25 research outputs found

    ΠžΠ‘ΠžΠ‘Π•ΠΠΠžΠ‘Π’Π˜ Π­Π›Π•ΠšΠ’Π ΠžΠœΠ•Π₯ΠΠΠžΠΠšΠ£Π‘Π’Π˜Π§Π•Π‘ΠšΠžΠ“Πž ΠŸΠ Π•ΠžΠ‘Π ΠΠ—ΠžΠ’ΠΠΠ˜Π― Π­ΠΠ•Π Π“Π˜Π˜ Π¦Π˜Π›Π˜ΠΠ”Π Π˜Π§Π•Π‘ΠšΠ˜ΠœΠ˜ ΠŸΠ¬Π•Π—ΠžΠšΠ•Π ΠΠœΠ˜Π§Π•Π‘ΠšΠ˜ΠœΠ˜ Π˜Π—Π›Π£Π§ΠΠ’Π•Π›Π―ΠœΠ˜ Π‘ Π’ΠΠ£Π’Π Π•ΠΠΠ˜ΠœΠ˜ ЭКРАНАМИ Π’ Π‘ΠžΠ‘Π’ΠΠ’Π• ΠŸΠ›ΠžΠ‘ΠšΠ˜Π₯ Π‘Π˜Π‘Π’Π•Πœ

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    The problem of sound emission is considered by a system formed from cylindrical piezoceramic radiators with internal acoustically soft screens. Longitudinal axis of emitters lie in one plane. This system is characterized by the interaction of electric, mechanical and acoustic fields in the process of conversion electrical energy to acoustical energy and acoustic fields in the process of forming them in the environments. The purpose of the work is to determine the peculiarities of the electromechanical acoustic transformation of energy by cylindrical piezoceramic radiators with internal screens in the composition of flat systems, taking into account all types of interaction.The research was carried out by the method of bound fields in multiply connected domains with the use of addition theorems for the cylindrical wave functions. The physical fields arising from the emission of sound by such a system are determined by the joint solution of the system of differential equations: the wave equation; equations of motion of thin piezoceramic shells with circular polarization in displacements; the equations of forced electrostatics for piezoceramics at given boundary conditions, the conditions of conjugation of fields at the boundaries of the division of domains and electric conditions.The solution of the problem is reduced to the solution of an infinite system of linear algebraic equations with respect to unknown coefficients of field expansions.An analysis of the results of numerical calculations, performed on the basis of the obtained analytical relations, called to establish a number of features in the electromechanical acoustic transformation of energy by emitters in the composition of flat systems. They include: the role of acoustic interaction in the process of energy conversion; determination of the mechanism of quantitative assessment of the influence of interaction on these processes; the dependence of the degree of violation of the radial symmetry of the acoustic loading of the emitters on the amount of acoustic interaction; the appearance of multimodality of the mechanical field of emitters in the structure of the plane system and the dependence of the redistribution of energy between all modes on the degree of disturbance of the radial symmetry of the acoustic loading of the emitters.РассмотрСна Π·Π°Π΄Π°Ρ‡Π° излучСния Π·Π²ΡƒΠΊΠ° плоской систСмой, ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΈΠ· цилиндричСских ΠΏΡŒΠ΅Π·ΠΎΠΊΠ΅Ρ€Π°ΠΌΠΈΡ‡Π΅ΡΠΊΠΈΡ… ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»Π΅ΠΉ с Π²Π½ΡƒΡ‚Ρ€Π΅Π½Π½ΠΈΠΌΠΈ акустичСски мягкими экранами. ΠŸΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½Ρ‹Π΅ оси ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»Π΅ΠΉ ΠΏΠ°Ρ€Π°Π»Π»Π΅Π»ΡŒΠ½Ρ‹ ΠΈ Π»Π΅ΠΆΠ°Ρ‚ Π² ΠΎΠ΄Π½ΠΎΠΉ плоскости. Указанная систСма характСризуСтся взаимодСйствиСм элСктричСских, мСханичСских ΠΈ акустичСских ΠΏΠΎΠ»Π΅ΠΉ Π² процСссС прСобразования излучатСлями элСктричСской энСргии Π² Π°ΠΊΡƒΡΡ‚ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ ΠΈ взаимодСйствиСм акустичСских ΠΏΠΎΠ»Π΅ΠΉ ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»Π΅ΠΉ Π² процСссС формирования ΠΏΠΎΠ»Π΅ΠΉ Π² ΠΎΠΊΡ€ΡƒΠΆΠ°ΡŽΡ‰ΠΈΡ… срСдах. ЦСлью Ρ€Π°Π±ΠΎΡ‚Ρ‹ являлось ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ закономСрностСй элСктромСханоакустичСского прСобразования энСргии цилиндричСскими ΠΏΡŒΠ΅Π·ΠΎΠΊΠ΅Ρ€Π°ΠΌΠΈΡ‡Π΅ΡΠΊΠΈΠΌΠΈ излучатСлями с Π²Π½ΡƒΡ‚Ρ€Π΅Π½Π½ΠΈΠΌΠΈ экранами Π² составС плоских систСм с ΡƒΡ‡Π΅Ρ‚ΠΎΠΌ всСх Π²ΠΈΠ΄ΠΎΠ² взаимодСйствия.ИсслСдования ΠΎΡΡƒΡ‰Π΅ΡΡ‚Π²Π»ΡΠ»ΠΈΡΡŒ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ связанных ΠΏΠΎΠ»Π΅ΠΉ Π² многосвязных областях с ΠΏΡ€ΠΈΠ²Π»Π΅Ρ‡Π΅Π½ΠΈΠ΅ΠΌ Ρ‚Π΅ΠΎΡ€Π΅ΠΌ слоТСния для цилиндричСских Π²ΠΎΠ»Π½ΠΎΠ²Ρ‹Ρ… Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΉ. ЀизичСскиС поля, Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡŽΡ‰ΠΈΠ΅ ΠΏΡ€ΠΈ ΠΈΠ·Π»ΡƒΡ‡Π΅Π½ΠΈΠΈ Π·Π²ΡƒΠΊΠ° Ρ‚Π°ΠΊΠΎΠΉ систСмой, ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ ΠΏΡƒΡ‚Π΅ΠΌ совмСстного Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ систСмы Π΄ΠΈΡ„Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Ρ… ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ: Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ³ΠΎ уравнСния; ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ двиТСния Ρ‚ΠΎΠ½ΠΊΠΈΡ… ΠΏΡŒΠ΅Π·ΠΎΠΊΠ΅Ρ€Π°ΠΌΠΈΡ‡Π΅ΡΠΊΠΈΡ… ΠΎΠ±ΠΎΠ»ΠΎΡ‡Π΅ΠΊ Π² пСрСмСщСниях; ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ Π²Ρ‹Π½ΡƒΠΆΠ΄Π΅Π½Π½ΠΎΠΉ элСктростатики для ΠΏΡŒΠ΅Π·ΠΎΠΊΠ΅Ρ€Π°ΠΌΠΈΠΊΠΈ ΠΏΡ€ΠΈ Π·Π°Π΄Π°Π½Π½Ρ‹Ρ… Π³Ρ€Π°Π½ΠΈΡ‡Π½Ρ‹Ρ… условиях, условиях сопряТСния ΠΏΠΎΠ»Π΅ΠΉ Π½Π° Π³Ρ€Π°Π½ΠΈΡ†Π°Ρ… Ρ€Π°Π·Π΄Π΅Π»Π° многосвязных областСй ΠΈ элСктричСских условиях.РСшСниС Π·Π°Π΄Π°Ρ‡ΠΈ свСдСно ΠΊ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡŽ бСсконСчной систСмы Π»ΠΈΠ½Π΅ΠΉΠ½Ρ‹Ρ… алгСбраичСских ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ ΠΎΡ‚Π½ΠΎΡΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ нСизвСстных коэффициСнтов Ρ€Π°Π·Π»ΠΎΠΆΠ΅Π½ΠΈΠΉ ΠΏΠΎΠ»Π΅ΠΉ Π² ряды ΠΏΠΎ Π²ΠΎΠ»Π½ΠΎΠ²Ρ‹ΠΌ функциям.Анализ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² числСнных расчСтов, Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Π½Ρ‹Ρ… Π½Π° основС ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… аналитичСских ΡΠΎΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΠΉ, ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ» ΡƒΡΡ‚Π°Π½ΠΎΠ²ΠΈΡ‚ΡŒ ряд закономСрностСй Π² элСктромСханоакустичСском ΠΏΡ€Π΅ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠΈ энСргии излучатСлями Π² составС плоских систСм. ΠŸΡ€ΠΈ этом ΡƒΡ‡Ρ‚Π΅Π½Ρ‹: взаимодСйствиС ΠΏΠΎΠ»Π΅ΠΉ Π² процСссС прСобразования энСргии; взаимодСйствиС ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»Π΅ΠΉ ΠΈ систСмы ΠΏΠΎ акустичСскому полю; ΡΡ‚Π΅ΠΏΠ΅Π½ΡŒ Π½Π°Ρ€ΡƒΡˆΠ΅Π½ΠΈΡ Ρ€Π°Π΄ΠΈΠ°Π»ΡŒΠ½ΠΎΠΉ симмСтрии акустичСского нагруТСния ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»Π΅ΠΉ ΠΎΡ‚ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Ρ‹ акустичСского взаимодСйствия; ΠΌΠ½ΠΎΠ³ΠΎΠΌΠΎΠ΄ΠΎΠ²ΠΎΡΡ‚ΡŒ мСханичСских ΠΏΠΎΠ»Π΅ΠΉ ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»Π΅ΠΉ Π² составС плоской систСмы ΠΈ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ‚ΡŒ пСрСраспрСдСлСния энСргии ΠΌΠ΅ΠΆΠ΄Ρƒ ΠΌΠΎΠ΄Π°ΠΌΠΈ ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠΉ ΠΎΡ‚ стСпСни Π½Π°Ρ€ΡƒΡˆΠ΅Π½ΠΈΡ Ρ€Π°Π΄ΠΈΠ°Π»ΡŒΠ½ΠΎΠΉ симмСтрии акустичСского нагруТСния ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»Π΅ΠΉ

    Π€Π˜Π—Π˜Π§Π•Π‘ΠšΠ˜Π• ΠŸΠžΠ›Π― ΠšΠ Π£Π“ΠžΠ’ΠžΠ“Πž Π¦Π˜Π›Π˜ΠΠ”Π Π˜Π§Π•Π‘ΠšΠžΠ“Πž ΠŸΠ¬Π•Π—ΠžΠšΠ•Π ΠΠœΠ˜Π§Π•Π‘ΠšΠžΠ“Πž ΠŸΠ Π˜Π•ΠœΠΠ˜ΠšΠ Π’ ΠŸΠ Π˜Π‘Π£Π’Π‘Π’Π’Π˜Π˜ ΠŸΠ›ΠžΠ‘ΠšΠžΠ“Πž ΠΠšΠ£Π‘Π’Π˜Π§Π•Π‘ΠšΠ˜ ΠœΠ―Π“ΠšΠžΠ“Πž ЭКРАНА

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    System in the form of a circular cylindrical piezoceramic transducer near a flat acoustic screen was analyzed. The aim of the work was to solve the problem of receiving plane sound waves by Β«cylindrical piezoceramic transducer – flat acoustically soft screenΒ» system.Considered system was characterized by a violation of the radial symmetry of the radiation load of the transducer while maintaining the radial symmetry of the electric load. At the same time, the energy perceived by the system under consideration is distributed between all modes of oscillation of the transducer, while the conversion of mechanical energy into electric is realized only at zero mole of oscillations.Special attention was paid to the method of coupled fields in multiply connected domains using the imaging method. The design model of the Β«transducer–creenΒ» system was formulated taking into account the interaction of acoustic, mechanical and electric fields in the process of energy conversion, the interaction of a cylindrical transducer with a flat screen and the interaction of a converter with elastic media outside and inside it. The physical fields of the system under consideration were determined by following solutions: the wave equation; equations of motion of thin piezoceramic cylindrical shells in displacements; equations of stimulated electrostatics for piezoceramics for given boundary conditions, conditions for coupling fields at interfaces and electrical conditions.A general conclusion was made concerning solving of an infinite system of linear algebraic equations with respect to the unknown coefficients of the expansion of the fields. As an example of the application of the obtained relations, a calculation was made and an analysis of the dependences of the electric fields of the system under consideration for various parameters of its construction on the direction of arrival on the plane wave system was conducted.РассмотрСна систСма Π² Π²ΠΈΠ΄Π΅ ΠΊΡ€ΡƒΠ³ΠΎΠ²ΠΎΠ³ΠΎ цилиндричСского ΠΏΡŒΠ΅Π·ΠΎΠΊΠ΅Ρ€Π°ΠΌΠΈΡ‡Π΅ΡΠΊΠΎΠ³ΠΎ прСобразоватСля Π²Π±Π»ΠΈΠ·ΠΈ плоского акустичСского экрана. ЦСлью Ρ€Π°Π±ΠΎΡ‚Ρ‹ являлось Ρ€Π΅ΡˆΠ΅Π½ΠΈΠ΅ Π·Π°Π΄Π°Ρ‡ΠΈ ΠΏΡ€ΠΈΠ΅ΠΌΠ° плоских Π·Π²ΡƒΠΊΠΎΠ²Ρ‹Ρ… Π²ΠΎΠ»Π½ систСмой «цилиндричСский ΠΏΡŒΠ΅Π·ΠΎΠΊΠ΅Ρ€Π°ΠΌΠΈΡ‡Π΅ΡΠΊΠΈΠΉ ΠΏΡ€Π΅ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒ – плоский акустичСски мягкий экран» с ΡƒΡ‡Π΅Ρ‚ΠΎΠΌ взаимодСйствия физичСских ΠΏΠΎΠ»Π΅ΠΉ прСобразоватСля ΠΌΠ΅ΠΆΠ΄Ρƒ собой ΠΈ прСобразоватСля с ΠΎΠΊΡ€ΡƒΠΆΠ°ΡŽΡ‰ΠΈΠΌΠΈ Π΅Π΅ ΡƒΠΏΡ€ΡƒΠ³ΠΈΠΌΠΈ срСдами.Указанная систСма характСризуСтся Π½Π°Ρ€ΡƒΡˆΠ΅Π½ΠΈΠ΅ΠΌ Ρ€Π°Π΄ΠΈΠ°Π»ΡŒΠ½ΠΎΠΉ симмСтрии Ρ€Π°Π΄ΠΈΠ°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ Π½Π°Π³Ρ€ΡƒΠ·ΠΊΠΈ прСобразоватСля ΠΏΡ€ΠΈ сохранСнии Ρ€Π°Π΄ΠΈΠ°Π»ΡŒΠ½ΠΎΠΉ симмСтрии элСктричСской Π½Π°Π³Ρ€ΡƒΠ·ΠΊΠΈ. ΠŸΡ€ΠΈ этом энСргия, воспринимаСмая рассматриваСмой систСмой, распрСдСляСтся ΠΌΠ΅ΠΆΠ΄Ρƒ всСми ΠΌΠΎΠ΄Π°ΠΌΠΈ ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠΉ прСобразоватСля, Π² Ρ‚ΠΎ врСмя ΠΊΠ°ΠΊ ΠΏΡ€Π΅ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ мСханичСской энСргии Π² ΡΠ»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ осущСствляСтся Ρ‚ΠΎΠ»ΡŒΠΊΠΎ Π½Π° Π½ΡƒΠ»Π΅Π²ΠΎΠΉ ΠΌΠΎΠ»Π΅ ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠΉ.ИсслСдованиС ΠΎΡΡƒΡ‰Π΅ΡΡ‚Π²Π»ΡΠ»ΠΎΡΡŒ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ связанных ΠΏΠΎΠ»Π΅ΠΉ Π² многосвязных областях с ΠΏΡ€ΠΈΠ²Π»Π΅Ρ‡Π΅Π½ΠΈΠ΅ΠΌ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° ΠΈΠ·ΠΎΠ±Ρ€Π°ΠΆΠ΅Π½ΠΈΠΉ. Π‘Ρ„ΠΎΡ€ΠΌΡƒΠ»ΠΈΡ€ΠΎΠ²Π°Π½Π° расчСтная модСль систСмы Β«ΠΏΡ€Π΅ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒ-экран», ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‰Π°Ρ ΡƒΡ‡Π΅ΡΡ‚ΡŒ взаимодСйствиС акустичСского, мСханичСского ΠΈ элСктричСского ΠΏΠΎΠ»Π΅ΠΉ Π² процСссС прСобразования энСргии, взаимодСйствиС цилиндричСского прСобразоватСля с плоским экраном ΠΈ взаимодСйствиС прСобразоватСля с ΡƒΠΏΡ€ΡƒΠ³ΠΈΠΌΠΈ срСдами Π²Π½Π΅ ΠΈ Π²Π½ΡƒΡ‚Ρ€ΠΈ Π΅Π³ΠΎ. ЀизичСскиС поля рассматриваСмой систСмы ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ ΠΏΡƒΡ‚Π΅ΠΌ совмСстного Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ: Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ³ΠΎ уравнСния; ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ двиТСния Ρ‚ΠΎΠ½ΠΊΠΈΡ… ΠΏΡŒΠ΅Π·ΠΎΠΊΠ΅Ρ€Π°ΠΌΠΈΡ‡Π΅ΡΠΊΠΈΡ… цилиндричСских ΠΎΠ±ΠΎΠ»ΠΎΡ‡Π΅ΠΊ Π² пСрСмСщСниях; ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ Π²Ρ‹Π½ΡƒΠΆΠ΄Π΅Π½Π½ΠΎΠΉ элСктростатики для ΠΏΡŒΠ΅Π·ΠΎΠΊΠ΅Ρ€Π°ΠΌΠΈΠΊΠΈ ΠΏΡ€ΠΈ Π·Π°Π΄Π°Π½Π½Ρ‹Ρ… Π³Ρ€Π°Π½ΠΈΡ‡Π½Ρ‹Ρ… условиях, условиях сопряТСния ΠΏΠΎΠ»Π΅ΠΉ Π½Π° Π³Ρ€Π°Π½ΠΈΡ†Π°Ρ… Ρ€Π°Π·Π΄Π΅Π»Π° областСй ΠΈ элСктричСских условиях.РСшСниС Π·Π°Π΄Π°Ρ‡ΠΈ свСдСно ΠΊ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡŽ бСсконСчной систСмы Π»ΠΈΠ½Π΅ΠΉΠ½Ρ‹Ρ… алгСбраичСских ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ ΠΎΡ‚Π½ΠΎΡΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ нСизвСстных коэффициСнтов разлоТСния ΠΏΠΎΠ»Π΅ΠΉ. Π’ качСствС ΠΏΡ€ΠΈΠΌΠ΅Ρ€Π° примСнСния ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… ΡΠΎΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΠΉ ΠΏΡ€ΠΎΠΈΠ·Π²Π΅Π΄Π΅Π½ расчСт ΠΈ Π°Π½Π°Π»ΠΈΠ· зависимостСй элСктричСских ΠΏΠΎΠ»Π΅ΠΉ рассматриваСмой систСмы ΠΏΡ€ΠΈ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°Ρ… Π΅Π΅ построСния ΠΎΡ‚ направлСния ΠΏΡ€ΠΈΡ…ΠΎΠ΄Π° Π½Π° систСму плоских Π²ΠΎΠ»Π½

    FEATURES OF ELECTROMECHANICAL ACOUSTIC ENERGY CONVERSION BY CYLINDRICAL PIEZOCERAMIC TRANSDUCERS WITH INTERNAL SCREENS IN COMPOSITION OF FLAT SYSTEMS

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    The problem of sound emission is considered by a system formed from cylindrical piezoceramic radiators with internal acoustically soft screens. Longitudinal axis of emitters lie in one plane. This system is characterized by the interaction of electric, mechanical and acoustic fields in the process of conversion electrical energy to acoustical energy and acoustic fields in the process of forming them in the environments. The purpose of the work is to determine the peculiarities of the electromechanical acoustic transformation of energy by cylindrical piezoceramic radiators with internal screens in the composition of flat systems, taking into account all types of interaction.The research was carried out by the method of bound fields in multiply connected domains with the use of addition theorems for the cylindrical wave functions. The physical fields arising from the emission of sound by such a system are determined by the joint solution of the system of differential equations: the wave equation; equations of motion of thin piezoceramic shells with circular polarization in displacements; the equations of forced electrostatics for piezoceramics at given boundary conditions, the conditions of conjugation of fields at the boundaries of the division of domains and electric conditions.The solution of the problem is reduced to the solution of an infinite system of linear algebraic equations with respect to unknown coefficients of field expansions.An analysis of the results of numerical calculations, performed on the basis of the obtained analytical relations, called to establish a number of features in the electromechanical acoustic transformation of energy by emitters in the composition of flat systems. They include: the role of acoustic interaction in the process of energy conversion; determination of the mechanism of quantitative assessment of the influence of interaction on these processes; the dependence of the degree of violation of the radial symmetry of the acoustic loading of the emitters on the amount of acoustic interaction; the appearance of multimodality of the mechanical field of emitters in the structure of the plane system and the dependence of the redistribution of energy between all modes on the degree of disturbance of the radial symmetry of the acoustic loading of the emitters

    PHYSICAL FIELDS OF CIRCULAR CYLINDRICAL PIEZOCERAMIC RECEIVER IN PRESENCE OF A FLAT ACOUSTIC SOFT SCREEN

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    System in the form of a circular cylindrical piezoceramic transducer near a flat acoustic screen was analyzed. The aim of the work was to solve the problem of receiving plane sound waves by Β«cylindrical piezoceramic transducer – flat acoustically soft screenΒ» system.Considered system was characterized by a violation of the radial symmetry of the radiation load of the transducer while maintaining the radial symmetry of the electric load. At the same time, the energy perceived by the system under consideration is distributed between all modes of oscillation of the transducer, while the conversion of mechanical energy into electric is realized only at zero mole of oscillations.Special attention was paid to the method of coupled fields in multiply connected domains using the imaging method. The design model of the Β«transducer–creenΒ» system was formulated taking into account the interaction of acoustic, mechanical and electric fields in the process of energy conversion, the interaction of a cylindrical transducer with a flat screen and the interaction of a converter with elastic media outside and inside it. The physical fields of the system under consideration were determined by following solutions: the wave equation; equations of motion of thin piezoceramic cylindrical shells in displacements; equations of stimulated electrostatics for piezoceramics for given boundary conditions, conditions for coupling fields at interfaces and electrical conditions.A general conclusion was made concerning solving of an infinite system of linear algebraic equations with respect to the unknown coefficients of the expansion of the fields. As an example of the application of the obtained relations, a calculation was made and an analysis of the dependences of the electric fields of the system under consideration for various parameters of its construction on the direction of arrival on the plane wave system was conducted

    Frequency properties of electrical fields of cylindrical sonar antenna with a flat baffle in the diametral plane

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    ΠŸΠΎΠ»Π½Ρ‹ΠΉ тСкст доступСн Π½Π° сайтС издания ΠΏΠΎ подпискС: http://radio.kpi.ua/article/view/S0021347016060054By means of method of coupled fields we obtain analytical relations describing electrical fields of cylindrical piezoceramic antennas with flat baffles in diametral plane. Numerical experiment results of frequency characteristics of antennas’ electrical fields dependently on parameters of antenna elements and embodiment are presented.ΠœΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ связанных ΠΏΠΎΠ»Π΅ΠΉ Π½Π°ΠΉΠ΄Π΅Π½Ρ‹ аналитичСскиС ΡΠΎΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΡ, ΠΎΠΏΠΈΡΡ‹Π²Π°ΡŽΡ‰ΠΈΠ΅ элСктричСскиС поля цилиндричСских ΠΏΡŒΠ΅Π·ΠΎΠΊΠ΅Ρ€Π°ΠΌΠΈΡ‡Π΅ΡΠΊΠΈΡ… Π°Π½Ρ‚Π΅Π½Π½ с плоским экраном Π² Π΄ΠΈΠ°ΠΌΠ΅Ρ‚Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ плоскости. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Ρ‹ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ числСнного Π°Π½Π°Π»ΠΈΠ·Π° частотных свойств элСктричСских ΠΏΠΎΠ»Π΅ΠΉ Π°Π½Ρ‚Π΅Π½Π½ Π² зависимости ΠΎΡ‚ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² ΠΎΠ±Ρ€Π°Π·ΡƒΡŽΡ‰ΠΈΡ… Π°Π½Ρ‚Π΅Π½Π½Ρ‹ элСмСнтов ΠΈ конструктивного исполнСния Π°Π½Ρ‚Π΅Π½Π½

    Physical fields of planar sonars which consists of cylindrical piezoceramic emitters

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    ΠœΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ зв’язаних ΠΏΠΎΠ»Ρ–Π² Π² багатозв’язних областях Π²ΠΈΡ€Ρ–ΡˆΠ΅Π½Π° Π·Π°Π΄Π°Ρ‡Π° Π²ΠΈΠΏΡ€ΠΎΠΌΡ–Π½ΡŽΠ²Π°Π½Π½Ρ Π·Π²ΡƒΠΊΡƒ ΠΏΠ»Π°Π½Π°Ρ€Π½ΠΎΡŽ Π°Π½Ρ‚Π΅Π½Π½ΠΎΡŽ Ρ€Π΅ΡˆΡ–Ρ‚ΠΊΠΎΡŽ, ΡƒΡ‚Π²ΠΎΡ€Π΅Π½ΠΎΡŽ Π· Ρ†ΠΈΠ»Ρ–Π½Π΄Ρ€ΠΈΡ‡Π½ΠΈΡ… п’єзокСрамічних Π²ΠΈΠΏΡ€ΠΎΠΌΡ–Π½ΡŽΠ²Π°Ρ‡Ρ–Π² силової Ρ‚Π° компСнсованої конструкцій Π· ΠΎΠΊΡ€ΡƒΠΆΠ½ΠΎΡŽ ΠΏΠΎΠ»ΡΡ€ΠΈΠ·Π°Ρ†Ρ–Ρ”ΡŽ, Π· урахуванням Π²Π·Π°Ρ”ΠΌΠΎΠ΄Ρ–Ρ— Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π½ΠΈΡ…, ΠΌΠ΅Ρ…Π°Π½Ρ–Ρ‡Π½ΠΈΡ… Ρ‚Π° Π·Π²ΡƒΠΊΠΎΠ²ΠΈΡ… ΠΏΠΎΠ»Ρ–Π² Ρƒ процСсі пСрСтворСння Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΈΡ‡Π½ΠΎΡ— Π΅Π½Π΅Ρ€Π³Ρ–Ρ— Π² акустичну Ρ‚Π° Π²Π·Π°Ρ”ΠΌΠΎΠ΄Ρ–Ρ— Π²ΠΈΠΏΡ€ΠΎΠΌΡ–Π½ΡŽΠ²Π°Ρ‡Ρ–Π² Π² Ρ€Π΅ΡˆΡ–Ρ‚Ρ†Ρ– ΠΏΠΎ Π·Π²ΡƒΠΊΠΎΠ²ΠΎΠΌΡƒ полю, Π·ΡƒΠΌΠΎΠ²Π»Π΅Π½ΠΎΡ— Π±Π°Π³Π°Ρ‚ΠΎΠΊΡ€Π°Ρ‚Π½ΠΈΠΌ Ρ€ΠΎΠ·ΡΡ–ΡŽΠ²Π°Π½Π½ΡΠΌ Ρ…Π²ΠΈΠ»ΡŒ Π½Π° Π΅Π»Π΅ΠΌΠ΅Π½Ρ‚Π°Ρ… Ρ€Π΅ΡˆΡ–Ρ‚ΠΊΠΈ. ΠžΡ‚Ρ€ΠΈΠΌΠ°Π½Ρ– Π°Π½Π°Π»Ρ–Ρ‚ΠΈΡ‡Π½Ρ– ΡΠΏΡ–Π²Π²Ρ–Π΄Π½ΠΎΡˆΠ΅Π½Π½Ρ, Ρ‰ΠΎ Π΄ΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ΡŒ Π²ΠΈΠΊΠΎΠ½Π°Ρ‚ΠΈ Ρ€ΠΎΠ·Ρ€Π°Ρ…ΡƒΠ½ΠΊΠΈ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ–Π² всіх Ρ„Ρ–Π·ΠΈΡ‡Π½ΠΈΡ… ΠΏΠΎΠ»Ρ–Π², Ρ‰ΠΎ ΠΏΡ€ΠΈΠΉΠΌΠ°ΡŽΡ‚ΡŒ ΡƒΡ‡Π°ΡΡ‚ΡŒ Π² Ρ€ΠΎΠ±ΠΎΡ‚Ρ–.Using related fields method in multi related areas the problem of sound emitting by planar sonar, which consist of cylindrical piezoceramic emitters was solved. This solution allows us to take into account the interaction of electrical, mechanical and sound fields during the process of converting electrical energy into acoustical and the interaction of the transmitters in the sound field, which is caused by numerous reflections of sound waves from the elements of the sonar. The analytical expressions, that allow to compute characteristics of all physical fields, that take part in sonar operation were obtained.ΠœΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ связанных ΠΏΠΎΠ»Π΅ΠΉ Π² многосвязных областях Ρ€Π΅ΡˆΠ΅Π½Π° Π·Π°Π΄Π°Ρ‡Π° излучСния Π·Π²ΡƒΠΊΠ° ΠΏΠ»Π°Π½Π°Ρ€Π½ΠΎΠΉ Π°Π½Ρ‚Π΅Π½Π½ΠΎΠΉ Ρ€Π΅ΡˆΠ΅Ρ‚ΠΊΠΎΠΉ, ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΈΠ· цилиндричСских ΠΏΡŒΠ΅Π·ΠΎΠΊΠ΅Ρ€Π°ΠΌΠΈΡ‡Π΅ΡΠΊΠΈΡ… ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»Π΅ΠΉ силовой ΠΈ компСнсированной конструкций с ΠΎΠΊΡ€ΡƒΠΆΠ½ΠΎΠΉ поляризациСй, с ΡƒΡ‡Π΅Ρ‚ΠΎΠΌ взаимодСйствия элСктричСских, мСханичСских ΠΈ Π·Π²ΡƒΠΊΠΎΠ²Ρ‹Ρ… ΠΏΠΎΠ»Π΅ΠΉ Π² процСссС прСобразования элСктричСской энСргии Π² Π°ΠΊΡƒΡΡ‚ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ ΠΈ взаимодСйствия ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»Π΅ΠΉ Π² Ρ€Π΅ΡˆΠ΅Ρ‚ΠΊΠ΅ ΠΏΠΎ Π·Π²ΡƒΠΊΠΎΠ²ΠΎΠΌΡƒ полю, обусловлСнного ΠΌΠ½ΠΎΠ³ΠΎΠΊΡ€Π°Ρ‚Π½Ρ‹ΠΌ рассСяниСм Π²ΠΎΠ»Π½ Π½Π° элСмСнтах Ρ€Π΅ΡˆΠ΅Ρ‚ΠΊΠΈ. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ аналитичСскиС выраТСния, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‰ΠΈΠ΅ Π²Ρ‹ΠΏΠΎΠ»Π½ΡΡ‚ΡŒ расчСты ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² всСх физичСских ΠΏΠΎΠ»Π΅ΠΉ, ΡƒΡ‡Π°ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… Π² Ρ€Π°Π±ΠΎΡ‚Π΅ Π°Π½Ρ‚Π΅Π½Π½Ρ‹
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