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1"use strict";(globalThis.webpackChunkvrgs_docs_v_3_1=globalThis.webpackChunkvrgs_docs_v_3_1||[]).push([[29138],{11467(s,e,a){a.r(e),a.d(e,{assets:()=>c,contentTitle:()=>m,default:()=>d,frontMatter:()=>t,metadata:()=>n,toc:()=>r});const n=JSON.parse('{"id":"general/wells-seismic/seismic-modelling-method","title":"Synthetic Seismic Modelling from Classified Meshes: Method and Implementation","description":"A detailed, paper-style account of how VRGS forward-models a band-limited synthetic seismic section from a classified triangulated mesh: reflector extraction, the 2-D extrusion reflectivity model, the Kirchhoff diffraction stack, co-located facies/impedance attributes, and the rendering pipeline.","source":"@site/docs/general/wells-seismic/seismic-modelling-method.md","sourceDirName":"general/wells-seismic","slug":"/general/wells-seismic/seismic-modelling-method","permalink":"/docs/next/general/wells-seismic/seismic-modelling-method","draft":false,"unlisted":false,"editUrl":"https://github.com/vrgeoscience/vrgs_docs_v3/tree/master/docs/general/wells-seismic/seismic-modelling-method.md","tags":[],"version":"current","sidebarPosition":4,"frontMatter":{"id":"seismic-modelling-method","title":"Synthetic Seismic Modelling from Classified Meshes: Method and Implementation","sidebar_label":"Seismic Modelling \u2014 Method","sidebar_position":4,"description":"A detailed, paper-style account of how VRGS forward-models a band-limited synthetic seismic section from a classified triangulated mesh: reflector extraction, the 2-D extrusion reflectivity model, the Kirchhoff diffraction stack, co-located facies/impedance attributes, and the rendering pipeline.","keywords":["seismic","forward modelling","kirchhoff","diffraction stack","reflectivity","facies","impedance","attributes","outcrop","synthetic seismic"]},"sidebar":"docs","previous":{"title":"Seismic Modelling","permalink":"/docs/next/general/wells-seismic/seismic-modelling"},"next":{"title":"Voxel Volumes (CT / MRI)","permalink":"/docs/next/general/wells-seismic/voxel-volumes"}}');var l=a(74848),i=a(28453);const t={id:"seismic-modelling-method",title:"Synthetic Seismic Modelling from Classified Meshes: Method and Implementation",sidebar_label:"Seismic Modelling \u2014 Method",sidebar_position:4,description:"A detailed, paper-style account of how VRGS forward-models a band-limited synthetic seismic section from a classified triangulated mesh: reflector extraction, the 2-D extrusion reflectivity model, the Kirchhoff diffraction stack, co-located facies/impedance attributes, and the rendering pipeline.",keywords:["seismic","forward modelling","kirchhoff","diffraction stack","reflectivity","facies","impedance","attributes","outcrop","synthetic seismic"]},m="Synthetic Seismic Modelling from Classified Meshes",c={},r=[{value:"Abstract",id:"abstract",level:2},{value:"1. Introduction",id:"1-introduction",level:2},{value:"2. Method",id:"2-method",level:2},{value:"2.1 Inputs",id:"21-inputs",level:3},{value:"2.2 Reflector extraction",id:"22-reflector-extraction",level:3},{value:"2.3 Reflectivity",id:"23-reflectivity",level:3},{value:"2.4 The two-dimensional extrusion assumption",id:"24-the-two-dimensional-extrusion-assumption",level:3},{value:"2.5 The Kirchhoff diffraction stack",id:"25-the-kirchhoff-diffraction-stack",level:3},{value:"2.6 Wavelet and band-limitation",id:"26-wavelet-and-band-limitation",level:3},{value:"2.7 Acquisition geometry",id:"27-acquisition-geometry",level:3},{value:"2.8 Co-located facies and impedance attributes (flattened overlay)",id:"28-co-located-facies-and-impedance-attributes-flattened-overlay",level:3},{value:"3. 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Future work",id:"6-future-work",level:2},{value:"References",id:"references",level:2},{value:"Related",id:"related",level:2}];function h(s){const e={a:"a",annotation:"annotation",blockquote:"blockquote",code:"code",em:"em",h1:"h1",h2:"h2",h3:"h3",header:"header",li:"li",math:"math",mfrac:"mfrac",mi:"mi",mn:"mn",mo:"mo",mover:"mover",mrow:"mrow",mspace:"mspace",mstyle:"mstyle",msub:"msub",msup:"msup",mtext:"mtext",munder:"munder",ol:"ol",p:"p",path:"path",semantics:"semantics",span:"span",strong:"strong",svg:"svg",table:"table",tbody:"tbody",td:"td",th:"th",thead:"thead",tr:"tr",ul:"ul",...(0,i.R)(),...s.components};return(0,l.jsxs)(l.Fragment,{children:[(0,l.jsx)(e.header,{children:(0,l.jsx)(e.h1,{id:"synthetic-seismic-modelling-from-classified-meshes",children:"Synthetic Seismic Modelling from Classified Meshes"})}),"\n",(0,l.jsxs)(e.blockquote,{children:["\n",(0,l.jsxs)(e.p,{children:[(0,l.jsx)(e.strong,{children:"Scope."})," This page is the ",(0,l.jsx)(e.em,{children:"methodological"})," companion to the\n",(0,l.jsx)(e.a,{href:"/docs/next/general/wells-seismic/seismic-modelling",children:"Seismic Modelling"})," user guide. 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1are architecture in enough detail to\nreproduce or extend the method. The user guide covers the workflow and the\ndialog; here we explain ",(0,l.jsx)(e.em,{children:"why"})," the result looks the way it does."]}),"\n"]}),"\n",(0,l.jsx)(e.h2,{id:"abstract",children:"Abstract"}),"\n",(0,l.jsxs)(e.p,{children:["We describe a forward operator that turns a ",(0,l.jsx)(e.strong,{children:"classified triangulated surface\nmesh"})," \u2014 an outcrop or interpreted horizon model carrying per-vertex ",(0,l.jsx)(e.em,{children:"facies"})," and\n",(0,l.jsx)(e.em,{children:"acoustic impedance"})," \u2014 into a ",(0,l.jsx)(e.strong,{children:"band-limited synthetic seismic section"}),". Contacts\nbetween facies are treated as reflecting elements; their reflectivity follows from\nthe impedance contrast across the contact, and their orientation follows from the\nin-plane impedance gradient under an explicit ",(0,l.jsx)(e.strong,{children:"two-dimensional extrusion\nassumption"}),". A ",(0,l.jsx)(e.strong,{children:"Kirchhoff diffraction stack"})," sums the contribution of every\nreflecting element into each trace using straight-ray traveltimes in a constant\nbackground velocity, geometric spreading, and an obliquity weight; each trace is\nthen convolved with a chosen wavelet. The same traversal records, co-located with\nthe modelled reflections, the ",(0,l.jsx)(e.strong,{children:"facies and impedance that produced them"}),", which\nare exposed as filterable attribute layers on the resulting section. We close with\nthe data model, the colour-mapped panel renderer, and the assumptions and\nlimitations of the approach."]}),"\n",(0,l.jsx)(e.h2,{id:"1-introduction",children:"1. Introduction"}),"\n",(0,l.jsxs)(e.p,{children:["Tying outcrop interpretation to the seismic scale is a recurring problem in\nreservoir geology: a contact that is obvious on a cliff face may image strongly,\nweakly, or only as a diffraction once it is band-limited and viewed under a\nparticular acquisition geometry. Rather than exporting to an external modelling\npackage, VRGS computes a synthetic section ",(0,l.jsx)(e.em,{children:"in situ"})," from the same classified mesh\nthe interpreter is already working with. The method is deliberately lightweight \u2014\na single-scattering (Born/Kirchhoff) approximation with straight rays \u2014 so that it\nruns interactively on a background worker and answers the qualitative question\n",(0,l.jsx)(e.em,{children:'"how would this geometry image?"'})," rather than producing a calibrated amplitude\nprediction."]}),"\n",(0,l.jsx)(e.h2,{id:"2-method",children:"2. 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The\nlayers are produced upstream (classification, painting, or the ",(0,l.jsx)(e.em,{children:"Add Test Facies +\nImpedance"})," helper) and are read by name; the operator does not classify."]}),"\n",(0,l.jsx)(e.h3,{id:"22-reflector-extraction",children:"2.2 Reflector extraction"}),"\n",(0,l.jsxs)(e.p,{children:["The mesh is traversed facet by facet. 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A facet whose three vertices share\na single facies is interior to a unit and ",(0,l.jsx)(e.strong,{children:"contributes nothing"}),". 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Doing the flatten ",(0,l.jsx)(e.em,{children:"per element"})," (not as a per-trace\npost-shift) keeps the band thin \u2014 the along-line window does not smear it."]}),"\n",(0,l.jsxs)(e.p,{children:["For ",(0,l.jsxs)(e.span,{className:"katex",children:[(0,l.jsx)(e.span,{className:"katex-mathml",children:(0,l.jsx)(e.math,{xmlns:"http://www.w3.org/1998/Math/MathML",children:(0,l.jsxs)(e.semantics,{children:[(0,l.jsxs)(e.mrow,{children:[(0,l.jsx)(e.mi,{children:"\u03b4"}),(0,l.jsx)(e.mo,{children:"="}),(0,l.jsx)(e.mn,{children:"0"})]}),(0,l.jsx)(e.annotation,{encoding:"application/x-tex",children:"\\delta = 0"})]})})}),(0,l.jsxs)(e.span,{className:"katex-html","aria-hidden":"true",children:[(0,l.jsxs)(e.span,{className:"base",children:[(0,l.jsx)(e.span,{className:"strut",style:{height:"0.6944em"}}),(0,l.jsx)(e.span,{className:"mord mathnormal",style:{marginRight:"0.03785em"},children:"\u03b4"}),(0,l.jsx)(e.span,{className:"mspace",style:{marginRight:"0.2778em"}}),(0,l.jsx)(e.span,{className:"mrel",children:"="}),(0,l.jsx)(e.span,{className:"mspace",style:{marginRight:"0.2778em"}})]}),(0,l.jsxs)(e.span,{className:"base",children:[(0,l.jsx)(e.span,{className:"strut",style:{height:"0.6444em"}}),(0,l.jsx)(e.span,{className:"mord",children:"0"})]})]})]})," this reduces to placing each contact at its true depth on the trace\nabove it \u2014 horizontal bands, no arch. With a regional dip, dipping bed-parallel contacts\ncollapse to a constant flattened depth and image as ",(0,l.jsx)(e.strong,{children:"horizontal bands"}),". The amplitude\nis flattened to match by the corresponding per-trace shift (each trace moved up by\n",(0,l.jsxs)(e.span,{className:"katex",children:[(0,l.jsx)(e.span,{className:"katex-mathml",children:(0,l.jsx)(e.math,{xmlns:"http://www.w3.org/1998/Math/MathML",children:(0,l.jsxs)(e.semantics,{children:[(0,l.jsxs)(e.mrow,{children:[(0,l.jsxs)(e.msub,{children:[(0,l.jsx)(e.mi,{children:"u"}),(0,l.jsx)(e.mtext,{children:"tr"})]}),(0,l.jsx)(e.mi,{children:"tan"}),(0,l.jsx)(e.mo,{children:"\u2061"}),(0,l.jsx)(e.mi,{children:"\u03b4"})]}),(0,l.jsx)(e.annotation,{encoding:"application/x-tex",children:"u_{\\text{tr}}\\tan\\delta"})]})})}),(0,l.jsx)(e.span,{className:"katex-html","aria-hidden":"true",children:(0,l.jsxs)(e.span,{className:"base",children:[(0,l.jsx)(e.span,{className:"strut",style:{height:"0.8444em",verticalAlign:"-0.15em"}}),(0,l.jsxs)(e.span,{className:"mord",children:[(0,l.jsx)(e.span,{className:"mord mathnormal",children:"u"}),(0,l.jsx)(e.span,{className:"msupsub",children:(0,l.jsxs)(e.span,{className:"vlist-t vlist-t2",children:[(0,l.jsxs)(e.span,{className:"vlist-r",children:[(0,l.jsx)(e.span,{className:"vlist",style:{height:"0.2806em"}
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1 each layer carries a histogram and a value\n",(0,l.jsx)(e.strong,{children:"filter"}),". Filtering masks the panel \u2014 samples outside the filter range (and cells\nwith no recorded attribute) are made transparent \u2014 so the interpreter can, for\nexample, isolate the reflections produced by a single facies or by impedance\ncontrasts above a threshold. Undefined cells are encoded as not-a-number and\ndiscarded in the shader, which is also how the filter mask is realised."]}),"\n",(0,l.jsx)(e.h3,{id:"34-concurrency",children:"3.4 Concurrency"}),"\n",(0,l.jsx)(e.p,{children:"The forward model runs on a background worker; the result object is published to the\nscene immediately and its render path is gated until the worker has finished\npopulating the buffers, so the UI stays responsive while a dense mesh is modelled."}),"\n",(0,l.jsx)(e.h2,{id:"4-parameter-reference-theory-view",children:"4. Parameter reference (theory view)"}),"\n",(0,l.jsxs)(e.table,{children:[(0,l.jsx)(e.thead,{children:(0,l.jsxs)(e.tr,{children:[(0,l.jsx)(e.th,{children:"Parameter"}),(0,l.jsx)(e.th,{children:"Symbol"}),(0,l.jsx)(e.th,{children:"Effect"})]})}),(0,l.jsxs)(e.tbody,{children:[(0,l.jsxs)(e.tr,{children:[(0,l.jsx)(e.td,{children:"Backgroun
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with ",(0,l.jsxs)(e.span,{className:"katex",children:[(0,l.jsx)(e.span,{className:"katex-mathml",children:(0,l.jsx)(e.math,{xmlns:"http://www.w3.org/1998/Math/MathML",children:(0,l.jsxs)(e.semantics,{children:[(0,l.jsx)(e.mrow,{children:(0,l.jsx)(e.mi,{children:"N"})}),(0,l.jsx)(e.annotation,{encoding:"application/x-tex",children:"N"})]})})}),(0,l.jsx)(e.span,{className:"katex-html","aria-hidden":"true",children:(0,l.jsxs)(e.span,{className:"base",children:[(0,l.jsx)(e.span,{className:"strut",style:{height:"0.6833em"}}),(0,l.jsx)(e.span,{className:"mord mathnormal",style:{marginRight:"0.10903em"},children:"N"})]})})]})," sets the record length"]})]}),(0,l.jsxs)(e.tr,{children:[(0,l.jsx)(e.td,{children:"Number of samples"}),(0,l.jsx)(e.td,{children:(0,l.jsxs)(e.span,{className:"katex",children:[(0,l.jsx)(e.span,{className:"katex-mathml",children:(0,l.jsx)(e.math,{xmlns:"http://www.w3.org/1998/Math/MathML",children:(0,l.jsxs)(e.semantics,{children:[(0,l.jsx)(e.mrow,{children:(0,l.jsx)(e.mi,{children:"N"})}),(0,l.jsx)(e.annotation,{encoding:"application/x-tex",children:"N"})]})})}),(0,l.jsx)(e.span,{className:"katex-html","aria-hidden":"true",children:(0,l.jsxs)(e.span,{className:"base",children:[(0,l.jsx)(e.span,{className:"strut",style:{height:"0.6833em"}}),(0,l.jsx)(e.span,{className:"mord mathnormal",style:{marginRight:"0.10903em"},children:"N"})]})})]})}),(0,l.jsx)(e.td,{children:"trace length / imaged depth"})]}),(0,l.jsxs)(e.tr,{children:[(0,l.jsx)(e.td,{children:"Wavelet frequency"}),(0,l.jsx)(e.td,{children:(0,l.jsxs)(e.span,{className:"katex",children:[(0,l.jsx)(e.span,{className:"katex-mathml",children:(0,l.jsx)(e.math,{xmlns:"http://www.w3.org/1998/Math/MathML",children:(0,l.jsxs)(e.semantics,{children:[(0,l.jsx)(e.mrow,{children:(0,l.jsx)(e.mi,{children:"f"})}),(0,l.jsx)(e.annotation,{encoding:"application/x-tex",children:"f"})]})})}),(0,l.jsx)(e.span,{className:"katex-html","aria-hidden":"true",children:(0,l.jsxs)(e.span,{className:"base",children:[(0,l.jsx)(e.span,{className:"strut",style:{height:"0.8889em",verticalAlign:"-0.1944em"}}),(0,l.jsx)(e.span,{className:"mord mathnormal",style:{marginRight:"0.10764em"},children:"f"})]})})]})}),(0,l.jsxs)(e.td,{children:["bandwidth \u2192 reflection thickness, ",(0,l.jsxs)(e.span,{className:"katex",children:[(0,l.jsx)(e.span,{className:"katex-mathml",children:(0,l.jsx)(e.math,{xmlns:"http://www.w3.org/1998/Math/MathML",children:(0,l.jsxs)(e.semantics,{children:[(0,l.jsxs)(e.mrow,{children:[(0,l.jsx)(e.mi,{children:"\u03bb"}),(0,l.jsx)(e.mi,{mathvariant:"normal",children:"/"}),(0,l.jsx)(e.mn,{children:"4"})]}),(0,l.jsx)(e.annotation,{encoding:"application/x-tex",children:"\\lambda/4"})]})})}),(0,l.jsx)(e.span,{className:"katex-html","aria-hidden":"true",children:(0,l.jsxs)(e.span,{className:"base",children:[(0,l.jsx)(e.span,{className:"strut",style:{height:"1em",verticalAlign:"-0.25em"}}),(0,l.jsx)(e.span,{className:"mord mathnormal",children:"\u03bb"}),(0,l.jsx)(e.span,{className:"mord",children:"/4"})]})})]})," resolution"]})]}),(0,l.jsxs)(e.tr,{children:[(0,l.jsx)(e.td,{children:"Azimuth, spacing, count, height"}),(0,l.jsx)(e.td,{children:"\u2014"}),(0,l.jsx)(e.td,{children:"acquisition line position and sampling"})]}),(0,l.jsxs)(e.tr,{children:[(0,l.jsx)(e.td,{children:"Offset mode / distance"}),(0,l.jsx)(e.td,{children:"\u2014"}),(0,l.jsx)(e.td,{children:"zero-offset vs. offset acquisition (fault-tip imaging)"})]})]})]}),"\n",(0,l.jsx)(e.h2,{id:"5-assumptions-and-limitations",children:"5. Assumptions and limitations"}),"\n",(0,l.jsxs)(e.ol,{children:["\n",(0,l.jsxs)(e.li,{children:[(0,l.jsx)(e.strong,{children:"Single scattering."})," No multiples, transmission loss, mode conversion, or\nattenuation; amplitudes are qualitative, not calibrated."]}),"\n",(0,l.jsxs)(e.li,{children:[(0,l.jsxs)(e.strong,{children:["Straight rays, constant ",(0,l.jsxs)(e.span,{className:"katex",children:[(0,l.jsx)(e.span,{className:"katex-mathml",children:(0,l.jsx)(e.math,{xmlns:"http://www.w3.org/1998/Math/MathML",children:(0,l.jsxs)(e.semantics,{children:[(0,l.jsx)(e.mrow,{children:(0,l.jsxs)(e.msub,{children:[(0,l.jsx)(e.mi,{children:"V"}),(0,l.jsx)(e.mn,{children:"0"})]})}),(0,l.jsx)(e.annotation,{encoding:"application/x-tex",children:"V_0"})]})})}),(0,l.jsx)(e.span,{className:"katex-html","aria-hidden":"true",children:(0,l.jsxs)(e.span,{className:"base",children:[(0,l.jsx)(e.span,{className:"strut",style:{height:"0.8333em",verticalAlign:"-0.15em"}}),(0,l.jsxs)(e.span,{className:"mord",children:[(0,l.jsx)(e.span,{className:"mord mathnormal",style:{marginRight:"0.22222em"},children:"V"}),(0,l.jsx)(e.span,{className:"msupsub",children:(0,l.jsxs)(e.span,{className:"vlist-t vlist-t2",children:[(0,l.jsxs)(e.span,{className:"vlist-r",children:[(0,l.jsx)(e.span,{className:"vlist",style:{height:"0.3011em"}
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Future work"}),"\n",(0,l.jsxs)(e.p,{children:["Angle-dependent reflectivity (AVO), curved-ray or eikonal traveltimes for a\nheterogeneous ",(0,l.jsxs)(e.span,{className:"katex",children:[(0,l.jsx)(e.span,{className:"katex-mathml",children:(0,l.jsx)(e.math,{xmlns:"http://www.w3.org/1998/Math/MathML",children:(0,l.jsxs)(e.semantics,{children:[(0,l.jsxs)(e.mrow,{children:[(0,l.jsxs)(e.msub,{children:[(0,l.jsx)(e.mi,{children:"V"}),(0,l.jsx)(e.mn,{children:"0"})]}),(0,l.jsx)(e.mo,{stretchy:"false",children:"("}),(0,l.jsx)(e.mi,{mathvariant:"bold",children:"x"}),(0,l.jsx)(e.mo,{stretchy:"false",children:")"})]}),(0,l.jsx)(e.annotation,{encoding:"application/x-tex",children:"V_0(\\mathbf x)"})]})})}),(0,l.jsx)(e.span,{className:"katex-html","aria-hidden":"true",children:(0,l.jsxs)(e.span,{className:"base",children:[(0,l.jsx)(e.span,{className:"strut",style:{height:"1em",verticalAlign:"-0.25em"}}),(0,l.jsxs)(e.span,{className:"mord",children:[(0,l.jsx)(e.span,{className:"mord mathnormal",style:{marginRight:"0.22222em"},children:"V"}),(0,l.jsx)(e.span,{className:"msupsub",children:(0,l.jsxs)(e.span,{className:"vlist-t vlist-t2",children:[(0,l.jsxs)(e.span,{className:"vlist-r",children:[(0,l.jsx)(e.span,{className:"vlist",style:{height:"0.3011em"},children:(0,l.jsxs)(e.span,{style:{top:"-2.55em",marginLeft:"-0.2222em",marginRight:"0.05em"},children:[(0,l.jsx)(e.span,{className:"pstrut",style:{height:"2.7em"}}),(0,l.jsx)(e.span,{className:"sizing reset-size6 size3 mtight",children:(0,l.jsx)(e.span,{className:"mord mtight",children:"0"})})]})}),(0,l.jsx)(e.span,{className:"vlist-s",children:"\u200b"})]}),(0,l.jsx)(e.span,{className:"vlist-r",children:(0,l.jsx)(e.span,{className:"vlist",style:{height:"0.15em"},children:(0,l.jsx)(e.span,{})})})]})})]}),(0,l.jsx)(e.span,{className:"mopen",children:"("}),(0,l.jsx)(e.span,{className:"mord mathbf",children:"x"}),(0,l.jsx)(e.span,{className:"mclose",children:")"})]})})]}),", multiple-arrival handling, and substitution of\nmeasured dip vectors for the computed impedance gradient are natural extensions, as\nis migrating the inline trace storage to a sidecar for very large gathers."]}),"\n",(0,l.jsx)(e.h2,{id:"references",children:"References"}),"\n",(0,l.jsxs)(e.ol,{children:["\n",(0,l.jsxs)(e.li,{children:["Ricker, N. (1953). ",(0,l.jsx)(e.em,{children:"The form and laws of propagation of seismic wavelets."}),"\nGeophysics, 18(1), 10\u201340."]}),"\n",(0,l.jsxs)(e.li,{children:["Klauder, J. R., Price, A. C., Darlington, S., & Albersheim, W. J. (1960).\n",(0,l.jsx)(e.em,{children:"The theory and design of chirp radars."})," Bell System Technical Journal, 39(4)."]}),"\n",(0,l.jsxs)(e.li,{children:["Schneider, W. A. (1978). ",(0,l.jsx)(e.em,{children:"Integral formulation for migration in two and three\ndimensions."})," Geophysics, 43(1), 49\u201376."]}),"\n",(0,l.jsxs)(e.li,{children:["Bleistein, N. (1987). ",(0,l.jsx)(e.em,{children:"On the imaging of reflectors in the earth."})," Geophysics,\n52(7), 931\u2013942."]}),"\n",(0,l.jsxs)(e.li,{children:["Carcione, J. M., Herman, G. C., & ten Kroode, A. P. E. (2002). ",(0,l.jsx)(e.em,{children:"Seismic\nmodeling."})," Geophysics, 67(4), 1304\u20131325."]}),"\n",(0,l.jsxs)(e.li,{children:["Sheriff, R. E., & Geldart, L. P. (1995). ",(0,l.jsx)(e.em,{children:"Exploration Seismology"})," (2nd ed.).\nCambridge University Press."]}),"\n"]}),"\n",(0,l.jsx)(e.h2,{id:"related",children:"Related"}),"\n",(0,l.jsxs)(e.ul,{children:["\n",(0,l.jsxs)(e.li,{children:[(0,l.jsx)(e.a,{href:"/docs/next/general/wells-seismic/seismic-modelling",children:"Seismic Modelling"})," \u2014 the user workflow and dialog reference."]}),"\n"]})]})}function d(s={}){const{wrapper:e}={...(0,i.R)(),...s.components};return e?(0,l.jsx)(e,{...s,children:(0,l.jsx)(h,{...s})}):h(s)}},28453(s,e,a){a.d(e,{R:()=>t,x:()=>m});var n=a(96540);const l={},i=n.createContext(l);function t(s){const e=n.useContext(i);return n.useMemo(function(){return"function"==typeof s?s(e):{...e,...s}},[e,s])}function m(s){let e;return e=s.disableParentContext?"function"==typeof s.components?s.components(l):s.components||l:t(s.components),n.createElement(i.Provider,{value:e},s.children)}}}]);

Line numbers count LF bytes from the start of the resource, as the search results do. Vendor segments are library code the classifier recognised; they are stored but not indexed. Bytes are shown as Latin1 characters, one per byte.