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・ Amplitude (video game)
・ Amplitude adjusting
・ Amplitude amplification
・ Amplitude and phase-shift keying
・ Amplitude damping channel
・ Amplitude death
・ Amplitude distortion
・ Amplitude domain reflectometry
・ Amplitude gate
・ Amplitude modulation
・ Amplitude modulation signalling system
・ Amplitude of accommodation
・ Amplitude of low frequency fluctuations
・ Amplitude panning
・ Amplitude Studios
Amplitude versus offset
・ Amplitude-companded single-sideband modulation
・ Amplitude-Comparison Monopulse
・ Amplitude-shift keying
・ Amplituhedron
・ AmpLive
・ Amplypterus
・ Amplypterus celebensis
・ Amplypterus mansoni
・ Amplypterus mindanaoensis
・ Amplypterus panopus
・ Amplypterus sumbawanensis
・ Ampm
・ Ampney
・ Ampney Crucis


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Amplitude versus offset : ウィキペディア英語版
Amplitude versus offset

In geophysics and reflection seismology, amplitude versus offset (AVO) or amplitude variation with offset is the general term for referring to the dependency of the seismic attribute, amplitude, with the distance between the source and receiver (the offset). AVO analysis is a technique that geophysicists can execute on seismic data to determine a rock’s fluid content, porosity, density or seismic velocity, shear wave information, fluid indicators (hydrocarbon indications).〔http://www.glossary.oilfield.slb.com/Display.cfm?Term=amplitude%20variation%20with%20offset Schlumberger Oilfield Glossary〕
The phenomenon is based on the relationship between the reflection coefficient and the angle of incidence and has been understood since the early 20th century when Karl Zoeppritz wrote down the Zoeppritz equations. Due to its physical origin, AVO can also be known as amplitude versus angle (AVA), but AVO is the more commonly used term because the offset is what a geophysicist can vary in order to change the angle of incidence. (See diagram)
==Background and theory==

For a seismic wave reflecting off an interface between two media at normal incidence, the expression for the reflection coefficient is relatively simple:
:R=\frac,
where Z_0 and Z_1 are the acoustic impedances of the first and second medium, respectively.

The situation becomes much more complicated in the case of non-normal incidence, due to mode conversion between P-waves and S-waves, and is described by the Zoeppritz equations.

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