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<article article-type="research-article" dtd-version="1.3" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xml:lang="en"><front><journal-meta><journal-id journal-id-type="publisher-id">btps</journal-id><journal-title-group><journal-title xml:lang="en">Safety of Technogenic and Natural Systems</journal-title><trans-title-group xml:lang="ru"><trans-title>Безопасность техногенных и природных систем</trans-title></trans-title-group></journal-title-group><issn pub-type="epub">2541-9129</issn><publisher><publisher-name>Don State Technical University</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.23947/2541-9129-2026-10-3-277-284</article-id><article-id custom-type="edn" pub-id-type="custom">GBFWHH</article-id><article-id custom-type="elpub" pub-id-type="custom">btps-594</article-id><article-categories><subj-group subj-group-type="heading"><subject>Research Article</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>CHEMICAL TECHNOLOGIES, MATERIALS  SCIENCES, METALLURGY</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="ru"><subject>ХИМИЧЕСКИЕ ТЕХНОЛОГИИ, НАУКИ О МАТЕРИАЛАХ, МЕТАЛЛУРГИЯ</subject></subj-group></article-categories><title-group><article-title>Geometrical Parameters of 14G2 Steel Structure as a Material with High Ballistic Resistance</article-title><trans-title-group xml:lang="ru"><trans-title>Геометрические параметры структуры стали 14Г2 как материала с высокой баллистической стойкостью</trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0001-6999-3520</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Пустовойт</surname><given-names>В. Н.</given-names></name><name name-style="western" xml:lang="en"><surname>Pustovoit</surname><given-names>V. N.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Виктор Николаевич Пустовойт, доктор технических наук, профессор, профессор кафедры «Материаловедение и технологии металлов»</p><p>344003, г. Ростов-на-Дону, пл. Гагарина, 1</p></bio><bio xml:lang="en"><p>Viktor N. Pustovoit, Dr. Sci. (Eng.), Professor of the Materials Science and Metal Technology Department </p><p>1, Gagarin Sq., Rostov-on-Don, 344003</p></bio><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0002-8558-1136</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Долгачев</surname><given-names>Ю. В.</given-names></name><name name-style="western" xml:lang="en"><surname>Dolgachev</surname><given-names>Yu. V.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Юрий Вячиславович Долгачев, доктор технических наук, доцент кафедры «Материаловедение и технологии металлов»</p><p>344003, г. Ростов-на-Дону, пл. Гагарина, 1</p></bio><bio xml:lang="en"><p>Yuri V. Dolgachev, Dr. Sci. (Eng.), Associate Professor of the Materials Science and Metal Technology Department</p><p>1, Gagarin Sq., Rostov-on-Don, 344003</p></bio><email xlink:type="simple">ydolgachev@donstu.ru</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0001-6466-412X</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Иванков</surname><given-names>И. В.</given-names></name><name name-style="western" xml:lang="en"><surname>Ivankov</surname><given-names>I. V.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Иван Вениаминович Иванков, аспирант кафедры «Материаловедение и технологии металлов» </p><p>344003, г. Ростов-на-Дону, пл. Гагарина, 1</p></bio><bio xml:lang="en"><p>Ivan V. Ivankov, Postgraduate Student of the Materials Science and Metal Technology Department</p><p>1, Gagarin Sq., Rostov-on-Don, 344003</p></bio><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Донской государственный технический университет</institution><country>Россия</country></aff><aff xml:lang="en"><institution>Don State Technical University</institution><country>Russian Federation</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2026</year></pub-date><pub-date pub-type="epub"><day>31</day><month>08</month><year>2026</year></pub-date><volume>10</volume><issue>3</issue><fpage>277</fpage><lpage>284</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Pustovoit V.N., Dolgachev Y.V., Ivankov I.V., 2026</copyright-statement><copyright-year>2026</copyright-year><copyright-holder xml:lang="ru">Пустовойт В.Н., Долгачев Ю.В., Иванков И.В.</copyright-holder><copyright-holder xml:lang="en">Pustovoit V.N., Dolgachev Y.V., Ivankov I.V.</copyright-holder><license license-type="creative-commons-attribution" xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:type="simple"><license-p>This work is licensed under a Creative Commons Attribution 4.0 License.</license-p></license></permissions><self-uri xlink:href="https://www.bps-journal.ru/jour/article/view/594">https://www.bps-journal.ru/jour/article/view/594</self-uri><abstract><sec><title>Introduction</title><p>Introduction. Increasing the ballistic resistance of armor materials is a pressing scientific and technical challenge driven by the need to develop protective materials that can effectively resist high-speed impacts. Homogeneous isotropic steels, which provide protection through a combination of hardness and toughness, have limited effectiveness under high-speed stress of approximately 103 m/s. These materials typically undergo brittle fracture or complete penetration without significant energy dissipation. A promising alternative approach is the use of heterogeneous and anisotropic materials with a more complex, organized structure that can alter crack propagation trajectories and increase fracture energy intensity. Natural ferrite-martensitic composites (NFMCs), formed in steels quenched from the intercritical temperature range, are an example of such materials. NFMC steels, produced by quenching from the intercritical temperature range, are currently being actively researched. It has been shown that changing the quenching temperature affects the volume ratio of ductile ferrite and high-strength martensite layers, which in turn influences the mechanical properties of the material. However, existing studies have been conducted primarily under static tension or bending conditions. When subjected to ballistic loading with extremely high strain rates, the mechanisms of crack arrest may differ significantly. In this context, the geometric parameters of the structure such as the orientation, length, and thickness of the layers, as well as their ratios, become more important than the strength properties of individual phases. Currently, there is a lack of systematic data on which specific structural characteristics of NFMC are crucial for ballistic resistance, and what optimal values should be. Therefore, the aim of this research is to determine the geometric parameters of NFMC steel structures that ensure effective use in armor protection systems.</p></sec><sec><title>Materials and Methods</title><p>Materials and Methods. The study was conducted on 14G2 steel samples measuring 140×70×7 mm. The NFMC structure was obtained by quenching the steel from the intercritical temperature range with an initial banded ferrite-pearlite structure. Bullet resistance tests were performed by shooting targets of this material at a distance of 50 m from a Dragunov sniper rifle with 7.62 mm cartridges with a heat-strengthened core at a bullet velocity of approximately 103 m/s. The geometric parameters of the structure were assessed using a metallographic method on a Neophot 21 microscope using ToupView software to obtain a quantitative assessment.</p></sec><sec><title>Results</title><p>Results. The microstructure of the studied natural ferritic-martensitic composite, which was a composite material with reinforcing fibers of discrete length, was shown. The results of determining the characteristic parameters of the steel composite geometry in accordance with GOST R 54 570–2011  were presented. The misorientation angle in the structure was 7÷11°. The volume fraction of martensite was 28.37% when quenched from a temperature of 735℃. The average width of the plates of the strengthening phase h̅ = 0.0051 mm and the average free path λ̅⊥ corresponding to the width of ferrite plates с̅ = 0.0131  mm were measured. The ratio c/h was 2.57. The calculated critical length of the martensite layer in NFMC from the condition of equilibrium of normal and shear stresses in it, in NFMC with a total rolling reduction of 70% was 18.3 μm. The data on the distribution of the size of martensite layers in 14G2 steel with the NFMC structure were shown.</p></sec><sec><title>Discussion</title><p>Discussion. The obtained data on geometric parameters of the structure of 14G2 steel, quenched from the intercritical temperature range (735℃) and having NFMC organization, meet the requirements for the composite material. In a layered composite with optimal geometry, as a crack propagates successively from one layer to another along the interface and the crack tip approaches it, delamination can form, hindering the initial crack's propagation. Existing ferrite-martensite interfaces with a length greater than the critical value act as an effective barrier to crack propagation.</p></sec><sec><title>Conclusion</title><p>Conclusion. It was found that high ballistic resistance of the natural ferrite-martensite composite was achieved with an optimal combination of geometric parameters of the composite material structure. At the same time, achieving such an NFMC optimum as armor protection can be ensured by the correct hot rolling technology (total reduction of 70% and higher) and choosing the optimal quenching temperature in the intercritical range.</p></sec></abstract><trans-abstract xml:lang="ru"><sec><title>Введение</title><p>Введение. Повышение баллистической стойкости броневых материалов представляет собой актуальную научно-техническую задачу, обусловленную необходимостью разработки защитных материалов, способных эффективно сопротивляться высокоскоростному ударному воздействию. При высокоскоростном нагружении порядка 103 м/с гомогенные изотропные стали, обеспечивающие защитные свойства за счёт сочетания твёрдости и вязкости, демонстрируют ограниченную эффективность: как правило, наблюдается либо хрупкое разрушение, либо сквозное пробитие без существенного рассеяния энергии. Перспективным альтернативным подходом является применение гетерогенных и анизотропных материалов, имеющих более сложную организованную структуру, способную изменять траекторию распространения трещин и повышать энергоёмкость разрушения. К таким материалам относятся естественные феррито-мартенситные композиты, формируемые в сталях при закалке из межкритического интервала температур (ЕФМК). В настоящее время активно исследуются ЕФМК-стали, получаемые закалкой из межкритического температурного интервала. Показано, что варьирование температуры закалки изменяет объёмное соотношение слоёв пластичного феррита и высокопрочного мартенсита, что, в свою очередь, оказывает влияние на механические свойства материала. Однако существующие исследования выполнены преимущественно в условиях статического растяжения или изгиба. При баллистическом нагружении, характеризующемся экстремально высокими скоростями деформации, механизмы торможения трещины могут принципиально отличаться. При этом на первый план выходят не столько прочностные характеристики фаз, сколько геометрические параметры структуры: ориентация, длина и толщина слоёв, а также их соотношение. В настоящее время отсутствуют систематические данные о том, какие именно структурные характеристики ЕФМК являются определяющими для баллистической стойкости и каковы их оптимальные значения. В связи с этим цель настоящего исследования заключается в определении геометрических параметров структуры ЕФМК-сталей, обеспечивающих эффективное применение данного материала в устройствах броневой защиты.</p></sec><sec><title>Материалы и методы</title><p>Материалы и методы. Образцами для исследования служили пластины из стали 14Г2 размером 140 × 70 × 7 мм. Формирование структуры ЕФМК осуществляли путём закалки из межкритического температурного интервала, при этом исходной являлась строчечная феррито-перлитная структура. Оценку пулестойкости проводили при обстреле мишеней из указанного материала с дистанции 50 м из винтовки СВД патронами калибра 7,62 мм (термоупрочнённый сердечник, начальная скорость пули составляла порядка 103 м/с). Геометрические параметры структуры изучали металлографическим методом на микроскопе Neophot 21 с количественной обработкой изображений в программе ToupView.</p></sec><sec><title>Результаты исследования</title><p>Результаты исследования. Показана микроструктура исследованного естественного ферритно-мартенситного композита, представляющая собой композиционный материал с упрочняющими волоками дискретной длины. </p><p>Представлены результаты определения характерных параметров геометрии стального композита в соответствии с ГОСТ Р 54570–20111 . Угол разориентировки в структуре составил 7–11°. Объемная доля мартенсита при закалке с температуры 735 ℃ составила 28,37 %. Измерены средняя ширина пластин упрочняющей фазы h̅ = 0.0051 мм и средний свободный путь λ̅⊥, соответствующий ширине ферритных пластин с̅ = 0.0131 мм; при этом соотношение c/h составило 2,57. Расчётная критическая длина мартенситного слоя в ЕФМК, определенная из условия равновесия нормальных и касательных напряжений в нём, для ЕФМК с суммарным обжатием при прокатке 70 % составила 18,3 мкм. Приведены данные распределения величины мартенситных слоев в стали 14Г2 со структурой ЕФМК.</p></sec><sec><title>Обсуждение</title><p>Обсуждение. Полученные данные о геометрических параметрах структуры стали 14Г2, закалённой из межкритического интервала температур (735 ℃) и характеризующейся формированием естественного феррито-мартенситного композита, соответствуют требованиям, предъявляемым к композиционным материалам. В слоистом композите с оптимальной геометрией при последовательном прохождении трещины из одного слоя в другой по поверхности раздела, а также при приближении её вершины к данной границе, возможно образование расслоения, затрудняющего дальнейшее распространение исходной трещины. Поверхности раздела феррит-мартенсит, длина которых превышает критическое значение, являются эффективными барьерами на пути её движения. </p></sec><sec><title>Заключение</title><p>Заключение. Установлено, что высокая баллистическая стойкость естественного феррито-мартенситного композита достигается при оптимальном сочетании геометрических параметров структуры данного композиционного материала. При этом получение оптимальных характеристик ЕФМК как броневой защиты может быть обеспечено за счёт рациональной технологии горячей прокатки — суммарного обжатия 70 % и выше — и выбора оптимальной температуры закалки в межкритическом интервале.</p></sec></trans-abstract><kwd-group xml:lang="ru"><kwd>композит</kwd><kwd>сталь</kwd><kwd>мартенсит</kwd><kwd>феррит</kwd><kwd>строчечность</kwd><kwd>баллистическая стойкость</kwd></kwd-group><kwd-group xml:lang="en"><kwd>composite</kwd><kwd>steel</kwd><kwd>martensite</kwd><kwd>ferrite</kwd><kwd>banding</kwd><kwd>ballistic resistance</kwd></kwd-group></article-meta></front><body><p>Introduction. Increasing the ballistic resistance of armor is a crucial issue in the design of modern military equipment [<xref ref-type="bibr" rid="cit1">1</xref>]. At high impact rates, in addition to the basic mechanical characteristics, strict requirements are imposed on alloys regarding the specific geometric arrangement of their internal structure [<xref ref-type="bibr" rid="cit2">2</xref>]. For homogeneous isotropic metal barriers, one of the key factors is the formation of a finely dispersed structure. The main challenge is that traditional homogeneous steels with an isotropic structure, such as tempered martensite, perform protective functions primarily through hardness and toughness. However, at high-energy, dynamic loads (about 10³ m/s), the effectiveness of such barriers is significantly reduced: either brittle destruction or through-penetration of the target occurs without significant dissipation of the kinetic energy of the indenter [<xref ref-type="bibr" rid="cit3">3</xref>]. An alternative approach involves the use of heterogeneous, anisotropic materials with a more complex structural arrangement [<xref ref-type="bibr" rid="cit4">4</xref>]. This article examines in detail the microstructural characteristics of steels with a natural ferrite-martensite composite structure (NFMC), which are considered a promising material for armor protection.</p><p>Over the past few decades, extensive research has been conducted on materials with NFMC structure, formed by heat treatment at temperatures in the intercritical range [<xref ref-type="bibr" rid="cit5">5</xref>]. These materials are referred to as “composites” due to significant differences in the properties between the two phase components that make up the material. Within this composition, highly ductile and relatively soft ferritic layers alternate with high-strength martensitic plates, creating a structure with a distinct texture that is oriented along the direction of rolling. The process of producing these multilayer composites is described in detail in our patent [<xref ref-type="bibr" rid="cit6">6</xref>]. These alloys exhibit the ability to effectively inhibit crack propagation by triggering interlayer delamination along interphase boundaries [7–9]. Earlier, the authors of publications [<xref ref-type="bibr" rid="cit10">10</xref>][<xref ref-type="bibr" rid="cit11">11</xref>] found that targeted control of the heating temperature for quenching directly changed the volume proportions of soft and hard components, determining the final level of operational properties. However, most of the tests were based on static stretching or bending methods [12–14]. In contrast, ballistic loading, characterized by extremely high strain rates, has different mechanisms of crack braking: inertial effects and wave processes begin to dominate [<xref ref-type="bibr" rid="cit3">3</xref>][<xref ref-type="bibr" rid="cit15">15</xref>]. In this case, the determining role is played not by the absolute strength of individual phases, but rather by the spatial parameters of the structure, such as orientation, length and thickness of the layers, their ratio, as well as the maximum length of the reinforcing layer. To date, the scientific literature has not provided comprehensive information on which structural parameters in the NFMC architecture are critical criteria for ensuring bullet resistance, nor have their optimal ranges been determined.</p><p>The aim of this research is to conduct a comprehensive analysis of geometric parameters of NFMC steel structure, including the grain-boundary angle, the dimensional proportions of cross-sectional layers, the critical length of martensitic layer, and other relevant metrics. The optimization of these parameters is expected to maximize the effectiveness of these steels in the design of armor protection systems. The relevance of the chosen factors is justified based on the following considerations: the amount of misorientation directly influences the level of shear stress that can cause the destruction of the high-strength phase; the ratio of the thicknesses of structural elements determines the predisposition to interfacial stratification; the critical length of martensitic layer makes it possible to evaluate the efficiency of load transfer from the matrix to the reinforcing phase. To successfully achieve this goal, it was necessary to consistently solve the following tasks:</p><p>− to assess the degree of orientation of NFMC alloy structure;</p><p>− to measure the volume fraction of the phases, the average cross-sectional width of the plates, as well as the average free path of the reinforcing phase in a soft ferritic base;</p><p>− to perform a theoretical calculation of the critical length of the martensitic layer;</p><p>− to analyze the ratio of the thicknesses of alternating ferritic and martensitic plates, which ensures the stable implementation of the mechanism for extinguishing the kinetic energy of a growing crack due to local interlayer stratification during intense high-speed impact.</p><p>Materials and Methods. The research was conducted on 14G2 steel samples with dimensions of 140×70×7 mm. The NFMC structure was formed by heat treatment — quenching of steel from the intercritical temperature range that initially had a banded ferrite-pearlite structure. The assessment of ballistic resistance was conducted using a comparative method. The characteristics of steel samples with NFMC structure and the same steel with the homogeneous structure of tempered martensite were compared.</p><p>Ballistic tests of targets made from these materials were performed from a distance of 50 m using a Dragunov sniper rifle (SVD). 7.62 mm caliber ammunition with a thermally reinforced core was used for firing. The flight speed of the damage agent was 103 m/s. Ten shots were fired at each type of obstacle.</p><p>As a result of the tests, we recorded a complete penetration of all targets with a homogeneous structure. However, when bullets hit plates with NFMC structure, we observed a ricochet effect, with only deformation depressions (dents) ranging from 1.5 to 2.0 millimeters remaining on the surface.</p><p>Geometric parameters of the structure were evaluated by a metallographic method using a Neophot 21 microscope and ToupView software to obtain quantitative data. At the same time, standard image preparation functions were used for subsequent analysis: framing, brightness adjustment, contrast adjustment, and other basic tools. In addition, built-in algorithms for applying a measuring grid and a scale were used, while the true size of the microstructures was determined by calibrating the micrometer object image. The automatic calculation of volume fractions of the structural components was conducted using the KOI-1 System software package, where stereological operations were performed based on setting brightness intervals. The study of the characteristics under consideration was performed on 15–20 fields of view for each individual sample. Micrographs were captured using a 10Mp ToupCam UA1000CA digital eyepiece camera with an optical resolution of 3584×2748 pixels. On the basis of the obtained microstructural data, the characteristic geometric parameters of the steel composite material were established according to standardized methods regulated by GOST R 54570–20111.</p><p>Research Results. According to the ballistic tests results, high bullet resistance of the material with the structure of natural ferrite-martensitic composite (NFMC) was established. Only the ricochet of the striking elements was recorded. This indicator compared favorably with the characteristics of metal with a similar chemical composition that had a homogeneous tempered martensite structure, the samples of which penetrated. In this regard, the results of the research are presented below (Fig. 1) on the microstructure of the specified NFMC composite material [<xref ref-type="bibr" rid="cit7">7</xref>] reinforced with discrete-length reinforcing fibers [<xref ref-type="bibr" rid="cit8">8</xref>].</p><fig id="fig-1"><caption><p>Fig. 1. Microstructure of 14G2 steel, oriented as a natural ferrite-martensitic composite (quenching at 735°С)</p></caption><graphic xlink:href="btps-10-3-g001.jpeg"><uri content-type="original_file">https://cdn.elpub.ru/assets/journals/btps/2026/3/hSZwr6JxZc30REAit9uWoBbFtyPoms0gmgQwPE9u.jpeg</uri></graphic></fig><p>Table 1 provides the results of determining the characteristic geometry parameters of the steel composite according to GOST R 54570–20112. Following the methodology of the mentioned standard, calculations were conducted based on the data obtained by superimposing the grid (Fig. 1) and then calculating the number of points of intersection of its lines with the studied phase.</p><table-wrap id="table-1"><caption><p>Table 1</p><p>Calculation data for 14G2 steel according to Figure 1</p></caption><table><tbody><tr><td>NL⊥(mm–1)</td><td>NL||(mm–1)</td><td>Al(NL⊥/NL||)</td><td>Ω12</td><td>PL⊥(mm–1)</td><td>PL||(mm–1)</td><td>Al(PL⊥/PL||)</td><td>Ω12</td></tr><tr><td>54.92</td><td>29.62</td><td>1.85</td><td>0.352</td><td>109.83</td><td>59.24</td><td>1.84</td><td>0.352</td></tr><tr><td>V = 28.37           SB⊥ = 0.0182 mm           λ⊥ = 0.0131 mm</td></tr></tbody></table></table-wrap><p>where NL⊥ — number of intersections of particles per unit length of the line perpendicular to the deformation axis; NL|| — number of intersections of particles per unit length of the line parallel to the deformation axis; PL⊥ — number of boundary crossings per unit length of the line perpendicular to the deformation axis; PL|| — number of boundary crossings per unit length of the line parallel to the deformation axis; Al — anisotropy coefficient; Ω12 — degree of alignment of the linear elements of the structure; V — volume fraction of martensite; SB⊥ — average distance (from the center to the center) for the alignment phase; λ⊥ — average free path (from edge to edge) for the alignment phase.</p><p>The angle of misorientation of the strengthening phase (Fig. 1), determined by the method of superimposing secant lines along the orientation axis of the martensitic strips, was 7–11°.</p><p>The volume fraction of martensite, calculated by stereological analysis of the microstructure using the KOI-1 System software, reached 28.37% after quenching at a temperature of 735℃.</p><p>In this work, we used the recommendations of GOST R 54 570-20113, to evaluate parameters such as the average distance between phase centers SB⊥ and the average free path λ⊥ (the distance between the phase boundaries) in the structure shown in Figure 1. After calculating these values, we found that the average thickness of the hardening phase plates was h = 0.0051 mm, and the average free path λ⊥, representing the width of ferritic plates, was c = 0.0131 mm. Thus, the thickness ratio of the ferritic and martensitic phases was c/h = 2.57.</p><p>The most important factor in any composite material reinforced with discrete reinforcing fibers is the longitudinal length of these fibers. This length must exceed a critical value lкр in order to ensure full loading of the martensitic layers of the composition under study. The critical length of the martensitic layer in naturally composite ferrite-martensitic materials (NFMC) was calculated based on the equilibrium condition of normal and tangential stresses within the material [<xref ref-type="bibr" rid="cit11">11</xref>]:</p><p>(1)</p><p>where h, b — thickness and width of the reinforcing layer; τ = σT / 2 — tangential stresses at the ferrite-martensite interface. It follows:</p><p>(2)</p><p>According to the calculation results using equation (2), considering the values of h and b measured in the NFMC with a total compression of 70% during rolling, the value of lкр = 18.3 µm was obtained. A histogram of the distribution of value l in 14G2 steel with NFMC structure is shown in Figure 2.</p><fig id="fig-2"><caption><p>Fig. 2. A histogram of the length distribution of martensite plates in a 14G2 steel sample, the structure of which is shown in Figure 1</p></caption><graphic xlink:href="btps-10-3-g002.jpeg"><uri content-type="original_file">https://cdn.elpub.ru/assets/journals/btps/2026/3/LHNBwcsn7R42lqdcVg1qQ5tbD03uwZ8j8FHNozDf.jpeg</uri></graphic></fig><p>Discussion. The obtained data on the geometric parameters of 14G2 steel structure, hardened from the intercritical temperature range (735°С) and having NFMC organization, met modern requirements for composite materials. The high degree of structure orientation, the length of the reinforcing plates was higher than their critical value, the ratio of the thickness of the matrix and the reinforcing layer were within the optimal values.</p><p>Coincidence of the values of orientation degree Ω12 (Table 1), found by two different methods, confirmed the reliability of the results. A high degree of structure orientation was indicated by the condition Ω12 &gt; 0. When the impact was directed orthogonally to the rolling plane of steel composite, the misorientation of the reinforcing phase played a significant role. This fact was due to the dependence of the shear stress magnitude required to break the “fiber” on the misorientation angle. To achieve high impact resistance, it was important to minimize misorientation, which could be achieved by a significant degree of compression during hot rolling (at least 70%). The maximum allowable misorientation level [<xref ref-type="bibr" rid="cit9">9</xref>] for these composites was 15° [<xref ref-type="bibr" rid="cit10">10</xref>]. In the microstructure of the material studied, the misorientation angle ranged from 7° to 11°</p><p>In the process of varying the quenching temperature, the ratio of volume fractions in the martensite-ferrite system could change. In particular, during the heat treatment of steel heated to lower temperatures, the volume fraction of martensitic component of the alloy decreased, but the carbon concentration increased at the same time. This presented an opportunity to deliberately adjust the mechanical properties of the material.</p><p>In numerous scientific papers dedicated to the study of the reasons for the high strength of composite materials [<xref ref-type="bibr" rid="cit11">11</xref>], the importance of the critical volume (Vкр) of the composite reinforcement component was convincingly demonstrated [<xref ref-type="bibr" rid="cit12">12</xref>]. The calculations of this parameter were conducted taking into account the strength limits of the matrix and hardening phase. The absolute value of the critical volume was estimated at approximately 50% [<xref ref-type="bibr" rid="cit13">13</xref>]. At the same time, similar estimations were made for the conditions of static loading of composites under tension (along the reinforcing fiber) or bending [<xref ref-type="bibr" rid="cit14">14</xref>], as well as during dynamic bending during impact strength tests [<xref ref-type="bibr" rid="cit16">16</xref>]. The ballistic stability of NFMC was evaluated under conditions of orthogonal high-power impact upon impact at a speed of ~10³ m/s. It was shown [<xref ref-type="bibr" rid="cit15">15</xref>] that at such speeds, the mechanical properties of composite components could not affect the dynamic resistance at all. Instead, the role of inertial forces, paths and methods of shock wave propagation increased dramatically [<xref ref-type="bibr" rid="cit17">17</xref>]. In this case, the concept of Vкр lost its original physical meaning and the proportion of the volume fractions of ferrite and martensite was assumed to be approximately 80/20. This unambiguously determined the thickness ratio of ferritic (c) and martensitic (h) plates at the level of c/h ≥ 3.</p><p>At this ratio, the growth of the crack was inhibited due to the stratification of the material within the ferritic matrix, significantly increasing the overall ballistic resistance [<xref ref-type="bibr" rid="cit5">5</xref>]. The measured ratio for the structure under study was 2.57, which was slightly lower than the threshold value mentioned above. This naturally reduced the likelihood of delamination during high-speed crack propagation and reduced the chance of ricochet during high-speed impact. To achieve an optimal c/h ratio in this scenario, it would be advisable to adjust the quenching temperature from the intercritical range to below 735°C.</p><p>When conducting ballistic tests on plates with a thickness of 7 mm, according to the previously described methodology, a target sample with an isotropic tempered martensite structure broke through, whereas a projectile invariably ricocheted from a target with the NFMC structure. This was due to the fact that the layered composite, with optimal geometric characteristics in all parameters, was able to form local stratifications [<xref ref-type="bibr" rid="cit5">5</xref>] as cracks propagated in it [<xref ref-type="bibr" rid="cit12">12</xref>] sequentially from one layer to another along the interface and as the crack tip approached it. As shown in Figure 3, these stratifications created conditions for the initial crack to move to a new position, which did not contribute to its further development. Thus, the ferrite-martensite phase interface with a length of l &gt; lкр could serve as an effective barrier to crack propagation. Figure 3a illustrates how the trajectory of the crack in the NFMC sample changed when a ricochet occurred. In this case, a bulge formed on the back of the target, and a crack could occur (Fig. 3b). However, there was no material shift beyond the back side.</p><fig id="fig-3"><caption><p>Fig. 3. The trajectory of a crack in the composite during a high-speed impact (a) and a crack on the back of the target (b) [5]</p></caption><graphic xlink:href="btps-10-3-g003.jpeg"><uri content-type="original_file">https://cdn.elpub.ru/assets/journals/btps/2026/3/A2Dl9w0shkeOcUEoxW5FAQuGUlklcfhj8vtlRPMG.jpeg</uri></graphic></fig><p>Conclusion. It has been established that the structure of NFMC steel has a high degree of orientation (Ω12 = 0.352), and this circumstance plays an important role in the case of a powerful impact.</p><p>The ratio of the average widths of martensite and ferrite plates was 2.57. This suggests that it would be beneficial to reduce the quenching temperature from the intercritical range below 735°C to ensure an optimal structural balance. The data on the length distribution of martensitic plates showed a maximum that coincided with the calculated critical length of the reinforcing fiber (18.3 µm). This is a significant indicator, as the ferrite-martensite interfaces with lengths greater than the critical value can act as an effective barrier to crack propagation.</p><p>It has been proven that the excellent ballistic resistance of a natural ferrite-martensitic composite is achieved exclusively through the optimal combination of all geometric parameters in the microstructure of the composite material. At the same time, the successful achievement of the described NFMC configuration optimum (as a specialized armor protection) can only be guaranteed through the use of correct hot rolling techniques (total workpiece compression of 70% or more), as well as careful selection of optimal quenching temperatures within the intercritical range.</p><p>1. GOST R 54570-2011. Steel. Methods for assessing the degree of banding or orientation of microstructures. (In Russ.). URL: https://internet-law.ru/gosts/gost/51810/ (Accessed: 17.05.2026).2. GOST R 54570-2011. Steel. 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