Frequency Dependence of Radar Meteor Echo Rates

1986 ◽  
Vol 6 (3) ◽  
pp. 303-306 ◽  
Author(s):  
R. M . Thomas ◽  
P. S. Whitham ◽  
W. G. Elford

AbstractMeteor rates have been measured with a large HF Radar at a number of frequencies. At the top end of the HF band our results match those of Greenhow (1963). However at lower frequencies we find high echo rates which indicate that past observations measured only a few percent of the total meteor flux incident on the Earth’s atmosphere. This explains the ‘missing mass’ discrepancy observed when radar results are compared with satellite or visual data. Accounting for’this missing mass results in a four-fold increase in the calculated total meteoroid mass influx to the surface of the Earth from 4000 to 16,000 tonnes per year. Our results also imply that the majority of echoes originate from altitudes above 100 km.

2007 ◽  
Vol 25 (9) ◽  
pp. 1987-1994 ◽  
Author(s):  
A. V. Koustov ◽  
D. André ◽  
E. Turunen ◽  
T. Raito ◽  
S. E. Milan

Abstract. Tomographic estimates of the electron density altitudinal and latitudinal distribution within the Hankasalmi HF radar field of view are used to predict the expected heights of F region coherent echoes by ray tracing and finding ranges of radar wave orthogonality with the Earth magnetic field lines. The predicted ranges of echoes are compared with radar observations concurrent with the tomographic measurements. Only those events are considered for which the electron density distributions were smooth, the band of F region HF echoes existed at ranges 700–1500 km, and there was a reasonable match between the expected and measured slant ranges of echoes. For a data set comprising of 82 events, the typical height of echoes was found to be 275 km.


1999 ◽  
Vol 51 (7-8) ◽  
pp. 685-689 ◽  
Author(s):  
Barbara Jenkins ◽  
Martin J. Jarvis
Keyword(s):  
Hf Radar ◽  

1980 ◽  
Vol 67 (5) ◽  
pp. 1502-1506 ◽  
Author(s):  
H. E. Bass ◽  
L. N. Bolen ◽  
Daniel Cress ◽  
Jerry Lundien ◽  
Mark Flohr

1973 ◽  
Vol 10 (8) ◽  
pp. 1191-1200 ◽  
Author(s):  
F. W. Jones ◽  
B. A. Ainslie

The geomagnetic perturbation fields due to conductivity discontinuities in the Earth are investigated. Two models, one in which the discontinuity extends to infinite depth, and a second one which consists of a dike of finite depth are considered. The perturbation fields are studied for several different frequencies of the alternating inducing field for each model. Both the H-polarization and E-polarization cases are considered and the perturbation field component profiles as a function of height above the surface of the conducting region are studied. The perturbation fields are strongly dependent on frequency, and significant differences are exhibited between the H-polarization and E-polarization cases.


1962 ◽  
Vol 40 (10) ◽  
pp. 1360-1369 ◽  
Author(s):  
James R. Wait

The paper is concerned with the connection between frequency domain and time domain for propagation in the earth–ionosphere wave guide. Attention is focussed on the extremely low frequency (e.l.f.) range. It is assumed that the propagation constant is proportional to (frequency)v where v is a fraction between 0 and 1. For such a frequency law, the corresponding transient responses are computed. These illustrate a number of important points. In particular, it is indicated that the frequency dependence of the propagation constant could be estimated directly from the wave forms themselves without resorting to conventional spectral analysis.


2020 ◽  
Vol 44 (4) ◽  
pp. 1221-1227 ◽  
Author(s):  
Xuemei Wei ◽  
Zhanwei Ma ◽  
Jinzhi Lu ◽  
Xinyuan Mu ◽  
Bin Hu

A four-fold increase in palladium-based acetylene dicarbonylation activity was obtained at low temperature due to the strong metal–support interaction between Pd and the earth-abundant α-Fe2O3 material.


Geophysics ◽  
1994 ◽  
Vol 59 (2) ◽  
pp. 215-223 ◽  
Author(s):  
Greg Turner

The frequency dependence of attenuation is typically far greater for subsurface radar waves than for seismic waves. Since this frequency dependence causes the subsurface radar pulse shape to change as it propagates through the earth, conventional wavelet deconvolution techniques are often inadequate to reconstruct the earth’s reflectivity series. The application of a time‐variant filter that undoes the effect of frequency‐dependent attenuation can substantially improve the resolution of subsurface radar data. This filter is minimum‐phase with amplitude characteristics equal to the inverse of the attenuation function of the medium investigated. Preliminary tests on data from surveys over a water tank, an underground mine stope, and fractured granite suggest that good results can also be achieved by assuming attenuation is linearly proportional to frequency, similar to a constant Q model.


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