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Next: INTERPOLATION STRATEGIES Up: Nichols: Integration along a Previous: Introduction

A MODEL PROBLEM

To illustrate the various interpolation techniques I will use a 2-D surface that is a plane wave of frequency, $\omega$, and slowness, p,

\begin{displaymath}
f(x,t) = sin( \omega ( t - p x ) ).\end{displaymath}

This function is shown in Figure [*] for a frequency of 20Hz and a slowness of 1/2000 $\rm ms^{-1}$.

 
raw-func
raw-func
Figure 1
Example continuous data, a mono-frequency plane wave with frequency 20Hz and slowness 1/2000 $\rm ms^{-1}$.
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If this data is sampled using typical seismic data sampling rates, 4ms in time and 25m in space, the data shown in figure [*] is obtained. This is the input data to the various interpolation schemes,

\begin{displaymath}
\tilde{f}(ix,it) = f(x_{ix},t_{it})\,;\ ix \in \{1,\ldots,nx \}, it \in \{1,\ldots,nt\}\end{displaymath}

The data is sampled at coordinates given by xix and tit.

 
sampled-func
sampled-func
Figure 2
Input data sampled every 4ms in time and 25m in space.
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In the following examples I consider the case of an integral path on a 2-D surface that is defined by time as a function of space, t(x). The aim of this paper is to obtain the integral along a particular path as the sum over all the traces of the trace scaled by a weighting function which is localized around the intersection of the integration trajectory and each trace, t(xix), with nearest sample point it(ix). The curve integral can then be expressed as a sum over the sampled data points.

\begin{displaymath}
\int_{xmin}^{xmax} f( x, t(x) ) \, dx = \sum_{ix=1}^{nx} \, 
 \sum_{j=-n}^{+m} w(ix,it,j) \tilde{f}(ix,it(ix) + j)\end{displaymath}


previous up next print clean
Next: INTERPOLATION STRATEGIES Up: Nichols: Integration along a Previous: Introduction
Stanford Exploration Project
11/17/1997