2274 poisson impedance
TRANSCRIPT
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Deriving the Poisson Impedance in
Hampson Russell Software
Kevin Gerli tz
Geophysicist, VHR Jakarta
April 2006
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The “Poisson Impedance” is an attribute that is derived from acombination of the P- and S-impedance values and is a good
hydrocarbon indicator. This method was described in a paper
called “Poisson Impedance” by Quakenbush, Shang and Tuttle in
The Leading Edge, February 2006.
This document illustrates a method of deriving the “Poisson
Impedance” logs from either P- and S-Impedance well logs or
seismic attribute volumes created from Simultaneous Inversion.
The relationship between the Poisson Impedance and the Fluid
Factor attribute will also be illustrated.
POISSON IMPEDANCE
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POISSON IMPEDANCE
The idea of the Poisson Impedance isillustrated in the figure on the left.
In the Acoustic Impedance / Shear
Impedance cross-plot, it is difficult
to discriminate the litho-fluiddistributions on the horizontal and
vertical axes. But rotating the axis
to be parallel with the trends would
ensure a distinct discrimination ofthe litho-fluid distributions.
The method for defining the Poisson
Impedance can be written as:
PI = AI – cSI
Where c is the term that optimizes
the rotation.From Quakenbush et al. (2006)
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POISSON IMPEDANCE
Recall that the Poisson’s Ratio can be written as:
)2(
)(2
2
)(2
22222
22
VsVp
V V
V V
V V
V V
S P
S P
S P
S P −
−
+=
−
−=σ
If we rewrite the PI=AI – cSI in terms of velocities and density,
then we can define the so-called “Poisson Velocity”
σ ρ ρ ρ ρ V cV V cV V PI S PS P =−=−= )(
Notice that we can now relate the Poisson’s Ratio (1) with the
Poisson Velocity (2) and if we define c=sqrt(2) and a scalingfactor, D, then
σ σ DV =
(1)
(2)
(3)
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POISSON IMPEDANCE
The significance of the c term is that it is the inverse of the slope
of the litho-fluid trends. For example, the Greenberg-Castagna Vp-
Vs equation is Vs = 0.77 Vp – 869 m/s. The inverse of the slope is
1/0.77 = 1.3 which is an approximation to the square root of 2 (i.e.,
1.41).
Implementing this relationship within Hampson-Russell Software
is quite easy to do and involves some simple Trace Maths scripts.
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POISSON IMPEDANCE
In order to create the
Poisson Impedance logs,
you first need to be in eLog
with a well that has both
the P- and S-Impedancelogs.
Click on the Math… button
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POISSON IMPEDANCE
Select the Log Maths
option and select the P-and S-impedance logs for
the input. Make the
Output Log Type of type
“Poisson Impedance”…
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POISSON IMPEDANCE
Type in the equation for
the Poisson Impedance.
If we use c=sqrt(2), thenthe equation is as shown…
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POISSON IMPEDANCE
Similarly, we can
derive the c term from
the cross-plot of the P-
and S-Impedance logsfor the wet trend and
calculate a regression
line. The inverse of
the slope could be
used as the c value, in
this case, 1/.746561 =
1.339.
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POISSON IMPEDANCE
The far right track shows
the computed Poisson
Impedance logs for the two
c values (red: c = 1.41, blue:
c=1.339). The Computed
Poisson Ratio curve is
shown beside it for
comparison.
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POISSON IMPEDANCE
The same
process can be
applied to the P-
and S-impedance
volumes derivedfrom the seismic
using
Simultaneous
Inversion. In thiscase, use
Process > Utility
> Trace Maths
and follow the
same workflow…
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POISSON IMPEDANCE
Here is the output Poisson Impedance volume with the low blue valuesindicating the gas zone. The PI log is spliced into the section.
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POISSON IMPEDANCE
The Poisson Impedance has a very close relationship with the “FluidFactor” attribute. The “Fluid Factor” concept was first introduced in
a paper by Smith and Gidlow in a paper called “Weighted stacking
for rock property estimation and detection of gas”, 1987,
Geophysical Prospecting.The basic idea of the Fluid Factor is that brine-saturated clastic
silicate rocks define a “mudrock line” trend on the Vp-Vs cross-plot
space (Castagna et al., 1985). The mudrock line equation is given
as : Vp = 1.16 Vs + 1360 m/s
The simple idea of the “Fluid
Factor” is that points that lie
further away from the brine wettrend are more likely to have
hydrocarbons.
From Smith and Gidlow (1987)
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POISSON IMPEDANCE
We can derive the following relationship between Vp/Vs andPoisson’s Ratio as follows:
2/1
2/1
1⎟ ⎠
⎞⎜⎝
⎛
−
−=
σ
σ
S
P
V
V
This is a direct linear relationship with Vp/Vs increasing with
increasing σ. The “pseudo-Poisson’s Ratio reflectivity” can thus
be defined as:
S
S
P
P
S P
S P
V
V
V
V
V V
V V Δ−
Δ=
Δ
/
)/(
σ ρ ρ V cV V PI S P =−= )(
Note that reflectivity equation above would be the same as thereflectivity of the previously derived Poisson Velocity.
(4)
(5)
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POISSON IMPEDANCE
The Fluid Factor was defined as the difference between the actualVp reflectivity and the reflectivity calculated from the mudrock line,
i.e.,
S
S
P
S
V
V
V
V c
Vp
VpF
Δ−
Δ=Δ
This was modified by Fatti et al. (1994) to include the density term
and write it in terms of acoustic and shear impedance reflectivities:
S
S
P
S
R
R
V
V c
Rp
RpF Δ−Δ=Δ (7)
(6)
Where c represents the slope of the wet clastic reservoir trend.
Using the mudrock line, c was defined as 1.16 in both the Smith
(1987) and Fatti (1994) papers. The Fluid Factor is thus the
reflectivity of the Poisson Impedance, where the Shear Impedance
has been additionally scaled so that amplitudes are close
to 0.
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REFERENCES
Castagna, J.P., Batzle, M.L., and Eastwood, R. L., 1985.Relationships between compressional and shear-wave velocities
in elastic silicate rocks: Geophysics, 50, p. 571 – 581.
Fatti, J.L., Smith, G.C., Vail, P.J., Strauss, P.J. and Levitt, P.R.,
1994. Detection of gas in sandstone reservoirs using AVO
analysis: a 3-D seismic case history using the Geostack
technique: Geophysics, 59, 1362 – 1376.
Quakenbush, M., Shang, B., and Tuttle, C, 2006. Poisson
Impedance: The Leading Edge, 25, 128 – 138.
Smith, G.C., and Gidlow, P.M., 1987. Weighted stacking for rock
property estimation and detection of gas: Geophysical
Prospecting, 35, 993 – 1014.