Title: Applied Geophysics
1GEOL 492/692
Applied Geophysics 4 credits SP07
call84362/87487Instructor Dr. John Louie, LME
217, ph 784-4219 louie_at_seismo.unr.edu and GEOL
493/693 Mining Exploration Geophysics 4 credits
SP07 call 89118/88005Instructor Dr. Gary
Oppliger, LME 304, ph 784-7056 oppliger_at_mines.unr.
edu Office hours 1200-1 pm M,T,W
2Electrical Properties of RocksandElectrical
Resistivity Methods
3Resistance
Definition of an OHM An ohm is a resistance in a
conductor that produces a potential difference of
one volt when a current of one ampere is flowing
through it. Â Â Â Â Â Â Â Â Â Â Â Â Â Â Â Â Â Â Â Â Â
R
4Ohms Law
http//hyperphysics.phy-astr.gsu.edu/hbase/electri
c/ohmlaw.htmlc1
5Resistance vs Resistivity
Resistance is relevant only to a particular
measurement circuit. Units Ohms
Resistivity is an intrinsic property of all
physical materials Units Ohm-Meters
Apparent Resistivity is a resistivity estimate
based on a assuming a half-space geometry.
Units Ohm-meters
6Electrical Resistivity vs Electrical Conductivity
Resistance ? (ohm-meters)
Conductivity s 1/? (mho/meters)
7Calculating Resistance from Resistivity
- http//www.cflhd.gov80/agm/index.htm
8Factors Influencing Electrical Conductivity in
Rocks
Porosity (connected/effective - fractures or
pores)
Pore saturation ( air or gas)
Hydrocarbon Fluid Saturation
Water salinity (TDS)
Clay Content
Metallic Sulfide Mineral Content
Fluid temperature
Rock Matrix intrinsic resistivity
9Archies Law
10Formation Factor
11The conductivity of most geological formations
can be fit to Archies Law
12Influence of Permeability
A rock with a non-conducting matrix must be
permeable (connected pores) as well as porous to
conduct electricity.  Darcy's Law           Â
                                               Â
                                                 Â
           Ohm's Law           Â
                                                Â
                                                 Â
                     where           Â
                                                 Â
                      Â
Despite the similarity between Darcys and Ohms
Laws, electric currents have zero viscosity so
even a narrow crack can provide an effective
electrical connection between pores that not
contribute to hydraulic permeability.
13Comparison of electric and hydraulic properties.
Electrical Hydraulic
Transverse resistance  T S hiri Hrl Transmissivity  Th Shiki KlH
Longitudinal conductance S Shi/ri H/rl Leakance LhSki/hi Kt/H
Average aquifer resistivities rl, rt Average hydraulic conductivities Kl, Kt
- http//www.cflhd.gov80/agm/index.htm
14Metallic Sulfide Mineral Content
Electrical resistivity of rocks with various wt
of sulfide.Â
- http//www.cflhd.gov80/agm/index.htm
15Effect of Water Temperature
http//appliedgeophysics.berkeley.edu7057/dc/figu
res/fig43_7.jpg
16Conductivity Ranges of Various Materials
http//www.cflhd.gov80/agm/index.htm
17http//www.cflhd.gov80/agm/index.htm
18http//www.cflhd.gov80/agm/index.htm
19http//www.cflhd.gov80/agm/index.htm
20Resistance vs Resistivity
Resistance is relevant only to a particular
measurement circuit. Units Ohms
Resistivity is an intrinsic property of all
physical materials Units Ohm-Meters
Apparent Resistivity is a resistivity estimate
based on a assuming a half-space geometry.
Units Ohm-meters
21Calculating Resistance from Resistivity
- http//www.cflhd.gov80/agm/index.htm
22Four Electrode Resistivity Measurement on rock
sample
are used to avoid electrode contact resistance
effects seen in two electrode measurements.
23Four electrode resistivity arrays
http//www.cflhd.gov/agm/images/fig90.jpg
24The Basic Concept of an Earth Resistivity
Measurement
http//www.cflhd.gov/agm/images/fig91.jpg
25Fig. 5.4g
Electrode Contact Resistance is typically much
higher than the intrinsic earth resistivity
26Fig. 5.4g
Electrode Contact Resistance is concentrated
around each electrode
27Fig. 5.4g
If a standard two electrode resistivity meter
were used to measure the earths resistance we
only obtain information on the quality of the
electrode contacts not the earths resistivity
28Pole-Pole Array
http//appliedgeophysics.berkeley.edu7057/dc/em44
.pdf
29Pole-Dipole Array
http//appliedgeophysics.berkeley.edu7057/dc/em44
.pdf
30Pole-Dipole Array
http//appliedgeophysics.berkeley.edu7057/dc/em44
.pdf
31Wenner Array
http//appliedgeophysics.berkeley.edu7057/dc/em44
.pdf
32Schlumberger
http//appliedgeophysics.berkeley.edu7057/dc/em44
.pdf
33Dipole-Dipole Array
34Fig. 5.4g
The electric potential varies as 1/r around a
single current electrode on a homogeneous
half-space
35Fig. 5.5g
36Fig. 5.9g
37Fig. 5.6g
Equal potential voltage surfaces between the
electrodes
38Depth of current flow between two current
electrodes
39Fig. 5.14g
40Fig. 5.13g (a)
41Fig. 5.13g (b)
42Fig. 5.13g (c)
43Fig. 5.12g (a)
44Fig. 5.12g (b)
45Fig. 5.12g (c)
46Fig. 5.14g
47Fig. 5.15g (a)
48Fig. 5.15g (b)
49Fig. 5.13g (b)
50Fig. 5.13g (c)
51Fig. 5.14g
52Fig. 5.15g (a)
53Fig. 5.15g (b)
54Fig. 5.18g (a)
55Fig. 5.18g (b)
56Fig. 5.18g (c)
57Fig. 5.19g
58Fig. 5.21g (a)
59Fig. 5.20g
60Fig. 5.21g (b)
61Fig. 5.21g (c)
62Fig. 5.22g
63Fig. 5.23g (a)
64Fig. 5.23g (c)
65Fig. 5.24g (a)
66Fig. 5.24g (c)
67Fig. 5.25g (a)
68Fig. 5.25g (b)
69Fig. 5.26g
70Fig. 5.27g (a)
71Fig. 5.27g (b)
72Fig. 5.28g
73Fig. 5.29g
74Fig. 5.30g (a,b)
75Fig. 5.30g (c,d)
76Fig. 5.31g
77Fig. 5.33g (a)
78Fig. 5.33g (b)
79Fig. 5.33g (c)
80Fig. 5.39g
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82One point removed
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84C\Shortcut to Geo-CD-ROM.exe
85Airborne EM Resistivity
86Airborne EM Resistivity
87http//ece.uprm.edu/pol/waves_review.pdf
88http//appliedgeophysics.berkeley.edu7057/dc/arch
ie/index.html
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