000 | 02044cam a2200373 a 4500 | ||
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003 | EG-NbEJU | ||
005 | 20240717094448.0 | ||
008 | 240717s1992 us a grb 001 0 eng d | ||
010 | _a2006018348 | ||
020 | _a0931830567 (Series) | ||
020 | _a1560800585 (Volume) | ||
035 | _a(OCoLC)ocm69792173 | ||
035 | _a(OCoLC)69792173 | ||
040 |
_aEG-NbEJU _cEG-NbEJU _dEG-NbEJU _beng |
||
041 | _aeng | ||
050 | 0 | 0 |
_aQC809 _b.E15W48 1992 |
100 | 1 |
_aWhittall , Kenneth Patrick , _d1955- |
|
245 | 1 | 0 |
_aInversion of Magnetotelluric data for a One-dimensional Conductivity / _cby : Kenneth P. Whittall and Douglas W. Oldenburg |
260 |
_aOklahoma , United Stste of America : _bThe Society of Exploration Geophysics , _c1992 |
||
300 |
_av , 114 pages : _billustrations ; _c24 cm. |
||
490 | 0 |
_aGeophysical monograph series ; _vno. 5 |
|
500 | _aNumber 5 : Inversion of Magnetotelluric Data for a One-Dimensional Conductivity by : Kenneth P. Whittall and Douglas W. Oldenburg | ||
504 | _aIncludes bibliographical references and index | ||
520 | _aThe magnetotelluric (MT) method, pioneered by Tikhonov (1950) and Cagniard (1953), has been applied with varying degrees of success to yield information about the Earth's electrical conductivity, temperature regimes, and geologic structure. The strengths and weaknesses of the MT method are now generally appreciated and the majority of research over the past few years has concentrated on data processing, forward modeling and inversion. Historically, MT interpretation has used one-dimensional (1-D) forward modeling algorithms, 1-D inversions, and 2-D forward modeling | ||
650 | 7 |
_aEarth Resistance _2LCSH _xMeasurement |
|
650 | 7 |
_aInverse Problems (Different Equations) _2LCSH |
|
650 | 7 |
_aContinuum mechanics _vTextbooks _2LCSH |
|
700 | 1 |
_aOldenburg , Douglas W. , _d1946- _eco-author |
|
700 | 1 |
_aFitterman , David V. , _eEditor of series |
|
830 | 0 |
_aGeophysical monograph series ; _vno. 5 |
|
901 | _asara sorur | ||
902 | _aENG_03_ (2358) | ||
942 |
_2lcc _cBK |
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999 |
_c3941 _d3941 |