Download - Gravity Surveying - fac.ksu.edu.sa
![Page 1: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/1.jpg)
1
Gravity Surveying
![Page 2: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/2.jpg)
2
Introduction
Gravity surveying…
Investigation on the basis of relative variations in the
Earth’s gravitational field caused by difference of density
between subsurface rocks
![Page 3: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/3.jpg)
Applications
• Exploration of fossil fuels (oil, gas, coal)
• Exploration of mineral deposits
• Exploration of groundwater resources
• Engineering/construction site investigation
• Cavity detection
• Regional and global tectonics
• Shape of the Earth, isostasy
3
![Page 4: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/4.jpg)
5
1. Density of rocks
![Page 5: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/5.jpg)
6
Rock density
Rock density depends mainly on…
• Mineral composition
• Porosity (compaction, cementation)
Lab or field determination of density is
useful for anomaly interpretation and
data reduction
![Page 6: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/6.jpg)
7
2. Equations in gravity surveying
![Page 7: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/7.jpg)
r G m1 m2 rr
r
8
First Newton´s Law
Newton´s Law of Gravitation
2F = -
(x2 - x1)2
+(y2 - y1)2
+(z2 - z1)2r =
M3kg-1s-2G = 6.67×10-11
Gravitational constant
![Page 8: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/8.jpg)
r r rr = gN
R
9
Second Newton´s Law
F = m a a = -G M r r
2
kgM = 5.977×1024
R = 6371 km
mass of a homogeneous Earth
mean radius of Earth
g N 9.81 m s2
gN: gravitational acceleration or „gravity“
for a spherical, non-rotating, homogeneous Earth, gN iseverywhere the same
![Page 9: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/9.jpg)
10
Units of gravity
• 1 gal = 10-2
m/s2
• 1 m gal = 10-3
gal = 10-5
m/s2
• 1 µ gal = 10-6
gal = 10-8
m/s2
(precision of a gravimeter for
geotechnical surveys)
• Gravity Unit: 10 gu = 1 mgal
• Mean gravity around the Earth: 9.81 m/s2
or 981000 mgal
![Page 10: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/10.jpg)
11
Keep in mind…
…that in exploration geophysics,
we are working with values about…
0.01-0.001 m gal 10-8
- 10-9
gN !!!
![Page 11: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/11.jpg)
r U r U r U r
r r dr
12
Gravitational potential field
The gravitational potential field is conservative (i.e. the work to move a mass
in this field is independent of the way)
The first derivative of U in a direction gives the component of gravity in that
direction
U = g = with U = i + j + kx y z
rF
m2
G m1
R
R R
U = g . r dr = -G m1 r 2
=∞ ∞
![Page 12: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/12.jpg)
13
Measurement component
The measured perturbations in gravity effectively correspond to the vertical
component of the attraction of the causative body
we can show that is usually
insignifiant since gz << g
Therefore…
g gz
![Page 13: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/13.jpg)
gr =
cos =r r
14
Grav. anomaly: point mass
from Newton's Law
Gm Gm (z -z)2 3
Gm
r 2
g = gz =
![Page 14: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/14.jpg)
17
3. Gravity of the Earth
![Page 15: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/15.jpg)
18
•
•
Shape of the Earth: spheroid
Spherical Earth with R = 6371 km is an approximation!
Rotation creates an ellipsoid or a spheroid
1
298.247=
Re - Rp
Re
Deviation from a spherical model:
Re - R = 7.2 km
R -Rp =14.3 km
![Page 16: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/16.jpg)
19
![Page 17: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/17.jpg)
20
The Earth´s ellipsoidal shape, rotation, irregular surface relief and internal massdistribution cause gravity to vary over it´s surface
![Page 18: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/18.jpg)
- Rcos
21
•
•
From the equator to the pole: gn increases, gc decreases
Total amplitude in the value of g: 5.2 gal
)22R
g = gn + gC = G (M
![Page 19: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/19.jpg)
22
Reference spheroid
• The reference spheroid is an oblate ellipsoid that
approximates the mean sea-level surface (geoid) with the
land above removed
• The reference spheroid is defined in the Gravity Formula
1967 and is the model used in gravimetry
• Because of lateral density variations, the geoid and
reference spheroid do not coincide
![Page 20: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/20.jpg)
23
Shape of the Earth: geoid
• It is the sea level surface (equipotential surface U = constant)
• The geoid is everywhere perpendicular to the plumb line
![Page 21: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/21.jpg)
24
![Page 22: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/22.jpg)
25
![Page 23: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/23.jpg)
26
Spheroid versus geoid
Geoid and spheroid usually do not coincide (India -105m, New Guinea +73 m)
![Page 24: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/24.jpg)
27
4. Measurement of gravity and interpretation
![Page 25: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/25.jpg)
28
Measurement of gravity
• Large pendulums
• Falling body techniques
• Gravimeters
•
•
Use spring techniques
Precision: 0.01 to 0.001 mgal
Relative measurements are usedsince absolute gravity
determination is complex and
long!
1
2g t 2z =
gLT = 2π
For a precision of 1 mgal
Distance for measurement 1 to 2 m
z known at 0.5 µm
t known at 10-8 s
Absolute measurements Relative measurements
![Page 26: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/26.jpg)
29
Scintrex CG-5
LaCoste-Romberg mod. G
Source: P. Radogna, University of Lausanne
Gravimeters
![Page 27: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/27.jpg)
g = x
g = x with T = 2πT k
30
k
m
4π2 m2
For one period
k is the elastic spring constant
Problem: low sensitivity since the
spring serves to both support the
mass and to measure the data. So this
technique is no longer used…
Stable gravimeters
Hook´s Law
![Page 28: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/28.jpg)
LaCoste-Romberg gravimeter
This meter consists of a hinged beam,
carrying a mass, supported by a spring
attached immediately above the hinge.
A „zero-lenght“ spring can be used, where the
tension in the spring is proportional to the
actual lenght of the spring.
•
•
•
More precise than stable gravimeters (betterthan 0.01 mgal)
Less sensitive to horizontal vibrations
Requires a constant temperature environment
31
![Page 29: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/29.jpg)
CG-5 Autograv
CG-5 electronic gravimeter:
CG-5 gravimeter uses a mass supported bya spring. The position of the mass is kept
fixed using two capacitors. The dV used to
keep the mass fixed is proportional to the
gravity.
••
•
•
Self levellingRapid measurement rate (6 meas/sec)
Filtering
Data storage
32
![Page 30: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/30.jpg)
33
Gravity surveying
![Page 31: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/31.jpg)
Factors that influence gravity
The magnitude of gravity depends on 5 factors:
• Latitude
• Elevation
• Topography of the surrounding terrains
• Earth tides
• Density variations in the subsurface:
this is the factor of interest in gravity exploration, but it is
much smaller than latitude or elevation effects!
34
![Page 32: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/32.jpg)
35
•
•
•
Gravity surveying
Good location is requiredUncertainties in elevations of gravity stations account for the greatest
errors in reduced gravity values (precision required about 1 cm) (use
dGPS)
Frequently read gravity at a base station (looping) needed
![Page 33: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/33.jpg)
37
Observed data corrections
gobs can be computed for the stations using g only after thefollowing corrections:
• Drift correction
• Tidal correction
• Distance ground/gravimeter („free air correction“ see below)
![Page 34: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/34.jpg)
38
Drift correction on observed data
Gradual linear change in reading with time, due to imperfect
elasticity of the spring (creep in the spring)
![Page 35: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/35.jpg)
39
Tidal correction on observed data
Effect of the Moon: about 0.1 mgal
Effect of the Sun: about 0.05 mgal
![Page 36: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/36.jpg)
40
After drift and tidal corrections, gobs can be computed using g, thecalibration factor of the gravimeter and the value of gravity at the base
![Page 37: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/37.jpg)
41
Gravity reduction: Bouguer anomaly
BA = gobs - gmodel
gmodel = g - FAC + BC -TC
•
•
•
•
•
gmodel
g
FAC
BC
TC
model for an on-land gravity survey
gravity at latitude (latitude correction)
free air correction
Bouguer correction
terrain correction
![Page 38: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/38.jpg)
g = g equator (1+1 sin2 +2 sin
4
42
)
Latitude correction
• 1 and 2 are constants dependent on the shape and speedof rotation of the Earth
• The values of 1 , 2 and gequator are definded in the GravityFormula 1967 (reference spheroid)
![Page 39: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/39.jpg)
43
Free air correction
The FAC accounts for variation in the distance of the
observation point from the centre of the Earth.
This equation must also be used to account for the distance
ground/gravimeter.
![Page 40: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/40.jpg)
44
Free air correction
FAC = 0.3086 h (h in meters)
GM
R 2g =
![Page 41: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/41.jpg)
45
Bouguer correction
• The BC accounts for the gravitational effect of the rocks
present between the observation point and the datum
• Typical reduction density for the crust is =2.67 g/cm3
BC = 2πG h
![Page 42: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/42.jpg)
46
Terrain correction
The TC accounts for the effect of topography.
The terrains in green and blue are taken into account in the TC
correction in the same manner.
![Page 43: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/43.jpg)
47
![Page 44: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/44.jpg)
48
![Page 45: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/45.jpg)
49
Residual gravity anomaly
The regional field can be
estimated by hand or
using more elaborated
methods (e.g. upward
continuation methods)
![Page 46: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/46.jpg)
50
Bouguer anomaly
![Page 47: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/47.jpg)
51
Interpretation: the inverse problem
Two ways of solving
the inverse problem:
• „Direct“ interpretation
• „Indirect“ interpretation
and automatic inversion
Warning: „direct“ interpretation has nothing to do with
„direct“ (forward) problem!
![Page 48: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/48.jpg)
52
Direct interpretation
Assomption: a 3D anomaly is
caused by a point mass (a 2D
anomaly is caused by a line
mass) at depth =z
x1/2 gives z
z
mass m
surface
![Page 49: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/49.jpg)
53
Direct interpretation
![Page 50: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/50.jpg)
54
Indirect interpretation
1. Construction of a reasonable model
2. Computation of its gravity anomaly
3. Comparison of computed with observed anomaly
4. Alteration of the model to improve correspondence of
5. observed and calculated anomalies and return to step (2)
![Page 51: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/51.jpg)
55
![Page 52: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/52.jpg)
56
Non-unicity of the solution
![Page 53: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/53.jpg)
57
Automatic inversion
Automatic computer inversion with a priori information for
more complex models (3D) using non-linear optimization
algorithms. Minimize a cost (error) function F
with n the number of data
Automatic inversion is used when the model is complex (3D)
![Page 54: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/54.jpg)
58
Automatic inversion
![Page 55: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/55.jpg)
59
Mining geophysics
![Page 56: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/56.jpg)
60
5. Microgravity: a case history
![Page 57: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/57.jpg)
• length:6 km
• difference in altitude: 323 m
• geology: alpine molassic bedrock (tertiary sandstone) and
an overlaying quaternary glacial fill
• depth of bedrock: varying from 1.5 m to 25 m
• The choice of the corridor had to consider the depth of the
61
bedrock Source: P. Radogna et al.
A SUBWAY PROJECT IN LAUSANNE, SWITZERLAND, AS AN
URBAN MICROGRAVIMETRY TEST SITEP. Radogna, R. Olivier, P. Logean and P. Chasseriau
Institute of Geophysics, University of Lausanne
![Page 58: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/58.jpg)
Zone II
Scintrex CG5
200 gravity stations 62Source: P. Radogna et al.
![Page 59: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/59.jpg)
Geological section,
approximately A´´-A´-A
63Source: P. Radogna et al.
![Page 60: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/60.jpg)
64
Source: P. Radogna et al.
![Page 61: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/61.jpg)
Profile A´´-A´-A
Source: P. Radogna et al.
65
![Page 62: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/62.jpg)
66
Building and basement gravity effect
![Page 63: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/63.jpg)
DEM for topographical corrections
BASEMENT FROM:
•Cadastral plan
•Building typology
•GIS
Source: P. Radogna et al.
67
![Page 64: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/64.jpg)
Bouguer Anomaly
Source: P. Radogna et al.
68
![Page 65: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/65.jpg)
Regional Anomaly
Source: P. Radogna et al.
69
![Page 66: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/66.jpg)
Residual Anomaly
Source: P. Radogna et al.
70
![Page 67: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/67.jpg)
Result…
Source: P. Radogna et al.
71
![Page 68: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/68.jpg)
Painting of the valley and the bridge before 1874
and actual picture of the same zone
Complex building corrections
Source: P. Radogna et al.
72
![Page 69: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/69.jpg)
Rectangular prisms are used for modeling the bridge’s pillars
Source: P. Radogna et al.
73
![Page 70: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/70.jpg)
Gravity effect of the bridge
•Formulation of rectangular
prism (Nagy, 1966)
•Pillar’s density is fixed
to 2.00 g/cm3
Source: P. Radogna et al.
74
![Page 71: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/71.jpg)
Standard corrections gravity anomaly withouttopographical corrections.
Reduction density : 2.40 g/cm3
Source: P. Radogna et al.
75
![Page 72: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/72.jpg)
76
6. Conclusions
![Page 73: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/73.jpg)
77
Advantages
• The only geophysical method that describes directly the
density of the subsurface materials
• No artificial source required
• Useful in urban environment!
![Page 74: Gravity Surveying - fac.ksu.edu.sa](https://reader030.vdocuments.site/reader030/viewer/2022020702/61f9b6f17f39a27f8d0240a1/html5/thumbnails/74.jpg)
78
•
•
•
•
•
Drawbacks
Expensive
Complex acquisition process
Complex data processing
Limited resolution
Very sensitive to non-unicity in the modeling solutions