Estimating source position accuracy of a large-aperture hydrophone array for bioacoustics

2001 ◽  
Vol 109 (1) ◽  
pp. 397-406 ◽  
Author(s):  
Magnus Wahlberg ◽  
Bertel Møhl ◽  
Peter Teglberg Madsen
2004 ◽  
Vol 115 (6) ◽  
pp. 2848-2858 ◽  
Author(s):  
G. A. Cranch ◽  
R. Crickmore ◽  
C. K. Kirkendall ◽  
A. Bautista ◽  
K. Daley ◽  
...  

2008 ◽  
Vol 60 (sp1) ◽  
pp. S35-S41 ◽  
Author(s):  
Yasunobu Uchiyama ◽  
Yoshitomo Maeda ◽  
Masatoshi Ebara ◽  
Ryuichi Fujimoto ◽  
Yoshitaka Ishisaki ◽  
...  

1998 ◽  
Vol 25 (3) ◽  
pp. 365-368 ◽  
Author(s):  
Jeffrey A. Hanson ◽  
Holly K. Given

2021 ◽  
Vol 9 ◽  
Author(s):  
Jan Rusz ◽  
Jaroslav Chum ◽  
Jiří Baše

Lightning generates sound waves across a wide range of frequencies, including infrasonic waves below 20 Hz. Source mechanism for these low frequency pulses is still area for debate. Infrasound pulses detected after rapid changes of electrostatic field during the thunderstorm activity were analyzed. The measurements were done by large aperture array of absolute microbarometers located in the Western part of the Czech Republic. Distances between four measuring sites are in the range of 4–10 km. The infrasound source position was calculated from time delays between the rapid change of electrostatic field and infrasound signal arrival to the individual microbarometers assuming propagation of spherical waves from the source. Only cases with a sufficient signal-to-noise ratio on all four microbarometers were analyzed. The variation of sound speed with height due to temperature height profile was taken into account. For most of the analyzed cases, the calculated infrasound source position corresponds to the lightning location determined by European lightning detection network (EUCLID). The calculated height of infrasound source is most often 3–5 km.


Author(s):  
T. Miyokawa ◽  
S. Norioka ◽  
S. Goto

Field emission SEMs (FE-SEMs) are becoming popular due to their high resolution needs. In the field of semiconductor product, it is demanded to use the low accelerating voltage FE-SEM to avoid the electron irradiation damage and the electron charging up on samples. However the accelerating voltage of usual SEM with FE-gun is limited until 1 kV, which is not enough small for the present demands, because the virtual source goes far from the tip in lower accelerating voltages. This virtual source position depends on the shape of the electrostatic lens. So, we investigated several types of electrostatic lenses to be applicable to the lower accelerating voltage. In the result, it is found a field emission gun with a conical anode is effectively applied for a wide range of low accelerating voltages.A field emission gun usually consists of a field emission tip (cold cathode) and the Butler type electrostatic lens.


Sign in / Sign up

Export Citation Format

Share Document