Further developments in the active control of free‐field sound using near‐field energy‐based error signals

2007 ◽  
Vol 121 (5) ◽  
pp. 3180-3180
Author(s):  
Ryan T. Chester ◽  
Timothy W. Leishman
Keyword(s):  
Active Control ◽  
Near Field ◽  
Free Field ◽  
Field Energy ◽  
Field Sound

Active control of free‐field sound using near‐field energy‐based error signals

2006 ◽  
Vol 120 (5) ◽  
pp. 3198-3198
Author(s):  
Ryan T. Chester ◽  
Timothy W. Leishman
Keyword(s):  
Active Control ◽  
Near Field ◽  
Free Field ◽  
Field Energy ◽  
Field Sound

scholarly journals Near‐Field Energy Transfer between a Luminescent 2D Material and Color Centers in Diamond

2019 ◽  
Vol 3 (2) ◽  
pp. 1900088 ◽  
Author(s):  
Richard Nelz ◽  
Mariusz Radtke ◽  
Abdallah Slablab ◽  
Zai‐Quan Xu ◽  
Mehran Kianinia ◽  
...  
Keyword(s):  
Energy Transfer ◽  
Near Field ◽  
Color Centers ◽  
Field Energy ◽  
2D Material

Visualizing near-field energy flow and radiation

2000 ◽  
Vol 42 (6) ◽  
pp. 46-54 ◽  
Author(s):  
E.K. Miller ◽  
F.J. Deadrick
Keyword(s):  
Energy Flow ◽  
Near Field ◽  
Field Energy

Hydrodynamic Noise and Radiated Mechanism of 3D Cavity

2012 ◽  
Vol 217-219 ◽  
pp. 2590-2593 ◽  
Author(s):  
Yu Wang ◽  
Bai Zhou Li
Keyword(s):  
Sound Pressure ◽  
Near Field ◽  
Low Frequency ◽  
Dipole Source ◽  
Fluctuating Pressure ◽  
Common Structure ◽  
Hydrodynamic Noise ◽  
Near Field Sound ◽  
Equivalent Sources ◽  
Field Sound

The flow past 3D rigid cavity is a common structure on the surface of the underwater vehicle. The hydrodynamic noise generated by the structure has attracted considerable attention in recent years. Based on LES-Lighthill equivalent sources method, a 3D cavity is analyzed in this paper, when the Mach number is 0.0048. The hydrodynamic noise and the radiated mechanism of 3D cavity are investigated from the correlation between fluctuating pressure and frequency, the near-field sound pressure intensity, and the propagation directivity. It is found that the hydrodynamic noise is supported by the low frequency range, and fluctuating pressure of the trailing-edge is the largest, which is the main dipole source.

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