18 research outputs found

    Π’Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠ΅ ΠΏΠΎΠ»Π΅ Π°Π½ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½ΠΎΠ³ΠΎ полупространства, подвиТная Π³Ρ€Π°Π½ΠΈΡ†Π° ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ³ΠΎ ΠΏΠΎΠ΄Π²Π΅Ρ€ΠΆΠ΅Π½Π° Π»ΠΎΠΊΠ°Π»ΡŒΠ½ΠΎΠΌΡƒ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ½ΠΎ-пСриодичСскому Ρ‚Π΅ΠΏΠ»ΠΎΠ²ΠΎΠΌΡƒ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡ‚Π²ΠΈΡŽ Π² условиях Ρ‚Π΅ΠΏΠ»ΠΎΠΎΠ±ΠΌΠ΅Π½Π° с внСшнСй срСдой

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    A noticeably raising interest in analytical research methods in the mathematical theory of the thermal conductivity of solids [1-3] was initiated by various causes, among which, as the most significant, special mention should go to the widespread practical engineering application of computer technology, mathematical modelling techniques and anisotropic materials of various origin. At present, the "anisotropic section" [3, 4] holds a most unique position in the mathematical theory of the thermal conductivity of solids, due both to the specificity of the mathematical models used in it, and to the fair-minded development need in fundamentally new high-performance and absolutely stable computational methods [4-6] to solve real, practically important engineering tasks.The spectrum of practical use of solutions to problems of the mathematical theory of the thermal conductivity, presented in an analytically closed form, is quite wide. In particular, such solutions are used to test new computational algorithms, and the problems generating these solutions are called test problems. And if in the traditional sections of the mathematical theory of the thermal conductivity a set of test problems is very extensive [1-3, 7], then test problems of the "anisotropic thermal conductivity" in regions with fixed and moving boundaries are inconsiderable in number [4, 8-14].The main objective of the research is to solve the problem of determining the temperature field of an anisotropic half-space, the boundary of which moves linearly and is subject to local pulse-periodic thermal action under conditions of heat exchange with the external environment.Π—Π°ΠΌΠ΅Ρ‚Π½ΠΎΠ΅ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΠ΅ интСрСса ΠΊ аналитичСским ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌ исслСдований Π² матСматичСской Ρ‚Π΅ΠΎΡ€ΠΈΠΈ тСплопроводности Ρ‚Π²Π΅Ρ€Π΄Ρ‹Ρ… Ρ‚Π΅Π» [1-3] ΠΈΠ½ΠΈΡ†ΠΈΠΈΡ€ΠΎΠ²Π°Π½ΠΎ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹ΠΌΠΈ ΠΏΡ€ΠΈΡ‡ΠΈΠ½Π°ΠΌΠΈ, срСди ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ…, ΠΊΠ°ΠΊ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ Π·Π½Π°Ρ‡ΠΈΠΌΡ‹Ρ…, слСдуСт Π²Ρ‹Π΄Π΅Π»ΠΈΡ‚ΡŒ ΡˆΠΈΡ€ΠΎΠΊΠΎΠ΅ Π²Π½Π΅Π΄Ρ€Π΅Π½ΠΈΠ΅ Π² ΠΈΠ½ΠΆΠ΅Π½Π΅Ρ€Π½ΡƒΡŽ ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΡƒ Π²Ρ‹Ρ‡ΠΈΡΠ»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ Ρ‚Π΅Ρ…Π½ΠΈΠΊΠΈ, ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² матСматичСского модСлирования ΠΈ Π°Π½ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½Ρ‹Ρ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² Ρ€Π°Π·Π»ΠΈΡ‡Π½ΠΎΠ³ΠΎ происхоТдСния. Π’ настоящСС врСмя Π² матСматичСской Ρ‚Π΅ΠΎΡ€ΠΈΠΈ тСплопроводности Ρ‚Π²Π΅Ρ€Π΄Ρ‹Ρ… Ρ‚Π΅Π» Β«Π°Π½ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½Ρ‹ΠΉ Ρ€Π°Π·Π΄Π΅Π»Β» [3,4] Π·Π°Π½ΠΈΠΌΠ°Π΅Ρ‚ особоС ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠ΅, обусловлСнноС ΠΊΠ°ΠΊ спСцификой ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅ΠΌΡ‹Ρ… Π² Π½Π΅ΠΌ матСматичСских ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ, Ρ‚Π°ΠΊ ΠΈ ΠΎΠ±ΡŠΠ΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΠΉ Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒΡŽ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ ΠΏΡ€ΠΈΠ½Ρ†ΠΈΠΏΠΈΠ°Π»ΡŒΠ½ΠΎ Π½ΠΎΠ²Ρ‹Ρ… Π²Ρ‹ΡΠΎΠΊΠΎΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… ΠΈ Π°Π±ΡΠΎΠ»ΡŽΡ‚Π½ΠΎ устойчивых Π²Ρ‹Ρ‡ΠΈΡΠ»ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² [4-6], ΠΎΡ€ΠΈΠ΅Π½Ρ‚ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… Π½Π° Ρ€Π΅ΡˆΠ΅Π½ΠΈΠ΅ Ρ€Π΅Π°Π»ΡŒΠ½Ρ‹Ρ…, практичСски Π²Π°ΠΆΠ½Ρ‹Ρ… ΠΈΠ½ΠΆΠ΅Π½Π΅Ρ€Π½Ρ‹Ρ… Π·Π°Π΄Π°Ρ‡.Π‘ΠΏΠ΅ΠΊΡ‚Ρ€ практичСского использования Ρ€Π΅ΡˆΠ΅Π½ΠΈΠΉ Π·Π°Π΄Π°Ρ‡ матСматичСской Ρ‚Π΅ΠΎΡ€ΠΈΠΈ тСплопроводности, прСдставлСнных Π² аналитичСски Π·Π°ΠΌΠΊΠ½ΡƒΡ‚ΠΎΠΌ Π²ΠΈΠ΄Π΅, достаточно ΡˆΠΈΡ€ΠΎΠΊ. Π’ частности, ΠΏΠΎΠ΄ΠΎΠ±Π½Ρ‹Π΅ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΡŽΡ‚ для тСстирования Π½ΠΎΠ²Ρ‹Ρ… Π²Ρ‹Ρ‡ΠΈΡΠ»ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠΎΠ², Π° сами Π·Π°Π΄Π°Ρ‡ΠΈ, ΠΏΠΎΡ€ΠΎΠΆΠ΄Π°ΡŽΡ‰ΠΈΠ΅ эти Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ, Π½Π°Π·Ρ‹Π²Π°ΡŽΡ‚ тСстовыми Π·Π°Π΄Π°Ρ‡Π°ΠΌΠΈ. И Ссли Π² Ρ‚Ρ€Π°Π΄ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Ρ… Ρ€Π°Π·Π΄Π΅Π»Π°Ρ… матСматичСской Ρ‚Π΅ΠΎΡ€ΠΈΠΈ тСплопроводности мноТСство тСстовых Π·Π°Π΄Π°Ρ‡ вСсьма ΠΎΠ±ΡˆΠΈΡ€Π½ΠΎ [1-3, 7] Ρ‚ΠΎ тСстовыС Π·Π°Π΄Π°Ρ‡ΠΈ Β«Π°Π½ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½ΠΎΠΉ тСплопроводности» Π² областях с Π½Π΅ΠΏΠΎΠ΄Π²ΠΈΠΆΠ½Ρ‹ΠΌΠΈ ΠΈ двиТущимися Π³Ρ€Π°Π½ΠΈΡ†Π°ΠΌΠΈ вСсьма нСмногочислСнны [4, 8-14].Основная Ρ†Π΅Π»ΡŒ ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π½Ρ‹Ρ… исслСдований – Ρ€Π΅ΡˆΠ΅Π½ΠΈΠ΅ Π·Π°Π΄Π°Ρ‡ΠΈ ΠΎΠ± ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½ΠΈΠΈ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠ³ΠΎ поля Π°Π½ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½ΠΎΠ³ΠΎ полупространства, Π³Ρ€Π°Π½ΠΈΡ†Π° ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ³ΠΎ пСрСмСщаСтся ΠΏΠΎ Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΌΡƒ Π·Π°ΠΊΠΎΠ½Ρƒ ΠΈ ΠΏΠΎΠ΄Π²Π΅Ρ€ΠΆΠ΅Π½Π° Π»ΠΎΠΊΠ°Π»ΡŒΠ½ΠΎΠΌΡƒ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ½ΠΎ-пСриодичСскому Ρ‚Π΅ΠΏΠ»ΠΎΠ²ΠΎΠΌΡƒ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡ‚Π²ΠΈΡŽ Π² условиях Ρ‚Π΅ΠΏΠ»ΠΎΠΎΠ±ΠΌΠ΅Π½Π° с внСшнСй срСдой

    ΠœΠ°Ρ‚Π΅ΠΌΠ°Ρ‚ΠΈΡ‡Π΅ΡΠΊΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ процСссов тСплопСрСноса Π² Ρ‚Π²Π΅Ρ€Π΄ΠΎΠΌ Ρ‚Π΅Π»Π΅ с Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅ΠΌ Π² Π²ΠΈΠ΄Π΅ ΡˆΠ°Ρ€ΠΎΠ²ΠΎΠ³ΠΎ слоя, ΠΏΠΎΠ³Π»ΠΎΡ‰Π°ΡŽΡ‰ΠΈΠΌ ΠΏΡ€ΠΎΠ½ΠΈΠΊΠ°ΡŽΡ‰Π΅Π΅ ΠΈΠ·Π»ΡƒΡ‡Π΅Π½ΠΈΠ΅

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    The paper deals with determining a temperature field of an isotropic solid with inclusion represented as a spherical layer that absorbing penetrating radiation. A hierarchy of simplified analogues of the basic model of the heat transfer process in the system under study was developed, including a β€œrefined model of concentrated capacity”, a β€œconcentrated capacity” model, and a β€œtruncated model of concentrated capacity”. Each of the mathematical models of the hierarchy is a mixed problem for a second-order partial differential equation of the parabolic type with a specific boundary condition that actually takes into account the spherical layer available in the system under study.The use of the Laplace integral transform and the well-known theorems of operational calculus in analytically closed form enabled us to find solutions to the corresponding problems of unsteady heat conduction. The β€œconcentrated capacitance” model was in detail analysed with the object under study subjected to the radiation flux of constant density. This model is associated with a thermally thin absorbing inclusion in the form of a spherical layer. It is shown that it allows us to submit the problem solution of unsteady heat conduction in the analytical form, which is the most convenient in terms of both its practical implementation and a theoretical assessment of the influence, the spherical layer width has on the temperature field of the object under study.Sufficient conditions are determined under which the temperature field of the analysed system can be identified with a given accuracy through the simplified analogues of the basic mathematical model. For simplified analogues of the basic model, the paper presents theoretical estimates of the maximum possible error when determining the radiated temperature field.РассмотрСна Π·Π°Π΄Π°Ρ‡Π° опрСдСлСния Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠ³ΠΎ поля ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½ΠΎΠ³ΠΎ Ρ‚Π²Π΅Ρ€Π΄ΠΎΠ³ΠΎ Ρ‚Π΅Π»Π° с Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅ΠΌ Π² Π²ΠΈΠ΄Π΅ ΡˆΠ°Ρ€ΠΎΠ²ΠΎΠ³ΠΎ слоя, ΠΏΠΎΠ³Π»ΠΎΡ‰Π°ΡŽΡ‰ΠΈΠΌ ΠΏΡ€ΠΎΠ½ΠΈΠΊΠ°ΡŽΡ‰Π΅Π΅ ΠΈΠ·Π»ΡƒΡ‡Π΅Π½ΠΈΠ΅. Π Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Π° иСрархия ΡƒΠΏΡ€ΠΎΡ‰Π΅Π½Π½Ρ‹Ρ… Π°Π½Π°Π»ΠΎΠ³ΠΎΠ² Π±Π°Π·ΠΎΠ²ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ процСсса тСплопСрСноса Π² ΠΈΠ·ΡƒΡ‡Π°Π΅ΠΌΠΎΠΉ систСмС, Π²ΠΊΠ»ΡŽΡ‡Π°ΡŽΡ‰Π°Ρ Β«ΡƒΡ‚ΠΎΡ‡Π½Π΅Π½Π½ΡƒΡŽ модСль сосрСдоточСнной Смкости», модСль «сосрСдоточСнная Π΅ΠΌΠΊΠΎΡΡ‚ΡŒΒ» ΠΈ Β«ΡƒΡΠ΅Ρ‡Π΅Π½Π½ΡƒΡŽ модСль сосрСдоточСнной Смкости». КаТдая ΠΈΠ· матСматичСских ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ ΠΈΠ΅Ρ€Π°Ρ€Ρ…ΠΈΠΈ прСдставляСт собой ΡΠΌΠ΅ΡˆΠ°Π½Π½ΡƒΡŽ Π·Π°Π΄Π°Ρ‡Ρƒ для уравнСния Π² частных ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ… Π²Ρ‚ΠΎΡ€ΠΎΠ³ΠΎ порядка параболичСского Ρ‚ΠΈΠΏΠ° со спСцифичСским ΠΊΡ€Π°Π΅Π²Ρ‹ΠΌ условиСм, фактичСски ΡƒΡ‡ΠΈΡ‚Ρ‹Π²Π°ΡŽΡ‰ΠΈΠΌ Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ ΡˆΠ°Ρ€ΠΎΠ²ΠΎΠ³ΠΎ слоя Π² ΠΈΠ·ΡƒΡ‡Π°Π΅ΠΌΠΎΠΉ систСмС.Π‘ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΠΈΠ½Ρ‚Π΅Π³Ρ€Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ прСобразования Лапласа ΠΈ извСстных Ρ‚Π΅ΠΎΡ€Π΅ΠΌ ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ исчислСния Π² аналитичСски Π·Π°ΠΌΠΊΠ½ΡƒΡ‚ΠΎΠΌ Π²ΠΈΠ΄Π΅ Π½Π°ΠΉΠ΄Π΅Π½Ρ‹ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… Π·Π°Π΄Π°Ρ‡ нСстационарной тСплопроводности. ΠŸΠΎΠ΄Ρ€ΠΎΠ±Π½ΠΎ ΠΏΡ€ΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡ€ΠΎΠ²Π°Π½Π° модСль «сосрСдоточСнная Π΅ΠΌΠΊΠΎΡΡ‚ΡŒΒ» Π² ситуации, ΠΊΠΎΠ³Π΄Π° Π½Π° ΠΎΠ±ΡŠΠ΅ΠΊΡ‚ исслСдований воздСйствуСт ΠΏΠΎΡ‚ΠΎΠΊ излучСния с постоянной ΠΏΠ»ΠΎΡ‚Π½ΠΎΡΡ‚ΡŒΡŽ. Π­Ρ‚Π° модСль ассоциируСтся с тСрмичСски Ρ‚ΠΎΠ½ΠΊΠΈΠΌ ΠΏΠΎΠ³Π»ΠΎΡ‰Π°ΡŽΡ‰ΠΈΠΌ Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅ΠΌ Π² Ρ„ΠΎΡ€ΠΌΠ΅ ΡˆΠ°Ρ€ΠΎΠ²ΠΎΠ³ΠΎ слоя. Показано, Ρ‡Ρ‚ΠΎ ΠΎΠ½Π° позволяСт ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²ΠΈΡ‚ΡŒ Ρ€Π΅ΡˆΠ΅Π½ΠΈΠ΅ рассматриваСмой Π·Π°Π΄Π°Ρ‡ΠΈ нСстационарной тСплопроводности Π² аналитичСском Π²ΠΈΠ΄Π΅, Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡƒΠ΄ΠΎΠ±Π½ΠΎΠΌ с Ρ‚ΠΎΡ‡ΠΊΠΈ зрСния ΠΈ Π΅Π³ΠΎ практичСского примСнСния, ΠΈ тСорСтичСской ΠΎΡ†Π΅Π½ΠΊΠΈ влияния ΡˆΠΈΡ€ΠΈΠ½Ρ‹ ΡˆΠ°Ρ€ΠΎΠ²ΠΎΠ³ΠΎ слоя Π½Π° Ρ„ΠΎΡ€ΠΌΠΈΡ€ΡƒΠ΅ΠΌΠΎΠ΅ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠ΅ ΠΏΠΎΠ»Π΅ ΠΎΠ±ΡŠΠ΅ΠΊΡ‚Π° исслСдований.ΠžΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ достаточныС условия, ΠΏΡ€ΠΈ Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ΠΈΠΈ ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠ΅ ΠΏΠΎΠ»Π΅ Π°Π½Π°Π»ΠΈΠ·ΠΈΡ€ΡƒΠ΅ΠΌΠΎΠΉ систСмы ΠΌΠΎΠΆΠ½ΠΎ ΠΈΠ΄Π΅Π½Ρ‚ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ с Π·Π°Π΄Π°Π½Π½ΠΎΠΉ Ρ‚ΠΎΡ‡Π½ΠΎΡΡ‚ΡŒΡŽ ΠΏΡ€ΠΈ ΠΏΠΎΠΌΠΎΡ‰ΠΈ ΡƒΠΏΡ€ΠΎΡ‰Π΅Π½Π½Ρ‹Ρ… Π°Π½Π°Π»ΠΎΠ³ΠΎΠ² Π±Π°Π·ΠΎΠ²ΠΎΠΉ матСматичСской ΠΌΠΎΠ΄Π΅Π»ΠΈ. Для ΡƒΠΏΡ€ΠΎΡ‰Π΅Π½Π½Ρ‹Ρ… Π°Π½Π°Π»ΠΎΠ³ΠΎΠ² Π±Π°Π·ΠΎΠ²ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ прСдставлСны тСорСтичСскиС ΠΎΡ†Π΅Π½ΠΊΠΈ максимально Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΠΉ ΠΏΠΎΠ³Ρ€Π΅ΡˆΠ½ΠΎΡΡ‚ΠΈ Π² ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½ΠΈΠΈ ΠΈΠ·Π»ΡƒΡ‡Π°Π΅ΠΌΠΎΠ³ΠΎ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠ³ΠΎ поля

    Anisotropic Half-Space Temperature Field with its Moving Boundary Being under Local Pulse-periodic Heat Action in Heat Exchange Conditions with External Environment

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    A noticeably raising interest in analytical research methods in the mathematical theory of the thermal conductivity of solids [1-3] was initiated by various causes, among which, as the most significant, special mention should go to the widespread practical engineering application of computer technology, mathematical modelling techniques and anisotropic materials of various origin. At present, the "anisotropic section" [3, 4] holds a most unique position in the mathematical theory of the thermal conductivity of solids, due both to the specificity of the mathematical models used in it, and to the fair-minded development need in fundamentally new high-performance and absolutely stable computational methods [4-6] to solve real, practically important engineering tasks.The spectrum of practical use of solutions to problems of the mathematical theory of the thermal conductivity, presented in an analytically closed form, is quite wide. In particular, such solutions are used to test new computational algorithms, and the problems generating these solutions are called test problems. And if in the traditional sections of the mathematical theory of the thermal conductivity a set of test problems is very extensive [1-3, 7], then test problems of the "anisotropic thermal conductivity" in regions with fixed and moving boundaries are inconsiderable in number [4, 8-14].The main objective of the research is to solve the problem of determining the temperature field of an anisotropic half-space, the boundary of which moves linearly and is subject to local pulse-periodic thermal action under conditions of heat exchange with the external environment

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    Mathematical Modeling of Heat Transfer Processes in a Solid With Spherical Layer-type Inclusion to Absorb Penetrating Radiation

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    The paper deals with determining a temperature field of an isotropic solid with inclusion represented as a spherical layer that absorbing penetrating radiation. A hierarchy of simplified analogues of the basic model of the heat transfer process in the system under study was developed, including a β€œrefined model of concentrated capacity”, a β€œconcentrated capacity” model, and a β€œtruncated model of concentrated capacity”. Each of the mathematical models of the hierarchy is a mixed problem for a second-order partial differential equation of the parabolic type with a specific boundary condition that actually takes into account the spherical layer available in the system under study.The use of the Laplace integral transform and the well-known theorems of operational calculus in analytically closed form enabled us to find solutions to the corresponding problems of unsteady heat conduction. The β€œconcentrated capacitance” model was in detail analysed with the object under study subjected to the radiation flux of constant density. This model is associated with a thermally thin absorbing inclusion in the form of a spherical layer. It is shown that it allows us to submit the problem solution of unsteady heat conduction in the analytical form, which is the most convenient in terms of both its practical implementation and a theoretical assessment of the influence, the spherical layer width has on the temperature field of the object under study.Sufficient conditions are determined under which the temperature field of the analysed system can be identified with a given accuracy through the simplified analogues of the basic mathematical model. For simplified analogues of the basic model, the paper presents theoretical estimates of the maximum possible error when determining the radiated temperature field

    Optimizing single-tool machining

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