Chaui-Berlinck recently published a paper in which he claims that the original West, Brown and Enquist (WBE) model for metabolic scaling(West et al., 1997) is fundamentally flawed (Chaui-Berlinck,2006). In particular, Chaui-Berlinck asserted that `the minimization procedure [of the original WBE model] is mathematically incorrect and ill-posed' and that the model `lacks self-consistency and correct statement'. These are strong accusations and should,therefore, be closely scrutinized. Unfortunately, Chaui-Berlinck's conclusions are incorrect because of rudimentary mathematical mistakes, and, even worse,these false conclusions are now being perpetuated in the literature. For example, Muller-Landau (Muller-Landau,2007), in a review for Faculty of 1000, recently drew attention to Chaui-Berlinck's paper by stating that `This article carefully dissects West, Brown and Enquist's(1997 )derivation of allometric scaling of metabolism. It illuminates important logical inconsistencies and mathematical problems with the argument'.

We note that none of the original authors nor the extended scaling community associated with the WBE model were asked to review Chaui-Berlinck's manuscript. As we show below, the entire basis of Chaui-Berlinck's paper stems from fundamental mathematical mistakes. In short, the conclusions of Chaui-Berlinck (and, subsequently, Muller-Landau) are completely incorrect. We conclude that Chaui-Berlinck's paper(Chaui-Berlinck, 2006) should be retracted.

The most egregious errors of Chaui-Berlinck are seen in his equation 5a. Specifically, Chaui-Berlinck makes two mistakes. He first mis-transcribes the original equation from WBE (West et al.,1997) and then makes a fundamental error in his calculus.

In his equation 5a, Chaui-Berlinck insists that he is carefully analyzing the mathematics of the WBE model. He obtains the quotient 0/0 in several equations and then concludes that, because of his analysis, the results of WBE are meaningless. However, Chaui-Berlinck's results of 0/0 only demonstrate both a misreading of the WBE paper and a basic mathematical error. The first mistake stems from Chaui-Berlinck incorrectly writing equation 9 from WBE as:
\[\ V_{\mathrm{b}}=\frac{V_{\mathrm{c}}}{({\beta}_{{>}}^{2}{\gamma})^{N}}\left\{\left(\frac{{\beta}_{{>}}}{{\beta}_{{<}}}\right)^{2\overline{k}}\left[\frac{1-(n{\beta}_{{>}}^{2}{\gamma})^{\overline{k}}}{1-(n{\beta}_{{>}}^{2}{\gamma})}\right]+\left[\frac{1-(n{\beta}_{{>}}^{2}{\gamma})^{N}}{1-(n{\beta}_{{>}}^{2}{\gamma})}\right]-\left[\frac{1-(n{\beta}_{{>}}^{2}{\gamma})^{\overline{k}}}{1-(n{\beta}_{{>}}^{2}{\gamma})}\right]\right\},\]
(1a)
but the correct expression, as given in WBE, is:
\[\ V_{\mathrm{b}}=\frac{V_{\mathrm{c}}}{({\beta}_{{>}}^{2}{\gamma})^{N}}\left\{\left(\frac{{\beta}_{{>}}}{{\beta}_{{<}}}\right)^{2\overline{k}}\left[\frac{1-(n{\beta}_{{<}}^{2}{\gamma})^{\overline{k}}}{1-(n{\beta}_{{<}}^{2}{\gamma})}\right]+\left[\frac{1-(n{\beta}_{{>}}^{2}{\gamma})^{N}}{1-(n{\beta}_{{>}}^{2}{\gamma})}\right]-\left[\frac{1-(n{\beta}_{{>}}^{2}{\gamma})^{\overline{k}}}{1-(n{\beta}_{{>}}^{2}{\gamma})}\right]\right\}.\]
(1b)

Notice that he swaps two β< for β> in the first term inside the parentheses. For the second mistake, he then goes on to evaluate equation 9 from WBE in a regime where the equation does not hold. Thus, Eqn 1b (above)contains expressions for geometric sums that hold only for values ofβ <, β>, n and γ such that

\(n{\beta}_{{<}}^{2}{\gamma}{\neq}1\)
and
\(n{\beta}_{{>}}^{2}{\gamma}{\neq}1\)
⁠. These expressions are not stated explicitly in WBE because they are apparent from basic rules for sums. The correct result can be obtained directly from equation 9 in the original WBE paper (or Eqn 1bhere) by taking the limitβ >→n–1/3, corresponding to
\(n{\beta}_{{>}}^{2}{\gamma}{\rightarrow}1\)
(becauseγ=n–1/3). Although it is true that the numerator and denominator of the second two terms inside the parentheses both go to zero in this limit, this does not equal the limit of the fraction. From introductory calculus, the limit of the fraction as a whole can be obtained using L'hospital's rule (for example, see http://mathworld.wolfram.com/LHospitalsRule.htmlor even a standard calculus class website such as http://www.math.tamu.edu/~fulling/coalweb/lhop.htm). Using L'hospital's rule simply amounts to taking the derivative of the numerator and denominator separately and only then taking the limit of the numerator and denominator in the resultant fraction.

As was done in the original WBE model, a finite geometric sum can be expressed as:
\[\ {{\sum}_{k=0}^{k=N-1}}x^{k}=\frac{1-x^{N}}{1-x},x{\neq}1.\]
(2)
The correct result for x=1 is found by taking the limit x→1 using L'hospital's rule:
\[\ {\mathrm{lim}_{x{\rightarrow}1}}\frac{1-x^{N}}{1-x}=\frac{{\mathrm{lim}_{x{\rightarrow}1}}\left[\frac{d}{dx}(1-x^{N})\right]}{{\mathrm{lim}_{x{\rightarrow}1}}\left[\frac{d}{dx}(1-x)\right]}=\frac{{\mathrm{lim}_{x{\rightarrow}1}}(-Nx^{N-1})}{{\mathrm{lim}_{x{\rightarrow}1}}(-1)}=N,\]
(3)
or going back to the original sum and recognizing that:
\[\ {{\sum}_{k=0}^{N-1}}1^{k}={{\sum}_{k=0}^{N-1}}1=N.\]
(4)

Unfortunately, Chaui-Berlinck's criticism did not incorporate these rules.

Now realizing that we can think of x as
\(n{\beta}_{{>}}^{2}{\gamma}\)
⁠, the sum from 0 to N–1 as over the N levels of the branching network, and using β<=n–1/2 along with our previous expressions for the other scaling ratios, equation 9 from WBE (i.e. Eqn 1b here) gives the correct result:
\[\ V_{\mathrm{b}}=V_{\mathrm{c}}n^{4N{/}3}\left[\frac{n^{-(N-\overline{k}){/}3}-n^{-N{/}3}}{1-n^{-1{/}3}}+n^{-N{/}3}(N-\overline{k})\right]=V_{\mathrm{c}}n^{4N{/}3}\left(\frac{n^{-\overline{N}{/}3}-n^{-N{/}3}}{1-n^{-1{/}3}}+n^{-N{/}3}{\ }\overline{N}\right).\]
(5)
Here, N̄=N–k̄,as originally reported in WBE. When NN̄and k̄1,with Vc and N̄constant, we have the original WBE prediction,
\(M{\infty}V_{\mathrm{b}}{\infty}n^{4N{/}3}{\infty}N_{\mathrm{c}}^{4{/}3}{\infty}B^{4{/}3}\)
⁠,where Nc is the number of capillaries in the organism and is directly related to metabolic rate. Consequently, the most critical claim made by Chaui-Berlinck is patently false.

Chaui-Berlinck makes several additional errors. In the equation at the top of the second column on p. 3050, Chaui-Berlinck's treatment of the geometric constants in the Lagrange multiplier calculation is not correct. Specifically,in the original WBE model, (4/3)π(l/2)3 is the service volume, and the geometric constant (4/3)π(1/2)3 is absorbed into the arbitrary constant λk, highlighting the fact that the distinction between a sphere and a cube does not matter for these arguments. Lastly, Chaui-Berlinck rehashes the mistaken ideas of Dodds et al.(Dodds et al., 2001) and Kozlowski and Konarzewski (Kozlowski and Konarzewski, 2004). Interestingly, Chaui-Berlinck perpetuates these flawed arguments once more but does not cite the responses, which does not present a balanced, fair or accurate view of the field(Brown et al., 2005; Savage et al., 2004). In summary, Chaui-Berlinck's paper is riddled with mathematical mistakes that reflect a misreading of the original WBE paper.

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