environmental and exploration geophysics ii
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Environmental and Exploration Geophysics II. Gravity Methods (V). t.h. wilson [email protected]. Department of Geology and Geography West Virginia University Morgantown, WV. Simple Geometrical Objects. The Sphere. The Sphere. - PowerPoint PPT PresentationTRANSCRIPT
Environmental and Exploration Geophysics II
t.h. [email protected]
Department of Geology and GeographyWest Virginia University
Morgantown, WV
Gravity Methods Gravity Methods (V)(V)
Diagnostic Position Depth Index Multiplier3/4 max 1/0.46 = 2.172/3 max 1/0.56 = 1.791/2 max 1/0.77 = 1.3051/3 max 1/1.04 = 0.961/4 max 1/1.24 = 0.81
(feet) 00852.0
(feet) 00852.0
feetfor 00852.0
metersfor 02793.0
)3/4(
3
2max
3/12max
2
3
2
3
2
3
max
R
Zg
ZgR
Z
R
Z
R
Z
RGg
The Sphere
You could measure the values of the depth index multipliers yourself from this plot of the normalized curve that describes the shape of the gravity anomaly associated with a sphere.
2
3
max
)3/4(
Z
RGg
32 2max
2
1
1
gshape term
g xz
The Sphere
Diagnostic Position Depth Index Multiplier3/4 max 1/0.58 = 1.722/3 max 1/0.71 = 1.411/2 max 1/1= 11/3 max 1/1.42 = 0.71/4 max 1/1.74 = 0.57
(feet) 01277.0
(feet) 01277.0
feetfor 01277.0
metersfor 0419.0
2
2max
2/1
max
2
2
2
max
R
Zg
ZgR
Z
R
Z
R
Z
RGg
Horizontal Cylinder
2
2
1
1xz
X3/4X2/3
X1/2
X1/3X1/4
Z=X1/2
Locate the points along the X/z Axis where the normalized curve falls to diagnostic values - 1/4, 1/2, etc.
The depth index multiplier is just the reciprocal of the value at X/Z.
X times the depth index multiplier yields Z
1.72
1.41
0.710.58
10.70.57
Depth Index
Multipliers
Z
RGg
2
max
2
2max
2
1
1
gshape term
g x
z
We left you with questions about these two anomalies last Thursday. Which anomaly is associated with a buried sphere and which with the horizontal cylinder?
Sphere:__?_ or Cylinder _?__
What is the depth Z?
If = 0.1 what is R ____?
Sphere:__?_ or Cylinder _?__
What is the depth Z?
If = 0.1 what is R ____?
Diagnosticpositions
MultipliersSphere
ZSphere MultipliersCylinder
ZCylinder
X3/4 = 0.95 2.17 2.06 1.72 1.63X2/3 = 1.15 1.79 2.06 1.41 1.62X1/2 = 1.6 1.305 2.09 1 1.6X1/3 = 2.1 0.96 2.02 0.7 1.47X1/4 = 2.5 0.81 2.03 0.57 1.43
The standard deviation in the estimates of Z assuming that you have a sphere is 0.027kilofeet. The range is 0.06 kilofeet.
When you assume that the anomaly is generated by a cylinder, the range in the estimate is 0.2 kilofeet and the standard deviation is 0.093 kilofeet.
Assuming that the anomaly is generated by a sphere yields more consistent estimates of Z.
Diagnosticpositions
MultipliersSphere
ZSphere MultipliersCylinder
ZCylinder
X3/4 = 1.2 2.17 2.6 1.72 2.06X2/3 = 1.4 1.79 2.5 1.41 1.97X1/2 = 2 1.305 2.6 1 2X1/3 = 2.84 0.96 2.72 0.7 1.99X1/4 = 3.54 0.81 2.87 0.57 2.02
The standard deviation in the estimates of Z assuming that you have a sphere is 0.14 kilofeet. The range is 0.37kilofeet.
When you assume that the anomaly is generated by a cylinder, the range in the estimate is 0.09 kilofeet and the standard deviation is 0.03 kilofeet.
Assuming that the anomaly is generated by a cylinder, in this case, yields more consistent estimates of Z.
Diagnosticpositions
MultipliersSphere
ZSphere MultipliersCylinder
ZCylinder
X3/4 = 0.95 2.17 2.06 1.72 1.63X2/3 = 1.15 1.79 2.06 1.41 1.62X1/2 = 1.6 1.305 2.09 1 1.6X1/3 = 2.1 0.96 2.02 0.7 1.47X1/4 = 2.5 0.81 2.03 0.57 1.43
Diagnosticpositions
MultipliersSphere
ZSphere MultipliersCylinder
ZCylinder
X3/4 = 1.2 2.17 2.6 1.72 2.06X2/3 = 1.4 1.79 2.5 1.41 1.97X1/2 = 2 1.305 2.6 1 2X1/3 = 2.84 0.96 2.72 0.7 1.99X1/4 = 3.54 0.81 2.87 0.57 2.02
If we take the average value of Zsphere as our estimate we obtain Z=2.05kilofeet which we can round off to 2kilofeet
If we take the average value of Zcyl as our estimate we obtain Z=2 kilofeet.
We left you with questions about these two anomalies last Thursday. Which anomaly is associated with a buried sphere and which with the horizontal cylinder?
Sphere: _X_ or Cylinder __
Depth Z = 2kf
If = 0.1 what is R ____?
Sphere:___ or Cylinder _X__
Depth Z = 2kf
If = 0.1 what is R ____?
(kilofeet) 77.12
(kilofeet) 77.12
2max
2/1max
R
Zg
ZgR
(kilofeet) 52.8
(kilofeet) 52.8
3
2max
3/12max
R
Zg
ZgR
Sphere
Cylinder
For the sphere, we find that R = 1 kilofoot
For the cylinder, we find that R is also = 1 kilofoot
If = 0.1gm/cm3
Diagnostic Position Depth Index Multiplier3/4 max 1/0.86 = 1.162/3 max 1/1.1 = 0.911/2 max 1/1.72= 0.581/3 max 1/2.76= 0.361/4 max 1/3.72= 0.27
Ztop
Zbottom
2R
(feet) 000575.0
(feet) 000575.0
metersfor 01886.0
feet 000575.0
2max
2/1max
2
max
2
max
R
Zg
ZgR
Z
Rg
Z
Rg
top
top
top
top
Vertical Cylinder
Note that the table of relationships is valid when Zbottom is at least 10 times the depth to the top Ztop, and when the radius of the cylinder is less than 1/2 the depth to the top.
Diagnostic Position Depth Index Multiplier3/4 max 1/1.48 = 0.682/3 max 1/1.96 = 0.511/2 max 1/3.16 = 0.321/3 max 1/5.16 = 0.191/4 max 1/6.65 = 0.15
(feet) 00936.0
(meters) 0307.0
)3026.2(2
)1/10ln(2
)/ln(2
max
max
12max
Wg
Wg
WG
WG
ZZWGg
Z1
Z2W
The above relationships were computed for Z2=10Z1 and W is small with respect to Z1
Vertical Sheet
The large scale geometry of these density contrasts does not vary significantly with the introduction of additional faults
The differences in calculated gravity are too small to distinguish between these two models
Roberts, 1990
Estimate landfill thickness
http://pubs.usgs.gov/imap/i-2364-h/right.pdf
Morgan 1996
Morgan 1996
Morgan 1996
Derived from Gravity Model Studies
Ghatge, 1993
It could even help you find your swimming pool
3. What is the radius of the smallest equidimensional void (e.g. chamber in a cave) that can be detected by a gravity survey for which the Bouguer gravity values have an accuracy of 0.05 mGals? Assume the voids are formed in limestone (density 2.7 gm/cm3) and that void centers are never closer to the surface than 100m. (Problem 6.5 from Burger et al.)
What simple geometrical object could be used to help you answer this questions?
What size anomaly are you trying to detect?
What equation should you use?
3
max 2
(4 / 3 )G Rg
Z
3. What is the radius …..?
(feet) 00852.0
(feet) 00852.0
feetfor 00852.0
metersfor 02793.0
)3/4(
3
2max
3/12max
2
3
2
3
2
3
max
R
Zg
ZgR
Z
R
Z
R
Z
RGg
Begin by recalling the list of formula we developed for the sphere.
(feet) 02793.0
metersfor 02793.0
3/12max
2
3
ZgR
Z
R
What are your givens?
& Z
Pb. 4: The curve in the following diagram represents a traverse across the center of a roughly equidimensional
ore body. The anomaly due to the ore body is obscured by a strong regional anomaly. Remove the regional anomaly and then evaluate the anomaly due to the ore body (i.e.
estimate it’s depth and approximate radius) given that the object has a relative density contrast of 0.75g/cm3 with
surrounding strata.
Horizontal Position (km)
0.0 0.5 1.0 1.5 2.0
Bou
guer
Ano
mal
y (m
Gal
)
-1.50
-1.25
-1.00
-0.75
-0.50
-0.25
0.00
Problem 5
residual
Regional
You could plot the data on a sheet of graph paper. Draw a line through the end points (regional trend) and measure the difference between the actual observation and the regional (the residual).
You could use EXCEL or PSIPlot to fit a line to the two end points and compute the difference between the fitted line (regional) and the observations.
In problem 5 your given three anomalies. These anomalies are assumed to be associated with three buried spheres. Determine their depths using the diagnostic positions and depth index multipliers we’ve been discussing in class. Carefully consider where the anomaly drops to one-half of its maximum value. Assume a minimum value of 0.
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0.45
0.5
-1500 -1000 -500 0 500 1000 1500
Distance from peak (m)
Bo
ug
uer
An
om
aly
(mG
als)
A.
C.
B.
Anomaly from object of unknown geometry
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1000 1500 2000 2500 3000
Distance (meters)
An
om
aly
(mG
als)
Given = 1 gm/cm3
• Problems 6.1 through 6.3 are due today Tuesday, Nov. 6th.
• Hand in gravity lab this Thursday, Nov. 8th .
• Turn in Part 1 (problems 1 & 2) of gravity problem set 3, Thursday, November 8th. Remember to show detailed computations for Sector 5 in the F-Ring for Pb. 2.
• Turn in Part 2 (problems 3-5) of gravity problem set 3, Tuesday, November 13th.
• Gravity paper summaries, Thursday, November 15th.