Full wave theory of focused pressure fields by bi-concave lenses

Author(s):  
Tomoo Kamakura ◽  
Kenichi Aoki ◽  
Toshiaki Nakamura
1998 ◽  
Vol 5 (6) ◽  
pp. 2284-2290 ◽  
Author(s):  
C. N. Lashmore-Davies ◽  
V. Fuchs ◽  
R. A. Cairns

1987 ◽  
Vol 30 (1) ◽  
pp. 115 ◽  
Author(s):  
Amnon Fruchtman ◽  
Kurt Riedel ◽  
H. Weitzner ◽  
D. B. Batchelor

2013 ◽  
Vol 55 (10) ◽  
pp. 105008
Author(s):  
J T Mendonça ◽  
R M O Galvão ◽  
C Amador

The propagation of radio waves through a horizontally stratified and slowly varying ionosphere is governed, in the case of oblique incidence, by a quartic equation (Booker 1938). Ray theory breaks down when two roots of this quartic are equal, for then coupling occurs between the characteristic waves, and full wave theory must be used. This paper is concerned with determining the conditions under which the two roots are equal; it is not concerned with the full wave theory. Values of the plasma frequency, and electron collision frequency, which lead to equal roots, are determined, and are exhibited in a set of curves. A full solution of the ‘Booker’ quartic is also given for a case of special interest. It is pointed out that the electric wave-field is unlikely to become very large in a slowly varying ionosphere, so that, if the ionosphere were irregular, scattering cannot be unduly enhanced by a plasma resonance.


1980 ◽  
Vol 61 (1) ◽  
pp. 21-39 ◽  
Author(s):  
G. L. Choy ◽  
V. F. Cormier ◽  
R. Kind ◽  
G. Muller ◽  
P. G. Richards

1972 ◽  
Vol 7 (3) ◽  
pp. 403-416 ◽  
Author(s):  
B. A. Aničin ◽  
V. M. Babovič ◽  
K. E. Lonngren

Nanosecond pulses are launched, and propagate on a positive column in the form of electron waves. The dispersion of the pulses is studied experimentally, and is found to be in agreement with monochromatic experiments and theory. Apart from wave attenuation, which is observed to depress signals of higher frequencies, Fourier analysis of the received pulses has revealed that the launching mechanism favours frequencies in the vicinity of 1/6ωp A full-wave theory, based on an extension of Goubau's excitation theorem, is derived, and successfully contrasted with experiment.


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