Electromagnetic Shock Tube capable of producing a Well-formed shock Wave of Low Attenuation

This paper is a continuing work from one author on the same topic of the transient aerodynamics during compressor stall/surge using a shock tube analogy by Huang [1, 2]. As observed by Mazzawy [3] for the high-speed high-pressure (HSHP) ratio compressors of the modern aero-engines, surge is an event characterized with the stoppage and reversal of engine flow within a matter of milliseconds. This large flow transient is accomplished through a pair of internally generated shock waves and expansion waves of high strength. The final results are often dramatic with a loud bang followed by the spewing out of flames from both the engine intake and exhaust, potentially damaging to the engine structure [3]. It has been demonstrated in the previous investigations by Marshall [4] and Huang [2] that the transient flow reversal phase of a surge cycle can be approximated by the shock tube analogy in understanding its generation mechanism and correlating the shock wave strength as a function of the pre-surge compressor pressure ratio. Kurkov [5] and Evans [8] used a guillotine analogy to estimate the inlet overpressure associated with the sudden flow stoppage associated with surge. This paper will expand the progressive surge model established by the shock tube analogy in [2] by including the dynamic effect of airflow stoppage using an “integrated-flow” sequential guillotine/shock tube model. It further investigates the surge formation (characterized by flow reversal) and propagation patterns (characterized by surge shock and expansion waves) after its generation at different locations inside a compressor. Calculations are conducted for a 12-stage compressor using this model under various surge onset stages and compared with previous experimental data [3]. The results demonstrate that the “integrated-flow” model closely replicates the fast moving surge shock wave overpressure from the stall initiation site to the compressor inlet.

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Shock-Wave-Induced Flow Past a Circular Cylinder in a Dusty-Gad Shock Tube

JSME international journal Ser 2 Fluids engineering heat transfer power combustion thermophysical properties ◽

10.1299/jsmeb1988.33.2_224 ◽

1990 ◽

Vol 33 (2) ◽

pp. 224-228

Author(s):

Hiromu SUGIYAMA ◽

Kazuyoshi TAKAYAMA ◽

Takahiro SHIROTA ◽

Hiromichi DOI

Keyword(s):

Shock Wave ◽

Circular Cylinder ◽

Shock Tube ◽

Flow Past ◽

Induced Flow ◽

Wave Induced

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An investigation of the interaction between a travelling shock wave and a solid rocket motor nozzle

10.32920/ryerson.14656911 ◽

2021 ◽

Author(s):

Harmanjit Singh Chopra

Keyword(s):

Shock Wave ◽

Shock Tube ◽

Reflected Shock Wave ◽

Convergence Region ◽

Rocket Motors ◽

Additional Information ◽

Reflected Shock ◽

Solid Propellant Rocket ◽

Computational Fluid Dynamics Cfd ◽

Nozzle Geometries

A gasdynamic mechanism has been identified as a potential source of combustion instability in solid-propellant rocket motors (SRMs). This mechanism involves the reinforcement of a reflected shock wave in the nozzle convergence region of an SRM's exhaust nozzle. A shock tube apparatus was developed for the experimental component of this study. Various factors, such as the effect of different nozzle geometries and driven channel pressures, were examined. Also, a model of the shock tube was developed for computational fluid dynamics (CFD) simulations. These simulations were generated for comparison with the experimental results and to provide additional information regarding the nature of the flow behaviour. A gasdynamic mechanism has been identified as a potential source of combustion instability in solid-propellant rocket motors (SRMs). This mechanism involves the reinforcement of a reflected shock wave in the nozzle convergence region of an SRM's exhaust nozzle.A shock tube apparatus was developed for the experimental component of this study. Various factors, such as the effect of different nozzle geometries and driven channel pressures, were examined. Also, a model of the shock tube was developed for computational fluid dynamics (CFD) simulations. These simulations were generated for comparison with the experimental results and to provide additional information regarding the nature of the flow behaviour.Experimental and numerical pressure-time profiles confirm the appearance of transient radial wave activity following the initial incidence of the normal shock wave on the convergence region of the nozzle. The results establish that the strength of this activity is markedly dependent upon the nozzle convergence wall angle and the location within the shock tube

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Interaction of Reflected Shock Wave with Shock Tube Wall

JOURNAL OF THE JAPAN SOCIETY FOR AERONAUTICAL AND SPACE SCIENCES ◽

10.2322/jjsass.52.153 ◽

2004 ◽

Vol 52 (603) ◽

pp. 153-159 ◽

Cited By ~ 3

Author(s):

Munetsugu Kaneko ◽

Igor Men’shov ◽

Yoshiaki Nakamura

Keyword(s):

Shock Wave ◽

Shock Tube ◽

Tube Wall ◽

Reflected Shock Wave ◽

Reflected Shock

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Low Attenuation Shock Tube: Driving Mechanism and Diaphragm Characteristics

Canadian Journal of Physics ◽

10.1139/p71-240 ◽

1971 ◽

Vol 49 (15) ◽

pp. 1982-1993 ◽

Cited By ~ 11

Author(s):

F. L. Curzon ◽

M. G. R. Phillips

Keyword(s):

Shock Wave ◽

Simple Model ◽

Shock Tube ◽

Electric Shock ◽

Strong Evidence ◽

Room Temperature ◽

Wave Motion ◽

Driving Mechanism ◽

Driver Gas ◽

Opening Process

The properties of an electric shock tube fitted with a diaphragm are examined. The diaphragm opening process and its effect on the motion of the shock wave are studied. A simple model to account for the diaphragm opening time is given and critical comparisons of theory and results with other work are made.The model works well both for shock tubes employing room temperature driver gas and also for those using heated driver gas. Furthermore, there is strong evidence that the diaphragm opening process is responsible for the accelerating phase of the shock wave motion in both types of shock tube.

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