2010
DOI: 10.3906/yer-0903-2
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Application of the Normalized Full Gradient (NFG) Method to Resistivity Data

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Cited by 3 publications
(6 citation statements)
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“…}\left( {\frac{1}{M}\mathop \sum \nolimits_{i = 1}^M \sqrt {{{\left( {{{\left( {\frac{{\partial G\left( {{x_i},\;{z_j}} \right)}}{{\partial x}}} \right)}^2} + {{\left( {\frac{{\partial G\left( {{x_i},\;{z_j}} \right)}}{{\partial z}}} \right)}^2}} \right)}^v}} }\right),\end{equation}$$in which i is the counter of observation data, j is the counter of interesting depth, M is the number of observations,0.28emGfalse(xi,zjfalse)/x$\;\partial G( {{x_i},\;{z_j}} )/\partial x$ and0.28emGfalse(xi,zjfalse)/z$\;\partial G( {{x_i},\;{z_j}} )/\partial z$ are the derivatives of Gfalse(xi,zjfalse)$G( {{x_i},\;{z_j}} )$ and v is called the degree of the NFG operator, which controls two important shaping parameters of an envelope, the peak value and the anomaly width of the NFG sections. Although v can be taken as 1, 2, 4, 8 and so forth, v = 1 is generally used for the potential field data (Aydin, 1997). Karsli (2001) suggested that higher order values are more reasonable for seismic applications because they narrow the recorded signal's width and improve the seismic resolution.…”
Section: Geophysical Backgroundsmentioning
confidence: 99%
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“…}\left( {\frac{1}{M}\mathop \sum \nolimits_{i = 1}^M \sqrt {{{\left( {{{\left( {\frac{{\partial G\left( {{x_i},\;{z_j}} \right)}}{{\partial x}}} \right)}^2} + {{\left( {\frac{{\partial G\left( {{x_i},\;{z_j}} \right)}}{{\partial z}}} \right)}^2}} \right)}^v}} }\right),\end{equation}$$in which i is the counter of observation data, j is the counter of interesting depth, M is the number of observations,0.28emGfalse(xi,zjfalse)/x$\;\partial G( {{x_i},\;{z_j}} )/\partial x$ and0.28emGfalse(xi,zjfalse)/z$\;\partial G( {{x_i},\;{z_j}} )/\partial z$ are the derivatives of Gfalse(xi,zjfalse)$G( {{x_i},\;{z_j}} )$ and v is called the degree of the NFG operator, which controls two important shaping parameters of an envelope, the peak value and the anomaly width of the NFG sections. Although v can be taken as 1, 2, 4, 8 and so forth, v = 1 is generally used for the potential field data (Aydin, 1997). Karsli (2001) suggested that higher order values are more reasonable for seismic applications because they narrow the recorded signal's width and improve the seismic resolution.…”
Section: Geophysical Backgroundsmentioning
confidence: 99%
“…q can be equal to any integer number; however, Berezkin (1973) showed that q = 2 could provide better results for oil–gas exploration. Previous research studies (Aydin, 1997; Aghajani et al., 2009a; Dondurur, 2005; Karsli, 2001; Oruç, 2011) proposed that q values of 1 and 2 give a good result in the downward continuation and help to find more accurate depth estimation of subsurface features from geophysical data. Anyhow, this parameter should be defined on field data via a parameter analysis.…”
Section: Geophysical Backgroundsmentioning
confidence: 99%
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