Phase determination and inversion of specular reflection data in neutron-surface scattering

1994 ◽  
Vol 307-309 ◽  
pp. 901-906 ◽  
Author(s):  
R. Lipperheide ◽  
G. Reiss ◽  
H. Fiedeldey ◽  
S.A. Sofianos ◽  
H. Leeb
Geophysics ◽  
1999 ◽  
Vol 64 (6) ◽  
pp. 1828-1835 ◽  
Author(s):  
Stanley J. Radzevicius ◽  
Gary L. Pavlis

We analyze data from two orthogonal seismic lines 336 m in length collected at Piñon Flat, California, over weathered granodiorite bedrock. Each line was made up of 10 reversed segments 84 m in length. We analyzed the first arrivals from these data and found dramatic variations in velocity along the profiles. An upper layer (approximately 2-m thick) known from trenching to be composed of soil and sandy grus had measured velocities ranging from 400 to 700 m/s. Velocities inferred from refraction analysis of first arrivals of the reversed lines revealed a heterogeneous lower layer below the soil with measured velocities of 1600–2700 m/s by a depth of 15 m. We interpret these data to be measuring velocities of a deeply weathered unit characterized by granodiorite corestones embedded in a matrix of saprolite. The most remarkable feature of these data emerged from attempting to process the same data as reflection data. Simple bandpass filtering in the 250–400 Hz band revealed a bright, impulsive arrival with three characteristic properties: (1) irregular velocity moveout that is inconsistent with that expected from a layered earth model, (2) the arrival is at a nearly constant time‐depth on all data, and (3) the arrival tends to be followed by a ringing coda whose frequency varies from trace to trace. This arrival ties exactly with a velocity discontinuity measured in a borehole located on one of the profiles that we interpret as the base of the weathered layer. We suggest this arrival is a specular reflection from a weathering front that occurs along horizontal sheeting joints at a fixed depth below the surface. This surface acts as an effective mirror for high‐frequency seismic waves which are then channeled upward through an intact, high-Q path of unaltered blocks of granodiorite to define the observed signals at the surface.


1972 ◽  
Vol 27 (12) ◽  
pp. 1798-1803 ◽  
Author(s):  
M.M.R. Williams

AbstractWe have developed a global scattering kernel which describes the scattering of gas atoms by spherical particles which are small compared with a mean free path in the gas. The global kernel, which is analogous in many ways to the thermal neutron scattering kernel employed in neutron thermalization studies, is given in terms of the gas-surface scattering law for the particle. Thus the global kernel can be studied as a function of specular reflection and incomplete accommodation. The recent model of KUŠČER and of CERCIGNANI is used for the latter investigation and we find that on the average the angular distribution of the scattered gas atoms depends sensitively on the tangential momentum accommodation coefficient but only very weakly on the energy coefficient. However, the phenomenon is strongly dependent on the speed of the approaching gas atom and, for low speed gas atoms, the sensitivity to energy accommodation becomes much more important. The net scattering rate is obtained and put in a form convenient for later calculations to be described in a series of companion papers.


Geophysics ◽  
2003 ◽  
Vol 68 (2) ◽  
pp. 559-565 ◽  
Author(s):  
Mark L. Moran ◽  
Roy J. Greenfield ◽  
Steve A. Arcone

We demonstrate that ground penetrating radar (GPR) reflection data from a temperate glacier are accurately modeled using a Helmholtz‐Kirchhoff diffraction integration technique that incorporates the radiation characteristics of point dipoles on a half‐space interface. This is accomplished by comparing field data to simulated data. Our 40‐MHz field data are from a 100 × 340 m (x‐ and y‐dimensions, respectively) survey grid containing 51 parallel survey lines. The field data were collected with the dipole oriented perpendicular to the survey line (x‐dipole). The synthetic data used isotropic, x‐dipole, and y‐dipole antennas, and reflections were calculated using a bed topography previously defined by 3D Kirchhoff migration. The comparisons between the real and synthetic waveforms show excellent agreement, including reflection arrival times, amplitude trends, interference patterns, and false layering from out‐of‐plane reflections. The location of reflectors determined from exploding reflector rays explains that bed reflections rapidly sink below background noise levels when reflections originate in the antenna's E‐plane. This occurs in both the simulated data and field data. Our results are of general importance for radio‐glaciology because they demonstrate that inappropriate dipole orientation with respect to the specular reflection point can lead to more than 12‐dB reduction in bottom reflection strength. Furthermore, a complicated bottom topography readily generates secondary, out‐of‐plane reflections that are easily confused with basal till layers.


1998 ◽  
Vol 80 (12) ◽  
pp. 2614-2617 ◽  
Author(s):  
J. Kasper ◽  
H. Leeb ◽  
R. Lipperheide

Geophysics ◽  
2001 ◽  
Vol 66 (2) ◽  
pp. 540-550 ◽  
Author(s):  
Albane C. Saintenoy ◽  
Albert Tarantola

The three electromagnetic properties appearing in Maxwell’s equations are dielectric permittivity, electrical conductivity and magnetic permeability. The study of point diffractors in a homogeneous, isotropic, linear medium suggests the use of logarithms to describe the variations of electromagnetic properties in the earth. A small anomaly in electrical properties (permittivity and conductivity) responds to an incident electromagnetic field as an electric dipole, whereas a small anomaly in the magnetic property responds as a magnetic dipole. Neither property variation can be neglected without justification. Considering radiation patterns of the different diffracting points, diagnostic interpretation of electric and magnetic variations is theoretically feasible but is not an easy task using ground‐penetrating radar. However, using an effective electromagnetic impedance and an effective electromagnetic velocity to describe a medium, the radiation patterns of a small anomaly behave completely differently with source‐receiver offset. Zero‐offset reflection data give a direct image of impedance variations while large‐offset reflection data contain information on velocity variations.


1998 ◽  
Vol 248 (1-4) ◽  
pp. 338-342 ◽  
Author(s):  
C.F. Majkrzak ◽  
N.F. Berk ◽  
J.A. Dura ◽  
S.K. Satija ◽  
A. Karim ◽  
...  

1990 ◽  
Vol 95 (B4) ◽  
pp. 4657 ◽  
Author(s):  
Robert B. Hawman ◽  
Robert H. Colburn ◽  
David A. Walker ◽  
Scott B. Smithson

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