{"id":7,"date":"2025-05-07T17:37:57","date_gmt":"2025-05-07T17:37:57","guid":{"rendered":"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/?page_id=7"},"modified":"2025-12-13T00:38:42","modified_gmt":"2025-12-13T00:38:42","slug":"methodology","status":"publish","type":"page","link":"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/methodology\/","title":{"rendered":"Methodology"},"content":{"rendered":"\n<p style=\"text-align: justify\">        We present a physics-guided, two-stage framework for dynamic thermal scene reconstruction from UAV\n        infrared imagery using 3D Gaussian Splatting. The core design principle is to decouple\n        <strong>static scene geometry<\/strong> from <strong>time-varying thermal dynamics<\/strong>:\n        Stage&nbsp;1 learns a stable 3D thermal representation at discrete timestamps, and Stage&nbsp;2 models\n        temperature evolution over time while keeping geometry fixed.<\/p>\n     \n <p style=\"text-align: justify\">\n        Given calibrated UAV thermal frames captured across a mission, our goal is to reconstruct a thermal scene that\n        supports <strong>novel-view synthesis<\/strong> and <strong>time-dependent temperature estimation<\/strong>.\n        Thermal imagery introduces challenges not present in RGB\u2014view-dependent attenuation, conduction-induced edge\n        blurring, and temporal thermal variation\u2014which we address with physics-aware components integrated into a\n        Gaussian splatting pipeline.\n      <\/p>\n\n\n\n<h3 class=\"wp-block-heading\"><strong>Thermal Image Formation Revisited<\/strong><\/h3>\n\n\n\n<p style=\"text-align: justify\">In contrast to visible light reconstruction, thermal image formation is heavily influenced by the temperature, which in a sense relies on dynamic atmospheric and material conditions. We model the observed thermal frame x<sub>t,<em>\u03b8<\/em><\/sub> at time <em>t<\/em> and viewpoint <em>\u03b8<\/em> as: <\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"408\" height=\"100\" src=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-6.24.38\u202fPM.png\" alt=\"\" class=\"wp-image-141\" style=\"width:158px;height:auto\" srcset=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-6.24.38\u202fPM.png 408w, https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-6.24.38\u202fPM-300x74.png 300w\" sizes=\"auto, (max-width: 408px) 100vw, 408px\" \/><\/figure>\n<\/div>\n\n\n<p style=\"text-align: justify\"><em>where <\/em>f(X)<em> is the canonical projection of an ideal, unperturbed thermal 3D scene, and <\/em>P<sub>t<\/sub>,<sub><em>\u03b8<\/em><\/sub> encodes viewpoint and time dependent physical distortions. To generate more accurate reconstructions, we seek to estimate the underlying 3D thermal state X<sup>~<\/sup> such that:<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"264\" height=\"61\" src=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-1.02.39\u202fPM.png\" alt=\"\" class=\"wp-image-129\" \/><\/figure>\n<\/div>\n\n\n<p>thereby correcting for the effects of environmental attenuation and surface level thermal diffusion.<\/p>\n\n\n\n<h2 class=\"wp-block-heading\"><strong>Stage 1: Static Physics Guided Thermal 3D Reconstruction<\/strong><\/h2>\n\n\n\n<h3 class=\"wp-block-heading\"><strong>1. Viewpoint Aware Attenuation Estimator (VAE)<\/strong><\/h3>\n\n\n\n<p style=\"text-align: justify\">The <strong>VAE module<\/strong> models the degradation of thermal intensity due to atmospheric interference. Inspired by classical radiative transfer principles, we represent thermal attenuation as:<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"175\" height=\"51\" src=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-6.16.49\u202fPM.png\" alt=\"\" class=\"wp-image-136\" \/><\/figure>\n<\/div>\n\n\n<p>where k denotes the attenuation factor, and <em>d<\/em> is the propagation path length.<\/p>\n\n\n\n<p style=\"text-align: justify\">We design a lightweight MLP that predicts the attenuation parameters (k(abs), k(sca), d) for each 3D Gaussian, conditioned on its spatial position and timestamp. This learned correction is applied directly to the Gaussian\u2019s appearance encoding (e.g., SH coefficients), yielding:<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"292\" height=\"47\" src=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-6.21.39\u202fPM.png\" alt=\"\" class=\"wp-image-139\" \/><\/figure>\n<\/div>\n\n\n<p>This step compensates for the viewpoint specific drop in thermal radiance and significantly reduces ghosting and floaters.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\"><strong>2. Thermal Diffusion Correction Unit (TDCU)<\/strong><\/h3>\n\n\n\n<p style=\"text-align: justify\">To address the edge blurring caused by heat transfer between adjacent surfaces, we introduce the <strong>Thermal Diffusion Correction Unit (TDCU)<\/strong>.\n In thermal imaging, heat is fundamentally a form of energy that naturally diffuses from hotter to cooler regions. As this energy propagates through conduction, it leads to smoothed temperature gradients across object boundaries. In practice, this manifests in thermal images as softened edges, where the temperature difference between adjacent surfaces becomes visually indistinct particularly problematic in scenes where fine boundaries carry semantic importance.\nTo mitigate that, we draw from the heat equation to simulate spatial temperature smoothing:<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"153\" height=\"66\" src=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-6.48.22\u202fPM.png\" alt=\"\" class=\"wp-image-148\" srcset=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-6.48.22\u202fPM.png 153w, https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-6.48.22\u202fPM-150x66.png 150w\" sizes=\"auto, (max-width: 153px) 100vw, 153px\" \/><\/figure>\n<\/div>\n\n\n<p>where <em>u<\/em> represents the surface temperature field and <em>\u03b1<\/em> captures local diffusivity.<\/p>\n\n\n\n<p style=\"text-align: justify\">Instead of relying on fixed physical coefficients, the TDCU is implemented as a deep residual network that ingests both the original image and its second order spatial gradients. By learning a spatially adaptive correction mask, the TDCU selectively sharpens edges that have been degraded by thermal conduction while preserving coherent heat flow patterns.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\"><strong>3. Surface Smoothness Regularizer (SSR)<\/strong><\/h3>\n\n\n\n<p style=\"text-align: justify\">While real world thermal distributions tend to change smoothly, abrupt transitions or sharp corners often arise from modeling errors. We introduce the <strong>Surface Smoothness Regularizer (SSR)<\/strong> to penalize spurious discontinuities. Drawing on the Harris corner metric, we compute a spatial map of irregular regions and weight their contribution to the loss:<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"304\" height=\"59\" src=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-7.01.45\u202fPM.png\" alt=\"\" class=\"wp-image-153\" srcset=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-7.01.45\u202fPM.png 304w, https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-7.01.45\u202fPM-300x58.png 300w\" sizes=\"auto, (max-width: 304px) 100vw, 304px\" \/><\/figure>\n<\/div>\n\n\n<p style=\"text-align: justify\">where <em>C<\/em> denotes the corner response, <em>i<\/em> is the current iteration, and L1 is the reconstruction error. This adaptive term progressively focuses the model on difficult regions during early training, encouraging structural coherence.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\"><strong>4. Full Optimization Objective<\/strong><\/h3>\n\n\n\n<p style=\"text-align: justify\">The total training loss combines three components: image fidelity, perceptual consistency, and structural smoothness:<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"366\" height=\"49\" src=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-7.08.24\u202fPM.png\" alt=\"\" class=\"wp-image-159\" srcset=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-7.08.24\u202fPM.png 366w, https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-7.08.24\u202fPM-300x40.png 300w\" sizes=\"auto, (max-width: 366px) 100vw, 366px\" \/><\/figure>\n<\/div>\n\n\n<p style=\"text-align: justify\">where lambda_s and lambda_p are empirically set to 0.2. The model is optimized end-to-end using Adam, with separate learning rate schedules for the Gaussian parameters and the physics based modules.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"567\" src=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-8.09.39\u202fPM-1024x567.png\" alt=\"\" class=\"wp-image-165\" srcset=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-8.09.39\u202fPM-1024x567.png 1024w, https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-8.09.39\u202fPM-300x166.png 300w, https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-8.09.39\u202fPM-768x426.png 768w, https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/05\/Screenshot-2025-05-09-at-8.09.39\u202fPM.png 1146w\" sizes=\"auto, (max-width: 767px) 89vw, (max-width: 1000px) 54vw, (max-width: 1071px) 543px, 580px\" \/><figcaption class=\"wp-element-caption\"><br><strong>Figure 5:<\/strong> <em><strong>Stage 1: Physics guided static thermal 3D reconstruction.<\/strong>.<\/em> The system builds on 3D Gaussian Splatting (3DGS) and integrates three physics aware modules: the <strong>Viewpoint Aware Attenuation Estimator (VAE)<\/strong> which models atmospheric effects to correct view dependent attenuation. The <strong>Thermal Diffusion Correction Unit (TDCU)<\/strong> refines edge clarity by compensating for heat conduction induced blurring, and finally the <strong>Surface Smoothness Regularizer (SSR)<\/strong> enforces physically consistent temperature continuity by penalizing discontinuities. Together, these components improve fidelity and realism in novel view synthesis of thermal infrared scenes.<\/figcaption><\/figure>\n<\/div>\n\n\n<h2 class=\"wp-block-heading\"><br><strong>Stage 2: Dynamic Thermal Modeling via Physics Guided Temporal Evolution<\/strong><\/h2>\n\n\n\n<article class=\"method-block\">\n<p style=\"text-align: justify\">\nStage&nbsp;2 extends the static reconstruction into a dynamic thermal model by predicting how temperature evolves through time while keeping geometry fixed. This matches the physical assumption that scene structure and appearance are static over short mission windows, while <strong>temperature changes<\/strong>.<\/p>\n\n      <h4>Inputs<\/h4>\n      <ul>\n<li>Frozen Gaussian geometry and SH appearance from Stage&nbsp;1<\/li>\n<li>Position encodings and time embeddings spanning intermediate timestamps<\/li>\n<li>We also allow additional scene cues if available (e.g., semantic\/geometric features) depending on the dataset, though our core pipeline remains SH-based<\/li>\n      <\/ul>\n\n      <h4>Thermal Property Estimation<\/h4>\n      <p style=\"text-align: justify\">\nWe predict physically meaningful per-Gaussian thermal properties that govern heat transfer, including emissivity, heat transfer, and heat capacity. These quantities parameterize a thermodynamic update that explains observed cooling\/heating patterns rather than fitting each timestep independently.<\/p>\n\n      <h4>Temporal Integration<\/h4>\n      <p style=\"text-align: justify\">\nGiven an initial temperature and predicted thermal properties, we compute per-step temperature variation and integrate across the discretized time interval to obtain <code>Temp_integral(t)<\/code>. We supervise both instantaneous temperature predictions and integrated evolution to enforce consistency and physical plausibility.<\/p>\n\n<h4>Stage 2 Output<\/h4>\n<ul>\n<li>\nA time continuous temperature estimate that supports rendering thermal novel views at arbitrary timestamps.<\/li>\n<li>Consistent thermal evolution over time, grounded by learned thermodynamic parameters.<\/li>\n      <\/ul>\n    <\/article>\n\n   \n\n\n\n <article class=\"method-block\">\n <h3>Training and Rendering<\/h3>\n<p style=\"text-align: justify\">\nBoth stages rely on differentiable Gaussian rasterization for rendering. We optimize against observed thermal frames using reconstruction losses and physics-aware regularization. Stage&nbsp;1 focuses on stable geometry and per-timestamp temperatures, while Stage&nbsp;2 optimizes temperature evolution under physical constraints with geometry frozen.\n      <\/p>\n    <\/article>\n\n    <article class=\"method-block\">\n      <h3>Pipeline Overview<\/h3>\n      <ul>\n        <li><strong>Stage 1<\/strong> recovers a stable static thermal 3D scene and <code>Temp(t)<\/code> at observed timestamps.<\/li>\n        <li><strong>Stage 2<\/strong> models time-varying temperature using learned thermal properties and temporal integration.<\/li>\n        <li>Geometry and appearance remain fixed; <strong>only temperature evolves<\/strong>, enabling dynamic thermal reconstruction.<\/li>\n      <\/ul>\n    <\/article>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"647\" src=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/12\/Screenshot-2025-12-12-at-7.30.40-PM-1024x647.png\" alt=\"\" class=\"wp-image-217\" srcset=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/12\/Screenshot-2025-12-12-at-7.30.40-PM-1024x647.png 1024w, https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/12\/Screenshot-2025-12-12-at-7.30.40-PM-300x190.png 300w, https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/12\/Screenshot-2025-12-12-at-7.30.40-PM-768x486.png 768w, https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/12\/Screenshot-2025-12-12-at-7.30.40-PM-1536x971.png 1536w, https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/wp-content\/uploads\/sites\/139\/2025\/12\/Screenshot-2025-12-12-at-7.30.40-PM-2048x1295.png 2048w\" sizes=\"auto, (max-width: 767px) 89vw, (max-width: 1000px) 54vw, (max-width: 1071px) 543px, 580px\" \/><figcaption class=\"wp-element-caption\"><br><strong>Figure 6. Overview of our proposed two stage thermal reconstruction framework.<\/strong><br>Stage 1 performs physics guided static thermal 3D reconstruction, producing optimized 3D Gaussians and per-Gaussian temperature at discrete timestamps. Stage 2 freezes geometric parameters and models temporal thermal evolution using time and position encoded inputs, predicting continuous temperature changes via thermodynamic integration for dynamic thermal novel view synthesis.<\/figcaption><\/figure>\n\n\n\n<p><\/p>\n","protected":false},"excerpt":{"rendered":"<p>We present a physics-guided, two-stage framework for dynamic thermal scene reconstruction from UAV infrared imagery using 3D Gaussian Splatting. The core design principle is to decouple static scene geometry from time-varying thermal dynamics: Stage&nbsp;1 learns a stable 3D thermal representation at discrete timestamps, and Stage&nbsp;2 models temperature evolution over time while keeping geometry fixed. Given &hellip; <\/p>\n<p class=\"link-more\"><a href=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/methodology\/\" class=\"more-link\">Continue reading<span class=\"screen-reader-text\"> &#8220;Methodology&#8221;<\/span><\/a><\/p>\n","protected":false},"author":261,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-7","page","type-page","status-publish","hentry"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.4 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Methodology - End-to-End Infrared UAV Mapping: An Integrated Framework for Thermal Scene Reconstruction<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/mscvprojects.ri.cmu.edu\/2025team16-2\/methodology\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Methodology - End-to-End Infrared UAV Mapping: An Integrated Framework for Thermal Scene Reconstruction\" \/>\n<meta property=\"og:description\" content=\"We present a physics-guided, two-stage framework for dynamic thermal scene reconstruction from UAV infrared imagery using 3D Gaussian Splatting. The core design principle is to decouple static scene geometry from time-varying thermal dynamics: Stage&nbsp;1 learns a stable 3D thermal representation at discrete timestamps, and Stage&nbsp;2 models temperature evolution over time while keeping geometry fixed. 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The core design principle is to decouple static scene geometry from time-varying thermal dynamics: Stage&nbsp;1 learns a stable 3D thermal representation at discrete timestamps, and Stage&nbsp;2 models temperature evolution over time while keeping geometry fixed. 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