907 research outputs found
Nonlinear acoustic waves in channels with variable cross sections
The point symmetry group is studied for the generalized Webster-type equation
describing non-linear acoustic waves in lossy channels with variable cross
sections. It is shown that, for certain types of cross section profiles, the
admitted symmetry group is extended and the invariant solutions corresponding
to these profiles are obtained. Approximate analytic solutions to the
generalized Webster equation are derived for channels with smoothly varying
cross sections and arbitrary initial conditions.Comment: Revtex4, 10 pages, 2 figure. This is an enlarged contribution to
Acoustical Physics, 2012, v.58, No.3, p.269-276 with modest stylistic
corrections introduced mainly in the Introduction and References. Several
typos were also correcte
Formation of system of support of development of small youth business
The results of the research of youth entrepreneurship problems have been adduced. Institutions and programs of its support have been considered. Measures to eliminate the identified problems of attracting young people to entrepreneurship have been recommended. The formation of a new program of support Β«Acceleration of youth entrepreneurshipΒ» and the creation of coordination centers in the subjects of the Russian Federation Β«Regional youth centerΒ» have been off red. The model of the system of support of small youth entrepreneurship, which will increase entrepreneurial activity among young people and create new jobs, has been presented
Development of the A/H6N1 influenza vaccine candidate based on A/Leningrad/134/17/57 (H2N2) master donor virus and the genome composition analysis using high resolution melting (HRM)
The avian influenza viruses of H6N1subtype present a potential danger for humans. The cold-adapted (ca) reassortant influenza virus Π/17/herring gull/Sarma/2006/887 (H6N1) was obtained in chicken embryos by the genetic reassortment based on the coldadapted A/Leningrad/134/17/57 (H2N2) master strain. The genome composition of the obtained reassortant was analyzed by means of real-time PCR with the high resolution melting (HRM) analysis using the intercalating fluorescent dye EvaGreen. Analysis of the gene segments showed that the reassortant Π/17/herring gull/Sarma/2006/887 (H6N1) contains the internal proteins coding genes (PB2, PB1, PA, NP, M, and NS) of the master donor virus and the surface antigens coding genes of the A/herring gull/Sarma/51c/2006 (H6N1) avian influenza virus. The study of the phenotypic properties showed that the virus Π/17/herring gull/Sarma/2006/887 (H6N1) is temperature sensitive (ts), ca in chicken embryos, and attenuated in mice when administered intranasally. This reassortant can be recommended as a live influenza vaccine candidate for humans.The avian influenza viruses of H6N1subtype present a potential danger for humans. The cold-adapted (ca) reassortant influenza virus Π/17/herring gull/Sarma/2006/887 (H6N1) was obtained in chicken embryos by the genetic reassortment based on the coldadapted A/Leningrad/134/17/57 (H2N2) master strain. The genome composition of the obtained reassortant was analyzed by means of real-time PCR with the high resolution melting (HRM) analysis using the intercalating fluorescent dye EvaGreen. Analysis of the gene segments showed that the reassortant Π/17/herring gull/Sarma/2006/887 (H6N1) contains the internal proteins coding genes (PB2, PB1, PA, NP, M, and NS) of the master donor virus and the surface antigens coding genes of the A/herring gull/Sarma/51c/2006 (H6N1) avian influenza virus. The study of the phenotypic properties showed that the virus Π/17/herring gull/Sarma/2006/887 (H6N1) is temperature sensitive (ts), ca in chicken embryos, and attenuated in mice when administered intranasally. This reassortant can be recommended as a live influenza vaccine candidate for humans
Very high frequency gravitational wave background in the universe
Astrophysical sources of high frequency gravitational radiation are
considered in association with a new interest to very sensitive HFGW receivers
required for the laboratory GW Hertz experiment. A special attention is paid to
the phenomenon of primordial black holes evaporation. They act like black body
to all kinds of radiation, including gravitons, and, therefore, emit an
equilibrium spectrum of gravitons during its evaporation. Limit on the density
of high frequency gravitons in the Universe is obtained, and possibilities of
their detection are briefly discussed.Comment: 14 page
Wavelength and intensity dependence of multiple forward scattering at above-threshold ionization in mid-infrared strong laser fields
The nonperturbative role of multiple forward scattering for Coulomb focusing
in mid-infrared laser fields and its dependence on a laser intensity and
wavelength are investigated for low-energy photoelectrons at above-threshold
ionization. We show that high-order rescattering events can have comparable
contributions to the Coulomb focusing and the effective number of rescattering
depends weakly on laser parameters in the classical regime. However, the
relative contribution of the forward scattering to the Coulomb focusing and the
Coulomb focusing in total decrease with the rise of the laser intensity and
wavelength
A divergent spirochete strain isolated from a resident of the southeastern United States was identified by multilocus sequence typing as Borrelia bissettii.
Atmospheric Gravity Perturbations Measured by Ground-Based Interferometer with Suspended Mirrors
A possibility of geophysical measurements using the large scale laser
interferometrical gravitational wave antenna is discussed. An interferometer
with suspended mirrors can be used as a gradiometer measuring variations of an
angle between gravity force vectors acting on the spatially separated
suspensions. We analyze restrictions imposed by the atmospheric noises on
feasibility of such measurements. Two models of the atmosphere are invoked: a
quiet atmosphere with a hydrostatic coupling of pressure and density and a
dynamic model of moving region of the density anomaly (cyclone). Both models
lead to similar conclusions up to numerical factors. Besides the hydrostatic
approximation, we use a model of turbulent atmosphere with the pressure
fluctuation spectrum f^{-7/3} to explore the Newtonian noise in a higher
frequency domain (up to 10 Hz) predicting the gravitational noise background
for modern gravitational wave detectors. Our estimates show that this could
pose a serious problem for realization of such projects. Finally, angular
fluctuations of spatially separated pendula are investigated via computer
simulation for some realistic atmospheric data giving the level estimate
10^{-11} rad/sqrt(Hz) at frequency 10^{-4} Hz. This looks promising for the
possibility of the measurement of weak gravity effects such as Earth inner core
oscillations.Comment: 13 pages, 4 pigures, LaTeX. To be published in Classical and Quantum
Gravit
Π Π°ΡΡΡΡ ΠΏΠΎΠΏΡΠ°Π²ΠΎΡΠ½ΡΡ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠ² ΠΏΡΠΈ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΈ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ ΠΏΠΎ ΠΠΈΠΊΠΊΠ΅ΡΡΡ Π½Π° Π½Π΅ΠΏΠ»ΠΎΡΠΊΠΎΠΉ ΠΏΠΎΠ²Π΅ΡΡ Π½ΠΎΡΡΠΈ
The exact determination of Vickers HV hardness is important for determining of the product material mechanical properties. An important aspect of measuring HV is to obtain its values on a non-planar surface. Regulatory documents contain table values of correction factorsΒ KΒ which depend on the surface shape (convex or concave, spherical or cylindrical), its curvature (diameterΒ D) and hardness (arithmetic meanΒ dΒ of indentation diagonal lengths) but this does not solved the problem. TheΒ KΒ values forΒ d/DΒ ratios not given in the tables are determined by interpolation from the closest to the measured tabulatedΒ d/DΒ values. The error in the representation of these tabulatedΒ d/DΒ values is fully included in the error of determining theΒ KΒ coefficient for the measuredΒ d/DΒ ratio. The aim of the work was to simplify the calculation of correction factorsΒ KΒ for Vickers hardness measurements on non-planar surfaces and to reduce the calculation error compared to the methodology governed by the regulations.The method presented is based on a statistical analysis ofΒ KΒ coefficients, presented in regulatory documents for cases considered in the form of tables. The sufficiency of using of a quadratic power function for approximatingΒ K(d/D) dependences and the necessity of fulfilling the physically justified conditionΒ KΒ β‘ 1 at zero curvature of tested surface have been substantiated. Simplification of calculation ofΒ KΒ coefficient and decrease of calculation error in comparison with the recommended in the regulatory documents obtaining ofΒ KΒ value by linear interpolation relative to two adjacent table values are shown.The reduction of the calculation error in comparison with the calculation recommended in the regulatory documents occurred because of the reason that when calculating by the developed formulas, the error in the value of the calculated for a specific value ofΒ d/DΒ coefficientΒ KΒ is averaged over all n values ofΒ d/DΒ given in the table of GOST for a given surface. That is, the error is reduced by a factor of about βn 2 in comparison with the calculation according to the regulated procedure. This is illustrated by the above numerical data and an example of the use of the method.The obtained formulas for calculation of correction coefficientsΒ KΒ when measuring hardness HV on spherical and cylindrical (concave and convex) surfaces are reasonable to use for automatic calculation of HV on items with a non-planar surface.Π’ΠΎΡΠ½ΠΎΠ΅ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ HV ΠΏΠΎ ΠΠΈΠΊΠΊΠ΅ΡΡΡ Π²Π°ΠΆΠ½ΠΎ Π΄Π»Ρ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ²ΠΎΠΉΡΡΠ² ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π° ΠΈΠ·Π΄Π΅Π»ΠΈΠΉ. ΠΠ°ΠΆΠ½ΡΠΌ Π°ΡΠΏΠ΅ΠΊΡΠΎΠΌ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ HV ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΠ΅ Π΅Ρ Π·Π½Π°ΡΠ΅Π½ΠΈΠΉ Π½Π° Π½Π΅ΠΏΠ»ΠΎΡΠΊΠΎΠΉ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ. ΠΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅ Π² Π½ΠΎΡΠΌΠ°ΡΠΈΠ²Π½ΡΠ΅ Π΄ΠΎΠΊΡΠΌΠ΅Π½ΡΡ ΡΠ°Π±Π»ΠΈΡΠ½ΡΡ
Π·Π½Π°ΡΠ΅Π½ΠΈΠΉ ΠΏΠΎΠΏΡΠ°Π²ΠΎΡΠ½ΡΡ
ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠ²Β Π, Π·Π°Π²ΠΈΡΡΡΠΈΡ
ΠΎΡ ΡΠΎΡΠΌΡ (Π²ΡΠΏΡΠΊΠ»Π°Ρ ΠΈΠ»ΠΈ Π²ΠΎΠ³Π½ΡΡΠ°Ρ, ΡΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΈΠ»ΠΈ ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠ°Ρ) ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ, Π΅Ρ ΠΊΡΠΈΠ²ΠΈΠ·Π½Ρ (Π΄ΠΈΠ°ΠΌΠ΅ΡΡΠ°Β D) ΠΈ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ (ΡΡΠ΅Π΄Π½Π΅Π³ΠΎ Π°ΡΠΈΡΠΌΠ΅ΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎΒ dΒ Π΄Π»ΠΈΠ½ Π΄ΠΈΠ°Π³ΠΎΠ½Π°Π»Π΅ΠΉ ΠΎΡΠΏΠ΅ΡΠ°ΡΠΊΠ°) Π½Π΅ ΡΠ΅ΡΠ°Π΅Ρ ΠΏΡΠΎΠ±Π»Π΅ΠΌΡ. ΠΠ½Π°ΡΠ΅Π½ΠΈΡΒ ΠΒ Π΄Π»Ρ ΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΠΉΒ d/D, Π½Π΅ ΠΏΡΠΈΠ²Π΅Π΄ΡΠ½Π½ΡΡ
Π² ΡΠ°Π±Π»ΠΈΡΠ°Ρ
, ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΡΡ ΠΈΠ½ΡΠ΅ΡΠΏΠΎΠ»ΡΡΠΈΠ΅ΠΉ ΠΎΡ Π±Π»ΠΈΠΆΠ°ΠΉΡΠΈΡ
ΠΊ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½Π½ΠΎΠΌΡ ΡΠ°Π±Π»ΠΈΡΠ½ΡΡ
Π·Π½Π°ΡΠ΅Π½ΠΈΠΉΒ d/D. ΠΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΡ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΈΡ ΡΡΠΈΡ
ΡΠ°Π±Π»ΠΈΡΠ½ΡΡ
Π·Π½Π°ΡΠ΅Π½ΠΈΠΉΒ d/DΒ ΠΏΠΎΠ»Π½ΠΎΡΡΡΡ Π²ΠΊΠ»ΡΡΠ°Π΅ΡΡΡ Π² ΠΏΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΠΈΡΠΊΠΎΠΌΠΎΠ³ΠΎ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ°Β ΠΒ Π΄Π»Ρ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΡΒ d/D. Π¦Π΅Π»Ρ ΡΠ°Π±ΠΎΡΡ β ΡΠΏΡΠΎΡΠ΅Π½ΠΈΠ΅ ΡΠ°ΡΡΡΡΠ° ΠΏΠΎΠΏΡΠ°Π²ΠΎΡΠ½ΡΡ
ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠ²Β ΠΒ ΠΏΡΠΈ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΈ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ ΠΏΠΎ ΠΠΈΠΊΠΊΠ΅ΡΡΡ Π½Π° Π½Π΅ΠΏΠ»ΠΎΡΠΊΠΈΡ
ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΡΡ
ΠΈ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΠΏΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΠΈ ΡΠ°ΡΡΡΡΠ° ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΎΠΉ, ΡΠ΅Π³Π»Π°ΠΌΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ Π½ΠΎΡΠΌΠ°ΡΠΈΠ²Π½ΡΠΌΠΈ Π΄ΠΎΠΊΡΠΌΠ΅Π½ΡΠ°ΠΌΠΈ.Π Π°Π·ΡΠ°Π±ΠΎΡΠΊΠ° ΠΎΡΠ½ΠΎΠ²Π°Π½Π° Π½Π° ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΎΠΌ Π°Π½Π°Π»ΠΈΠ·Π΅ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠ²Β Π, ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Π½ΡΡ
Π² Π½ΠΎΡΠΌΠ°ΡΠΈΠ²Π½ΡΡ
Π΄ΠΎΠΊΡΠΌΠ΅Π½ΡΠ°Ρ
Π΄Π»Ρ ΡΠ°ΡΡΠΌΠΎΡΡΠ΅Π½Π½ΡΡ
ΡΠ»ΡΡΠ°Π΅Π² Π² Π²ΠΈΠ΄Π΅ ΡΠ°Π±Π»ΠΈΡ. ΠΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½Π° Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΠΊΠ²Π°Π΄ΡΠ°ΡΠΈΡΠ½ΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½Π½ΠΎΠΉ ΡΡΠ½ΠΊΡΠΈΠΈ Π΄Π»Ρ Π°ΠΏΠΏΡΠΎΠΊΡΠΈΠΌΠ°ΡΠΈΠΈ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠ΅ΠΉΒ Π(d/D) ΠΈ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎΡΡΡ Π²ΡΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΈ ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΡΠ»ΠΎΠ²ΠΈΡΒ ΠΒ β‘ 1 ΠΏΡΠΈ Π½ΡΠ»Π΅Π²ΠΎΠΉ ΠΊΡΠΈΠ²ΠΈΠ·Π½Π΅ ΠΈΡΠΏΡΡΡΠ΅ΠΌΠΎΠΉ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ ΡΠΏΡΠΎΡΠ΅Π½ΠΈΠ΅ ΡΠ°ΡΡΡΡΠ° ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ°Β ΠΒ ΠΈ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΠΏΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΠΈ ΡΠ°ΡΡΡΡΠ° ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄ΠΎΠ²Π°Π½Π½ΡΠΌ Π² Π½ΠΎΡΠΌΠ°ΡΠΈΠ²Π½ΡΡ
Π΄ΠΎΠΊΡΠΌΠ΅Π½ΡΠ°Ρ
ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΠ΅ΠΌ Π·Π½Π°ΡΠ΅Π½ΠΈΡΒ ΠΒ Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΉ ΠΈΠ½ΡΠ΅ΡΠΏΠΎΠ»ΡΡΠΈΠ΅ΠΉ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π΄Π²ΡΡ
ΡΠΎΡΠ΅Π΄Π½ΠΈΡ
ΡΠ°Π±Π»ΠΈΡΠ½ΡΡ
Π·Π½Π°ΡΠ΅Π½ΠΈΠΉ.Π‘Π½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΠΏΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΠΈ ΡΠ°ΡΡΡΡΠ° ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΡΠ°ΡΡΡΡΠΎΠΌ, ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄ΠΎΠ²Π°Π½Π½ΡΠΌ Π² Π½ΠΎΡΠΌΠ°ΡΠΈΠ²Π½ΡΡ
Π΄ΠΎΠΊΡΠΌΠ΅Π½ΡΠ°Ρ
, ΠΏΡΠΎΠΈΡΡ
ΠΎΠ΄ΠΈΡ Π·Π° ΡΡΡΡ ΡΠΎΠ³ΠΎ, ΡΡΠΎ ΠΏΡΠΈ ΡΠ°ΡΡΡΡΠ΅ ΠΏΠΎ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π½ΡΠΌ ΡΠΎΡΠΌΡΠ»Π°ΠΌ ΠΏΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΡ Π² Π·Π½Π°ΡΠ΅Π½ΠΈΠΈ ΡΠ°ΡΡΡΠΈΡΠ°Π½Π½ΠΎΠ³ΠΎ Π΄Π»Ρ ΠΊΠΎΠ½ΠΊΡΠ΅ΡΠ½ΠΎΠ³ΠΎ Π·Π½Π°ΡΠ΅Π½ΠΈΡΒ d/DΒ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ°Β ΠΒ ΡΡΡΠ΅Π΄Π½ΡΠ΅ΡΡΡ ΠΏΠΎ Π²ΡΠ΅ΠΌΒ nΒ Π·Π½Π°ΡΠ΅Π½ΠΈΡΠΌΒ d/D, ΠΏΡΠΈΠ²Π΅Π΄ΡΠ½Π½ΡΠΌ Π² ΡΠ°Π±Π»ΠΈΡΠ΅ ΠΠΠ‘Π’Π° Π΄Π»Ρ Π΄Π°Π½Π½ΠΎΠΉ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ. Π’ΠΎ Π΅ΡΡΡ ΡΠ½ΠΈΠΆΠ°Π΅ΡΡΡ ΠΏΡΠΈΠΌΠ΅ΡΠ½ΠΎ Π² βn 2 ΡΠ°Π· ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΡΠ°ΡΡΡΡΠΎΠΌ ΠΏΠΎ ΡΠ΅Π³Π»Π°ΠΌΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ΅. ΠΡΠΎ ΠΈΠ»Π»ΡΡΡΡΠΈΡΡΡΡ ΠΏΡΠΈΠ²Π΅Π΄ΡΠ½Π½ΡΠ΅ ΡΠΈΡΠ»Π΅Π½Π½ΡΠ΅ Π΄Π°Π½Π½ΡΠ΅ ΠΈ ΠΏΡΠΈΠΌΠ΅Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ.ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠΎΡΠΌΡΠ»Ρ Π΄Π»Ρ ΡΠ°ΡΡΡΡΠ° ΠΏΠΎΠΏΡΠ°Π²ΠΎΡΠ½ΡΡ
ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠ²Β ΠΒ ΠΏΡΠΈ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΈ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ HV Π½Π° ΡΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΈΡ
(Π²ΠΎΠ³Π½ΡΡΡΡ
ΠΈ Π²ΡΠΏΡΠΊΠ»ΡΡ
) ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΡΡ
ΡΠ΅Π»Π΅ΡΠΎΠΎΠ±ΡΠ°Π·Π½ΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°ΡΡ Π΄Π»Ρ Π°Π²ΡΠΎΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ°ΡΡΡΡΠ° HV Π½Π° ΠΈΠ·Π΄Π΅Π»ΠΈΡΡ
Ρ Π½Π΅ΠΏΠ»ΠΎΡΠΊΠΎΠΉ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΡΡ
ΠΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠΉ ΡΠΎΠ»ΡΠΈΠ½Ρ ΡΠ΅ΠΌΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ ΡΡΠ°Π»ΠΈ
Highly loaded transmission gears are cemented and hardened. An important parameter of the hardened cemented layer is its effective thickness hef . Metal banding and the unavoidable instrumental error in hardness measuring have a great influence on the reliability of hefΒ determination. The purpose of this article was to develop a methodology to improve the reliability of determining of the effective thickness hefΒ of the hardened layer in steel after carburizing and quenching.The value of hefΒ is the distance h from the surface of the product to the hardness zone of 50 HRC. The article substantiates that approximation of hardness change from the distance h to the product surface will allow to obtain a more reliable dependence of hardness change in the investigated area when making hardness measurements in a wider range of distance h. Therefore, to increase the reliability of hef determination, results of the HV0.5 hardness measurement in an extended range of changes in h in the vicinity of the analyzed zone were used. The HV0.5 measurement results are converted to HRC hardness values using the formula recommended by the international standard. The HRC(h) distribution of HRC hardness values in the measurement area is interpolated by a second-degree polynomial which physically correctly reflects the change in metal hardness in the analyzed area. The resulting polynomial is used to determine of the distance hef at which the hardness takes on a value of 50 HRC. The methodology was used to determine the hefΒ of an 18KhGT steel gear wheel after carburizing and quenching. It is shown that results of two independent measurements of the hef sample differ from each other by 0.003 mm. This is significantly less than the permissible error of 0.02 mm of the hefΒ determination according to the standard technique. The error of hef determination is reduced by extending the range of variation of h and statistically valid interpolation of the monotonic change in hardness with the distance from the surface of the item in the measurement area. The developed method of determining the effective thickness hefΒ of the hardened steel layer consists in determining the distribution of its hardness in the expanded vicinity of the hef area, approximating the obtained dependence by a polynomial of the second degree and solving the square equation obtained with its use. The technique provides a significant reduction in the influence of the structural banding of the metal and the inevitable error in measuring hardness on the result of determining the hefΒ . Its application will allow to optimize the cementation regimes of gear wheels to increase their service life.ΠΡΡΠΎΠΊΠΎΠ½Π°Π³ΡΡΠΆΠ΅Π½Π½ΡΠ΅ Π·ΡΠ±ΡΠ°ΡΡΠ΅ ΠΊΠΎΠ»ΡΡΠ° ΡΡΠ°Π½ΡΠΌΠΈΡΡΠΈΠΉ ΠΏΠΎΠ΄Π²Π΅ΡΠ³Π°ΡΡ ΡΠ΅ΠΌΠ΅Π½ΡΠ°ΡΠΈΠΈ ΠΈ Π·Π°ΠΊΠ°Π»ΠΊΠ΅. ΠΠ°ΠΆΠ½ΡΠΌ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠΌ ΡΠΏΡΠΎΡΠ½ΡΠ½Π½ΠΎΠ³ΠΎ ΡΠ΅ΠΌΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ ΡΠ²Π»ΡΠ΅ΡΡΡ Π΅Π³ΠΎ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½Π°Ρ ΡΠΎΠ»ΡΠΈΠ½Π° hefΒ . ΠΠΎΠ»ΡΡΠΎΠ΅ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΠΎΡΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ hefΒ ΠΎΠΊΠ°Π·ΡΠ²Π°ΡΡ ΠΏΠΎΠ»ΠΎΡΡΠ°ΡΠΎΡΡΡ ΠΌΠ΅ΡΠ°Π»Π»Π° ΠΈ Π½Π΅ΠΈΠ·Π±Π΅ΠΆΠ½Π°Ρ ΠΈΠ½ΡΡΡΡΠΌΠ΅Π½ΡΠ°Π»ΡΠ½Π°Ρ ΠΏΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΡ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ. Π¦Π΅Π»Ρ ΡΠ°Π±ΠΎΡΡ β ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠ° ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΡ Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΠΎΡΡΠΈ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠΉ ΡΠΎΠ»ΡΠΈΠ½Ρ hefΒ ΡΠΏΡΠΎΡΠ½ΡΠ½Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ Π² ΡΡΠ°Π»ΠΈ ΠΏΠΎΡΠ»Π΅ ΡΠ΅ΠΌΠ΅Π½ΡΠ°ΡΠΈΠΈ ΠΈ Π·Π°ΠΊΠ°Π»ΠΊΠΈ.ΠΠ° Π²Π΅Π»ΠΈΡΠΈΠ½Ρ hefΒ ΠΏΡΠΈΠ½ΠΈΠΌΠ°ΡΡ ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΠ΅ h ΠΎΡ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΈΠ·Π΄Π΅Π»ΠΈΡ Π΄ΠΎ Π·ΠΎΠ½Ρ Ρ ΡΠ²ΡΡΠ΄ΠΎΡΡΡΡ 50 HRC. Π ΡΠ°Π±ΠΎΡΠ΅ ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΎ, ΡΡΠΎ Π°ΠΏΠΏΡΠΎΠΊΡΠΈΠΌΠ°ΡΠΈΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ ΠΎΡ ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΡ h Π΄ΠΎ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΈΠ·Π΄Π΅Π»ΠΈΡ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΡ ΠΏΠΎΠ»ΡΡΠΈΡΡ Π±ΠΎΠ»Π΅Π΅ Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΡΡ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ Π² ΠΈΡΡΠ»Π΅Π΄ΡΠ΅ΠΌΠΎΠΉ Π·ΠΎΠ½Π΅ ΠΏΡΠΈ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠΈ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ Π² Π±ΠΎΠ»Π΅Π΅ ΡΠΈΡΠΎΠΊΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΠΉ h. ΠΠΎΡΡΠΎΠΌΡ Π΄Π»Ρ ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΡ Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΠΎΡΡΠΈ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ hefΒ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ HV0,5 Π² ΡΠ°ΡΡΠΈΡΠ΅Π½Π½ΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ h Π² ΠΎΠΊΡΠ΅ΡΡΠ½ΠΎΡΡΠΈ Π°Π½Π°Π»ΠΈΠ·ΠΈΡΡΠ΅ΠΌΠΎΠΉ Π·ΠΎΠ½Ρ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ HV0,5 ΠΏΠ΅ΡΠ΅ΡΡΠΈΡΠ°Π½Ρ Π² Π·Π½Π°ΡΠ΅Π½ΠΈΡ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ HRC ΠΏΠΎ ΡΠΎΡΠΌΡΠ»Π΅, ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄ΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΌΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΡΠΌ ΡΡΠ°Π½Π΄Π°ΡΡΠΎΠΌ. Π Π°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ HRC(h) Π·Π½Π°ΡΠ΅Π½ΠΈΠΉ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ HRC Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΠΈΠ½ΡΠ΅ΡΠΏΠΎΠ»ΠΈΡΠΎΠ²Π°Π½ΠΎ ΠΏΠΎΠ»ΠΈΠ½ΠΎΠΌΠΎΠΌ Π²ΡΠΎΡΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ, ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΈ Π²Π΅ΡΠ½ΠΎ ΠΎΡΡΠ°ΠΆΠ°ΡΡΠΈΠΌ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ ΠΌΠ΅ΡΠ°Π»Π»Π° Π² Π°Π½Π°Π»ΠΈΠ·ΠΈΡΡΠ΅ΠΌΠΎΠΉ Π·ΠΎΠ½Π΅. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠΉ ΠΏΠΎΠ»ΠΈΠ½ΠΎΠΌ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ Π΄Π»Ρ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΡ hefΒ , ΠΏΡΠΈ ΠΊΠΎΡΠΎΡΠΎΠΌ ΡΠ²ΡΡΠ΄ΠΎΡΡΡ ΠΏΡΠΈΠ½ΠΈΠΌΠ°Π΅Ρ Π·Π½Π°ΡΠ΅Π½ΠΈΠ΅ 50 HRC. ΠΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Π° Π΄Π»Ρ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ hefΒ Π·ΡΠ±ΡΠ°ΡΠΎΠ³ΠΎ ΠΊΠΎΠ»Π΅ΡΠ° ΠΈΠ· ΡΡΠ°Π»ΠΈ 18Π₯ΠΠ’ ΠΏΠΎΡΠ»Π΅ ΡΠ΅ΠΌΠ΅Π½ΡΠ°ΡΠΈΠΈ ΠΈ Π·Π°ΠΊΠ°Π»ΠΊΠΈ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ Π΄Π²ΡΡ
Π½Π΅Π·Π°Π²ΠΈΡΠΈΠΌΡΡ
ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ hefΒ ΠΎΠ±ΡΠ°Π·ΡΠ° ΠΎΡΠ»ΠΈΡΠ°ΡΡΡΡ Π΄ΡΡΠ³ ΠΎΡ Π΄ΡΡΠ³Π° Π½Π° 0,003 ΠΌΠΌ. ΠΡΠΎ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ ΠΌΠ΅Π½ΡΡΠ΅ Π΄ΠΎΠΏΡΡΡΠΈΠΌΠΎΠΉ ΠΏΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΠΈ 0,02 ΠΌΠΌ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ hefΒ ΠΏΠΎ ΡΡΠ°Π½Π΄Π°ΡΡΠ½ΠΎΠΉ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ΅. ΠΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ hefΒ ΡΠ½ΠΈΠΆΠ΅Π½Π° Π·Π° ΡΡΡΡ ΡΠ°ΡΡΠΈΡΠ΅Π½ΠΈΡ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π° ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ h ΠΈ ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈ ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΈΠ½ΡΠ΅ΡΠΏΠΎΠ»ΡΡΠΈΠΈ ΠΌΠΎΠ½ΠΎΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ Ρ ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΠ΅ΠΌ ΠΎΡ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΈΠ·Π΄Π΅Π»ΠΈΡ Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ.Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π½Π°Ρ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠΉ ΡΠΎΠ»ΡΠΈΠ½Ρ hefΒ ΡΠΏΡΠΎΡΠ½ΡΠ½Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ ΡΡΠ°Π»ΠΈ Π·Π°ΠΊΠ»ΡΡΠ°Π΅ΡΡΡ Π² ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠΈ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ Π΅Ρ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ Π² ΡΠ°ΡΡΠΈΡΠ΅Π½Π½ΠΎΠΉ ΠΎΠΊΡΠ΅ΡΡΠ½ΠΎΡΡΠΈ ΠΎΠ±Π»Π°ΡΡΠΈ hefΒ , Π°ΠΏΠΏΡΠΎΠΊΡΠΈΠΌΠ°ΡΠΈΠΈ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΠΎΠΉ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΏΠΎΠ»ΠΈΠ½ΠΎΠΌΠΎΠΌ Π²ΡΠΎΡΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ ΠΈ ΡΠ΅ΡΠ΅Π½ΠΈΠΈ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΠΎΠ³ΠΎ Ρ Π΅Π³ΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΊΠ²Π°Π΄ΡΠ°ΡΠ½ΠΎΠ³ΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ. ΠΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°Π΅Ρ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ΅ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ Π²Π»ΠΈΡΠ½ΠΈΡ ΡΡΡΡΠΊΡΡΡΠ½ΠΎΠΉ ΠΏΠΎΠ»ΠΎΡΡΠ°ΡΠΎΡΡΠΈ ΠΌΠ΅ΡΠ°Π»Π»Π° ΠΈ Π½Π΅ΠΈΠ·Π±Π΅ΠΆΠ½ΠΎΠΉ ΠΏΠΎΠ³ΡΠ΅ΡΠ½ΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΡΠ²ΡΡΠ΄ΠΎΡΡΠΈ Π½Π° ΡΠ΅Π·ΡΠ»ΡΡΠ°Ρ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ hefΒ . ΠΡ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΡ ΠΎΠΏΡΠΈΠΌΠΈΠ·ΠΈΡΠΎΠ²Π°ΡΡ ΡΠ΅ΠΆΠΈΠΌΡ ΡΠ΅ΠΌΠ΅Π½ΡΠ°ΡΠΈΠΈ Π·ΡΠ±ΡΠ°ΡΡΡ
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