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GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

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GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007. Multielectrode Resistivity survey. ( MUEL1 ). MOHAMED AL RAJHI, MARTIN VEASEY, EVA PUDLEINER, PETER TAKA’CS. Satellite image of the Carpathian Basin. By NOAA17. Introduction:. - PowerPoint PPT Presentation
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GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007 MOHAMED AL RAJHI, MARTIN VEASEY, EVA PUDLEINER, PETER TAKA’CS
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Page 1: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

GEOPHYSICAL FIELD SCHOOLLake Balaton, Hungary

August 31 to September 14, 2007

MOHAMED AL RAJHI, MARTIN VEASEY, EVA PUDLEINER, PETER TAKA’CS

Page 2: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

By NOAA17

Page 3: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

Our survey was part of a geophysical project in the Pannonian-basin .

Different methods were used to better our understanding of the evolutional chapters of Lake Balaton.

The large scale structure is the extensional basin (due to subduction of African Plate), which suffered later from compression.

Enying Ridge

Lake Balaton

N

15km

Page 4: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

•The Enying ridge (South from Lake Balaton’s Eastern shore ) is a significant geological structure in the region but the reason

for its existence is unclear.

•The resistivity survey attempts to address this problem and give some possible interpretations.

Page 5: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007
Page 6: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007
Page 7: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

K is a geometric factor that depends on the arrangement of the four electrodes

*Current (I) is directed into the ground via two outer electrodes (C1 & C2).

*The potential difference (∆Φ) is measured at various points (P1 & P2)

between the current electrodes .

*Apparent resistivity (ρa) is given by:

ρa= k (∆Φ/ I)

Page 8: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

*Porosity

*Degree of water saturation in the rock

*Pore space connection

*Dry or wet conditions

Page 9: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

ARES-G4

*ARES-G4 control box measures current, voltage & apparent resistivity.

*5 cables are used in the array .

*Cable length is 32m .

*Electrode Spacing is 4m .

*Spread length is 156m.

*Maximum Depth ≈ 30m.

Electrode-Cable Connection

Page 10: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

M.H.Loke, 2004

*The Schlumberger array works by keeping the potential electrodes at constant seperation while the current electrodes are expanded.

*The Wenner array works by keeping constant spacing between

all the electrodes .

* Wenner-Schlumberger is a combination of the two.

Page 11: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

*Topography from GPS is converted to EOV.

*Data from ARES-G4 and the topography is read into RES2DINV software.

*An inversion process takes place using forward modeling to obtain a model that best fits the measured pseudo section.

Page 12: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

Inversion:

Page 13: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007
Page 14: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007
Page 15: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007
Page 16: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

90100110120130140

Ele

va

tio

n (

mB

f)

50 100 150 200 250 300 350 400 450 500 550 600 650

50 100 150 200 250 300 350 400 450 500 550 600 650

90100110120130140

Ele

va

tion

(mB

f)

0 1 0 2 0 3 0 4 0 5 0 6 0 7 0 8 0 9 0 1 0 0

Page 17: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007
Page 18: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

1 01 52 02 53 03 54 04 55 05 56 06 57 07 58 08 59 09 51 0 01 0 51 1 01 1 51 2 01 2 51 3 01 3 51 4 01 4 51 5 0

587000

586000

174000Dip ≈1.3°

Dip ≈4.5°

Ωm

Page 19: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

120

140

160

Elev

atio

n (m

Bf)

0 200 400 600

0 200 400 600

120

140

160

Elevation (mBf)

0 100res [o h m m ]

200

150

100

50

0

d a y 9 /3

120130140150160

Elev

atio

n (m

Bf)

0 200 400

0 200 400

120130140150160

Elevation (mBf)

0 100res [o h m m ]

300

200

100

0

d ay 5 /12 5 0 m so u th o f th is p o in t

enying5enying4

Page 20: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

1 01 52 02 53 03 54 04 55 05 56 06 57 07 58 08 59 09 51 0 01 0 51 1 01 1 51 2 01 2 51 3 01 3 51 4 01 4 51 5 0

Page 21: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

80

90

100

110

120

Ele

vatio

n (m

Bf)

0 50 100 150 200 250 300 350 400

0 50 100 150 200 250 300 350 400

80

90

100

110

120

Elevation (m

Bf)

1 01 52 02 53 03 54 04 55 05 56 06 57 07 58 08 59 09 51 0 01 0 51 1 01 1 51 2 01 2 51 3 01 3 51 4 01 4 51 5 0

NOT CONTINUOUS?

585000584000

173000

Page 22: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

• Old Pannonian Lake that previously covered the area may have deposited multiple limestone layers and clay/shale in between.

•Shallow marine environment would respond quickly to any climatic changes.

•Deformation causes tilting of layers.

•Differential erosion. (More resistive limestone layers erode more slowly than clay/shale)

Page 23: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

>THE INVERSION ESSENTIALLY CREATES A BEST FIT MODEL.

INTERPRETATIONS ARE AMBIGUOUS. (OTHER MEASUREMENTS NEEDED)

NEAR SURFACE RESISTIVITY VARIATIONS CAN MASK THE EFFECTS OF DEEPER VARIATIONS.

THE GPS MEASUREMENTS ARE APPROXIMATELY +/- 5m IN THE (X,Y) PLANE. THE ERROR IN THE (Z) DIRECTION

(ELEVATION) IS ABOUT +/- 10m.

Page 24: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

Water level fluctuation -> small lakes, limestone caps on hills at about 120-130m hight above sea level.

The high resistive layer (Enying1 Western end) could be dipping towards the South.

Interpretation without a 3-D Model is very ambiguous.

Page 25: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

Fülöp József: Magyarország geológiája – Paleozoikum I.

Gyalog László, Horváth István: A Velencei-hegység és a Balatonfő földtana; Budapest 2004

Lóczy Lajos Geological Map.

M.H.Loke, (1996-2004), (Revision date : 26th July 2004)

Philip Kearey, Michael Brooks, Ian Hill: An introduction to geophysical exploration; Blackwell Publishing Company 2002

Page 26: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

Thanks to

Zoltán Hámori for leading the survey

All other groups for sharing their data and results

ELTE Space Research Group for the maps

All the staff of University of Leeds and Eötvös Loránd University

Page 27: GEOPHYSICAL FIELD SCHOOL Lake Balaton, Hungary August 31 to September 14, 2007

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