{"id":62,"date":"2022-07-14T00:09:15","date_gmt":"2022-07-14T00:09:15","guid":{"rendered":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/chapter\/quantification-of-inversion-quality\/"},"modified":"2023-03-11T17:15:13","modified_gmt":"2023-03-11T17:15:13","slug":"quantification-of-inversion-quality","status":"publish","type":"chapter","link":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/chapter\/quantification-of-inversion-quality\/","title":{"raw":"4.5  Quantification of Inversion Quality","rendered":"4.5  Quantification of Inversion Quality"},"content":{"raw":"<div class=\"quantification-of-inversion-quality\">\r\n<p class=\"import-Normal\">Several approaches are commonly used to gain insight into the reliability of tomograms. For small inverse problems, it is possible to calculate the model resolution matrix (e.g., Menke<em>,<\/em> 1984) and present the diagonals, rows, and columns of these matrices as cross-sectional images. Conceptually, the <em>model resolution matrix<\/em> is the lens or filter through which the inversion <em>sees <\/em>the study region. For a linear inverse problem, the parameter estimates are expressed by Equation 14.<\/p>\r\n\r\n<table style=\"border: none; border-collapse: collapse; width: 100%;\">\r\n<tbody>\r\n<tr>\r\n<td style=\"width: 10%;\"><\/td>\r\n<td style=\"width: 80%; text-align: center;\">[latex]\\displaystyle m=[J^{\\mathrm{T}}C{_{D}}^{-1}J+\\varepsilon D^{\\mathrm{T}}D]^{-1}J^{\\mathrm{T}}C{_{D}}^{-1}d_{obs}\\approx [J^{\\mathrm{T}}C{_{D}}^{-1}J+\\varepsilon D^{\\mathrm{T}}D]^{-1}J^{\\mathrm{T}}C{_{D}}^{-1}Jm_{true}[\/latex]<\/td>\r\n<td style=\"width: 10%; text-align: right;\">(14)<\/td>\r\n<\/tr>\r\n<\/tbody>\r\n<\/table>\r\n<p class=\"import-Normal\">In this case, the model resolution matrix <em class=\"import-GWPCambria\">R<\/em> is defined as shown in Equation 15.<a id=\"equation_15\"><\/a><\/p>\r\n\r\n<table style=\"border: none; border-collapse: collapse; width: 100%;\">\r\n<tbody>\r\n<tr>\r\n<td style=\"width: 10%;\"><\/td>\r\n<td style=\"width: 80%; text-align: center;\">[latex]\\displaystyle R=[J^{\\mathrm{T}}C{_{D}}^{-1}J+\\varepsilon D^{\\mathrm{T}}D]^{-1}J^{\\mathrm{T}}C{_{D}}^{-1}J[\/latex]<\/td>\r\n<td style=\"width: 10%; text-align: right;\">(15)<\/td>\r\n<\/tr>\r\n<\/tbody>\r\n<\/table>\r\n<p class=\"import-Normal\">Consequently, the parameter estimates are the product of the true parameter values and the resolution matrix as shown in Equation 16.<\/p>\r\n\r\n<table style=\"border: none; border-collapse: collapse; width: 100%;\">\r\n<tbody>\r\n<tr>\r\n<td style=\"width: 10%;\"><\/td>\r\n<td style=\"width: 80%; text-align: center;\">[latex]\\displaystyle m=Rm_{true}[\/latex]<\/td>\r\n<td style=\"width: 10%; text-align: right;\">(16)<\/td>\r\n<\/tr>\r\n<\/tbody>\r\n<\/table>\r\n<p class=\"import-Normal\">For linear problems, where <em class=\"import-GWPCambria\">J<\/em> is independent of <em class=\"import-GWPCambria\">m<\/em><sub class=\"import-GWPsubscript\"><em><em>true<\/em><\/em><\/sub>, <em class=\"import-GWPCambria\">R<\/em> can be calculated prior to data collection. Given an estimate of measurement errors, the model resolution matrix can be calculated using Equation\u00a015 and used as a tool to assess and refine hypothetical survey designs and regularization criteria. In interpreting inversion results, <em class=\"import-GWPCambria\">R<\/em> is useful for identifying likely inversion artifacts (Day-Lewis et al.<em>,<\/em> 2005). The model resolution matrix quantifies the spatial averaging inherent to tomography; hence, it gives insight into which regions of a tomogram are well resolved versus poorly resolved. This information is valuable if tomograms are to be converted to quantitative estimates of porosity, concentration, or other hydrogeologic parameters. Calculation of resolution matrices, however, remains computationally prohibitive for many problems, particularly those involving 3-D inversion. Hence, few commercially available software packages support calculation of <em class=\"import-GWPCambria\">R<\/em>, and it is instead more common to look at an inverse problem\u2019s cumulative squared sensitivity vector (<em class=\"import-GWPCambria\">S<\/em>) as shown in Equation 17.<a id=\"equation_17\"><\/a><\/p>\r\n\r\n<table style=\"border: none; border-collapse: collapse; width: 100%;\">\r\n<tbody>\r\n<tr>\r\n<td style=\"width: 10%;\"><\/td>\r\n<td style=\"width: 80%; text-align: center;\">[latex]\\displaystyle S=\\mathrm{diag}(J^{T}J)[\/latex]<\/td>\r\n<td style=\"width: 10%; text-align: right;\">(17)<\/td>\r\n<\/tr>\r\n<\/tbody>\r\n<\/table>\r\n<p class=\"import-Normal\">Here, <em class=\"import-GWPCambria\">J<\/em> is the sensitivity matrix defined in <a href=\"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/chapter\/regularization-in-electrical-imaging-inversion#equation_10\">Equation\u00a010a<\/a> and diag(\u00a0) indicates the diagonal elements of a matrix. The sensitivity matrix can be used to gain semi-quantitative insight into how resolution varies spatially over a tomogram. Pixels with high values of sensitivity are relatively well informed by the measured data, whereas pixels with low values of sensitivity are poorly informed. It is important to note that, in contrast to <em class=\"import-GWPCambria\">R<\/em>, <em class=\"import-GWPCambria\">S<\/em> does not account for the effects of regularization criteria (as contained in <em class=\"import-GWPCambria\">D<\/em>) or measurement error (as contained in <em class=\"import-GWPCambria\">C<\/em><sub class=\"import-GWPsubscript\"><em><em>D<\/em><\/em><\/sub>). Rather, <em class=\"import-GWPCambria\">S<\/em> is based only on the survey geometry and measurement sensitivity. An example sensitivity map is provided in the case study in <a href=\"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/chapter\/4d-resistivity-of-a-biostimulation-experiment\/\">Section\u00a05.2<\/a> and qualitatively in <a href=\"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/part\/designing-surveys\/#figure_4\">Figure\u00a04<\/a>. Another question is whether inversion results are consistent with our conceptual models of the site\u2014this is a different definition of inversion quality. A good review exploring this idea is presented by Linde (2014).<\/p>\r\n\r\n<\/div>","rendered":"<div class=\"quantification-of-inversion-quality\">\n<p class=\"import-Normal\">Several approaches are commonly used to gain insight into the reliability of tomograms. For small inverse problems, it is possible to calculate the model resolution matrix (e.g., Menke<em>,<\/em> 1984) and present the diagonals, rows, and columns of these matrices as cross-sectional images. Conceptually, the <em>model resolution matrix<\/em> is the lens or filter through which the inversion <em>sees <\/em>the study region. For a linear inverse problem, the parameter estimates are expressed by Equation 14.<\/p>\n<table style=\"border: none; border-collapse: collapse; width: 100%;\">\n<tbody>\n<tr>\n<td style=\"width: 10%;\"><\/td>\n<td style=\"width: 80%; text-align: center;\">[latex]\\displaystyle m=[J^{\\mathrm{T}}C{_{D}}^{-1}J+\\varepsilon D^{\\mathrm{T}}D]^{-1}J^{\\mathrm{T}}C{_{D}}^{-1}d_{obs}\\approx [J^{\\mathrm{T}}C{_{D}}^{-1}J+\\varepsilon D^{\\mathrm{T}}D]^{-1}J^{\\mathrm{T}}C{_{D}}^{-1}Jm_{true}[\/latex]<\/td>\n<td style=\"width: 10%; text-align: right;\">(14)<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p class=\"import-Normal\">In this case, the model resolution matrix <em class=\"import-GWPCambria\">R<\/em> is defined as shown in Equation 15.<a id=\"equation_15\"><\/a><\/p>\n<table style=\"border: none; border-collapse: collapse; width: 100%;\">\n<tbody>\n<tr>\n<td style=\"width: 10%;\"><\/td>\n<td style=\"width: 80%; text-align: center;\">[latex]\\displaystyle R=[J^{\\mathrm{T}}C{_{D}}^{-1}J+\\varepsilon D^{\\mathrm{T}}D]^{-1}J^{\\mathrm{T}}C{_{D}}^{-1}J[\/latex]<\/td>\n<td style=\"width: 10%; text-align: right;\">(15)<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p class=\"import-Normal\">Consequently, the parameter estimates are the product of the true parameter values and the resolution matrix as shown in Equation 16.<\/p>\n<table style=\"border: none; border-collapse: collapse; width: 100%;\">\n<tbody>\n<tr>\n<td style=\"width: 10%;\"><\/td>\n<td style=\"width: 80%; text-align: center;\">[latex]\\displaystyle m=Rm_{true}[\/latex]<\/td>\n<td style=\"width: 10%; text-align: right;\">(16)<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p class=\"import-Normal\">For linear problems, where <em class=\"import-GWPCambria\">J<\/em> is independent of <em class=\"import-GWPCambria\">m<\/em><sub class=\"import-GWPsubscript\"><em><em>true<\/em><\/em><\/sub>, <em class=\"import-GWPCambria\">R<\/em> can be calculated prior to data collection. Given an estimate of measurement errors, the model resolution matrix can be calculated using Equation\u00a015 and used as a tool to assess and refine hypothetical survey designs and regularization criteria. In interpreting inversion results, <em class=\"import-GWPCambria\">R<\/em> is useful for identifying likely inversion artifacts (Day-Lewis et al.<em>,<\/em> 2005). The model resolution matrix quantifies the spatial averaging inherent to tomography; hence, it gives insight into which regions of a tomogram are well resolved versus poorly resolved. This information is valuable if tomograms are to be converted to quantitative estimates of porosity, concentration, or other hydrogeologic parameters. Calculation of resolution matrices, however, remains computationally prohibitive for many problems, particularly those involving 3-D inversion. Hence, few commercially available software packages support calculation of <em class=\"import-GWPCambria\">R<\/em>, and it is instead more common to look at an inverse problem\u2019s cumulative squared sensitivity vector (<em class=\"import-GWPCambria\">S<\/em>) as shown in Equation 17.<a id=\"equation_17\"><\/a><\/p>\n<table style=\"border: none; border-collapse: collapse; width: 100%;\">\n<tbody>\n<tr>\n<td style=\"width: 10%;\"><\/td>\n<td style=\"width: 80%; text-align: center;\">[latex]\\displaystyle S=\\mathrm{diag}(J^{T}J)[\/latex]<\/td>\n<td style=\"width: 10%; text-align: right;\">(17)<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p class=\"import-Normal\">Here, <em class=\"import-GWPCambria\">J<\/em> is the sensitivity matrix defined in <a href=\"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/chapter\/regularization-in-electrical-imaging-inversion#equation_10\">Equation\u00a010a<\/a> and diag(\u00a0) indicates the diagonal elements of a matrix. The sensitivity matrix can be used to gain semi-quantitative insight into how resolution varies spatially over a tomogram. Pixels with high values of sensitivity are relatively well informed by the measured data, whereas pixels with low values of sensitivity are poorly informed. It is important to note that, in contrast to <em class=\"import-GWPCambria\">R<\/em>, <em class=\"import-GWPCambria\">S<\/em> does not account for the effects of regularization criteria (as contained in <em class=\"import-GWPCambria\">D<\/em>) or measurement error (as contained in <em class=\"import-GWPCambria\">C<\/em><sub class=\"import-GWPsubscript\"><em><em>D<\/em><\/em><\/sub>). Rather, <em class=\"import-GWPCambria\">S<\/em> is based only on the survey geometry and measurement sensitivity. An example sensitivity map is provided in the case study in <a href=\"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/chapter\/4d-resistivity-of-a-biostimulation-experiment\/\">Section\u00a05.2<\/a> and qualitatively in <a href=\"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/part\/designing-surveys\/#figure_4\">Figure\u00a04<\/a>. Another question is whether inversion results are consistent with our conceptual models of the site\u2014this is a different definition of inversion quality. A good review exploring this idea is presented by Linde (2014).<\/p>\n<\/div>\n","protected":false},"author":1,"menu_order":19,"template":"","meta":{"pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"class_list":["post-62","chapter","type-chapter","status-publish","hentry"],"part":128,"_links":{"self":[{"href":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/wp-json\/pressbooks\/v2\/chapters\/62","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/wp-json\/wp\/v2\/users\/1"}],"version-history":[{"count":16,"href":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/wp-json\/pressbooks\/v2\/chapters\/62\/revisions"}],"predecessor-version":[{"id":455,"href":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/wp-json\/pressbooks\/v2\/chapters\/62\/revisions\/455"}],"part":[{"href":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/wp-json\/pressbooks\/v2\/parts\/128"}],"metadata":[{"href":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/wp-json\/pressbooks\/v2\/chapters\/62\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/wp-json\/wp\/v2\/media?parent=62"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/wp-json\/pressbooks\/v2\/chapter-type?post=62"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/wp-json\/wp\/v2\/contributor?post=62"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/books.gw-project.org\/electrical-imaging-for-hydrogeology\/wp-json\/wp\/v2\/license?post=62"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}