Detonation-Driven Shock Tubes and Tunnels

A more than 40 years, high-enthalpy facilities suitable for aerodynamic testing are still mostly based on the shock tunnel principle. Recent use of these facilities involves the development of space planes and reentry vehicles for studying the complex aerothermochemistry associated with flight at high velocities. The effects of thermal and chemical relaxation in air become important for flight velocities greater than approximately 4km/s. In addition, high-enthalpy, aerodynamic-impulse facilities are not only used to study high-temperature effects but are also suitable for generating high Mach number, high Reynolds number flows to investigate viscosity-dominated effects at low-enthalpy conditions. In aiming at higher-flow velocities, that is, higher stagnation enthalpies, it became obvious quickly that a technological barrier exists that would be very hard to overcome with conventional shock tubes. Therefore, Stalker modified the conventional shock tunnel to a free-piston shock tunnel. In these facilities, the driver gas is compressed by a heavy piston accelerated to nearly sonic speed. Between the piston and the main diaphragm, high values of temperature and pressure are achieved to generate a strong shockwave propagating along the driven section of the shock tunnel. Before the diaphragm opens, the piston is decelerated by the increasing driver gas pressure. Sophisticated techniques were developed for controlling and tuning this deceleration process because of its great importance for driver

[1]  M. A. Nettleton,et al.  The diffraction of a planar detonation wave at an abrupt area change , 1979, Journal of Fluid Mechanics.

[2]  G. W. Garrison ELECTRICAL CONDUCTIVITY OF A SEEDED NITROGEN PLASMA. , 1968 .

[3]  P. B. Coates,et al.  A simple shock tube with detonating driver gas , 1965, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[4]  F. R. Riddell,et al.  Theory of Stagnation Point Heat Transfer in Dissociated Air , 1958 .

[5]  R. J. Stalker,et al.  A study of the free-piston shock tunnel. , 1967 .

[6]  Donald R. Wilson,et al.  Numerical simulation of transient combustion process in pulse detonation engine , 2000 .

[7]  Frank K. Lu,et al.  An experimental and computational study of oxyhydrogen detonation wave propagation in a tube , 2000 .

[8]  Donald R. Wilson,et al.  Development of a high-pressure detonation-driven shock tube facility , 1996 .

[9]  John I. Erdos,et al.  Recent Advances in Detonation Techniques for High-Enthalpy Facilities , 2000 .

[10]  Yu Hongru,et al.  Oxyhydrogen combustion and detonation driven shock tube , 1999 .

[11]  M. Lenartz Development of a Detonation Driver for a Shock Tunnel , 1995 .

[12]  John I. Erdos,et al.  Dual Mode Shock-Expansion/Reflected-Shock Tunnel , 1997 .

[13]  Joseph Falcovitz,et al.  Numerical Simulations of Detonation in Converging Chambers , 1997 .

[14]  W. Gordon,et al.  Limit and spin effects in hydrogen-oxygen detonations , 1958 .

[15]  Donald R. Wilson,et al.  Experiments on Weakly-Ionized Air and Nitrogen Plasmas for Hypersonic Propulsion Facility Development , 1999 .

[16]  A. Hertzberg,et al.  SUMMARY OF SHOCK TUNNEL DEVELOPMENT AND APPLICATION TO HYPERSONIC RESEARCH , 1961 .

[17]  John I. Erdos,et al.  Expansion of the scramjet ground test envelope of the Hypulse facility , 1996 .

[18]  B. H. K. Lee,et al.  Detonation-driven shocks in a shock tube. , 1967 .

[19]  H. Grönig,et al.  Gaseous detonation driver for a shock tunnel , 1992 .

[20]  John H. S. Lee,et al.  Dynamic Parameters of Gaseous Detonations , 1984 .

[21]  Donald R. Wilson,et al.  Design of an electrical conductivity channel for shock tunnel , 1996 .

[22]  W. Stuessy,et al.  Exploratory study of conductivity in detonation waves , 1999 .

[23]  J Erdos,et al.  Options for enhancement of the performance of shock-expansion tubes and tunnels , 1995 .

[24]  John I. Erdos,et al.  An experimental and computational study leading to new test capabilities for the HYPULSE facility with a detonation driver , 1996 .