228 research outputs found

    High surface area activated carbon prepared from wood-based spent mushroom substrate for supercapacitors and water treatment

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    Edible white-rot fungi are commonly cultivated on wood-based substrates and selectively degrade lignin to a larger extent during their growth. Spent mushroom substrate (SMS) is produced in huge amounts by the mushroom industry and today there is a lack of proven methods to valorize this kind of biomass waste, which in most cases is landfilled or used as fuel. This study demonstrates that birch wood-based SMS from the cultivation of oyster mushrooms can be converted into high-quality activated carbon (AC) with an extremely high surface area of about 3000 m2 /g. These activated carbons showed good performance when used in electrodes for supercapacitors, with energy storage parameters nearly identical to AC produced from high-quality virgin birch wood. Moreover, AC produced from SMS showed high potential as an adsorbent for cleaning reactive orange-16 azo dye from aqueous solutions as well as contaminants from synthetic effluents and from real sewage water. The kinetics of adsorption were well represented by the Avrami fractional order model and isotherms of adsorption by the Liu model. The theoretical maximum reactive orange-16 adsorption capacities were approximately 519 mg/g (SMS-based carbon) and 553 mg/g (virgin birch-based carbon). The removal of contaminants from synthetic effluents made of different dyes and inorganic compounds was around 95% and 83% depending on the effluent composition. The removal of contaminants from raw sewage water was around 84%, and from treated sewage water was around 68%. Overall, the results showed that activated carbon prepared from waste generated during cultivation of white-rot fungi is as good as activated carbon prepared from high-quality virgin wood

    Minimax approximation of a complex-valued function modulus by means of linear programming

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    Β© 2016 IEEE.The problem of approximating the complex-valued function modulus using a minimax criterion is of interest in many technical applications, such as standard process controlling systems with limiting the transient oscillations, low-side-lobe antenna arrays, or multiplexing devices having a deep channel isolation. The paper introduces approximate formulas to compute the absolute value of a complex number based on piecewise linear inequalities, thanks to which the approximation problem may be reduced to the minimax linear programming problem allowing the use of standard application packages. Computational experiments, the results of which are discussed, have proven the efficiency of the proposed computing algorithm combining high speed and good approximation accuracy

    Covalent Organic Framework (COF-1) under High Pressure

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    COF-1 has a structure with rigid 2D layers composed of benzene and B3O3 rings and weak van der Waals bonding between the layers. The as-synthesized COF-1 structure contains pores occupied by solvent molecules. A high surface area empty-pore structure is obtained after vacuum annealing. High-pressure XRD and Raman experiments with mesitylene-filled (COF-1-M) and empty-pore COF-1 demonstrate partial amorphization and collapse of the framework structure above 12–15 GPa. The ambient pressure structure of COF-1-M can be reversibly recovered after compression up to 10–15 GPa. Remarkable stability of highly porous COF-1 structure at pressures at least up to 10 GPa is found even for the empty-pore structure. The bulk modulus of the COF-1 structure (11.2(5) GPa) and linear incompressibilities (k[100]=111(5) GPa, k[001]=15.0(5) GPa) were evaluated from the analysis of XRD data and cross-checked against first-principles calculations.\ua0\ua9 2019 Wiley-VCH Verlag GmbH & Co. KGaA, Weinhei

    Hydrogen storage in high surface area graphene scaffolds

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    Using an optimized KOH activation procedure we prepared highly porous graphene scaffoldmaterials with SSA values up to 3400mΒ² g⁻¹ and a pore volume up to 2.2 cmΒ³ gΛ‰ΒΉ, which are among the highest for carbon materials. Hydrogen uptake of activated graphene samples was evaluated in a broad temperature interval (77–296 K). After additional activation by hydrogen annealing the maximal excess H2 uptake of 7.5 wt% was obtained at 77 K. A hydrogen storage value as high as 4 wt% was observed already at 193 K (120 bar Hβ‚‚), a temperature of solid COβ‚‚, which can be easily maintained using common industrial refrigeration methods

    Activated carbons with extremely high surface area produced from cones, bark and wood using the same procedure

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    Activated carbons have been previously produced from a huge variety of biomaterials often reporting advantages of using certain precursors. Here we used pine cones, spruce cones, larch cones and a pine bark/wood chip mixture to produce activated carbons in order to verify the influence of the precursor on properties of the final materials. The biochars were converted into activated carbons with extremely high BET surface area up to similar to 3500 m(2) g(-1) (among the highest reported) using identical carbonization and KOH activation procedures. The activated carbons produced from all precursors demonstrated similar specific surface area (SSA), pore size distribution and performance to electrodes in supercapacitors. Activated carbons produced from wood waste appeared to be also very similar to "activated graphene" prepared by the same KOH procedure. Hydrogen sorption of AC follows expected uptake vs. SSA trends and energy storage parameters of supercapacitor electrodes prepared from AC are very similar for all tested precursors. It can be concluded that the type of precursor (biomaterial or reduced graphene oxide) has smaller importance for producing high surface area activated carbons compared to details of carbonization and activation. Nearly all kinds of wood waste provided by the forest industry can possibly be converted into high quality AC suitable for preparation of electrode materials

    О пСрспСктивС создания элСмСнтов памяти Π½Π° основС наночастиц крСмния

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    Phase-change memory is based on a change in the optical, electrical, or other properties of a substance during a phase transition, for example, transition from the amorphous to the crystalline state. Already realized and potential applications of such memory are associated with the use for this purpose of multicomponent alloys based on metals, semiconductors. However, single-component nanoparticles, including Si ones, are also of interest in view of the prospects for their use as nanoscale memory units. In particular, possibility of creating such memory units is confirmed by the fact that the bulk phase of the amorphous silicon has an optical absorption coefficient which is by an order of magnitude greater than that of the crystalline, although, it is difficult to release this effect for an individual nanoparticle whose size does not exceed the wavelength of light. In this work, using molecular dynamics (MD) and the Stillinger-Weber potential, we studied the laws of melting and conditions of crystallization for silicon nanoparticles containing up to 100,000 atoms. It has been shown that upon cooling a silicon nanodroplet at a rate of 0.2 TK/s and higher rates, its transition into the amorphous state takes place, whereas single-component metal nanodroplets crystallize even at cooling rates of 1 TK/s. Upon subsequent heating of amorphous silicon nanoparticles containing more than 50,000 atoms, they crystallize in the definite temperature range 1300β€”1400 K. It is concluded that it is principally possible to create memory units based on the above phase transitions. The transition of a nanoparticle to the amorphous state is achieved by its melting and subsequent cooling to the room temperature at a rate of 0.2 TK/s, and switching to the crystalline state is achieved by heating it to 1300β€”1400 K at a rate of 0.2 TK/s and subsequent cooling. On the basis of results of MD experiments, a conclusion is made that there exist a minimal size of silicon nanoparticles, for which producing memory units based on the change of the phase state, is not possible. It was found that for the temperature change rate of 0.2 TK/s, the minimal size in question 12.4 nm that corresponds to 50,000 atoms.ΠŸΠ°ΠΌΡΡ‚ΡŒ, связанная с ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ Ρ„Π°Π·ΠΎΠ²ΠΎΠ³ΠΎ состояния (phase–change memory), основана Π½Π° ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΈ оптичСских, элСктричСских ΠΈΠ»ΠΈ ΠΈΠ½Ρ‹Ρ… свойств вСщСства ΠΏΡ€ΠΈ Ρ„Π°Π·ΠΎΠ²ΠΎΠΌ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π΅, Π½Π°ΠΏΡ€ΠΈΠΌΠ΅Ρ€ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π΅ ΠΈΠ· Π°ΠΌΠΎΡ€Ρ„Π½ΠΎΠ³ΠΎ состояния Π² кристалличСскоС. На сСгодняшний дСнь ΡƒΠΆΠ΅ Ρ€Π΅Π°Π»ΠΈΠ·ΠΎΠ²Π°Π½Π½Ρ‹Π΅ ΠΈ ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Π΅ примСнСния Ρ‚Π°ΠΊΠΎΠΉ памяти связаны Π² ΠΏΠ΅Ρ€Π²ΡƒΡŽ ΠΎΡ‡Π΅Ρ€Π΅Π΄ΡŒ с использованиСм ΠΌΠ½ΠΎΠ³ΠΎΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½Ρ‹Ρ… сплавов Π½Π° основС химичСских элСмСнтов, относящихся ΠΊ ΠΌΠ΅Ρ‚Π°Π»Π»Π°ΠΌ ΠΈ ΠΏΠΎΠ»ΡƒΠΏΡ€ΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠ°ΠΌ. Однако ΠΎΠ΄Π½ΠΎΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½Ρ‹Π΅ наночастицы, Π²ΠΊΠ»ΡŽΡ‡Π°Ρ наночастицы Si, Ρ‚Π°ΠΊΠΆΠ΅ ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²Π»ΡΡŽΡ‚ интСрСс Π² качСствС пСрспСктивных Π½Π°Π½ΠΎΡ€Π°Π·ΠΌΠ΅Ρ€Π½Ρ‹Ρ… элСмСнтов памяти. Π’ частности, Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ создания Ρ‚Π°ΠΊΠΈΡ… элСмСнтов памяти подтвСрТдаСтся Ρ‚Π΅ΠΌ, Ρ‡Ρ‚ΠΎ Ρƒ объСмной Ρ„Π°Π·Ρ‹ Π°ΠΌΠΎΡ€Ρ„Π½ΠΎΠ³ΠΎ крСмния Π·Π½Π°Ρ‡Π΅Π½ΠΈΠ΅ коэффициСнта оптичСского поглощСния Π½Π° порядок большС, Ρ‡Π΅ΠΌ Ρƒ кристалличСского. РазумССтся, этот эффСкт Π·Π°Ρ‚Ρ€ΡƒΠ΄Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ Ρ€Π΅Π°Π»ΠΈΠ·ΠΎΠ²Π°Ρ‚ΡŒ для ΠΎΡ‚Π΄Π΅Π»ΡŒΠ½ΠΎΠΉ наночастицы, Ρ€Π°Π·ΠΌΠ΅Ρ€ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΉ Π½Π΅ ΠΏΡ€Π΅Π²Ρ‹ΡˆΠ°Π΅Ρ‚ Π΄Π»ΠΈΠ½Ρƒ Π²ΠΎΠ»Π½Ρ‹ свСта. Π’ Π΄Π°Π½Π½ΠΎΠΉ Ρ€Π°Π±ΠΎΡ‚Π΅ с использованиСм молСкулярной Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ (ΠœΠ”) ΠΈ ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»Π° Π‘Ρ‚ΠΈΠ»Π»ΠΈΠ½Π΄ΠΆΠ΅Ρ€Π°β€”Π’Π΅Π±Π΅Ρ€Π° исслСдованы закономСрности плавлСния ΠΈ условия кристаллизации наночастиц крСмния, содСрТащих Π΄ΠΎ 105 Π°Ρ‚ΠΎΠΌΠΎΠ². Показано, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈ ΠΎΡ…Π»Π°ΠΆΠ΄Π΅Π½ΠΈΠΈ нанокапСль крСмния со ΡΠΊΠΎΡ€ΠΎΡΡ‚ΡŒΡŽ 0,2 ВК/с ΠΈ Π²Ρ‹ΡˆΠ΅ ΠΈΠΌΠ΅Π΅Ρ‚ мСсто ΠΈΡ… ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄ Π² Π°ΠΌΠΎΡ€Ρ„Π½ΠΎΠ΅ состояниС, Ρ‚ΠΎΠ³Π΄Π° ΠΊΠ°ΠΊ ΠΎΠ΄Π½ΠΎΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½Ρ‹Π΅ мСталличСскиС Π½Π°Π½ΠΎΠΊΠ°ΠΏΠ»ΠΈ ΠΊΡ€ΠΈΡΡ‚Π°Π»Π»ΠΈΠ·ΡƒΡŽΡ‚ΡΡ Π² ΠœΠ”-экспСримСнтах Π΄Π°ΠΆΠ΅ ΠΏΡ€ΠΈ скоростях охлаТдСния 1 ВК/с. ΠŸΡ€ΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π΅ΠΌ Π½Π°Π³Ρ€Π΅Π²Π΅ Π°ΠΌΠΎΡ€Ρ„Π½Ρ‹Ρ… наночастиц крСмния, содСрТащих Π±ΠΎΠ»Π΅Π΅ 5β€…βˆ™β€…104 Π°Ρ‚ΠΎΠΌΠΎΠ², происходит ΠΈΡ… кристаллизация Π² ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Π½ΠΎΠΌ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠΌ ΠΈΠ½Ρ‚Π΅Ρ€Π²Π°Π»Π΅ ΠΎΡ‚ 1300 Π΄ΠΎ 1400 К. Π‘Π΄Π΅Π»Π°Π½ Π²Ρ‹Π²ΠΎΠ΄ ΠΎ ΠΏΡ€ΠΈΠ½Ρ†ΠΈΠΏΠΈΠ°Π»ΡŒΠ½ΠΎΠΉ возмоТности создания элСмСнтов памяти, основанных Π½Π° Π΄Π°Π½Π½Ρ‹Ρ… Ρ„Π°Π·ΠΎΠ²Ρ‹Ρ… ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π°Ρ…. ΠŸΠ΅Ρ€Π΅Ρ…ΠΎΠ΄ наночастицы Π² Π°ΠΌΠΎΡ€Ρ„Π½ΠΎΠ΅ состояниС достигаСтся ΠΏΡƒΡ‚Π΅ΠΌ Π΅Π΅ плавлСния ΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π΅Π³ΠΎ охлаТдСния Π΄ΠΎ ΠΊΠΎΠΌΠ½Π°Ρ‚Π½ΠΎΠΉ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ со ΡΠΊΠΎΡ€ΠΎΡΡ‚ΡŒΡŽ 0,2 ВК/с, Π° ΠΏΠ΅Ρ€Π΅ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅ Π² кристалличСскоС состояниС β€” ΠΏΡƒΡ‚Π΅ΠΌ Π΅Π΅ Π½Π°Π³Ρ€Π΅Π²Π° Π΄ΠΎ 1300β€”1400 К со ΡΠΊΠΎΡ€ΠΎΡΡ‚ΡŒΡŽ 0,2 ВК/с ΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π΅Π³ΠΎ охлаТдСния. На основС Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² ΠœΠ”-экспСримСнтов сдСлан Π²Ρ‹Π²ΠΎΠ΄ ΠΎ сущСствовании минимального Ρ€Π°Π·ΠΌΠ΅Ρ€Π° наночастиц крСмния, Π½ΠΈΠΆΠ΅ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ³ΠΎ ΠΏΡ€ΠΈ Π·Π°Π΄Π°Π½Π½ΠΎΠΉ скорости измСнСния Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ созданиС элСмСнтов памяти, основанных Π½Π° ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΈ Ρ„Π°Π·ΠΎΠ²ΠΎΠ³ΠΎ состояния, становится ΠΏΡ€ΠΈΠ½Ρ†ΠΈΠΏΠΈΠ°Π»ΡŒΠ½ΠΎ Π½Π΅Π²ΠΎΠ·ΠΌΠΎΠΆΠ½Ρ‹ΠΌ. УстановлСно, Ρ‡Ρ‚ΠΎ для скорости измСнСния Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ 0,2β€‚Π’Πš/с Ρ‚Π°ΠΊΠΎΠΉ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹ΠΉ Ρ€Π°Π·ΠΌΠ΅Ρ€ составляСт 12,4 Π½ΠΌ (число Π°Ρ‚ΠΎΠΌΠΎΠ² β€” порядка 5β€…βˆ™β€…104 Π°Ρ‚ΠΎΠΌΠΎΠ²)

    Magnetic properties of carbon phases synthesized using high pressure-high temperature treatment

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    Two sets of samples were synthesized at 3.5 GPa near the point of C60 cage collapse at different annealing times. A clear structural transformation from mixture of C60 polymeric phases to graphite-like hard carbon phase was confirmed by X-ray diffraction and Raman spectroscopy. Magnetic force microscopy and superconducting quantum interference device were used to characterize the magnetic properties of the synthesized samples. We found that the sample preparation conditions used in this study are not suitable to produce bulk magnetic carbon.Comment: 26 pages, 7 figure

    ΠŸΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Антитромбина-III ΠΏΡ€ΠΈ Π½ΠΎΠ²ΠΎΠΉ коронавирусной ΠΈΠ½Ρ„Π΅ΠΊΡ†ΠΈΠΈ (Covid-19) Π² условиях ΡΠΊΡΡ‚Ρ€Π°ΠΊΠΎΡ€ΠΏΠΎΡ€Π°Π»ΡŒΠ½ΠΎΠΉ ΠΌΠ΅ΠΌΠ±Ρ€Π°Π½Π½ΠΎΠΉ оксигСнации (клиничСскоС наблюдСниС)

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    COVID-19 is a disease that, in addition to respiratory failure, leads to thrombosis and bleeding due to coagulation disorders. Extracorporeal membrane oxygenation (ECMO), required in cases of a deterioration of gas exchange function of the lungs, contributes to changes in blood coagulation indicators, which leads to an increased risk of hemorrhagic complications and thrombosis. In the article, a clinical case of a severe course of COVID-19 is reported, which required ECMO. During the treatment, antithrombin-III was used, which allowed avoiding life-threatening complications and successfully completing the procedure.Β COVID-19 являСтся Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠ΅ΠΌ, приводящим ΠΏΠΎΠΌΠΈΠΌΠΎ Π΄Ρ‹Ρ…Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ нСдостаточности ΠΊ Ρ‚Ρ€ΠΎΠΌΠ±ΠΎΠ·Π°ΠΌ ΠΈ кровотСчСниям вслСдствиС Π½Π°Ρ€ΡƒΡˆΠ΅Π½ΠΈΠΉ Π² систСмС гСмостаза. Π­ΠΊΡΡ‚Ρ€Π°ΠΊΠΎΡ€ΠΏΠΎΡ€Π°Π»ΡŒΠ½Π°Ρ мСмбранная оксигСнация (ЭКМО), Ρ‚Ρ€Π΅Π±ΡƒΡŽΡ‰Π°ΡΡΡ ΠΏΡ€ΠΈ сниТСнии Π³Π°Π·ΠΎΠΎΠ±ΠΌΠ΅Π½Π½ΠΎΠΉ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΈ Π»Π΅Π³ΠΊΠΈΡ…, вносит свой Π²ΠΊΠ»Π°Π΄ Π² измСнСния ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»Π΅ΠΉ свСртывания ΠΊΡ€ΠΎΠ²ΠΈ, Ρ‡Ρ‚ΠΎ Π²Π΅Π΄Π΅Ρ‚ ΠΊ ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΡŽ риска ослоТнСний гСморрагичСского Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€Π° ΠΈ Ρ‚Ρ€ΠΎΠΌΠ±ΠΎΠ·ΠΎΠ². Π’ ΡΡ‚Π°Ρ‚ΡŒΠ΅ прСдставлСн клиничСский случай тяТСлого тСчСния COVID-19, ΠΏΠΎΡ‚Ρ€Π΅Π±ΠΎΠ²Π°Π²ΡˆΠΈΠΉ провСдСния ЭКМО. Π’ Ρ…ΠΎΠ΄Π΅ лСчСния Π±Ρ‹Π» использован Антитромбин-III, Ρ‡Ρ‚ΠΎ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΎ ΠΈΠ·Π±Π΅ΠΆΠ°Ρ‚ΡŒ ΠΆΠΈΠ·Π½Π΅ΡƒΠ³Ρ€ΠΎΠΆΠ°ΡŽΡ‰ΠΈΡ… ослоТнСний ΠΈ ΡƒΡΠΏΠ΅ΡˆΠ½ΠΎ Π·Π°Π²Π΅Ρ€ΡˆΠΈΡ‚ΡŒ ΠΏΡ€ΠΎΡ†Π΅Π΄ΡƒΡ€Ρƒ.

    Enhancement in graphitization of coal tar pitch by functionalized carbon nanotubes

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    In this study, the influence of the addition of carbon nanotubes (CNTs) and carbon black (CB) on the graphitization temperature and microstructure of coal tar pitch (CTP) are investigated. X-ray diffraction patterns of carbon residues indicate that minimum interlayer spacing (d002) values are obtained at 2000Β°C for CTP/CNT. Moreover, the Raman spectrum of CTP/CNTs is similar to graphite, and the relative intensity of Raman lines shows that CTP/CB is less graphitized at 2000Β°C. In addition, scanning electron microscopy images show that when CB is added sample textures tend to disordered morphologies. However, CNTs, not only improve the morphology of CTP, but also act as nuclei for the growth of graphite flaky crystallites. The role of the CTP/CNT interface and the defects of CNTs on the graphitization degree are studied using transmission electron microscopy, and a mechanism for the graphitization of CTP, in the presence of CNTs, is proposed
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