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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Sustain.</journal-id>
<journal-title>Frontiers in Sustainability</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Sustain.</abbrev-journal-title>
<issn pub-type="epub">2673-4524</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/frsus.2021.739395</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Sustainability</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>A Thermodynamic Measure of Sustainability</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name><surname>Sciubba</surname> <given-names>Enrico</given-names></name>
<xref ref-type="corresp" rid="c001"><sup>&#x0002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/86183/overview"/>
</contrib>
</contrib-group>
<aff><institution>Department of Industrial and Mechanical Engineering, University Niccol&#x000F2; Cusano</institution>, <addr-line>Rome</addr-line>, <country>Italy</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Eduardo Antonio Pina, University of Zaragoza, Spain</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Umberto Lucia, Politecnico di Torino, Italy; Daniel Florez-Orrego, University of S&#x000E3;o Paulo, Brazil</p></fn>
<corresp id="c001">&#x0002A;Correspondence: Enrico Sciubba <email>enrico.sciubba&#x00040;unicusano.it</email></corresp>
<fn fn-type="other" id="fn001"><p>This article was submitted to Quantitative Sustainability Assessment, a section of the journal Frontiers in Sustainability</p></fn></author-notes>
<pub-date pub-type="epub">
<day>17</day>
<month>12</month>
<year>2021</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>2</volume>
<elocation-id>739395</elocation-id>
<history>
<date date-type="received">
<day>10</day>
<month>07</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>22</day>
<month>11</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x000A9; 2021 Sciubba.</copyright-statement>
<copyright-year>2021</copyright-year>
<copyright-holder>Sciubba</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/"><p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p></license>
</permissions>
<abstract><p>A novel thermodynamic approach to the quantification of the &#x0201C;degree of sustainability&#x0201D; is proposed and discussed. The method includes a rigorous -and innovative- conversion procedure of the so-called externalities that leads to their expression in terms of the exergy of their equivalent primary resources consumption. Such a thermodynamic approach suggests a detailed re-evaluation of the concept of sustainability because it is well-known that the Second Law strictly negates the possibility for any open and evolving system to maintain itself in a &#x0201C;sustainable&#x0201D; state without availing itself of a continuous supply of low-entropy (i.e., high specific exergy) input. If a human society is modeled as an open system, its capacity to &#x0201C;grow sustainably&#x0201D; depends not only on how it uses non-renewable resources, but also on the rate at which it exploits the renewable ones. The necessary inclusion of different forms of energy- and material flows in such an analysis constitutes <italic>per se</italic> an argument in favor of a resource-based exergy metrics. While it is true that the thermodynamically oriented approach proposed here neglects all of the non-thermodynamic attributes of a &#x0201C;sustainable system&#x0201D; (in the Bruntland sense), it is also clear that it constitutes a rigorous basis on which different physically possible scenarios can be rigorously evaluated. Non-thermodynamic indicators can be still used at a &#x0201C;second level analysis&#x0201D; and maintain their usefulness to indicate which one of the &#x0201C;thermodynamically least unsustainable&#x0201D; scenarios is most convenient from an ethical or socio-economic perspective for the considered community or for the society as a whole. The proposed indicator is known as &#x0201C;Exergy Footprint,&#x0201D; and the advantages of its systematic application to the identification of &#x0201C;sustainable growth paths&#x0201D; is discussed in the Conclusions.</p></abstract>
<kwd-group>
<kwd>environmental indicators</kwd>
<kwd>non-equilibrium systems</kwd>
<kwd>exergy</kwd>
<kwd>exergy footprint</kwd>
<kwd>sustainability</kwd>
</kwd-group>
<counts>
<fig-count count="12"/>
<table-count count="1"/>
<equation-count count="18"/>
<ref-count count="61"/>
<page-count count="16"/>
<word-count count="10826"/>
</counts>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="s1">
<title>Introduction</title>
<p>After a debate that lasted for several decades, environmental considerations have been accepted as an essential -and necessary- part of the assessment of energy conversion systems. As of the time of this writing, several paradigms are in place to identify and quantify the &#x0201C;anthropogenic environmental impact,&#x0201D; and major Environmental and Governmental Agencies shelved the crude &#x0201C;emission level control&#x0201D; of the &#x02018;80s to prescribe comprehensive and detailed analysis of the local and global implications of the interactions of anthropic processes with the biosphere (both locally and at large). In fact, the large majority of current regulations go well-beyond the simple &#x0201C;assessment of ecological damage&#x0201D; (intended simply as &#x0201C;pollution&#x0201D;). Quantifiers of such interactions, known as Environmental Indicators (EI in the following), have been and are still being proposed and applied to different systems under diverse scenarios and with different system boundaries, to provide a sufficiently accurate and reliable decision support basis for decision makers. The definition of a reliable and robust EI invariably poses some problems: for example, some of the most popular EIs are based on a restricted number of control parameters (quality of air, public health, social equity, etc.) and offer only an incomplete measure of the actual environmental impact. Moreover, most of the &#x0201C;sustainability&#x0201D; indicators currently adopted in Biosciences are not rooted on rigorous thermodynamic principles and often require rather arbitrarily &#x0201C;weighed&#x0201D; decisions on the part of the analyst, which may generate confusion among final users. This paper proposes a method to <italic>construct thermodynamically correct Environmental Indicators to rigorously address the problem of &#x0201C;sustainability.&#x0201D;</italic> Approaching the problem under this point of view, it becomes immediately clear that if the problem is tackled starting from fundamental principles a thermodynamic redefinition of the very concept of sustainability is necessary. In fact, Second Law negates the possibility for any open and evolving system to maintain itself in a &#x0201C;sustainable&#x0201D; state without availing itself of a continuous supply of low-entropy input<xref ref-type="fn" rid="fn0001"><sup>1</sup></xref><sup>,</sup><xref ref-type="fn" rid="fn0002"><sup>2</sup></xref>. Therefore, the idea that &#x0201C;future generations&#x0201D; may successfully &#x0201C;satisfy their needs&#x0201D; (UN, <xref ref-type="bibr" rid="B55">1987</xref>) while their resource base is irreversibly dwindling leads either to the enforcement of an untenable Malthusian level of numerosity control of the population (Sciubba and Zullo, <xref ref-type="bibr" rid="B43">2009</xref>) or to an extreme degree of &#x0201C;prosperous de-growth&#x0201D; (Galor and Moav, <xref ref-type="bibr" rid="B20">2001</xref>; Mart&#x000ED;nez-Alier et al., <xref ref-type="bibr" rid="B26">2010</xref>) in all likeliness unacceptable by our progeny.</p>
</sec>
<sec id="s2">
<title>A Brief Critical Analysis of the Sustainability Concept</title>
<p>The modern concept of environmental sustainability dates back to the early &#x02018;60s, when the then dominating view of technology-driven economic growth came under the fire of a generic criticism based on the perception that the quality of the environment is closely linked to economic development. Admittedly, in those years academic support for the &#x0201C;steady state&#x0201D; economy (i.e., no-growth in mass throughput) was less than lukewarm, but as public opinion became strongly involved through the environmental movements, public Agencies and Governments became actively involved, promoting new procedures and issuing new regulations (Paul, <xref ref-type="bibr" rid="B32">1998</xref>). Perhaps the most important step was the 1968 foundation of the Club of Rome), followed by their publication in 1972 of <italic>Limits to Growth</italic> (Club of Rome, <xref ref-type="bibr" rid="B5">1972</xref>). Other initiatives followed, like the establishment of the Worldwatch Institute in 1975, and finally the term <italic>sustainable development</italic> was officially coined by the United Nations Commission (usually referred to as the &#x0201C;Brundtland Commission&#x0201D; from the name of its president, Gro Harlem Brundtland). It must be mentioned that the Commission report was largely based on the suggestions formulated in the previous decade by Daly and Costanza (Daly, <xref ref-type="bibr" rid="B10">1977</xref>, <xref ref-type="bibr" rid="B11">1996</xref>; Costanza et al., <xref ref-type="bibr" rid="B7">1997</xref>). This 1987 report (UN, <xref ref-type="bibr" rid="B55">1987</xref>), <italic>Our Common Future</italic>, contains the (too) often cited definition of &#x0201C;<italic>development which meets the needs of the present without compromising the ability of future generations to meet their own needs</italic>.&#x0201D;</p>
<p>In the last four decades, the concept was further developed, leading to the <italic>United Nations Millennium Declaration</italic> (September 2000 in Rio de Janeiro) which set out eight &#x0201C;United Nations Millennium Development Goals&#x0201D; (MDG), to be achieved by 2015, committing world leaders to fight poverty, hunger, disease, illiteracy, environmental degradation, and discrimination against minorities (UNEP, <xref ref-type="bibr" rid="B56">1992</xref>). Following suit, the World Summit on Sustainable Development (WSSD, Johannesburg 2002), produced the first political declaration (the &#x0201C;<italic>Johannesburg Plan of Implementation</italic>&#x0201D;) setting global goals and targets on the access to water, sanitation and modern energy services, on increasing energy primary-to-final use efficiency, on the exploitation of renewable energy sources, on establishing and maintaining sustainable fisheries and forests, on the enforcement of a more accurate monitoring and management of chemicals, etc. The rationale here was that of decoupling environmental degradation from economic growth and of achieving &#x0201C;sustainable patterns of consumption and production.&#x0201D;</p>
<p>The term &#x0201C;eco-development&#x0201D; had already appeared in the UN Environment Program review in 1978, and its most important feature was the recommendation that environmental and developmental ideas be considered concurrently. The paradigmatic definition of the Brundtland Commission elaborated on this approach, but it contains two rather obscure points that need clarification:</p>
<list list-type="alpha-lower">
<list-item><p>The concept of &#x0201C;needs,&#x0201D; explicitly defined as the essential needs of individuals, including obviously their socio-economical rights to which overriding priority should be given. Specifically, who is in charge of dictating a standard for these &#x0201C;needs&#x0201D; that is acceptable to the entire world population? And if &#x0201C;local needs&#x0201D; are regarded as necessary, what supernational Authority is responsible for their definition and updates? Most importantly perhaps, how are the &#x0201C;needs of the future generations&#x0201D; established, especially in view of the fact that &#x0201C;sustainable development&#x0201D; planning requires long-term decisions and policies?</p></list-item>
<list-item><p>The idea that a simple change in consumers&#x00027; attitude and an improvement in final energy uses, coupled with the expected technological advances, may suffice to allow for a perennial &#x0201C;sustainable development,&#x0201D; be it with or without a growth in the global material throughput (Daly, <xref ref-type="bibr" rid="B11">1996</xref>).</p></list-item>
</list>
<p>Some scholars correctly observed already in those early years that it is exactly the vagueness of the definition of the &#x0201C;sustainability issue&#x0201D; that made it palatable to decision makers worldwide: it is becoming painfully clear today that &#x0201C;sustainable development&#x0201D; is something everyone can agree to, but that merely positing it does not provide exact guidelines on how to achieve its goal.</p>
<p>Today, we are faced with practical questions such as: What does sustainable development really mean for different communities? How can we put the concept into practice? How do we know if we are transitioning toward a sustainable world? These questions demand for a <italic>measure</italic> of environmental effects, both at local and global scales, and this is why current &#x0201C;environmental policy declarations&#x0201D; make explicit use of both local and global EI, defined (EPA, <xref ref-type="bibr" rid="B17">2008</xref>) as &#x0201C;&#x02026; <italic>a numerical value that helps provide insight into the state of the environment or human health&#x02026; Indicators are developed based on quantitative measurements or statistics of environmental condition that are tracked over time.&#x0201D;</italic> They &#x0201C;<italic>&#x02026; can be developed and used at a wide variety of geographic scales, from local to regional to national levels. By monitoring the environment using indicators</italic> &#x02026; (it is possible to)&#x02026; <italic>share meaningful environmental information with the public, and ensure that high-quality environmental decisions are made</italic>.&#x0201D;</p>
<p>Another problem is that the concept of sustainability is not only rather fuzzy (a criticism that nowadays most schools of thought agree upon) but that it also lacks a rigorous scientific foundation. The very idea that a chemically and thermally non-homogeneous open system of constant total mass may be &#x0201C;sustainable&#x0201D; <italic>tout court</italic> (i.e., that it may remain in its -possibly dynamic- state &#x0201C;forever&#x0201D;) conflicts with the dictates of the Second Law of Thermodynamics (Valero-Delgado et al., <xref ref-type="bibr" rid="B58">2011</xref>). The main problem is that the currently accepted definitions of &#x0201C;sustainability,&#x0201D; &#x0201C;sustainable development,&#x0201D; &#x0201C;sustainable growth&#x0201D; etc. make implicit or explicit recourse not only to exact physical sciences (to which thermodynamic laws apply), but also to several different branches of knowledge like Economics, Social- and Political Sciences, all of which are intrinsically ruled by &#x0201C;value judgements&#x0201D; that cannot be easily falsified in Popper&#x00027;s sense<xref ref-type="fn" rid="fn0003"><sup>3</sup></xref> and are in general axiomatically posited<xref ref-type="fn" rid="fn0004"><sup>4</sup></xref>. The (too!) often published &#x0201C;three pillars paradigm&#x0201D; (<xref ref-type="fig" rid="F1">Figure 1</xref>) that asserts that the concept of Sustainability stems out of three fields of knowledge, Social, Economics and Environmental sciences, has been strongly criticized by influential scholars (Thompson, <xref ref-type="bibr" rid="B53">2017</xref>; Purvis et al., <xref ref-type="bibr" rid="B34">2019</xref>), but the idea is so catchy and so heavily publicized, even on public media, that most decision makers take it for granted.</p>
<fig id="F1" position="float">
<label>Figure 1</label>
<caption><p>The concept of the three pillars of sustainability (adapted from Purvis et al., <xref ref-type="bibr" rid="B34">2019</xref>).</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="frsus-02-739395-g0001.tif"/>
</fig>
<p>The approach taken in this paper is in this perspective frankly &#x0201C;reductionist.&#x0201D; When addressing problems like &#x0201C;rational resource exploitation&#x0201D; and &#x0201C;equitable resource distribution&#x0201D;, the role of Physical Sciences is predominant: it is rather clear that a resource-based metrics is less biased and must be favored, and as a consequence the non-thermodynamic attributes of a &#x0201C;sustainable system&#x0201D; ought to be considered at a &#x0201C;second step level&#x0201D; and be carefully reformulated in terms of their primary resource equivalent. In such a perspective, it is clear that the inherent fuzziness of the current concept of &#x0201C;sustainability&#x0201D; is due to the neglect of the fundamental separation between its thermodynamic<xref ref-type="fn" rid="fn0005"><sup>5</sup></xref> basis, that should be the plinth on which possible &#x0201C;pillars&#x0201D; rest, and the socio-economic one, which falls under the domain of different branches of science, is measured by different quantifiers, and ought to consider the thermodynamic part as a preliminary filter and therefore abandon the glorious idea that a &#x0201C;sustainable state&#x0201D; be attainable by a simple resource re-allocation.</p>
</sec>
<sec id="s3">
<title>Environmental Indicators as Quantifiers of the State of a System</title>
<p>Environmental Indicators are used at different aggregation levels in industrial, economic, social and environmental studies as a synthetic and significant way of &#x0201C;representing reality.&#x0201D; They facilitate a concise and reproducible information exchange between specialists (scientists at large) and non-specialists (herein collectively denominated &#x0201C;decision makers,&#x0201D; including in this term the public opinion). As their name implies, EIs ought to be quantifiers that measure the &#x0201C;environmental quality&#x0201D; at a local, industrial, regional, national or global scale and should be used to directly compare -and possibly integrate- different scenarios. A careful examination of most of these quantifiers reveals that the problems lie in the link between the formulation of each indicator and the phenomenological model it subsumes. Combining some widely accepted inventories of necessary properties of an Environmental Indicator (Jackson et al., <xref ref-type="bibr" rid="B22">2000</xref>; Dale and Beyeler, <xref ref-type="bibr" rid="B9">2001</xref>; Gong and Wall, <xref ref-type="bibr" rid="B21">2001</xref>; Sciubba, <xref ref-type="bibr" rid="B41">2013</xref>) we can extract a useful conceptual list of evaluation criteria:</p>
<list list-type="alpha-lower">
<list-item><p>The EI must be expressed by a -possibly simple- numeric or alphanumeric expression, i.e., they are scalars;</p></list-item>
<list-item><p>The application of an EI to real world situation must produce results that can be unambiguously ranked (from &#x0201C;bad&#x0201D; to &#x0201C;good,&#x0201D; from &#x0201C;desirable&#x0201D; to &#x0201C;damaging,&#x0201D; etc.);</p></list-item>
<list-item><p>The EI must be calculated on the basis of easily measurable, intrinsic properties of both the system to which it refers (= the potential &#x0201C;polluter source&#x0201D;) and of the (local or global) environment (the &#x0201C;polluted system&#x0201D;);</p></list-item>
<list-item><p>The EI must be properly normalized, so that it may be used to compare different communities under different environmental conditions, or different scenarios and time series for the same community;</p></list-item>
<list-item><p>The EI must be calculated on the basis of an unambiguous, reproducible method under a well-defined set of fundamental assumptions;</p></list-item>
<list-item><p>The EI must be anticipatory, i.e., it can be used both for diagnostic and prognostic purposes;</p></list-item>
<list-item><p>The EI must comply with the accepted laws of physics.</p></list-item>
</list>
<p>In conclusion, the EI that we shall consider in the present study are a) purely thermodynamic; b) resource- based; c) global; d) exergy-based. The fourth attribute is justified by the well-established record of results brought about by the adoption of exergy in the analysis of technical systems (Dewulf et al., <xref ref-type="bibr" rid="B13">2008</xref>).</p>
</sec>
<sec id="s4">
<title>Thermodynamics and Resource Exploitment</title>
<p>The fundamental idea of this study is that a human society can be modeled as a (non-equilibrium) thermodynamic system (Demirel, <xref ref-type="bibr" rid="B12">2007</xref>; Lebon and Jou, <xref ref-type="bibr" rid="B24">2008</xref>). In such an approach, the relationship between a &#x0201C;human society&#x0201D; (<bold><italic>H</italic></bold>) and &#x0201C;the environment&#x0201D; (<bold><italic>O</italic></bold>) can be quantified using thermodynamic tools. Since diverse forms of energy flows are involved that cannot be simply algebraically combined (like for instance chemical energy, thermal energy, human labor etc.), and since it is rather obvious that &#x0201C;thermodynamic sustainability&#x0201D; is inextricably linked to the Second Law, we shall use without further justification exergy<xref ref-type="fn" rid="fn0006"><sup>6</sup></xref> as the sole quantifier for our considerations (for a definition of exergy and a detailed discussion on its properties and applications, see for example (Fratzscher, <xref ref-type="bibr" rid="B19">1965</xref>; Moran, <xref ref-type="bibr" rid="B30">1982</xref>; Szargut et al., <xref ref-type="bibr" rid="B50">1988</xref>; Wall, <xref ref-type="bibr" rid="B59">1997</xref>; Wall and Gong, <xref ref-type="bibr" rid="B60">2001</xref>).</p>
<sec>
<title>Methodological Remarks</title>
<p>In an Exergy Analysis every material flow is attributed an equivalent &#x0201C;exergetic power&#x0201D; by multiplying its mass flowrate by the specific exergy of the material, <italic>&#x00116;</italic><sub><italic>j</italic></sub> &#x0003D; <italic>&#x01E41;</italic><sub><italic>j</italic></sub><italic>e</italic><sub><italic>j</italic></sub><xref ref-type="fn" rid="fn0007"><sup>7</sup></xref>. Immaterial flows carry different exergy amounts depending on both the energy intensity and &#x0201C;type&#x0201D;: mechanical and electrical power carries an exergy equal to its value in W, while thermal energy flows possess an exergy content equal to their enthalpic value multiplied by a temperature-dependent factor lower than unity that reflects their inability to be completely converted into work (Moran, <xref ref-type="bibr" rid="B30">1982</xref>). Chemical energy flows (e.g., &#x0201C;heat of reaction&#x0201D;) are attributed an exergy equivalent by means of an exergy evaluation of the reactants and products and of the reference environment in which the reaction takes place (Kotas, <xref ref-type="bibr" rid="B23">1985</xref>).</p>
<sec>
<title>The Exergy Budget</title>
<p>Exergy is not conserved: in every real process a portion of the incoming exergy is destroyed (annihilated) by irreversibility: in fact, this destruction is proportional to the irreversible entropy generation rate (Gouy-Stodola theorem). In the following of this paper, the exergy destruction rate is denoted by <italic>&#x00116;</italic><sub>&#x003B4;</sub>, and it is important to notice that it denotes in fact a fictitious &#x0201C;flow&#x0201D; that does not correspond to any physical quantity: it is but a mere arithmetical expedient to represent the difference between the input and the output so that we may formally talk of an exergy &#x0201C;balance.&#x0201D; In time-dependent processes it is often useful to include an &#x0201C;accumulation&#x0201D; term whose rate <italic>&#x00116;</italic><sub><italic>acc</italic></sub> quantifies the amount of incoming exergy converted into internal &#x0201C;production processes&#x0201D; within the system: in a transparent reference to biological systems, this corresponds to a &#x0201C;growth&#x0201D; and its integral in time is sometimes denoted as &#x0201C;embodied exergy&#x0201D; (Yantovsky, <xref ref-type="bibr" rid="B61">1994</xref>). In the following, since one of the systems (&#x0201C;<bold>H</bold>&#x0201D;) is an anthropic community (an industrial sector, a city, a Country&#x02026;), this accumulation measures for example the cumulative exergy of the goods generated internally (industrial commodities, construction, consumer goods, etc.). Natural flows (wind, irradiation, water flows&#x02026;) also carry an exergy that can be calculated according to the same rules. Referring specifically to the &#x0201C;system society,&#x0201D; its input <italic>&#x00116;</italic><sub><italic>in</italic></sub> consists in material flows of ores, fossil fuels and goods from the environment and immaterial flows like solar radiation, hydraulic- and wind power, geothermal power etc., also originated in the environment. This inflow of (low-entropy) material and immaterial streams feeds the conversion processes inside of the system that convert the primary resources into final exergy use (consumer goods, buildings, transportation systems, food, etc.). Since all real processes are irreversible, at each step in the conversion chain a portion of the incoming exergy flow is destroyed (annihilated), and the cumulative destruction is denoted by <italic>&#x00116;</italic><sub>&#x003B4;,<italic>H</italic></sub>. The system also discharges &#x0201C;waste&#x0201D; into the environment, both as scrapped material byproducts and process effluents or as -generally low temperature- thermal flows: their cumulative amount is referred to as <italic>&#x00116;</italic><sub><italic>W,H</italic></sub>.</p>
</sec>
<sec>
<title>Time Evolution of H</title>
<p>Every anthropic system, be it a single production line, a city or an entire Country, is an open system evolving in time. But in Classical Thermodynamics the concept of &#x0201C;time&#x0201D; has no meaning and all processes are analyzed assuming they may be described by a succession of (quasi-) equilibrium states. When we deal with natural systems time becomes though an essential parameter, because the time history of the systems object of the study is really what we are after. Therefore, the &#x0201C;balances&#x0201D; described in this context must be intended as integral values over the entire duration of the time window of interest. In the model we are proposing, this time dependence is enforced in two ways:</p>
<list list-type="alpha-lower">
<list-item><p>The &#x0201C;internal dynamics&#x0201D; of each system are allowed to vary in a prescribed fashion: for instance, with reference to <xref ref-type="fig" rid="F2">Figure 2</xref>, the growth rate of <bold>H</bold>, measured by <italic>&#x00116;</italic><sub><italic>acc</italic></sub> is specified as a <italic>f(t)</italic> (this is equivalent to defining a scenario to which the model is applied), and the history of system evolution becomes a function of this quantity and of the boundary conditions;</p></list-item>
<list-item><p>The boundary conditions (<italic>&#x00116;</italic><sub><italic>in</italic></sub>, <italic>&#x00116;</italic><sub><italic>out</italic></sub>, <italic>&#x00116;</italic><sub><italic>b</italic></sub>) may display in turn a time dependence (daily, seasonal, or otherwise) that is not considered as an internal variable of the system and depends on the considered scenario as well.</p></list-item>
</list>
<fig id="F2" position="float">
<label>Figure 2</label>
<caption><p>The constant-mass open-system model with accumulation in H (growth).</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="frsus-02-739395-g0002.tif"/>
</fig>
<p>In general, the evolution of a system on a realistically extended time scale can be described by an initial and usually rather flat transient, possibly followed by a more or less steady condition of a variable duration and by a final &#x0201C;approach of the limit&#x0201D; for very long times. Since our goal here is to describe a possible model, in the following we shall assume that all systems under examination have a characteristic evolution time much longer than the window of observation, so that they may be treated as &#x0201C;dynamically steady&#x0201D; systems.</p>
</sec>
</sec>
<sec>
<title>Closed Systems</title>
<p>Consider first (<xref ref-type="fig" rid="F3">Figure 3</xref>) a &#x0201C;closed system model&#x0201D;: let us identify the environment <bold>O</bold> with &#x0201C;planet Earth,&#x0201D; modeled as a closed system (no external material or immaterial inputs), and consider a scenario in which a society <bold><italic>H</italic></bold> grows in time by mining some materials and tapping some energy out of <bold><italic>O</italic></bold>&#x00027;s reservoirs: it is convenient to combine both fluxes into a single exergy flux <italic>&#x00116;</italic><sub><italic>in,H,NR</italic></sub>. Under the additional (albeit irrelevant for our present purposes) assumption of a Hubbertian extraction rate, the interaction of the two systems will evolve as shown in <xref ref-type="fig" rid="F4">Figure 4</xref>: the resources are gradually exhausted, and when the&#x0222B;&#x00116;<sub><italic>in,H,NR</italic></sub> <italic>dt</italic> reaches the value <italic>E</italic><sub>0,<italic>NR</italic></sub>, the cumulative exergy content of the NR reservoirs in <bold>O</bold> at the initial time, their extraction necessarily ceases<xref ref-type="fn" rid="fn0008"><sup>8</sup></xref> and the accumulation rate becomes necessarily negative and inevitably leads to the disappearance of <bold>H</bold>. Clearly, a non-sustainable scenario.</p>
<fig id="F3" position="float">
<label>Figure 3</label>
<caption><p>The closed-system model of society/environment interaction.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="frsus-02-739395-g0003.tif"/>
</fig>
<fig id="F4" position="float">
<label>Figure 4</label>
<caption><p>Qualitative representation of the time evolution of <italic>&#x00116;</italic><sub><italic>in,H</italic></sub> in a closed system.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="frsus-02-739395-g0004.tif"/>
</fig>
<p>Notice that if we wish to account for space exploration and consider that humanity may be able to exploit resources from an additional series of reservoirs located in other celestial bodies, the above conclusions would still stand, provided one expands the original control volume to include the extra-terrestrial &#x0201C;sources&#x0201D; <bold>S</bold> (<xref ref-type="fig" rid="F5">Figure 5</xref>). The timescale of the scenario obviously changes, but the long-term outlook remains the same: any &#x0201C;closed system&#x0201D; model negates the possibility of a &#x0201C;thermodynamic sustainable state&#x0201D; for the composite system, unless a steady state is reached for which the accumulation is driven solely by the renewable portion of the incoming resources (Sciubba and Zullo, <xref ref-type="bibr" rid="B43">2009</xref>):</p>
<disp-formula id="E1"><label>(1)</label><mml:math id="M1"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>R</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>W</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>Equation 1 is valid under the assumption that the waste flow is sufficiently &#x0201C;small&#x0201D; to be completely buffered by <bold>O</bold>&#x00027;s internal dynamics.</p>
<fig id="F5" position="float">
<label>Figure 5</label>
<caption><p>The closed-system model extended to out-of-earth reservoirs.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="frsus-02-739395-g0005.tif"/>
</fig>
</sec>
<sec>
<title>Open Systems</title>
<p>Things change though if we adopt an open system model (<xref ref-type="fig" rid="F6">Figure 6</xref>) in which <bold><italic>O</italic></bold> receives a steady influx of (material or immaterial) exergy from outer space and <bold>H</bold> feeds both on renewable (<italic>&#x00116;</italic><sub><italic>in,H,R</italic></sub>) and non-renewable (<italic>&#x00116;</italic><sub><italic>in,H,NR</italic></sub>) resources.</p>
<fig id="F6" position="float">
<label>Figure 6</label>
<caption><p>The open-system model with accumulation in H (growth).</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="frsus-02-739395-g0006.tif"/>
</fig>
<p>The exergy budget for the environment <bold>O</bold> reads:</p>
<disp-formula id="E2"><label>(2a)</label><mml:math id="M2"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>B</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>W</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>R</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>N</mml:mi><mml:mi>R</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>O</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>It is convenient to introduce a subsystem <bold>B</bold> of <bold>O</bold> [that we shall call &#x0201C;immediate surroundings&#x0201D; following (Moran and Sciubba, <xref ref-type="bibr" rid="B29">1994</xref>)] that represents the portion of the environment that directly participates to the biodegradation. Its exergy budget is:</p>
<disp-formula id="E3"><label>(2b)</label><mml:math id="M3"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>B</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>B</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>The societal system <bold>H</bold> has also its own exergy budget:</p>
<disp-formula id="E4"><label>(2c)</label><mml:math id="M4"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>And considering the entire combined system <bold>O&#x0222A;B&#x0222A;H</bold>, the global system budget is:</p>
<disp-formula id="E5"><label>(2d)</label><mml:math id="M5"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>O</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>B</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>Equation (2a) indicates that in the long run the fossil reservoirs will be exhausted, and therefore in the context of our search for a possible sustainable state the term <italic>&#x00116;</italic><sub><italic>in,H,NR</italic></sub> ought to be set equal to zero. Equation (2b) reveals that the flux <italic>&#x00116;</italic><sub><italic>B</italic></sub> denotes a primary exergy &#x0201C;investment&#x0201D; by <bold>O</bold> to biodegrade (by buffering, dilution and diffusion processes) the effluents of <bold>H</bold> that cumulatively carry an exergy <italic>&#x00116;</italic><sub><italic>w,H</italic></sub>. Equation (2c) expresses the &#x0201C;steadiness&#x0201D; condition requiring that the algebraic sum of the exergy flow rates absorbed, discharged, accumulated and destroyed by <bold>H</bold> be equal to zero at all times, and finally equation (2d) constitutes the global balance for the combined system (<bold><italic>O</italic></bold> &#x0222A;<bold><italic>H</italic></bold>). Notice that subsystem <bold>B</bold> has been introduced here for computational convenience only: &#x0201C;immediate surroundings&#x0201D; is an intentionally vague denomination for that part of the biosphere providing the exergy flux for bio-recovery through a complex cascade of processes fed by a portion of the instantaneous difference <italic>&#x00116;</italic><sub><italic>in</italic></sub> &#x02212; <italic>&#x00116;</italic><sub><italic>out</italic></sub>. In our model <italic>&#x00116;</italic><sub><italic>B</italic></sub> is a &#x0201C;service&#x0201D; provided by <bold>O</bold> to <bold>H</bold> (through <bold>B</bold>) to compensate for the changes that would otherwise be induced by the wastes <italic>&#x00116;</italic><sub><italic>w,H</italic></sub> on the steady-state of <bold>O</bold>: biodegradation is an &#x0201C;output&#x0201D; from <bold>O</bold> and takes up (uses and consumes) some of the external input <italic>&#x00116;</italic><sub><italic>in</italic></sub>. Not surprisingly, this equation suggests that there is a &#x0201C;primary resource cost&#x0201D; to the growth of a society <bold>H</bold>.</p>
<p>In spite of the oversimplification embedded in such a model, the meaning of equations (2) is clear: a steady state is indeed possible for <bold>H</bold>, as long as a sufficient external exergy flow rate is available to the system. This result is in line with previous statements by several Authors (Boltzmann, <xref ref-type="bibr" rid="B2">1905</xref>; Lotka, <xref ref-type="bibr" rid="B25">1922</xref>; Schroedinger, <xref ref-type="bibr" rid="B36">1945</xref>; Boulding, <xref ref-type="bibr" rid="B4">1966</xref>) about life being &#x0201C;<italic>maintained by the planet exergy destruction rate</italic>&#x0201D;<xref ref-type="fn" rid="fn0009"><sup>9</sup></xref>. The above example demonstrates the meaning of &#x0201C;thermodynamic sustainability.&#x0201D; Clearly, such a simplified model falls short of accounting for even the most basic phenomenological evolutionary scenarios (accumulation of exergy in the form of fossil fuels and ores, different timescales for the biodegradation action of the biosphere, etc.).</p>
</sec>
</sec>
<sec id="s5">
<title>Thermodynamically Sustainable Growth</title>
<p>Natural systems are complex and display non-linear behavior, because they possess self-regulating mechanisms consisting of a vast web of positive and negative feedback processes that operate concurrently and regulate the carrying, regeneration, and assimilation capacity of the respective systems. As stated above, they are clearly in &#x0201C;non-equilibrium&#x0201D;: how does the model of <xref ref-type="fig" rid="F6">Figure 6</xref> account for situations in which, for instance, <bold>H</bold> &#x0201C;grows&#x0201D; in time and is non-homogeneous? To get some insight, let us analyze the term <italic>&#x00116;</italic><sub><italic>acc,H</italic></sub> that represents the &#x0201C;accumulation&#x0201D; (embodiment) of exergy into <bold>H</bold>: such an embodiment can be material (mined ores are transformed into artifacts) and/or immaterial (exergy extracted from <bold>O</bold> is consumed in the production processes). Equation (2c) can be recast in a more useful form by assuming that the biodegradation effort be proportional to the exergy of the waste flows:</p>
<disp-formula id="E6"><label>(3)</label><mml:math id="M6"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>&#x003BA;</mml:mi><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>Where <bold>&#x003BA;</bold> is a (not necessarily linear and not necessarily scalar) function of the respective thermodynamic states of <bold>O</bold> and <bold>H</bold> and of the intensity of the waste flux: &#x003BA; &#x0003D; &#x003BA;(<italic>O, H</italic>, <italic>&#x00116;</italic><sub><italic>w,H</italic></sub>). The balance for <bold>H</bold> becomes:</p>
<disp-formula id="E7"><label>(4)</label><mml:math id="M7"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>We can now use equations (2d) and (4) to assess the thermodynamic sustainability of the open system (<bold>O</bold>&#x0222A;<bold>H</bold>):</p>
<list list-type="alpha-lower">
<list-item><p>A positive rate of accumulation in <bold>H</bold> is possible if the exergy input rate <italic>&#x00116;</italic><sub><italic>in,H</italic></sub> from <bold>O</bold> to <bold>H</bold> is larger than the sum of the waste exergy discharged by <bold>H</bold> and of the internal rate of exergy destruction in the society;</p></list-item>
<list-item><p>For a constant <italic>&#x00116;</italic><sub><italic>in</italic></sub> &#x02212; <italic>&#x00116;</italic><sub><italic>out</italic></sub>, the admissible rate of accumulation decreases if the biodegradation service requested of <bold>B</bold> increases (larger amount of wastes or higher <bold>&#x003BA;</bold>, i.e., more polluting wastes);</p></list-item>
<list-item><p>A higher conversion efficiency on the part of <bold>H</bold> is reflected both in a lower <italic>&#x00116;</italic><sub><italic>w,H</italic></sub> and a lower <italic>&#x00116;</italic><sub>&#x003B4;,<italic>H</italic></sub> and results in an increase of the admissible accumulation rate;</p></list-item>
<list-item><p>Combining equation (4) and (2d), we obtain:
<disp-formula id="E8"><label>(5)</label><mml:math id="M8"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>1</mml:mn><mml:mo>&#x0002B;</mml:mo><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>O</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p></list-item>
</list>
<p>Which sets a global upper limit to the accumulation rate <italic>&#x00116;</italic><sub><italic>acc,H</italic></sub>.</p>
<p>Equations (2&#x02013;5) constitute therefore a suitable, and global, model for assessing the thermodynamic sustainability of a human society interacting with an open environment. On this basis it is therefore possible to derive proper global indicators. In fact, the above representation of the composite system <bold>O&#x0222A;H</bold> enables analysts to apply standard concepts of exergy analysis and define at least three different forms of &#x0201C;efficiency&#x0201D;: an &#x0201C;intrinsic efficiency&#x0201D; of <bold>H</bold> is obtained by calculating the ratio of the <italic>useful product</italic> of all processes enacted within its boundaries (<italic>&#x00116;</italic><sub><italic>acc,H</italic></sub>) to the total incoming exergy flux <italic>&#x00116;</italic><sub><italic>in,H</italic></sub>:</p>
<disp-formula id="E9"><label>(6)</label><mml:math id="M9"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x003B7;</mml:mi></mml:mrow><mml:mrow><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>The reciprocal of &#x003B7;<sub><italic>H</italic></sub>, <italic>c</italic><sub><italic>H</italic></sub>, is an &#x0201C;exergy cost&#x0201D; that measures the exergy rate [in W] needed to produce a unitary rate of accumulation:</p>
<disp-formula id="E10"><label>(7)</label><mml:math id="M10"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mi>H</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>Both &#x003B7;<sub><italic>H</italic></sub> and <italic>c</italic><sub><italic>H</italic></sub> are indeed <bold><italic>global</italic></bold> EIs, because they neither explicitly nor implicitly relate to &#x0201C;local&#x0201D; conditions around or within <bold>H</bold>, and <bold><italic>relevant</italic></bold>, because they provide a quantitative measure of how well <bold>H</bold> &#x0201C;exploits&#x0201D; the exergy flow it extracts from <bold>O</bold>. <bold>H</bold> could increase its accumulation capability either by reducing <italic>&#x00116;</italic><sub>&#x003B4;,<italic>H</italic></sub> (i.e., improving its internal processes to reduce irreversibility and therefore increase &#x003B7;<sub><italic>H</italic></sub> and decrease <italic>c</italic><sub><italic>H</italic></sub>) or/and <italic>&#x00116;</italic><sub><italic>w,H</italic></sub> (i.e., reducing the unused portion of <italic>&#x00116;</italic><sub><italic>in,H</italic></sub> released as waste into <bold>O</bold> by implementing more effective recycling procedures).</p>
<p>If we consider that the environment uses a portion of its exergy supply (<italic>&#x00116;</italic><sub><italic>B</italic></sub>) to buffer the waste it receives from <bold>H</bold>, another measure of efficiency can be defined:</p>
<disp-formula id="E11"><label>(8)</label><mml:math id="M11"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x003B7;</mml:mi></mml:mrow><mml:mrow><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>t</mml:mi><mml:mi>e</mml:mi><mml:mi>n</mml:mi><mml:mi>d</mml:mi><mml:mi>e</mml:mi><mml:mi>d</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>B</mml:mi><mml:mo>,</mml:mo><mml:mi>O</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:mi>&#x003BA;</mml:mi><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>This appears to be a better efficiency indicator, because it accounts for the gross exergy input into <bold>H</bold> and includes the &#x0201C;hidden&#x0201D; load placed by <bold>H</bold> on the environment by forcing some biodegradation action. Its reciprocal, the cost <italic>c</italic><sub><italic>H,ext</italic></sub>, measures the exergy Watts needed to produce a unitary rate of accumulation including the environmental &#x0201C;service&#x0201D; provided by <bold>B</bold>:</p>
<disp-formula id="E12"><label>(9)</label><mml:math id="M12"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:mi>&#x003BA;</mml:mi><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>From the &#x0201C;combined system&#x0201D; point of view the useful exergy flux available for the accumulation in <bold>H</bold> is though <italic>&#x00116;</italic><sub><italic>in</italic></sub> &#x02212; <italic>&#x00116;</italic><sub><italic>out</italic></sub>, so that a global system efficiency can be defined:</p>
<disp-formula id="E13"><label>(10)</label><mml:math id="M13"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x003B7;</mml:mi></mml:mrow><mml:mrow><mml:mi>H</mml:mi><mml:mo>&#x0222A;</mml:mo><mml:mi>O</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>Its reciprocal, the cost <italic>c</italic><sub><italic>H</italic>&#x0222A;<italic>O</italic></sub>, measures the gross exergy Watts needed to produce a unitary rate of accumulation, i.e., a global &#x0201C;production cost&#x0201D;:</p>
<disp-formula id="E14"><label>(11)</label><mml:math id="M14"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mi>H</mml:mi><mml:mo>,</mml:mo><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>The above indicators provide a global measure of the ability of <bold>H</bold> to interact with <bold>O</bold> and exploit a given portion of the overall available &#x0201C;fuel,&#x0201D; defined as the difference between the incoming (low entropy) exergy flux and the (high entropy) portion re-radiated by <bold>O</bold>. The cost defined by equation (11) represents the total amount of primary exergy <italic>&#x00116;</italic><sub><italic>in</italic></sub> &#x02212; <italic>&#x00116;</italic><sub><italic>out</italic></sub> needed to &#x0201C;produce&#x0201D; a unit of accumulated exergy <italic>&#x00116;</italic><sub><italic>acc,H</italic></sub>: this is the &#x0201C;thermodynamic impact&#x0201D; of <bold>H</bold>&#x00027;s growth on the environment.</p>
<p>The method can be extended to more than one system interacting with <bold>O</bold> and also easily manipulated to include interactions between several systems <bold>H</bold><sub><bold>1</bold></sub>, <bold>H</bold><sub><bold>2</bold></sub>&#x02026;: notice that the above defined costs are time dependent and can be used to assess the evolution of the interplay between systems and the environment and of the state of the combined system <bold>O</bold> &#x0002B; <bold>H</bold><sub><bold>1</bold></sub> &#x0002B; <bold>H</bold><sub><bold>2</bold></sub> etc.</p>
<p>Notice also that a continuously decreasing value of either one of the above efficiency indicators in time (or, which is equivalent, an increase in the costs) signals a situation in which <bold>H</bold> (or indeed the combined system <bold>O</bold>&#x0222A;<bold>H</bold>) may be on a thermodynamically unsustainable path: in fact, <italic>&#x00116;</italic><sub><italic>acc,H</italic></sub> &#x0003D; 0 is the limit case of &#x0201C;steadiness&#x0201D; (survival with no growth) and <italic>&#x00116;</italic><sub><italic>acc,H</italic></sub> &#x0003C; 0 indicates negative growth, an obviously unsustainable condition. In conclusion, both the efficiency indicators and the costs are proper EI.</p>
</sec>
<sec id="s6">
<title>Exergy Based Indicators</title>
<p>While the above exergy-based description is perfectly suitable to evaluate the primary resources (solar irradiation, water, air and material taken directly from some natural <italic>reservoir</italic> in the environment surrounding the system), exergy <italic>per se</italic> is not a proper quantifier for secondary resources, i.e., resources on which some &#x0201C;work&#x0201D; or &#x0201C;action&#x0201D; has been performed by a system to bring them to the state at which they cross the control surface. The correct measure of the &#x0201C;exergy cost&#x0201D; of such pre-treated resources is the total amount of natural resources directly and indirectly expended in their transformation from the &#x0201C;state 0&#x0201D; to the state in which they cross the boundary of the system, measured in units of exergy. This is their <italic>embodied exergy content</italic><xref ref-type="fn" rid="fn0010"><sup>10</sup></xref>. Quite clearly, the identification of the production chains (the direct one and all of the indirect processes that generate the individual externally manufactured inputs) and the definition of the limits for the <italic>indirect</italic> exergy supply (i.e., the proper identification of the relevant control volume) are crucial issues in such an approach.</p>
<p>The embodied exergy content of a product or service can be calculated following, for instance, the Cumulative Exergy Content CExC (Szargut et al., <xref ref-type="bibr" rid="B50">1988</xref>), the Thermo-Ecological (or Exergo-Ecological) Cost TEC (Szargut, <xref ref-type="bibr" rid="B47">1995</xref>, <xref ref-type="bibr" rid="B48">1999</xref>, <xref ref-type="bibr" rid="B49">2005</xref>) or the Extended Exergy EEA (Sciubba, <xref ref-type="bibr" rid="B37">1998</xref>, <xref ref-type="bibr" rid="B38">2001</xref>; Colombo et al., <xref ref-type="bibr" rid="B6">2013</xref>) methods. All three methods maintain that any external intervention that adds or subtracts exergy from a stream before it crosses the control surface can be accounted for in terms of expended primary exergy. Since the terms in the balance equations (2) through (5) are completely quantifiable and homogeneous, the expenditures related to these external interventions can be algebraically added. The most popular methods used to derive exergy-based EIs, namely, the CExC, the TEA and the EEA, are presented and compared in the following sections, with the purpose of illustrating the difference between their respective EIs and to assess their commensurability (i.e., the existence of a procedure to convert one into the other). The three procedures are examined separately, with reference to the respective &#x0201C;control volumes&#x0201D; depicted in <xref ref-type="fig" rid="F7">Figure 7</xref> (CExC), <xref ref-type="fig" rid="F8">Figure 8</xref> (TEA) and <xref ref-type="fig" rid="F9">Figure 9</xref> (EEA)<xref ref-type="fn" rid="fn0011"><sup>11</sup></xref>.</p>
<fig id="F7" position="float">
<label>Figure 7</label>
<caption><p>The control volume for a Cumulative Exergy Consumption (CExC) analysis.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="frsus-02-739395-g0007.tif"/>
</fig>
<fig id="F8" position="float">
<label>Figure 8</label>
<caption><p>The control volume for a Thermo-Ecological (TEA) analysis.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="frsus-02-739395-g0008.tif"/>
</fig>
<fig id="F9" position="float">
<label>Figure 9</label>
<caption><p>For the calculation of the thermo-ecological exergy cost <italic>tec</italic>. <italic>&#x00116;</italic><sub><italic>M</italic></sub>, exergy rate of materials; <italic>&#x00116;</italic><sub><italic>NR</italic></sub>, exergy rate of non-renewables; <italic>&#x00116;</italic><sub><italic>R</italic></sub>, exergy rate of renewable energy carriers; <italic>&#x00116;</italic><sub><italic>D</italic></sub>, exergy rate of effluents; <italic>&#x00116;</italic><sub><italic>P</italic></sub>, exergy rate of main product; <italic>&#x00116;</italic><sub><italic>BP</italic></sub>, exergy rate of by-products; <italic>&#x00116;</italic><sub>&#x003B4;</sub>, exergy destruction rate.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="frsus-02-739395-g0009.tif"/>
</fig>
<sec>
<title>The Cumulative Exergy Consumption</title>
<p>This method was introduced by Szargut (<xref ref-type="bibr" rid="B46">1967</xref>) and perfected in later works by his group (Szargut et al., <xref ref-type="bibr" rid="B50">1988</xref>; Szargut, <xref ref-type="bibr" rid="B48">1999</xref>). It consists in the analysis of the complete line of production of a material good from raw materials to the final product: the corresponding control volume is shown in <xref ref-type="fig" rid="F7">Figure 7</xref>. The rationale of CExC is that <italic>the exergy expenditure necessary to produce a material commodity (i.e., the exergy embodied in it) is equal to the sum of all exergy contributions along the production line</italic>. The assumptions are as follows:</p>
<list list-type="alpha-lower">
<list-item><p>All raw materials entering the control volume directly from the Environment possess a &#x0201C;raw exergy&#x0201D; equal to their reference exergy (Valero et al., <xref ref-type="bibr" rid="B57">1986</xref>);</p></list-item>
<list-item><p>Materials that enter the control volume after having undergone a pre-treatment are attributed an exergy content equal to their raw value plus all of the exergy expenditures necessary for the pretreatment;</p></list-item>
<list-item><p>At each generic <italic>i-th</italic> production step, a portion of the incoming exergy flow is rejected to the environment in the form of &#x0201C;byproducts&#x0201D;: these flows, be they discharges, scrap material, or rejected energy that may be in principle recycled in different production lines, are collectively denominated <italic>&#x00116;</italic><sub><italic>w,i</italic></sub>;</p></list-item>
<list-item><p>The incoming exergy flows include both renewable and non-renewable sources;</p></list-item>
<list-item><p>The exergy outflow from production step <italic>i</italic> to production step <italic>i</italic> &#x0002B; <italic>1</italic> is considered a &#x0201C;product&#x0201D; of step <italic>i</italic> and a &#x0201C;fuel&#x0201D; for step <italic>i</italic> &#x0002B; <italic>1</italic>: <italic>&#x00116;</italic><sub><italic>out,i</italic></sub> &#x0003D; <italic>&#x00116;</italic><sub><italic>in,i</italic>&#x0002B;1</sub>: since the sum of the inputs into component <italic>i</italic> (<italic>&#x00116;</italic><sub><italic>in,i</italic></sub>) is in turn the &#x0201C;fuel&#x0201D; for its &#x0201C;product&#x0201D; <italic>&#x00116;</italic><sub><italic>out,i</italic></sub>, and <inline-formula><mml:math id="M15"><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mtext>&#x000A0;</mml:mtext><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, a &#x0201C;cumulative exergy cost&#x0201D; for the final (<italic>N-th</italic>) product of a technological production line can be defined as:
<disp-formula id="E15"><label>(12)</label><mml:math id="M16"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:mi>c</mml:mi><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:msub><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mstyle displaystyle="true"><mml:mo>&#x02211;</mml:mo></mml:mstyle><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mtext>&#x02003;&#x000A0;&#x000A0;&#x000A0;&#x02003;</mml:mtext><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:msubsup><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:msubsup></mml:mstyle><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mi>f</mml:mi><mml:mrow><mml:mo stretchy="true">(</mml:mo><mml:mrow><mml:mstyle displaystyle="true"><mml:msubsup><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:msubsup></mml:mstyle><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="true">)</mml:mo></mml:mrow></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:mrow></mml:mfrac><mml:mo>&#x0003E;</mml:mo><mml:mn>1</mml:mn><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>J</mml:mi><mml:mo>/</mml:mo><mml:mi>J</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p></list-item></list>
<p>Where the function <inline-formula><mml:math id="M18"><mml:mi>f</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msubsup><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:msubsup><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math></inline-formula>, a <italic>process structure function</italic>, is used instead of the simple <inline-formula><mml:math id="M19"><mml:msubsup><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:msubsup><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext></mml:math></inline-formula>to account for non-linear production chains (in the presence of a loop in the process flow diagram, the exergy destructions cannot be simply added, because of feedback effects).</p>
<p>The above definitions imply that if a product is generated starting from the very same raw materials by two different technological lines having different amounts of irreversible losses, its <italic>cexc</italic> assumes two different values. Thus, <italic>the cexc is a genuine measure of the environmental load posed on the primary resources available in the environment, and therefore a proper EI</italic>.</p>
<p>If <italic>M</italic><sub><italic>X</italic></sub> kg/yr of a (material or immaterial) commodity with a specific exergy <italic>e</italic><sub><italic>X</italic></sub> [J/kg] are generated per unit time, the total <inline-formula><mml:math id="M20"><mml:mi>C</mml:mi><mml:mi>E</mml:mi><mml:mi>x</mml:mi><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>X</mml:mi></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mi>i</mml:mi><mml:mi>s</mml:mi><mml:mtext>&#x000A0;</mml:mtext><mml:mi>e</mml:mi><mml:mi>q</mml:mi><mml:mi>u</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi><mml:mtext>&#x000A0;</mml:mtext><mml:mi>t</mml:mi><mml:mi>o</mml:mi><mml:mtext>&#x000A0;</mml:mtext><mml:mi>c</mml:mi><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>*</mml:mo></mml:mrow></mml:msup><mml:msubsup><mml:mrow><mml:mi>M</mml:mi></mml:mrow><mml:mrow><mml:mi>X</mml:mi></mml:mrow><mml:mrow><mml:mo>*</mml:mo></mml:mrow></mml:msubsup><mml:msub><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>X</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:msub></mml:math></inline-formula> [J<sub>primaryexergyresources</sub>/yr]. In the case of multiple products, proper allocation rules are suggested by Szargut (<xref ref-type="bibr" rid="B49">2005</xref>). The CExC does not contain any reference to the monetary circuit of the society in which the plant is located and is thus a purely technological EI. Since though neither the exergy destruction nor the exergy of the discharges are good indicators of environmental damage, the CExC must be regarded only as an indicator of the degree of resource exploitation.</p>
</sec>
<sec>
<title>The Thermo-Ecological Cost Analysis</title>
<p>Szargut later introduced (Szargut, <xref ref-type="bibr" rid="B47">1995</xref>, <xref ref-type="bibr" rid="B48">1999</xref>; Szargut et al., <xref ref-type="bibr" rid="B51">2002</xref>) the Thermo-Ecological Analysis, TEA, to include in the CExC the environmental externality: the relevant control volume is shown in <xref ref-type="fig" rid="F7">Figures 7</xref>, <xref ref-type="fig" rid="F8">8</xref>. The thermo-ecological cost <italic>tec</italic> (Szargut used the symbol &#x003BE;) is defined (Thermo-Ecological Portal, <xref ref-type="bibr" rid="B52">2020</xref>) as &#x0201C;<italic>the cumulative consumption of non-renewable exergy connected with the fabrication of a particular product with inclusion of additional consumption resulting from the necessity of compensation of environmental losses caused by rejection of harmful substances to the environment</italic>.&#x0201D; Obviously, the analysis must be conducted in a life-time sense.</p>
<p>The thermoecological cost <italic>tec</italic> is calculated as a ratio of exergy flows, and constitutes a measure of the primary non-renewable exergy directly or indirectly consumed in the production line under analysis. It can be determined by solving a set of thermoecological cost balance equations. With reference to <xref ref-type="fig" rid="F8">Figure 8</xref>, the rationale behind the calculation of the <italic>tec</italic> is the following:</p>
<list list-type="alpha-lower">
<list-item><p>The non-renewable exergy input is a net resource consumption (extracting ores and fossil fuels has a negative effect on <bold>O</bold>);</p></list-item>
<list-item><p>The processing of a material input and the generation of &#x0201C;secondary&#x0201D; energy carriers are affected by two sources of potential environmental damage: the exergy spent in the extraction and in the preparation of finished and semi-finished materials (i.e., their CExC, which includes the primary exergy consumed in the production line and has a negative effect on <bold>O</bold>), and the emissions generated in their preparation (direct negative effect on <bold>O</bold>);</p></list-item>
<list-item><p>The effluents may cause potential damage because of thermal- or chemical pollution on <bold>O</bold> (direct negative effect on <bold>O</bold>);</p></list-item>
<list-item><p>The by-products and the main product share the TEC according to exergy-based allocation rules (Serra and Torres, <xref ref-type="bibr" rid="B45">2003</xref>).</p></list-item>
</list>
<p>Once the mass- and energy balances of the process have been calculated, its exergy flow diagram can be constructed (in a way similar to that of CExC) to identify the non-renewable portion of the TEC of the material- and energy flows <italic>&#x00116;</italic><sub><italic>M</italic></sub> and <italic>&#x00116;</italic><sub><italic>NR</italic></sub>. The &#x0201C;environmental damage&#x0201D; portion of the TEC for each flow is computed by means of the so-called monetary indices of harmful impact (Szargut, <xref ref-type="bibr" rid="B49">2005</xref>)<xref ref-type="fn" rid="fn0012"><sup>12</sup></xref>:</p>
<disp-formula id="E17"><label>(14)</label><mml:math id="M21"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x003B6;</mml:mi></mml:mrow><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>N</mml:mi><mml:mi>R</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi>w</mml:mi></mml:mrow><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>G</mml:mi><mml:mi>D</mml:mi><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>D</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:mstyle displaystyle="true"><mml:msub><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:msub></mml:mstyle><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi>w</mml:mi></mml:mrow><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>Where <italic>E</italic><sub><italic>tot,NR</italic></sub> [J] is the annual exergy consumption of non-renewable natural resources, <italic>w</italic><sub><italic>k</italic></sub> [&#x020AC;/J] is a monetary coefficient of ecological damage per exergy unit of the k-th effluent, <italic>GDP</italic><sub><italic>D</italic></sub> [&#x020AC;] is the Gross Cumulative Product of the Domestic sector in the region where the process is located and <italic>P</italic><sub><italic>k</italic></sub> [J] the annual production of the k-th effluent rejected to the environment in the geographical domain of interest [for a detailed discussion, see the Thermoecological Portal (Thermo-Ecological Portal, <xref ref-type="bibr" rid="B52">2020</xref>)]. The <italic>tec</italic> measures the average cost in terms of primary exergy caused by the direct and indirect &#x0201C;environmental damage&#x0201D; caused by each technological chain in the country where it is located. For example, for a process whose only relevant emission is CO<sub>2</sub>, the total cost (CExC&#x0002B;TEC) for <italic>M</italic><sub><italic>X</italic></sub> kg/yr of the X commodity becomes</p>
<disp-formula id="E19"><label>(15)</label><mml:math id="M23"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:mi>M</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>c</mml:mi><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>c</mml:mi><mml:mtext>&#x000A0;</mml:mtext><mml:mo>*</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:mi>e</mml:mi><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>X</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:mi>t</mml:mi><mml:mi>e</mml:mi><mml:msub><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mi>S</mml:mi><mml:mo>,</mml:mo><mml:mi>C</mml:mi><mml:mi>O</mml:mi><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mi>S</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mi>S</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:msubsup><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:msubsup></mml:mstyle><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>S</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>S</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="true">(</mml:mo><mml:mrow><mml:mstyle displaystyle="true"><mml:msubsup><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:msubsup></mml:mstyle><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="true">)</mml:mo></mml:mrow></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:mrow></mml:mfrac></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mtext>&#x02003;&#x02003;&#x02003;&#x02003;&#x02003;&#x02003;&#x02003;&#x02003;&#x02003;&#x02003;&#x02003;&#x02003;</mml:mtext><mml:mo>&#x0002B;</mml:mo><mml:mstyle displaystyle="true"><mml:munder><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:munder></mml:mstyle><mml:msub><mml:mrow><mml:mi>&#x003B6;</mml:mi></mml:mrow><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>S</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>A TEC analysis is more involved than a CExC one: additional, strongly disaggregated data are needed to calculate the total consumption of the Domestic sector, the total emission of each pollutant in the country, and the monetary index of harmfulness of each pollutant &#x003C3;<sub><italic>j</italic></sub> needed for the calculation of the <italic>w</italic><sub><italic>j</italic></sub> in equation (14). In his original formulation, Szargut adopted the regulated pollutant taxation values, but he also maintained that a more rational value for &#x003C3; may be obtained by an iterative application of the TEC method.</p>
<p>The TEC has been criticized on two accounts: first, its calculation is perforce based on an extremely disaggregated and not easily accessible database; second, the definition of the index of harmful impact depends explicitly on the GDP<sub>D</sub>, which is known to be poorly correlated to the monetary circulation in a society (Meadows and Randers, <xref ref-type="bibr" rid="B27">1992</xref>; Mebratu, <xref ref-type="bibr" rid="B28">1998</xref>; Mudacumura et al., <xref ref-type="bibr" rid="B31">2005</xref>; Mart&#x000ED;nez-Alier et al., <xref ref-type="bibr" rid="B26">2010</xref>). A third objection, raised here for the first time, is that a low <italic>tec</italic> is no guarantee of sustainability: even if the non-renewable resources used in a production process were completely substituted by non-renewable ones, the society as a whole might have a cumulative resource consumption rate <italic>&#x00116;</italic><sub><italic>in,H</italic></sub> higher than that available in the Environment (see equation 5).</p>
</sec>
<sec>
<title>The Extended Exergy Accounting Method</title>
<p>The EEA method (Sciubba, <xref ref-type="bibr" rid="B37">1998</xref>, <xref ref-type="bibr" rid="B38">2001</xref>, <xref ref-type="bibr" rid="B42">2021</xref>) is for all purposes an extension of the CExC. Its fundamental axiom is that the three Externalities (Labor, Capital and Environmental Cost) can be assigned &#x0201C;equivalent exergy values,&#x0201D; under a set of assumptions derived from an exergy budget of the region in which the process is located. With reference to <xref ref-type="fig" rid="F10">Figure 10</xref>, the assumptions are:</p>
<list list-type="alpha-lower">
<list-item><p>The exergy &#x0201C;inflow&#x0201D; consists of both renewable and non-renewable physical streams into <bold>H</bold> and of the &#x0201C;imported&#x0201D; material and immaterial exergy flows from other regions;</p></list-item>
<list-item><p>A specific &#x0201C;extended exergy&#x0201D; [J/kg or J/unit] is defined as the equivalent exergy of each production factor: ee<sub>energy</sub> = e<sub>energy</sub> &#x0002B; ee<sub>externalities</sub>; ee<sub>material</sub> = e<sub>material</sub> &#x0002B; ee<sub>externalities</sub>. In practice, the <italic>cexc</italic> plus the externality &#x0201C;costs&#x0201D;;</p></list-item>
<list-item><p>A portion of the total exergy influx <italic>&#x00116;</italic><sub><italic>in,H</italic></sub> is &#x0201C;used&#x0201D; to sustain the population (included in its totality in the Domestic sector). This portion is called <italic>extended exergy of Labor</italic>, <inline-formula><mml:math id="M24"><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>L</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, and is set equal to &#x003B1;&#x00116;<sub><italic>in</italic></sub>, &#x003B1; &#x0003C; 1 being an econometric coefficient external to the theory that must be derived from the global exergy budget of the Country (Sciubba, <xref ref-type="bibr" rid="B39">2011</xref>);</p></list-item>
<list-item><p>The monetary circulation in the Country, <italic>M</italic><sub><italic>e</italic></sub>, is converted into another extended exergy flux, the Extended Exergy of Capital, <inline-formula><mml:math id="M25"><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>K</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>&#x003B2;</mml:mi><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>L</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>&#x003B1;</mml:mi><mml:mi>&#x003B2;</mml:mi><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>. The econometric coefficient &#x003B2; is also external to theory and must be calculated on the basis of financial/monetary data relevant to the Country under examination (Sciubba, <xref ref-type="bibr" rid="B39">2011</xref>; Colombo et al., <xref ref-type="bibr" rid="B6">2013</xref>; Biondi and Sciubba, <xref ref-type="bibr" rid="B1">2021</xref>). Using statistical labor and monetary data, it is possible to calculate the specific extended exergy of Labor <italic>ee</italic><sub><italic>L</italic></sub> [J/workhour] and of Capital <italic>ee</italic><sub><italic>K</italic></sub> [J/&#x020AC;]. These quantities represent the amount of primary exergy resources needed to generate 1 workhour and 1 monetary unit, respectively;</p></list-item>
<list-item><p>All EE forms are homogeneous and enjoy the additive property. Being &#x0201C;costs,&#x0201D; they also admit of a conservation equation (cost balance).</p></list-item>
</list>
<fig id="F10" position="float">
<label>Figure 10</label>
<caption><p>The control volume for an Extended Exergy Accounting (EEA) analysis.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="frsus-02-739395-g0010.tif"/>
</fig>
<p>EEA can be applied equally well to individual production lines, but its natural targets are very large complex systems like Cities, Industrial districts and Countries, where both the CExC and the TEC may run into congruency problems. In the case of a Country, the region in which the process is located is subdivided (<xref ref-type="fig" rid="F10">Figure 10</xref>) in 7 Sectors: Domestic (DO), Extractive (EX), Conversion (CO), Industrial (IN), Transportation (TR), Tertiary (TE) and Agricultural (AG). Each Sector exchanges fluxes of extended exergy with other sectors, with the environment and/or with another system called &#x0201C;Abroad&#x0201D; that accounts for the import/export. Every single process <bold>S</bold> exchanges extended exergy fluxes with some of the sectors; in particular, <inline-formula><mml:math id="M26"><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>L</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is assumed to be originated only in DO, and <inline-formula><mml:math id="M27"><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>K</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> in TE. Imported commodities are handled through TE.</p>
<p>Once the above quantities are known, a balance for the EE<sub>j</sub> of each individual production line is performed, resulting in a specific extended exergy cost, ee<sub>c</sub> [J<sub>primaryexergy</sub>/unit] that reflects the total amount of primary exergy resources consumed for the production of 1 unit of product X.</p>
<p>To calculate the Environmental externality, EEA adopts a <italic>remediation approach</italic> (<xref ref-type="fig" rid="F11">Figure 11</xref>): to eliminate (or maintain within the regulated limits) the emission of <italic>m</italic><sub><italic>k</italic></sub> [kg/s] of pollutant <italic>k</italic>, a (fictitious or real) process is inserted downstream of <bold>S</bold> that uses additional primary exergy to reduce the concentration <italic>c</italic><sub><italic>k</italic></sub> to its limit value (<italic>c</italic><sub><italic>k</italic>0</sub> or <italic>c</italic><sub><italic>k,regulated</italic></sub>) before discharging the exhaust into the environment. This additional consumption (per unit of product of <bold><italic>S</italic></bold>) consists of materials <inline-formula><mml:math id="M29"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:mi>M</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math></inline-formula>, energy (<inline-formula><mml:math id="M30"><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>E</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>), labor (<inline-formula><mml:math id="M31"><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>L</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>) and capital (<inline-formula><mml:math id="M32"><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>K</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>): the normalized sum of these quantities, denominated <italic>ee</italic><sub><italic>ENV</italic></sub>, is added to the <italic>ee</italic><sub><italic>c</italic></sub>.</p>
<fig id="F11" position="float">
<label>Figure 11</label>
<caption><p>Illustrative sketch of the procedure for the calculation of EE<sub>env</sub> in EEA. <inline-formula><mml:math id="M28"><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>r</mml:mi><mml:mi>o</mml:mi><mml:mi>d</mml:mi><mml:mi>u</mml:mi><mml:mi>c</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>r</mml:mi><mml:mi>o</mml:mi><mml:mi>d</mml:mi><mml:mi>u</mml:mi><mml:mi>c</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi></mml:mrow></mml:msub><mml:mo>&#x000B1;</mml:mo><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>r</mml:mi><mml:mi>o</mml:mi><mml:mi>d</mml:mi><mml:mi>u</mml:mi><mml:mi>c</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>M</mml:mi><mml:mo>,</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>L</mml:mi><mml:mo>,</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>K</mml:mi><mml:mo>,</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="frsus-02-739395-g0011.tif"/>
</fig>
<p>The calculation of the <italic>ee</italic><sub><italic>c</italic></sub> requires a similar data mining effort as the TEC: highly disaggregated data are needed for each Sector, for the technologically feasible effluent treatment processes and for the econometric coefficients &#x003B1; and &#x003B2;. Procedures to calculate the latter in terms of monetary and statistical employment data are reported in (Esterv&#x000E5;g, <xref ref-type="bibr" rid="B18">2003</xref>; Dewulf et al., <xref ref-type="bibr" rid="B13">2008</xref>; Se&#x000E7;kin et al., <xref ref-type="bibr" rid="B44">2012</xref>; Colombo et al., <xref ref-type="bibr" rid="B6">2013</xref>; Dai et al., <xref ref-type="bibr" rid="B8">2014</xref>; Biondi and Sciubba, <xref ref-type="bibr" rid="B1">2021</xref>).</p>
</sec>
</sec>
<sec id="s7">
<title>Comparison Between TEA and EEA</title>
<p>Both the <italic>tec</italic> and the <italic>eec</italic> are genuine resource consumption quantifiers, since both express a measure of the &#x0201C;environmental load&#x0201D; placed on system <bold>O</bold> by activities originating in <bold>H</bold>. They are obviously correlated (a production line with a minimal <italic>tec</italic> is likely to also have a minimal <italic>eec</italic>), and thus it is interesting to investigate whether the correlation admits of a mathematical expression.</p>
<p>For the sake of comparison, consider a process that produces <italic>N</italic> units/(unit time) of a commodity and emits <italic>m</italic> kg of CO<sub>2</sub> per unit. Let us also assume that the product exergy e<sub>P</sub>, the exergy of the discharges e<sub>D</sub>, the amount of non-renewables <italic>&#x00116;</italic><sub><italic>NR</italic></sub> and the exergy destruction rates are known. The <italic>ee</italic><sub><italic>c</italic></sub> is:</p>
<disp-formula id="E21"><label>(16)</label><mml:math id="M34"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:mi>e</mml:mi><mml:msub><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>X</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mtext>&#x000A0;</mml:mtext><mml:mi>e</mml:mi><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mi>M</mml:mi></mml:mrow></mml:msub><mml:mi>N</mml:mi><mml:mo>&#x0002B;</mml:mo><mml:mi>e</mml:mi><mml:msub><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>X</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:mi>e</mml:mi><mml:msub><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mi>L</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi>&#x01E86;</mml:mi></mml:mrow><mml:mrow><mml:mi>X</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:mi>e</mml:mi><mml:msub><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mi>K</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>X</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mtext>&#x02003;&#x02003;&#x000A0;&#x02003;</mml:mtext><mml:mrow><mml:mrow><mml:mo>&#x0002B;</mml:mo><mml:mi>e</mml:mi><mml:msub><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mi>N</mml:mi><mml:mi>V</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi>&#x01E41;</mml:mi></mml:mrow><mml:mrow><mml:mi>X</mml:mi><mml:mo>,</mml:mo><mml:mi>N</mml:mi><mml:mo>,</mml:mo><mml:mi>C</mml:mi><mml:mi>O</mml:mi><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>/</mml:mo><mml:mi>N</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>J</mml:mi><mml:mo>/</mml:mo><mml:mi>u</mml:mi><mml:mi>n</mml:mi><mml:mi>i</mml:mi><mml:mi>t</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>In the case of multiple products, proper allocation rules are suggested in (Sciubba, <xref ref-type="bibr" rid="B38">2001</xref>; Colombo et al., <xref ref-type="bibr" rid="B6">2013</xref>): they are formally the same as those adopted in TEC, but the structure of equation (16) allows for a more disaggregated account for the individual contributions (Labor, Capital and Environmental Remediation Cost), thus making the allocation easier. A perusal of equations (15, 16) suggests that the numerical values emerging from the calculation of the <italic>cexc</italic>&#x0002B;<italic>tec</italic> and <italic>ee</italic><sub><italic>c</italic></sub> are incommensurable, which is confirmed by a simple virtual experiment. Consider the reasonably realistic &#x0201C;sustainable&#x0201D; scenario described below:</p>
<list list-type="roman-lower">
<list-item><p>Each single component of the process (or society) is optimized and is affected by the minimum attainable degree of irreversibility: <inline-formula><mml:math id="M35"><mml:mrow><mml:mo stretchy="true">(</mml:mo><mml:mrow><mml:msubsup><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:msubsup><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="true">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mo class="qopname">min</mml:mo></mml:math></inline-formula>; the sum of the exergy destructions extended to all components (or sectors) is the smallest one possible with the current technological level;</p></list-item>
<list-item><p>The configuration (connectivity) of each conversion process is optimized so that the propagation of irreversibility from one component to the other is also minimized: <inline-formula><mml:math id="M36"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="true">(</mml:mo><mml:mrow><mml:msubsup><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:msubsup><mml:msub><mml:mrow><mml:mi>&#x00116;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003B4;</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="true">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:mo class="qopname">min</mml:mo></mml:math></inline-formula>;</p></list-item>
<list-item><p>Each effluent <italic>k</italic>-including all of the rejected flows <italic>&#x00116;</italic><sub><italic>w</italic>,1,<italic>S</italic></sub>- is conveyed to a treatment plant that reduces its temperature to <italic>T</italic><sub>0</sub> &#x0002B; &#x003B5; and its concentration to <italic>c</italic><sub>0,<italic>k</italic></sub> &#x0002B; &#x00394;<italic>c</italic><sub><italic>kb</italic></sub>, &#x003B5; being a small quantity (say, 1-2K<italic>), c</italic><sub>0<italic>k</italic></sub> the standard concentration of <italic>k</italic> in the environment and &#x00394;<italic>c</italic><sub><italic>kb</italic></sub> the buffering capacity of the environment for <italic>k</italic>.</p></list-item>
</list>
<p>Under the above scenario, equation (15) simplifies to:</p>
<graphic xlink:href="frsus-02-739395-e0001.tif"/>
<p>Because term <italic>I</italic> is completely offset by the environmental buffering (that requires only renewable resources), term <italic>II</italic> is minimal (assumption ii) and term <italic>III</italic> is zero because no non-renewable resources are used to reduce the potential ecological damage. Thus, the cumulative exergy consumption attains its minimum value.</p>
<p>Equation (16) becomes:</p>
<graphic xlink:href="frsus-02-739395-e0002.tif"/>
<p>Here, both <italic>IV</italic> and <italic>V</italic> reach their minima, the former because irreversibility is minimized within the system and the latter because the posited assumptions minimize <italic>ee</italic><sub><italic>ENV</italic></sub>. Of consequence, the extended exergy cost only attains its minimum value if the Capital and Labor terms are minimized as well. Even in such a case though, because of the inclusion in ee<sub>c</sub> of the equivalent primary exergy consumption of Labor and Capital production factors, the two minima (<italic>tec</italic><sub><italic>min</italic></sub> and <italic>eec</italic><sub><italic>min</italic></sub>) cannot be transformed one into the other by a rational formula: in fact, they not only differ numerically, but cannot be consistently rescaled, because:</p>
<list list-type="alpha-upper">
<list-item><p>&#x02013; The RHS of equation (18) contains terms (<inline-formula><mml:math id="M39"><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>L</mml:mi><mml:mo>,</mml:mo><mml:mi>X</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula><mml:math id="M40"><mml:msub><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>E</mml:mi><mml:mi>E</mml:mi></mml:mrow><mml:mo>&#x0002E;</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:mi>K</mml:mi><mml:mo>,</mml:mo><mml:mi>X</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>) that are not included in equation (17);</p></list-item>
<list-item><p>&#x02013; The calculation of the environmental externality is performed according to two completely different criteria. <xref ref-type="fig" rid="F12">Figure 12</xref> illustrates the different types of &#x0201C;flows&#x0201D; considered by the two methods.</p></list-item>
</list>
<fig id="F12" position="float">
<label>Figure 12</label>
<caption><p>For the comparison of the <italic>tec</italic> with the <italic>eec</italic>.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="frsus-02-739395-g0012.tif"/>
</fig>
</sec>
<sec id="s8">
<title>The Exergy Footprint</title>
<p>In light of the above considerations, we can now introduce a novel indicator, the Exergy Footprint <italic>ExF</italic>, defined (Sciubba, <xref ref-type="bibr" rid="B40">2012</xref>) as <italic>the amount of primary exergy (in J) globally consumed over the life of a commodity, including material, energy, labor, capital and environmental remediation costs and calculated on a life-time basis</italic>.</p>
<p>The <italic>ExF</italic> is the integral in time of the <italic>eec</italic>, and it is clear that the Second Law places a lower limit to its numerical value: even if we could adopt a &#x0201C;perfect recycling,&#x0201D; some external exergy source would be necessary to sustain the process and compensate for the exergy destruction. We recover here the idea that thermodynamic sustainability (<italic>eec</italic> = 1 when calculated for the whole Society) is impossible: therefore it would be more proper to speak of a &#x0201C;degree of unsustainability,&#x0201D; &#x003BE; &#x0003D; <italic>(eec-1)/eec</italic>.</p>
<p>The <italic>ExF</italic> provides useful -and unique- information at several levels:</p>
<list list-type="alpha-lower">
<list-item><p>If two different technological chains produce a (material or immaterial) commodity X, the one with the lower <italic>Ex</italic>F is less unsustainable;</p></list-item>
<list-item><p>Since the environmental remediation cost is included in the calculation, &#x0201C;cleaner&#x0201D; technologies have -<italic>ceteris paribus</italic>- a lower <italic>Ex</italic>;</p></list-item>
<list-item><p>If a process modification is considered that changes the &#x0201C;energy mix&#x0201D; of the input or of the output (for instance replacing an electrical boiler with a fossil-fueled one or vice versa), the <italic>Ex</italic>F automatically accounts for the different &#x0201C;quality&#x0201D; of the input or output. The same is true for material substitution: if one or more material inputs are substituted with others having a different <italic>cexc</italic> and a different <italic>eec</italic>, this is automatically reflected in the <italic>Ex</italic>;</p></list-item>
<list-item><p>At a more aggregated level, the <italic>Ex</italic> can be used to assess the degree of unsustainability of different infrastructures. For example, between two planned road paths, or between a bridge over a river vs. a tunnel, or between two different sites for an airport, etc.;</p></list-item>
<list-item><p>At an even more aggregated level, the <italic>Ex</italic> can provide unique information about the different degree of unsustainability of different societal policies, like what energy mix to adopt, whether or not to promote specific energy conversion systems or agricultural productions, whether to import materials or finite goods from other countries or produce them inland, etc.</p></list-item>
</list>
</sec>
<sec sec-type="conclusions" id="s9">
<title>Conclusions</title>
<p>The current concept of &#x0201C;sustainability,&#x0201D; though almost acritically accepted by media and decision makers, is far too vague to be amenable to practical and meaningful scientific use. In a thermodynamic sense, a closed system is never sustainable (unless it is at equilibrium, i.e., &#x0201C;dead&#x0201D;), and an open one may be sustainable or not depending on whether the exergy input rate is higher (or not) than the sum of the exergy destruction and accumulation rates within the system, augmented by the exergy expenditure required by the environment to buffer the effect of the effluents. It is therefore important to realize that there are two facets to a &#x0201C;sustainable development&#x0201D;: the first is of thermodynamic nature, governed by the relevant system equations described in this paper, and the second described by socio-economical indices, whose interpretation is outside of the bounds of Thermodynamics. As for the former, it is convenient to adopt exergy as a general quantifier, because it not only attributes a thermodynamically correct value to any type of flux, but also directly relates irreversibility to unsustainability: reversible processes are intrinsically sustainable (too bad there is none known in the Universe!).</p>
<p>It is rather clear that the socio-economical interpretation must be supported by the thermodynamic one, in the sense that if a system &#x0201C;uses&#x0201D; the incoming exergy flow in a way that leads to a total net depletion rate of (fossil or renewable) exergy sources, no societal organizational form can survive in the long run unless new exergy inputs are provided at a sufficient rate. It is true that the specific form of the societal organization may affect -<italic>ceteris paribus</italic>- the exergy depletion rate, but this does not imply that such a &#x0201C;minimum exergy consumption&#x0201D; society may be acceptable from an ethical point of view: this decision implies a <italic>value choice</italic> and is outside of the realm of Thermodynamics. Studies that do not separate these two issues are therefore bound to reach wrong and misleading conclusions.</p>
<p>Indicators of the &#x0201C;resource efficiency&#x0201D; of a system (be it a production line, a natural species, a human settlement, an entire nation) can be defined only in the thermodynamic system logic and at the largest system physical scale: they are termed here &#x0201C;global.&#x0201D; It is important to realize that &#x0201C;local&#x0201D; indicators are completely legitimate, but since they are by definition concerned either with a set that generally includes non-thermodynamically relevant quantities or with a limited subset of the state variables of the system, they cannot be taken as genuine indicators of the degree of sustainability as formulated above.</p>
</sec>
<sec sec-type="data-availability" id="s10">
<title>Data Availability Statement</title>
<p>The original contributions presented in the study are included in the article/supplementary material, further inquiries can be directed to the corresponding author/s.</p>
</sec>
<sec id="s11">
<title>Author Contributions</title>
<p>The author confirms being the sole contributor of this work and has approved it for publication.</p>
</sec>
<sec sec-type="COI-statement" id="conf1">
<title>Conflict of Interest</title>
<p>The author declares that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="s12">
<title>Publisher&#x00027;s Note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
</body>
<back>
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</ref-list>
<sec id="s13">
<title>List of Symbols</title>
<table-wrap position="float" id="T1">
<table frame="hsides" rules="groups">
<tbody>
<tr style="border-bottom: thin solid #000000;">
<td valign="top" align="left"><bold>B</bold></td>
<td valign="top" align="left">immediate surroundings of a system</td>
<td valign="top" align="left">&#x003B7;</td>
<td valign="top" align="left">Efficiency</td>
</tr>
<tr>
<td valign="top" align="left">c [J/unit]</td>
<td valign="top" align="left">cost</td>
<td valign="top" align="left">&#x003BA;</td>
<td valign="top" align="left">Waste-pollution coefficient</td>
</tr>
<tr>
<td valign="top" align="left"><italic>&#x00116;</italic> [W]</td>
<td valign="top" align="left">Exergy Flow</td>
<td valign="top" align="left"><bold>Suffixes</bold></td>
<td/>
</tr>
<tr>
<td valign="top" align="left">E [J]</td>
<td valign="top" align="left">Exergy</td>
<td valign="top" align="left"><italic>0</italic></td>
<td valign="top" align="left">Initial Conditions</td>
</tr>
<tr>
<td valign="top" align="left">EI</td>
<td valign="top" align="left">Environmental Indicator</td>
<td valign="top" align="left">acc</td>
<td valign="top" align="left">accumulated</td>
</tr>
<tr>
<td valign="top" align="left">EPA</td>
<td valign="top" align="left">Environmental Protection Agency</td>
<td valign="top" align="left">b</td>
<td valign="top" align="left">consumed by <bold>B</bold></td>
</tr>
<tr>
<td valign="top" align="left"><bold>H</bold></td>
<td valign="top" align="left">Human society</td>
<td valign="top" align="left"><italic>in</italic></td>
<td valign="top" align="left">input</td>
</tr>
<tr>
<td valign="top" align="left">NR</td>
<td valign="top" align="left">Non-renewable source</td>
<td valign="top" align="left"><italic>out</italic></td>
<td valign="top" align="left">output</td>
</tr>
<tr>
<td valign="top" align="left"><bold>O</bold></td>
<td valign="top" align="left">Environment</td>
<td valign="top" align="left"><italic>w</italic></td>
<td valign="top" align="left">waste</td>
</tr>
<tr>
<td valign="top" align="left">t [s]</td>
<td valign="top" align="left">Time</td>
<td valign="top" align="left">&#x003B4;</td>
<td valign="top" align="left">exergy destruction</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<fn-group>
<fn id="fn0001"><p><sup>1</sup>One of the Reviewers correctly remarked that secondary fuels (biomass) is in fact a &#x0201C;high entropy&#x0201D; resource, but that its use brings advantages in terms of the Environmental Externality. A more correct classification would refer to such resources as &#x0201C;low Extended Exergy&#x0201D; fuels (see section The Extended Exergy Accounting Method below).</p></fn>
<fn id="fn0002"><p><sup>2</sup>A related issue, not specifically addressed in this study, is that of re-evaluating on a Thermodynamic basis some of the local indicators adopted in biological, social and ethnological sciences. Such EIs t are usually based on a &#x0201C;numerosity&#x0201D; index of a selected population (the <italic>indicator species</italic>) and on its time evolution in the environmental niche of observation. For a more detailed discussion (Sciubba, <xref ref-type="bibr" rid="B41">2013</xref>).</p></fn>
<fn id="fn0003"><p><sup>3</sup>Popper&#x00027;s falsificationist methodology (Popper, <xref ref-type="bibr" rid="B33">1979</xref>) holds that scientific theories are characterized by entailing predictions that future observations might reveal to be false. But to be falsified, a theory must be complete (it must contain an exact definition of its domain of application and of the relevant boundary conditions) and consequential (all of its predictions can be derived by some fundamental axioms by a procedure devoid of arbitrariness).</p></fn>
<fn id="fn0004"><p><sup>4</sup>A paradigmatic example is the longstanding debate between advocates of a strong population control and supporters of a &#x0201C;prosperous way down&#x0201D; (see Galor and Moav, <xref ref-type="bibr" rid="B20">2001</xref>; Sciubba and Zullo, <xref ref-type="bibr" rid="B43">2009</xref>; Mart&#x000ED;nez-Alier et al., <xref ref-type="bibr" rid="B26">2010</xref>) for a detailed analysis of the issue). Both approaches address the same problem (resource exhaustion), but the proposed solutions diverge rather radically and are in fact incommensurable, since they are based on completely different premises that involve value judgements.</p></fn>
<fn id="fn0005"><p><sup>5</sup>We include in this &#x0201C;thermodynamic basis&#x0201D; also the biological, biophysical and environmental sciences at large.</p></fn>
<fn id="fn0006"><p><sup>6</sup>In the context of this paper, exergy is <italic>the minimum amount of adiabatic work necessary to bring a system from an initial state S</italic><sub>0</sub> <italic>of equilibrium with the environment to an arbitrary final state S</italic><sub>1</sub> <italic>by means of processes that involve solely S and the environment</italic>. For a complete and rigorous treament of the topic (see Moran, <xref ref-type="bibr" rid="B30">1982</xref>; Kotas, <xref ref-type="bibr" rid="B23">1985</xref>).</p></fn>
<fn id="fn0007"><p><sup>7</sup>The specific exergy of materials (see for example Szargut, <xref ref-type="bibr" rid="B49">2005</xref>).</p></fn>
<fn id="fn0008"><p><sup>8</sup>This is the well-known &#x0201C;Hubbert scenario&#x0201D;, currently known to represent an oversimplification of the actual resource exploitation curve. Among other weaknesses, it neglects changes in the extraction/refining technology and in the final demand. It is used here only to exemplify what would be the long-term situation of a &#x0201C;fossils only&#x0201D; society. A more rigorous analysis is presented in Sciubba and Zullo (<xref ref-type="bibr" rid="B43">2009</xref>).</p></fn>
<fn id="fn0009"><p><sup>9</sup>Boltzmann (&#x0201C;&#x02026;<italic>The general struggle for existence of animal beings is therefore not a struggle for raw materials &#x02013; these, for organisms, are air, water and soil, all abundantly available&#x02013; nor for energy, which exists in plenty in any body in the form of heat, but a struggle for entropy</italic>,&#x0201D; Boltzmann, <xref ref-type="bibr" rid="B2">1905</xref>) and Schroedinger (&#x0201C;<italic>What an organism feeds upon is negative entropy</italic>,&#x0201D; Schroedinger, <xref ref-type="bibr" rid="B36">1945</xref>) expressed the same principle in terms of entropy production, which is equivalent to exergy destruction. Lotka (<xref ref-type="bibr" rid="B25">1922</xref>) used the expression &#x0201C;<italic>consumption of available energy</italic>&#x0201D;.</p></fn>
<fn id="fn0010"><p><sup>10</sup>The concept of &#x0201C;embodied exergy&#x0201D; was first proposed by Yantovsky (<xref ref-type="bibr" rid="B61">1994</xref>).</p></fn>
<fn id="fn0011"><p><sup>11</sup>CexC, TEC and EEA owe a significant portion of their theoretical foundation to Thermo-Economics, a method originated in Eastern Germany in the late &#x02018;50es (Rant, <xref ref-type="bibr" rid="B35">1956</xref>; Elsner and Fratzscher, <xref ref-type="bibr" rid="B16">1959</xref>; Bosnjakovic, <xref ref-type="bibr" rid="B3">1965</xref>; Fratzscher, <xref ref-type="bibr" rid="B19">1965</xref>), reframed in a monetary context in the US by Tribus, El-Sayed and Evans in the 70&#x00027;es (El-Sayed and Gaggioli, <xref ref-type="bibr" rid="B15">1989</xref>; El Sayed, <xref ref-type="bibr" rid="B14">2003</xref>) and reformulated in its current form by Tsatsaronis (<xref ref-type="bibr" rid="B54">1984</xref>) and Valero (Valero et al., <xref ref-type="bibr" rid="B57">1986</xref>; Serra and Torres, <xref ref-type="bibr" rid="B45">2003</xref>) in the 80&#x00027;es. The original TE paradigm adopts a monetary measure in its cost definition, the TEC -using the very same formalism- introduces a purely exergy cost similar to those described in section 4 above. The CExC avoids any reference to monetary units, and the EEA is an extension of the CExC (see below, section The Extended Exergy Accounting Method) that makes use of the TE cost allocation rules.</p></fn>
<fn id="fn0012"><p><sup>12</sup>Notice that the calculation scheme presented in the Thermo-Ecological Portal (<xref ref-type="bibr" rid="B52">2020</xref>) is slightly different from, and probably not as rigorous as, the one originally proposed by Szargut (<xref ref-type="bibr" rid="B49">2005</xref>): here, equation (14) is taken from the original formulation, while the first part (the extended balance that includes the non-renewables) is adapted from the Thermoecological portal.</p></fn>
</fn-group>
</back>
</article>