The Law of Parsimony and the Negative Charge of the Bubbles

Why the bubbles are negatively charged? This is almost 100 years old question, which many scientists have striven and still are striving to answer using the latest developments of the MD simulations and various physical analytical methods. We scrutinize with this paper the basic literature on this t...

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Main Authors: Stoyan I. Karakashev, Nikolay A. Grozev
Format: Article
Language:English
Published: MDPI AG 2020-10-01
Series:Coatings
Subjects:
Online Access:https://www.mdpi.com/2079-6412/10/10/1003
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spelling doaj-ffce5503be0d4ba382d46b1051ac2e892020-11-25T04:05:28ZengMDPI AGCoatings2079-64122020-10-01101003100310.3390/coatings10101003The Law of Parsimony and the Negative Charge of the BubblesStoyan I. Karakashev0Nikolay A. Grozev1Department of Physical Chemistry, Sofia University, 1 James Bourchier Blvd, 1164 Sofia, BulgariaDepartment of Physical Chemistry, Sofia University, 1 James Bourchier Blvd, 1164 Sofia, BulgariaWhy the bubbles are negatively charged? This is almost 100 years old question, which many scientists have striven and still are striving to answer using the latest developments of the MD simulations and various physical analytical methods. We scrutinize with this paper the basic literature on this topic and conduct our own analysis. Following the philosophical law of parsimony: “Entities should not be multiplied without necessity”, we assume that the simplest explanation is the right one. It is well known that the negative change of the Gibbs free energy is a solid criterion for spontaneous process. Hence, we calculated the energies of adsorption of OH<sup>−</sup>, H<sub>3</sub>O<sup>+</sup> and HCO<sub>3</sub><sup>−</sup> ions on the air/water interface using the latest theoretical developments on the dispersion interaction of inorganic ions with the air/water interface. Thus, we established that the adsorption of OH<sup>−</sup> and HCO<sub>3</sub><sup>−</sup> ions is energetically favorable, while the adsorption of H<sub>3</sub>O<sup>+</sup> is energetically unfavorable. Moreover, we calculated the change of the entropy of these ions upon their transfer from the bulk to the air/water interface. Using the well-known formula Δ<i>G</i> = Δ<i>H</i> − <i>T</i>Δ<i>S</i>, we established that the adsorption of OH<sup>−</sup> and HCO<sub>3</sub><sup>−</sup> ions on the air/water interface decreases their Gibbs free energy. On the contrary, the adsorption of H<sub>3</sub>O<sup>+</sup> ions on the air/water interface increases their Gibbs free energy. Thus, we established that both OH<sup>-</sup> and HCO<sub>3</sub><sup>−</sup> ions adsorb on the air/water interface, while the H<sub>3</sub>O<sup>+</sup> ions are repelled by the latter. Therefore, electrical double layer (EDL) is formed at the surface of the bubble–negatively charged adsorption layer of OH<sup>−</sup> and HCO<sub>3</sub><sup>−</sup> ions and positively charged diffuse layer of H<sub>3</sub>O<sup>+</sup> ions.https://www.mdpi.com/2079-6412/10/10/1003ion-specific effectsDI wateradsorption of ionsbubbles
collection DOAJ
language English
format Article
sources DOAJ
author Stoyan I. Karakashev
Nikolay A. Grozev
spellingShingle Stoyan I. Karakashev
Nikolay A. Grozev
The Law of Parsimony and the Negative Charge of the Bubbles
Coatings
ion-specific effects
DI water
adsorption of ions
bubbles
author_facet Stoyan I. Karakashev
Nikolay A. Grozev
author_sort Stoyan I. Karakashev
title The Law of Parsimony and the Negative Charge of the Bubbles
title_short The Law of Parsimony and the Negative Charge of the Bubbles
title_full The Law of Parsimony and the Negative Charge of the Bubbles
title_fullStr The Law of Parsimony and the Negative Charge of the Bubbles
title_full_unstemmed The Law of Parsimony and the Negative Charge of the Bubbles
title_sort law of parsimony and the negative charge of the bubbles
publisher MDPI AG
series Coatings
issn 2079-6412
publishDate 2020-10-01
description Why the bubbles are negatively charged? This is almost 100 years old question, which many scientists have striven and still are striving to answer using the latest developments of the MD simulations and various physical analytical methods. We scrutinize with this paper the basic literature on this topic and conduct our own analysis. Following the philosophical law of parsimony: “Entities should not be multiplied without necessity”, we assume that the simplest explanation is the right one. It is well known that the negative change of the Gibbs free energy is a solid criterion for spontaneous process. Hence, we calculated the energies of adsorption of OH<sup>−</sup>, H<sub>3</sub>O<sup>+</sup> and HCO<sub>3</sub><sup>−</sup> ions on the air/water interface using the latest theoretical developments on the dispersion interaction of inorganic ions with the air/water interface. Thus, we established that the adsorption of OH<sup>−</sup> and HCO<sub>3</sub><sup>−</sup> ions is energetically favorable, while the adsorption of H<sub>3</sub>O<sup>+</sup> is energetically unfavorable. Moreover, we calculated the change of the entropy of these ions upon their transfer from the bulk to the air/water interface. Using the well-known formula Δ<i>G</i> = Δ<i>H</i> − <i>T</i>Δ<i>S</i>, we established that the adsorption of OH<sup>−</sup> and HCO<sub>3</sub><sup>−</sup> ions on the air/water interface decreases their Gibbs free energy. On the contrary, the adsorption of H<sub>3</sub>O<sup>+</sup> ions on the air/water interface increases their Gibbs free energy. Thus, we established that both OH<sup>-</sup> and HCO<sub>3</sub><sup>−</sup> ions adsorb on the air/water interface, while the H<sub>3</sub>O<sup>+</sup> ions are repelled by the latter. Therefore, electrical double layer (EDL) is formed at the surface of the bubble–negatively charged adsorption layer of OH<sup>−</sup> and HCO<sub>3</sub><sup>−</sup> ions and positively charged diffuse layer of H<sub>3</sub>O<sup>+</sup> ions.
topic ion-specific effects
DI water
adsorption of ions
bubbles
url https://www.mdpi.com/2079-6412/10/10/1003
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