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Featured researches published by S. A. Losev.


32nd Thermophysics Conference | 1997

Modeling of diatomic molecules dissociation under quasistationary conditions

O. P. Shatalov; S. A. Losev

The description of high-temperature chemically reacting gas flow requires the model representations of chemical reactions rate constants. At present there is a rich variety of two-temperature models of dissociation rate constants. At the same time it is known that behind the front of a shock wave, the process of dissociation proceeds mainly in quasistationa ry state (QSS) , when the vibrational excitation of a molecule is compensated by the loss of vibrational energy during the dissociation. In this paper a brief revue of some models is given and it is shown that in QSS conditions these models have practically coinsident numerical values,that removes a question on their choice. Statament of the problem


Journal of Engineering Physics | 1996

Avogadro program: Environmental problems of heat engineering

G. Ya. Gerasimov; S. A. Losev; V. N. Makarov

Results of some studies of formation and transformation of harmful substances during combustion of organic fuels are presented. The studies were conducted within the framework of the program “Environmental Problems of Heat Engineering” of the AVOGADRO system.


Shock Waves@ Marseille II. Physico-Chemical Processes and Nonequilibrium Flow. Proc. 19th Int. Symp. on Shock Waves. June 1993 | 1995

Two-Temperature Chemical Kinetics. Dissociation of Diatomic Molecules Behind a Strong Shock Wave

S. A. Losev; O. P. Shatalov

Experimental data about the vibrational temperature during the process of dissociation of diatomic molecules are discussed. The experiments allowed to substantiate the two- temperature model of the dissociation rate constant K d (T,T v ). Constancy of the vibrational temperature T v , revealed in experiments during the quasistationary stage of the dissociation permits to present the rate constant as a function of T (translational temperature) only, with T v =const, and to recommend an expression for K d to the range of high and extremely high temperatures, where the experimental data are absent.


Journal of Engineering Physics | 1985

Some techniques for physical experiments in a shock tube with a nozzle

I. E. Zabelinskii; S. A. Losev; O. P. Shatalov

The authors describe a technique for experiments in a shock tube with a nozzle: operation of the high-pressure chamber, the pumping system, measurements of velocity and pressure, and absorption measurements in the nozzles.


Journal of Applied Mechanics and Technical Physics | 1975

Study of vibrational deactivation of molecules of carbon dioxide gas during cooling of stream in a supersonic nozzle

N. V. Evtyukhin; S. A. Losev; V. N. Makarov; V. A. Pavlov; M. S. Yalovik

The vibrational temperature of the antisymmetrical type of vibrations (v3) of the CO2 molecule at the exit of a supersonic nozzle is measured in the present work using the method of recording the infrared emission. Freezing in of thev3-type vibrations was observed during the flow of undiluted carbon dioxide in a nozzle. In this case the vibrational temperature T3 considerably exceeded the translational temperature. On the basis of a comparison of the experimental results with calculation it can be concluded that vibrational deactivation of CO2 molecules occurs three to five times faster than the excitation of the vibrations during heating in a shock wave. All the experiments were conducted under the following conditions: maximum expansion of gas in nozzle A/A* = 115, temperature range 1900–2400 °K, pressure range 1–17.5 atm.


Journal of Applied Mechanics and Technical Physics | 1972

Relaxation equation for the vibrational energy of the molecules in the gas behind an intense shock front

B. V. Kuksenko; S. A. Losev; O. P. Shatalov

Here e is the v ibra t ional energy per unit volume of the gas, e ~ is the equi l ibr ium value of e, T is the re laxat ion t ime, E* is the average v ib ra t iona l energy lost dur ing each molecular d issocia t ion, and n is the number density of molecu les . In a descr ip t ion of the re laxa t ion p rocesses in intense shock waves in a gas, the anharmonic i ty and thus mul t iquantum t rans i t ions and d i ssoc ia t ion become impor tant . To de te rmine whether Eq. (1) can be used in this case, we mus t examine the sys tem of kinetic equations for the number of molecules x i at each v ibra t ional level under the assumpt ion that t r ans i t i ons i ~ j a re poss ib le between any two levels , and that t r ans i t ions i * d a re possible f rom any level to the d issocia t ion cont inuum:


AIAA Paper | 1994

Thermochemical nonequilibrium kinetic models in strong shock waves in air

S. A. Losev; V. N. Makarov; M.Y. Pogosbekyan; O. P. Shatalov; V.S. Nikol’sky


Journal of Engineering Physics | 2005

Kinetic models of combustion of kerosene and its components

G. Ya. Gerasimov; S. A. Losev


Reviews of Plasma Chemistry. Edited by B. M. Smirnov | 1991

Recommended data on the rate constants of chemical reactions between molecules consisting of N and O atoms

O.E. Krivonosova; S. A. Losev; V.P. Nalivaiko; Y.K. Mukoseev; O. P. Shatalov


Journal of Applied Spectroscopy | 1969

Ultraviolet absorption cross sections of molecular oxygen at 3000–10,000° K

S. A. Losev; O. P. Shatalov; M. S. Yalovik

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V. A. Pavlov

Moscow State University

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