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Communication

The Effects of Acid and Water in the Formation of Anodic Alumina: DFT and Experiment Study

1
High Value Fine Chemicals Research Center, Department of Chemistry & Chemical Engineering, Jinzhong University, Jinzhong 030619, China
2
Shaanxi Applied Physics and Chemistry Research Institute, Xi’an 710061, China
*
Author to whom correspondence should be addressed.
Molecules 2023, 28(6), 2427; https://doi.org/10.3390/molecules28062427
Submission received: 31 January 2023 / Revised: 26 February 2023 / Accepted: 1 March 2023 / Published: 7 March 2023
(This article belongs to the Topic Theoretical, Quantum and Computational Chemistry)

Abstract

:
The DFT method is employed to study the adsorption and reaction behaviors of HC2O4, H2PO4, HSO4 and H2O on neutral and anodic aluminum slabs. With the exception of adsorption, the three acid radicals can successively take the two H atoms from the adsorbed H2O on the anodic aluminum slabs, which is the key step of the formation of anodic alumina. The dehydrogenation reaction is dominated by the Coulombic interaction of O and H, respectively belonging to acid radicals and the adsorbed H2O or OH, rather than by the interaction of electronic orbits located on the two kinds of atoms. The experiment of anodic polarization of aluminum verifies the calculation result well.

Graphical Abstract

1. Introduction

The anodic alumina layer has been used in many fields, such as corrosion resistance [1], capacitors [2], biomaterials [3] and biosensors [4].The alumina film obtained through the anodic oxidation of aluminum in acidic electrolytes has been investigated for its wide range of uses.
Many factors influence the morphology and crystal structure of anodic alumina. The anodizing parameters including anodic potential [5,6], electrolyte [7,8] and temperature [6,9,10,11] have been investigated. The electrolyte component is the key factor affecting anodic alumina. Oxalic acid, phosphoric acid and sulfuric acid solutions are usually used to form the anodic alumina. When the anodic oxidation was performed in oxalic acid solutions [12,13,14], the concentrations were usually 0.3 M, and the temperature, voltage and time varied with different morphologies. The solutions containing phosphoric acid [15,16,17,18,19,20] were usually used when fabricating porous alumina. Sulfuric acid [21,22,23] was also used in the fabrication of porous alumina. In most cases, the combined application of the three acids was carried out in order to regulate the size and morphology of pores in the anodic alumina. Some other acids [24,25,26,27] are occasionally used, and their aims are also obtaining various porous anodic alumina. The morphology of alumina film closely relates to acid radicals in the electrolyte.
The factors influencing the formation of alumina morphology have been carefully studied in experiments, but the microscopic mechanism at the molecular level was rarely involved. Microscopic mechanism investigation involves the change of the Al–O bond and the composition of oxides. Su [28] studied the field-enhanced water dissociation at the growing oxide surface in order to explain the dissolution of alumina and the pore formation in the anodic alumina. This work solved one of problems raised 22 years ago by Thompson and coworkers [29]. Thompson and coworkers [29] also mentioned phosphorous and carbon contained in the anodic alumina formed in phosphate and oxalate solution, respectively. They pointed out that phosphorus extends over about two thirds of the film thickness. Garcia-Vergara and coworkers [30] also found the phosphorous signal in the anodic alumina film fabricated by anodizing in Na2HPO4 electrolyte. The phosphorous is present from the surface of the film to relative depths of in the range ~0.7 to ~0.8 of the film thickness. Thompson [31] obtained a similar result. A relatively pure anodic alumina contains 3–4 wt% phosphorous [29]. The changing mechanism of the Al-O bond and composition of oxides need to be further explored.
What are the roles of acid radicals and water during the formation of anodic alumina? Does the oxygen of alumina come from the acid radicals or water? How does the oxygen of alumina become separated from the molecule? The initial adsorption and interaction of acid radicals and water have a relationship with those questions. In the present work, the adsorption and interaction of electrolyte molecules will be studied using the DFT method.

2. Results

2.1. The Adsorption of Molecules

The small molecules of H2O, HC2O4, H2PO4 and HSO4 were randomly placed on three aluminum slabs of (100), (110) and (111), see Figure S1. The three slabs are, respectively, given 0 or +1 charges to represent neutral or anodic conditions in the calculation. The adsorption energies (Eads) of H2O and acid radicals are listed in Table 1. Their adsorption states are shown in Figure S2.
The Eads is calculated using the following equation:
Eads = Eslab-molecule − Eslab − Emolecule
where the Eslab-molecule is the energy of the aluminum slab adsorbed with the small molecule, the Eslab is the energy of the aluminum slab and the Emolecule is the energy of the small molecule. All of the adsorption energies of H2O and the three acid radicals are negative. The four small molecules can stably adsorb on the three kinds of aluminum faces under neutral or anodic conditions. The adsorption energies of the three acid radicals are bigger than that of H2O, and the adsorption of acid radicals is more stable. The H2O and the three acid radicals have bigger Eads; in other words, the four small molecules have more stable adsorption states when the aluminum faces are in the anodic condition.
The directly stable adsorption is the first behavior of the H2O and the three acid radicals on the three aluminum faces.

2.2. The Acid Radicals Replacing the Adsorbed H2O

Because the three acid radicals adsorb more stably than H2O, the adsorbed H2O may be replaced by acid radicals leaving the aluminum surface. The models of the acid radicals substituting the adsorbed H2O were built as shown as Figure S3. The acid radicals approach the adsorbed H2O from the side. The calculation results show that the adsorbed H2O really can be replaced by the acid radicals. These courses are represented by Figure S3, too. The replacing energy values (Erep) of the three replacing courses are listed in Table 2. The Erep is calculated using the following equation:
Erep = Erep after − Eslab-water − Eacid radical
where the Erep after is the energy of the adsorbed H2O replaced by the acid radical, the Eslab-water is the energy of the aluminum slab with adsorbed H2O and the Eacid radical is the energy of the acid radical. The negative Erep values mean that the replacing courses are feasible.
The three acid radicals replacing the adsorbed H2O is the second behavior of the four small molecules.

2.3. The Acid Radicals Bonding with the H of Adsorbed H2O

The acid radicals of HC2O4, H2PO4 and HSO4 have the O atoms enriched with negative charge, so they have the ability to bond with the H of adsorbed H2O. In the initial models, the O atom of the acid radical is near to the H of adsorbed H2O on the neutral aluminum slab. After the calculation of geometry optimization, the acid radical does connect with the adsorbed H2O through O–H–O, as shown as Figure 1. The H–O bond of H2O is stretched to a longer length. The change in bonding energy (Ebon) of the acid radical and adsorbed H2O is calculated using the following equation:
Ebon = E(slab-H2O-acid radical) − Eslab-H2O − Eacid radical
where the E(slab-H2O-acid radical) is the energy of the acid radical connecting with the adsorbed H2O on the neutral aluminum slab, the Eslab-H2O is the energy of the neutral aluminum slab with adsorbed H2O and the Eacid radical is the energy of the acid radical. The Ebon values of the three acid radicals are listed in Table 3. The negative Ebon values indicate that the connection between the acid radicals and adsorbed H2O are reasonable.
The three acid radicals connecting with the adsorbed H2O on the neutral aluminum slab is the third behavior of the four small molecules.
The adsorption of radicals is more stable than water, yet the molecular structures of radicals remain stable on the neutral or positively charged slab, see Figure S2. It has been confirmed that the concentrations of light elements are very low in the anodic alumina [32]. This implies that the adsorption of radicals with complete structure has no important contribution to Al–O formation. The O–H of adsorbed water is easily stretched by the radicals, see Figure 1 and Table 3, so the third behavior of water and radicals may be the dominant way in which the Al–O bond is formed.

2.4. The Acid Radicals Stripping off H from Adsorbed H2O and OH

On the neutral aluminum slabs, the acid radicals can stretch the H–O bond of adsorbed H2O to a longer length, but they do not have the ability to snap it. Under the anodic condition, the three acid radicals have enough power to successfully take the two H atoms away from the adsorbed H2O, see Figure 2. The O atom of the adsorbed H2O is finally left to bond with the aluminum on the surface. The processes of acid radicals stripping off H are represented through chemical equations in Figure 3. Every equation has two reaction directions. The “1” direction is the acid radical stripping off H from the adsorbed H2O or OH, and the “2” direction is the corresponding reverse reaction. The energy change of the reaction of the acid radical stripping off H (Estr) is calculated using the following equation:
Estr = E(OH or O+acid) − Eslab-H2O or OH − Eacid radical
where the E(OH or O+acid) is the energy of the acid and adsorbed OH (one of the H atoms of H2O is stripped) or adsorbed O (the two H atoms of H2O are stripped), the Eslab-H2O or OH is the energy of the anodic aluminum slab adsorbed with H2O or OH and the Eacid radical is the energy of the acid radical. Every step of the acid radical taking the H atom away from the adsorbed H2O or OH has a negative Estr value (see Table 4), in other words, the reverse reactions are not feasible.
The acid radical continuously stripping the two H atoms off the adsorbed H2O on the anodic aluminum slab is the fourth behavior of the four molecules. The binding energies of absorption for the three acid radicals (see Table 1) are actually lower than those of reacting with H2O (see Table 4). The reaction of extracting H from H2O has a larger tendency than adsorption for the three radicals. It can be deduced that the adsorption of radicals really occurs, with much less influence on the formation of the Al–O bond. In the course of alumina formation, the function of the acid radical is to pull off the two H atoms of the adsorbed H2O, and the role of H2O is the supplier of oxygen in alumina.

2.5. The Reasons for Acid Radicals Stripping off H Atoms of H2O

The acid radicals stripping off the H atoms of the adsorbed H2O are chemical reactions including the changing of chemical bonds. DFT energies about bond changes are some of the most accurate theoretical results, and can be interpreted by analysis of the Klopman–Salem equation [32] from a molecular orbital theory perspective. The Coulombic and/or covalent interactions between the acid radicals and H atoms determine the reactions in the Klopman–Salem equation:
Δ E = Q Nu Q EI ε R + 2 ( β C Nu C EI ) 2 E Nu , HOMO   E EI , HOMO
where ΔE is the energy change of the reaction, QNu is the charge of the nucleophile, QEI is the charge of the electrophile, ε is the local dielectric constant, R is the distance between the nucleophile and electrophile, β is the resonance integral, c is the coefficient of the molecular orbit to form the new bond, ENu,HOMO is the HOMO energy of the nucleophile and EEI,LUMO is the LUMO energy of the electrophile. In the present work, the nucleophiles are acid radicals and the electrophiles are the H atoms of adsorbed H2O. In the Klopman– Salem equation, the first term and the second term represent the Coulombic interaction and orbital interaction between acid radicals and H atoms, respectively.
If the orbital interaction determines the reaction of acid radicals stripping off H atoms, the ΔE should inversely relate to the difference between ENu,HOMO and EEI,LUMO, as shown in the second term of the Klopman–Salem equation. Figure 4 shows the difference between Eacid radical,HOMO (the HOMO energy of the acid radical) and EH (the orbital energy of H in the adsorbed H2O and OH). The value of (EHSO4,HOMO − EH) is the smallest one, which is close to that of (EH2PO4,HOMO − EH). The value of (EHCO4,HOMO − EH) is the largest one. In Table 4, the reaction energy change of HSO4 stripping off H is the lowest one, the H2PO4 has the largest reaction energy change and the HCO4 has a large reaction energy change, too. The results in Table 4 have no regular relationship with the values of (Eacid radical,HOMO − EH), and, thus, the orbital interaction does not determine the reaction of acid radicals stripping off H atoms.
If the Coulombic interaction determines the reaction of acid radicals stripping off H atoms, the ΔE should positively relate to the product of QNuQEI, as shown in the first term of the Klopman–Salem equation. Figure 5 shows the charges of the O atom of HCO4, H2PO4 and HSO4. These O atoms directly interact with the H atoms with charge of QH. The order of charge values is QO, H2PO4 > QO, HCO4 > QO, HSO4, so there should be QHQO, H2PO4 > QHQO, HCO4 > QHQO, HSO4 for the three acid radicals interacting with the same kind of H. In Table 4, the reaction energy changes of HCO4, H2PO4 and HSO4 are also in the order of H2PO4 > HCO4 > HSO4. The order of ΔE is same as that of the products of QHQO, acid radical, so ΔE positively relates to the product of QHQO. The reactions of dehydrogenation may be dominated by the Coulombic interaction.
Since the reaction is solely affected by Coulombic interaction (the first term of the Klopman–Salem equation), there are two further inferences. The first one is that the acid radical with larger-charged O has the greater ability to extract the same kind of H atom of adsorbed H2O. The second one is that it is easier for a larger-charged H of adsorbed H2O to be stripped off by the same acid radical.
The positive charge of the slab makes the charge of H of adsorbed H2O and OH increase, as shown as Table 5. This means the QH, neutral is smaller than the QH, positive. The product of QH, neutralQO, acid radical is smaller than that of QH, positiveQO, acid radical. The product value of charges indicates that the reaction of stripping off H on the positively charged slab is easier. The H atoms of H2O adsorbed on the neutral slab really cannot be stripped off, see Figure 1, while those on the positively charged slab can be taken away by the same acid radical, see Figure 2. The second inference is reasonable.
According to the courses of proving the two inferences, the acid radical with larger-charged O in favor of the dehydrogenation of adsorbed H2O and the positive charge of the anodic slab are necessary for accelerating the process of the H leaving the adsorbed H2O.

2.6. The Experimental Verification

The calculation results, see Table 4, indicate that the abilities of dehydrogenation of the three acids are in the order phosphoric acid > oxalic acid > sulfuric acid. In other words, the forming of the anodic alumina is the easiest in the phosphoric acid aqueous solution, and it is the most difficult in the sulfuric acid aqueous solution.
In order to verify the theoretic results, the anodic alumina will, respectively, grow in the three acid solutions. The aluminum foil with (100), (110) and (111) faces, see Figure 6a, is immersed into the acid solution to perform anodic polarization. In the sulfuric acid solution, the current rises with the increasing potential of the aluminum anode. In the oxalic acid solution, the change in current has a similar trend to that in the sulfuric acid solution, but the current of the oxalic acid solution is smaller than that of the sulfuric acid solution. In the phosphoric acid solution, the current maintains the smallest value, and the polarization curve is far under the curves generated in the oxalic and sulfuric acids solutions, as shown in Figure 6b. The reduction in the current arises from the coverage of the anodic surface by the growth of alumina. The polarization curves of Figure 6b imply that the phosphoric acid has the most powerful ability to extract H from the H2O adsorbed on the anodic surface, and to facilitate the growth of anodic alumina. The sulfuric acid is the weakest one. The oxalic acid lies between the former two acids.
The experiment result has the same trend as the theoretic calculation. It verifies the theoretic interpretation of the formation course of anodic alumina.
The acid radical stepwisely removes the hydrogen atoms of H2O adsorbed on the anodic surface. The ability of dehydrogenation is in the order H3PO4 > H2CO4 > H2SO4. The reaction of dehydrogenation is dominated by the Coulombic interaction between the oxygen anion of the acid radical and the hydrogen of the water, rather than by the frontier molecular orbits of the acid radical and water.
This work only supplies a reference for selecting acid and interprets the initial stage of alumina formation. The incrassation of alumina involves the transfer of oxygen and aluminum ions in the alumina layer and the dehydrogenation of water on the alumina surface. These processes need a follow-up study.

3. Materials and Methods

3.1. Computation

The oxalic acid, phosphoric acid and sulfuric acid are frequently used as the acid component of electrolyte in preparing anodic alumina. In the aqueous solution of oxalic acid, phosphoric acid or sulfuric acid, the three kinds of acid radicals HC2O4, H2PO4 or HSO4, respectively, are the dominant species. The (100), (110) and (111) are the main exposed faces on the aluminum surface. The water, three acid radicals and Al (100), (110) and (111) faces were selected as the specific model to investigate the roles of water and acid in the formation of the Al–O bond of anodic alumina.
Al (100), (110) and (111) slabs (p5 × 5) with 5 layers and 20 Å vacuum range were built, see Figure S1. The atomic coordinates of the inner three layers (blue) are fixed, while the atoms of the outer two layers (pink) relax freely. The small molecules including H2O, HC2O4, H2PO4 and HSO4 were placed on the center of slabs in the course of calculation. Computations were performed using DMOl3 code, which adopts fully self-consistent DFT calculations to solve Kohn–Sham equations. The generalized gradient approximation (GGA), with the functional PBE for metallic surfaces adsorbing with some small molecules [33], was employed. For all models, the double numerical plus polarization (DNP) [34] was selected as the basis set. The ultrasoft pseudopotentials for Al, S, P, O, C and H were used in all calculations. The energy convergence tolerance was 2 × 10−5 eV per atom.

3.2. Experiment

Commercial aluminum foils was prepared. They simultaneously have three faces of (100), (110) and (111), which was confirmed through the analysis of X-ray diffraction (XRD) on a PAN-analytical-X’Pert PRO X diffractometer equipped with Cu Kα radiation (λ = 0.15406 nm). The aluminum foils were cut into small squares with a tail as the outgoing line. The side length of the squares is 10 mm. The squares were washed subsequently with acetone and ethanol. Electrochemical tests were successively performed in the oxalic acid solution (0.1 mol/L), phosphoric acid solution (0.1 mol/L) and sulfuric acid solution (0.1 mol/L). The Versatile Multichannel Potentiostat 2/Z (VMP2, Princeton Applied Research) was employed in the test. The Ag/AgCl reference electrode was adopted to obtain the relative potential. The potential sweeping speed is 10 mV s−1 in this work.

4. Conclusions

The H2O, HCO4, H2PO4 and HSO4 have four kinds of adsorption behaviors on the aluminum slabs: (1) all of them can spontaneously adsorb on the aluminum slabs; (2) the HCO4, H2PO4 and HSO4 have the ability to replace the adsorbed H2O; (3) the HCO4, H2PO4 and HSO4 can connect with the adsorbed H2O through the O–H–O bond on the neutral aluminum slabs and (4) on the anodic aluminum slabs, the HCO4, H2PO4 and HSO4 connected with the adsorbed H2O can further polarize the O–H bond of H2O and strip off its H. The three radicals can continuously extract the second H of H2O. The process going on in cycles leaves the O being left to form alumina. The third and fourth behaviors are the key steps of the formation of anodic alumina. The effect of radicals is to take the H away from the H2O. The effect of the H2O is to supply the O for anodic alumina.
The dehydrogenation processes between the acid radicals and adsorbed H2O on the anodic aluminum slab are thermodynamically feasible and have no potential barriers. These processes are dominated by the Coulombic interaction of the O of radicals and H of adsorbed H2O or OH, rather than by the interaction of electronic orbits located on the two kinds of atoms. The experiment verifies the theoretic interpretation of formation course of anodic alumina well.
The energy changes of extracting H on the three faces are different. The effect of aluminum slab structures influence the anodic alumina formation, too. This factor will be investigated in the follow-up study.

Supplementary Materials

The following supporting information can be downloaded at: https://www.mdpi.com/article/10.3390/molecules28062427/s1, Figure S1: The acid radicals and water adsorb on the neutral and positively charged slabs; Figure S2: The acid radicals substitute water on the neutral and positively charged slabs; Figure S3: The acid radicals substitute water on the natural and positively charged slabs.

Author Contributions

Conceptualization, Z.Z.; methodology, Z.Z. and J.K.; validation, Z.Z., J.K. and Y.D.; formal analysis, P.L.; investigation, X.L.; resources, Y.Q.; data curation, Z.Z. and N.L.; writing—original draft preparation, Z.Z.; writing—review and editing, Z.Z.; visualization, J.L.; supervision, X.L.; project administration, Z.Z.; funding acquisition, Y.D. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by the National Science Fund for Distinguished Young Scholars (Grant No. 52000092).

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Data generated in this study are stored at Jinzhong University and are available upon reasonable request.

Acknowledgments

We acknowledge the technical support from Xian-Feng Du in Xian Jiaotong University. We also acknowledge the software support from Qiang Wang in The Xinjiang Technical Institute of Physics & Chemistry, Chinese Academy of Sciences.

Conflicts of Interest

The authors declare no conflict of interest.

Sample Availability

Samples of aluminium and three acids are available from the authors.

References

  1. Senbahavalli, R.; Mohanapriya, S.; Raj, V. Enhanced corrosion resistance of anodic non-porous alumina (ANPA) coatings on aluminium fabricated from mixed organic-inorganic electrolytes. Mater. Discov. 2016, 3, 29–37. [Google Scholar] [CrossRef]
  2. Hourdakis, E.; Nassiopoulou, A.G. High-Density MIM Capacitors with Porous Anodic Alumina Dielectric. IEEE Trans. Electron Devices 2010, 57, 2679–2683. [Google Scholar] [CrossRef]
  3. Thorat, S.B.; Diaspro, A.; Salerno, M. In vitro investigation of coupling-agent-free dental restorative composite based on nano-porous alumina fillers. J. Dent. 2014, 42, 279–286. [Google Scholar] [CrossRef]
  4. Macias, G.; Hernández-Eguía, L.P.; Ferré-Borrull, J.; Pallares, J.; Marsal, L.F. Gold-Coated Ordered Nanoporous Anodic Alumina Bilayers for Future Label-Free Interferometric Biosensors. ACS Appl. Mater. Interfaces 2013, 5, 8093–8098. [Google Scholar] [CrossRef] [PubMed]
  5. Stępniowski, W.J.; Zasada, D.; Bojar, Z. First step of anodization influences the final nanopore arrangement in anodized alumina. Surf. Coat. Technol. 2011, 206, 1416–1422. [Google Scholar] [CrossRef]
  6. Stępniowski, W.J.; Nowak-Stępniowska, A.; Bojar, Z. Quantitative arrangement analysis of anodic alumina formed by short anodizations in oxalic acid. Mater. Charact. 2013, 78, 79–86. [Google Scholar] [CrossRef]
  7. Shingubara, S.; Morimoto, K.; Sakaue, H.; Takahagi, T. Self-Organization of a Porous Alumina Nanohole Array Using a Sulfuric/Oxalic Acid Mixture as Electrolyte. Electrochem. Solid-State Lett. 2004, 7, E15–E17. [Google Scholar] [CrossRef]
  8. Kashi, M.A.; Ramazani, A.; Rahmandoust, M.; Noormohammadi, M. The effect of pH and composition of sulfuric–oxalic acid mixture on the self-ordering configuration of high porosity alumina nanohole arrays. J. Phys. D Appl. Phys. 2007, 40, 4625–4630. [Google Scholar] [CrossRef]
  9. Zaraska, L.; Stępniowski, W.J.; Ciepiela, E.; Sulka, G.D. The effect of anodizing temperature on structural features and hexagonal arrangement of nanopores in alumina synthesized by two-step anodizing in oxalic acid. Thin Solid Films 2013, 534, 155–161. [Google Scholar] [CrossRef]
  10. Stępniowski, W.J.; Michalska-Domańska, M.; Norek, M.; Czujko, T. Fast Fourier transform based arrangement analysis of poorly organized alumina nanopores formed via self-organized anodization in chromic acid. Mater. Lett. 2014, 117, 69–73. [Google Scholar] [CrossRef]
  11. Stępniowski, W.J.; Nowak-Stępniowska, A.; Presz, A.; Czujko, T.; Varin, R.A. The effects of time and temperature on the arrangement of anodic aluminum oxide nanopores. Mater. Charact. 2014, 91, 1–9. [Google Scholar] [CrossRef]
  12. Chi, C.-S.; Lee, J.-H.; Kim, I.; Oh, H.-J. Effects of Microstructure of Aluminum Substrate on Ordered Nanopore Arrays in Anodic Alumina. J. Mater. Sci. Technol. 2015, 31, 751–758. [Google Scholar] [CrossRef]
  13. Sevgi, A.; Evrim, B.; Birgül, Y. The nanoporous anodic alumina oxide formed by two-step anodization. Thin Solid Films 2018, 648, 94–102. [Google Scholar]
  14. Roslyakov, I.V.; Gordeeva, E.O.; Napolskii, K.S. Role of Electrode Reaction Kinetics in Self-Ordering of Porous Anodic Alumina. Electrochim. Acta 2017, 241, 362–369. [Google Scholar] [CrossRef]
  15. Kondo, R.; Nakajima, D.; Kikuchi, T.; Natsui, S.; Suzuki, R.O. Superhydrophilic and superhydrophobic aluminum alloys fabricated via pyrophosphoric acid anodizing and fluorinated SAM modification. J. Alloys Compd. 2017, 725, 379–387. [Google Scholar] [CrossRef]
  16. Hashimoto, H.; Shigehara, Y.; Ono, S.; Asoh, H. Heat-induced structural transformations of anodic porous alumina formed in phosphoric acid. Microporous Mesoporous Mater. 2018, 265, 77–83. [Google Scholar] [CrossRef]
  17. Yu, M.; Zhang, W.; Zhang, S. Morphology evolution of porous anodic alumina in mixed H3PO4/NH4F electrolytes. Surf. Coat. Technol. 2018, 334, 500–508. [Google Scholar] [CrossRef]
  18. Akiya, S.; Kikuchi, T.; Natsui, S.; Sakaguchi, N.; Suzuki, R.O. Self-ordered Porous Alumina Fabricated via Phosphonic Acid Anodizing. Electrochim. Acta 2016, 190, 471–479. [Google Scholar] [CrossRef] [Green Version]
  19. Kikuchi, T.; Takenaga, A.; Natsui, S.; Suzuki, R.O. Advanced hard anodic alumina coatings via etidronic acid anodizing. Surf. Coat. Technol. 2017, 326, 72–78. [Google Scholar] [CrossRef]
  20. Takenaga, A.; Kikuchi, T.; Natsui, S.; Suzuki, R.O. Exploration for the Self-ordering of Porous Alumina Fabricated via Anodizing in Etidronic Acid. Electrochim. Acta 2016, 211, 515–523. [Google Scholar] [CrossRef] [Green Version]
  21. Cojocaru, C.S.; Padovani, J.M.; Wade, T.; Mandoli, C.; Jaskierowicz, G.; Wegrowe, J.E.; Fontcuberta i Morral, A.; Pribat, D. Conformal Anodic Oxidation of Aluminum Thin Films. Nano Lett. 2005, 5, 675–680. [Google Scholar] [CrossRef] [PubMed]
  22. Pashchanka, M.; Schneider, J.J. Self-Ordering Regimes of Porous Anodic Alumina Layers Formed in Highly Diluted Sulfuric Acid Electrolytes. J. Phys. Chem. C 2016, 120, 14590–14596. [Google Scholar] [CrossRef]
  23. Kondo, R.; Kikuchi, T.; Natsui, S.; Suzuki, R.O. Fabrication of self-ordered porous alumina via anodizing in sulfate solutions. Mater. Lett. 2016, 183, 285–289. [Google Scholar] [CrossRef] [Green Version]
  24. Kikuchi, T.; Yamamoto, T.; Natsui, S.; Suzuki, R.O. Fabrication of Anodic Porous Alumina by Squaric Acid Anodizing. Electrochim. Acta 2014, 123, 14–22. [Google Scholar] [CrossRef] [Green Version]
  25. Kikuchi, T.; Nakajima, D.; Kawashima, J. Fabrication of anodic porous alumina via anodizing in cyclicoxocarbon acids. Appl. Surf. Sci. 2014, 313, 276–285. [Google Scholar] [CrossRef] [Green Version]
  26. Kikuchi, T.; Nishinaga, O.; Natsui, S.; Suzuki, R.O. Self-Ordering Behavior of Anodic Porous Alumina via Selenic Acid Anodizing. Electrochim. Acta 2014, 137, 728–735. [Google Scholar] [CrossRef] [Green Version]
  27. Akiya, S.; Kikuchi, T.; Natsui, S.; Suzuki, R.O. Nanostructural characterization of large-scale porous alumina fabricated via anodizing in arsenic acid solution. Appl. Surf. Sci. 2017, 403, 652–661. [Google Scholar] [CrossRef] [Green Version]
  28. Su, Z.; Bühl, M.; Zhou, W. Dissociation of Water During Formation of Anodic Aluminum Oxide. J. Am. Chem. Soc. 2009, 131, 8697–8702. [Google Scholar] [CrossRef]
  29. Thompson, G.E.; Xu, Y.; Skeldon, P.; Shimizu, K.; Han, S.H.; Wood, G.C. Anodic oxidation of aluminium. Philos. Mag. B 1987, 55, 651–667. [Google Scholar] [CrossRef]
  30. Garcia-Vergara, S.J.; Molchan, I.S.; Zhou, F.; Habazaki, H.; Kowalski, D.; Skeldon, P.; Thompson, G.E. Incorporation and migration of phosphorus species within anodic films on an Al-W alloy. Surf. Interface Anal. 2011, 43, 893–902. [Google Scholar] [CrossRef]
  31. Xu, Y.; Thompson, G.; Wood, G. Direct observation of the cell material comprising porous anodic films formed on aluminium. Electrochim. Acta 1982, 27, 1623–1625. [Google Scholar] [CrossRef]
  32. Fleming, I. Molecular Orbitals and Organic Chemical Reactions; Reference Edition; John Wiley & Sons: Hoboken, NJ, USA, 2010; pp. 138–139. [Google Scholar]
  33. Blanck, S.; Loehlé, S.; Steinmann, S.N.; Michel, C. Adhesion of lubricant on aluminium through adsorption of additive head-groups on alumina: A DFT study. Tribol. Int. 2020, 145, 106140. [Google Scholar] [CrossRef]
  34. Delley, B. An all-electron numerical method for solving the local density functional for polyatomic molecules. J. Chem. Phys. 1990, 92, 508–517. [Google Scholar] [CrossRef]
Figure 1. The acid radicals connecting with the adsorbed H2O through O–H–O bond: (a) the (100), (b) the (110), (c) the (111) surfaces.
Figure 1. The acid radicals connecting with the adsorbed H2O through O–H–O bond: (a) the (100), (b) the (110), (c) the (111) surfaces.
Molecules 28 02427 g001aMolecules 28 02427 g001b
Figure 2. The acid radicals stripping off the two H of H2O by two steps on the anodic aluminum slabs: (a) the (100)+1, (b) the (110)+1, (c) the (111)+1 surfaces.
Figure 2. The acid radicals stripping off the two H of H2O by two steps on the anodic aluminum slabs: (a) the (100)+1, (b) the (110)+1, (c) the (111)+1 surfaces.
Molecules 28 02427 g002
Figure 3. The equations of acid radicals stripping off H in H2O on the anodic aluminum slabs.
Figure 3. The equations of acid radicals stripping off H in H2O on the anodic aluminum slabs.
Molecules 28 02427 g003
Figure 4. The energy levels and shapes of H in OH adsorbing on the anodic aluminum slabs: (1) (111)+1, (2) (110)+1, (3) (100)+1; the energy levels and shapes of HOMO of acid radicals: (4) HCO4, (5) H2PO4, (6) HSO4; the energy levels and shapes of H in H2O adsorbing on the anodic aluminum slabs: (7) (110)+1, (8) (100)+1, (9) (111)+1.
Figure 4. The energy levels and shapes of H in OH adsorbing on the anodic aluminum slabs: (1) (111)+1, (2) (110)+1, (3) (100)+1; the energy levels and shapes of HOMO of acid radicals: (4) HCO4, (5) H2PO4, (6) HSO4; the energy levels and shapes of H in H2O adsorbing on the anodic aluminum slabs: (7) (110)+1, (8) (100)+1, (9) (111)+1.
Molecules 28 02427 g004
Figure 5. The charges of the O atoms in acid radicals.
Figure 5. The charges of the O atoms in acid radicals.
Molecules 28 02427 g005
Figure 6. (a) The XRD peaks of aluminum foil. (b) The anodic polarization of aluminum in acid solutions.
Figure 6. (a) The XRD peaks of aluminum foil. (b) The anodic polarization of aluminum in acid solutions.
Molecules 28 02427 g006
Table 1. The adsorption energies (Eads/eV) of small molecules.
Table 1. The adsorption energies (Eads/eV) of small molecules.
SlabsH2OHC2O4H2PO4HSO4
(100)0−0.34−3.65−4.06−2.93
(110)0−0.47−3.39−3.28−3.08
(111)0−0.36−2.78−3.70−3.18
(100)+1−0.50−4.62−5.16−3.69
(110)+1−0.53−3.90−3.67−3.75
(111)+1−0.56−3.99−5.22−3.80
Table 2. The Erep (eV) values of acid radicals replacing H2O.
Table 2. The Erep (eV) values of acid radicals replacing H2O.
SlabsHC2O4H2PO4HSO4
(100)0−3.31−3.72−2.59
(110)0−2.92−2.81−2.61
(111)0−2.42−3.33−2.82
(100)+1−4.11−4.65−3.18
(110)+1−3.37−3.14−3.22
(111)+1−3.42−4.65−3.23
Table 3. The Ebon (eV) values of acid radicals bonding with the H of adsorbed H2O.
Table 3. The Ebon (eV) values of acid radicals bonding with the H of adsorbed H2O.
SlabsHC2O4H2PO4HSO4
(100)0−2.23−1.41−0.52
(110)0−1.70−0.83−0.04
(111)0−2.49−1.73−0.80
Table 4. The Estr (eV) values of acid radicals stripping off one of the H in H2O. The a, b, c, d, e and f correspond to the labels of reactions in Figure 3. Subscript “1” is for the direction of reactions in Figure 3.
Table 4. The Estr (eV) values of acid radicals stripping off one of the H in H2O. The a, b, c, d, e and f correspond to the labels of reactions in Figure 3. Subscript “1” is for the direction of reactions in Figure 3.
Slabsa1b1a1 + b1c1d1c1 + d1e1f1e1 + f1
(100)+1−3.21−2.54−5.75−3.24−2.57−5.81−2.57−1.91−4.48
(110)+1−2.33−2.15−4.48−2.42−2.24−4.66−1.76−1.58−3.34
(111)+1−2.97−3.37−6.34−3.08−3.48−6.56−2.49−2.89−5.38
Table 5. The charges of the two H of adsorbed H2O; the charges of the H of adsorbed OH.
Table 5. The charges of the two H of adsorbed H2O; the charges of the H of adsorbed OH.
SlabsHHSlabsH
(100)0-H2O0.2740.274(100)0-OH0.261
(110)0-H2O0.2670.267(110)0-OH0.260
(111)0-H2O0.2820.282(111)0-OH0.298
(100)+1-H2O0.3220.322(100)+1-OH0.323
(110)+1-H2O0.3110.311(110)+1-OH0.312
(111)+1-H2O0.3280.328(111)+1-OH0.343
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Zhang, Z.; Kang, J.; Li, X.; Li, P.; Du, Y.; Qin, Y.; Li, N.; Li, J. The Effects of Acid and Water in the Formation of Anodic Alumina: DFT and Experiment Study. Molecules 2023, 28, 2427. https://doi.org/10.3390/molecules28062427

AMA Style

Zhang Z, Kang J, Li X, Li P, Du Y, Qin Y, Li N, Li J. The Effects of Acid and Water in the Formation of Anodic Alumina: DFT and Experiment Study. Molecules. 2023; 28(6):2427. https://doi.org/10.3390/molecules28062427

Chicago/Turabian Style

Zhang, Zhengwei, Jin Kang, Xiaodong Li, Ping Li, Yali Du, Yufan Qin, Ningyi Li, and Jiebin Li. 2023. "The Effects of Acid and Water in the Formation of Anodic Alumina: DFT and Experiment Study" Molecules 28, no. 6: 2427. https://doi.org/10.3390/molecules28062427

APA Style

Zhang, Z., Kang, J., Li, X., Li, P., Du, Y., Qin, Y., Li, N., & Li, J. (2023). The Effects of Acid and Water in the Formation of Anodic Alumina: DFT and Experiment Study. Molecules, 28(6), 2427. https://doi.org/10.3390/molecules28062427

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