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Бюллетени и Вестники - Библиотека аль-Фараби | Казахский национальный университет имени аль-Фараби

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The slope of the PSDF curve (γ) corresponds to several evolutionary processes taking place on the surface [27]. Analysis of the results based on fractal analysis and Minkowski functionals (see Figure 2-3) indicate a distinctive morphology for the sample synthesized after 50 minutes. The density of CNWs in these samples is much lower compared to others, leading to a minimum value. conductivity (see table one).

Figure 1 shows 3D models of the CNWs at dif- dif-ferent synthesis durations. As can be seen, the  mor-phology of the obtained CNWs differs significantly,  both in height and in the topology
Figure 1 shows 3D models of the CNWs at dif- dif-ferent synthesis durations. As can be seen, the mor-phology of the obtained CNWs differs significantly, both in height and in the topology

Influence of plasma and heat treatments on the properties of ZnO nanorods

Plasma treatment leads to a change in the ratio between the intensities of intrinsic and impurity photoluminescence bands. The intensity of the NBE band in PT samples increased after treatment in hydrogen plasma (Figure 4, spectrum 3) by ~17 times compared to the original spectrum (Figure 4, spectrum 1).

Figure 1 – Morphology of ZnO samples: a, b – initial; c, d – subjected to thermal annealing in  a muffle furnace at a temperature of 450 °C for one hour; e, f – treated in hydrogen plasma with
Figure 1 – Morphology of ZnO samples: a, b – initial; c, d – subjected to thermal annealing in a muffle furnace at a temperature of 450 °C for one hour; e, f – treated in hydrogen plasma with

Capacitive electrodes based on a combination of activated carbon and graphene

This is due to their lower series resistance of the AC-rGO mixture, as shown previously. The decrease in specific capacitance is due to an increase in the thickness of the carbon layer and, accordingly, to an increase in the electrical resistance of the electrode.

Figure 1 – SEM images of the carbon materials: (a) GO film on silicon substrate,   (b) rGO, (c) activated carbon, and (d) carbon black
Figure 1 – SEM images of the carbon materials: (a) GO film on silicon substrate, (b) rGO, (c) activated carbon, and (d) carbon black

Study of the structure and properties of SiC ceramics

The results of microstructural analysis of the obtained sample of SiC ceramics are shown in Figure 1. The composition of the charge for sintering carbide ceramics with nanoadditives forming a liquid phase has been developed: MnOnano 1.5 wt.

Table 1 – Thermodynamic values for chemical elements and ceramic compounds of the composition: MnO nano  1.5 wt
Table 1 – Thermodynamic values for chemical elements and ceramic compounds of the composition: MnO nano 1.5 wt

Features of the production and calibration of reference hardness test blocks

2 Development of production technology The main requirement for a measure of hardness is the uniformity of the working surface and the stability of physical and mechanical properties over time. In all countries, in the production of hardness blocks, different technologies are used for their manufacture. In the process of developing the technology for the production of hardness blocks, a chemical and microstructural analysis of the hardness blocks produced by the Tochpribor software, manufactured in 1989, was carried out.

In the production of hardness blocks, the conversion of hardness numbers according to different hardness scales is used, for example, 25 HRC hardness blocks correspond to a hardness level of 200 HB. The use of steels, in the production of which electrolytic remelting or vacuum holding of steel was used, makes it possible to increase the uniformity of hardness measures. The technology of manufacturing hardness blocks as reference measuring instruments is complex and time-consuming.

Based on a branch in Karaganda, KazStandard controlled the small-scale production of hardness measures according to the Brinell, Rockwell and Super-Rockwell scales. This will therefore provide the domestic market of Kazakhstan with a sufficient number of hardship measures at prices acceptable to users. Investigate the reasons for the heterogeneity of hardness measurements to eliminate it.

Table 3 shows the requirements for the chemical  composition of U8A-U10A, KhG, KhVG steels used  for the production of hardness measures.
Table 3 shows the requirements for the chemical composition of U8A-U10A, KhG, KhVG steels used for the production of hardness measures.

Study of functional properties stability of SnO 2 films on the duration thermal exposure and temperature changes

The resistance of the films was determined by 10 measurements in different parts of the samples. An increase in crystallite size and their perfection contributes to a decrease in the resistance of the films. In connection with the foregoing, the question arises about the stability of the properties of the films under long-term thermal exposure.

However, the application of the films took place after three months of aging of the film-forming systems. As shown in Figure 3a, no noticeable changes are observed in the structure of the films obtained from a film-forming system with pH=1.40 after three hours of annealing at 250°C. Six hours of annealing at 250 °C did not lead to any change in the structure of the films obtained from the film-forming system with pH = 1.40 (Figure 4a).

After six hours of annealing at 2500C, no cubic crystals are observed in the structure of the films obtained from the film-forming system with pH=1.49 (Figure 4c). The transparency of the samples obtained from the SnCl4/EtOH system with pH=1.46 and 1.49, with an increase in the duration of annealing up to 9 hours at 2500C, changes within the measurement accuracy. Electrochemical stability of fluorine doped tin oxide (FTO) coating at different pH conditions // Journal of the Electrochemical Society.

Table 1 – Resistance of samples obtained from solutions  of SnCl 4  of different acidity, after a single annealing
Table 1 – Resistance of samples obtained from solutions of SnCl 4 of different acidity, after a single annealing

Standard model and predictions for the Higgs boson

Figure 2 shows the diagrams that contribute to the correction of the mass of the Higgs boson. In the Lagrangian (11), all parameters were known from the experiment before the discovery of the Higgs boson, except the mass of the Higgs boson. From the Lagrangian (11), it follows the Feynman rules for the interaction of the Higgs boson with 𝑊𝑊𝑊𝑊± and 𝑍𝑍𝑍𝑍 bosons.

In the analyzes of the decay channels H → γγ and H → ZZ → 4l the mass of the Higgs boson had been. Measurements of the mass of the Higgs boson in the diphoton decay mode at the LHC, with the 35.9 fb-1. This decay channel is one of the most important decay modes in the search for the Higgs boson at the LHC.

The article is dedicated to the tenth anniversary of the discovery of the Higgs boson. Measurement of the Higgs boson width and evidence of its off-drop contributions to ZZ production // Nat. Measurements of properties of the Higgs boson decaying into the four-lepton final state.

Figure 1 – Potential of the Higgs field
Figure 1 – Potential of the Higgs field

The impact of technological parameters of the torch to physical and chemical properties of a gas-thermal burner

The influence of technological parameters of the burner on the physical and chemical properties of the gas-thermal burner. To determine the dependence of the physical and chemical properties of a burner with a gas thermal burner on the geometry of the burner nozzles and mass. Determining the heat flux density is necessary to determine the optimal trajectory of the dust particles in the burner.

It can be seen that at a distance of 0.8 m the average value of the flow density is 38 kW/. In the result of the calculated work, the trajectories for a particle movement in the torch are obtained (Figure 9). Thus, in the result of the research carried out, a significant impact of the technological parameters of the gas thermal equipment on the physical and chemical properties of the burner during the treatment of SMPE (HVAF method) has been established.

The necessary heat flux density for the complete melting of the UHMWPE particles not exceeding the destruction threshold was determined. The required dose of the UHMWPE powders introduced into the burner flame was determined. The optimal geometry of the torch, the trajectory of particles in the torch and the spray distances were determined based on the calculations of the "torch-polymer particle interaction".

Figure 1 – Optical image of UHMWPE particles (a), particle size distribution (b)
Figure 1 – Optical image of UHMWPE particles (a), particle size distribution (b)

Statistical modeling of spray formation, combustion, and evaporation of liquid fuel droplets

Liquid fuel is injected through a nozzle located in the center of the bottom of the combustion chamber. The figures below show the results of numerical experiments on the influence of the initial rate of heptane injection into the combustion chamber on the atomization and combustion processes. The distribution of the temperature plume and the combustion chamber height for heptane is shown in Figure 8.

Along with the increase in the droplet injection speed, the height of the plume core increases. Based on the results of the above numerical experiments, the optimal mode of combustion of heptane droplets in the combustion chamber is determined at an injection velocity of 300 m/s. The distribution of the concentration of carbon dioxide released in the combustion products is shown in Figure 12.

The distribution of released moisture in the combustion chamber was studied at different times of the entire combustion process (Fig. 13). With a statistical model, injection droplets reach 1.8 cm in height and 0.5 cm in the radius of the combustion chamber. Investigation of the influence of the different Reynolds numbers on the atomization and combustion processes of liquid fuels // Bulgarian Chemical Communications.

Figure 1 – Evolution trend of the carbon coefficient over the period 1990-2020
Figure 1 – Evolution trend of the carbon coefficient over the period 1990-2020

Thermophysical characteristics of friction materials based on bronze with 12% tin with the addition of GK-1 graphite powder and foundry coke

In the second case, to determine the thermophysical characteristics of the samples, a thermal constant analyzer Hot Disk TPS 2500S (Sweden) was used, which is based on the non-stationary method of a flat heat source (hot disk method) [19, 20 ] . Based on the analysis of the constructed function, the thermal conductivity and thermal diffusivity of the test sample were determined. However, the high thermal conductivity value of the input component did not lead to an increase in the thermal conductivity of the final composite.

This is due to a significant decrease in the density of the material, due to the introduction of a lighter component as an addition. It is possible that a decrease in the percentage of graphite leads to an increase in the thermal characteristics of the final composition. In addition to the density of the materials, the difference in the thermal conductivity coefficient values ​​between the studied materials is explained by the difference in the properties of their additives.

Based on the materials of the European Congress of Powder Metallurgy EuroPM2017 // Powder metallurgy: collection of scientific articles. Determination of the thermal conductivity tensor and heat capacity of insulating solids by the transient hot strip method // Journal of Applied Physics. Thermal and electrical conductivity of porous metals produced by powder metallurgy methods // Proceedings of the Physical Society.

Figure 1 – The shape of the particles of the initial powders used   to obtain the friction material: a) PMS-1; b) PO-1; c) GK-1; d) foundry coke
Figure 1 – The shape of the particles of the initial powders used to obtain the friction material: a) PMS-1; b) PO-1; c) GK-1; d) foundry coke

Obtaining manganese silicide films on a silicon substrate by the diffusion method

The dependence of the structure of the formed films on the substrate temperature was also investigated. The topology of the resulting films of manganese silicides and their elemental composition were evaluated using an X-ray microanalyzer in a Ukha-840 scanning electron microscope. The composition of the films grown in the temperature range T=910÷1040°C, obtained using an X-ray microanalyzer, was found to be close to the composition of bulk HSM (MnSi).

An analysis of the structural data suggests that the resulting films, at T≥970°C, grow the HCM film in the form of grains. Further thermal annealing of the samples in the temperature range T=350÷800°C led to the enlargement of the formed HSM grains. Photomicrographs of the HSM film grown by us are shown in Fig. 1. a) with a resolution of 10 µm.

As a result of the conducted studies, the mechanism of manganese diffusion in silicon was established, leading to the formation of higher manganese silicides on the silicon surface. It has been proven that the films grown on the silicon surface consist of HSM grains with the dominant orientation of the c-axis perpendicular to the substrate. Investigating the influence of layer surface on photoelectric properties in higher manganese silicide (HSM) Si--M structures // Surface.

Table 1 – Physical parameters of manganese silicide films (vacuum Р~10 6  mm Hg, rapid cooling) Diffusion temperature,
Table 1 – Physical parameters of manganese silicide films (vacuum Р~10 6 mm Hg, rapid cooling) Diffusion temperature,

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Figure 2 – Optical properties of ZnO films obtained by chemical deposition:
Figure 3 – Diffractogram of the initial ZnO sample The photoluminescence spectra of ZnO samples  synthesized by chemical solution deposition were  studied (Figure 4)
Figure 1 – SEM images of the carbon materials: (a) GO film on silicon substrate,   (b) rGO, (c) activated carbon, and (d) carbon black
Figure 4 – XRD patterns of the graphene oxide: GO – as- as-synthisized GO, VA – vacuum annealing, VA+UV200min
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