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Self‐potential (SP) Method
•or spontaneous polarization method is based on the surface measurement
of natural potentials resulting from electrochemical reactions in the
subsurface.
subsurface.
•does not require electric currents to be injected into the ground as in the
RESISTIVITY & IP methods
RESISTIVITY & IP methods.
•has been used in base metal exploration, to detect the presence of massive
b di i t t t th IP th d hi h i d t d i tl t
ore bodies, in contrast to the IP method which is used to predominantly to
investigate disseminated ore bodies.
•has been increasingly used in groundwater & geothermal investigations,
environmental and engineering applications‐‐‐> mapping seepage flow
associated with dams, geological mapping, delineate shear zones and near‐
associated with dams, geological mapping, delineate shear zones and near
surface faults.
•ranks as the cheapest of surface geophysical methods in terms of
•ranks as the cheapest of surface geophysical methods in terms of
equipment necessary and amongst the simplest to operate in the field.
Occurrence of Self‐potentials
•SP method is passive, i.e. differences in natural ground potentials are
measured between any two points on the ground surface.
•The potentials measured can range from < a millivolt (mV) to > 1
Volt.
• + or – sigh of the potential is an important diagnostic factor in the
interpretation of SP anomalies
interpretation of SP anomalies.
•Self‐potentials are generated by a number of natural sources (exact
Self potentials are generated by a number of natural sources (exact
physical processes still unclear).
Occurrence of Self‐potentials
•Natural ground potentials consist of 2 components
1. Background Potentials‐‐‐fluctuate with time caused by different
1. Background Potentials fluctuate with time caused by different
processes ranging from AC currents induced by thunderstorms,
variations in Earth’s magnetic fields, effects of heavy rainfalls
2. Mineral Potentials‐‐‐constant due to electrochemical processes
h l d f ll l
Mechanism of Self‐potentials
•Some physical processes caused sources of SP are still unclear.
•Groundwater is thought to be common factor responsible for SP.
P t ti l t d b th fl f t b t ti
•Potentials are generated by the flow of water, by water reacting as
an electrolyte and as a solvent of different minerals.
•Electrical conductivity to produce potentials of porous rocks depends
on porosity and on mobility of water to pass through the pore spaces
‐‐‐depend on ionic mobilities, solution concentrations, viscosity,
depend on ionic mobilities, solution concentrations, viscosity,
temperature & pressure.
•There are a few types of SP :
•There are a few types of SP :
1.Electrokinetic potential
2 Thermoelectric potential
2. Thermoelectric potential
3. Electrochemical potential
4. Mineral/mineralization potential
/ p
Fl i f fl id ( l t l t ) th h ill
Electrokinetic potential
• Flowing of fluid (electrolyte) through a capillary or porous
medium generates potentials along the flow path.
• The potentials are alternatively called as electrofiltration
• The potentials are alternatively called as electrofiltration,
electromechanical or streaming potentials.
• The effect is believed to be due to electrokinetic coupling
The effect is believed to be due to electrokinetic coupling
between the fluid ions and the walls of the capillary.
• The electrokinetic potential (Ek) generated between the ends of
The electrokinetic potential (Ek) generated between the ends of
the capillary passage is given by
= Dielectric permittivity of pore fluid
= Electrical resistivity of pore fluid
= Electrofiltration coupling coefficient
= Pressure difference
= Dynamic viscosity of pore fluid
E di t i i th di ti th di t i
Electrokinetic potential
• Ek gradient is in the same direction as the pressure gradient, i.e.
opposite to the direction of the electrolyte flow.
• E normally providse amplitudes of some mV to several hundreds
• Ek normally providse amplitudes of some mV to several hundreds
of mV.
• Ek can be found associated with flow of subsurface water and
Ek can be found associated with flow of subsurface water and
thermal fluids
• Ek effects have been observed over zones of water leakage
Ek effects have been observed over zones of water leakage
through fissures in the rock floor of reservoirs, over terrains with
large elevation changes, and in geothermal areas.
P t ti l di t ill k l if
Thermoelectric potential
• Potential gradient will appear across a rock sample if a
temperature gradient is maintained across the rock sample.
• Thermoelectric coupling coefficient (TEC) is defined as the ratio of
• Thermoelectric coupling coefficient (TEC) is defined as the ratio of
the voltage to the temperature difference‐‐‐> TEC=∆V/∆T
• TEC values of rocks vary from ‐0 09 to + 1 36 mV/°C
TEC values of rocks vary from 0.09 to + 1.36 mV/ C
average ~ 0.27 mV/°C
• SP generated from TE potentials are of smaller amplitudes than
• SP generated from TE potentials are of smaller amplitudes than
usually seen in geothermal areas.
• More concentrated areas of high temperature at shallow depth,
More concentrated areas of high temperature at shallow depth,
such as thermal fluids in a fault zone, could give rise to anomalies
of greater amplitude.
• Boundaries of SP anomalies measured in several geothermal
areas appear to correlate with zones of known anomalous high
heat flow‐‐‐‐>portion of anomalies is generated by TE mechanism.
If th t ti f th l t l t i th d i l ll
Electrochemical potential
• If the concentration of the electrolytes in the ground varies locally,
potential differences are set up due to the difference in mobilities of
anions and cations in solutions of different concentrations‐‐‐called
anions and cations in solutions of different concentrations called
liquid‐junction or diffusion potentials.
• For this mechanism to explain the continued occurrence of such
p
potentials, a source capable of maintaining imbalances in the
electrolytic concentration is needed, otherwise the concentrations
differences will disappear with time by diffusion.
• Electrical potential is also generated when 2 identical metal
l t d i d i l ti f diff t t ti
electrodes are immersed in solutions of different concentrations‐‐‐
called Nernst potential.
• Diffusion + Nernst potentials = Electrochemical or static self
• Diffusion + Nernst potentials = Electrochemical, or static, self‐
potential.
O f th t t l l t l t i N Cl
Electrochemical potential
• One of the most common natural electrolytes is NaCl.
• For NaCl solutions of different concentration (C1,C2) but at the same
temperature T (°C) the amplitude of the electrochemical potential
temperature, T ( C), the amplitude of the electrochemical potential
(Ec) is given by
• For example, if C1:C2 = 5:1 ‐‐‐‐‐> Ec ≈ 50 mV
i th t i t t i i l l ti f SP i t d ith
Mineral potential
• is the most important in mineral exploration of SP associated with
massive sulphide ore bodies.
• Large negative ( ) SP anomalies (100 1000mV)can be observed
• Large negative (‐) SP anomalies (100‐1000mV)can be observed
particularly over deposits of pyrite, chalcopyrite, pyrrhotite,
magnetite, and graphite.
g , g p
• The potentials are almost invariably negative over the top of the
deposit and are quite stable in time.
• Sato and Mooney (1960) have provided the most complete
explanation of the electrochemical processes caused the observed
SP anomalies.
• However this hypothesis does not explain all the occurrences of the
SP i di h h l h i l li d
SP indicates that the actual physical processes are more complicated
and no yet truly understood.
Measurement of Self‐potentials
• simple and inexpensive.
• 2 non‐polarizable porous‐pot electrodes connected to a precision
p p p p
voltmeters capable of measuring to at least 1 mV
• Each electrode is made up of a copper electrode dipped in a
saturated solution of copper sulphate which can percolate through
the porous base to the pot.
• An alternate zinc electrode in saturated zinc sulphate solution or
silver in silver chloride can be used.
Maximum depth of sensitivity of SP method = ~60‐100m depending
b d d t f b d
on ore body and nature of overburden.
Porous pot electrodes
2 fi ld t h i 2 l t d fi ti
Measurement of Self‐potentials
2 field techniques or 2 electrode configurations
1.Potential gradient method (dipole/leap frog/gradient configuration)
fi i f 2 l d (5 10 )
‐fix separation of 2 electrodes (5 or 10 m)
‐measure potential difference between 2 electrodes = potential
gradient [mV/V]
gradient [mV/V]
‐2 porous are leap‐frogged along traverse with care of correct polarity
of potential recorded
of potential recorded
‐observation points = midpoint between 2 electrodes
Measurement of Self‐potentials
2.Potential amplitude, or total field method (fixed‐base)
configuration
‐keep one electrode fixed at a base station
‐measure potential difference [mV] between base & 2nd
electrodes moving along traverse
‐lower level of cumulative errors & confusing polarity
‐disadvantages of transporting long wire
Interpretation of Self‐Potential Data
• SP anomalies are often interpreted qualitatively by
– Profile shape
– Amplitude
– Polarity (+ or ‐)
C
– Contour pattern
• Top of ore body is assumed to lie directly beneath position of
minimum potential
minimum potential.
• For quantitative interpretation, it is possible to calculate the
potential distributions around polarized bodies of simple shape,
potential distributions around polarized bodies of simple shape,
such as sphere, ellipsoid, and dipole, by making some
simplifications and assumptions concerning the potential on the
surface of the sources.
SP profiles over buried polarized rod
SP fil b i d l i d h
SP profiles over buried polarized sphere
mV]
SP
[m
SP anomalies generated by buried metal pipelines and well casings at Meso California USA
SP anomalies generated by buried metal pipelines and well casings at Meso, California, USA
An SP profile across pegmatite dikes in gneiss
Self‐potential (SP) Method.pdf
Self‐potential (SP) Method.pdf
Self‐potential (SP) Method.pdf

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Self‐potential (SP) Method.pdf

  • 1. Self‐potential (SP) Method •or spontaneous polarization method is based on the surface measurement of natural potentials resulting from electrochemical reactions in the subsurface. subsurface. •does not require electric currents to be injected into the ground as in the RESISTIVITY & IP methods RESISTIVITY & IP methods. •has been used in base metal exploration, to detect the presence of massive b di i t t t th IP th d hi h i d t d i tl t ore bodies, in contrast to the IP method which is used to predominantly to investigate disseminated ore bodies. •has been increasingly used in groundwater & geothermal investigations, environmental and engineering applications‐‐‐> mapping seepage flow associated with dams, geological mapping, delineate shear zones and near‐ associated with dams, geological mapping, delineate shear zones and near surface faults. •ranks as the cheapest of surface geophysical methods in terms of •ranks as the cheapest of surface geophysical methods in terms of equipment necessary and amongst the simplest to operate in the field.
  • 2. Occurrence of Self‐potentials •SP method is passive, i.e. differences in natural ground potentials are measured between any two points on the ground surface. •The potentials measured can range from < a millivolt (mV) to > 1 Volt. • + or – sigh of the potential is an important diagnostic factor in the interpretation of SP anomalies interpretation of SP anomalies. •Self‐potentials are generated by a number of natural sources (exact Self potentials are generated by a number of natural sources (exact physical processes still unclear).
  • 3. Occurrence of Self‐potentials •Natural ground potentials consist of 2 components 1. Background Potentials‐‐‐fluctuate with time caused by different 1. Background Potentials fluctuate with time caused by different processes ranging from AC currents induced by thunderstorms, variations in Earth’s magnetic fields, effects of heavy rainfalls 2. Mineral Potentials‐‐‐constant due to electrochemical processes
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  • 5. h l d f ll l Mechanism of Self‐potentials •Some physical processes caused sources of SP are still unclear. •Groundwater is thought to be common factor responsible for SP. P t ti l t d b th fl f t b t ti •Potentials are generated by the flow of water, by water reacting as an electrolyte and as a solvent of different minerals. •Electrical conductivity to produce potentials of porous rocks depends on porosity and on mobility of water to pass through the pore spaces ‐‐‐depend on ionic mobilities, solution concentrations, viscosity, depend on ionic mobilities, solution concentrations, viscosity, temperature & pressure. •There are a few types of SP : •There are a few types of SP : 1.Electrokinetic potential 2 Thermoelectric potential 2. Thermoelectric potential 3. Electrochemical potential 4. Mineral/mineralization potential / p
  • 6. Fl i f fl id ( l t l t ) th h ill Electrokinetic potential • Flowing of fluid (electrolyte) through a capillary or porous medium generates potentials along the flow path. • The potentials are alternatively called as electrofiltration • The potentials are alternatively called as electrofiltration, electromechanical or streaming potentials. • The effect is believed to be due to electrokinetic coupling The effect is believed to be due to electrokinetic coupling between the fluid ions and the walls of the capillary. • The electrokinetic potential (Ek) generated between the ends of The electrokinetic potential (Ek) generated between the ends of the capillary passage is given by = Dielectric permittivity of pore fluid = Electrical resistivity of pore fluid = Electrofiltration coupling coefficient = Pressure difference = Dynamic viscosity of pore fluid
  • 7. E di t i i th di ti th di t i Electrokinetic potential • Ek gradient is in the same direction as the pressure gradient, i.e. opposite to the direction of the electrolyte flow. • E normally providse amplitudes of some mV to several hundreds • Ek normally providse amplitudes of some mV to several hundreds of mV. • Ek can be found associated with flow of subsurface water and Ek can be found associated with flow of subsurface water and thermal fluids • Ek effects have been observed over zones of water leakage Ek effects have been observed over zones of water leakage through fissures in the rock floor of reservoirs, over terrains with large elevation changes, and in geothermal areas.
  • 8. P t ti l di t ill k l if Thermoelectric potential • Potential gradient will appear across a rock sample if a temperature gradient is maintained across the rock sample. • Thermoelectric coupling coefficient (TEC) is defined as the ratio of • Thermoelectric coupling coefficient (TEC) is defined as the ratio of the voltage to the temperature difference‐‐‐> TEC=∆V/∆T • TEC values of rocks vary from ‐0 09 to + 1 36 mV/°C TEC values of rocks vary from 0.09 to + 1.36 mV/ C average ~ 0.27 mV/°C • SP generated from TE potentials are of smaller amplitudes than • SP generated from TE potentials are of smaller amplitudes than usually seen in geothermal areas. • More concentrated areas of high temperature at shallow depth, More concentrated areas of high temperature at shallow depth, such as thermal fluids in a fault zone, could give rise to anomalies of greater amplitude. • Boundaries of SP anomalies measured in several geothermal areas appear to correlate with zones of known anomalous high heat flow‐‐‐‐>portion of anomalies is generated by TE mechanism.
  • 9. If th t ti f th l t l t i th d i l ll Electrochemical potential • If the concentration of the electrolytes in the ground varies locally, potential differences are set up due to the difference in mobilities of anions and cations in solutions of different concentrations‐‐‐called anions and cations in solutions of different concentrations called liquid‐junction or diffusion potentials. • For this mechanism to explain the continued occurrence of such p potentials, a source capable of maintaining imbalances in the electrolytic concentration is needed, otherwise the concentrations differences will disappear with time by diffusion. • Electrical potential is also generated when 2 identical metal l t d i d i l ti f diff t t ti electrodes are immersed in solutions of different concentrations‐‐‐ called Nernst potential. • Diffusion + Nernst potentials = Electrochemical or static self • Diffusion + Nernst potentials = Electrochemical, or static, self‐ potential.
  • 10. O f th t t l l t l t i N Cl Electrochemical potential • One of the most common natural electrolytes is NaCl. • For NaCl solutions of different concentration (C1,C2) but at the same temperature T (°C) the amplitude of the electrochemical potential temperature, T ( C), the amplitude of the electrochemical potential (Ec) is given by • For example, if C1:C2 = 5:1 ‐‐‐‐‐> Ec ≈ 50 mV
  • 11. i th t i t t i i l l ti f SP i t d ith Mineral potential • is the most important in mineral exploration of SP associated with massive sulphide ore bodies. • Large negative ( ) SP anomalies (100 1000mV)can be observed • Large negative (‐) SP anomalies (100‐1000mV)can be observed particularly over deposits of pyrite, chalcopyrite, pyrrhotite, magnetite, and graphite. g , g p • The potentials are almost invariably negative over the top of the deposit and are quite stable in time. • Sato and Mooney (1960) have provided the most complete explanation of the electrochemical processes caused the observed SP anomalies. • However this hypothesis does not explain all the occurrences of the SP i di h h l h i l li d SP indicates that the actual physical processes are more complicated and no yet truly understood.
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  • 13. Measurement of Self‐potentials • simple and inexpensive. • 2 non‐polarizable porous‐pot electrodes connected to a precision p p p p voltmeters capable of measuring to at least 1 mV • Each electrode is made up of a copper electrode dipped in a saturated solution of copper sulphate which can percolate through the porous base to the pot. • An alternate zinc electrode in saturated zinc sulphate solution or silver in silver chloride can be used. Maximum depth of sensitivity of SP method = ~60‐100m depending b d d t f b d on ore body and nature of overburden.
  • 15. 2 fi ld t h i 2 l t d fi ti Measurement of Self‐potentials 2 field techniques or 2 electrode configurations 1.Potential gradient method (dipole/leap frog/gradient configuration) fi i f 2 l d (5 10 ) ‐fix separation of 2 electrodes (5 or 10 m) ‐measure potential difference between 2 electrodes = potential gradient [mV/V] gradient [mV/V] ‐2 porous are leap‐frogged along traverse with care of correct polarity of potential recorded of potential recorded ‐observation points = midpoint between 2 electrodes
  • 16. Measurement of Self‐potentials 2.Potential amplitude, or total field method (fixed‐base) configuration ‐keep one electrode fixed at a base station ‐measure potential difference [mV] between base & 2nd electrodes moving along traverse ‐lower level of cumulative errors & confusing polarity ‐disadvantages of transporting long wire
  • 17. Interpretation of Self‐Potential Data • SP anomalies are often interpreted qualitatively by – Profile shape – Amplitude – Polarity (+ or ‐) C – Contour pattern • Top of ore body is assumed to lie directly beneath position of minimum potential minimum potential. • For quantitative interpretation, it is possible to calculate the potential distributions around polarized bodies of simple shape, potential distributions around polarized bodies of simple shape, such as sphere, ellipsoid, and dipole, by making some simplifications and assumptions concerning the potential on the surface of the sources.
  • 18. SP profiles over buried polarized rod
  • 19. SP fil b i d l i d h SP profiles over buried polarized sphere
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  • 25. mV] SP [m SP anomalies generated by buried metal pipelines and well casings at Meso California USA SP anomalies generated by buried metal pipelines and well casings at Meso, California, USA
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  • 27. An SP profile across pegmatite dikes in gneiss