675 research outputs found
Ультрафлокуляция – как метод повышения эффективности процесса извлечения тонкодисперсного угля из хвостов обогащения
На прикладі хвостів вуглезбагачення ОФ "Распадська" (р. Междуріченськ Кемеровської області, РФ) встановлено, що використання ультрафлокулярної обробки дає нижче-наступні переваги при витяганні тонкодисперсного вугілля методом седиментації в радіальному згущувачі:
• зниження витрати флокулянтів – в 2,5-3,5 разу.
• збільшення витягання вугільного концентрату з хвостів на 23…26%.
• зменшення зольності концентрату, вилученого з хвостів з 18 до 12%.
• зменшення вологості прес-фільтраційного кека концентрату, вилученого з хвостів з 40 до 35%.На примере хвостов углеобогащения ОФ "Распадская" (г. Междуреченск Кемеровской области, РФ) установлено, что использование ультрафлокулярной обработки дает нижеследующие преимущества при извлечении тонкодисперсного угля методом седиментации в радиальном сгустителе:
• снижение расхода флокулянтов – в 2,5-3,5 раза.
• увеличение извлечения угольного концентрата из хвостов на 23…26%.
• уменьшение зольности концентрата, извлекаемого из хвостов с 18 до 12%.
• уменьшение влажности пресс-фильтрационного кека концентрата, извлекаемого из хвостов с 40 до 35%
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A generative inference framework for analysing patterns of cultural change in sparse population data with evidence for fashion trends in LBK culture
Cultural change can be quantified by temporal changes in frequency of different cultural artefacts and it is a central question to identify what underlying cultural transmission processes could have caused the observed frequency changes. Observed changes, however, often describe the dynamics in samples of the population of artefacts, whereas transmission processes act on the whole population. Here we develop a modelling framework aimed at addressing this inference problem. To do so, we firstly generate population structures from which the observed sample could have been drawn randomly and then determine theoretical samples at a later time t2 produced under the assumption that changes in frequencies are caused by a specific transmission process. Thereby we also account for the potential effect of time-averaging processes in the generation of the observed sample. Subsequent statistical comparisons (e.g. using Bayesian inference) of the theoretical and observed samples at t2 can establish which processes could have produced the observed frequency data. In this way, we infer underlying transmission processes directly from available data without any equilibrium assumption. We apply this framework to a dataset describing pottery from settlements of some of the first farmers in Europe (the LBK culture) and conclude that the observed frequency dynamic of different types of decorated pottery is consistent with age-dependent selection, a preference for 'young' pottery types which is potentially indicative of fashion trends
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Numerical simulations of optical properties of Saharan dust aerosols with emphasis on lidar applications
In the framework of the Saharan Mineral Dust Experiment (SAMUM) for the first time the spectral dependence of particle linear depolarization ratios was measured by combining four lidar systems. In this paper these measurements are compared with results from scattering theory based on the T-matrix method. For this purpose, in situ measurements—size distribution, shape distribution and refractive index—were used as input parameters; particle shape was approximated by spheroids. A sensitivity study showed that lidar-related parameters—lidar ratio Sp and linear depolarization ratio δp—are very sensitive to changes of all parameters. The simulated values of the δp are in the range of 20% and 31% and thus in the range of the measurements. The spectral dependence is weak, so that it could not be resolved by the measurements. Calculated lidar ratios based on the measured microphysics and considering equivalent radii up to 7.5μm show a range of possible values between 29 and 50 sr at λ = 532 nm. Larger Sp might be possible if the real part of the refractive index is small and the imaginary part is large. A strict validation was however not possible as too many microphysical parameters influence Sp and δp that could not be measured with the required accuracy
Mixing of mineral dust with urban pollution aerosol over Dakar (Senegal): Impact on dust physico-chemical and radiative properties.
In the framework of the Saharan Mineral Dust Experiment (SAMUM) in 2008, the mixing of the urban pollution
plume of Dakar (Senegal) with mineral dust was studied in detail using the German research aircraft Falcon which was
equipped with a nadir-looking high spectral resolution lidar (HSRL) and extensive aerosol in situ instrumentation. The
mineral dust layer as well as the urban pollution plume were probed remotely by the HSRL and in situ. Back trajectory
analyses were used to attribute aerosol samples to source regions.We found that the emission from the region of Dakar
increased the aerosol optical depth (532 nm) from approximately 0.30 over sea and over land east of Dakar to 0.35 in the city outflow. In the urban area, local black carbon (BC) emissions, or soot respectively, contributed more than 75% to aerosol absorption at 530 nm. In the dust layer, the single-scattering albedo at 530 nm was 0.96 � 0.99, whereas
we found a value of 0.908 �± 0.018 for the aerosol dominated by urban pollution. After 6h of transport over the North
Atlantic, the externally mixed mode of secondary aerosol particles had almost completely vanished, whereas the BC
agglomerates (soot) were still externally mixed with mineral dust particles
Regional Saharan dust modelling during the SAMUM 2006 campaign
The regional dust model system LM-MUSCAT-DES was developed in the framework of the SAMUM project. Using the
unique comprehensive data set of near-source dust properties during the 2006SAMUMfield campaign, the performance
of the model system is evaluated for two time periods in May and June 2006. Dust optical thicknesses, number size
distributions and the position of the maximum dust extinction in the vertical profiles agree well with the observations.
However, the spatio-temporal evolution of the dust plumes is not always reproduced due to inaccuracies in the dust
source placement by the model. While simulated winds and dust distributions are well matched for dust events caused
by dry synoptic-scale dynamics, they are often misrepresented when dust emissions are caused by moist convection or
influenced by small-scale topography that is not resolved by the model. In contrast to long-range dust transport, in the
vicinity of source regions the model performance strongly depends on the correct prediction of the exact location of
sources. Insufficiently resolved vertical grid spacing causes the absence of inversions in the model vertical profiles and
likely explains the absence of the observed sharply defined dust layers
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Ground-based off-line aerosol measurements at Praia, Cape Verde, during the Saharan Mineral Dust Experiment: Microphysical properties and mineralogy
A large field experiment of the Saharan Mineral Dust Experiment (SAMUM) was performed in Praia, Cape Verde, in
January and February 2008. This work reports on the aerosol mass concentrations, size distributions and mineralogical
composition of the aerosol arriving at Praia. Three dust periods were recorded during the measurements, divided by
transitional periods and embedded in maritime-influenced situations. The total suspended particle mass/PM10/PM2.5
were 250/180/74μg/m3 on average for the first dust period (17–21 January) and 250/230/83μg/m3 for the second (24–26
January). The third period (28 January to 2 February) was the most intensive with 410/340/130 μg/m3. Four modes were
identified in the size distribution. The first mode (50–70 nm) and partly the second (700–1100 nm) can be regarded as
of marine origin, but some dust contributes to the latter. The third mode (2–4 μm) is dominated by advected dust, while
the intermittently occurring fourth mode (15–70 μm) may have a local contribution. The dust consisted of kaolinite
(dust/maritime period: 35%wt./25%wt.),K-feldspar (20%wt./25%wt.), illite (14%wt./10%wt.), quartz (11%wt./8%wt.),
smectites (6%wt./4%wt.), plagioclase (6%wt./1%wt.), gypsum (4%wt./7%wt.), halite (2%wt./17%wt.) and calcite
(2%wt./3%wt.)
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State of mixing, shape factor, number size distribution, and hygroscopic growth of the Saharan anthropogenic and mineral dust aerosol at Tinfou, Morocco
The Saharan Mineral Dust Experiment (SAMUM) was conducted in May and June 2006 in Tinfou, Morocco. A H-TDMA system and a H-DMA-APS system were used to obtain hygroscopic properties of mineral dust particles at 85% RH. Dynamic shape factors of 1.11, 1.19 and 1.25 were determined for the volume equivalent diameters 720, 840 and 960 nm, respectively.
During a dust event, the hydrophobic number fraction of 250 and 350 nm particles increased significantly from 30 and 65% to 53 and 75%, respectively, indicating that mineral dust particles can be as small as 200 nm in diameter. Lognormal functions for mineral dust number size distributions were obtained from total particle number size distributions and fractions of hydrophobic particles. The geometric mean diameter for Saharan dust particles was 715 nm during the dust event and 570 nm for the Saharan background aerosol.
Measurements of hygroscopic growth showed that the Saharan aerosol consists of an anthropogenic fraction (predominantly non natural sulphate and carbonaceous particles) and of mineral dust particles. Hygroscopic growth and hysteresis curve measurements of the ‘more’ hygroscopic particle fraction indicated ammonium sulphate as a main component of the anthropogenic aerosol. Particles larger than 720 nm in diameter were completely hydrophobic meaning that mineral dust particles are not hygroscopic
Airborne observations of the Eyjafjalla volcano ash cloud over Europe during air space closure in April and May 2010
© Author(s) 2011. This work is distributed under the Creative Commons Attribution 3.0 LicenseAirborne lidar and in-situ measurements of aerosols and trace gases were performed in volcanic ash plumes over Europe between Southern Germany and Iceland with the Falcon aircraft during the eruption period of the Eyjafjalla1 volcano between 19 April and 18 May 2010. Flight planning and measurement analyses were supported by a refined Meteosat ash product and trajectory model analysis. The volcanic ash plume was observed with lidar directly over the volcano and up to a distance of 2700 km downwind, and up to 120 h plume ages. Aged ash layers were between a few 100 m to 3 km deep, occurred between 1 and 7 km altitude, and were typically 100 to 300 km wide. Particles collected by impactors had diameters up to 20 μm diameter, with size and age dependent composition. Ash mass concentrations were derived from optical particle spectrometers for a particle density of 2.6 g cm-3 and various values of the refractive index (RI, real part: 1.59; 3 values for the imaginary part: 0, 0.004 and 0.008). The mass concentrations, effective diameters and related optical properties were compared with ground-based lidar observations. Theoretical considerations of particle sedimentation constrain the particle diameters to those obtained for the lower RI values. The ash mass concentration results have an uncertainty of a factor of two. The maximum ash mass concentration encountered during the 17 flights with 34 ash plume penetrations was below 1 mg m-3. The Falcon flew in ash clouds up to about 0.8 mg m-3 for a few minutes and in an ash cloud with approximately 0.2 mg -3 mean-concentration for about one hour without engine damage. The ash plumes were rather dry and correlated with considerable CO and SO2 increases and O3 decreases. To first order, ash concentration and SO2 mixing ratio in the plumes decreased by a factor of two within less than a day. In fresh plumes, the SO2 and CO concentration increases were correlated with the ash mass concentration. The ash plumes were often visible slantwise as faint dark layers, even for concentrations below 0.1 mg m-3. The large abundance of volatile Aitken mode particles suggests previous nucleation of sulfuric acid droplets. The effective diameters range between 0.2 and 3 μm with considerable surface and volume contributions from the Aitken and coarse mode aerosol, respectively. The distal ash mass flux on 2 May was of the order of 500 (240-1600) kgs -1. The volcano induced about 10 (2.5-50) Tg of distal ash mass and about 3 (0.6-23) Tg of SO2 during the whole eruption period. The results of the Falcon flights were used to support the responsible agencies in their decisions concerning air traffic in the presence of volcanic ash.Peer reviewe
Mass deposition fluxes of Saharan mineral dust to the tropical northeast Atlantic Ocean: an intercomparison of methods
Mass deposition fluxes of mineral dust to the tropical northeast Atlantic Ocean were determined within this study. In the framework of SOPRAN (Surface Ocean Processes in the Anthropocene), the interaction between the atmosphere and the ocean in terms of material exchange were investigated at the Cape Verde atmospheric observatory (CVAO) on the island Sao Vicente for January 2009. Five different methods were applied to estimate the deposition flux, using different meteorological and physical measurements, remote sensing, and regional dust transport simulations. The set of observations comprises micrometeorological measurements with an ultra-sonic anemometer and profile measurements using 2-D anemometers at two different heights, and microphysical measurements of the size-resolved mass concentrations of mineral dust. In addition, the total mass concentration of mineral dust was derived from absorption photometer observations and passive sampling. The regional dust model COSMO-MUSCAT was used for simulations of dust emission and transport, including dry and wet deposition processes. This model was used as it describes the AOD's and mass concentrations realistic compared to the measurements and because it was run for the time period of the measurements. The four observation-based methods yield a monthly average deposition flux of mineral dust of 12–29 ng m−2 s−1. The simulation results come close to the upper range of the measurements with an average value of 47 ng m−2 s−1. It is shown that the mass deposition flux of mineral dust obtained by the combination of micrometeorological (ultra-sonic anemometer) and microphysical measurements (particle mass size distribution of mineral dust) is difficult to compare to modeled mass deposition fluxes when the mineral dust is inhomogeneously distributed over the investigated area
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Size distribution, mass concentration, chemical and mineralogical composition and derived optical parameters of the boundary layer aerosol at Tinfou, Morocco, during SAMUM 2006
During the SAMUM 2006 field campaign in southern Morocco, physical and chemical properties of desert aerosols
were measured. Mass concentrations ranging from 30μgm−3 for PM2.5 under desert background conditions up to
300 000μgm−3 for total suspended particles (TSP) during moderate dust storms were measured. TSP dust concentrations
are correlated with the local wind speed, whereasPM10 andPM2.5 concentrations are determined by advection from
distant sources. Size distributions were measured for particles with diameter between 20 nm and 500μm (parametrizations
are given). Two major regimes of the size spectrum can be distinguished. For particles smaller than 500 nm
diameter, the distributions show maxima around 80 nm, widely unaffected of varying meteorological and dust emission
conditions. For particles larger than 500 nm, the range of variation may be up to one order of magnitude and up to
three orders of magnitude for particles larger than 10μm. The mineralogical composition of aerosol bulk samples was
measured by X-ray powder diffraction. Major constituents of the aerosol are quartz, potassium feldspar, plagioclase,
calcite, hematite and the clay minerals illite, kaolinite and chlorite. A small temporal variability of the bulk mineralogical
composition was encountered. The chemical composition of approximately 74 000 particles was determined by
electron microscopic single particle analysis. Three size regimes are identified: for smaller than 500 nm in diameter, the
aerosol consists of sulphates and mineral dust. For larger than 500 nm up to 50μm, mineral dust dominates, consisting
mainly of silicates, and—to a lesser extent—carbonates and quartz. For diameters larger than 50μm, approximately
half of the particles consist of quartz. Time series of the elemental composition show a moderate temporal variability
of the major compounds. Calcium-dominated particles are enhanced during advection from a prominent dust source in
Northern Africa (Chott El Djerid and surroundings). The particle aspect ratio was measured for all analysed particles.
Its size dependence reflects that of the chemical composition. For larger than 500 nm particle diameter, a median aspect
ratio of 1.6 is measured. Towards smaller particles, it decreases to about 1.3 (parametrizations are given). From the
chemical/mineralogical composition, the aerosol complex refractive index was determined for several wavelengths
from ultraviolet to near-infrared. Both real and imaginary parts show lower values for particles smaller than 500 nm in
diameter (1.55–2.8 × 10−3i at 530 nm) and slightly higher values for larger particles (1.57–3.7 × 10−3i at 530 nm)
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