376 research outputs found
Spatial heterogeneity of soil properties of recreational areas of Volgograd
The article presents the developed soil maps and maps of spatial variability of soil properties (pH, total salt and carbonate content, organic carbon, density) in some recreational areas of Volgograd. The anthropogenic soils in the studied recreational areas include various urbostratozems (Urbic Technosols (Transportic)), Ekranic Technosols (Transportic), as well as quasizems (Phaeozems (Tehnic)), among the agrogenic ones β accumulation-carbonate agrozems (Cambisols (Aric, Protocalcic). Natural soils are represented by light and dark humus soils, chestnut soils, solonetz, as well as stratozems and psammozems. According to the data of isolinear mapping, it was found that acid-alkaline properties of soils of green zones vary from slightly alkaline to alkaline depending on the soil horizon and anthropogenic load. The mapping did not reveal salinization of the upper 0β30 cm layer. Values of organic carbon vary greatly (1β10%) and are conditioned by the presence or absence of meliorative artificial layers, as well as by the character of territory use. The content of calcium carbonates in the upper 30 cm is small and varies from 0.7 to 5%. It is established that the physical properties (density) directly depend on the level of anthropogenic load, increasing in footpaths and lawns. Spatial assessment of the properties of urban soils is important for identifying areas with an excess or on the contrary β low content of certain chemical and physical indicators for the planning of landscaping and gardening of urban areas
The bone panaris in children
The most widespread festering-inflammatory disease of brush is a panaris. Panaris β an acute purulent inflammation of the finger tissue. Forms panaris, accompanied by lesions of bone , the most difficult to treatment. Analyzed the case histories of 64 children hospitalized in the Department of purulent surgery DGKB β 9 for 2017-2019 with clinical bone panaris. In the study, disease duration before resorting to the surgeon was on average 5.8 days. 37.5% of patients were self-treatment. Outpatient treatment by a surgeon in the community was conducted in 32.8% of cases. In the analysis of anamnestic data in 14 children developed a bone panaris finger after trauma. In most cases, damaged distal phalanx of the second finger of the left and right hand. All patients complained of pain in the finger, swelling, local hyperemia of the skin. The clinical picture of bone panaris dominated local changes. The x-ray revealed the heterogeneity of the bone structure in 4 patients, the violation of the integrity of the cortical layer in 1 child, marginal bone destruction phalanx in 43 children, sequestration of the nail phalanx in 3 patients, no changes were detected in 13 patients. Treatment of bone panaris surgery. In the complex post-operative care included: anti-bacterial, antihistamines, preparation that improve blood rheology and local treatment with antiseptic bandage, physiotherapy. Diagnosis of bone panaris based on clinical and radiological data. The main method of treatment is surgicalΠ‘Π°ΠΌΡΠΌ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½Π½ΡΠΌ Π³Π½ΠΎΠΉΠ½ΠΎ-Π²ΠΎΡΠΏΠ°Π»ΠΈΡΠ΅Π»ΡΠ½ΡΠΌ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠ΅ΠΌ ΠΊΠΈΡΡΠΈ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΏΠ°Π½Π°ΡΠΈΡΠΈΠΉ. ΠΠ°Π½Π°ΡΠΈΡΠΈΠΉ β ΠΎΡΡΡΠΎΠ΅ Π³Π½ΠΎΠΉΠ½ΠΎΠ΅ Π²ΠΎΡΠΏΠ°Π»Π΅Π½ΠΈΠ΅ ΡΠΊΠ°Π½Π΅ΠΉ ΠΏΠ°Π»ΡΡΠ°. Π€ΠΎΡΠΌΡ ΠΏΠ°Π½Π°ΡΠΈΡΠΈΡ, ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π°ΡΡΠΈΠ΅ΡΡ ΠΏΠΎΡΠ°ΠΆΠ΅Π½ΠΈΡΠΌΠΈ ΠΊΠΎΡΡΠ΅ΠΉ, Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡΠ»ΠΎΠΆΠ½Ρ Π΄Π»Ρ Π»Π΅ΡΠ΅Π½ΠΈΡ. ΠΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Ρ ΠΈΡΡΠΎΡΠΈΠΈ Π±ΠΎΠ»Π΅Π·Π½ΠΈ 64 Π΄Π΅ΡΠ΅ΠΉ, Π³ΠΎΡΠΏΠΈΡΠ°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
Π² ΠΎΡΠ΄Π΅Π»Π΅Π½ΠΈΠ΅ Π³Π½ΠΎΠΉΠ½ΠΎΠΉ Ρ
ΠΈΡΡΡΠ³ΠΈΠΈ ΠΠΠΠ β 9 Π·Π° 2017-2019 Π³ΠΎΠ΄Ρ Ρ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΏΠ°Π½Π°ΡΠΈΡΠΈΠ΅ΠΌ ΠΊΠΎΡΡΠΈ. Π ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ ΠΏΡΠΎΠ΄ΠΎΠ»ΠΆΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΡ Π΄ΠΎ ΠΎΠ±ΡΠ°ΡΠ΅Π½ΠΈΡ ΠΊ Ρ
ΠΈΡΡΡΠ³Ρ ΡΠΎΡΡΠ°Π²ΠΈΠ»Π° Π² ΡΡΠ΅Π΄Π½Π΅ΠΌ 5,8 Π΄Π½Ρ. 37,5% ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΏΡΠΎΡΠ»ΠΈ ΡΠ°ΠΌΠΎΠ»Π΅ΡΠ΅Π½ΠΈΠ΅. ΠΠΌΠ±ΡΠ»Π°ΡΠΎΡΠ½ΠΎΠ΅ Π»Π΅- ΡΠ΅Π½ΠΈΠ΅ Ρ
ΠΈΡΡΡΠ³ΠΎΠΌ ΠΏΠΎ ΠΌΠ΅ΡΡΡ ΠΆΠΈΡΠ΅Π»ΡΡΡΠ²Π° ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΎΡΡ Π² 32,8% ΡΠ»ΡΡΠ°Π΅Π². ΠΡΠΈ Π°Π½Π°Π»ΠΈΠ·Π΅ Π°Π½Π°ΠΌΠ½Π΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π΄Π°Π½Π½ΡΡ
Ρ 14 Π΄Π΅ΡΠ΅ΠΉ ΡΠ°Π·Π²ΠΈΡΠΈΠ΅ ΠΊΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠ°Π½Π°ΡΠΈΡΠΈΡ ΠΏΡΠΎΠΈΠ·ΠΎΡΠ»ΠΎ ΠΏΠΎΡΠ»Π΅ ΡΡΠ°Π²ΠΌΡ. Π Π±ΠΎΠ»ΡΡΠΈΠ½ΡΡΠ²Π΅ ΡΠ»ΡΡΠ°Π΅Π² ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½Π° Π΄ΠΈΡΡΠ°Π»ΡΠ½Π°Ρ ΡΠ°Π»Π°Π½Π³Π° Π²ΡΠΎΡΠΎΠ³ΠΎ ΠΏΠ°Π»ΡΡΠ° Π»Π΅Π²ΠΎΠΉ ΠΈ ΠΏΡΠ°Π²ΠΎΠΉ ΠΊΠΈΡΡΠΈ. ΠΡΠ΅ Π±ΠΎΠ»ΡΠ½ΡΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ²Π»ΡΠ»ΠΈ ΠΆΠ°Π»ΠΎΠ±Ρ Π½Π° Π±ΠΎΠ»ΠΈ Π² ΠΏΠ°Π»ΡΡΠ΅, ΠΎΡΠ΅ΠΊΠΈ, Π»ΠΎΠΊΠ°Π»ΡΠ½ΡΡ Π³ΠΈΠΏΠ΅ΡΠ΅ΠΌΠΈΡ ΠΊΠΎΠΆΠΈ. Π ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΊΠ°ΡΡΠΈΠ½Π΅ ΠΊΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠ°Π½Π°ΡΠΈΡΠΈΡ ΠΏΡΠ΅ΠΎΠ±Π»Π°Π΄Π°Π»ΠΈ ΠΌΠ΅ΡΡΠ½ΡΠ΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ. Π Π΅Π½ΡΠ³Π΅Π½ Π²ΡΡΠ²ΠΈΠ» Π½Π΅ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΡΡΡ ΡΡΡΡΠΊΡΡΡΡ ΠΊΠΎΡΡΠΈ Ρ 4 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², Π½Π°ΡΡΡΠ΅Π½ΠΈΠ΅ ΡΠ΅Π»ΠΎΡΡΠ½ΠΎΡΡΠΈ ΠΊΠΎΡΡΠΈΠΊΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ Ρ 1 ΡΠ΅Π±Π΅Π½ΠΊΠ°, ΡΠ°Π·ΡΡΡΠ΅Π½ΠΈΠ΅ ΠΊΡΠ°Π΅Π²ΠΎΠΉ ΡΠ°Π»Π°Π½Π³ΠΈ ΠΊΠΎΡΡΠΈ Ρ 43 Π΄Π΅ΡΠ΅ΠΉ, ΡΠ΅ΠΊΠ²Π΅ΡΡΡΠ°ΡΠΈΡ ΡΠ°Π»Π°Π½Π³ΠΈ Π½ΠΎΠ³ΡΡ Ρ 3 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ Π½Π΅ Π²ΡΡΠ²Π»Π΅Π½ΠΎ Ρ 13 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ². ΠΠ΅ΡΠ΅Π½ΠΈΠ΅ ΠΊΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠ°Π½Π°ΡΠΈΡΠΈΡ Ρ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ΅. Π ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡ ΠΏΠΎΡΠ»Π΅ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΡ
ΠΎΠ΄Π° Π²Ρ
ΠΎΠ΄ΡΡ: Π°Π½ΡΠΈΠ±Π°ΠΊΡΠ΅ΡΠΈΠ°Π»ΡΠ½ΡΠ΅, Π°Π½ΡΠΈΠ³ΠΈΡΡΠ°ΠΌΠΈΠ½Π½ΡΠ΅ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΡ, ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΡ, ΡΠ»ΡΡΡΠ°ΡΡΠΈΠ΅ ΡΠ΅ΠΎΠ»ΠΎΠ³ΠΈΡ ΠΊΡΠΎΠ²ΠΈ, ΠΈ ΠΌΠ΅ΡΡΠ½ΠΎΠ΅ Π»Π΅ΡΠ΅Π½ΠΈΠ΅ Π°Π½ΡΠΈΡΠ΅ΠΏΡΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΏΠΎΠ²ΡΠ·ΠΊΠ°ΠΌΠΈ, ΡΠΈΠ·ΠΈΠΎΡΠ΅ΡΠ°ΠΏΠΈΡ. ΠΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠ° ΠΊΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠ°Π½Π°ΡΠΈΡΠΈΡ ΠΎΡΠ½ΠΎΠ²Π°Π½Π° Π½Π° ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
Π΄Π°Π½Π½ΡΡ
. ΠΡΠ½ΠΎΠ²Π½ΡΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ Π»Π΅ΡΠ΅Π½ΠΈΡ ΡΠ²Π»ΡΠ΅ΡΡΡ Ρ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΈ
Continuity theorems for the queueing system
In this paper continuity theorems are established for the number of losses
during a busy period of the queue. We consider an queueing
system where the service time probability distribution, slightly different in a
certain sense from the exponential distribution, is approximated by that
exponential distribution. Continuity theorems are obtained in the form of one
or two-sided stochastic inequalities. The paper shows how the bounds of these
inequalities are changed if further assumptions, associated with specific
properties of the service time distribution (precisely described in the paper),
are made. Specifically, some parametric families of service time distributions
are discussed, and the paper establishes uniform estimates (given for all
possible values of the parameter) and local estimates (where the parameter is
fixed and takes only the given value). The analysis of the paper is based on
the level crossing approach and some characterization properties of the
exponential distribution.Comment: Final revision; will be published as i
Dynamics of soil freezing and thawing in the agroforestry landscape
The article presents the dynamics of soil freezing and thawing in the agroforestry landscape of the dry-steppe zone. These processes in winters with unstable snow cover have their own characteristics. The purpose of this study was to investigate the character of soil freezing and thawing in the agroforestry landscape under conditions of low snowfall winters. Observations were carried out in the winter period of 2020β2021 at the existing runoff-erosion research station in Volgograd. The dynamics of soil freezing and thawing was studied using Danilin freeze-thaw meters installed in the field and in the center of a four-row forest belt. Simultaneously, snow cover height was measured in triplicate with a snow measuring rod. The weather conditions were characterized by alternating thaws, which promoted snow cover melt, and frosts, which increased the depth of soil freezing. The formation of a 10-15 cm snow cover did not affect soil freezing. In the absence of snow on the background of a brief thaw, the lower boundary of the frozen layer in the field decreased by 11 cm compared to the forest belt, which even in the leafless state affected the inflow of solar thermal energy. Average freezing at the end of winter was 85 cm in the field and 67 cm in the forest belt. Thawing in the field was faster. During the first two weeks, the rate of soil thawing averaged 2.3 cm/day in the field and 1.3 cm/day in the forest belt. After that, the depth of freezing in the whole agroforestry landscape became equal. During the next two weeks, the thawing rate doubled. After complete soil thawing in the field in the forest belt, the thickness of the frozen layer averaged 32 cm
On the frequency of oscillations in the pair plasma generated by a strong electric field
We study the frequency of the plasma oscillations of electron-positron pairs
created by the vacuum polarization in an uniform electric field with strength E
in the range 0.2 Ec < E < 10 Ec. Following the approach adopted in [1] we work
out one second order ordinary differential equation for a variable related to
the velocity from which we can recover the classical plasma oscillation
equation when E -> 0. Thereby, we focus our attention on its evolution in time
studying how this oscillation frequency approaches the plasma frequency. The
time-scale needed to approach to the plasma frequency and the power spectrum of
these oscillations are computed. The characteristic frequency of the power
spectrum is determined uniquely from the initial value of the electric field
strength. The effects of plasma degeneracy and pair annihilation are discussed.Comment: to appear in Physics Letters
Phase-sensitive amplification of 11 WDM channels across bandwidth of 8 nm in a fibre optic parametric amplifier
We experimentally demonstrate phase-sensitive fibre optic parametric amplification with gain >10dB and optical noise figure below 3dB for 11 channels spaced of 100 GHz. We employ all-fibre dispersion management to achieve a wideband phase-matching between signals and their copies
Ground Beetles (Coleoptera, Carabidae) Assemblages Features Formation in Large and Medium Industrial Cities of Russia (The Case Study in Kazan, Kemerovo and Grozny)
The article presents the results of the analysis of the Carabid fauna of three cities: Grozny, Kemerovo, Kazan. It was established that communities of ground beetles clearly respond to varying degrees of recreation by changing the biotopic distribution and ecological structure: the emergence of super dominant species, a decrease in the abundance of zoophages, an increase in the share of stratobionts, and the presence of indicator species
The Bubble regime of laser-plasma acceleration: monoenergetic electrons and the scalability
The Bubble regime of electron acceleration in ultra-relativistic laser plasma
is considered. It has been shown that the bubble can produce ultra-short dense
bunches of electrons with quasi-monoenergetic energy spectra. The first
experiment in this regime done at LOA has confirmed the peaked electron
spectrum (J. Faure, et al., {\it submitted}, 2004). The generated electron
bunch may have density an order of magnitude higher than that of the background
plasma. The bubble is able to guide the laser pulse over many Rayleigh lengths,
thus no preformed plasma channel is needed for high-energy particle
acceleration in the bubble regime. In the present work we discuss a simple
analytical model for the bubble fields as well as the scaling laws.Comment: accepted for publication in Plasma Physics and Controlled Fusion,
200
Strong laser fields as a probe for fundamental physics
Upcoming high-intensity laser systems will be able to probe the
quantum-induced nonlinear regime of electrodynamics. So far unobserved QED
phenomena such as the discovery of a nonlinear response of the quantum vacuum
to macroscopic electromagnetic fields can become accessible. In addition, such
laser systems provide for a flexible tool for investigating fundamental
physics. Primary goals consist in verifying so far unobserved QED phenomena.
Moreover, strong-field experiments can search for new light but weakly
interacting degrees of freedom and are thus complementary to accelerator-driven
experiments. I review recent developments in this field, focusing on photon
experiments in strong electromagnetic fields. The interaction of
particle-physics candidates with photons and external fields can be
parameterized by low-energy effective actions and typically predict
characteristic optical signatures. I perform first estimates of the accessible
new-physics parameter space of high-intensity laser facilities such as POLARIS
and ELI.Comment: 7 pages, Key Lecture at the ELI Workshop and School on "Fundamental
Physics with Ultra-High Fields", 9 September - 2 October 2008 at Frauenworth
Monastery, German
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