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MAGNETOTELLURIC (MT) METHOD
[object Object],[object Object],[object Object],[object Object],Magnetotellurics (MT ), background
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Magnetotellurics (MT ), background
electromagnetic induction
natural electromagnetic field
   B ( t ) _______    t E ( t ) electric - magnetic phenomena represented by the Maxwell’s equations
H ( t ) electric - magnetic phenomena represented by the Maxwell’s equations    D ( t ) _______    t J ( t )  +
[object Object],[object Object],[object Object],[object Object],[object Object],MT response calculation, concept
EM induction ~  wave diffusion   spectral content, not  propagation parameters incident waves transmitted waves surface reflected waves
[object Object],[object Object],[object Object],[object Object],   surface  1 h 1 z 1 =   0 . . . z  2 z 3 z N - 1 z N  2 h 2  N - 1 h N - 1  N  (Ohm.m) z (m)
  __________ E x   =  A  exp (- k   z ) k  =  √   i      0   /  H y   =   ( A  exp (- k   z )) z  =  depth k ________ i       ,[object Object],[object Object],solution to Maxwell’s equations in simple medium E x   =  A  exp (- k   z )   +  B  exp ( + k   z ) H y   =   ( A  exp (- k   z )  - B  exp ( + k   z )) k ________ i      
[object Object],[object Object],[object Object],[object Object],Skin Effect and Penetration Depth E x   =  A  exp (- k   z )     E x   ( z   =   0)   =  A      E x   ( z   =    )   =  A   /   e   _________    =  √  2      /   (     0 )     = 2    f   f  =  frequency
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Skin Effect and Penetration Depth
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Skin Effect and Penetration Depth
Skin Effect and Penetration Depth
MT  field set-up
MT  field set-up
MT Time series data
Data processing  sequence
E x  =   Z xx   H x   +   Z xy   H y  E y  =   Z yx   H x   +   Z yy   H y     E  =   Z  H    sounding curves Data Processing (Frequency Domain)  a   =   0.2  T  |   Z   |   2    =   atan  Im  Z _______ Re  Z
Modeling and Interpretation
[object Object],[object Object],[object Object],[object Object],1-D MT modeling 1   –   R j  exp ( –   2 k j   h j )   _____________________     1   +  R j  exp ( –   2 k j   h j )   Z j   =  Z I,j   R j   = Z I,j   –  Z j + 1 __________ Z I,j   +  Z j + 1
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],1-D MT modeling, algorithm  surface  1 h 1 z 1 =   0  z  2  2 h 2 . . .  z N - 1  N - 1 h N - 1 z N  N
 
2-D resistivity section from 1-D models on  a profile    correlation of    resistivity units from    station to station    correlation of    resistivity units with    geology and    lithology
pseudosection (data) 2-D smooth model hot-spring hot-spring

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