92 research outputs found

    The Multisensor Array Based on Grown-On-Chip Zinc Oxide Nanorod Network for Selective Discrimination of Alcohol Vapors at Sub-ppm Range

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    We discuss the fabrication of gas-analytical multisensor arrays based on ZnO nanorods grown via a hydrothermal route directly on a multielectrode chip. The protocol to deposit the nanorods over the chip includes the primary formation of ZnO nano-clusters over the surface and secondly the oxide hydrothermal growth in a solution that facilitates the appearance of ZnO nanorods in the high aspect ratio which comprise a network. We have tested the proof-of-concept prototype of the ZnO nanorod network-based chip heated up to 400 Β°C versus three alcohol vapors, ethanol, isopropanol and butanol, at approx. 0.2–5 ppm concentrations when mixed with dry air. The results indicate that the developed chip is highly sensitive to these analytes with a detection limit down to the sub-ppm range. Due to the pristine differences in ZnO nanorod network density the chip yields a vector signal which enables the discrimination of various alcohols at a reasonable degree via processing by linear discriminant analysis even at a sub-ppm concentration range suitable for practical applications

    Fractal analysis of the AFM-images of Cu–Ga–Se films, prepared by chemical bath deposition

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    Π‘ использованиСм Π°Ρ‚ΠΎΠΌΠ½ΠΎ-силовой микроскопии исслСдована морфология повСрхности Ρ‚ΠΎΠ½ΠΊΠΈΡ… ΠΏΠ»Π΅Π½ΠΎΠΊ Cu–Ga–Se, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… совмСстным гидрохимичСским осаТдСниСм сСлСнидов ΠΌΠ΅Π΄ΠΈ (I) Cu2Se ΠΈ галлия Ga2Se3. Π‘ ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ Ρ„Ρ€Π°ΠΊΡ‚Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° АБМ-ΠΈΠ·ΠΎΠ±Ρ€Π°ΠΆΠ΅Π½ΠΈΠΉ установлСна Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ‚ΡŒ ΠΌΠ΅ΠΆΠ΄Ρƒ условиями осаТдСния Ρ‚ΠΎΠ½ΠΊΠΈΡ… ΠΏΠ»Π΅Π½ΠΎΠΊ Cu–Ga–Se ΠΈ ΠΈΡ… Ρ„Ρ€Π°ΠΊΡ‚Π°Π»ΡŒΠ½ΠΎΠΉ Ρ€Π°Π·ΠΌΠ΅Ρ€Π½ΠΎΡΡ‚ΡŒΡŽ, рассчитанной ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ подсчСта ΠΊΡƒΠ±ΠΎΠ² ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ триангуляции. Π’Π°ΠΊΠΆΠ΅ ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌ формирования ΠΈ роста ΠΏΠ»Π΅Π½ΠΎΠΊ ΠΏΡ€ΠΈ гидрохимичСском осаТдСнии дисСлСнида ΠΌΠ΅Π΄ΠΈ (I) ΠΈ галлия.The surface morphology of Cu–Ga–Se thin films prepared by chemical bath deposition of copper (I) Cu2Se and gallium selenides Ga2Se3 was investigated by means of an atomic-force microscopy. The dependence between the conditions of the deposition of Cu–Ga–Se thin films and their fractal dimension, calculated by counting cubes and by triangulation, was defined by means of fractal analysis. A mechanism for the formation and growth of films at chemical bath deposition of copper (I) and gallium selenides was proposed well as.ΠŸΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΠ° развития Π£Ρ€Π€Π£ Π½Π° 2013 Π³ΠΎΠ΄ (ΠΏ.1.2.2.3

    ΠœΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ Ρ‚Ρ€Π΅Ρ…ΠΌΠ΅Ρ€Π½Ρ‹Ρ… пористых иСрархичСских ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ², ΠΎΡ€Π³Π°Π½ΠΈΠ·ΠΎΠ²Π°Π½Π½Ρ‹Ρ… посрСдством самосборки наносфСр

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    The article considers possibilities of using modeling fo r the development of two promising areas of modernΒ nanomaterials, i. e.Β  materials with a hierarchy of pores organized hierarchical self- assembly and hierarchical structuresΒ with nanoporous elements. TheΒ  pore size of hierarchical structures was estimated by means of quasi- two-dimensional projectionΒ of three-dimensional deterministic fractal Julien aggregate. Three-dimensional modeling of hierarchicalΒ  structuresΒ organized by means of nanosphere self-assembly was conducted in the Autodesk 3ds Max environment. The article providesΒ analysis of dependences of porosity, density, specificΒ  surface area of fractal structures on the size of aggregates (withΒ theΒ  appearance of new pore levels of hierarchical materials),Β  dependences of the porosity change in the case of replacementΒ of primary identical spherical particles on porous spheres.РассмотрСны возмоТности примСнСния модСлирования для развития Π΄Π²ΡƒΡ… пСрспСктивных направлСний соврСмСнного наноматСриаловСдСния: ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² с ΠΈΠ΅Ρ€Π°Ρ€Ρ…ΠΈΠ΅ΠΉ ΠΏΠΎΡ€, собранных посрСдством иСрархичСской самосборки, Π° Ρ‚Π°ΠΊΠΆΠ΅ иСрархичСских структур ΠΈΠ· нанопористых  элСмСнтов. Π‘ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌΒ ΠΊΠ²Π°Π·ΠΈΠ΄Π²ΡƒΠΌΠ΅Ρ€Π½ΠΎΠΉ ΠΏΡ€ΠΎΠ΅ΠΊΡ†ΠΈΠΈ Ρ‚Ρ€Π΅Ρ…ΠΌΠ΅Ρ€Π½ΠΎΠ³ΠΎ Π΄Π΅Ρ‚Π΅Ρ€ΠΌΠΈΠ½ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎΒ  Ρ„Ρ€Π°ΠΊΡ‚Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ Π°Π³Ρ€Π΅Π³Π°Ρ‚Π° Π–ΡŽΠ»ΡŒΠ΅Π½Π°Β ΠΎΡ†Π΅Π½Π΅Π½ Ρ€Π°Π·ΠΌΠ΅Ρ€ ΠΏΠΎΡ€ Π² иСрархичСских структурах. Π’Ρ€Π΅Ρ…ΠΌΠ΅Ρ€Π½ΠΎΠ΅Β  ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ иСрархичСских структур, организованных посрСдством самосборки наносфСр,Β  ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Π² срСдС Autodesk 3ds Max. ΠŸΡ€ΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡ€ΠΎΠ²Π°Π½Ρ‹Β Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ‚ΠΈ пористости, плотности,Β  ΡƒΠ΄Π΅Π»ΡŒΠ½ΠΎΠΉ ΠΏΠ»ΠΎΡ‰Π°Π΄ΠΈ повСрхности Ρ„Ρ€Π°ΠΊΡ‚Π°Π»ΡŒΠ½Ρ‹Ρ… структур ΠΎΡ‚ Ρ€Π°Π·ΠΌΠ΅Ρ€ΠΎΠ²Β Π°Π³Ρ€Π΅Π³Π°Ρ‚ΠΎΠ² (ΠΏΡ€ΠΈΒ  Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΠΈ Π½ΠΎΠ²Ρ‹Ρ… ΡƒΡ€ΠΎΠ²Π½Π΅ΠΉ ΠΏΠΎΡ€ иСрархичСских ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ²), Π° Ρ‚Π°ΠΊΠΆΠ΅ измСнСния пористости ΠΏΡ€ΠΈ Π·Π°ΠΌΠ΅Π½Π΅ ΠΏΠ΅Ρ€Π²ΠΈΡ‡Π½Ρ‹Ρ… ΠΈΠ΄Π΅Π½Ρ‚ΠΈΡ‡Π½Ρ‹Ρ… сфСричСских частиц Π½Π° пористыС сфСры

    Photoluminescence and its damping kinetics of nanoporous alumina m embranes formed in solutions of various carboxylic acids

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    The article is devoted to the study of the photoluminescence of carbon-containing anodic alumina obtained in various electrolytes based on carboxylic (tartaric and oxalic) acids. We studied the emission and excitation spectra of luminescence, as well as the PL decay of nanostructured anodic alumina membranes. It is shown that such membranes exhibit photoluminescence (excitation wavelength 330 nm) in the wavelength range 350-600 nm with a maximum at 460 nm. They have two PL centers with maxima at 440 and 490 nm and lifetimes of 0.2 and 4.0 ns, respectively. It is shown that the PL peak at 440 nm can be related to the emission of COO– - ions, and the peak at 490 nm can be related to the PL of defects in partially oxidized amorphous carbon

    The sorption of water molecules in the pores of anodic alumina films during aluminum anodizing in oxalic acid

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    The thermogravimetric analysis of membranes of anodic aluminum oxide (AAO) was carried out. The results showed that in the process of anodic growth, water molecules are adsorbed in the pores of Al2O3, the amount of which is determined by the anodizing voltage of aluminum. The relationship is revealed and the graphs of the relationship between anodizing voltage, annealing temperature, and weight loss of nanostructured membranes of AAO are presented. It has been established that the adsorption of water molecules on the surface of AAO is explained by the presence of a surface charge, which disappears after annealing at 200–300 Β°C. An increase in the amount of adsorbed water with an increase in the anodizing voltage from 20 to 40β€…V indicates a decrease in the surface charge density

    Results from the Indo-USSR ozonesonde intercomparison experiment

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    A total of seventeen vertical profiles of ozone were obtained during an Indo-USSR collaborative experiment on ozonesonde intercomparison conducted at Thumba during March 1983. The vertical distribution of ozone was measured using rocket-borne, balloon-borne as well as ground-based instruments. Four different rocket ozonesondes from India and USSR and the balloon ozonesonde were used to makein situ observations of ozone concentrations in addition to the Dobson spectrophotometric observations of total ozone and Umkehr. The rocket and the balloon launchings were effected in three salvos and measurements were made at different times of the day as well as during night. The results of all these measurements are used to obtain a mean ozone vertical distribution over Thumba foT the spring equinoxial period. The mean profile shows the maximum ozone concentration at 27 km with a value of (3.86Β±0-52)Γ—1012 molecules per cc. Comparison of this mean profile with available satellite data for the equatorial regions shows that, in general, the Thumba values are lower by 10–15% at altitudes below 40 km and larger at altitudes above 50 km compared to the satellite results. The data also show evidence for a day-to-day variability and a possible day-to-night variability in the ozone vertical distribution with the night-time values higher than the daytime values at all altitudes above 35 km and the difference is found to increase with the increasing altitude

    ИсслСдованиС Ρ‚Π΅ΠΏΠ»ΠΎΠ²Ρ‹Ρ… характСристик Π½Π°Π³Ρ€Π΅Π²Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ элСмСнта ΠΈΠ· алюминия с нанопористым оксидом алюминия

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    In this work, we studied the thermal characteristics of flat heaters made of aluminum with a strip heating element in the form of carbon fiber. In order to provide the necessary insulation of the heating element from the metal base, a layer of porous anodic aluminum oxide with a thickness of 20 ΞΌm was formed on the aluminum surface. The ends of the carbon fiber filament were metallized with a layer of copper for subsequent soldering during the assembly of the electric heater. The carbon fiber filament of electric heater had an electrical resistance of 60 Ohms. Studies of the propagation of heat fluxes in the volume of a board made of aluminum with nanoporous aluminum oxide were carried out using thermal imaging measurements. The paper presents the dependence of temperature changes on the surface of the lid of a heating element made of aluminum and on the opposite side β€” heat transfer side with heating time. The results showed that the heat generated by a linear heating element of carbon fiber, quickly distributed throughout the entire volume of the aluminum plate of the heating element. This indicates a high thermal conductivity of the aluminum base of the heater, the parameters of which allow to achieve the required thermal characteristics of the heater.Одной ΠΈΠ· Π°ΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½Ρ‹Ρ… Π·Π°Π΄Π°Ρ‡ Π² сфСрС стационарного отоплСния, Π½Π° Ρ€Π΅ΡˆΠ΅Π½ΠΈΠ΅ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΉ Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½Ρ‹ усилия многочислСнных Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Ρ‡ΠΈΠΊΠΎΠ², являСтся экономия элСктричСской энСргии. ΠΠ°Π³Ρ€Π΅Π²Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ систСмы ΠΌΠΎΠ³ΡƒΡ‚ ΠΈΠΌΠ΅Ρ‚ΡŒ самыС Ρ€Π°Π·Π½ΠΎΠΎΠ±Ρ€Π°Π·Π½Ρ‹Π΅ конструкции, Π½ΠΎ ΡΡƒΡ‰Π΅ΡΡ‚Π²ΡƒΡŽΡ‚ основныС трСбования ΠΊ ΠΈΡ… Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠ΅, Π° ΠΈΠΌΠ΅Π½Π½ΠΎ: обСспСчСниС высокой надСТности ΠΏΡ€ΠΈ эксплуатации, ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡ‡Π½ΠΎΡΡ‚ΡŒ, ΡƒΡΡ‚ΠΎΠΉΡ‡ΠΈΠ²ΠΎΡΡ‚ΡŒ ΠΊ внСшним воздСйствиям ΠΈ ΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½ΠΎΡΡ‚ΡŒ элСктричСских характСристик. Основной элСмСнт любого Π½Π°Π³Ρ€Π΅Π²Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ устройства β€” Π½Π°Π³Ρ€Π΅Π²Π°Ρ‚Π΅Π»ΡŒ. Π’ настоящСС врСмя плоскиС рСзистивныС Π½Π°Π³Ρ€Π΅Π²Π°Ρ‚Π΅Π»ΠΈ нашли ΡˆΠΈΡ€ΠΎΠΊΠΈΠΉ спСктр примСнСния Π² Π½Π°Π³Ρ€Π΅Π²Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… устройствах, ΠΏΡ€Π΅Π΄Π½Π°Π·Π½Π°Ρ‡Π΅Π½Π½Ρ‹Ρ… для формирования Π·Π΄ΠΎΡ€ΠΎΠ²ΠΎΠ³ΠΎ ΠΌΠΈΠΊΡ€ΠΎΠΊΠ»ΠΈΠΌΠ°Ρ‚Π° Π² помСщСниях, поддСрТания Π·Π°Π΄Π°Π½Π½Ρ‹Ρ… ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² Π² Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… тСхнологичСских процСссах, Π² систСмах антиоблСдСнСния, Π² сСльском хозяйствС ΠΈ Π² ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½ΠΎΡΡ‚ΠΈ. Π˜ΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ‹ Ρ‚Π΅ΠΏΠ»ΠΎΠ²Ρ‹Π΅ характСристики плоских Π½Π°Π³Ρ€Π΅Π²Π°Ρ‚Π΅Π»Π΅ΠΉ, ΠΈΠ·Π³ΠΎΡ‚ΠΎΠ²Π»Π΅Π½Π½Ρ‹Ρ… ΠΈΠ· алюминия, с Π»Π΅Π½Ρ‚ΠΎΡ‡Π½Ρ‹ΠΌ элСмСнтом Π½Π°Π³Ρ€Π΅Π²Π° Π² Π²ΠΈΠ΄Π΅ ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π²ΠΎΠ»ΠΎΠΊΠ½Π°. Π‘ Ρ†Π΅Π»ΡŒΡŽ обСспСчСния Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΠΉ изоляции Π½Π°Π³Ρ€Π΅Π²Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ элСмСнта ΠΎΡ‚ мСталличСского основания Π½Π° повСрхности алюминия Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π»ΠΈ слой пористого Π°Π½ΠΎΠ΄Π½ΠΎΠ³ΠΎ оксида алюминия Ρ‚ΠΎΠ»Ρ‰ΠΈΠ½ΠΎΠΉ 20 ΠΌΠΊΠΌ. ΠšΠΎΠ½Ρ†Ρ‹ Π½ΠΈΡ‚ΠΈ ΠΈΠ· ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π²ΠΎΠ»ΠΎΠΊΠ½Π° ΠΌΠ΅Ρ‚Π°Π»Π»ΠΈΠ·ΠΈΡ€ΠΎΠ²Π°Π»ΠΈ слоСм ΠΌΠ΅Π΄ΠΈ для ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π΅ΠΉ ΠΏΠ°ΠΉΠΊΠΈ Π² процСссС сборки элСктричСского нагрСватСля. ЭлСктричСскоС сопротивлСниС нагрСватСля с Π½ΠΈΡ‚ΡŒΡŽ ΠΈΠ· ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π²ΠΎΠ»ΠΎΠΊΠ½Π° составляло 60 Ом. ИсслСдования распространСния Ρ‚Π΅ΠΏΠ»ΠΎΠ²Ρ‹Ρ… ΠΏΠΎΡ‚ΠΎΠΊΠΎΠ² Π² объСмС ΠΏΠ»Π°Ρ‚Ρ‹ ΠΈΠ· алюминия с нанопористым оксидом алюминия ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ с использованиСм Ρ‚Π΅ΠΏΠ»ΠΎΠ²ΠΈΠ·ΠΈΠΎΠ½Π½Ρ‹Ρ… ΠΈΠ·ΠΌΠ΅Ρ€Π΅Π½ΠΈΠΉ. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Π° Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ‚ΡŒ измСнСния Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ Π½Π° повСрхности ΠΊΡ€Ρ‹ΡˆΠΊΠΈ Π½Π°Π³Ρ€Π΅Π²Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ элСмСнта ΠΈΠ· алюминия ΠΈ Π½Π° ΠΏΡ€ΠΎΡ‚ΠΈΠ²ΠΎΠΏΠΎΠ»ΠΎΠΆΠ½ΠΎΠΉ Ρ‚Π΅ΠΏΠ»ΠΎΠΎΡ‚Π΄Π°ΡŽΡ‰Π΅ΠΉ сторонС ΠΎΡ‚ Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ Π½Π°Π³Ρ€Π΅Π²Π°. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, Ρ‡Ρ‚ΠΎ Ρ‚Π΅ΠΏΠ»ΠΎ, Π³Π΅Π½Π΅Ρ€ΠΈΡ€ΡƒΠ΅ΠΌΠΎΠ΅ Π»ΠΈΠ½Π΅ΠΉΠ½Ρ‹ΠΌ Π½Π°Π³Ρ€Π΅Π²Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹ΠΌ элСмСнтом ΠΈΠ· ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π½ΠΎΠΉ Π½ΠΈΡ‚ΠΈ, быстро пСрСраспрСдСлятся ΠΏΠΎ всСму ΠΎΠ±ΡŠΠ΅ΠΌΡƒ алюминиСвой пластины с Π½Π°Π³Ρ€Π΅Π²Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹ΠΌ элСмСнтом. Π­Ρ‚ΠΎ ΡΠ²ΠΈΠ΄Π΅Ρ‚Π΅Π»ΡŒΡΡ‚Π²ΡƒΠ΅Ρ‚ ΠΎ высокой тСплопроводности алюминиСвой основы нагрСватСля, ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΉ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΡ‚ΡŒ достиТСниС Ρ‚Ρ€Π΅Π±ΡƒΠ΅ΠΌΡ‹Ρ… Ρ‚Π΅ΠΏΠ»ΠΎΠ²Ρ‹Ρ… характСристик нагрСватСля

    Influence of Electrolyte Temperature on the Formation of the Morphology of the Porous Structure of Anodic Aluminum Oxide

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    The results of research on anodizing thin aluminum films 100 nm thick on SiO2–Si plates at 30 V in a 0.3 M aqueous solution of oxalic acid are presented. The effect of the electrolyte temperature on the morphology of porous anodic aluminum oxide (PAAO) films is studied. The pore diameter and interpore distance are determined by the computer analysis of the SEM images of the morphology of the anode films using the ImageJ software. The data obtained show that the pore diameter does not depend on the temperature of the electrolyte and the time of the process, but is determined only by the anodizing voltage. In the electrolyte temperature range of 5 to 40Β°C, the pore diameter of the PAAO films is 20 Β± 0.5 nm, and the interpore distance is 77.7 nm. The research results indicate that a change in the temperature of the electrolyte, in contrast to the anodizing voltage, affects only the growth rate of the anode film, and not its porous morphology
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