228 research outputs found
High surface area activated carbon prepared from wood-based spent mushroom substrate for supercapacitors and water treatment
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
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
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 12β15 GPa. The ambient pressure structure of COF-1-M can be reversibly recovered after compression up to 10β15 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
Using an optimized KOH activation procedure we prepared highly porous graphene scaffoldmaterials with SSA values up to 3400mΒ² gβ»ΒΉ and a pore volume up to 2.2 cmΒ³ gΛΒΉ, which are among the highest for carbon materials. Hydrogen uptake of activated graphene samples was evaluated in a broad temperature interval (77β296 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
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
Π ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π΅ ΡΠΎΠ·Π΄Π°Π½ΠΈΡ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² ΠΏΠ°ΠΌΡΡΠΈ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π½Π°Π½ΠΎΡΠ°ΡΡΠΈΡ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ
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 1300β1400 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 1300β1400 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.ΠΠ°ΠΌΡΡΡ, ΡΠ²ΡΠ·Π°Π½Π½Π°Ρ Ρ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΡΠ°Π·ΠΎΠ²ΠΎΠ³ΠΎ ΡΠΎΡΡΠΎΡΠ½ΠΈΡ (phaseβchange memory), ΠΎΡΠ½ΠΎΠ²Π°Π½Π° Π½Π° ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΈ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΈΡ
, ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΠ»ΠΈ ΠΈΠ½ΡΡ
ΡΠ²ΠΎΠΉΡΡΠ² Π²Π΅ΡΠ΅ΡΡΠ²Π° ΠΏΡΠΈ ΡΠ°Π·ΠΎΠ²ΠΎΠΌ ΠΏΠ΅ΡΠ΅Ρ
ΠΎΠ΄Π΅, Π½Π°ΠΏΡΠΈΠΌΠ΅Ρ ΠΏΠ΅ΡΠ΅Ρ
ΠΎΠ΄Π΅ ΠΈΠ· Π°ΠΌΠΎΡΡΠ½ΠΎΠ³ΠΎ ΡΠΎΡΡΠΎΡΠ½ΠΈΡ Π² ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠ΅. ΠΠ° ΡΠ΅Π³ΠΎΠ΄Π½ΡΡΠ½ΠΈΠΉ Π΄Π΅Π½Ρ ΡΠΆΠ΅ ΡΠ΅Π°Π»ΠΈΠ·ΠΎΠ²Π°Π½Π½ΡΠ΅ ΠΈ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΡΠ΅ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ°ΠΊΠΎΠΉ ΠΏΠ°ΠΌΡΡΠΈ ΡΠ²ΡΠ·Π°Π½Ρ Π² ΠΏΠ΅ΡΠ²ΡΡ ΠΎΡΠ΅ΡΠ΅Π΄Ρ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠ½ΠΎΠ³ΠΎΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½ΡΠ½ΡΡ
ΡΠΏΠ»Π°Π²ΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ², ΠΎΡΠ½ΠΎΡΡΡΠΈΡ
ΡΡ ΠΊ ΠΌΠ΅ΡΠ°Π»Π»Π°ΠΌ ΠΈ ΠΏΠΎΠ»ΡΠΏΡΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠ°ΠΌ. ΠΠ΄Π½Π°ΠΊΠΎ ΠΎΠ΄Π½ΠΎΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½ΡΠ½ΡΠ΅ Π½Π°Π½ΠΎΡΠ°ΡΡΠΈΡΡ, Π²ΠΊΠ»ΡΡΠ°Ρ Π½Π°Π½ΠΎΡΠ°ΡΡΠΈΡΡ Si, ΡΠ°ΠΊΠΆΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΡΡ ΠΈΠ½ΡΠ΅ΡΠ΅Ρ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
Π½Π°Π½ΠΎΡΠ°Π·ΠΌΠ΅ΡΠ½ΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² ΠΏΠ°ΠΌΡΡΠΈ. Π ΡΠ°ΡΡΠ½ΠΎΡΡΠΈ, Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΡΠΎΠ·Π΄Π°Π½ΠΈΡ ΡΠ°ΠΊΠΈΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² ΠΏΠ°ΠΌΡΡΠΈ ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π°Π΅ΡΡΡ ΡΠ΅ΠΌ, ΡΡΠΎ Ρ ΠΎΠ±ΡΠ΅ΠΌΠ½ΠΎΠΉ ΡΠ°Π·Ρ Π°ΠΌΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ Π·Π½Π°ΡΠ΅Π½ΠΈΠ΅ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΠΎΠ³Π»ΠΎΡΠ΅Π½ΠΈΡ Π½Π° ΠΏΠΎΡΡΠ΄ΠΎΠΊ Π±ΠΎΠ»ΡΡΠ΅, ΡΠ΅ΠΌ Ρ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ. Π Π°Π·ΡΠΌΠ΅Π΅ΡΡΡ, ΡΡΠΎΡ ΡΡΡΠ΅ΠΊΡ Π·Π°ΡΡΡΠ΄Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎ ΡΠ΅Π°Π»ΠΈΠ·ΠΎΠ²Π°ΡΡ Π΄Π»Ρ ΠΎΡΠ΄Π΅Π»ΡΠ½ΠΎΠΉ Π½Π°Π½ΠΎΡΠ°ΡΡΠΈΡΡ, ΡΠ°Π·ΠΌΠ΅Ρ ΠΊΠΎΡΠΎΡΠΎΠΉ Π½Π΅ ΠΏΡΠ΅Π²ΡΡΠ°Π΅Ρ Π΄Π»ΠΈΠ½Ρ Π²ΠΎΠ»Π½Ρ ΡΠ²Π΅ΡΠ°. Π Π΄Π°Π½Π½ΠΎΠΉ ΡΠ°Π±ΠΎΡΠ΅ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΠΎΠΉ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ (ΠΠ) ΠΈ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»Π° Π‘ΡΠΈΠ»Π»ΠΈΠ½Π΄ΠΆΠ΅ΡΠ°βΠΠ΅Π±Π΅ΡΠ° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ ΠΏΠ»Π°Π²Π»Π΅Π½ΠΈΡ ΠΈ ΡΡΠ»ΠΎΠ²ΠΈΡ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΠ·Π°ΡΠΈΠΈ Π½Π°Π½ΠΎΡΠ°ΡΡΠΈΡ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ, ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠΈΡ
Π΄ΠΎ 105 Π°ΡΠΎΠΌΠΎΠ². ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΠΏΡΠΈ ΠΎΡ
Π»Π°ΠΆΠ΄Π΅Π½ΠΈΠΈ Π½Π°Π½ΠΎΠΊΠ°ΠΏΠ΅Π»Ρ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ ΡΠΎ ΡΠΊΠΎΡΠΎΡΡΡΡ 0,2 Π’Π/Ρ ΠΈ Π²ΡΡΠ΅ ΠΈΠΌΠ΅Π΅Ρ ΠΌΠ΅ΡΡΠΎ ΠΈΡ
ΠΏΠ΅ΡΠ΅Ρ
ΠΎΠ΄ Π² Π°ΠΌΠΎΡΡΠ½ΠΎΠ΅ ΡΠΎΡΡΠΎΡΠ½ΠΈΠ΅, ΡΠΎΠ³Π΄Π° ΠΊΠ°ΠΊ ΠΎΠ΄Π½ΠΎΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½ΡΠ½ΡΠ΅ ΠΌΠ΅ΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π½Π°Π½ΠΎΠΊΠ°ΠΏΠ»ΠΈ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΠ·ΡΡΡΡΡ Π² ΠΠ-ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Ρ
Π΄Π°ΠΆΠ΅ ΠΏΡΠΈ ΡΠΊΠΎΡΠΎΡΡΡΡ
ΠΎΡ
Π»Π°ΠΆΠ΄Π΅Π½ΠΈΡ 1 Π’Π/Ρ. ΠΡΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠ΅ΠΌ Π½Π°Π³ΡΠ΅Π²Π΅ Π°ΠΌΠΎΡΡΠ½ΡΡ
Π½Π°Π½ΠΎΡΠ°ΡΡΠΈΡ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ, ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠΈΡ
Π±ΠΎΠ»Π΅Π΅ 5β
ββ
104 Π°ΡΠΎΠΌΠΎΠ², ΠΏΡΠΎΠΈΡΡ
ΠΎΠ΄ΠΈΡ ΠΈΡ
ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΠ·Π°ΡΠΈΡ Π² ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Π½ΠΎΠΌ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠΌ ΠΈΠ½ΡΠ΅ΡΠ²Π°Π»Π΅ ΠΎΡ 1300 Π΄ΠΎ 1400 Π. Π‘Π΄Π΅Π»Π°Π½ Π²ΡΠ²ΠΎΠ΄ ΠΎ ΠΏΡΠΈΠ½ΡΠΈΠΏΠΈΠ°Π»ΡΠ½ΠΎΠΉ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠΈ ΡΠΎΠ·Π΄Π°Π½ΠΈΡ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² ΠΏΠ°ΠΌΡΡΠΈ, ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΡΡ
Π½Π° Π΄Π°Π½Π½ΡΡ
ΡΠ°Π·ΠΎΠ²ΡΡ
ΠΏΠ΅ΡΠ΅Ρ
ΠΎΠ΄Π°Ρ
. ΠΠ΅ΡΠ΅Ρ
ΠΎΠ΄ Π½Π°Π½ΠΎΡΠ°ΡΡΠΈΡΡ Π² Π°ΠΌΠΎΡΡΠ½ΠΎΠ΅ ΡΠΎΡΡΠΎΡΠ½ΠΈΠ΅ Π΄ΠΎΡΡΠΈΠ³Π°Π΅ΡΡΡ ΠΏΡΡΠ΅ΠΌ Π΅Π΅ ΠΏΠ»Π°Π²Π»Π΅Π½ΠΈΡ ΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠ΅Π³ΠΎ ΠΎΡ
Π»Π°ΠΆΠ΄Π΅Π½ΠΈΡ Π΄ΠΎ ΠΊΠΎΠΌΠ½Π°ΡΠ½ΠΎΠΉ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΡΠΎ ΡΠΊΠΎΡΠΎΡΡΡΡ 0,2 Π’Π/Ρ, Π° ΠΏΠ΅ΡΠ΅ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅ Π² ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΠΎΡΡΠΎΡΠ½ΠΈΠ΅ β ΠΏΡΡΠ΅ΠΌ Π΅Π΅ Π½Π°Π³ΡΠ΅Π²Π° Π΄ΠΎ 1300β1400 Π ΡΠΎ ΡΠΊΠΎΡΠΎΡΡΡΡ 0,2 Π’Π/Ρ ΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠ΅Π³ΠΎ ΠΎΡ
Π»Π°ΠΆΠ΄Π΅Π½ΠΈΡ. ΠΠ° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΠ-ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠΎΠ² ΡΠ΄Π΅Π»Π°Π½ Π²ΡΠ²ΠΎΠ΄ ΠΎ ΡΡΡΠ΅ΡΡΠ²ΠΎΠ²Π°Π½ΠΈΠΈ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠ°Π·ΠΌΠ΅ΡΠ° Π½Π°Π½ΠΎΡΠ°ΡΡΠΈΡ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ, Π½ΠΈΠΆΠ΅ ΠΊΠΎΡΠΎΡΠΎΠ³ΠΎ ΠΏΡΠΈ Π·Π°Π΄Π°Π½Π½ΠΎΠΉ ΡΠΊΠΎΡΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΡΠΎΠ·Π΄Π°Π½ΠΈΠ΅ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² ΠΏΠ°ΠΌΡΡΠΈ, ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΡΡ
Π½Π° ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΈ ΡΠ°Π·ΠΎΠ²ΠΎΠ³ΠΎ ΡΠΎΡΡΠΎΡΠ½ΠΈΡ, ΡΡΠ°Π½ΠΎΠ²ΠΈΡΡΡ ΠΏΡΠΈΠ½ΡΠΈΠΏΠΈΠ°Π»ΡΠ½ΠΎ Π½Π΅Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΡΠΌ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π΄Π»Ρ ΡΠΊΠΎΡΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ 0,2βΠ’Π/Ρ ΡΠ°ΠΊΠΎΠΉ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡΠ½ΡΠΉ ΡΠ°Π·ΠΌΠ΅Ρ ΡΠΎΡΡΠ°Π²Π»ΡΠ΅Ρ 12,4 Π½ΠΌ (ΡΠΈΡΠ»ΠΎ Π°ΡΠΎΠΌΠΎΠ² β ΠΏΠΎΡΡΠ΄ΠΊΠ° 5β
ββ
104 Π°ΡΠΎΠΌΠΎΠ²)
Magnetic properties of carbon phases synthesized using high pressure-high temperature treatment
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
ΠΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΠ½ΡΠΈΡΡΠΎΠΌΠ±ΠΈΠ½Π°-III ΠΏΡΠΈ Π½ΠΎΠ²ΠΎΠΉ ΠΊΠΎΡΠΎΠ½Π°Π²ΠΈΡΡΡΠ½ΠΎΠΉ ΠΈΠ½ΡΠ΅ΠΊΡΠΈΠΈ (Covid-19) Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ ΡΠΊΡΡΡΠ°ΠΊΠΎΡΠΏΠΎΡΠ°Π»ΡΠ½ΠΎΠΉ ΠΌΠ΅ΠΌΠ±ΡΠ°Π½Π½ΠΎΠΉ ΠΎΠΊΡΠΈΠ³Π΅Π½Π°ΡΠΈΠΈ (ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠ΅ Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΠ΅)
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 ΡΠ²Π»ΡΠ΅ΡΡΡ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠ΅ΠΌ, ΠΏΡΠΈΠ²ΠΎΠ΄ΡΡΠΈΠΌ ΠΏΠΎΠΌΠΈΠΌΠΎ Π΄ΡΡ
Π°ΡΠ΅Π»ΡΠ½ΠΎΠΉ Π½Π΅Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎΡΡΠΈ ΠΊ ΡΡΠΎΠΌΠ±ΠΎΠ·Π°ΠΌ ΠΈ ΠΊΡΠΎΠ²ΠΎΡΠ΅ΡΠ΅Π½ΠΈΡΠΌ Π²ΡΠ»Π΅Π΄ΡΡΠ²ΠΈΠ΅ Π½Π°ΡΡΡΠ΅Π½ΠΈΠΉ Π² ΡΠΈΡΡΠ΅ΠΌΠ΅ Π³Π΅ΠΌΠΎΡΡΠ°Π·Π°. ΠΠΊΡΡΡΠ°ΠΊΠΎΡΠΏΠΎΡΠ°Π»ΡΠ½Π°Ρ ΠΌΠ΅ΠΌΠ±ΡΠ°Π½Π½Π°Ρ ΠΎΠΊΡΠΈΠ³Π΅Π½Π°ΡΠΈΡ (ΠΠΠΠ), ΡΡΠ΅Π±ΡΡΡΠ°ΡΡΡ ΠΏΡΠΈ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠΈ Π³Π°Π·ΠΎΠΎΠ±ΠΌΠ΅Π½Π½ΠΎΠΉ ΡΡΠ½ΠΊΡΠΈΠΈ Π»Π΅Π³ΠΊΠΈΡ
, Π²Π½ΠΎΡΠΈΡ ΡΠ²ΠΎΠΉ Π²ΠΊΠ»Π°Π΄ Π² ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ ΡΠ²Π΅ΡΡΡΠ²Π°Π½ΠΈΡ ΠΊΡΠΎΠ²ΠΈ, ΡΡΠΎ Π²Π΅Π΄Π΅Ρ ΠΊ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΡ ΡΠΈΡΠΊΠ° ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ Π³Π΅ΠΌΠΎΡΡΠ°Π³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠ° ΠΈ ΡΡΠΎΠΌΠ±ΠΎΠ·ΠΎΠ². Π ΡΡΠ°ΡΡΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ»ΡΡΠ°ΠΉ ΡΡΠΆΠ΅Π»ΠΎΠ³ΠΎ ΡΠ΅ΡΠ΅Π½ΠΈΡ COVID-19, ΠΏΠΎΡΡΠ΅Π±ΠΎΠ²Π°Π²ΡΠΈΠΉ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ ΠΠΠΠ. Π Ρ
ΠΎΠ΄Π΅ Π»Π΅ΡΠ΅Π½ΠΈΡ Π±ΡΠ» ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ ΠΠ½ΡΠΈΡΡΠΎΠΌΠ±ΠΈΠ½-III, ΡΡΠΎ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΎ ΠΈΠ·Π±Π΅ΠΆΠ°ΡΡ ΠΆΠΈΠ·Π½Π΅ΡΠ³ΡΠΎΠΆΠ°ΡΡΠΈΡ
ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ ΠΈ ΡΡΠΏΠ΅ΡΠ½ΠΎ Π·Π°Π²Π΅ΡΡΠΈΡΡ ΠΏΡΠΎΡΠ΅Π΄ΡΡΡ.
Enhancement in graphitization of coal tar pitch by functionalized carbon nanotubes
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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