Acoustic Interactions With Turbulent Jets

1971 ◽  
Vol 93 (1) ◽  
pp. 42-46 ◽  
Author(s):  
C. D. Simcox ◽  
R. F. Hoglund

The interaction of a monochromatic acoustic wave with a fluctuating vorticity field is considered. The vorticity is first considered as varying harmonically both in time and space. The results show that significant changes in the time-averaged vorticity can occur. The changes are found to result from a rapid and repeated stretching and convection of the existing vorticity field by the applied acoustic field. By Fourier analysis this is extended to spectral relations to account for acoustic-turbulent interactions. The results of the study provide a consistent explanation of experimentally observed acoustic-turbulent interactions in jets, which at first appear to be contradictory.

Author(s):  
Michael W. Sracic ◽  
Jordan D. Petrie ◽  
Henry A. Moroder ◽  
Ryan T. Koniecko ◽  
Andrew R. Abramczyk ◽  
...  

Acoustic levitation is an advantageous particle positioning mechanism currently employed for applications of x-ray spectroscopy and micro-material manufacturing[1], [2]. By levitating a particle using only acoustic pressure waves, one eliminates the need for a container or other physical structure which may contaminate the specimen. Unfortunately, the pressure field generated by a standing acoustic wave is susceptible to periodic instabilities, and a particle that is levitated in this field tends to vibrate. The amplitude of the vibration is largest in the directions that are orthogonal to the axis in which the acoustic wave is generated. Therefore, by generating additional acoustic waves in each orthogonal axis, the vibration amplitude of the levitated particle is significantly reduced. The authors have shown this phenomenon to be true in a previous study[3]. In this paper, the authors explore the details of the pressure field that is generated with the device. A single degree-of-freedom relationship is developed between the acoustic field pressure, the location of the levitated particle, and the mechanical vibration needed to produce levitation. In order to levitate a 100 micrometer diameter water droplet at 55 kilohertz, the calculations suggest that the transducer must achieve an average surface vibration amplitude of at least 6.43 micrometers. This mechanical vibration must produce a root means-squared pressure amplitude of 933 Pascal. Under these conditions, the particle will levitate approximately 0.4 millimeters below a zero pressure node. To validate the use of the single degree of freedom relationships and to explore the acoustic field for one, two, and three-axis levitation, the authors designed and prototyped an acoustic levitator capable of generating standing waves in three orthogonal directions. Using a simple electrical control circuit, the acoustic wave transducers of each axis can be turned on individually or simultaneously. An experiment was developed to measure the pressure of the acoustic field using a microphone. Preliminary pressure magnitude results were measured for one-axis levitation along the center of the vertical axis of the levitator. The measurements suggest that the theoretical development provides a valid first approximation for the pressure magnitude and required mechanical vibration amplitude.


2010 ◽  
Vol 132 (8) ◽  
Author(s):  
Satbir Singh ◽  
Mark P. B. Musculus

Previous velocity and scalar measurements in both single-phase jets and two-phase diesel fuel sprays indicate that after the flow at the nozzle decelerates, ambient-gas entrainment increases compared to a steady jet. Previous studies using simplified analytical models and computational fluid dynamics (CFD) simulations using a one-dimensional (1D) inviscid, incompressible momentum equation have predicted that an “entrainment wave” propagates downstream along the jet axis during and after the deceleration, increasing entrainment by up to a factor of 3. In this study, entrainment is analyzed using the full compressible, unsteady Navier–Stokes momentum equations in axisymmetric two-dimensional (2D) CFD simulations of single-pulsed transient round gas jets. The 2D simulations confirm the existence of the entrainment wave, although the region of increased entrainment is distributed over a wider axial region of the jet than predicted by the simplified 1D model, so that the peak entrainment rate increases by only 50% rather than by a factor of 3. In the long time limit, both models show that the rate of mixing relative to the local injected fluid concentration increases significantly, approaching a factor of 3 or more increase in the wake of the entrainment wave (relative to a steady jet). Analysis of the terms in the momentum equation shows that the entrainment wave in the full 2D CFD predictions occurs in two phases. The entrainment first increases slightly due to a radial pressure gradient induced by a relatively fast acoustic wave, which the simple 1D model does not account for. The acoustic wave is followed by a slower momentum wave of decreased axial velocity initiated at the nozzle, which is convected downstream at the local flow velocities. The largest increase in entrainment accompanies the momentum wave, which is captured by the 1D momentum-equation model.


1959 ◽  
Vol 10 (1) ◽  
pp. 47-64 ◽  
Author(s):  
J. H. Foxwell ◽  
R. E. Franklin

SummaryWhen a vibrating structure encloses a volume of fluid, the acoustic effects within this volume modify considerably the response characteristics of the structure, provided that the cylinder is vibrating in radial modes only. Measurements made of the displacement caused by a particular sound wave are of the same order as the values predicted. The calculation of the response of the cylinder to an acoustic wave also yields the sound field inside the cylinder and, again, the results are in general agreement with practical experience.


1973 ◽  
Vol 51 (23) ◽  
pp. 2459-2463 ◽  
Author(s):  
S. S. Mathur ◽  
M. S. Sagoo

The propagation of microwaves in piezoelectric semiconductors irradiated with an acoustic field has been discussed. It has been shown that the acoustic wave produces appreciably large variation in the carrier concentration in a piezoelectric semiconductor as opposed to a nonpiezoelectric semiconductor. Consequently, the microwaves propagating through such piezoelectric semiconductors get modulated. The resulting sum and difference microwave frequencies do not have the same magnitude. This modulation of the difference frequency under optimum conditions is found to be of the order of 3% in cadmium sulfide, and is measurable. This measurement can be used to determine the piezoelectric constant of a semiconductor.


2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Huaping Wang ◽  
Lei Zhang ◽  
Shahnawaz Shah ◽  
Rongrong Zhu ◽  
Bin Zheng

AbstractWith the ability to focus and rotate the acoustic field in a given region while keeping the outside region unchanged, the acoustic concentrator and rotator has been developed for the versatile manipulations of acoustic wave. In this letter, we report the design of acoustic concentrator and rotator facilitated by linear coordinate transformation. Compared with the previous ones that have inhomogeneous parameter distributions, the designed devices are composed of several parts with homogeneous parameters, which can be achieved with the help of few homogeneous layered structures. Simulations are also performed to verify the functions of the designed device. The proposed acoustic concentrators and rotators would be useful in numerous applications such as acoustic sensing and communication.


1996 ◽  
Vol 35 (Part 1, No. 5B) ◽  
pp. 3196-3199
Author(s):  
Nobuhiro Tasaki ◽  
Koichi Mizutani ◽  
Keinosuke Nagai

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