Magnetic Anomaly Method for Analysis of Depth, Location, and Shape Geometry Resources
Two FORTRAN programs convolution one dimention and enhanced local wave number are used <br /> <br /> to obtain information on depth, location and geometry of the source of total field magnetic anomaly data <br /> <br /> in this last assignment. In this data processing of phys...
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id-itb.:243572017-01-25T15:52:06ZMagnetic Anomaly Method for Analysis of Depth, Location, and Shape Geometry Resources ADITYA (NIM : 124 05 013), SRI Indonesia Final Project INSTITUT TEKNOLOGI BANDUNG https://digilib.itb.ac.id/gdl/view/24357 Two FORTRAN programs convolution one dimention and enhanced local wave number are used <br /> <br /> to obtain information on depth, location and geometry of the source of total field magnetic anomaly data <br /> <br /> in this last assignment. In this data processing of physical characteristics of the source of anomalous <br /> <br /> dimension and contrast susceptibility were not taken into account. The source geometry is estimated by <br /> <br /> structural index of the depth and position. Once one gets the value of the depth, location, geometry of the <br /> <br /> source then those compared with the results of the depth, location, and geometry of the source obtained <br /> <br /> the second data processing by the programs on total field magnetic anomaly data wa added with noise. By <br /> <br /> this method, we can get information about the differences in the result of the depth, location, and <br /> <br /> geometry of the source of the noise given total field magnetic anomaly data with total field anomaly data <br /> <br /> without noise that were processed with both FORTRAN programs. text |
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Two FORTRAN programs convolution one dimention and enhanced local wave number are used <br />
<br />
to obtain information on depth, location and geometry of the source of total field magnetic anomaly data <br />
<br />
in this last assignment. In this data processing of physical characteristics of the source of anomalous <br />
<br />
dimension and contrast susceptibility were not taken into account. The source geometry is estimated by <br />
<br />
structural index of the depth and position. Once one gets the value of the depth, location, geometry of the <br />
<br />
source then those compared with the results of the depth, location, and geometry of the source obtained <br />
<br />
the second data processing by the programs on total field magnetic anomaly data wa added with noise. By <br />
<br />
this method, we can get information about the differences in the result of the depth, location, and <br />
<br />
geometry of the source of the noise given total field magnetic anomaly data with total field anomaly data <br />
<br />
without noise that were processed with both FORTRAN programs. |
format |
Final Project |
author |
ADITYA (NIM : 124 05 013), SRI |
spellingShingle |
ADITYA (NIM : 124 05 013), SRI Magnetic Anomaly Method for Analysis of Depth, Location, and Shape Geometry Resources |
author_facet |
ADITYA (NIM : 124 05 013), SRI |
author_sort |
ADITYA (NIM : 124 05 013), SRI |
title |
Magnetic Anomaly Method for Analysis of Depth, Location, and Shape Geometry Resources |
title_short |
Magnetic Anomaly Method for Analysis of Depth, Location, and Shape Geometry Resources |
title_full |
Magnetic Anomaly Method for Analysis of Depth, Location, and Shape Geometry Resources |
title_fullStr |
Magnetic Anomaly Method for Analysis of Depth, Location, and Shape Geometry Resources |
title_full_unstemmed |
Magnetic Anomaly Method for Analysis of Depth, Location, and Shape Geometry Resources |
title_sort |
magnetic anomaly method for analysis of depth, location, and shape geometry resources |
url |
https://digilib.itb.ac.id/gdl/view/24357 |
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1821844646800654336 |