Difference between revisions of "Advancement"
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{{MitoPedia | {{MitoPedia | ||
|abbr=d<sub>tr</sub>''Ī¾'' | |abbr=d<sub>tr</sub>''Ī¾'' | ||
|description=In an isomorphic analysis, any form of [[flow]] is the '''advancement''' of a process per unit of time, expressed in a specific [[motive unit]] [MUās<sup>-1</sup>], ''e.g.'', ampere for electric flow or current [Aā”Cās<sup>-1</sup>], watt for heat flow [Wā”Jās<sup>-1</sup>], and for chemical flow the unit is [molāsĀ<sup>-1</sup>] ('''extent of reaction''' per time). The corresponding motive [[force]]s are the partial exergy (Gibbs energy) changes per advancement [JāMU<sup>-1</sup>], expressed in volt for electric force [Vā”JāC<sup>-1</sup>], dimensionless for thermal force [JāJ<sup>-1</sup>], and for chemical force the unit is [Jāmol<sup>-1</sup>], which deserves a specific acronym ([Jol]) comparable to volt. For chemical processes of reaction and diffusion, the advancement is the amount of motive substance [mol]. The concept was originally introduced by De Donder [1]. Central to the concept of advancement is the [[stoichiometric number]], ''Ī½''<sub> | |description=In an isomorphic analysis, any form of [[flow]] is the '''advancement''' of a process per unit of time, expressed in a specific [[motive unit]] [MUās<sup>-1</sup>], ''e.g.'', ampere for electric flow or current [Aā”Cās<sup>-1</sup>], watt for heat flow [Wā”Jās<sup>-1</sup>], and for chemical flow the unit is [molāsĀ<sup>-1</sup>] ('''extent of reaction''' per time). The corresponding motive [[force]]s are the partial exergy (Gibbs energy) changes per advancement [JāMU<sup>-1</sup>], expressed in volt for electric force [Vā”JāC<sup>-1</sup>], dimensionless for thermal force [JāJ<sup>-1</sup>], and for chemical force the unit is [Jāmol<sup>-1</sup>], which deserves a specific acronym ([Jol]) comparable to volt. For chemical processes of reaction (spontaneous from high-potential substrates to low-potential products) and compartmental diffusion (spontaneous from a high-potential compartment to a low-potential compartment), the advancement is the amount of motive substance that has undergone a compartmental transformation [mol]. The concept was originally introduced by De Donder [1]. Central to the concept of advancement is the [[stoichiometric number]], ''Ī½''<sub>''i''</sub>, associated with each motive component ''i'' (transformant [2]). | ||
In a chemical reaction, r, the motive entity is the stoichiometric amount of reactant, d<sub>r</sub>''n''<sub> | In a chemical reaction, r, the motive entity is the stoichiometric amount of reactant, d<sub>r</sub>''n''<sub>''i''</sub>, with stoichiometric number ''Ī½''<sub>''i''</sub>. The advancement of the chemical reaction, d<sub>r</sub>''Ī¾'' [mol], is then defined as | ||
Ā d<sub>r</sub>''Ī¾'' = d<sub>r</sub>''n''<sub> | Ā d<sub>r</sub>''Ī¾'' = d<sub>r</sub>''n''<sub>''i''</sub>Ā·''Ī½''<sub>''i''</sub><sup>-1</sup> | ||
The flow of the chemical reaction, ''I''<sub>r</sub> [molĀ·s<sup>-1</sup>], is advancement per time, | The flow of the chemical reaction, ''I''<sub>r</sub> [molĀ·s<sup>-1</sup>], is advancement per time, | ||
Ā ''I''<sub>r</sub> = d<sub>r</sub>''Ī¾''Ā·d''t''<sup>-1</sup> | Ā ''I''<sub>r</sub> = d<sub>r</sub>''Ī¾''Ā·d''t''<sup>-1</sup> | ||
This concept of advancement is extended to compartmental diffusion and the advancement of charged particles [3], and to any discontinuous transformation in compartmental systems [2], | |||
:::: [[File:Advancement.png|100px]] | |||
|info=[[Gnaiger_1993_Pure Appl Chem |Gnaiger (1993) Pure Appl Chem]] | |info=[[Gnaiger_1993_Pure Appl Chem |Gnaiger (1993) Pure Appl Chem]] | ||
}} | }} | ||
Ā Communicated by [[Gnaiger E]] 2018-10-16 | Ā Communicated by [[Gnaiger E]] 2018-11-01, 2018-10-16 | ||
== Advancement per volume == | |||
:::: The advancement of a transformation in a closed homogenous system (chemical reaction) or discontinuous system (diffusion) causes a change of [[concentration]] of substances ''i''. | |||
::::Ā» [[Advancement per volume]], d<sub>tr</sub>''Y'' = d<sub>tr</sub>''Ī¾''āV<sup>-1</sup> | ::::Ā» [[Advancement per volume]], d<sub>tr</sub>''Y'' = d<sub>tr</sub>''Ī¾''āV<sup>-1</sup> | ||
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:::# De Donder T (1936) Thermodynamic theory of affinity: a book of principles. Oxford, England: Oxford University Press. | :::# De Donder T (1936) Thermodynamic theory of affinity: a book of principles. Oxford, England: Oxford University Press. | ||
:::# Gnaiger E (1993) Nonequilibrium thermodynamics of energy transformations. Pure Appl Chem 65:1983-2002. - [[Gnaiger 1993 Pure Appl Chem |Ā»Bioblast linkĀ«]] | :::# Gnaiger E (1993) Nonequilibrium thermodynamics of energy transformations. Pure Appl Chem 65:1983-2002. - [[Gnaiger 1993 Pure Appl Chem |Ā»Bioblast linkĀ«]] | ||
Ā | ::::# Prigogine I (1967) Introduction to thermodynamics of irreversible processes. Interscience New York, 3rd ed:147pp. - [[Prigogine 1967 Interscience |Ā»Bioblast linkĀ«]] | ||
{{MitoPedia concepts | {{MitoPedia concepts | ||
|mitopedia concept=MiP concept, Ergodynamics | |mitopedia concept=MiP concept, Ergodynamics | ||
}} | }} |
Revision as of 18:25, 1 November 2018
Description
In an isomorphic analysis, any form of flow is the advancement of a process per unit of time, expressed in a specific motive unit [MUās-1], e.g., ampere for electric flow or current [Aā”Cās-1], watt for heat flow [Wā”Jās-1], and for chemical flow the unit is [molās-1] (extent of reaction per time). The corresponding motive forces are the partial exergy (Gibbs energy) changes per advancement [JāMU-1], expressed in volt for electric force [Vā”JāC-1], dimensionless for thermal force [JāJ-1], and for chemical force the unit is [Jāmol-1], which deserves a specific acronym ([Jol]) comparable to volt. For chemical processes of reaction (spontaneous from high-potential substrates to low-potential products) and compartmental diffusion (spontaneous from a high-potential compartment to a low-potential compartment), the advancement is the amount of motive substance that has undergone a compartmental transformation [mol]. The concept was originally introduced by De Donder [1]. Central to the concept of advancement is the stoichiometric number, Ī½i, associated with each motive component i (transformant [2]).
In a chemical reaction, r, the motive entity is the stoichiometric amount of reactant, drni, with stoichiometric number Ī½i. The advancement of the chemical reaction, drĪ¾ [mol], is then defined as
drĪ¾ = drniĀ·Ī½i-1
The flow of the chemical reaction, Ir [molĀ·s-1], is advancement per time,
Ir = drĪ¾Ā·dt-1
This concept of advancement is extended to compartmental diffusion and the advancement of charged particles [3], and to any discontinuous transformation in compartmental systems [2],
Abbreviation: dtrĪ¾
Reference: Gnaiger (1993) Pure Appl Chem
Communicated by Gnaiger E 2018-11-01, 2018-10-16
Advancement per volume
- The advancement of a transformation in a closed homogenous system (chemical reaction) or discontinuous system (diffusion) causes a change of concentration of substances i.
- Ā» Advancement per volume, dtrY = dtrĪ¾āV-1
References
- De Donder T (1936) Thermodynamic theory of affinity: a book of principles. Oxford, England: Oxford University Press.
- Gnaiger E (1993) Nonequilibrium thermodynamics of energy transformations. Pure Appl Chem 65:1983-2002. - Ā»Bioblast linkĀ«
- Prigogine I (1967) Introduction to thermodynamics of irreversible processes. Interscience New York, 3rd ed:147pp. - Ā»Bioblast linkĀ«
MitoPedia concepts: MiP concept, Ergodynamics