Eötvös Correction

Use the Moving Platform Gravity > Corrections by Steps > Eötvös Correction menu option, (geogxnet.dll(Geosoft.GX.Gravity.EotvosCorrection;Run)*), to calculate the Eötvös correction.

Eötvös Correction dialog options

Eötvös equation

Select one of the three variations of the Eötvös correction. The difference between them is in the order of 0.2 milligals (mGal):

  • Exact

  • Glicken

  • Harlan

Correction equations are detailed in the Application Notes.

Script Parameter: EOTVOS_CORRECTION.EQUATION [0 - Exact (default); 1 - Glicken; 2 - Harlan]

Time channel

Select the time channel from the drop-down list. If the current database includes a "Time" channel, it will be automatically selected.

Script Parameter: EOTVOS_CORRECTION.TIME

Units

Specify whether the selected time channel is in hours or seconds.

  • The Eötvös equation requires time in hours. If your time is in seconds, it will be converted automatically.
  • Script Parameter: EOTVOS_CORRECTION.UNITS [0 - Hours; 1 - Seconds]

    Latitude channel

    Select the latitude channel from the drop-down list.

    If a channel named "Latitude" exists in the database, it will be selected by default.

    Script Parameter: EOTVOS_CORRECTION.LATITUDE

    Heading channel

    Provide the heading channel name. If it exists, it will be used; otherwise, it will be generated and saved to the database.

    Script Parameter: EOTVOS_CORRECTION.HEADING

    Velocity channel

    Provide the velocity channel name. If it exists, it will be used; otherwise, it will be generated and saved in units of knots.

    Script Parameter: EOTVOS_CORRECTION.VELOCITY

    Altitude channel

    For airborne surveys, select the channel containing altitude data.

    The Eötvös correction requires elevation relative to the ellipsoid. GPS elevations are typically referenced to the ellipsoid; however, if ellipsoidal elevation is not available, elevation relative to the geoid can be used as a fallback. The error introduced by substituting geoid-based elevation for ellipsoidal elevation is negligible.

    Script Parameter: EOTVOS_CORRECTION.ALTITUDE

    Output Eötvös channel

    Specify the name of the output channel for the Eötvös correction.

    Script Parameter: EOTVOS_CORRECTION.OUTPUT

    Application Notes

    Earth’s rotation produces outward centrifugal acceleration. Objects moving across the rotating Earth experience additional acceleration related to their east-west velocity, with the effects strongest at the equator and decreasing with latitude.

    • A body moving east (in the direction that Earth spins) experiences an increase in centrifugal acceleration.

    • A body moving west experiences decreased centrifugal acceleration.

    The vertical component of this acceleration and a small acceleration related to the motion of the curved Earth are known as the Eötvös effect. This effect can be as large as 30 milligals (mGal) and should be accounted for in moving platform surveys.

    The Eötvös effect is defined as:

    The first term corresponds to the Eötvös effect; the second term is a refinement, which is much smaller in amplitude. To take into account Earth’s ellipsoidal shape, R can be expanded into Earth’s major axis, Earth’s flattening, the latitude, and the observation height to yield the Exact equation below. Two other published variations for the Eötvös effect are also offered.

    [Exact]:

    [Harlan, 1968]1:

     

    [Glicken, 1962]2:

    Where:

    E

    Eötvös correction (milligals)

    R

    Earth’s radius at latitude φ

    V

    Velocity in knots

    Ws

    Angular velocity of Earth’s rotation = 7.2921158533E-5 rad/s

    α

    Heading (direction of movement of the vehicle, measured clockwise from true north)

    ε

    Earth’s eccentricity = (ra-rb) / ra

    φ

    Latitude of the vehicle

    h

    Observation height (height above geoid)

    ra

    Earth’s major axis = 6378137.0 m

    rb

    Earth’s minor axis = 6356752.3141 m

    νe and νn

    Velocities in easting & northing directions calculated from the heading and velocity channels

    References

    • R. B. Harlan, "Eötvös corrections for airborne gravimetry", Journal of Geophysical Research, vol 73, no 14 (July 15, 1968).
    • M. Glicken, "Eötvös corrections for a moving gravity meter", Geophysics, vol 27, no 4 (1962), pp. 531-533.

    *GX.NET tools are embedded in the geogxnet.dll file located in the \Geosoft\Desktop Applications\bin folder. To run this GX interactively (outside the menu), first navigate to the bin directory and provide the GX.NET tool in the required format. See the Run GX topic for more guidance.