145.png" xlink:type="simple"/></inline-formula></p><p>Let L: the maximum of the aggregate loss process so that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x146.png" xlink:type="simple"/></inline-formula> see, [<xref ref-type="bibr" rid="scirp.63977-ref7">7</xref>] , formula (12.6.2).</p><p>In [<xref ref-type="bibr" rid="scirp.63977-ref14">14</xref>] , it had been shown that</p><disp-formula id="scirp.63977-formula234"><label>(2.5.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x147.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x148.png" xlink:type="simple"/></inline-formula> (2.5.3)</p><p>Formula (6.2.1) of [<xref ref-type="bibr" rid="scirp.63977-ref28">28</xref>] has been simplified in [<xref ref-type="bibr" rid="scirp.63977-ref27">27</xref>] as</p><disp-formula id="scirp.63977-formula235"><label>(2.5.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x149.png"  xlink:type="simple"/></disp-formula><p>Hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x150.png" xlink:type="simple"/></inline-formula>can be evaluated using numerical integration.</p><p>Similarly, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x151.png" xlink:type="simple"/></inline-formula>appearing in [<xref ref-type="bibr" rid="scirp.63977-ref28">28</xref>] has been simplified in [<xref ref-type="bibr" rid="scirp.63977-ref27">27</xref>] as</p><disp-formula id="scirp.63977-formula236"><label>(2.5.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/19-1490406x152.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s3"><title>3. Results and Discussion</title><p>Data: Our data is a set of 160,000 claim amounts spread over a period of 6 months i.e. from April, 2013 to September, 2013 obtained from Bajaj Allianz General Insurance company, India from its motor insurance portfolio covering all its branches in India. No adjustment was made for inflation for the time horizon is narrow. It needs to be mentioned that the data is utilized more for the illustration of the various methodologies rather than for the extraction of any concrete meaningful conclusion. Since the inter arrival time of claim was difficult to track, the intensity parameter was estimated on the basis of the number of claims arriving per day during the period.</p><p>Summary statistics of the data as shown in <xref ref-type="table" rid="table1">Table 1</xref> reveal the existence of high coefficient of skewness which suggests that a highly skewed right tailed distribution such as the Burr XII can be a probable candidate for modeling this data. The histogram of the data plotted in <xref ref-type="fig" rid="fig1">Figure 1</xref> and the empirical probability density function plotted in <xref ref-type="fig" rid="fig2">Figure 2</xref> show the same trend. These figures too indicate a high degree of skewness towards the right which in a way justifies the use of Burr XII distribution for modeling our data.</p><p>For finding the maximum likelihood estimators for the parameters of the Burr XII distribution, the use of the algorithm mentioned in [<xref ref-type="bibr" rid="scirp.63977-ref9">9</xref>] has been made. The log likelihood got maximized at the 30<sup>th</sup> iteration thereby giving the estimated values of the parameters as shown in <xref ref-type="table" rid="table2">Table 2</xref>. Initial assessment of the fit was done through some</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Summary statistics for the Insurance claim data</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Sample Size</th><th align="center" valign="middle" >Mean</th><th align="center" valign="middle" >Standard deviation</th><th align="center" valign="middle" >Min</th><th align="center" valign="middle" >25% Quantile</th><th align="center" valign="middle" >Median</th><th align="center" valign="middle" >75% Quantile</th><th align="center" valign="middle" >Max</th><th align="center" valign="middle" >Skewness</th><th align="center" valign="middle" >Kurtosis</th></tr></thead><tr><td align="center" valign="middle" >160,000</td><td align="center" valign="middle" >1.78834e+04</td><td align="center" valign="middle" >22,805.81</td><td align="center" valign="middle" >523</td><td align="center" valign="middle" >6043.00</td><td align="center" valign="middle" >10,583.00</td><td align="center" valign="middle" >19,374.25</td><td align="center" valign="middle" >188,209</td><td align="center" valign="middle" >3.576628</td><td align="center" valign="middle" >18.94972</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Parameter estimates for the Burr XII distribution obtained through the Watkin algorithm and the value of the EDF statistics along with their p-values indicated in parentheses</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Parameter</th><th align="center" valign="middle" >Estimates</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x153.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.670876e+05</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x154.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >8.6572840e−01</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x155.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.047651e+06</td></tr><tr><td align="center" valign="middle" >Anderson Darling statistics</td><td align="center" valign="middle" >5969.454 (0.002)</td></tr><tr><td align="center" valign="middle" >Cramer Von statistics</td><td align="center" valign="middle" >933.8827 (0.006)</td></tr></tbody></table></table-wrap><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Histogram of the observed claim data on motor insurance</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/19-1490406x156.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Estimate of the probability density function for the claim data on motor insurance</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/19-1490406x157.png"/></fig><p>graphical displays. <xref ref-type="fig" rid="fig3">Figure 3</xref> show the histogram for a set of data simulated from the Burr XII distribution with the values of the parameters as estimated using the algorithm. This histogram has some resemblance with the histogram for the observed data as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The QQ plot displayed in <xref ref-type="fig" rid="fig4">Figure 4</xref> indicate moderate deviation from the straight line passing through the origin which leads us to conclude that the fit is moderately good. The assessment of the fit was also done through the computation of two statistics namely the Anderson Darling statistics and the Cramer von statistics which are based on the empirical distribution function [<xref ref-type="bibr" rid="scirp.63977-ref32">32</xref>] . <xref ref-type="table" rid="table2">Table 2</xref> shows the values of the Anderson Darling and Cramer Von statistics for testing the goodness of fit along with their p-values which were obtained through the Monte-Carlo simulation based on 100 iterations [<xref ref-type="bibr" rid="scirp.63977-ref33">33</xref>] .</p><p>Hence, we have little evidence to believe that the Burr XII distribution adequately describes the claim data. However, in the subsequent sections, we have used this fitted Burr distribution along with another Burr XII distribution with a set of illustrative values for its parameters mainly with the objective of depicting the computational methodologies associated with the Burr XII distribution in obtaining some of the important Actuarial Quantities.</p><p><xref ref-type="table" rid="table3">Table 3</xref> and <xref ref-type="table" rid="table4">Table 4</xref> display the upper and lower bounds to the probability of ultimate ruin in case of Burr XII distributed claim severity using the stable Recursive algorithm. In <xref ref-type="table" rid="table3">Table 3</xref>, the claim severity is the fitted Burr XII distribution whereas the <xref ref-type="table" rid="table4">Table 4</xref> is constructed with an illustrative Burr XII distribution. The number of intervals for the stable recursive algorithms has been taken to be n = 160 and an illustrative value for the security loading factor has been taken as θ = 0.3. The upper bounds to the error of estimation have also been indicated in both the tables.</p><p>In both the tables, it has been observed that the probability of ultimate ruin is decreasing with an increase in the initial capital which is as expected. In case of our fitted Burr XII distribution, the difference between the upper</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Histogram for a data set simulated from for Burr XII distribution with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x159.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x160.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x161.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/19-1490406x158.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> QQ Plot between the empirical quantiles estimated from the motor insurance data and the theoretical quantiles for Burr XII distribution with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x163.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x164.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x165.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/19-1490406x162.png"/></fig><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Upper and lower bounds to the ultimate ruin probabilities for Burr distribution with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x166.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x167.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x168.png" xlink:type="simple"/></inline-formula> computed through the stable recursive algorithm</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Value of initial surplus u (Rs in Lakhs)</th><th align="center" valign="middle" >Lower bound to the probability of ruin</th><th align="center" valign="middle" >Upper bound to the probability of ruin</th><th align="center" valign="middle" >Probability of ultimate ruin</th><th align="center" valign="middle" >Upper bound to the error of estimation</th></tr></thead><tr><td align="center" valign="middle" >10 20 30 40 50 60 70 80 90 100 200 500 1000</td><td align="center" valign="middle" >1.142307e−01 1.625645e−02 2.154203e−03 2.655454e−04 3.038352e−05 3.226737e−05 3.176367e−07 2.895590e−08 2.442391e−09 1.904733e−10 1.916410e−23 1.378756e−81 1.854485e−175</td><td align="center" valign="middle" >1.226913e−01 2.152154e−02 4.033019e−03 8.060850e−04 1.715703e−04 3.882505e−05 9.325516e−06 2.373527e−06 6.390523e−07 1.816993e−07 8.640573e−12 2.823172e−17 7.133608e−19</td><td align="center" valign="middle" >1.184610e−01 1.888890e−02 3.093611e−03 5.357697e−04 1.009769e−04 2.102589e−05 4.821576e−06 1.201242e−06 3.207473e−07 9.094491e−08 4.320286e−12 1.411586e−17 3.566804e−19</td><td align="center" valign="middle" >8.460656e−03 5.265093e−03 1.878815e−03 5.406304e−04 1.411867e−04 3.559831e−05 9.007879e−06 2.344572e−06 6.366099e−07 1.815089e−07 8.640573e−12 2.823172e−17 7.133608e−19</td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Upper and lower bounds to the ultimate ruin probabilities for Burr distribution with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x169.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x170.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x171.png" xlink:type="simple"/></inline-formula> computed through the stable recursive algorithm</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Value of initial surplus u (Rs in Lakhs)</th><th align="center" valign="middle" >Lower bound to the probability of ruin</th><th align="center" valign="middle" >Upper bound to the probability of ruin</th><th align="center" valign="middle" >Probability of ultimate ruin</th><th align="center" valign="middle" >Upper bound to the error of estimation</th></tr></thead><tr><td align="center" valign="middle" >10 20 30 40 50 60 70 80 90 100 200 500 1000</td><td align="center" valign="middle" >7.692126e−01 7.691945e−01 7.691764e−01 7.691582e−01 7.691401e−01 7.691220e−01 7.691038e−01 7.690857e−01 7.690675e−01 7.690494e−01 7.688679e−01 7.683230e−01 7.674131e−01</td><td align="center" valign="middle" >7.692126e−01 7.691945e−01 7.691764e−01 7.691582e−01 7.691401e−01 7.691220e−01 7.691038e−01 7.690857e−01 7.690675e−01 7.690494e−01 7.688679e−01 7.683230e−01 7.674131e−01</td><td align="center" valign="middle" >7.692126e−01 7.691945e−01 7.691764e−01 7.691582e−01 7.691401e−01 7.691220e−01 7.691038e−01 7.690857e−01 7.690675e−01 7.690494e−01 7.688679e−01 7.683230e−01 7.674131e−01</td><td align="center" valign="middle" >8.904433e−12 3.561995e−11 8.015000e−11 1.424981e−10 2.226674e−10 3.206607e−10 4.364815e−10 5.701327e−10 7.216172e−10 8.909379e−10 3.565763e−09 2.231996e−08 8.947729e−08</td></tr></tbody></table></table-wrap><p>and the lower bounds to the probability of ultimate ruin seems to be decreasing in the absolute sense which has lead to the decline in the upper bound to the error of estimation. In case of the Burr XII distribution with a set of illustrative values for its parameters (<xref ref-type="table" rid="table4">Table 4</xref>), which we would choose to call the illustrative Burr XII in the subsequent sections, it is observed that there is no visible difference between the upper and lower bounds to the probability of ultimate ruin and hence the algorithm seems to be giving more accurate results in this case. The probable reasons for the equality of both the bounds can be that for this set of illustrative values of the parameters for the Burr XII distribution, the function h(x) is getting stabilized (approaching p<sub>1</sub>) more rapidly.</p><p><xref ref-type="table" rid="table5">Table 5</xref> shows the probability of ultimate ruin for the fitted Burr XII distribution obtained through the method of product integration whereas the <xref ref-type="table" rid="table6">Table 6</xref> displays the corresponding values for the illustrative Burr XII distribution. For accelerating the convergence, we have used the Richardson’s extrapolation technique as mentioned in [<xref ref-type="bibr" rid="scirp.63977-ref21">21</xref>] with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x172.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x173.png" xlink:type="simple"/></inline-formula> thereby giving<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x174.png" xlink:type="simple"/></inline-formula>. Both the tables reveal that the values of the ultimate ruin probabilities obtained through the method of product integration are fairly consistent with those obtained through the stable recursive algorithm. One notable trend observed in the computation of the probability</p><table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Ultimate ruin probabilities for Burr XII distribution with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x175.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x176.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x177.png" xlink:type="simple"/></inline-formula> obtained through product integration</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Value of the initial surplus u (Rs in Lakhs)</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x178.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >10 20 30 40 50 60 70 80 90 100 200 500 1000</td><td align="center" valign="middle" >1.184138e−01 1.873948e−02 2.966592e−03 4.693954e−04 7.427929e−05 1.175717e−05 1.867170e−06 3.020832e−07 5.284120e−08 1.176783e−08 4.626994e−11 1.456966e−14 2.089981e−17</td></tr></tbody></table></table-wrap><table-wrap id="table6" ><label><xref ref-type="table" rid="table6">Table 6</xref></label><caption><title> Ultimate ruin probabilities for Burr XII distribution with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x179.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x180.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x181.png" xlink:type="simple"/></inline-formula> obtained through product integration</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Value of the initial surplus u (Rs in Lakhs)</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x182.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >10 20 30 40 50 60 70 80 90 100 200 500 1000</td><td align="center" valign="middle" >0.7692126 0.7691945 0. 7691764 0.7691582 0.7691401 0.7691220 0.7691038 0.7690857 0.7690675 0.7690494 0.7688679 0.7683230 0.7674130</td></tr></tbody></table></table-wrap><p>of ultimate ruin through both the algorithms is that in case of our fitted Burr XII distribution with an increase in the value of the initial capital, the values for the probability of ultimate ruin are decreasing at a significantly high rate whereas this declined at a moderate rate in case of the illustrative Burr XII distribution.</p><p>In computing the moments of the time to ruin, in contrast to [<xref ref-type="bibr" rid="scirp.63977-ref27">27</xref>] , where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x183.png" xlink:type="simple"/></inline-formula> has been obtained through the stable algorithms described in [<xref ref-type="bibr" rid="scirp.63977-ref29">29</xref>] , <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x184.png" xlink:type="simple"/></inline-formula>in our case, has been computed through the stable recursive algorithm mentioned above. For the illustrative Burr distribution, we have also computed the second moment for a few values of the initial capital since the computing time for the evaluation of the second moment is significantly high. The high execution time is attributed to the fact that the computation of the second moment has taken</p><p>the first moment as an input. For numerical integration, we have used Simpson’s <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x185.png" xlink:type="simple"/></inline-formula> rule for numerical in-</p><p>tegration. All of the computations have been done using the R software [<xref ref-type="bibr" rid="scirp.63977-ref34">34</xref>] .</p><p>From <xref ref-type="table" rid="table7">Table 7</xref> showing the first moment <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x186.png" xlink:type="simple"/></inline-formula> (mean) of the time to ruin for the fitted Burr XII distribution as well as for the illustrative Burr XII, we make the following observations;</p><p>1) Mean (in years) of the time to ruin for the illustrative Burr XII i.e. Burr XII with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x187.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x188.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x189.png" xlink:type="simple"/></inline-formula> as indicated in column (3) for the various values of u is consistent with practical rationalism as the value goes on increasing with an increase in the initial capital for it is expected that induction of more capital should prolong the occurrence of ruin (if any).</p><p>2) Mean (in years) of the time to ruin for the fitted Burr XII distribution i.e. Burr XII with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x190.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x191.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x192.png" xlink:type="simple"/></inline-formula> is not consistent in the above sense (column (2)). Probable reasons for this inconsistency can be the occurrence of error in the evaluation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x193.png" xlink:type="simple"/></inline-formula> and also in numerical integration. As seen in Equation (2.5.4), numerator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x194.png" xlink:type="simple"/></inline-formula> of the expression for the mean of the time to ruin is the difference of two quantities and it is the latter part which is evaluated numerically and although not shown explicitly, both the parts were of very low order (of the order 1e−04) and were highly affected by the occurrence of numerical error leading to inconsistent results. One important point to be noted is that compared to the illustrative Burr XII distribution, the fitted Burr XII distribution has very low second order moment (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x195.png" xlink:type="simple"/></inline-formula>) and the second order moment of the underlying claim severity distribution is an important factor in determining the mean of the time to ruin, in fact the latter exists if and only if the second order moment of the claim severity distribution exists [<xref ref-type="bibr" rid="scirp.63977-ref28">28</xref>] . This low value of the second order moment for the fitted Burr XII distribution might have been the cause for this inconsistency in the pattern of the mean of the time to ruin.</p><p><xref ref-type="table" rid="table8">Table 8</xref> displays the second order moments of the time to Ruin for our illustrative Burr XII distribution for a few values of the initial capital.</p><p>In obtaining the mean of the time to ruin, an illustrative value of λ has been taken as λ = 32.78 and the same value is retained in obtaining the second moment of the time to ruin.</p></sec><sec id="s4"><title>4. Conclusions</title><p>Considering the fact that heavy tailed right skewed distribution like Burr XII arises frequently in case of risk modeling in general insurance, our work may be useful for insurance practitioners and experts from the financial industry. Our main objective was to compute the probability of ultimate ruin in case the claim severity is distributed as Burr XII distribution and this was implemented through the application of two numerical algorithms.</p><table-wrap id="table7" ><label><xref ref-type="table" rid="table7">Table 7</xref></label><caption><title> First moment (mean) of the time to ruin in case of Burr XII distributed claim severity distribution</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Value of the initial surplus u (in unit of Rs 1 lakh) (1)</th><th align="center" valign="middle" >Mean (in years) of the time to ruin for Burr XII with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x196.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x197.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x198.png" xlink:type="simple"/></inline-formula> (2)</th><th align="center" valign="middle" >Mean (in years) of the time to ruin for Burr XII with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x199.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x200.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x201.png" xlink:type="simple"/></inline-formula> (3)</th></tr></thead><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >16.066847</td><td align="center" valign="middle" >0.09771947</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >10.207575</td><td align="center" valign="middle" >0.09772715</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >8.3243480</td><td align="center" valign="middle" >0.09773484</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >7.8522660</td><td align="center" valign="middle" >0.09774253</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >7.7381620</td><td align="center" valign="middle" >0.09775021</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >7.7089970</td><td align="center" valign="middle" >0.09775790</td></tr><tr><td align="center" valign="middle" >70</td><td align="center" valign="middle" >7.7007810</td><td align="center" valign="middle" >0.09776559</td></tr><tr><td align="center" valign="middle" >80</td><td align="center" valign="middle" >7.6982140</td><td align="center" valign="middle" >0.09777328</td></tr><tr><td align="center" valign="middle" >90</td><td align="center" valign="middle" >7.6973290</td><td align="center" valign="middle" >0.09778098</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7.6969920</td><td align="center" valign="middle" >0.09778866</td></tr></tbody></table></table-wrap><table-wrap id="table8" ><label><xref ref-type="table" rid="table8">Table 8</xref></label><caption><title> Second moment of the time to ruin in case of Burr distributed claim severity distribution</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Value of the initial surplus u (in unit of Rs 1 lakh)</th><th align="center" valign="middle" >Second order moment of the time to ruin for Burr XII with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x202.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x203.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x204.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.09799326</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >0.09800281</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >0.09801237</td></tr></tbody></table></table-wrap><p>However, no effort has been made to judge which method gives the better estimate to the probability of ultimate ruin as there is no exact expression for it in case of Burr XII claim severity distribution. Although, there are instances in literature [<xref ref-type="bibr" rid="scirp.63977-ref12">12</xref>] , where the probability of ultimate ruin obtained through the Pollachez Khinchin formula has been used as a baseline method and the accuracies of other methods judged in terms of it, yet we have not gone to the extent of making this comparison between the two methods. The work reveals fairly good amount of consistencies in the approximate values of the probability of ultimate ruin obtained by the two numerical algorithms under consideration.</p><p>Also, in obtaining the moments of the time to ruin, it was found that in case of the illustrative Burr, the first moment (mean) of the time to ruin is increasing with an increase in the value of the initial surplus. This is to be expected in practice, because the induction of larger surpluses tends to prolong the time to ruin (if it ever happens). However in case of our fitted Burr XII distribution, there was deviation from this intuitive logic, implying that the mean of the time to ruin was found to be decreasing with an increase in initial surplus. The numerical error accumulated via the two numerical algorithms namely the numerical computation of the value of ultimate ruin probability through the stable recursive algorithm and then inserting it as an input into another numerical algorithm to compute the mean of the time to ruin might be the cause of this deviation. The executing time for computing the second moment was too high thereby limiting us just to the computation of this moment for a very few values of the initial surplus.</p><p>Extension of this work can be directed towards the computation of other actuarial quantities like aggregate claim models, number of claims until ruin etc in case of Burr XII claim severity. Further analysis is required to give more explicit error bounds to the solutions generated via the two numerical algorithms and the control of error in the numerical computation of the moments of the time to ruin.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The authors would like to thank the anonymous referees of the Journal for imparting valuable suggestions that helped us to improve the paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>JagritiDas,Dilip C.Nath, (2016) Burr Distribution as an Actuarial Risk Model and the Computation of Some of Its Actuarial Quantities Related to the Probability of Ruin. Journal of Mathematical Finance,06,213-231. doi: 10.4236/jmf.2016.61019</p></sec><sec id="s7"><title>Appendix 1</title>A.1. The Newton Raphson Method: The Multiparameter Situation<p>One of the most used methods for optimization in the Multi Parameter situation in Statistics is the Newton- Raphson method which is described briefly as given below:</p><p>Assume <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x205.png" xlink:type="simple"/></inline-formula> is a vector of p (say) unknown parameters and the log likelihood of the distri-</p><p>bution involving <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x206.png" xlink:type="simple"/></inline-formula> is given by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x207.png" xlink:type="simple"/></inline-formula>. Then the MLE for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x208.png" xlink:type="simple"/></inline-formula> are obtained by solving the equations</p><disp-formula id="scirp.63977-formula237"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x209.png"  xlink:type="simple"/></disp-formula><p>Let us now define what is known as the gradient matrix and the Hessian matrix given by.</p><p>The gradient matrix is given by</p><disp-formula id="scirp.63977-formula238"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x210.png"  xlink:type="simple"/></disp-formula><p>And the Hessian matrix is given by</p><disp-formula id="scirp.63977-formula239"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x211.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.63977-formula240"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x212.png"  xlink:type="simple"/></disp-formula><p>Then the iterative relationship for the multi parameter Newton Raphson method is given by</p><disp-formula id="scirp.63977-formula241"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x213.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x214.png" xlink:type="simple"/></inline-formula> is the estimated value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x215.png" xlink:type="simple"/></inline-formula> at the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x216.png" xlink:type="simple"/></inline-formula> iteration. The iteration is carried out until there is no significant difference between <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x216.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x217.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x216.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x217.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x218.png" xlink:type="simple"/></inline-formula></p>A.2. Multi Parameter Newton Raphson for Weibull Distribution<p>The log likelihood of the Weibull distribution is given by (2.1.5).</p><p>The Gradient matrix for Weibull is given by</p><disp-formula id="scirp.63977-formula242"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x219.png"  xlink:type="simple"/></disp-formula><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x220.png" xlink:type="simple"/></inline-formula>and</p><disp-formula id="scirp.63977-formula243"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x221.png"  xlink:type="simple"/></disp-formula><p>and the Hessian matrix is given by</p><disp-formula id="scirp.63977-formula244"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x222.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.63977-formula245"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x223.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63977-formula246"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x224.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63977-formula247"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x225.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63977-formula248"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x226.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.63977-formula249"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x227.png"  xlink:type="simple"/></disp-formula>A.3. Multiparameter Newton Raphson for Burr XII Distribution<p>The Log likelihood of Burr XII distribution is given by (2.1.6).</p><p>Its Gradient matrix is given by</p><disp-formula id="scirp.63977-formula250"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x228.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.63977-formula251"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x229.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63977-formula252"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x230.png"  xlink:type="simple"/></disp-formula><p>The hessian matrix is given by</p><disp-formula id="scirp.63977-formula253"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x231.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.63977-formula254"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x232.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63977-formula255"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x233.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63977-formula256"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x234.png"  xlink:type="simple"/></disp-formula></sec><sec id="s8"><title>Appendix 2</title>Tests Based on Empirical Distribution Function<p>A statistics measuring the difference between the Empirical <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x235.png" xlink:type="simple"/></inline-formula> and the fitted <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x235.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x236.png" xlink:type="simple"/></inline-formula> distribution function is called an EDF (empirical distribution function) Statistics and is based on the vertical distances between the distributions.</p><p>A class of measures of discrepancy given by the Cramer-Von Mises Family is</p><disp-formula id="scirp.63977-formula257"><graphic  xlink:href="http://html.scirp.org/file/19-1490406x237.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x238.png" xlink:type="simple"/></inline-formula> is a suitable function which gives weights to the squared differences <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x238.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x239.png" xlink:type="simple"/></inline-formula> When</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x240.png" xlink:type="simple"/></inline-formula>, we obtain the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x241.png" xlink:type="simple"/></inline-formula> statistic of Cramer Von Mises.</p><p>When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x242.png" xlink:type="simple"/></inline-formula>, we have the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/19-1490406x243.png" xlink:type="simple"/></inline-formula> statistic of Anderson and Darling. 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