<?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.2016.76042</article-id><article-id pub-id-type="publisher-id">AM-64927</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>
 
 
  A New Look at Generalized Means
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>arah</surname><given-names>M. Tooth</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>John</surname><given-names>A. Dobelman</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, Rice University, Houston, TX, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>dobelman@stat.rice.edu(JAD)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>24</day><month>03</month><year>2016</year></pub-date><volume>07</volume><issue>06</issue><fpage>468</fpage><lpage>472</lpage><history><date date-type="received"><day>28</day>	<month>December</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>21</month>	<year>March</year>	</date><date date-type="accepted"><day>24</day>	<month>March</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>
 
 
  Since antiquity, the relationships between 2-tuples and their Pythagorean means have been represented in geometric forms. In this paper, we extend the practice to generalized power means through new representations, and also to 3-tuples. These geometric forms give rise to new algebraic expressions for summary statistics of 2- and 3-tuples.
 
</p></abstract><kwd-group><kwd>Geometry</kwd><kwd> Power Means</kwd><kwd> Pythagorean Means</kwd><kwd> Outliers</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The study of means dates to antiquity. Pappus of Alexandria, who lived at the end of the third century AD, wrote on the relationships between the “three means” and gave reference to the work of previous geometers [<xref ref-type="bibr" rid="scirp.64927-ref1">1</xref>] . These three means: the arithmetic, geometric, and harmonic, along with a fourth, called the quadratic or root mean squared, represent the most commonly used means even today: the geometric mean finds use in finance and the study of populations, and also in conversion of aspect ratios for film processing; the harmonic mean is used in physics and economics for the treatment of rates and ratios; the quadratic mean is at the heart of ordinary least squares regression, which is used in many diverse fields; and it hardly needs to be said that the arithmetic mean has widespread use as the most used measure of central tendency.</p><p>Because of their practical importance, we consider these four means as special named cases of what [<xref ref-type="bibr" rid="scirp.64927-ref2">2</xref>] called “ordinary means” but which are more generally known as power means or generalized means. In this paper, we will modify the notation used by [<xref ref-type="bibr" rid="scirp.64927-ref2">2</xref>] and [<xref ref-type="bibr" rid="scirp.64927-ref3">3</xref>] and define the power means such that for the N-tuple x with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x6.png" xlink:type="simple"/></inline-formula> the p-th power mean of x is</p><disp-formula id="scirp.64927-formula272"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403027x7.png"  xlink:type="simple"/></disp-formula><p>We find this definition convenient to work with, although we note that the cases given for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x8.png" xlink:type="simple"/></inline-formula> represent the limits as the general case approaches those values, as shown by [<xref ref-type="bibr" rid="scirp.64927-ref2">2</xref>] . We also note that, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x9.png" xlink:type="simple"/></inline-formula>, the power mean is closely related to the p-norm, which differs only by a factor of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x10.png" xlink:type="simple"/></inline-formula> The special named cases of the power mean are: arithmetic mean,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x11.png" xlink:type="simple"/></inline-formula>; geometric mean,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x12.png" xlink:type="simple"/></inline-formula>; and the harmonic mean, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x13.png" xlink:type="simple"/></inline-formula>, which together make the Pythagorean means; and quadratic mean,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x14.png" xlink:type="simple"/></inline-formula>.</p><p>Power means may be regarded as statistics which give more weight to large values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x15.png" xlink:type="simple"/></inline-formula> when p is large and positive, and more weight to small values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x16.png" xlink:type="simple"/></inline-formula> when p is large and negative. Because of this property, they can be used comparably with percentiles, but with two important distinctions: the power mean function is continuous and differentiable; and unlike percentiles, power means are not robust to outliers. It is this second property which we consider the most important for its use in the treatment of datasets where outliers are of high importance.</p><p>In this paper, we explore geometric representations of power means as a method of investigating the properties of power means. We first describe past geometric representations of the means of 2-tuples, and then introduce our alternative method. Second, we describe how our method can be expanded to represent 3-tuples.</p></sec><sec id="s2"><title>2. Geometric Representations</title><p>Reference [<xref ref-type="bibr" rid="scirp.64927-ref1">1</xref>] describes how Pappus of Alexandria defines the arithmetic, geometric, and harmonic means according to a series of ratios in his Collection, Book III. Pappus then uses a geometric representation to demonstrate how, if two means are known, the third can always be found. The first geometric representation also comes from Pappus. From [<xref ref-type="bibr" rid="scirp.64927-ref1">1</xref>] :</p><p>“Pappus first gives a construction by which another geometer (αλλoςτις) [lit. the other] claimed to have solved this problem, but he does not seem to have understood it, and returns to the same problem later”.</p><p>It is not Pappus’s solution, but that of the unnamed geometer, with the addition of the quadratic mean by [<xref ref-type="bibr" rid="scirp.64927-ref4">4</xref>] , which has become the common form. It is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. This form is limited to represent the means of a 2-tuple, herein x. If we set AB = max x<sub>i</sub> and BC = min x<sub>i</sub>, then M<sub>1</sub> = FO, M<sub>0</sub> = BD, M<sub>−</sub><sub>1</sub> = DE and M<sub>2</sub> = BF.</p><p>We firstly propose a simple extension of the traditional representation in <xref ref-type="fig" rid="fig1">Figure 1</xref> which allows the representation of any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x17.png" xlink:type="simple"/></inline-formula>. We do this by removing the lines assigned to particular cases and introducing a single variable length which can equal any value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x18.png" xlink:type="simple"/></inline-formula>. This modified form is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. Here again, AB = max x<sub>i</sub> and BC = min x<sub>i</sub>, but in this new representation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x19.png" xlink:type="simple"/></inline-formula> where g(p) is a sigmoid function with domain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x20.png" xlink:type="simple"/></inline-formula> and range [min(x), max(x)].</p><p>Setting AB = a; BC = b, and solving <xref ref-type="fig" rid="fig2">Figure 2</xref> for M<sub>p</sub> gives:</p><disp-formula id="scirp.64927-formula273"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403027x21.png"  xlink:type="simple"/></disp-formula><p>While it may be debated whether Equation (2) is simpler to work with for general purposes than Equation (1), it has the clear advantage of being invertible. While we must solve Equation (1) for p numerically, solving Equation (2) for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x22.png" xlink:type="simple"/></inline-formula> gives the closed form:</p><disp-formula id="scirp.64927-formula274"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403027x23.png"  xlink:type="simple"/></disp-formula><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Traditional geometric representation of means</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7403027x24.png"/></fig><p>A sampling of values of p, M<sub>p</sub> and θ when a = 3 and b = 1 are shown in <xref ref-type="table" rid="table1">Table 1</xref>. For all a and b, there are three</p><p>fixed points in the mapping between M<sub>p</sub> and BD(θ) which are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x25.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x26.png" xlink:type="simple"/></inline-formula>.</p><p>To construct a geometric representation of the power means of a 3-tuple x as a natural extension of our N = 2 representation, we establish a number of desirable criteria. An N = 3 representation should have: a) an arrangement of line segments with lengths equal to each element x in the series; b) a curved path, on which any position can be described using only an angle<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x27.png" xlink:type="simple"/></inline-formula>; c) a line segment M with a length that is a function of θ, that is, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x28.png" xlink:type="simple"/></inline-formula>where f is monotone increasing; and d) a geometry such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x29.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x30.png" xlink:type="simple"/></inline-formula>. The resulting representation is shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><p>In <xref ref-type="fig" rid="fig3">Figure 3</xref>, the dimensions are assigned as follows: AB = max x, BC = min x, BD = M. While it will be intuitive to assign AC = med x and thus form a triangle of the elements of n, the simple example x = 1, 2, 5 illustrates why this is not possible. Because max x &gt; min x + med x, we cannot form a triangle with these three lengths.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Modified geometric representation of power means</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7403027x31.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Representation for power means of 3-tuples</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7403027x32.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Sample values for a = 3; b = 1</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="3"  >Example Values</th></tr></thead><tr><td align="center" valign="middle" >p</td><td align="center" valign="middle" >M<sub>p</sub></td><td align="center" valign="middle" >θ</td></tr><tr><td align="center" valign="middle" >−&#165;</td><td align="center" valign="middle" >1.000</td><td align="center" valign="middle" >0.000</td></tr><tr><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >1.500</td><td align="center" valign="middle" >1.318</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.732</td><td align="center" valign="middle" >π/2</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.000</td><td align="center" valign="middle" >1.823</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2.236</td><td align="center" valign="middle" >2.034</td></tr><tr><td align="center" valign="middle" >&#165;</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >π</td></tr></tbody></table></table-wrap><p>However, solving the system in <xref ref-type="fig" rid="fig3">Figure 3</xref> gives Equation (4), which shows that our power mean, as repre- sented by BD, is independent of AC (i.e. independent of med x).</p><disp-formula id="scirp.64927-formula275"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403027x33.png"  xlink:type="simple"/></disp-formula><p>A sampling of values of p, M<sub>p</sub> and θ when a = 1 and c = 3 is shown in <xref ref-type="table" rid="table2">Table 2</xref>. As with the 2-tuple case, there are three fixed points in the mapping between <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x34.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x35.png" xlink:type="simple"/></inline-formula> for all a and c. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x36.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x37.png" xlink:type="simple"/></inline-formula> are consistent with the 2-tuple case, but rather than a fixed point at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x38.png" xlink:type="simple"/></inline-formula>, the 3-tuple has a fixed</p><p>point at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x39.png" xlink:type="simple"/></inline-formula>.</p><p>One consequence of this relationship is that, if we set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x40.png" xlink:type="simple"/></inline-formula>, then our N = 3 system in <xref ref-type="fig" rid="fig3">Figure 3</xref> becomes <xref ref-type="fig" rid="fig4">Figure 4</xref>, which has a greater resemblance to the N = 2 representation from [<xref ref-type="bibr" rid="scirp.64927-ref4">4</xref>] , shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>, than our own N = 2 representation in <xref ref-type="fig" rid="fig2">Figure 2</xref>. Note that unlike previous N = 2 representations where the semi- circle has a diameter of max x + minx, these figures have semi-circles with diameter max x − minx.</p><disp-formula id="scirp.64927-formula276"><label>(5a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403027x41.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64927-formula277"><label>(5b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403027x42.png"  xlink:type="simple"/></disp-formula><p>Like the traditional form in Equation (1), Equation (4) is differentiable (Equation (5a)). It is also invertible, (Equation (5b)) a property which the traditional form lacks.</p><p>Finally, a comparison of <xref ref-type="fig" rid="fig2">Figure 2</xref> and <xref ref-type="fig" rid="fig3">Figure 3</xref> suggests characteristics of a similar representation of means for N-tuples for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x43.png" xlink:type="simple"/></inline-formula> In both figures, N segments are arranged in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x44.png" xlink:type="simple"/></inline-formula> dimensions, and the mean <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x45.png" xlink:type="simple"/></inline-formula> can be represented as the distance between one vertex and a semi-circle which lies in an orthogonal plane and connects two other vertices. As a result, the entire system can be represented as a semi-circle and a triangle which lie in two orthogonal planes, where the triangle is a projection from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x46.png" xlink:type="simple"/></inline-formula> to 2 dimensions. It follows,</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Sample values for a = 1; c = 3</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="3"  >Example Values</th></tr></thead><tr><td align="center" valign="middle" >p</td><td align="center" valign="middle" >M<sub>p</sub></td><td align="center" valign="middle" >θ</td></tr><tr><td align="center" valign="middle" >−&#165;</td><td align="center" valign="middle" >1.000</td><td align="center" valign="middle" >0.000</td></tr><tr><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >1.500</td><td align="center" valign="middle" >0.813</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.732</td><td align="center" valign="middle" >1.047</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.000</td><td align="center" valign="middle" >1.318</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2.236</td><td align="center" valign="middle" >π/2</td></tr><tr><td align="center" valign="middle" >&#165;</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >π</td></tr></tbody></table></table-wrap><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Projection of modified representation for 3-tuples</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7403027x47.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Modified representation for 2-tuples by Ercolano (1972)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7403027x48.png"/></fig><p>then, that provided both <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x49.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x50.png" xlink:type="simple"/></inline-formula> are unchanged, each additional <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403027x51.png" xlink:type="simple"/></inline-formula> will have progressively less influence on the overall shape of the function. This same behavior is seen in the algebraic form given in Equation (1), implying that the geometric representation has similar limiting properties to the algebraic.</p></sec><sec id="s3"><title>Acknowledgements</title><p>The authors would like to thank Rice University Professor Frank Jones, as well as William Longley and Reid Atcheson, for helpful discussions.</p></sec><sec id="s4"><title>Cite this paper</title><p>Sarah M.Tooth,John A.Dobelman, (2016) A New Look at Generalized Means. Applied Mathematics,07,468-472. doi: 10.4236/am.2016.76042</p></sec></body><back><ref-list><title>References</title><ref id="scirp.64927-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Heath, T. (1921) Greek Mathematics. Vol. 2, Oxford University Press, Cambridge.</mixed-citation></ref><ref id="scirp.64927-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Hardy, G., Littlewood, J. and Pólya, G. (1934) Inequalities. 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