Incorporation of Nonlinear Capabilities in the Standard Stability Prediction Program

Predictive algorithms now in general use cannot characterize high-amplitude pressure oscillations that are frequently observed in solid propellant rocket motor combustion chambers. In fact, programs such as the Standard Stability Prediction (SSP) code are based on a linear theory, which has serious shortcomings. Therefore, it is necessary to address both correction of the flawed linear theory and incorporation of models to allow prediction of important nonlinear effects. These include: 1) limit cycle behavior in which the pressure fluctuations may dwell for a considerable period of time near their peak amplitude, 2) elevated mean chamber pressure (DC shift), and 3) a triggering amplitude above which pulsing may cause an apparently stable system to transition to violent oscillations. Culick’s wellestablished nonlinear model provides useful guidance in dealing with the system limit cycle transition. It is demonstrated in this paper that his calculations represent the classical steepening mechanism by which the wave system evolves from an initial set of standing acoustic modes into a shock-like, traveling, steep-fronted wave. However, a very important missing element is the ability to predict the accompanying mean pressure shift; clearly, the program user requires information regarding the maximum chamber pressure that might be experienced during operation of the motor, as well as the peak amplitudes reached by the pressure oscillations. Recent theoretical work has resulted in a firm foundation upon which to build the required predictive capabilities. These are described in detail, and it is demonstrated that the new theory yields results that are in excellent agreement with experimental data.

[1]  J. Levine,et al.  A numerical study of nonlinear instability phenomena in solid rocket motors , 1981 .

[2]  Fred E. C. Culick,et al.  Rotational axisymmetric mean flow and damping of acoustic waves in asolid propellant rocket. , 1966 .

[3]  J. N. Levine,et al.  A numerical study of nonlinear instability phenomena in solid rocketmotors , 1983 .

[4]  H. B. Mathes,et al.  Pressure oscillations in post-Challenger Space Shuttle redesigned solid rocket motors , 1993 .

[5]  G. Flandro,et al.  On the origin of the DC shift , 1997 .

[6]  Fred E. C. Culick,et al.  Pulsed Instabilities in Solid-Propellant Rockets , 1995 .

[7]  W. G. Brownlee Nonlinear axial combustion instability in solid propellant motors , 1964 .

[8]  Gary A. Flandro Approximate analysis of nonlinear instability with shock waves , 1982 .

[9]  Merrill W. Beckstead,et al.  Limiting Amplitude Analysis. , 1973 .

[10]  Fred E. C. Culick,et al.  Combustion Instabilities in Propulsion Systems , 1996 .

[11]  J. F. Bird,et al.  AN EROSION MECHANISM FOR NON-LINEAR INSTABILITY IN THE AXIAL MODES OF SOLID PROPELLANT ROCKET MOTORS, , 1962 .

[12]  F. Culick A Note on Rayleigh's Criterion , 1987 .

[13]  Edward Warren Price Combustion instability in solid propellant rocket motors , 1986 .

[14]  H. B. Mathes,et al.  Stability testing of full scale tactical motors , 1991 .

[15]  F. E. C. Culick,et al.  Modeling for Active Control of Combustion and Thermally Driven Oscillations , 1991, 1991 American Control Conference.

[16]  Fred E. C. Culick,et al.  Nonlinear behavior of acoustic waves in combustion chambers. I, II. [stability in solid propellant rocket engine and T burner , 1976 .

[17]  V. Yang,et al.  Triggering of Longitudinal Pressure Oscillations in Combustion Chambers. I: Nonlinear Gasdynamics , 1990 .

[18]  Vigor Yang,et al.  Prediction of the stability of unsteady motions in solid-propellant rocket motors , 1992 .

[19]  Gary A. Flandro,et al.  Aeroacoustic Instability in Rockets , 2001 .

[20]  Gary A. Flandro,et al.  On flow turning , 1995 .

[21]  Fred E. C. Culick,et al.  Non-Linear Growth and Limiting Amplitude of Acoustic Oscillations in Combustion Chambers , 1971 .

[22]  Wilmot Grant Brownlee,et al.  An experimental investigation of unstable combustion in solid propellant rocket motors , 1959 .

[23]  F. Culick Some recent results for nonlinear acoustics in combustion chambers , 1994 .

[24]  Fred E. C. Culick Acoustic oscillations in solid propellant rocket chambers , 1966 .

[25]  G. A. Flandro,et al.  Effects of vorticity on rocket combustion stability , 1995 .

[26]  Fred E. C. Culick,et al.  Stability of Longitudinal Oscillations with Pressure and Velocity Coupling in a Solid Propellant Rocket , 1970 .

[27]  F. T. McClure,et al.  Combustion Instability: Acoustic Interaction with a Burning Propellant Surface , 1959 .

[28]  Leon Green,et al.  Observations on the Irregular Reaction of Solid Propellant Charges , 1956 .

[30]  K. Kuo Experimental Observations of Combustion Instability , 1984 .

[31]  Fred E. C. Culick Combustion instabilities: mating dance of chemical, combustion, and combustor dynamics , 2000 .

[32]  High-Frequency Combustion Instability in Solid Propellant Rockets. Part 1 , 1954 .

[33]  W. G. Brownlee,et al.  Shock propagation in solid-propellant rocket combustors. , 1966 .

[34]  G. A. Flandro Energy balance analysis of nonlinear combustion instability , 1985 .

[35]  S. Malhotra On combustion instability in solid rocket motors , 2004 .

[36]  H. B. Mathes,et al.  Nonlinear Stability Testing of Full-Scale Tactical Motors , 1997 .

[37]  Fred E. C. Culick The Stability of One-Dimensional Motions in a Rocket Motor , 1973 .

[38]  R. W. Hart,et al.  Theory of acoustic instability in solid-propellant rocket combustion , 1965 .

[39]  F. Culick Stability of Three-Dimensional Motions in a Combustion Chamber , 1975 .

[40]  H. Gibeling,et al.  Navier-Stokes analysis of solid propellant rocket motor internal flows , 1989 .