From dae71376df94aca3db30b32870161d18e4966916 Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Wed, 7 Sep 2022 09:47:49 +0800 Subject: [PATCH 01/17] Update conf.py --- docs/conf.py | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/docs/conf.py b/docs/conf.py index df3376c..7aa9848 100644 --- a/docs/conf.py +++ b/docs/conf.py @@ -14,7 +14,7 @@ # import os import sys -import guzzle_sphinx_theme #, sphinx_rtd_theme +# import guzzle_sphinx_theme , sphinx_rtd_theme sys.path.insert(0, os.path.abspath('.')) sys.path.insert(0, os.path.abspath('..')) From e886dcb408decdfd062c3455559ed44f4fa88d67 Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Wed, 7 Sep 2022 09:48:25 +0800 Subject: [PATCH 02/17] Update conf.py --- docs/conf.py | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/docs/conf.py b/docs/conf.py index 7aa9848..018f014 100644 --- a/docs/conf.py +++ b/docs/conf.py @@ -27,9 +27,9 @@ author = u'Kouadio K. Laurent' # The short X.Y version -version = u'1.2' +version = u'1.1' # The full version, including alpha/beta/rc tags -release = u'v1.2.0' +release = u'v1.1.7' # -- General configuration --------------------------------------------------- From 301cf37bf7bc9abab299b0b88b088fad1ee4ae5f Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Wed, 7 Sep 2022 09:51:06 +0800 Subject: [PATCH 03/17] Update conf.py --- docs/source/conf.py | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/docs/source/conf.py b/docs/source/conf.py index 6a41fc0..0edabea 100644 --- a/docs/source/conf.py +++ b/docs/source/conf.py @@ -14,7 +14,7 @@ # import os import sys -import guzzle_sphinx_theme #, sphinx_rtd_theme +# import guzzle_sphinx_theme #, sphinx_rtd_theme sys.path.insert(0, os.path.abspath('.')) sys.path.insert(0, os.path.abspath('..')) From b9db79d2648e5b9eeab1e5fa56c490a9247dcb4d Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Wed, 7 Sep 2022 09:52:01 +0800 Subject: [PATCH 04/17] Delete conf.py --- docs/conf.py | 215 --------------------------------------------------- 1 file changed, 215 deletions(-) delete mode 100644 docs/conf.py diff --git a/docs/conf.py b/docs/conf.py deleted file mode 100644 index 018f014..0000000 --- a/docs/conf.py +++ /dev/null @@ -1,215 +0,0 @@ -# -*- coding: utf-8 -*- -# -# Configuration file for the Sphinx documentation builder. -# -# This file does only contain a selection of the most common options. For a -# full list see the documentation: -# http://www.sphinx-doc.org/en/master/config - -# -- Path setup -------------------------------------------------------------- - -# If extensions (or modules to document with autodoc) are in another directory, -# add these directories to sys.path here. If the directory is relative to the -# documentation root, use os.path.abspath to make it absolute, like shown here. -# -import os -import sys -# import guzzle_sphinx_theme , sphinx_rtd_theme - -sys.path.insert(0, os.path.abspath('.')) -sys.path.insert(0, os.path.abspath('..')) -sys.path.insert(0, os.path.abspath('../..')) - -# -- Project information ----------------------------------------------------- - -project = u'pycsamt' -copyright = u'2021, Kouadio K. Laurent' -author = u'Kouadio K. Laurent' - -# The short X.Y version -version = u'1.1' -# The full version, including alpha/beta/rc tags -release = u'v1.1.7' - - -# -- General configuration --------------------------------------------------- - -# If your documentation needs a minimal Sphinx version, state it here. -# -# needs_sphinx = '1.0' - -# Add any Sphinx extension module names here, as strings. They can be -# extensions coming with Sphinx (named 'sphinx.ext.*') or your custom -# ones. -extensions = [ - 'sphinx.ext.autodoc', - 'sphinx.ext.doctest', - 'sphinx.ext.viewcode', - 'sphinx.ext.coverage', - 'sphinx.ext.imgmath', - #'numpydoc', - 'sphinx.ext.napoleon', - 'sphinx.ext.autosummary', - #"sphinx_rtd_theme", - #"guzzle_sphinx_theme", - 'sphinx.ext.githubpages', -] - -#Configuring Napoleon -napoleon_google_docstring = True -napoleon_numpy_docstring = True -# Add any paths that contain templates here, relative to this directory. -templates_path = ['_templates'] - -# The suffix(es) of source filenames. -# You can specify multiple suffix as a list of string: -# -# source_suffix = ['.rst', '.md'] -source_suffix = '.rst' - -# The master toctree document. -master_doc = 'index' - -# The language for content autogenerated by Sphinx. Refer to documentation -# for a list of supported languages. -# -# This is also used if you do content translation via gettext catalogs. -# Usually you set "language" from the command line for these cases. -language = 'en' - -# List of patterns, relative to source directory, that match files and -# directories to ignore when looking for source files. -# This pattern also affects html_static_path and html_extra_path. -exclude_patterns = [u'_build', 'Thumbs.db', '.DS_Store'] - -# The name of the Pygments (syntax highlighting) style to use. -pygments_style = 'sphinx' - - -# -- Options for HTML output ------------------------------------------------- - -# The theme to use for HTML and HTML Help pages. See the documentation for -# a list of builtin themes. -# -#html_theme = 'classic' -html_theme ='bizstyle'#'guzzle_sphinx_theme' #'sphinx_rtd_theme', #bizstyle - -# Theme options are theme-specific and customize the look and feel of a theme -# further. For a list of options available for each theme, see the -# documentation. -# -# html_theme_options = {} - -# Add any paths that contain custom static files (such as style sheets) here, -# relative to this directory. They are copied after the builtin static files, -# so a file named "default.css" will overwrite the builtin "default.css". -html_static_path = ['_static'] - -# Custom sidebar templates, must be a dictionary that maps document names -# to template names. -# -# The default sidebars (for documents that don't match any pattern) are -# defined by theme itself. Builtin themes are using these templates by -# default: ``['localtoc.html', 'relations.html', 'sourcelink.html', -# 'searchbox.html']``. -# -# html_sidebars = {} - - -# -- Options for HTMLHelp output --------------------------------------------- - -# Output file base name for HTML help builder. -htmlhelp_basename = 'pycsamtdoc' - - -# -- Options for LaTeX output ------------------------------------------------ - -latex_elements = { - # The paper size ('letterpaper' or 'a4paper'). - # - # 'papersize': 'letterpaper', - - # The font size ('10pt', '11pt' or '12pt'). - # - # 'pointsize': '10pt', - - # Additional stuff for the LaTeX preamble. - # - # 'preamble': '', - - # Latex figure (float) alignment - # - # 'figure_align': 'htbp', -} - -# Grouping the document tree into LaTeX files. List of tuples -# (source start file, target name, title, -# author, documentclass [howto, manual, or own class]). -latex_documents = [ - (master_doc, 'pycsamt.tex', u'pycsamt Documentation', - u'Kouadio K. Laurent', 'manual'), -] - - -# -- Options for manual page output ------------------------------------------ - -# One entry per manual page. List of tuples -# (source start file, name, description, authors, manual section). -man_pages = [ - (master_doc, 'pycsamt', u'pycsamt Documentation', - [author], 1) -] - - -# -- Options for Texinfo output ---------------------------------------------- - -# Grouping the document tree into Texinfo files. List of tuples -# (source start file, target name, title, author, -# dir menu entry, description, category) -texinfo_documents = [ - (master_doc, 'pycsamt', u'pycsamt Documentation', - author, 'pycsamt', 'A package for audio-frequency magnetotellurics', - 'Miscellaneous'), -] - - -# -- Options for Epub output ------------------------------------------------- - -# Bibliographic Dublin Core info. -epub_title = project -epub_author = author -epub_publisher = author -epub_copyright = copyright - -# The unique identifier of the text. This can be a ISBN number -# or the project homepage. -# -# epub_identifier = '' - -# A unique identification for the text. -# -# epub_uid = '' - -# A list of files that should not be packed into the epub file. -epub_exclude_files = ['search.html'] - -#--- Intersphinx ---------------------- -intersphinx_mapping = { - 'python': ('https://docs.python.org/', None), - 'numpy': ('http://docs.scipy.org/doc/numpy/', None), - 'mtpy': ('https://mtpy2.readthedocs.io/en/develop/', None) -} - -# -- Extension configuration ------------------------------------------------- -MOCK_MODULES = [ - 'osgeo', - 'osgeo.ogr', - 'osgeo.gdal', - 'osgeo.osr', - 'strata',#'mtpy', -] - -import mock - -for mod_name in MOCK_MODULES: - sys.modules[mod_name] = mock.Mock() From 91de105e348b4b6365eb49acd11890108e39f6e6 Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Wed, 7 Sep 2022 16:07:01 +0800 Subject: [PATCH 05/17] Update requirements.txt --- requirements.txt | 1 - 1 file changed, 1 deletion(-) diff --git a/requirements.txt b/requirements.txt index 3d97ee3..d6dad9a 100644 --- a/requirements.txt +++ b/requirements.txt @@ -16,4 +16,3 @@ tqdm mtpy geopandas joblib -gdal From df742e7ca5352eb5b582612b95914d59f0870546 Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Thu, 8 Sep 2022 08:09:11 +0800 Subject: [PATCH 06/17] Update paper.bib --- paper.bib | 8 ++++++-- 1 file changed, 6 insertions(+), 2 deletions(-) diff --git a/paper.bib b/paper.bib index e4004a8..f54824f 100644 --- a/paper.bib +++ b/paper.bib @@ -30,7 +30,7 @@ @article{Berdichevskyetal1998 pages={585–606} } @article{Carlsonetal2005, - title={Applications of controlled source and natural source audio-frequency magnetotellurics to groundwater exploration}, + title={{Applications of controlled source and natural source audio-frequency magnetotellurics to groundwater exploration}}, volume={1}, ISBN={9781622760664}, ISSN={15548015}, @@ -44,6 +44,7 @@ @article{deGrootetal1990 journal={Geophysics}, author={DeGroot-Hedlin,C and Constable,S.}, year={1990}, + DOI={10.1190/1.1442813}, pages={1613–1624} } @article{Goldaketal2015, @@ -143,6 +144,7 @@ @article{Labsonetal1985 volume={50}, number={4}, journal={Geophysics}, author={Labson, V . F and Beckert, A and Morrisson, H.F and Conti, U}, + DOI={10.1190/1.1441940}, year={1985}, pages={656–664} } @misc{Mykle1996, @@ -225,13 +227,15 @@ @article{Wessel1998 volume={79}, journal={Eos Trans. Am. Geophys. Union}, author={Wessel,D.E. and Smith,W.H}, + DOI={10.1029/98eo00426}, year={1998}, pages={579} } - @article{Weaver2000, + @article{Weaveretal2000, title={Characterization of the magnetotelluric tensor in terms of its invariants}, author={John T. Weaver and Aman K Agarwal and Frederick E. M. Lilley}, journal={Geophysical Journal International}, + DOI={10.1046/j.1365-246x.2000.00089.x}, year={2000}, volume={141}, pages={321-336} From 31c345101723c82c7d47375a4dd46e101a592d7b Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Thu, 8 Sep 2022 08:10:51 +0800 Subject: [PATCH 07/17] Update paper.md --- paper.md | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/paper.md b/paper.md index 77c883d..6a03759 100644 --- a/paper.md +++ b/paper.md @@ -1,5 +1,5 @@ --- -title: "pycsamt: A package for robust AMT data processing" +title: "New, improved version of pycsamt package for robust AMT data processing" tags: - Python - pycsamt @@ -78,7 +78,7 @@ at the missing frequency signals. Note that the recovery tensor is used to (re)c ![A missing data recovery at the missing and attenuation signal at two randomly selected stations E12 and E27](examples/paper_figures/recovered_tensors.PNG){width="5.260416666666667in" } Furthermore, the skew analysis can also be performed at the 50 stations to show the dimensionality -(1D, 2D or 3D) of the structures [e.g. Figure 3] [@Bahr1991; @Swift1969; @Weaver2000]. The script ("_~.ctools.restoreZ_") for recovering lost data is located in the *processing* sub-packages. It accepts as input a list of raw standard Electrical Data Interchange (EDI) files [@Wightetal1988], a collection of +(1D, 2D or 3D) of the structures [e.g. Figure 3] [@Bahr1991; @Swift1969; @Weaveretal2000]. The script ("_~.ctools.restoreZ_") for recovering lost data is located in the *processing* sub-packages. It accepts as input a list of raw standard Electrical Data Interchange (EDI) files [@Wightetal1988], a collection of EDI-object from *.edi* module or MTpy Edi-objects [@Kirkbyetal2019]. It returns a Z object composed of a 2×2 matrix known as the complex impedance tensor which can be exported to EDI-file for other purpose. ![An example of dimensionality analysis. Skew value greater than 5 degrees shows 3D dimensional structures and 2D or 1D otherwise](examples/paper_figures/fig.skew.PNG){width="5.260416666666667in" } From a087dd4f9b90226709d2fe44b44e940a1489bc85 Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Thu, 8 Sep 2022 08:17:10 +0800 Subject: [PATCH 08/17] Update paper.bib --- paper.bib | 8 -------- 1 file changed, 8 deletions(-) diff --git a/paper.bib b/paper.bib index f54824f..5594446 100644 --- a/paper.bib +++ b/paper.bib @@ -29,14 +29,6 @@ @article{Berdichevskyetal1998 year={1998}, pages={585–606} } - @article{Carlsonetal2005, - title={{Applications of controlled source and natural source audio-frequency magnetotellurics to groundwater exploration}}, - volume={1}, - ISBN={9781622760664}, - ISSN={15548015}, - DOI={10.4133/1.2923511}, - year={2005}, pages={440–450} - } @article{deGrootetal1990, title={{Occam’s inversion to generate smooth, two-dimensional models from magnetotelluric data}}, volume={55}, From 67b747869b2801e39712463a52104ef51067c4af Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Thu, 8 Sep 2022 08:17:48 +0800 Subject: [PATCH 09/17] Update paper.md --- paper.md | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/paper.md b/paper.md index 6a03759..b99e806 100644 --- a/paper.md +++ b/paper.md @@ -31,7 +31,7 @@ geology and can provide significant details.(ii) second, it includes a backpack for use in difficult terrain. (iii) Third, the technique requires no high-voltage electrodes, and logistics are relatively easy to support in the field. Stations can be acquired almost anywhere and can be placed any distance apart. This allows for large-scale regional reconnaissance exploration or detailed surveys of local -geology and has no environmental impact [@Carlsonetal2005; @Zonge2000]. Unfortunately, this advantage also +geology and has no environmental impact [@Zonge2000]. Unfortunately, this advantage also requires careful processing because the natural signals are not under our control and suffer from frequency ranges with little or no signal. This is one of the main problems in collecting NSAMT data is the signal level in the "attenuation band" also known as the "dead-band" [@Wangetal2017; @Zongeetal1991]. In this @@ -55,7 +55,7 @@ an inner handler to calibrate and to scale the raw data from different hardware . It also recomputes the deviation errors before processing [@Mykle1996]. Its recent development is composed of six main sub-packages as displayed in [Figure 1]. -![Brief illustration of the main sub-packages: core (key functions and methods), modeling (deals with the inversion softwares such Occam2D of @deGrootetal1990, ModEM of @Kelbertetal2014), utils, processing and geodrill (for geology and drilling)](examples/paper_figures/fig.packages.png){width="5.260416666666667in" } +![Brieve illustration of the main sub-packages: core (key functions and methods), modeling (deals with the inversion softwares such Occam2D of @deGrootetal1990, ModEM of @Kelbertetal2014), utils, processing and geodrill (for geology and drilling)](examples/paper_figures/fig.packages.png){width="5.260416666666667in" } Commonly the amplitude of natural electromagnetic fields shows a minimum in the frequency range of 1–2 kHz and decays with increasing frequency. The fields from discharges and thunderstorms propagate in the earth’s From ee7cd62be5d29708eb4d694b31a3f11563c35872 Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Thu, 8 Sep 2022 08:19:18 +0800 Subject: [PATCH 10/17] Update paper.md --- paper.md | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/paper.md b/paper.md index b99e806..126edeb 100644 --- a/paper.md +++ b/paper.md @@ -37,7 +37,7 @@ ranges with little or no signal. This is one of the main problems in collecting in the "attenuation band" also known as the "dead-band" [@Wangetal2017; @Zongeetal1991]. In this work, I exhibited the result of a simple and fast code application as a new feature in the _pycsamt_ package to recover the frequencies lost in the attenuation band. In practice, the recovery technique is not new since -it has been applied with Zonge International engineering [@Zheng2010]. However, in addition to recovering +it has been applied with Zonge International company [@Zheng2010]. 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zGeMxD#y1d70~*QsPvdY%OZAq$D(M4C`ErEqjCcS|37kVpFXmGWN{w=w!w&oHaxG#uIcnke2sw@AANe+SQhwZDQ!xi3vMxS>s}XaEEfXC@mX{)+VrZHaF%()JZ`h|e^VMSl`LWEqySrfb+ld4+zNHTyQybwi zS>HpE40C`5HXuS*)2x9IpDzo9dy=;VY?PkD5gx>6!5yIA=|-=FY`qaQww5LVk}&@& zDG3JPJK%P!WMGpZf$(u#J;FeKugwoe;CajS Date: Mon, 12 Dec 2022 00:29:56 +0800 Subject: [PATCH 12/17] Update README.md --- README.md | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/README.md b/README.md index f08e236..18c9248 100644 --- a/README.md +++ b/README.md @@ -1,6 +1,6 @@ # _pycsamt_: A package for audio-frequency magnetotellurics -[![Documentation Status](https://readthedocs.org/projects/pycsamt/badge/?version=latest)](https://pycsamt.readthedocs.io/en/latest/?badge=latest) [![Build Status](https://travis-ci.com/WEgeophysics/pyCSAMT.svg?branch=master)](https://travis-ci.com/WEgeophysics/pyCSAMT) [![Requirements Status](https://requires.io/github/WEgeophysics/pycsamt/requirements.svg?branch=master)](https://requires.io/github/WEgeophysics/pycsamt/requirements/?branch=master) +[![Documentation Status](https://readthedocs.org/projects/pycsamt/badge/?version=latest)](https://pycsamt.readthedocs.io/en/latest/?badge=latest) [![Build Status](https://travis-ci.com/WEgeophysics/pyCSAMT.svg?branch=master)](https://travis-ci.com/WEgeophysics/pyCSAMT) ![GitHub](https://img.shields.io/github/license/WEgeophysics/pycsamt?color=blue&label=licence&logo=GNU&logoColor=red) ![GitHub release (latest by date)](https://img.shields.io/github/v/release/WEgeophysics/pyCSAMT?color=orange) [![DOI](https://zenodo.org/badge/DOI/10.5281/zenodo.5674430.svg)](https://doi.org/10.5281/zenodo.5674430) [![PyPI version](https://badge.fury.io/py/pycsamt.svg)](https://badge.fury.io/py/pycsamt) ![GitHub repo size](https://img.shields.io/github/repo-size/WEgeophysics/pycsamt?color=0A4CEE&style=flat-square) From e1b1787145f480f6b3c9d879af4f185a1fd9c291 Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Mon, 12 Dec 2022 00:35:42 +0800 Subject: [PATCH 13/17] Update README.md --- README.md | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/README.md b/README.md index 18c9248..719e962 100644 --- a/README.md +++ b/README.md @@ -61,4 +61,4 @@ We use or link some third-party software (beside the usual tool stack: [Numba](h 1. Department of Geophysics, School of Info-physics and Geomatics Engineering, [Central South University](https://en.csu.edu.cn/), China. 2. Equipe de Recherche Géophysique Appliquée, Laboratoire de Geologie Ressources Minerales et Energetiques, UFR des Sciences de la Terre et des Ressources Minières, [Université Félix Houphouët-Boigny]( https://www.univ-fhb.edu.ci/index.php/ufr-strm/), Cote d'Ivoire. -* Developer: 1, 2- Kouadio Laurent, / . +* Developer: 1, 2- Kouadio Laurent, / . From 8d447b8c0a21da81debc112f7db50f5ca403235b Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Tue, 10 Jan 2023 23:47:53 +0800 Subject: [PATCH 14/17] Delete paper.md --- paper.md | 96 -------------------------------------------------------- 1 file changed, 96 deletions(-) delete mode 100644 paper.md diff --git a/paper.md b/paper.md deleted file mode 100644 index 126edeb..0000000 --- a/paper.md +++ /dev/null @@ -1,96 +0,0 @@ ---- -title: "New, improved version of pycsamt package for robust AMT data processing" -tags: - - Python - - pycsamt - - processing - - AMT -authors: - - name: Kouao Laurent Kouadio^[Co-first author] - orcid: 0000-0001-7259-7254 - affiliation: "1, 2" -affiliations: - - name: Department of Geophysics, School of Geosciences and Info-physics, Central South University, China - index: 1 - - name: Equipe de Recherche Géophysique Appliquée, Laboratoire de Geologie Ressources Minerales et Energetiques, UFR des Sciences de la Terre et des Ressources Minières, Université Félix Houphouët-Boigny, Cote d'Ivoire - index: 2 -date: 02 September 2022 -bibliography: paper.bib ---- - - -# Summary - -Audio-frequency magnetotelluric (AMT) is a geophysical method widely used to map geologic contacts and structures, and to detect deep geological structures in a few meters to kilometers because of its good vertical resolution and wide range of exploration depth [@Goldaketal2015; @Sandbergetal1982; @Zongeetal1991]. Formerly, _pycsamt_ was devoted to solving relevant problems of the controlled source audio-frequency magnetotellurics(CSAMT)such as the correction of near-field -data, transition zone, and especially the static shift effect [@Berdichevskyetal1998; @Huetal2013; @Jiracek1990; @Kouadioetal2022]) -hence the suffix of CSAMT. The recent development is extended to all AMT methods -(i.e., above 1Hz) such as the natural source AMT (NSAMT) method. The latter has some advantages compared to -other geophysical methods like CSAMT [@Kouadioetal2020; @Sandbergetal1982; @Zongeetal1991]). -Among others, we list three: (i) First NSAMT is useful for imaging both deep geologic structure and near-surface -geology and can provide significant details.(ii) second, it includes a backpack portable system that allows -for use in difficult terrain. (iii) Third, the technique requires no high-voltage electrodes, and logistics -are relatively easy to support in the field. Stations can be acquired almost anywhere and can be placed any -distance apart. This allows for large-scale regional reconnaissance exploration or detailed surveys of local -geology and has no environmental impact [@Zonge2000]. Unfortunately, this advantage also -requires careful processing because the natural signals are not under our control and suffer from frequency -ranges with little or no signal. This is one of the main problems in collecting NSAMT data is the signal level -in the "attenuation band" also known as the "dead-band" [@Wangetal2017; @Zongeetal1991]. In this -work, I exhibited the result of a simple and fast code application as a new feature in the _pycsamt_ package -to recover the frequencies lost in the attenuation band. In practice, the recovery technique is not new since -it has been applied with Zonge International company [@Zheng2010]. However, in addition to recovering -signals from dead-band frequencies, I added a capability to strengthen amplitude signals (improve signal -noise-to ratio) in the subsequent processing of NSAMT data by using filters such as trimming moving-average -(MA), fixed-length MA [@Sandersetal2006], adaptative MA [@Torres-verdìnetal1992] (mostly used -for electromagnetic array profiling), and Savitzky-Golay. Indeed, the latter has the advantage of preserving -the original shape and features of the signal better than other types of filtering approaches. The proposed -code is tested in an experiment area with NSAMT data to show its efficaciousness in data recovery. The noise data -is composed of 50 stations with 54 frequencies ranging from 6Hz to 80kHz. The results show good recovery of -missing data at all weak and missing signals in the dead-band. - - -# Statement of need - -In short, _pycsamt_ follows the modular approach of software like MTpy [@Kriegeretal2014] and GMT [@Wessel1998] and contains -an inner handler to calibrate and to scale the raw data from different hardware into the appropriate units (SI) -. It also recomputes the deviation errors before processing [@Mykle1996]. Its recent development is composed of six main sub-packages -as displayed in [Figure 1]. - -![Brieve illustration of the main sub-packages: core (key functions and methods), modeling (deals with the inversion softwares such Occam2D of @deGrootetal1990, ModEM of @Kelbertetal2014), utils, processing and geodrill (for geology and drilling)](examples/paper_figures/fig.packages.png){width="5.260416666666667in" } - -Commonly the amplitude of natural electromagnetic fields shows a minimum in the frequency range of 1–2 kHz -and decays with increasing frequency. The fields from discharges and thunderstorms propagate in the earth’s -ionosphere cavity [@Goldsteinetal1975] and become the main natural signals at frequencies above 1 -Hz. Indeed, the amplitude of man-made noise (human activities, existence of factories near the survey sites, -power lines,etc) increases considerably and can dominate the natural source fields at higher frequencies [@Bastanietal2011]. -As a result, the raised noise degrades the quality of standard NSAMT data. Therefore, the NSAMT -signal at a frequency range above 1 kHz is unpredictable and may not be utilized for regular MT measurements -[@Smithetal1998; @Vozoff1991]. Most notably, the NSAMT dead-band is between approximately 1 kHz and -5 kHz (centered at around 2-3kHz), but also a signal low in the vicinity of 1-10 Hz where the transition to -magnetospheric energy sources occurs [@Goldaketal2015]. In this band, natural source signals are -generally absent. The EM energy is dissipated and often cultural electromagnetic noise fills the gap -[@Zonge2000]. To fix this gap around 1Hz and the dead-band, the response is extrapolated from results -observed at top frequencies (for instance 20, 40, 250, and 500 Hz). Moreover, according to the work of [@Labsonetal1985], -experience has indicated that the NSAMT signal level at 2kHz can be expected to approach 10-61nT/Hz-1/2 content example. -The script developed takes into account of aforementioned details to recover the signal. For illustration, [Figure 2] shows the -raw data of station E12 and E27 collected at all frequencies. The blue dot markers are the tensor data recovered -at the missing frequency signals. Note that the recovery tensor is used to (re)compute the apparent resistivity. After recovering the signal, the latter exhibits a field strength amplitude for the next processing step like a filtering. - -![A missing data recovery at the missing and attenuation signal at two randomly selected stations E12 and E27](examples/paper_figures/recovered_tensors.PNG){width="5.260416666666667in" } - -Furthermore, the skew analysis can also be performed at the 50 stations to show the dimensionality -(1D, 2D or 3D) of the structures [e.g. Figure 3] [@Bahr1991; @Swift1969; @Weaveretal2000]. The script ("_~.ctools.restoreZ_") for recovering lost data is located in the *processing* sub-packages. It accepts as input a list of raw standard Electrical Data Interchange (EDI) files [@Wightetal1988], a collection of -EDI-object from *.edi* module or MTpy Edi-objects [@Kirkbyetal2019]. It returns a Z object composed of a 2×2 matrix known as the complex impedance tensor which can be exported to EDI-file for other purpose. - -![An example of dimensionality analysis. Skew value greater than 5 degrees shows 3D dimensional structures and 2D or 1D otherwise](examples/paper_figures/fig.skew.PNG){width="5.260416666666667in" } - -# Acknowledgments - -I thank Liu Jianxing and Liu Rong of Central South University for their constructive suggestions. I'm also -gratefull to Kouamelan Serge Kouamelan of the School of Earth Science and Mineral Resources (STRM) -of Felix Houphouet Boigny University for its support in the software API construction. - - -# References - - - From 604eeb76a42c10f7f11e0b08d19759eefed09cf6 Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Tue, 10 Jan 2023 23:56:16 +0800 Subject: [PATCH 15/17] Update README.md --- README.md | 9 ++------- 1 file changed, 2 insertions(+), 7 deletions(-) diff --git a/README.md b/README.md index 719e962..b2e4382 100644 --- a/README.md +++ b/README.md @@ -10,16 +10,12 @@ * **Purpose** Previously, the software was intended for controlled source audio-frequency magnetotelluric (CSAMT) data processing (hereinafter the suffix CSAMT) and mostly related - to the groundwater exploration. The recent development is focused on the audio-magnetotelluric(AMT) methods i.e the frequency above 1Hz. It encompasses the CSAMT, the natural source AMT (NSAMT) and later the radio AMT. Indeed, the AMT methods are used broadly in diverse of exploration problems such as mineral, hydrocarbon, groundwater resources, as well as the fault-zone mapping above the 1km depth. + to the groundwater exploration. The recent development is focused on the audio-magnetotelluric(AMT) methods. Indeed, the AMT methods are used broadly in diverse of exploration problems such as mineral, hydrocarbon, groundwater resources, as well as the fault-zone mapping above the 1km depth. _pycsamt_ is designed to bring a piece of solution to the problems encountered by using AMT methods. It contains steps of AMT data processing and deals with [OCCAM2D](https://marineemlab.ucsd.edu/Projects/Occam/index.html) of [DeGroot-Hedlin and Constable, 1990](https://doi.org/10.1190/1.1442303) , the [MT2DInvMatlab](https://doi.org/10.1016/j.cageo.2008.10.010) of [Lee et al., 2009](https://doi.org/10.1016/j.cageo.2008.10.010) and [ModEM](https://sites.google.com/site/modularem/download) of [Kelbert et al., 2014](https://doi.org/10.1016/j.cageo.2014.01.010) for the modeling purpose. - It also provides processing tools for filtering data and restoring amplitudes at weak frequency (tensor or or scalar values ) in the "dead-dand" especially for the NSAMT where the natural signals are not under our control and suffer from frequency ranges with little or no signal. Some implemented filters are the trimming moving-average (MA), the fixed dipole-length MA (both proposed by [Zonge International Engineering (Zonge, 2000)]( http://www.zonge.com/legacy/PDF_DatPro/Astatic.pdf )) and the adaptative MA based on idea of [Torres-verdìn and Bostick, 1992](https://doi.org/10.1190/1.2400625). These filters are mostly used for fast removing the static effect especially in electromagnetic-array profiling survey. Some others filters such as "simple" for outliers removal and "PCA" can also be applied upstream for a particular data where the interferences are very strong (e.g. intenses humman activities, power lines, ...). Moreover, the "Savitzky-Golay" filter is also added to remove high-frequency noise from data since it has the advantage of preserving the original shape and features of the signal better than other types of filtering approaches such as MA techniques (simple, exponential, cumulative, weight). - - * **A specific WE sub-package** - - Besides the processing features, the software implements a special water exploration (WE) sub-package (geology + drilling ) referred as `geodrill`, entirely dedicated to improve the groundwater exploration techniques. The aim is to reduce the numerous unsucessful drillings mostly occurred due to their wrong locations after AMT geophysical surveys. It consists to minimize the use of supplement methods to AMT which commonly increases the operating budgets to right locate the drilling thereby reducing the misinterpretation of modeling results(e.g., demarcating the appropriate fracture zones). More details can be found in the **Citations** section. + It also provides processing tools for filtering and processing data( the trimming moving-average (MA), the fixed dipole-length MA ([Zonge International Engineering (Zonge, 2000)]( http://www.zonge.com/legacy/PDF_DatPro/Astatic.pdf )), the adaptative MA ( [Torres-verdìn and Bostick, 1992](https://doi.org/10.1190/1.2400625)). These filters are mostly used for fast removing the static effect especially in electromagnetic-array profiling survey. Some others filters such as "simple" for outliers removal and "PCA" can also be applied upstream for a particular data where the interferences are very strong (e.g. intenses humman activities, power lines, ...). Moreover, the "Savitzky-Golay" filter is also added to remove high-frequency noise from data since it has the advantage of preserving the original shape and features of the signal better than other types of filtering approaches such as MA techniques (simple, exponential, cumulative, weight). * **Note** @@ -29,7 +25,6 @@ ## Documentation * [Installation Guide](https://pycsamt.readthedocs.io/en/latest/installation.html?highlight=installation) -* [Demo of PS technique](https://pycsamt.readthedocs.io/en/latest/demo.html?highlight=demo) * [API Documentation](https://pycsamt.readthedocs.io/en/latest/) * [Home Page](https://github.com/WEgeophysics/pyCSAMT/wiki) * [User Guide](https://github.com/WEgeophysics/pyCSAMT/blob/develop/docs/pyCSAMT%20User%20Guide.pdf) From fc4553352514aeb56d575021387c84886fa76383 Mon Sep 17 00:00:00 2001 From: Daniel03 <59920007+WEgeophysics@users.noreply.github.com> Date: Tue, 10 Jan 2023 23:56:53 +0800 Subject: [PATCH 16/17] Update README.md --- README.md | 1 - 1 file changed, 1 deletion(-) diff --git a/README.md b/README.md index b2e4382..5a79918 100644 --- a/README.md +++ b/README.md @@ -3,7 +3,6 @@ [![Documentation Status](https://readthedocs.org/projects/pycsamt/badge/?version=latest)](https://pycsamt.readthedocs.io/en/latest/?badge=latest) [![Build Status](https://travis-ci.com/WEgeophysics/pyCSAMT.svg?branch=master)](https://travis-ci.com/WEgeophysics/pyCSAMT) ![GitHub](https://img.shields.io/github/license/WEgeophysics/pycsamt?color=blue&label=licence&logo=GNU&logoColor=red) ![GitHub release (latest by date)](https://img.shields.io/github/v/release/WEgeophysics/pyCSAMT?color=orange) [![DOI](https://zenodo.org/badge/DOI/10.5281/zenodo.5674430.svg)](https://doi.org/10.5281/zenodo.5674430) [![PyPI version](https://badge.fury.io/py/pycsamt.svg)](https://badge.fury.io/py/pycsamt) - ![GitHub repo size](https://img.shields.io/github/repo-size/WEgeophysics/pycsamt?color=0A4CEE&style=flat-square) ## Overview From 98306776776d1e8579ffd2bee926e45bef79f120 Mon Sep 17 00:00:00 2001 From: WEgeophysics Date: Mon, 3 Jul 2023 20:15:01 +0800 Subject: [PATCH 17/17] add expection for reading Tipper data --- pycsamt/modeling/occam2d.py | 16 +++++++--------- 1 file changed, 7 insertions(+), 9 deletions(-) diff --git a/pycsamt/modeling/occam2d.py b/pycsamt/modeling/occam2d.py index 888292d..69035cc 100644 --- a/pycsamt/modeling/occam2d.py +++ b/pycsamt/modeling/occam2d.py @@ -435,8 +435,7 @@ def parse_block_data(self, datablocks=None): return_counts= True) sites.astype('int32') freq.astype('int32') - - + # get mode and create model array k_=None m_= [int(s) for s in datum] @@ -448,8 +447,8 @@ def parse_block_data(self, datablocks=None): self.occam_dtype_ =k_ self.occam_dtype_value = values break - cf =False + if self.occam_dtype_ =='log_te_tm': self.te_appRho =np.zeros((len(freq), len(sites))) self.te_phase = np.zeros((len(freq), len(sites))) @@ -471,7 +470,11 @@ def parse_block_data(self, datablocks=None): self.tm_phase = np.zeros((len(freq), len(sites))) self.tm_error_appRho = np.zeros((len(freq), len(sites))) self.tm_error_phase = np.zeros((len(freq), len(sites))) - + else: + raise CSex.pyCSAMTError_occam2d( + "Three dimensional and Tipper are not implemented yet." + " Please use MTpy (https://github.com/MTgeophysics/mtpy.git)" + " or ModEM (http://www.coas.oregonstate.edu) instead.") # create for each mode id datablocks for kk, rowlines in enumerate(self.data): @@ -926,9 +929,6 @@ def read_occam2d_modelfile(self, model_fn=None, mesh_fn=None , iter_fn=None): print('** {0:<27} {1} {2}'.format('Occam Roughness params', '=', self.model_roughness)) - - - class Startup(object): """ Occam startup file Actually read startup file. @@ -1559,8 +1559,6 @@ def truncate_response (data , station_data, station_names ): getattr(self, 'resp_{0}_{1}'.format( occ, fwo.lower())).shape)) - - class Mesh(object): """ Read Occam read mesh file