Banded Contour Map
– a residual
magnetic map where color (or gray-scale) bands are used instead of standard
contour lines, and each color band represents the same magnitude values. The
width of a contour band equals a preselected interval between mapped values. B.C.M. can be very helpful in delineation of faults and determining
their upthrown/downthrown sides by the criterion of an abrupt color bandwidth
change. [75].
See also Interruption Zones
and Basement Fault Block Pattern.
Band-Pass Filter
– a
spectral domain filter that retains (passes) a pre-selected range of wavelengths
or wavenumbers (spatial frequencies). Wavelengths between two specified Cutoff values will be retained. [99, 201,
223].
See Band-Pass Filtering.
Band-Pass Filtering
– a procedure
that enhances a pre-selected range of the potential field components, regional
or residual, based on their wavelengths or wavenumbers (spatial frequencies).
The wavelength of anomaly is partially dependent on the depth to the source and,
hence, B.F.
can be used to separate qualitatively the deeper sources from the shallower
ones. [201,
223].
See also Energy Leakage.
Bandwidth
– a range
of spatial frequencies or wavelengths contained in a profile or grid of data;
also the range of spatial frequencies over which a given filter is designed to
operate in the pass or reject mode, or the range of frequencies containing
significant energy for a given anomaly. [223,
257].
See Bandpass Filter and Wavelength.
Barometric Altimeter
– an
instrument to measure and record the elevation above sea level with common
accuracy of about 0.3 m (1.0 ft). Corrections must be made for temporal and
spatial variations caused by weather. Temperature and humidity corrections are
also needed for precise ground elevations. [57].
Bartlett Filter
– an
edge-smoothing space domain grid and line filter which modifies the original
data values (line curves or grid surface) within Rolloff
Window to ensure their
smooth transition to zero at the ends of survey lines or edges of a grid. B.F. is also referred to as Triangular
Filter. [201].
Base Station
– the
reference magnetic or gravity observation station. In airborne magnetic surveys,
it is used to monitor and record the Diurnal Variations (which should be removed from the observed magnetic
data) and magnetic storms as well as provide GPS correction
data. B.S.
should be set up in the magnetically quiet area, away from power lines,
pipelines, roads or other sources of noise. In gravity surveys, B.S.
is used as a reference point to anchor geodetic survey data as well as to
determine an instrumental Drift. The local gravity base stations are tied to the national
gravity base stations with a known Absolute
Gravity value to allow
the merging of different survey datasets as well as correct application of Latitude
Correction. See also International
Standardized Gravity Network,
Ground Magnetometer and Differential GPS and
Magnetic Storm.
Base Station Magnetometer
– see Ground
Magnetometer.
Basement
– a term used
primarily in oil and gas exploration to refer to the crystalline rocks beneath
the sedimentary section. Usually this term is synonymous with Crystalline
Basement. However the term Economic Basement is used when metamorphic rocks exist which are of high enough grade
that no hydrocarbons are expected within them. This may be different from Magnetic
Basement, which is the top of the first continuously magnetic
layer below the sedimentary section. As a rule, B. is composed
of igneous and metamorphic rocks. In many regions, B. is of the Precambrian age but it also may be younger. Magnetic
susceptibility of B.
rocks is much higher than that of the sedimentary section, up to 100-1000 times
and even more. In addition, heterogeneity of B.
yields very high susceptibility contrasts. Because of all that, for magnetic
exploration B. is the dominant regional subsurface structure that contributes to the
total intensity of the magnetic field after applying IGRF
Correction. [13,
18,
75, 76,
107,
210].
Basement Fault Block Pattern
– an assemblage of Crystalline
Basement blocks of
varying shapes, sizes and often depths, separated by alignments of weakness
zones, i.e., intra-basement faults. B.F.B.P.
may exert a profound control on the structure and stratigraphy of the
sedimentary section, both during and after the deposition of sediments. B.F.B.P.
also controls the topography (i.e., surface relief) of the Crystalline
Basement which, in
turn, controls additionally the structure and stratigraphy of the sedimentary
section through the mechanism of gravitational compaction. [74,
75,
76].
See also Banded Contour Map
and Basement.
Basement Relief
– a range of
the basement surface depths in the survey area. The rough basement has a “high
relief” and the flat basement has a “low relief”. See also Anomaly
Relief.
Bay – a transient magnetic disturbance with the period of about an hour. It originates outside the Earth and has the appearance of “a bay along the sea coast” on the geomagnetic field curve recorded at Base Station or other stationary point of measurements. [223].
BHGM
– 1) borehole
gravimeter model; 2) borehole gravity measurements using a remote-controlled
gravimeter lowered into cased or uncased wells. The maximum achievable amplitude
and wavelength resolution of BHGM
is estimated as 0.002–0.005 mGal and 7–12 m. [36,
123].
See Borehole Gravity, Amplitude
Resolution, and Wavelength
Resolution.
BHGM Density
– a rock
density directly measured in a borehole (i.e., apparent Density) using
a remote-controlled gravimeter lowered into a cased or uncased well. See BHGM.
Bi-Cubic Spline Method
– a grid
resampling method which involves two steps: 1) using the
spline curves along the rows of the original grid to calculate
interpolated values that will correspond to the columns in a new (resampled)
grid; and 2) using the column values obtained in the first step to calculate a
spline curve along each resampled column. B.-C.S.M.
is very effective for resampling datasets with relatively small changes of
values between adjacent grid cells and for smoothing noisy grids. See Resampling.
Bi-Directional Gridding
– a
gridding method that, at first, interpolates the data along the flight lines and
then re-interpolates across the flight lines to create a rectangular Grid. Generally, B.G. enhances
anomalous trends that are orthogonal to the direction of the flight lines. [126]. See Gridding
and Minimum Curvature.
Big G
– see Universal
Gravitational Constant.
Bipole Map
– a map that
represents the line-by-line image of the traverse line data as the sequence of
bar-graphs with their heights proportional to the amplitudes of horizontal
derivatives computed along each traverse line. The polarity of bar graphs is
depicted with a color: for example, red for positive values, blue for negative
values. Each bar graph is plotted at the location of the computed value of a
horizontal derivative. A wavelength-dependent Automatic Gain Control (AGC)
filter is applied to control the dynamic range of horizontal derivatives so that
both small- and large-amplitude anomalies could be displayed. Before applying a
horizontal derivative operator, the traverse line data are filtered with a
low-pass filter in order to suppress high-frequency noise. B.M.
of the 1-st, 2-d, 3-d and 4-th horizontal derivatives can also be calculated. [163]. See Shaded
Stacked Profiles.
Bird
– a
streamlined cylindrical housing (suspended from an aircraft by a cable) where
the sensors are mounted in some airborne surveys. To eliminate magnetic effects
of aircraft, B. is towered by cable at a distance of 50-100 m below and
behind the aircraft. Fixed Wing
Survey is commonly
flown with sensors mounted in the aircraft tail stinger and (Gradiometry option) wings, while helicopters are more likely to tow
B. [223,
238].
See also Fixed Wing Survey and Helicopter
Survey.
Blackman Filter
– an edge
smoothing spectral domain filter that smoothes the grid data values at the edges
of a grid to ensure their smooth transition to zero. B.F. is an
alternative to Hanning Filter,
Hamming Filter and
Bartlett Filter.
[201]. See Edge Smoothing Filters.
Blakely Test
– an
interactive calculation of the maximum values of the gridded magnetic or gravity
data using Blakely-Simpson Method.
See also Gridding.
Blakely-Simpson Method
– an
automated polynomial fitting method of locating maxima on contoured maps of the
gridded gravity or magnetic data. The calculating algorithm compares each grid
intersection with its eight nearest neighbors in four directions (along the row,
column and both diagonals) to determine the presence of a maximum. This
comparison is tested with the system of inequalities. For each satisfied
inequality requirement, the horizontal location and magnitude of the particular
maximum are found by interpolating a second-order polynomial through the trio of
grid intersection points. B.-S.M. requires
no assumptions about the sources except the direction of magnetization in the
magnetic case. At the horizontal gradient maps, abrupt source edges and
near-vertical contacts are more precisely delineated than non-vertical contacts.
Along with other methods, B.-S.M. is used in Boundary
Analysis. [26].
Borehole Gravimeter
– a
remote reading Gravimeter
which can be lowered into a cased or uncased well.
The difference between the gravity readings at two different true
vertical depths gives Apparent
Density value (See Borehole
Gravity). The density
computed is a bulk density value with its sourve coming mostly between the depth
interval measured. Depending on the
size of this interval, B.
G. can detect effects
of sources located tens to hundreds of feet/meters away from the well. [36,
223].
See also Airborne Gravity Meter
and Shipboard Gravimeter.
Borehole Gravity
– a method and
instrumentation for gravity observations (measurements) with the gravimeter
being lowered into a cased or uncased well with the purpose of direct rock
density measurements. Two gravity measurements are needed to calculate the
density of the interval between the measurement points:
p = 3.686 – 128.5 )g / )h1 = 3.686 – 39.18 )g /)h2
;
where “p” is Apparent Density; in g / cm3; “)g” is the gravity difference in mGal;“)h1”
is the depth difference in meters; “)h2”
is the depth difference in feet. Precise measurement of the vertical distance
between stations is necessary to compute accurate densities over small
intervals. Generally, borehole conditions have little effect on B.G.
data. Maximum wellbore deviations should not exceed 15º. [211,
223].
See also BHGM.
Borehole Magnetics
– a method and
instrumentation to provide measurements of the magnetic properties of rocks in
boreholes. B.M.
acquisition system usually incorporates both Susceptibility
and Total Magnetic Field measurements by using three orthogonally oriented fluxgate
magnetometers. See Fluxgate Magnetometer,
Magnetic Stratigraphy, and Magnetic
Susceptibility Logging.
Bottom Gravity
– a
method and instrumentation to collect and process measurements of the Earth’s
gravity field with Gravimeter
being lowered on the sea bottom. A
shipborne-type gravimeter is modified to fit inside a pressure case mounted on a
self-balancing platform. B.
G. provides high
resolution of sourve bodies and detection of subtle anomalies which often cannot
be detected by conventional sea surface measurements.
See also TOWDOG.
Bott-Smith
Method
– a method of
estimating a depth “H”
to the source of the gravity anomaly:
H
= 0.86 g-max/hoz-max,
where
“g-max” is the
maximum gravity value (i.e., peak of anomaly) and “hoz-max”
is the maximum value of Horizontal
Derivative. Coefficient 0.86 is applied for 3-D source bodies,
and 0.65 is applied for 2-D bodies. B.-S.M.
is also referred to as Smith Rule or Maximum Depth
Rule. [27].
See Depth Rules.
Bouguer Anomaly
– a) a local
anomaly observed in Bouguer Gravity.
B.A.
represents the sum of gravity responses of all bodies that have densities
deviating from the accepted correction model; b) more often, the value obtained
after the known values of the gravity field at that location are removed, i.e.
“B. A. =
observed gravity-corrected Earth’s model”.
These known values (Earth’s model) include:
1) latitude effect, i.e. Latitude
Correction; 2)
elevation effect which includes both free-air and Bouguer effects, i.e. Free-Air
Correction and Bouguer
Correction; and,
usually, 3) terrain effects, i.e. Terrain
Correction.
The resulting B. A. gravity field is not the same as the gravity field which
would have been observed at the datum elevation, because the shape of anomalies
due to remaining density irregularities still are appropriate to the elevation
of the point of measurement rather than to those of the datum elevation. [32,
34
,
215,
223].
Bouguer Correction
– a correction
which is applied to the gravity data to eliminate the gravitational effect of
the subsurface mass between the point of measurement (i.e. Station) and
datum (usually, the sea level). B.C.
formula can be presented as
B.C.
= – 0.04192 Dh1 = – 0.01278 Dh2
where “D” is the assumed average rock density between the station and datum
elevations or, in the case of stations below the datum elevation, the assumed
density of rock that is missing between the station and datum in g/cm3;
“h1”
is the elevation above sea level (or datum) or thickness of Bouguer
Slab in meters; “h2”
is of the same meaning
as “h1” but in feet. For
land and airborne surveys, B.C.
is always subtracted from the observed data. Two main assumptions are made here:
1) the elevation difference between points of measurements and Datum
can be “filled-in” with a simple infinite slab (for this reason, B.C.
sometimes is referred to as Slab
Correction); 2) the “fill-in” has a reasonable density
distribution. If the estimate of the correction density is wrong, it will result
in either undercorrecting or overcorrecting of data and, thus, accentuate the
topography. If proper average densities for rocks above sea level were used,
there should be little or no correlation between Bouguer
Gravity and topography. There are two B.C. types: a) Simple
Bouguer Correction
which involves making a slab correction based on the station elevation; b) Complete
Bouguer Correction
which involves making Terrain Correction as well as the slab correction. In marine (shipborne)
gravity surveys, B.C. replaces
the sea water with rock, and “D”
in the preceeding formula is the difference
in specific gravity of this Replacement
Rock and that of the sea water and it is added to the observed data.
[34, 54, 134, 137, 173, 215, 223,
234,
238].
See also Bullard B Correction, Free-Air
Correction and
Nettleton Test.
Bouguer Density
– a density
value for the infinite slab of a finite thickness (Bouguer Slab)
that is used for the calculation of Bouguer
Correction. Often, B.D. equals 2.67 g/cm3. [19].
Bouguer Flat Plate
– see Bouguer
Slab.
Bouguer Gravity
– the
gravity field obtained after Free-Air
Correction, Bouguer Correction, Theoretical Gravity
Correction, and,
usually, Terrain
Correction have been
applied to the observed (measured) gravity data. B.G. is often
referred to as Simple Bouguer Field
for the gravity field before applying the terrain correction and Complete
Bouguer Field for the
gravity field after applying the terrain correction. In concept, B.G. is the residual gravity field that is left after removal of
all possible components of the Earth model to represent the effects of density
inhomogeneities due to the local geology. In practice, gravity anomalies
observed in B.G.
are caused by lateral density contrasts within the sedimentary section and Basement (i.e., within Crust)
and sub-crust of the Earth. If proper average densities for rocks above sea
level were used in Bouguer Correction, there should be minimal correlation between B.G. and topography. Sometimes, such correlation is expected and
unavoidable when density changes quickly. For land surveys above sea level, B.G. formula can be presented as
B.G.
= “observed data” + “free-air
correction” –
–
“Bouguer correction” + “terrain correction” – “theoretical gravity
correction.”
[25,
34,
134,
173,
215].
See also Bouguer Anomaly and Bouguer Slab.
Bouguer Gravity Field
– see Bouguer
Gravity.
Bouguer Plate
–
see Bouguer
Slab.
Bouguer Reduction – see Bouguer Correction
Bouguer Slab
– an infinite length slab of a finite thickness and assumed
density (often, 2.67 g/cm3) between the point of measurement and Datum (usually, the sea level). B.S. is used
in the calculation of Bouguer Correction.
B.S. is also referred to as Bouguer Plate.
[54,
223].
Bouguer
Spherical Cap
– the
Earth’s segment that includes all rocks above Datum
(usually, the sea
level) between the observation station and the arc distance along the curved
Earth’s surface out to 166.735 km. B.S.C.
has the height “h” (observation station elevation) which is the same as the
thickness of Bouguer Slab.
The gravity effect of B.S.C. at its apex is
B.S.C.
= 2pGrh,
where “G” is Universal
Gravitational Constant;
“h” is the station elevation; “r” is the
assumed rock density (usually, 2.67 g/cm3). The gravity effect of B.S.C. can also be expressed by the formula
B.S.C. =
A + B,
where “A” is Flat-Plate
Bouguer Factor; “B” is Bullard B
Correction. [137,
234].
Boundary Analysis
– a
methodology that delineates and maps structural discontinuities associated with Density
and Magnetization boundaries.
Originally, B.A. was based mainly on Blakely-Simpson
Method in application
for horizontal gradient maps. At present, the concepts of Analytic
Signal Derivative and Enhanced
Analytic Signal as
well as other techniques can also be used for the same purposes. [26,
52,
116].
Box Filter
– a
processing algorithm which calculates values for the interpolated cells in Grid using local averaging. B.F. tends to
reduce a magnitude and size of grid anomalies.
Boxcar Filter
–
a theoretical approximation of the filter response curve
presented by a rectangular window function which retains (passes) the range of
data components within the window length and rejects all data components beyond
the length of this window. [223].
See also Filter Cutoff
and Filter Order.
Bulk Density
– the weight of a rock material divided by its volume
including the volume of a pore space. [33,
63].
See also Density.
Bull’s Eye Effect
– a
result of Undersampling in the direction of a strike of the short-wavelength anomaly.
B.E.E. appears
in the form of a trend of small separated circular or elongated contours
(“bull’s eyes”) on Contour Map or Color-Scaled Map.
The source of this effect is the inability of gridding algorithms to interpolate
data perfectly when Traverse Line spacing is longer than an extent of a short-wavelength
anomaly. For example, the surface interpolated by Minimum
Curvature algorithm in the absence of data point constrains is a
circle in two dimensions. In Bi-directional
Gridding anomalies
perpendicular to traverse lines are usually well represented, while those at
acute angles are also mapped as bull’s eyes. Sometimes, B.E.E.
is referred to as Pill
Box Effect. [126].
Bullard B Correction
– an
adjustment to Bouguer Correction which accounts for the curvature of the Earth’s
surface. It is recommended that B.B.C.
be applied to the data when Terrain
Correction is calculated for radii greater than 100 km from the
observation station. B.B.C.
can also be defined as the difference between the gravity effects of Bouguer
Spherical Cap and
equally thick infinite flat plate (Bouguer
Slab). [135,
136,
234].
Butterworth
Filter
– a spectral
domain filter which retains (passes) one end of the data spectrum according to
the specified cutoff (central) frequency or wavenumber. B.F.
is characterized by a very flat amplitude response within the passband. There
are low-pass and high-pass options available. The transition between the passed
and rejected spectrum portions can be made steeper or smoother depending on the
pre-selected degree of B.F. (the higher degree—the steeper transition and vice
versa). B.F.
is usually applied in Microleveling. Mathematically, B.F.
can be presented as
F(k) = 1 / [1 + (k / kc
) n ],
where “kc”
is Central Wavenumber;
“n” is a
degree (order) of the Butterworth filter function. [67,
124,
201, 223].
See also Stabilized Downward
Continuation.