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Difference between revisions of "Gnaiger 2018 EBEC2018"

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|year=2018
|year=2018
|event=EBEC2018 Budapest HU
|event=EBEC2018 Budapest HU
|abstract=ā€˜.. ''the sum of the '''electrical pressure difference''' and the '''osmotic pressure difference''' (i.e. the electrochemical potential difference) of protons''ā€™ [1] links to non-ohmic flux-force relationships between proton leak and protonmotive force (pmf). This is experimentally established, has direct consequences on mitochondrial physiology, but is theoretically little understood [2,3]. Here I distinguish pressure from potential differences (diffusion: Ī”''Ī¼<sub>H</sub>+'' or Ī”<sub>d</sub>''F''<sub>H</sub>+; electric: Ī”''ĪØ'' or Ī”<sub>el</sub>''F''), to explain non-ohmic flux-'''[[force]]''' relationships on the basis of four thermodynamic theorems. (1) Einsteinā€™s diffusion equation [4] explains the [[concentration]] gradient (d''c''/d''z'') in Fickā€™s law as the product of chemical potential gradient (the vector force and resistance determine the velocity, ''v'', of a particle) and local concentration, ''c''. This yields the chemical [[pressure]] gradient (vanā€™t Hoff): d<sub>d</sub>''Ī ''/d''z'' = ''RT''āˆ™d''c''/d''z''. [[Flux]] [5] is the product of ''v'' and ''c''; ''c'' varies with force. Therefore, flux-force relationships are non-linear. (2) The pmf is not a vector force; the gradient is replaced by a pressure difference, and local concentration by a distribution function or free activity, ''Ī±''. Flux is a function of ''Ī±'' and force, ''J''<sub>d</sub> = ''b''āˆ™''Ī±''āˆ™Ī”<sub>d</sub>''F''<sub>B</sub> = -''b''āˆ™Ī”<sub>d</sub>''Ī ''<sub>B</sub> [6]. (3) At Ī”<sub>el</sub>''F'' = -Ī”<sub>d</sub>''F''<sub>H</sub>+, the diffusion pressure of protons, Ī”<sub>d</sub>''Ī ''<sub>H</sub>+ = ''RT''āˆ™Ī”<sub>c</sub><sub>H</sub>+ [Pa=Jāˆ™m<sup>-3</sup>] is balanced by electric pressure, maintained by counterions of H<sup>+</sup>. Diffusional and electric pressures are isomorphic, additive, and yield protonmotive pressure (pmp). (4) The dependence of [[proton leak]] on pmf varies with Ī”<sub>el</sub>''F'' versus Ī”<sub>d</sub>''F''<sub>H</sub>+, in agreement with experimental evidence. The flux-force relationship is concave at high mitochondrial volume fractions, but near-exponential at small mt-matrix volume ratios. Linear flux-pmp relationships imply a near-exponential dependence of the proton leak on the pmf.
|abstract=ā€˜.. ''the sum of the '''electrical pressure difference''' and the '''osmotic pressure difference''' (i.e. the electrochemical potential difference) of protons''ā€™ [1] links to non-ohmic flux-force relationships between proton leak and protonmotive force ''pmF''. This is experimentally established, has direct consequences on mitochondrial physiology, but is theoretically little understood [2,3]. Here I distinguish pressure from potential differences (diffusion: Ī”''Ī¼''<sub>H<sup>+</sup></sub> or Ī”<sub>d</sub>''F''<sub>H<sup>+</sup></sub>; electric: Ī”''ĪØ'' or Ī”<sub>el</sub>''F''<sub>p<sup>+</sup></sub>), to explain non-ohmic flux-'''[[force]]''' relationships on the basis of four thermodynamic theorems. (''1'') Einsteinā€™s diffusion equation [4] explains the [[concentration]] gradient (d'''''c'''''/d'''''z''''') in Fickā€™s law as the product of chemical potential gradient (the vector force and resistance determine the velocity '''''v''''' of a particle) and local concentration '''''c'''''. This yields the chemical [[pressure]] gradient (vanā€™t Hoff): d<sub>'''d'''</sub>'''''Ī '''''/d'''''z''''' = ''RT''āˆ™d'''''c'''''/'''d''z'''''. [[Flux]] [5] is the product of '''''v''''' and '''''c'''''; '''''c''''' varies with force. Therefore, flux-force relationships are non-linear. (''2'') The ''pmF'' is not a vector force; the gradient is replaced by a pressure difference, and local concentration by a distribution function or free activity ''Ī±''. Flux is a function of ''Ī±'' and force, ''J''<sub>d</sub> = -''u''<sub>d</sub>āˆ™''Ī±''āˆ™Ī”<sub>d</sub>''F<sub>X</sub>'' = -''u''<sub>d</sub>āˆ™Ī”<sub>d</sub>''Ī <sub>X</sub>'' [6]. (''3'') At Ī”<sub>el</sub>''F''<sub>p<sup>+</sup></sub> = -Ī”<sub>d</sub>''F''<sub>H</sub>+, the diffusion pressure of protons, Ī”<sub>d</sub>''Ī ''<sub>H</sub>+ = ''RT''āˆ™Ī”''c''<sub>H</sub>+ [Pa=Jāˆ™m<sup>-3</sup>] is balanced by electric pressure, maintained by counterions of H<sup>+</sup>. Diffusional and electric pressures are isomorphic, additive, and yield protonmotive pressure ''pmp''. (''4'') The dependence of [[proton leak]] on ''pmF'' varies with Ī”<sub>el</sub>''F''<sub>p<sup>+</sup></sub> versus Ī”<sub>d</sub>''F''<sub>H</sub>+, in agreement with experimental evidence. The flux-force relationship is concave at high mitochondrial volume fractions, but near-exponential at small mt-matrix volume ratios. Linear flux-''pmp'' relationships imply a near-exponential dependence of the proton leak on the ''pmF'' ([7]; added 2022-07-04).
|editor=[[Gnaiger E]]
|editor=[[Gnaiger E]]
|mipnetlab=AT Innsbruck Gnaiger E
|mipnetlab=AT Innsbruck Gnaiger E
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:::# Gnaiger E (1993) Nonequilibrium thermodynamics of energy transformations. Pure Appl Chem 65:1983-2002. - [[Gnaiger_1993_Pure_Appl_Chem |Ā»Bioblast linkĀ«]] Ā 
:::# Gnaiger E (1993) Nonequilibrium thermodynamics of energy transformations. Pure Appl Chem 65:1983-2002. - [[Gnaiger_1993_Pure_Appl_Chem |Ā»Bioblast linkĀ«]] Ā 
:::# Gnaiger E (1989) Mitochondrial respiratory control: energetics, kinetics and efficiency. In: Energy transformations in cells and organisms. Wieser W, Gnaiger E (eds), Thieme, Stuttgart:6-17. - [[Gnaiger_1989_Energy_Transformations |Ā»Bioblast linkĀ«]]
:::# Gnaiger E (1989) Mitochondrial respiratory control: energetics, kinetics and efficiency. In: Energy transformations in cells and organisms. Wieser W, Gnaiger E (eds), Thieme, Stuttgart:6-17. - [[Gnaiger_1989_Energy_Transformations |Ā»Bioblast linkĀ«]]
:::# Gnaiger E (2020) Mitochondrial pathways and respiratory control. An introduction to OXPHOS analysis. 5<sup>th</sup> ed. https://doi.org/10.26124/bec:2020-0002 - The symbols in the above abstract have been adjusted to those in the 5<sup>th</sup> ed.


{{Labeling
{{Labeling

Latest revision as of 22:17, 4 July 2022

The protonmotive force under pressure: an isomorphic analysis.

Link: EBEC2018

Gnaiger E (2018)

Event: EBEC2018 Budapest HU

ā€˜.. the sum of the electrical pressure difference and the osmotic pressure difference (i.e. the electrochemical potential difference) of protonsā€™ [1] links to non-ohmic flux-force relationships between proton leak and protonmotive force pmF. This is experimentally established, has direct consequences on mitochondrial physiology, but is theoretically little understood [2,3]. Here I distinguish pressure from potential differences (diffusion: Ī”Ī¼H+ or Ī”dFH+; electric: Ī”ĪØ or Ī”elFp+), to explain non-ohmic flux-force relationships on the basis of four thermodynamic theorems. (1) Einsteinā€™s diffusion equation [4] explains the concentration gradient (dc/dz) in Fickā€™s law as the product of chemical potential gradient (the vector force and resistance determine the velocity v of a particle) and local concentration c. This yields the chemical pressure gradient (vanā€™t Hoff): ddĪ /dz = RTāˆ™dc/dz. Flux [5] is the product of v and c; c varies with force. Therefore, flux-force relationships are non-linear. (2) The pmF is not a vector force; the gradient is replaced by a pressure difference, and local concentration by a distribution function or free activity Ī±. Flux is a function of Ī± and force, Jd = -udāˆ™Ī±āˆ™Ī”dFX = -udāˆ™Ī”dĪ X [6]. (3) At Ī”elFp+ = -Ī”dFH+, the diffusion pressure of protons, Ī”dĪ H+ = RTāˆ™Ī”cH+ [Pa=Jāˆ™m-3] is balanced by electric pressure, maintained by counterions of H+. Diffusional and electric pressures are isomorphic, additive, and yield protonmotive pressure pmp. (4) The dependence of proton leak on pmF varies with Ī”elFp+ versus Ī”dFH+, in agreement with experimental evidence. The flux-force relationship is concave at high mitochondrial volume fractions, but near-exponential at small mt-matrix volume ratios. Linear flux-pmp relationships imply a near-exponential dependence of the proton leak on the pmF ([7]; added 2022-07-04).


ā€¢ Bioblast editor: Gnaiger E ā€¢ O2k-Network Lab: AT Innsbruck Gnaiger E


Affiliations

  1. D. Swarovski Research Lab, Dept Visceral, Transplant Thoracic Surgery, Medical Univ Innsbruck
  2. Oroboros Instruments
Innsbruck, Austria. - [email protected]

References

  1. Mitchell P (1966) Chemiosmotic coupling in oxidative and photosynthetic phosphorylation. Glynn Research, Bodmin. Biochim Biophys Acta Bioenergetics 1807:1507-38. - Ā»Bioblast linkĀ«
  2. Garlid KD, Beavis AD, Ratkje SK (1989) On the nature of ion leaks in energy-transducing membranes. Biochim Biophys Acta 976:109-20. - Ā»Bioblast linkĀ«
  3. Beard DA (2005) A biophysical model of the mitochondrial respiratory system and oxidative phosphorylation. PLOS Comput Biol 1(4):e36. - Ā»Bioblast linkĀ«
  4. Einstein A (1905) Ɯber die von der molekularkinetischen Theorie der WƤrme geforderte Bewegung von in ruhenden FlĆ¼ssigkeiten suspendierten Teilchen. Ann Physik 4, XVII:549-60. - Ā»Bioblast linkĀ«
  5. Gnaiger E (1993) Nonequilibrium thermodynamics of energy transformations. Pure Appl Chem 65:1983-2002. - Ā»Bioblast linkĀ«
  6. Gnaiger E (1989) Mitochondrial respiratory control: energetics, kinetics and efficiency. In: Energy transformations in cells and organisms. Wieser W, Gnaiger E (eds), Thieme, Stuttgart:6-17. - Ā»Bioblast linkĀ«
  7. Gnaiger E (2020) Mitochondrial pathways and respiratory control. An introduction to OXPHOS analysis. 5th ed. https://doi.org/10.26124/bec:2020-0002 - The symbols in the above abstract have been adjusted to those in the 5th ed.


Labels: MiParea: Respiration 




Regulation: Flux control, Ion;substrate transport, mt-Membrane potential  Coupling state: LEAK 


Event: Oral  MitoEAGLE