Stability analysis for the onset of thermoacoustic oscillations in a gas-filled looped tube

Abstract

This paper develops a stability analysis for the onset of thermoacoustic oscillations in a gas-filled looped tube with a stack inserted, subject to a temperature gradient. Analysis is carried out based on approximate theories for a thermoviscous diffusion layer derived from the thermoacoustic-wave equation taking account of the temperature dependence of the viscosity and the heat conductivity. Assuming that the stack consists of many pores axially and that the thickness of the diffusion layer is much thicker than the pore radius, the diffusion wave equation with higher-order terms included is applied for the gas in the pores of the stack. For the gas outside of the pores, the theory of a thin diffusion layer is applied. In a section called the buffer tube over which the temperature relaxes from that at the hot end of the stack to room temperature, the effects of the temperature gradient are taken into account. With plausible temperature distributions specified on the walls of the stack and the buffer tube, the solutions to the equations in both theories are obtained and a frequency equation is finally derived analytically by matching the conditions at the junctions between the various sections. Seeking a real solution to the frequency equation, marginal conditions of instability are obtained numerically not only for the one-wave mode but also for the two-wave mode, where the tube length corresponds to one wavelength and two wavelengths, respectively. It is revealed that the marginal conditions depend not only on the thickness of the diffusion layer but also on the porosity of the stack. Although the toroidal geometry allows waves to be propagated in both senses along the tube, it is found that the wave propagating in the sense from the cold to the hot end through the stack is always greater, so that a travelling wave in this sense emerges as a whole. The spatial and temporal variations of excess pressure and mean axial velocity averaged over the cross-section of a flow passage are displayed for the two modes of oscillations at the marginal state. The spatial distribution of mean acoustic energy flux (acoustic intensity) over one period is also shown. It is unveiled that the energy flux is generated only in the stack, and it decays slowly in the other sections by lossy effects due to a boundary layer. Mechanisms for the generation of the acoustic energy flux are also discussed.

Weakly Nonlinear Propagation in Thermoacoustic Engines: A Numerical Study of Higher Harmonics Generation up to the Appearance of Shock Waves

“…Signals at positions 0 and 1 are identical. Since the wave is not purely traveling [41], a small counterpropagating wavefront can also be observed, emphasized by the gray line. These results are to be compared with those obtained experimentally by Biwa et al for a similar configuration …”

On general expressions of temporal means of mass flux, shear stress and heat flux due to thermoacoustic waves

“…In fact, the linearized version of (1) has been solved in this way to derive marginal conditions for the onset of thermoacoustic oscillations in a gas-filled tube [2]. Although no attempt to include the nonlinear terms has been made, it is expected to obtain autonomous excitation of thermoacoustic waves of finite amplitude.…”

“…This shows that the gradient of the mean pressure   p is of quadratic order in disturbance and that the mean of the pressure gradient squared is expressed in terms of the derivative of the mean pressure gradient. It is noted that finite effects of span length, represented by the first two terms on the second line in (1), do not contribute to (2). In a similar fashion, mean values of the mass flux, shear stress and heat flux on the wall are expressed in terms of the mean of the products of spatial and/or temporal gradients of the excess pressure, which are in turn expressed in terms of the mean pressure gradient through (2).…”

“…It is noted that finite effects of span length, represented by the first two terms on the second line in (1), do not contribute to (2). In a similar fashion, mean values of the mass flux, shear stress and heat flux on the wall are expressed in terms of the mean of the products of spatial and/or temporal gradients of the excess pressure, which are in turn expressed in terms of the mean pressure gradient through (2). Hence once the mean excess pressure is available, all means are obtained in terms of it.…”

Nonlinear theory for thermoacoustic waves in a narrow channel and pore subject to a temperature gradient

“…Because self-excited oscillations are generated in real devices, it is expected that the nonlinear equations (3.46) and (4.19) will be able to support time-periodic solutions. In the linear case, in fact, it is shown by Hyodo & Sugimoto (2014) that the linearised versions of those equations describe a marginal state of instability and yield a periodic oscillation, though infinitesimally small in amplitude. On the basis of an a priori assumption based on the existence of periodic solutions, general relations among mean values over one period are considered.…”