2274 poisson impedance

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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 

    P

    This is a direct linear relationship with Vp/Vs increasing with

    increasing σ. The “pseudo-Poisson’s Ratio reflectivity” can thus

    be defined as:

    P

    P

    S P

    S P

    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.,

    P

    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:

    P

     R

     R

    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.