# Difference between revisions of "Horizontal resolution"

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Aliasing is discussed in problem 9.4. | Aliasing is discussed in problem 9.4. | ||

− | [[file:Ch06_fig6-2a.png|thumb|{{figure number|6.2a.}} Geometry of first Fresnel zone.]] | + | [[file:Ch06_fig6-2a.png|thumb|center|{{figure number|6.2a.}} Geometry of first Fresnel zone.]] |

− | [[file:Ch06_fig6-2b.png|thumb|{{figure number|6.2b.}} Amplitude versus reflector radius.]] | + | [[file:Ch06_fig6-2b.png|thumb|center|{{figure number|6.2b.}} Amplitude versus reflector radius.]] |

=== Solution === | === Solution === |

## Latest revision as of 16:13, 8 November 2019

Series | Geophysical References Series |
---|---|

Title | Problems in Exploration Seismology and their Solutions |

Author | Lloyd P. Geldart and Robert E. Sheriff |

Chapter | 6 |

Pages | 181 - 220 |

DOI | http://dx.doi.org/10.1190/1.9781560801733 |

ISBN | ISBN 9781560801153 |

Store | SEG Online Store |

## Contents

## Question

Assume that a salt dome can be approximated by a vertical circular cylinder with a flat top of radius 400 m at a depth of 3200 m. If the average velocity above the top is 3800 m/s, what is the minimum frequency that will give a recognizable reflection from the dome?

### Background

Huygens’s principle (see problem 3.1) states that waves are reflected from all illuminated parts of a reflector, the phase varying with the two-way traveltime from source to reflecting point to receiver. Thus the receiver records energy from all points of the reflecting area, the “reflection” being the sum of all of the increments, each with a different phase.

The *first Fresnel zone* (often referred to as “*the Fresnel zone*”) is the portion of the reflector from which the reflected energy arrives more-or-less in-phase so that it adds constructively. For constant velocity, it is a circle centered at the reflecting point and extending out to where the slant distance is such that (see Figure 6.2a). Because , the Fresnel zone radius is

**(**)

The annular ring defined by and , where , is the second Fresnel zone, the outer radius being , and so on for successive zones. The amplitude of the total reflected energy as a function of is plotted in Figure 6.2b (see Sheriff and Geldart, 1995, section 6.2.3 for more details). The amplitude depends mainly on the first zone, the contributions of successive pairs of the other zones effectively cancelling each other. The first Fresnel zone is usually taken as the limit of the horizontal resolution for unmigrated seismic data, reflectors smaller than this appearing almost as point diffractors.

Aliasing is discussed in problem 9.4.

### Solution

For a recognizable reflection (as opposed to a diffraction) on an unmigrated section, the radius of the dome should be at least as large as that of the first Fresnel zone, that is,

Solving for the frequency , we have

For frequencies lower than 38 Hz, the top of the dome is smaller than the Fresnel zone and the reflection energy falls off so that the reflection may not be recognized as such.

## Continue reading

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Characteristics of different types of events and noise | Reflection and refraction laws and Fermat’s principle |

Previous chapter | Next chapter |

Geometry of seismic waves | Characteristics of seismic events |

## Also in this chapter

- Characteristics of different types of events and noise
- Horizontal resolution
- Reflection and refraction laws and Fermat’s principle
- Effect of reflector curvature on a plane wave
- Diffraction traveltime curves
- Amplitude variation with offset for seafloor multiples
- Ghost amplitude and energy
- Directivity of a source plus its ghost
- Directivity of a harmonic source plus ghost
- Differential moveout between primary and multiple
- Suppressing multiples by NMO differences
- Distinguishing horizontal/vertical discontinuities
- Identification of events
- Traveltime curves for various events
- Reflections/diffractions from refractor terminations
- Refractions and refraction multiples
- Destructive and constructive interference for a wedge
- Dependence of resolvable limit on frequency
- Vertical resolution
- Causes of high-frequency losses
- Ricker wavelet relations
- Improvement of signal/noise ratio by stacking