<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2013.44093</article-id><article-id pub-id-type="publisher-id">AM-30706</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Condition for Successful Square Transformation in Time Series Modeling
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>.</surname><given-names>Ohakwe</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>O.</surname><given-names>Iwuoha</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>E.</surname><given-names>L. Otuonye</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Statistics, Faculty of Biological and Physical Sciences, 
Abia State University, Uturu, Nigeria</addr-line></aff><aff id="aff1"><addr-line>Department of Statistics, Faculty of Science, Federal University Otuoke, Yenagoa, Nigeria</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>ohakwej@fuotuoke.edu.ng(.O)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>16</day><month>04</month><year>2013</year></pub-date><volume>04</volume><issue>04</issue><fpage>680</fpage><lpage>687</lpage><history><date date-type="received"><day>January</day>	<month>7,</month>	<year>2013</year></date><date date-type="rev-recd"><day>March</day>	<month>4,</month>	<year>2013</year>	</date><date date-type="accepted"><day>March</day>	<month>11,</month>	<year>2013</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 study we establish the probability density function of the square transformed left-truncated N(1,σ<sup>2</sup>) error component of the multiplicative time series model and the functional expressions for its mean and variance. Furthermore the mean and variance of the square transformed left-truncated N(1,σ<sup>2</sup>) error component and those of the untransformed component were compared for the purpose of establishing the interval for σ where the properties of the two distributions are approximately the same in terms of equality of means and normality. From the results of the study, it was established that the two distributions are normally distributed and have means ≌1.0 correct to 1 dp in the interval 0 &lt; σ &lt; 0.027, hence a successful square transformation where necessary is achieved for values of σ such that 0 &lt; σ &lt; 0.027. 
 
</p></abstract><kwd-group><kwd>Error Component; Multiplicative Time Series Model; Square Transformation; Moments</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Consider a normally distributed random variable X with probability density function <img src="12-7401335\5caa6710-7afa-4182-8fa4-0044d5ab6b04.jpg" /> specified as</p><p><img src="12-7401335\600e152a-0ae5-481b-8aaf-7cc443ac09df.jpg" /><img src="12-7401335\389fe38f-1cd6-4d72-b0a6-319c64c9cd55.jpg" /> (1)</p><p>Often in practice, the random variable X which has a <img src="12-7401335\7fc1a10b-2dd7-4ca3-a929-b520d54c6014.jpg" /> distribution do not admit values less than or equal to zero. We therefore disregard or truncate all values of <img src="12-7401335\1855ae59-8f1c-4f42-8afa-6fcc2ddb87e3.jpg" /> to take care of the admissible region X &gt; 0. Now if the values of X below or equal to zero cannot be observed due to censoring or truncation, then the resulting distribution is a left-truncated normal distribution.</p><p>[<xref ref-type="bibr" rid="scirp.30706-ref1">1</xref>] obtained the probability density function of the left-truncated normal distribution as</p><disp-formula id="scirp.30706-formula28659"><label>(2)</label><graphic position="anchor" xlink:href="12-7401335\3ea5644f-8444-41c9-b87f-fb9f5293b3be.jpg"  xlink:type="simple"/></disp-formula><p>with mean <img src="12-7401335\fbff0e27-7deb-46e2-b55e-94bdd16a449b.jpg" /> and variance <img src="12-7401335\76e1503a-a8d8-4b9a-959f-dcfe41dc95e9.jpg" /> given by</p><disp-formula id="scirp.30706-formula28660"><label>(3)</label><graphic position="anchor" xlink:href="12-7401335\475269b3-cc0f-4227-bf71-1d6c8340adff.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.30706-formula28661"><label>(4)</label><graphic position="anchor" xlink:href="12-7401335\faefd18b-685a-4c27-a782-870585c4bc09.jpg"  xlink:type="simple"/></disp-formula><p>The study of the properties of normally distributed random variables when certain outcomes are constrained or restricted has been a rich and fertile one—with applications in regression analysis, inventory management and time series modeling to mention but a few.</p><p>A time series is a collection of observations made sequentially in time. Examples occur in a variety of fields, ranging from economics to engineering and methods of analyzing time series constitute an important area of statistics [<xref ref-type="bibr" rid="scirp.30706-ref2">2</xref>]. Time series analysis comprises methods that attempt to understand such time series, often either to understand the underlying context of the data points (Where did they come from? What generated them?), or to make forecasts. Time series forecasting is the use of a model to forecast or predict future events based on known past events.</p><p>Methods for time series analyses are often divided into three classes: descriptive methods, time domain methods and frequency domain methods. Frequency domain methods centre on spectral analysis and recently wavelet analysis [3,4] can be regarded as model-free analyses. Time domain methods [5,6] have a distribution-free subset consisting of the examination of the autocorrelation and cross-correlation analysis.</p><p>Descriptive methods [2,7] involve the separation of an observed time series into components representing trend (long term direction), the seasonal (systematic, calendar related movements), cyclical (long term oscillations or swings about the trend) and irregular (unsystematic, short term fluctuations) components. The descriptive method is known as time series decomposition. If short period of time are involved, the cyclical component is superimposed into the trend [<xref ref-type="bibr" rid="scirp.30706-ref2">2</xref>] and the observed time series <img src="12-7401335\e09f347f-ec69-4d79-b12c-7487b6fa69b2.jpg" /> can be decomposed into the trendcycle component<img src="12-7401335\2e94b529-27c3-49a7-9357-4592e0424088.jpg" />, seasonal component <img src="12-7401335\83000e3b-c9ae-4d32-9829-d31978314897.jpg" /> and the irregular/residual component<img src="12-7401335\44d6a63e-5b70-43ce-90e3-b87e969fca25.jpg" />.</p><p>The decomposition model of interest in this study is the multiplicative time series model given by</p><disp-formula id="scirp.30706-formula28662"><label>(5)</label><graphic position="anchor" xlink:href="12-7401335\efc8e45a-52e2-4cdb-bc98-38f1a4798e4f.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="12-7401335\ddf1fd65-a3fe-429a-87b8-e8e8cf117192.jpg" /> are independent, identically distributed normal errors with mean 1 and variance <img src="12-7401335\44573304-d0b4-40f4-a311-dfbd948e5753.jpg" />.</p><p>Data transformation is a mathematical operation that changes the measurement scale of a variable. Reasons for transformation include stabilizing variance, normalizing, reducing the effect of outliers, making a measurement scale more meaningful, and to linearize a relationship [<xref ref-type="bibr" rid="scirp.30706-ref8">8</xref>]. For further details on reasons for transformation, see [9- 11]. Many time series analyst assume normality and it is well known that variance stabilization implies normality of the series. The most popular and common data transformations are the power transformation namely the logarithm, square root, inverse, inverse square root, square and inverse square transformations. A statistical procedure for choice of appropriate data transformation can be obtained in [8,11]. It is important to note that, if we apply square transformation on model (5), we still obtain a multiplicative time series model given by</p><disp-formula id="scirp.30706-formula28663"><label>(5b)</label><graphic position="anchor" xlink:href="12-7401335\f7532d7c-c05e-4ee5-ac68-bfaebc4ecfdd.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="12-7401335\882950a1-a0f7-4dc7-8783-104b6b733279.jpg" /> and <img src="12-7401335\12fb15e9-acbe-4ff9-90cc-b109b6591650.jpg" /></p><p>Studies on the effects of transformation on the error component of the multiplicative time series model) are not new in the statistical literature. The overall aim of such studies is to establish the conditions for successful transformation. A successful transformation is achieved when the desirable properties of a data set remains unchanged after transformation. The basic properties or assumptions of interest for this study are: 1) Unit mean and 2) constant variance. In this end, [<xref ref-type="bibr" rid="scirp.30706-ref1">1</xref>] investigated the effect of logarithmic transformation on the error component <img src="12-7401335\166135af-0331-4b24-87df-75759a0f578a.jpg" /> of a multiplicative time series model where <img src="12-7401335\c035a751-d7a0-41aa-ac3a-73c1477c2b07.jpg" /> and discovered that the logarithm transform; <img src="12-7401335\532204ed-1b03-4732-b6a3-4c1157a05f99.jpg" />can be assumed to be normally distributed with mean, zero and the same variance, s<sup>2</sup> for s &lt; 0.1. Similarly [12,13] had studied the effects of inverse and square root transformations on the error component of the same model. [<xref ref-type="bibr" rid="scirp.30706-ref12">12</xref>] discovered that the inverse transform <img src="12-7401335\3032cc4e-8cae-4622-bd8a-4e9af0a4328d.jpg" /> can be assumed to be normally distributed with mean, one and the same variance provided<img src="12-7401335\00171a2c-a8e8-4ee8-93ed-afc9d9f93cb9.jpg" />. Similarly [<xref ref-type="bibr" rid="scirp.30706-ref13">13</xref>] discovered that the square root transform; <img src="12-7401335\d302e45b-a857-4122-95c7-e08f206b722b.jpg" />can be assumed to be normally distributed with unit mean and variance, 4σ<sup>2</sup> for<img src="12-7401335\64c66a18-76f5-4f48-b8f3-480f3e30f6d3.jpg" />, where σ<sup>2</sup> is the variance of the original error component before transformation. Furthermore, [<xref ref-type="bibr" rid="scirp.30706-ref14">14</xref>] has studied the implication of square root transformation on a two-parameter Gamma distributed error component of a multiplicative error model and discovered that the unit mean assumption is approximately maintained, but the variance of the transformed distributions is one-quarter of the original variance.</p><p>In this paper we study the implication of square transformation on the error component of the multiplicative time series model with a view to establish the interval for σ, for which the transformation is successful. The paper is organized into 6 sections. Section 1 contains the introduction. The probability density function, mean and variance of the square transformed left-truncated <img src="12-7401335\424946f3-597b-4181-a412-759d636013d3.jpg" /> error component are established in Section 2. Comparison of the square transformed and the untransformed distributions were compared in Section 3. Finally the summary and conclusion, references and appendix are respectively contained in Sections 4-6.</p></sec><sec id="s2"><title>2. Probability Distribution of the Square Transformed Error Component</title><p>Using the transformation,</p><disp-formula id="scirp.30706-formula28664"><label>(6)</label><graphic position="anchor" xlink:href="12-7401335\545dad1a-2ab0-48f3-9368-5a959edbe11d.jpg"  xlink:type="simple"/></disp-formula><p>in (2) and the admissible values of<img src="12-7401335\ea56abaa-9568-4769-89ea-9cf56f092e45.jpg" />, we would then find the probability density function (pdf) of<img src="12-7401335\1d693cc5-9b60-463a-a459-08e757e53a0b.jpg" />. From this point forward it is important to note from (5) and (5b), that symbolically <img src="12-7401335\1fcb4c65-123b-49aa-ac1f-18fab060823e.jpg" /> and<img src="12-7401335\0569fc06-95c2-43ba-a707-752dd6c734eb.jpg" />. Applying the transformation in (6) implies that</p><disp-formula id="scirp.30706-formula28665"><label>. (7)</label><graphic position="anchor" xlink:href="12-7401335\fc474066-9a1e-47a3-b482-3329919c256b.jpg"  xlink:type="simple"/></disp-formula><p>But, the pdf of y, <img src="12-7401335\ec6b1e3e-cbac-48f8-abd3-d6bc8990f5a2.jpg" />is given by</p><disp-formula id="scirp.30706-formula28666"><label>(8)</label><graphic position="anchor" xlink:href="12-7401335\5ec487be-bbb7-4aec-a132-ca30719ec71d.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="12-7401335\7f26ed97-0083-4bb5-a70b-c88cfbb53d94.jpg" /> is the absolute value of the Jacobian of the transformation [<xref ref-type="bibr" rid="scirp.30706-ref15">15</xref>]. Thus</p><p><img src="12-7401335\cdb6098f-32ca-477e-b692-ea42f9bbd210.jpg" /></p><p>hence</p><disp-formula id="scirp.30706-formula28667"><label>(9)</label><graphic position="anchor" xlink:href="12-7401335\a44381d8-505f-4a80-a961-88cc2ffbe7ba.jpg"  xlink:type="simple"/></disp-formula><p>The crucial question is now “is (9) a proper pdf?”. If it is to be a proper pdf, it must satisfy the condition;</p><p>1) <img src="12-7401335\9844fcdf-0c2a-4e57-b9b4-5cc809219f9a.jpg" /></p><p>hence we now proceed to show that the integral of (9) is equal to unity as follows:</p><disp-formula id="scirp.30706-formula28668"><label>(10)</label><graphic position="anchor" xlink:href="12-7401335\f0a82d2c-2c91-4f2a-b7d7-0f5b7f913624.jpg"  xlink:type="simple"/></disp-formula><p>Let</p><disp-formula id="scirp.30706-formula28669"><label>(11a)</label><graphic position="anchor" xlink:href="12-7401335\569ba676-16b9-48af-bfac-836ad4bf0ee0.jpg"  xlink:type="simple"/></disp-formula><p>hence</p><disp-formula id="scirp.30706-formula28670"><label>(11b)</label><graphic position="anchor" xlink:href="12-7401335\8999d17e-7bad-4a43-9b69-bb313fbd96bf.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.30706-formula28671"><label>(11c)</label><graphic position="anchor" xlink:href="12-7401335\c1f015f1-602c-4f67-8542-01e7792c9bf1.jpg"  xlink:type="simple"/></disp-formula><p>therefore, substituting the results in (11a) through (11c) into (10) yields</p><p><img src="12-7401335\ace0e16e-f598-42cf-9172-1c4782ea97dd.jpg" /></p><p>and this shows that (9) is a proper pdf.</p><sec id="s2_1"><title>2.1. Mean of the Square Transformed Distribution, <img src="12-7401335\195fb4a7-4aa7-462b-b66a-584a52f701e0.jpg" /></title><p>By definition</p><disp-formula id="scirp.30706-formula28672"><label>(12)</label><graphic position="anchor" xlink:href="12-7401335\9192db5d-9580-489b-8a2a-dcda54bcf8f8.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="12-7401335\52a85884-1fe0-48cc-80c2-fb5fbd4ac859.jpg" />.</p><p>Applying the substitution given in (11) into (12), we obtain</p><disp-formula id="scirp.30706-formula28673"><label>(13)</label><graphic position="anchor" xlink:href="12-7401335\b6e5a88e-44a0-4fc2-bc82-4395f7771717.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="12-7401335\4a5973d3-8895-491c-b772-d3a6036f47d3.jpg" /></p><p>and</p><p><img src="12-7401335\13b5486a-2ffe-4e2a-b746-56b58f782fef.jpg" /></p><p>If we let</p><disp-formula id="scirp.30706-formula28674"><label>(14)</label><graphic position="anchor" xlink:href="12-7401335\8db01274-c6ca-45c8-8bb7-c003fe06c1ba.jpg"  xlink:type="simple"/></disp-formula><p>in<img src="12-7401335\652a9d98-f046-44c0-a163-70be45935ab9.jpg" />, we obtain</p><disp-formula id="scirp.30706-formula28675"><label>(15a)</label><graphic position="anchor" xlink:href="12-7401335\82c9a2c4-9522-47b8-9cd4-2dcea16afe93.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.30706-formula28676"><label>(15b)</label><graphic position="anchor" xlink:href="12-7401335\9af370a0-09a5-4d3a-ba7d-fcab2fcb0585.jpg"  xlink:type="simple"/></disp-formula><p>hence</p><disp-formula id="scirp.30706-formula28677"><label>(16)</label><graphic position="anchor" xlink:href="12-7401335\139e3628-9454-4f8d-9669-53c0889e9ae7.jpg"  xlink:type="simple"/></disp-formula><p>By integration by parts the following results are obtained</p><disp-formula id="scirp.30706-formula28678"><label>(17a)</label><graphic position="anchor" xlink:href="12-7401335\cc4929d9-df8f-494e-bd72-826e1f91fda1.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.30706-formula28679"><label>(17b)</label><graphic position="anchor" xlink:href="12-7401335\239bf80e-ea0f-48d7-8ed6-1eba0866a7f8.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.30706-formula28680"><label>(17c)</label><graphic position="anchor" xlink:href="12-7401335\f889b15e-fb1a-4b6d-8ecf-8ca8b90c262c.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.30706-formula28681"><label>(17d)</label><graphic position="anchor" xlink:href="12-7401335\8e9ce300-d37e-45df-931d-044efcb64c77.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.30706-formula28682"><label>(17e)</label><graphic position="anchor" xlink:href="12-7401335\ac4aa6e1-a1f6-4dc8-8f27-60b8a716e216.jpg"  xlink:type="simple"/></disp-formula><p>hence</p><disp-formula id="scirp.30706-formula28683"><label>(18)</label><graphic position="anchor" xlink:href="12-7401335\cea1e0cc-9bfd-4bea-ba0b-1d6e5b1623eb.jpg"  xlink:type="simple"/></disp-formula><p>Furthermore, if we let</p><disp-formula id="scirp.30706-formula28684"><label>(19)</label><graphic position="anchor" xlink:href="12-7401335\e7fa8409-5a26-41ac-944c-d4dc69caa64c.jpg"  xlink:type="simple"/></disp-formula><p>in<img src="12-7401335\7e94e194-7811-4e5a-bac7-3e1b6812ed88.jpg" />, we obtain</p><disp-formula id="scirp.30706-formula28685"><label>(20a)</label><graphic position="anchor" xlink:href="12-7401335\aca4df81-7c1f-4b30-9dc3-7e32d42c3676.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.30706-formula28686"><label>(20b)</label><graphic position="anchor" xlink:href="12-7401335\0374873f-00d0-491c-add5-8f728a32d665.jpg"  xlink:type="simple"/></disp-formula><p>thus</p><disp-formula id="scirp.30706-formula28687"><label>(21)</label><graphic position="anchor" xlink:href="12-7401335\fd91d093-5457-4f8f-b3e9-0cabe92a8c5d.jpg"  xlink:type="simple"/></disp-formula><p>Substituting the results of (18), (21) and the value of k into (13), we obtain</p><disp-formula id="scirp.30706-formula28688"><label>(22)</label><graphic position="anchor" xlink:href="12-7401335\7c7f97ec-2d4f-4473-940b-5705d0c2597f.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s2_2"><title>2.2. Variance of the Square Transformed Distribution<img src="12-7401335\e2a6e36f-6fac-4201-be8f-343a02940c48.jpg" />, <img src="12-7401335\3fc3099a-b8c8-41e3-8204-2d15582a9fd7.jpg" /></title><p>By definition</p><p><img src="12-7401335\528774e5-2448-4c08-a4b6-745e688b9467.jpg" />but</p><disp-formula id="scirp.30706-formula28689"><label>(23)</label><graphic position="anchor" xlink:href="12-7401335\e0eac68f-bb48-469d-9940-c62b13d86c57.jpg"  xlink:type="simple"/></disp-formula><p>Applying the transformation given in (11) into (23), we have that</p><disp-formula id="scirp.30706-formula28690"><label>(24)</label><graphic position="anchor" xlink:href="12-7401335\5e5dfbf5-803c-42f0-9589-e87451f5a3d0.jpg"  xlink:type="simple"/></disp-formula><p>But</p><disp-formula id="scirp.30706-formula28691"><label>(25)</label><graphic position="anchor" xlink:href="12-7401335\5784ff13-b98e-4733-a247-af928717c4ee.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.30706-formula28692"><label>(26)</label><graphic position="anchor" xlink:href="12-7401335\9ee22bc9-7306-4bbe-a294-71fbe72e9625.jpg"  xlink:type="simple"/></disp-formula><p>Applying the substitution in (14) and its corresponding results in (15) into (26), we have that</p><disp-formula id="scirp.30706-formula28693"><label>(27)</label><graphic position="anchor" xlink:href="12-7401335\14d6d9d7-d658-4ed5-989e-4714a623cf91.jpg"  xlink:type="simple"/></disp-formula><p>Using the results given in (17), it can be shown after a series of algebraic manipulations, that (27) is equal to</p><disp-formula id="scirp.30706-formula28694"><label>(28)</label><graphic position="anchor" xlink:href="12-7401335\7717b7bb-2f00-418c-931d-615a1d9a77b9.jpg"  xlink:type="simple"/></disp-formula><p>hence</p><disp-formula id="scirp.30706-formula28695"><label>(29)</label><graphic position="anchor" xlink:href="12-7401335\e2dee5a6-9e36-412c-b8d1-7e2df1e7c087.jpg"  xlink:type="simple"/></disp-formula><p>Furthermore applying the substitution in (19) and its corresponding results in (20a) and (20b) into</p><p><img src="12-7401335\50b3d1c2-a3ff-4073-bc23-b95de4477c09.jpg" />, we obtain</p><disp-formula id="scirp.30706-formula28696"><label>(30)</label><graphic position="anchor" xlink:href="12-7401335\c39a3282-fe4d-49bd-8cef-aa6b2476535c.jpg"  xlink:type="simple"/></disp-formula><p>Substituting the results in (29) and (30) and the value of k into (24), we have that</p><disp-formula id="scirp.30706-formula28697"><label>(31)</label><graphic position="anchor" xlink:href="12-7401335\aea87c52-3cc8-4a92-81fd-8ea8af140461.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.30706-formula28698"><label>(32)</label><graphic position="anchor" xlink:href="12-7401335\644ac439-6fae-42e3-b4db-5e20ed9d0ddd.jpg"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s3"><title>3. Condition for Successful Square Transformation</title><p>In this section, the interval <img src="12-7401335\6a55c93a-9e88-423a-b0d3-23753254a51d.jpg" /> for which the desirable properties of the square transformed left-truncated <img src="12-7401335\3d5a080c-8af1-43da-9411-2d692e8f0914.jpg" /> distribution is approximately the same to that of the untransformed. The properties of interest are unit mean and normality and as a result we would first determine the interval <img src="12-7401335\a2ca25b6-5d82-4de0-9792-8603ca3133f8.jpg" /> for which the means of the transformed and the untransformed distributions of interest are both equal to unity (That is<img src="12-7401335\bb0e58cb-0ba3-4cd5-9603-7e8a2baacba8.jpg" />). Secondly we would determine the</p><p><xref ref-type="table" rid="table1">Table 1</xref>. An abridged table showing the computations of E(X), E(Y), Var(X) and Var(Y).</p><p><img src="12-7401335\c76f2871-cfe1-4b52-bd40-13d4d69350c8.jpg" /></p><p>value of <img src="12-7401335\f4e07b0f-3d51-478b-97c3-d34c2efbf6df.jpg" /> for which the curve shapes of the two probability distributions are bell-shaped and symmetrical about a unit mean.</p><p>For the purpose of this investigation, <img src="12-7401335\851a2e63-5c09-4ded-a5e1-7cd4bb6723e5.jpg" />, <img src="12-7401335\9a9de61f-796d-42ab-86a2-02b1a71c75ab.jpg" />and <img src="12-7401335\f38ee5bb-e143-4494-80ea-b30d13283d97.jpg" /> using Equations (3), (4), (22) and (32) are computed for values of<img src="12-7401335\c2f039f6-5192-44a0-9edd-4c5c77b617be.jpg" />,<img src="12-7401335\191314c5-d243-4596-8c03-04c5a90bf4ac.jpg" />. The results of the computations are given in <xref ref-type="table" rid="table1">Table 1</xref> (For want of space, <xref ref-type="table" rid="table1">Table 1</xref> is an abridged table). From <xref ref-type="table" rid="table1">Table 1</xref>, the following results are true;</p><p>1) <img src="12-7401335\1bf504c7-17e4-4ff3-94d0-c3a72b617ae6.jpg" />to one decimal place (dp) for the interval<img src="12-7401335\e726cc1d-7c62-4e8c-a5e3-d1d8becc1692.jpg" />.</p><p>2) <img src="12-7401335\629e4e91-cdc3-47fd-9e13-30455925c7df.jpg" />to two decimal places for the interval<img src="12-7401335\7a1f1ea0-0f62-4988-8174-4b963eeed09a.jpg" />. In order to determine the number of decimal place(s) to use, we investigate the normality of the pdf curves of the square transformed and that of the untransformed distributions at the points b = 0.027 and 0.280. The investigation of normality at the two points is based on the previous studies of [1,12,13] whereby, normality of a pdf curve at a point b implied normality at points<img src="12-7401335\f4d54cb8-89a0-45bf-858c-63aa62c2bc48.jpg" />. Bell-shaped curves and symmetry about a unit mean would be a measure of normality. The pdf curves of the two distributions of interest for b = 0.027, 0.280 are given in Figures 1 and 2.</p><p>From the Figures, it is obvious that there is a clear departure from normality for the pdf curves for b = 0.280, therefore the acceptable interval is<img src="12-7401335\62bb5b75-693f-4b1d-81e1-59b921b66894.jpg" />, since there is clear evidence of normality at b = 0.027. It is also clear from <xref ref-type="table" rid="table1">Table 1</xref> that<img src="12-7401335\88f11a07-1a16-44c3-8332-e06fb8dc0646.jpg" />. Furthermore it is also evidenced from <xref ref-type="table" rid="table1">Table 1</xref> that<img src="12-7401335\cb211afa-dfeb-48cd-915e-4f2a0276aa18.jpg" />, <img src="12-7401335\bac3773c-9e7e-4953-9aae-49bbb2ba780e.jpg" />, hence<img src="12-7401335\3b1132e4-936e-4a49-bfe8-1c0995287aa7.jpg" />, <img src="12-7401335\5375649b-be92-48aa-9193-96bdc077fa67.jpg" />correct to one decimal place (dp).</p></sec><sec id="s4"><title>4. Summary and Conclusion</title><p>In this study we have established the pdf of the square transformed left-truncated <img src="12-7401335\171015c4-620a-4544-aba7-45d3192f8cda.jpg" /> error component of the multiplicative time series model and the functional expressions for its mean and variance. Furthermore the mean and variance of the square transformed left-truncated <img src="12-7401335\ca09a16f-24b2-40a5-9d53-859fbb647d25.jpg" /> error component and those of the untransformed component were compared for the purpose of establishing the interval for σ where the properties of the two distributions are approximately the same in terms of equality of means and normality. From the results of the study, it was established that the two distributions are normally distributed and have means <img src="12-7401335\d0209c07-3157-4e03-a502-59b9a4aba3e5.jpg" /> correct to 1dp in the interval<img src="12-7401335\1b5b25dd-7016-49bf-956d-9ac1668cf7bf.jpg" />.</p><p>Based on the results of this study we therefore conclude that successful square transformation where necessary is achieved for values of σ such that<img src="12-7401335\33d54acc-2559-46ac-8173-adfe8979cf0f.jpg" />. However caution has to be exercised since square transformation leads to increased error variance.</p></sec><sec id="s5"><title>REFERENCES</title></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.30706-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">I. S. 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