acoustic radiator
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2021 ◽  
Vol 118 (30) ◽  
pp. e2024984118
Author(s):  
Curtis Rasmussen ◽  
Andrea Alù

The quality factor of a passive, linear, small acoustic radiator is fundamentally limited by its volume normalized to the emitted wavelength, imposing severe constraints on the bandwidth and efficiency of compact acoustic sources and of metamaterials composed of arrangements of small acoustic resonators. We demonstrate that these bounds can be overcome by loading a piezoelectric transducer with a non-Foster active circuit, showing that its radiation bandwidth and efficiency can be largely extended beyond what is possible in passive radiators, fundamentally limited only by stability considerations. Based on these principles, we experimentally observe a threefold bandwidth enhancement compared to its passive counterpart, paving the way toward non-Foster acoustic radiation and more broadly active metamaterials that overcome the bandwidth constraints hindering passive systems.


Metals ◽  
2019 ◽  
Vol 9 (5) ◽  
pp. 490 ◽  
Author(s):  
H. Puga ◽  
J. Barbosa ◽  
V. H. Carneiro

New alloy processes have been developed and casting techniques are continuously evolving. Such constant development implies a consequent development and optimization of melt processing and treatment. The present work proposes a method for studying the influence of acoustic pressure in the overall refinement of sand cast aluminum alloys, using and correlating experimental and numerical approaches. It is shown that the refinement/modification of the α-Al matrix is a consequence of the acoustic activation caused in the liquid metal directly below the face of the acoustic radiator. Near the feeder, there is a clear homogeneity in the morphology of the α-Al with respect to grain size and grain circularity. However, the damping of acoustic pressure as the melt is moved away from the feeder increases and the influence of ultrasound is reduced, even though the higher cooling rate seems to compensate for this effect.


2019 ◽  
Vol 37 ◽  
pp. 563-577 ◽  
Author(s):  
Jianfeng Wang ◽  
Qingjie Sun ◽  
Jiangkun Ma ◽  
Junbo Teng ◽  
Peng Jin ◽  
...  

2018 ◽  
Vol 64 (2) ◽  
pp. 237-244 ◽  
Author(s):  
A. A. Abdrashitov ◽  
E. A. Marfin ◽  
D. V. Chachkov

2011 ◽  
Vol 57 (3) ◽  
pp. 326-333 ◽  
Author(s):  
A. D. Mansfel’d ◽  
A. V. Sokolov ◽  
G. P. Volkov
Keyword(s):  

Author(s):  
Reza Kashani ◽  
Jeff Monfort

A commonly used technique for mitigating thermoacoustic instability in an enclosed combustion environment is removing more acoustic energy from the combustor, at the frequency corresponding to the acoustic mode(s) of the combustor which are sympathetic to such instability. This approach is based on adding tuned acoustic damping to the combustion environment. By incorporating in-situ adjustability into acoustic damping devices, they can change their mechanical attributes, e.g., mass and/or stiffness, and adapt themselves in a semi-active manner to the varying instability frequency. Adaptive-passive thermoacoustic mitigation solutions have less weight penalty than the alternative active solutions mainly because the adaptation is done in a semi-active way, at slow pace, with a small and less power-hungry actuation mechanisms. Moreover, the flexibility they offer make them highly desirable for land and marine instability mitigation applications. In this work, semi-active adjustment of a novel tuned acoustic damper, namely an acoustic radiator, is explored. The paper describes the inner working of a semi-active (adaptive-passive) acoustic radiator and the relevant control schemes to adapt them to the instability frequency on hand. The damping effectiveness of the proposed damper, is demonstrated experimentally. It should be mentioned that the semi-active control strategies developed for acoustic radiators can also be used, with minor modifications, for semi-active control of other acoustic damping mechanisms such as Helmholtz resonators and quarter-wave tubes.


2008 ◽  
Vol 51 (3) ◽  
pp. 177-192
Author(s):  
A. I. Smirnov ◽  
V. G. Burdukovskaya ◽  
A. G. Koshkin ◽  
A. I. Khil’ko

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