3 edition of Non-ideal gas effects on shock waves in weakly ionized gases found in the catalog.
Non-ideal gas effects on shock waves in weakly ionized gases
by Institute for Computer Applications in Science and Engineering, NASA Langley Research Center, National Technical Information Service, distributor in Hampton, VA, Springfield, VA
|Statement||Robert Rubinstein, Aaron H. Auslender.|
|Series||ICASE report -- no. 2000-3, [NASA contractor report] -- NASA/CR-2000-209839, NASA contractor report -- NASA CR-209839.|
|Contributions||Auslender, Aaron H., Institute for Computer Applications in Science and Engineering.|
|The Physical Object|
Physics of Fully Ionized Gases: Second Revised Edition (Dover Books on Physics) Paperback – July 7, Subjects include the motion of a particle, macroscopic behavior of a plasma, waves in a plasma, equilibria and their stability, and encounters between changed particles. Physics of Shock Waves and High-Temperature Hydrodynamic Cited by: Normal Shock Wave Oblique Shock Wave rarefaction waves viscous and thermal boundary layers far-field acoustic wave Figure Fluid mechanics phenomena in re-entry – Po = atm → Ps = atm (tremendous force change!!) – sudden transfer of energy from kinetic (ordered) to thermal (random)File Size: 1MB.
Ionizing Cylindrical Shock Waves in a Rotating Homogeneous Non-ideal Gas. with time. This increase can be achieved by the pressure exerted on the fluid by an expanding surface (a contact sur-face or a piston). This surface may be, physically, the surface of the stellar corona or the condensed explosives or the. Shock Structure Analysis and Aerodynamics in a Weakly Ionized Gas Flow R. Saeks Accurate Automation Corporation, Chattanooga, Tennessee S. Popovic Old Dominion University, Norfolk, Virginia A.S. Chow Marshall Space Flight Center, Marshall Space Flight Center, Alabama August Nat onal Aeronaut cs and Space Adm n strat on.
Key Words: Shock wave, Magnetogasdynamics, Non-ideal gas, Self-similar flow, Heat transfer effects, Gravitational field INTRODUCTION The influence of radiation on the shock wave and on the flow-field behind the shock front has always been of great interest, for instance in the field of nuclear power and space research. Consequently. Interaction of shock waves with a weakly ionized gas generated by discharges has been studied. An additional thermal mechanism of the shock wave dispersion on the boundary between a neutral gas and discharge has been proposed [A. Markhotok, S. Popovic, and L. Vuskovic, Proceedings of the 15th International Conference on Atomic Processes in Plasmas, .
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Non-ideal Gas Effects on Shock Waves in Weakly Ionized Gases Robert Rubinstein ICASE, Hampton, Virginia Aaron H. Auslender NASA Langley Research Center, Hampton, Virginia Institute for Computer Applications in Science and Engineering NASA Langley Research Center Hampton, VA Operated by Universities Space Research Association January Abstract.
A shock wave inaweakly ionized gas can be preceeded by acharge separation region if the Debye length is larger than the shock width.
It has been proposed that electrostatic contributions to pressure in the charge separation region can increase the sound speed ahead of the shock well above the sound speed in a neutral gas at the same temperature and therefore increase the shock.
Get this from a library. Non-ideal gas effects on shock waves in weakly ionized gases. [Robert Rubinstein; Aaron H Auslender; Institute for Computer Applications in Science and Engineering.]. NON-IDEAL GAS EFFECTS ON SHOCK WAVES IN WEAKLY IONIZED GASES.
By Robert Rubinstein and Aaron H. Auslender. Abstract. A shock wave inaweakly ionized gas can be preceeded by acharge separation region if the Debye length is larger than the shock width.
It has been proposed that electrostatic contributions to pressure in the charge separation Author: Robert Rubinstein and Aaron H. Auslender. A virial equation of state is developed for a weakly ionized gas. Using both ab initio quantum mechanical and approximate potentials it is shown that in cases where strong ion-molecule interactions exist at short range, significant non-ideal gas effects may be evident under common experimental conditions of temperature and ion by: 3.
Shock-Waves, Non-Ideal Gases, Magnetic Field 1. Introduction The assumption that the medium isan ideal gas is no more valid when the flow takes place in extreme conditions. Anisinov and Spiner  have studied a prob-lem of point explosion in low density non ideal gas.
Request PDF | Propagation of strong shock waves in a non-ideal gas | We studied the problem of converging cylindrical and spherical strong shock waves collapsing at. Shock Waves in Non –Ideal Gases.
paper an attempt is made to discuss certain properties of shock – waves in non-ideal gas. Rankine-Hugoniot relations are obtained for different values of.
Ionized Gases: Physics of Ionizing Shock Waves in Monatomic Gases at Large Mach Numbers Rarefied Gas Dynamics, Parts I and II August Shock wave propagation in weakly ionized plasmasCited by: shock layer structure. The effect of shock diffusion and attenuation is due to supersonic disturbance propagation from downstream to the upstream region across the shock along the filaments.
Introduction Shock wave (SW) propagation into weakly ionized plasmas has been investigated for the last 20 years . The main features of this Cited by: 7. This book is devoted to the physical properties of nonideal plasma which is compressed so strongly that the effects of interparticle interactions govern the plasma behavior.
Compression of Inert Gases by Powerful Shock Waves; Isentropic Expansion of Shock-Compressed Metals The Electrical Conductivity of Non-ideal Weakly Ionized Plasma. The effects due to the non-ideal gas on the strong imploding cylindrical and spherical shock waves were studied in view of the equation of state as given by Landau and Lifshitz.
Such problem is of great interest in astrophysics and space science as it is highly relevant to the problem of the origin of cosmic rays , , , .Cited by: 4.
NON-IDEAL GAS EFFECTS ON SHOCK WAVES IN WEAKLY IONIZED GASES ROBERT RUBINSTEIN* AND AARON H. AUSLENDERt Abstract. A shock wave in a weakly ionized gas can be preceeded by a charge separation region if the Debye length is larger than the shock width.
It has been proposed that electrostatic contributions to pressure. Besides shock waves in gases, the distinctive features of shock propagation through a weakly ionized plasma are considered.
Contents: Structure and Basic Properties of Shock Waves in Gases; Shock Wave Propagation Through a Gas; Interaction of a Plane Shock Wave with Disturbances and Stability of Shock Waves; Reflection of a Shock Wave from a.
Self-Similar Cylindrical Ionizing Shock Waves in a Non-Ideal Gas with Radiation Heat-Flux. azimuthal magnetic field is c onsidered due to its relevance to the experiments on pinch effect and exploding wires.
A gas-ionizing cylindrical shock wave, generated by line ex-plosion, is propagated in the nonideal gas. The counter. Although most applications involve molecular gases, the dispersion effects with a comparable intensity are observed in noble gases. Interaction of shock wave with ionized gas generates rapidly moving multiple electric layers, which form regions of increased electron : L.
Vušković, S. Popovićs. Experimental studies of shock waves in weakly ionized plasmas were performed in longitudinal continuos or pulsed glow discharges. The discharge tube, cm i.d. and cm full length, was made of quartz. Shock waves were generated by a spark discharge at the one end of the tube.
The shock wave entered the discharge. Shock dynamics of strong imploding cylindrical and spherical shock waves with non-ideal gas effects R K Anand imploding cylindrical and spherical shock waves in non-ideal gases during the Shock dynamics of strong imploding cylindrical and spherical shock waves with non-ideal gas effects R K Anand.) Cited by: 4.
The goal of this research was to determine the principal mechanism(s) for the shock velocity increase in weakly ionized gases.
This paper reports experimental data on the propagation of spark-generated shock waves (1weakly ionized nitrogen, air, and argon glow discharges (1effects due solely to the presence of electrons and effects Cited by: 1.
glow discharge plasma to weak (non-ionizing) shock waves of Mach number in the range - 3. Our results show that there is an increase in the velocity of a shock wave when it makes a transition from a neutral gas to a weakly ionized plasma. The observations also indicate that the shock acceleration cannot be accounted for by thermal effects only.
Similarity Solutions are obtained for one-dimensional adiabatic flow behind ionizing cylindrical shock wave propagating in a rotating non-ideal gas in presence of an azimuthal magnetic field. The electrical conductivity in the medium ahead of the shock is assumed to be negligible, which becomes infinitely large after passage of the shock.
In order to obtain the similarity solutions. On imploding cylindrical and spherical shock waves in a perfect gas By N. F. PONCHAUT, H. G. HORNUNG, D. I. PULLINAND C. A. MOUTON California Institute of Technology, Pasadena CAUSA (Received 4 July and in revised form 6 January ) The problem of a cylindrically or spherically imploding and reﬂecting shock wave in.account the effects of both conduction and radiation in the two confines of Rosseland radiative diffusion and Plank radiative emission.
dt r Since at elevated temperatures that overcome in the difficulty associated with shock waves a gas is partly ionized, electromagnetic effects .