pith. machine review for the scientific record. sign in

arxiv: 2604.09728 · v1 · submitted 2026-04-09 · 💻 cs.CV · physics.app-ph· physics.data-an

Recognition: 2 theorem links

· Lean Theorem

Data-Driven Automated Identification of Optimal Feature-Representative Images in Infrared Thermography Using Statistical and Morphological Metrics

Authors on Pith no claims yet

Pith reviewed 2026-05-10 16:53 UTC · model grok-4.3

classification 💻 cs.CV physics.app-phphysics.data-an
keywords infrared thermographydefect detectionimage selectionnon-destructive testingMinkowski functionalsstatistical metricsCFRPautomated analysis
0
0 comments X

The pith

Three metrics enable automatic selection of defect-representative images from infrared thermography sequences without prior spatial information.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper develops a data-driven method to identify the most representative images within IRT sequences for revealing subsurface defects and structural anomalies. Conventional metrics like signal-to-noise ratio require prior knowledge of defect locations or reference regions, which prevents fully automated and unsupervised use. The proposed approach relies on three complementary indices that assess statistical heterogeneity, representative area size via Minkowski functionals, and total variation energy to rank images by their defect visibility. Experimental validation uses pulse-heated data from a carbon fiber-reinforced polymer plate with six artificial defects at known depths, backed by thermal model simulations. This setup aims to support reliable automated image selection in non-destructive testing workflows.

Core claim

The central claim is that the Homogeneity Index of Mixture (HI), Representative Elementary Area (REA), and Total Variation Energy (TVE) metrics—derived from local intensity distribution deviations, two-dimensional Minkowski-functional adaptations, and geometrical-topological energy—provide robust and unbiased ranking of images in IRT datasets by defect representation without requiring any prior spatial information about defect locations or defect-free regions, as demonstrated on experimental pulse-heated CFRP plate data containing defects at depths from 0.135 mm to 0.810 mm and supported by one-dimensional N-layer thermal simulations.

What carries the argument

The three complementary metrics—Homogeneity Index of Mixture quantifying statistical heterogeneity via local-to-global intensity distribution deviations, Representative Elementary Area adapted from Minkowski functionals for two-dimensional images, and Total Variation Energy index for sensitivity to localized anomalies—that together enable data-driven ranking and selection of optimal feature-representative images.

If this is right

  • Enables automated defect-oriented image selection from IRT sequences in a fully unsupervised manner.
  • Produces reliable ranking of image sequences based solely on the proposed metrics.
  • Validated through experimental pulse-heated IRT data on a CFRP plate with artificial defects at multiple depths.
  • Supported by one-dimensional N-layer thermal model simulations for additional confirmation.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The approach could extend to sequence selection tasks in other non-destructive testing modalities that generate time- or parameter-varying image data.
  • Integration into industrial pipelines might allow real-time automated processing for quality control without manual image review.
  • Performance on real-world defects rather than artificial ones remains an open question for broader deployment.

Load-bearing premise

The three metrics will consistently rank images by defect visibility across different materials, defect types, and heating conditions without any reference to known defect locations or defect-free regions.

What would settle it

Testing the metrics on IRT sequences from a new material or with natural defects and checking whether the top-ranked images match the actual defect locations once those locations are independently verified by destructive inspection or another reference method.

Figures

Figures reproduced from arXiv: 2604.09728 by Harutyun Yagdjian, Martin Gurka.

Figure 1
Figure 1. Figure 1: The following schematic representation provides a visual flowchart [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Schematically representation of CFRP plate. [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 6
Figure 6. Figure 6: Schematic overview of the window selection strategy. A deterministic approach is contrasted with statistical approaches, which include random and static window selection [PITH_FULL_IMAGE:figures/full_fig_p010_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: The following flowchart illustrates Stage 2 of the proposed calculation methodology. The calculation of the [PITH_FULL_IMAGE:figures/full_fig_p010_7.png] view at source ↗
Figure 11
Figure 11. Figure 11: The proposed methodology, when applied to both amplitude and phase sequences derived from PPT data, yields highly comparable results. A representative example is shown in [PITH_FULL_IMAGE:figures/full_fig_p015_11.png] view at source ↗
read the original abstract

Infrared thermography (IRT) is a widely used non-destructive testing technique for detecting structural features such as subsurface defects. However, most IRT post-processing methods generate image sequences in which defect visibility varies strongly across time, frequency, or coefficient/index domains, making the identification of defect-representative images a critical challenge. Conventional evaluation metrics, such as the signal-to-noise ratio (SNR) or the Tanimoto criterion, often require prior knowledge of defect locations or defect-free reference regions, limiting their suitability for automated and unsupervised analysis. In this work, a data-driven methodology is proposed to identify images within IRT datasets that are most likely to contain and represent structural features, particularly anomalies and defects, without requiring prior spatial information. The approach is based on three complementary metrics: the Homogeneity Index of Mixture (HI), which quantifies statistical heterogeneity via deviations of local intensity distributions from a global reference distribution; a Representative Elementary Area (REA), derived from a Minkowski-functional adaptation of the Representative Elementary Volume concept to two-dimensional images; and a geometrical-topological Total Variation Energy (TVE) index, also based on two-dimensional Minkowski functionals, designed to improve sensitivity to localized anomalies. The framework is validated experimentally using pulse-heated IRT data from a carbon fiber-reinforced polymer (CFRP) plate containing six artificial defects at depths between 0.135 mm and 0.810 mm, and is further supported by one-dimensional N-layer thermal model simulations. The results demonstrate robust and unbiased ranking of image sequences and provide a reliable basis for automated defect-oriented image selection in IRT.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 1 minor

Summary. The paper proposes a data-driven framework for automatically identifying defect-representative images in IRT sequences without requiring prior knowledge of defect locations or reference regions. It defines three metrics—Homogeneity Index of Mixture (HI) based on local vs. global intensity distributions, Representative Elementary Area (REA) adapted from Minkowski functionals, and Total Variation Energy (TVE) also using 2D Minkowski functionals—and claims experimental validation on pulse-heated data from a single CFRP plate containing six artificial defects plus supporting 1D N-layer thermal simulations, asserting that the metrics enable robust, unbiased ranking for automated defect-oriented selection.

Significance. If the metrics deliver consistent rankings, the work would address a practical bottleneck in IRT post-processing by removing dependence on reference regions or known defect positions, a limitation of conventional metrics such as SNR and Tanimoto. The first-principles construction of HI, REA, and TVE from statistical heterogeneity and morphological descriptors is a clear strength and could extend to other imaging domains where unsupervised feature selection is needed.

major comments (2)
  1. [Abstract] Abstract: The assertion that the framework 'provides a reliable basis for automated defect-oriented image selection' and demonstrates 'robust and unbiased ranking' is not supported by any quantitative results, error analysis, ranking scores, or direct comparisons to baselines such as SNR or Tanimoto; the central claim therefore rests on unshown evidence.
  2. [Experimental validation] Experimental validation section: The reported experiments use pulse-heated IRT data from only a single CFRP specimen with six flat-bottom holes at fixed depths (0.135–0.810 mm); this limited setup does not test whether HI, REA, and TVE produce consistent defect-visibility rankings when material thermal properties, defect morphology, or heating transients vary, which is required for the unsupervised generalization claim.
minor comments (1)
  1. [Abstract] Abstract: The 1D N-layer thermal model simulations are mentioned as supporting evidence but lack any description of layer parameters, boundary conditions, or how their outputs quantitatively corroborate the experimental metric rankings.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive and detailed comments. We have addressed each major point below with targeted revisions to strengthen the quantitative support and clarify the scope of the validation.

read point-by-point responses
  1. Referee: [Abstract] Abstract: The assertion that the framework 'provides a reliable basis for automated defect-oriented image selection' and demonstrates 'robust and unbiased ranking' is not supported by any quantitative results, error analysis, ranking scores, or direct comparisons to baselines such as SNR or Tanimoto; the central claim therefore rests on unshown evidence.

    Authors: We agree that the abstract would benefit from explicit quantitative backing. The manuscript presents results on image rankings via the three metrics, but to directly address this, we have added a new table in the revised version reporting ranking consistency scores (e.g., Kendall tau coefficients across defect depths), standard deviations from repeated metric computations, and side-by-side comparisons against SNR and Tanimoto on the same IRT sequences. These additions provide the numerical evidence for the claims of robust, unbiased selection. revision: yes

  2. Referee: [Experimental validation] Experimental validation section: The reported experiments use pulse-heated IRT data from only a single CFRP specimen with six flat-bottom holes at fixed depths (0.135–0.810 mm); this limited setup does not test whether HI, REA, and TVE produce consistent defect-visibility rankings when material thermal properties, defect morphology, or heating transients vary, which is required for the unsupervised generalization claim.

    Authors: The single-specimen design with six defects at varying depths does provide internal variation in thermal contrast and morphology, supplemented by 1D N-layer simulations that systematically vary thermal diffusivity, layer thicknesses, and heating pulse parameters. We acknowledge this does not fully cover all possible material or defect variations. In revision, we have inserted an explicit limitations paragraph stating the current scope and have expanded the simulation results to include additional transient and property sweeps, while noting that broader multi-material testing remains future work. revision: partial

Circularity Check

0 steps flagged

No circularity: metrics constructed from independent statistical and morphological definitions

full rationale

The three metrics (HI via local-vs-global intensity distribution deviations, REA and TVE via direct 2D Minkowski functional adaptations) are defined from first principles without reference to defect locations, fitted parameters, or prior self-citations. They are then applied to external pulse-heated CFRP experimental data and 1D simulations; the resulting image rankings do not reduce by construction to the input definitions or to any self-referential loop. The derivation chain remains self-contained and externally falsifiable.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the unproven domain assumption that the three metrics correlate with defect presence in the absence of any spatial reference; no free parameters or invented entities are mentioned in the abstract.

axioms (1)
  • domain assumption The Homogeneity Index, Representative Elementary Area, and Total Variation Energy metrics reliably indicate the presence of structural features without reference regions.
    This assumption is required for the unsupervised ranking to work as claimed.

pith-pipeline@v0.9.0 · 5599 in / 1241 out tokens · 57713 ms · 2026-05-10T16:53:09.387044+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

44 extracted references · 37 canonical work pages

  1. [1]

    Maldague, S

    X. Maldague, S. Marinetti. Pulse phase infrared thermography. Journal of Applied Physics 1 March 1996; 79 (5): 2694–2698. https://doi.org/10.1063/1.362662

  2. [2]

    Shepard and J.R

    S.M. Shepard and J.R. Lhota and B.A. Rubadeux and D. Wang and T. Ahmed, Reconstruction and enhancement of active thermographic image sequences. Optical Engineering 42.5 (2003): 1337-1342

  3. [3]

    N. Rajic, Principal component thermography for flaw contrast enhancement and flaw depth characterisation in composite structures, Composite Structures, Volume 58, Issue 4, 2002, Pages 521-528, ISSN 0263-8223, https://doi.org/10.1016/S0263-8223(02)00161-7

  4. [4]

    Klein, M., Maldague, X.P., Pilla, M., & Salerno, A. (2002). New absolute contrast for pulsed thermography. Quantitative InfraRed Thermography, 53-58. https://doi.org/10.21611/QIRT.2002.004

  5. [5]

    Benitez, X

    H. Benitez, X. Maldague, C. Ibarra-Castanedo, H. Loaiza, A. Bendada and E. Caicedo. Modified Differential Absolute Contrast using Thermal Quadrupoles for the Nondestructive Testing of Finite Thickness Specimens by Infrared Thermography. 2006 Canadian Conference on Electrical and Computer Engineering, Ottawa, ON, Canada, 2006, pp. 1039-1042, https://doi.or...

  6. [6]

    Hernán D. Benítez, Clemente Ibarra-Castanedo, AbdelHakim Bendada, Xavier Maldague, Humberto Loaiza, Eduardo Caicedo, Definition of a new thermal contrast and pulse correction for defect quantification in pulsed thermography, Infrared Physics & Technology, Volume 51, Issue 3, 2008, Pages 160-167, ISSN 1350-4495, https://doi.org/10.1016/j.infrared.2007.01.001

  7. [7]

    Yagdjian, M

    H. Yagdjian, M. Gurka, Alternative data evaluation methodology for infrared thermography analogous to the Shock Response Spectrum analysis method, NDT & E International, Volume 146, 2024, 103154, ISSN 0963- 8695, https://doi.org/10.1016/j.ndteint.2024.103154

  8. [8]

    Yagdjian, J

    H. Yagdjian, J. Lecompagnon, P. Hirsch, M. Gurka, Optimization of thermal shock response spectrum as infrared thermography post-processing methodology using Latin hypercube sampling and analytical thermal N-layer model, Infrared Physics & Technology, Volume 143, 2024, 105582, ISSN 1350-4495, https://doi.org/10.1016/j.infrared.2024.105582

  9. [9]

    Yagdjian, J

    H. Yagdjian, J. Lecompagnon, P. Hirsch, M. Ziegler, M. Gurka; Application of the thermal shock response spectrum (TSRS) methodology to various forms of heat sources by pulse thermography and comparison by using a rotating line scan contour search algorithm. J. Appl. Phys. 7 November 2024; 136 (17): 175101. https://doi.org/10.1063/5.0232015

  10. [10]

    Ibarra-Castanedo, Quantitative subsurface defect evaluation by pulsed phase thermography: depth retrieval with the phase, (2005)

    C. Ibarra-Castanedo, Quantitative subsurface defect evaluation by pulsed phase thermography: depth retrieval with the phase, (2005)

  11. [11]

    Panella, A

    F. Panella, A. Pirinu, V. Dattoma. A Brief Review and Advances of Thermographic Image - Processing Methods for IRT Inspection: a Case of Study on GFRP Plate. Exp Tech 45, 429–443 (2021). https://doi.org/10.1007/s40799-020-00414-4

  12. [12]

    Infrared testing of CFRP components: Comparisons of approaches using the Tanimoto criterion. NDT in Canada 2015, 15–17 Jun 2015, Edmonton,

    S. Sojasi, F. Khodayar, F. Lopez, C. Ibarra-Castanedo, X. P. V. Maldague, V. P. Vavilov, and A. Chulkov, “Infrared testing of CFRP components: Comparisons of approaches using the Tanimoto criterion. NDT in Canada 2015, 15–17 Jun 2015, Edmonton,” e-J. Nondestr. Test. 20(7), (2015). https://www.ndt.net/?id=17960

  13. [13]

    Vavilov and D

    V. Vavilov and D. Burleigh, Infrared Thermography and Thermal Nondestructive Testing (Springer Nature Switzerland AG, 2020), https://doi.org/10.1007/978-3-030-48002-8

  14. [14]

    Meola and S

    C. Meola and S. Boccardi, Giovanni Maria Carlomagno, Infrared Thermography in the Evaluation of Aerospace Composite Materials (Woodhead Publishing , 2017 ), pp. 1–24, ISBN 9781782421719, https://doi.org/10.1016/B978-1-78242-171-9.00001-2

  15. [15]

    Infrared thermography processing based on higher-order statistics,

    F. J. Madruga, C. Ibarra-Castanedo, O. M. Conde, J. M. López-Higuera, and X. Maldague, “Infrared thermography processing based on higher-order statistics,” NDT&E Int.43 (8), 661–666 (2010), ISSN 0963- 8695, https://doi.org/10.1016/j.ndteint.2010.07.002

  16. [16]

    Mandelis, Diffusion-Wave Fields, Springer New York, New York, NY , 2001

    A. Mandelis. (2001). Diffusion-Wave Fields. https://doi.org/10.1007/978-1-4757-3548-2

  17. [17]

    J. G. Rosas, M. Blanco, A criterion for assessing homogeneity distribution in hyperspectral images. Part 1: Homogeneity index bases and blending processes, Journal of Pharmaceutical and Biomedical Analysis, Volume 70, 2012, Pages 680-690, ISSN 0731-7085, https://doi.org/10.1016/j.jpba.2012.06.036

  18. [18]

    Torquato, Random Heterogeneous Materials: Microstructure and Macroscopic Properties https://doi.org/10.1007/978-1-4757-6355-3

    S. Torquato, Random Heterogeneous Materials: Microstructure and Macroscopic Properties https://doi.org/10.1007/978-1-4757-6355-3

  19. [19]

    Pierre-Yves Sacré, Pierre Lebrun, Pierre-François Chavez, Charlotte De Bleye, Lauranne Netchacovitch, Eric Rozet, Régis Klinkenberg, Bruno Streel, Philippe Hubert, Eric Ziemons, A new criterion to assess distributional homogeneity in hyperspectral images of solid pharmaceutical dosage forms, Analytica Chimica Acta, Volume 818, 2014, Pages 7-14, ISSN 0003-...

  20. [20]

    Shih-Hao Chou, Yue-Lou Song, Shu-San Hsiau, A Study of the Mixing Index in Solid Particles, KONA Powder and Particle Journal, 2017, Volume 34, Pages 275-281, Released on J-STAGE February 28, 2017, Advance online publication August 30, 2016, Online ISSN 2187-5537, Print ISSN 0288-4534, https://doi.org/10.14356/kona.2017018

  21. [21]

    Stieß, Mechanische Verfahrenstechnik - Partikeltechnologie 1, Springer Berlin Heidelberg, https://doi.org/10.1007/978/3-540-32552-9

    M. Stieß, Mechanische Verfahrenstechnik - Partikeltechnologie 1, Springer Berlin Heidelberg, https://doi.org/10.1007/978/3-540-32552-9

  22. [22]

    C. D. Rielly, Mixing Theory, in Pharmaceutical Blending and Mixing, Wiley, Chichester 2015, https://doi.org/10.1002/9781118682692.ch1

  23. [23]

    Mahrous, E.o Curti, S

    M. Mahrous, E.o Curti, S. V. Churakov, N. I. Prasianakis, Petrophysical initialization of core-scale reactive transport simulations on Indiana limestones: Pore-scale characterization, spatial autocorrelations, and representative elementary volume analysis, Journal of Petroleum Science and Engineering, Volume 213, 2022, 110389, ISSN 0920-4105, https://doi....

  24. [24]

    Kellers, MP

    B. Kellers, MP. Lautenschlaeger , N. Rigos, J. Weinmiller, T. Danner, A. Latz. Systematic Workflow for Efficient Identification of Local Representative Elementary Volumes Demonstrated with Lithium-Ion Battery Cathode Microstructures. Batteries. 2023; 9(7):390. https://doi.org/10.3390/batteries9070390

  25. [25]

    Sadeghnejad, M

    S. Sadeghnejad, M. Reinhardt, F. Enzmann, P. Arnold, B. Brandstätter, H. Ott, F. Wilde, S. Hupfer, T. Schäfer, M. Kersten, Minkowski functional evaluation of representative elementary volume of rock microtomography images at multiple resolutions, Advances in Water Resources, Volume 179, 2023, 104501, ISSN 0309-1708, https://doi.org/10.1016/j.advwatres.2023.104501

  26. [26]

    D. Wu, G. Busse, Lock-in thermography for nondestructive evaluation of materials,Revue Générale de Thermique, Volume 37, Issue 8, 1998, Pages 693-703, ISSN 0035-3159, https://doi.org/10.1016/S0035- 3159(98)80047-0

  27. [27]

    R., López-Higuera J

    Hidalgo-Gato R., Andres J. R., López-Higuera J. M., Madruga F. J. (2013), Quantification by signal to noise ratio of active infrared thermography data processing techniques. Optics and Photonics Journal, 2013, 3(4A), 20-26. https://doi.org/10.4236/opj.2013.34A004

  28. [28]

    A. M.P. Boelens, H. A. Tchelepi, QuantImPy: Minkowski functionals and functions with Python, SoftwareX, Volume 16, 2021, 100823, ISSN 2352-7110, https://doi.org/10.1016/j.softx.2021.100823

  29. [29]

    Popow, M

    V. Popow, M. Gurka, Full factorial analysis of the accuracy of automated quantification of hidden defects in an anisotropic carbon fibre reinforced composite shell using pulse phase thermography, NDT & E International 116 (2020) 102359. https://doi.org/10.1016/j.ndteint.2020.102359

  30. [30]

    2009.A Statistical Learning Perspective of Genetic Programming

    VDI e. V., VDI-Wärmeatlas, Springer Vieweg Berlin, Heidelberg (2013), https://doi.org/10.1007/978-3-642- 19981-3

  31. [31]

    Genest, E

    M. Genest, E. Grinzato, P. Bison, S. Marinetti, C. Ibarra-Castanedo, X. Maldague, Shape Effect on Blind Frequency for Depth Inversion in Pulsed Thermography, (2006). 5th International Workshop, Advances in Signal Processing for NDE of Materials - Aug 2005 - Québec City (Canada). https://www.ndt.net/?id=3346

  32. [32]

    Myrach, C

    P. Myrach, C. Maierhofer, M. Reischel, M. Rahammer, N. Holtmann, Untersuchung der Auflösungsgrenzen der Lockin-Thermografie zur Prüfung von Faserverbundwerkstoffen . (2014) DGZfP-Jahrestagung

  33. [33]

    OPTICAL FILTER FOR FLASH LAMPS IN PULSED THERMAL IMAG-ING,

    J. Sun, “OPTICAL FILTER FOR FLASH LAMPS IN PULSED THERMAL IMAG-ING,” US 7,538,938 B2. USA

  34. [34]

    H.Yagdjian, M. Gurka, Impact of the thermal afterglow effect on infrared thermography data evaluation methods, Infrared Physics & Technology, 2024, 105349, ISSN 1350-4495, https://doi.org/10.1016/j.infrared.2024.105349

  35. [35]

    Rosas, S

    J.G. Rosas, S. Armenta, J. Cruz, M. Blanco, A new approach to determine the homogeneity in hyperspectral imaging considering the particle size, Analytica Chimica Acta, Volume 787, 2013, Pages 173-180, ISSN 0003-2670, https://doi.org/10.1016/j.aca.2013.05.040

  36. [36]

    Mixing indexes considering the combination of mean and dispersion information from intensity images for the performance estimation of micromixing

    Hai Fu, Xuling Liua, Songjing Li. Mixing indexes considering the combination of mean and dispersion information from intensity images for the performance estimation of micromixing. RSC Adv., 2017,7, 10906- 10914, https://doi.org/10.1039/C6RA23783E

  37. [37]

    Hedderich, L

    J. Hedderich, L. Sachs, Angewandte Statistik: Methodensammlung mit R, Springer-Verlag, https://doi.org/10.1007/978-3-662-62294-0

  38. [38]

    Chattamvelli, R

    R. Chattamvelli, R. Shanmugam, Descriptive Statistics for Scientists and Engineers, https://doi.org/10.1007/978-3-031-32330-0

  39. [39]

    A new look at the statistical model identification.IEEE Transactions on Automatic Control19, 716–723 (1974)

    H. Akaike, A new look at the statistical model identification, in IEEE Transactions on Automatic Control, vol. 19, no. 6, pp. 716-723, December 1974, doi: 10.1109/TAC.1974.1100705

  40. [40]

    Kurz, Christian U

    Jochen H. Kurz, Christian U. Grosse, Hans-Wolf Reinhardt, Strategies for reliable automatic onset time picking of acoustic emissions and of ultrasound signals in concrete, Ultrasonics, Volume 43, Issue 7, 2005, Pages 538-546, ISSN 0041-624X, https://doi.org/10.1016/j.ultras.2004.12.005

  41. [41]

    Yagdjian, J

    H. Yagdjian, J. Vogtmann, M. Gurka. Development of a new methodology for automated quantification of Impact induces damage pattern in CFRP measured by IRT and X-Ray radiography. ECCM20 - The 20th European Conference on Composite Materials, 2022

  42. [42]

    Kelley, Sample size planning for the coefficient of variation from the accuracy in parameter estimation approach

    K. Kelley, Sample size planning for the coefficient of variation from the accuracy in parameter estimation approach. Behavior Research Methods 39, 755–766 (2007). https://doi.org/10.3758/BF03192966

  43. [43]

    Yagdjian, M

    H. Yagdjian, M. Gurka, One-dimensional N-layer thermal modelling for effective machine learning training data generation for nondestructive testing of composite parts with infrared thermography, Composites Part B: Engineering, Volume 288, 2025, 111902, ISSN 1359-8368, https://doi.org/10.1016/j.compositesb.2024.111902

  44. [44]

    difference of thermal diffusion length

    P. Burgholzer, Thermodynamic Limits of Spatial Resolution in Active Thermography. Int J Thermophys 36, 2328–2341 (2015). https://doi.org/10.1007/s10765-015-1890-7 Appendix A The subsequent appendix presents the corresponding metric curves for the remaining regions of interest (ROIs), shown analogously to Figure 9. It is to be noted that all curves are nor...